Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season
Open accessAbstract
We present results from an analysis of all data taken by the BICEP2, Keck Array, and BICEP3 CMB polarization experiments up to and including the 2018 observing season. We add additional Keck Array observations at 220 GHz and BICEP3 observations at 95 GHz to the previous 95/150/220 GHz dataset. The Q/U maps now reach depths of 2.8, 2.8, and 8.8 μK_{CMB} arcmin at 95, 150, and 220 GHz, respectively, over an effective area of ≈600 square degrees at 95 GHz and ≈400 square degrees at 150 and 220 GHz. The 220 GHz maps now achieve a signal-to-noise ratio on polarized dust emission exceeding that of Planck at 353 GHz. We take auto- and cross-spectra between these maps and publicly available WMAP and Planck maps at frequencies from 23 to 353 GHz and evaluate the joint likelihood of the spectra versus a multicomponent model of lensed ΛCDM+r+dust+synchrotron+noise. The foreground model has seven parameters, and no longer requires a prior on the frequency spectral index of the dust emission taken from measurements on other regions of the sky. This model is an adequate description of the data at the current noise levels. The likelihood analysis yields the constraint r_{0.05}<0.036 at 95% confidence. Running maximum likelihood search on simulations we obtain unbiased results and find that σ(r)=0.009. These are the strongest constraints to date on primordial gravitational waves.
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TL;DR
The BICEP/Keck collaboration analyzed all BICEP2, Keck Array, and BICEP3 CMB polarization data through the 2018 observing season, combined with WMAP and Planck maps, to constrain primordial gravitational waves. They report the strongest limit to date, \(r_{0.05}<0.036\) at 95% confidence, with no significant evidence for \(r>0\).
Key findings
- The baseline likelihood gives \(r_{0.05}=0.014^{+0.010}_{-0.011}\) and \(r_{0.05}<0.036\) at 95% confidence; simulations give \(\sigma(r)=0.009\) and a median 95% upper limit of \(r_{0.05}<0.019\).
- Foreground parameters: \(A_{d,353}=4.4^{+0.8}_{-0.7}\,\mu\mathrm{K}^2\), \(A_{\mathrm{sync},23}<1.4\,\mu\mathrm{K}^2\) at 95% confidence, and \(\beta_d=1.49^{+0.13}_{-0.12}\); the synchrotron amplitude now peaks at zero.
- New maps reach depths of 2.8, 2.8, and 8.8 \(\mu\mathrm{K}_{\mathrm{cmb}}\,\mathrm{arcmin}\) at 95, 150, and 220 GHz over effective areas of \(\approx 600\) square degrees at 95 GHz and \(\approx 400\) square degrees at 150 and 220 GHz.
- The 220 GHz maps achieve signal-to-noise on polarized dust emission exceeding that of Planck at 353 GHz; the maximum-likelihood model has PTE 0.94, and the previous limits improved from \(r_{0.05}<0.12\) (BKP) to \(<0.09\) (BK14) to \(<0.07\) (BK15) to \(<0.036\) (BK18).
Methods
- Analysis of BICEP2, Keck Array, and BICEP3 CMB polarization data through the 2018 observing season, adding Keck 220 GHz and BICEP3 95 GHz data to the previous 95/150/220 GHz dataset; maps are made into Q/U, purified to B-modes, apodized, Fourier transformed, and used to form auto- and cross-spectra.
- Joint likelihood uses 66 BB auto- and cross-spectra between BICEP/Keck maps and WMAP 23/33 GHz plus Planck 30, 44, 143, 217, and 353 GHz maps, over \(20<\ell<330\) with 9 bandpowers per spectrum.
- The model is lensed \(\Lambda\)CDM + \(r\) + dust + synchrotron + noise with eight parameters, evaluated with Hamimeche-Lewis likelihood and CosmoMC MCMC; the dust frequency spectral index prior is removed, and the bandpower covariance matrix comes from 499 signal-and-noise simulations.
Limitations
- The paper states that dust decorrelation and foreground complexity more generally “will remain a serious concern” as sensitivity improves, and that the sample variance of the lensing component already dominates \(\sigma(r)\).
- The paper states that the baseline does not allow the dust decorrelation parameter \(\Delta_d\) to vary freely because it is biasing with respect to \(r\); it also notes that including EE spectra assumes an exact EE/BB ratio of 2 and “should not be overinterpreted.”
- The paper states residual uncertainties from point-source polarized flux may yield an upward bias on \(r\) of \(1-3\times10^{-3}\), and noise-bias imperfections may yield a downward bias of \(2\times10^{-3}\); these are subdominant to the statistical uncertainty.
- Evident from the text: the analysis fixes the tensor spectral index \(n_t=0\), assumes a power-law dust spatial spectrum and Gaussian dust fluctuations, and relies on external WMAP/Planck data for foreground separation.
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- Findingreasoning§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 5
The BK18 result r_{0.05}<0.036 represents a fractional improvement equivalent to the two previous steps combined.
“The BK18 result described in this letter, r 0 . 05 < 0 . 036, represents a fractional improvement equivalent to the two previous steps combined.”
Quote in the paperNot a substantial claim - Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 1
The foreground model is an adequate description of the data at the current noise levels.
“This model is an adequate description of the data at the current noise levels.”
- Also stated in: § BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 4 · plain
“This model is an acceptable fit to the data with the probability to exceed (PTE) the observed value of χ 2 being 0.94.”
Quote in the paperSubstantial claim- The authors state this as an assumption: The synchrotron frequency spectrum is a simple power law A_sync ∝ ν^β_s.
- The authors state this as an assumption: The dust spatial power spectrum is a power law D_ℓ ∝ ℓ^α_d.
- The authors state this as an assumption: The synchrotron spatial power spectrum is a power law D_ℓ ∝ ℓ^α_s.
- Also stated in: § BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 4 · plain
- Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 1
The 220 GHz maps achieve a signal-to-noise on polarized dust emission exceeding that of Planck at 353 GHz.
“The 220GHz maps now achieve a signal-to-noise on polarized dust emission exceeding that of Planck at 353 GHz.”
- Also stated in: § BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 6 · plain
“The signal-to-noise on polarized dust emission of our 220 GHz band is now considerably higher than that of the Planck 353 GHz band-i.e. the 220 × 220 noise point is much further below the dust band than the P353 × P353 point.”
Quote in the paperNot a substantial claim - Also stated in: § BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 6 · plain
- Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 3
For r, the zero-to-peak likelihood ratio is 0.46.
“For r , the zero-to-peak likelihood ratio is 0.46.”
Quote in the paperNot a substantial claim - Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 1
The likelihood analysis yields the constraint r_{0.05} < 0.036 at 95% confidence.
“The likelihood analysis yields the constraint r 0 . 05 < 0 . 036 at 95% confidence.”
- Also stated in: § BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 1 · plain
“r 0 . 05 < 0 . 036 at 95% confidence”
- Also stated in: § ACKNOWLEDGMENTS · p. 7 · plain
“The upper limit on the tensor-to-scalar ratio tightens to r 0 . 05 < 0 . 036 at 95% confidence.”
Quote in the paperSubstantial claim - Also stated in: § BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 1 · plain
- Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 3
The baseline analysis yields r_{0.05}=0.014^{+0.010}_{-0.011}.
“r 0 . 05 = 0 . 014 +0 . 010 -0 . 011 ( r 0 . 05 < 0 . 036 at 95% confidence)”
Quote in the paperSubstantial claim - Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 3
The baseline analysis yields A_{sync,23}<1.4 μK^2 at 95% confidence.
“A sync , 23 < 1 . 4 µ K 2 at 95% confidence”
Quote in the paperSubstantial claim - Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 4
The data do not prefer allowing decorrelation of the dust pattern in the model.
“and that the data do not prefer allowing decorrelation of the dust pattern in the model.”
Quote in the paperNot a substantial claim - Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 4
The maximum likelihood model has parameters r_{0.05}=0.011, A_{d,353}=4.4 μK^2, A_{sync,23}=0.6 μK^2, β_d=1.5, β_s=-3.0, α_d=-0.66, α_s=0.00, and ε=-0.11.
“The maximum likelihood model has parameters r 0 . 05 = 0 . 011, A d , 353 = 4 . 4 µ K 2 , A sync , 23 = 0 . 6 µ K 2 , β d = 1 . 5, β s = -3 . 0, α d = -0 . 66, α s = 0 . 00, and ϵ = -0 . 11.”
Quote in the paperNot a substantial claim- The authors state this as an assumption: The synchrotron frequency spectrum is a simple power law A_sync ∝ ν^β_s.
- The authors state this as an assumption: The dust spatial power spectrum is a power law D_ℓ ∝ ℓ^α_d.
- The authors state this as an assumption: The synchrotron spatial power spectrum is a power law D_ℓ ∝ ℓ^α_s.
- Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 6
Running without foreground parameters on simulations containing neither lensing nor dust gives σ(r_{0.05})=0.002.
“Running without foreground parameters on simulations which contain neither lensing or dust gives σ ( r 0 . 05 ) = 0 . 002.”
Quote in the paperNot a substantial claim - Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 4
The maximum likelihood model is an acceptable fit to the data with a probability to exceed the observed χ^2 of 0.94.
“This model is an acceptable fit to the data with the probability to exceed (PTE) the observed value of χ 2 being 0.94.”
Quote in the paperNot a substantial claim- The authors state this as an assumption: The synchrotron frequency spectrum is a simple power law A_sync ∝ ν^β_s.
- The authors state this as an assumption: The dust spatial power spectrum is a power law D_ℓ ∝ ℓ^α_d.
- The authors state this as an assumption: The synchrotron spatial power spectrum is a power law D_ℓ ∝ ℓ^α_s.
- Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 5
The BK18 simulations have a median 95% upper limit of r_{0.05}<0.019.
“The BK18 simulations have a median 95% upper limit of r 0 . 05 < 0 . 019.”
Quote in the paperSubstantial claim - Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 3
The baseline lensed-ΛCDM+dust model from BK15 remains a good description of the data.
“The model plotted is a 'baseline' lensed-ΛCDM+dust model from our previous BK15 analysis, which remains a good description of the data.”
Quote in the paperNot a substantial claim - Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 5
Running without foreground parameters on simulations containing no dust gives σ(r_{0.05})=0.007.
“while running without foreground parameters on simulations which contain no dust gives σ ( r 0 . 05 ) = 0 . 007.”
Quote in the paperNot a substantial claim - Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 3
The baseline analysis yields β_d=1.49^{+0.13}_{-0.12}.
“β d = 1 . 49 +0 . 13 -0 . 12”
Quote in the paperNot a substantial claim - Findingreasoning§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 3
The probability to get a likelihood ratio smaller than 0.46 is 11% if r=0.
“we estimate that the probability to get a likelihood ratio smaller than this is 11% if, in fact, r = 0.”
Quote in the paperNot a substantial claim - Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 6
The BK18 data is consistent with ΛCDM plus a remarkably simple dust-only foreground model.
“Figure 2 shows that the BK18 data is consistent with ΛCDM plus a remarkably simple dust only foreground model.”
Quote in the paperSubstantial claim - Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 3
Compared to BK15, the uncertainties are dramatically reduced for the auto- and cross-spectra of the 95 and 220 GHz bands.
“Comparing this plot to Fig. 2 of BK15 we can see that the uncertainties are dramatically reduced for the autoand cross-spectra of the 95 and 220GHz bands.”
Quote in the paperNot a substantial claim - Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 3
The baseline analysis yields A_{d,353}=4.4^{+0.8}_{-0.7} μK^2.
“A d , 353 = 4 . 4 +0 . 8 -0 . 7 µ K 2”
Quote in the paperNot a substantial claim - Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 5
Running the baseline BK18 analysis on simulations containing no lensing B-modes gives σ(r_{0.05})=0.004.
“Running the baseline BK18 analysis on simulations which contain no lensing B -modes gives σ ( r 0 . 05 ) = 0 . 004”
Quote in the paperNot a substantial claim - Findingown data§ Appendix B: Internal Consistency Tests of New Data · p. 10
In the initial jackknife analysis, a few χ2 and χ values were sufficiently beyond the tails of the simulation distributions that it was unlikely to happen by chance.
“In the initial pass of the jackknife analysis there were a few χ 2 and χ values sitting sufficiently beyond the tails of the simulation distributions that it was unlikely to happen by chance.”
Quote in the paperSubstantial claim - Findingown data§ 1. Likelihood Evolution · p. 14
Switching from BK15 to BK18 data causes the synchrotron amplitude constraint A_sync to shift down to peak at zero.
“In addition the synchrotron amplitude constraint A sync shifts down to peak at zero.”
Quote in the paperNot a substantial claim- The authors state this as an assumption: The power spectrum of the polarized dust emission in the BICEP/Keck field follows a power law.
- Findingown data§ 2. Likelihood Variation · p. 17
With β_d free, the Planck 353 GHz band provides a significant part of the β_d constraint.
“With β d now free, the Planck 353 GHz band provides a significant part of the β d constraint (red curve wider than black in the rightmost panel).”
Quote in the paperNot a substantial claim - Findingown data§ ACKNOWLEDGMENTS · p. 8
Adding BICEP/Keck data through the 2018 season plus BAO data to the Planck 2018 baseline analysis tightens the constraint on r from r0.05 < 0.11 to r0.05 < 0.035.
“The constraint on r tightens from r 0 . 05 < 0 . 11 to r 0 . 05 < 0 . 035.”
Quote in the paperSubstantial claim- The authors state this as an assumption: The power spectrum of the polarized dust emission in the BICEP/Keck field follows a power law.
- Findingown data§ 2. Likelihood Variation · p. 17
There appears to be some tension between the WMAP bands (23 and 33 GHz) and the LFI bands (30 and 44 GHz) in terms of their cross correlation with the BICEP/Keck maps.
“It appears that there is some tension between the WMAP bands (23 and 33 GHz) and the LFI bands (30 and 44 GHz) in terms of their cross correlation with the BICEP/ Keck maps.”
Quote in the paperNot a substantial claim - Findingown data§ 2. Likelihood Variation · p. 15
In the BK18 analysis, the ∆d curve peaks at unity, indicating no decorrelation.
“In contrast to Fig. 21 of BK15 the ∆ d curve peaks at unity (no decorrelation).”
Quote in the paperNot a substantial claim - Findingown data§ 2. Likelihood Variation · p. 17
Dropping both WMAP and LFI results in a highly degraded constraint on A_sync.
“Unsurprisingly dropping both WMAP and LFI results in a highly degraded constraint on A sync (cyan).”
Quote in the paperNot a substantial claim - Findingown data§ 2. Likelihood Variation · p. 18
The reduction of 0.3 in -2 log(L) for the real data offers no significant evidence for detection of decorrelation.
“The reduction of 0.3 for the real data offers no significant evidence for detection of decorrelation.”
Quote in the paperNot a substantial claim - Findingown data§ 2. Likelihood Variation · p. 18
The mean of simulations responds exactly as the sum of the '-sync' and '-r' cases.
“The mean of simulations responds exactly as the sum of the ' -sync' and ' -r ' cases.”
Quote in the paperNot a substantial claim - Findingown data§ 1. Likelihood Evolution · p. 15
With improved sensitivity of BK18, the constraint on β_d becomes β_d = 1.49 +0.13 -0.12.
“With the improved sensitivity of BK18 the constraint becomes β d = 1 . 49 +0 . 13 -0 . 12 .”
Quote in the paperNot a substantial claim - Findingown data§ 2. Likelihood Variation · p. 18
Fixing r=0 results in an increase of 1.0 for the mean of simulations.
“Fixing r = 0 results in an increase of 1.0 for the mean of simulations (which have r = 0).”
Quote in the paperSubstantial claim - Findingcitation§ 1. Likelihood Evolution · p. 15
The predicted lensing BB spectrum for Planck 2018 baseline cosmological parameters has shifted down by 5% for l < 500 relative to the previous Planck 2013-based spectrum.
“The predicted lensing BB spectrum for the Planck 2018 baseline cosmological parameters [2, Table 2] has shifted down by 5% (for ℓ < 500).”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [2]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 4
At 150 and 220 GHz the B maps are dominated by polarized dust emission.
“At 150 and 220 GHz the B maps are dominated by polarized dust emission.”
Quote in the paperSubstantial claim - Findingown data§ 2. Likelihood Variation · p. 18
The increase of 0.6 in -2 log(L) for the real data when fixing r=0 indicates no significant evidence for r > 0.
“The increase for the real data is 0.6 indicating no significant evidence for r > 0.”
Quote in the paperSubstantial claim - Findingown data§ Appendix B: Internal Consistency Tests of New Data · p. 10
Removing two small sub-sets of data moved the problematic jackknife values in such that there were no longer clear problems.
“Through a long process we determined that removing two small sub-sets of data moved these values in such that there were no longer clear problems.”
Quote in the paperSubstantial claim - Findingown data§ Appendix D: Multi Frequency Spectra · p. 13
In the bin-by-bin analysis, the resulting CMB values are consistent with lensed-ΛCDM.
“The results are shown in Fig. 16-the resulting CMB values are consistent with lensed-ΛCDM while the dust values are consistent with the level of dust found in the baseline analysis.”
Quote in the paperNot a substantial claim - Findingown data§ Appendix C: 95 & 220 GHz Spectral Stability · p. 10
The comparison of BK15 and BK18 95 GHz BB spectra shows a large improvement in sensitivity.
“The upper part of Fig. 13 compares the two BB spectra-the large improvement in sensitivity is clear.”
Quote in the paperNot a substantial claim - Findingown data§ 1. Likelihood Evolution · p. 15
Dropping the β_d prior in the BK18 baseline analysis makes A_d just slightly wider.
“In Fig. 17 dropping the β d prior corresponds to the transition from yellow to red curvesr and A sync show very little change while A d gets just slightly wider.”
Quote in the paperNot a substantial claim - Findingown data§ Appendix D: Multi Frequency Spectra · p. 13
In the bin-by-bin analysis, the dust values are consistent with the level of dust found in the baseline analysis.
“The results are shown in Fig. 16-the resulting CMB values are consistent with lensed-ΛCDM while the dust values are consistent with the level of dust found in the baseline analysis.”
Quote in the paperNot a substantial claim - Findingown data§ 1. Likelihood Evolution · p. 15
The joint analysis of Planck 2018 TT,TE,EE+lowE+lensing and BK18 likelihood includes small additional constraining power on r from the Planck likelihood.
“By doing this we also include the small additional constraining power on r which comes from the Planck TT,TE,EE+lowE+lensing likelihood.”
Quote in the paperNot a substantial claim - Findingown data§ 3. Bandpass Uncertainty · p. 22
For all 8 parameters fit in the maximum likelihood framework, expected biases from ±2% bandcenter shifts are low and within statistical uncertainties.
“We show that, for all 8 parameters that we fit for in our maximum likelihood framework, the expected biases are low and within statistical uncertainties.”
Quote in the paperSubstantial claim - Findingown data§ 3. Bandpass Uncertainty · p. 22
None of the shifts observed in real data for r and dust parameters due to bandpass nuisance parameters are statistically significant compared to random fluctuations in simulations.
“We compute the realization-to-realization shift in the likelihood peak and found none of the shifts observed in real data for r and dust parameters to be statistically significant compared to random fluctuations in simulations.”
Quote in the paperSubstantial claim - Findingcitation§ 1. Temperature-to-Polarization Leakage from Residual Beam Mismatch · p. 21
Beam simulations with crosstalk deprojected show that the contribution to ∆(r) from crosstalk is small.
“Beam simulations with crosstalk deprojected (as described in Ref. [34]) show that the contribution to ∆( r ) from crosstalk is small.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [34]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Findingown data§ 2. Likelihood Variation · p. 18
The +A_L-ε case shows no preference for varying the lensing scale factor away from unity for either the real data or the simulations.
“The + A L -ϵ case shows no preference for varying the lensing scale factor away from unity for either the real data (as expected given the results in Fig. 19 above) or the simulations.”
Quote in the paperNot a substantial claim - Findingown data§ 2. Likelihood Variation · p. 18
Fixing the lensing spectrum rescale factor A_BB_L = 0.5 produces very large increases in -2 log(L) for simulations and data, indicating strong incompatibility with such a model.
“If we fix the lensing spectrum rescale factor A BB L = 0 . 5 we see very large increases in -2 log( L ) for simulations and data indicating strong incompatibility with such a model.”
Quote in the paperNot a substantial claim - Findingown data§ 4. Exploration of Alternate Foreground Models · p. 20
The MHD model has a level of synchrotron now in strong conflict with the data.
“The MHD model [59, 60] is also unchanged from BK15 and has a level of synchrotron which is now in strong conflict with the data.”
Quote in the paperNot a substantial claim0 of 2 sources checked- cites [59]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites [60]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Findingown data§ 3. Bandpass Uncertainty · p. 22
Compared to the BK18 baseline, the shift in the 95% upper limit on r due to bandpass nuisance parameters is 3 × 10^-5, negligible compared to statistical uncertainty.
“Compared to the BK18 baseline, the shift in the 95% upper limit on r due to the addition of these nuisance parameters is 3 × 10 -5 , negligible compared to the statistical uncertainty.”
Quote in the paperNot a substantial claim - Findingown data§ 3. Bandpass Uncertainty · p. 22
Bandpass parameter uncertainties are estimated to be small, at the 1% level or less.
“We consider various sources of uncertainty in these measurements and estimate them to be small, at the 1% level or less.”
Quote in the paperSubstantial claim - Findingown data§ 2. Likelihood Variation · p. 18
Setting A_d,353 = 2 μK2 is strongly incompatible with the simulations and data.
“Likewise setting A d , 353 = 2 µ K 2 is strongly incompatible with the simulations and data.”
Quote in the paperNot a substantial claim - Findingown data§ 3. Bandpass Uncertainty · p. 22
The worst case scenario for bandcenter shifts would result in a bias on r of |∆(r)| = 8.4 ± 5 × 10^-4, well below the statistical uncertainty σ(r) = 0.009.
“In particular, we show that the worst case scenario would result in a bias on r of | ∆( r ) | = 8 . 4 ± 5 × 10 -4 , well below the statistical uncertainty σ ( r ) = 0 . 009”
Quote in the paperSubstantial claim - Findingown data§ 4. Exploration of Alternate Foreground Models · p. 19
Amplitude modulated Gaussian dust simulations show no detectable bias on r.
“However, in practice the third line of the table shows no detectable bias.”
Quote in the paperNot a substantial claim - Findingown data§ 1. Temperature-to-Polarization Leakage from Residual Beam Mismatch · p. 21
Compared to BK15, the reduction in T→P bias nearly matches the reduction in statistical uncertainty.
“Compared to BK15 results, the reduction in T → P bias (∆( r ) = 2 . 7 ± 1 . 9 × 10 -3 → 1 . 5 ± 1 . 1 × 10 -3 ) nearly matches the reduction in statistical uncertainty ( σ ( r ) = 0 . 020 → 0 . 009).”
Quote in the paperNot a substantial claim - Interpretationnone given§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 6
We are already in the regime where the sample variance of the lensing component dominates σ(r).
“In addition, we are already in the regime where the sample variance of the lensing component dominates σ ( r ).”
Quote in the paperNot a substantial claim - Premisecitation§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 2
BK14 improved the constraint using Keck Array data at 95 GHz taken during the 2014 season.
“In Ref. [11, hereafter BK14] we improved the constraint using Keck Array data at 95 GHz taken during the 2014 season”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [11]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Study design and conductown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 1
The maximum likelihood search on simulations yields unbiased results.
“Running maximum likelihood search on simulations we obtain unbiased results and find that σ ( r ) = 0 . 009.”
- Also stated in: § BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 4 · plain
“In Appendix E 3 we verify that the likelihood analysis is unbiased”
Quote in the paperSubstantial claim - Also stated in: § BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 4 · plain
- Premisecitation§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 6
Adding a lensing template derived from SPTpol and Planck data to the BK14 analysis resulted in an improved constraint on r.
“we have recently demonstrated a path forward by adding a 'lensing template' derived from SPTpol and Planck data to the BK14 analysis, resulting in an improved constraint on r [49].”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [49]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisecitation§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 2
BK15 improved the constraint again by adding Keck Array data at 95 GHz and 220 GHz taken during the 2015 season.
“and in Ref. [12, hereafter BK15] we improved again adding Keck Array data at 95 GHz and 220 GHz taken during the 2015 season.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [12]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisecitation§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 2
Inflation makes an additional prediction, not yet observed, of a background of tensor perturbations, also known as gravitational waves.
“Inflation makes an additional prediction which has not yet been observed-a background of tensor perturbations, also known as gravitational waves (see Ref. [3] for a review and citations to the original literature).”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [3]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 1
These are the strongest constraints to date on primordial gravitational waves.
“These are the strongest constraints to date on primordial gravitational waves.”
Quote in the paperSubstantial claim - Study design and conductown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 4
Varying the baseline analysis choices and data selection does not significantly alter the results.
“In Appendix E2 we vary the baseline analysis choices and data selection, finding that these do not significantly alter the results”
Quote in the paperNot a substantial claim - Premisenone given§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 6
The lensing B-modes can be spatially separated from a primordial component.
“However, the lensing B -modes can be spatially separated from a primordial component”
Quote in the paperSubstantial claim - Study design and conductown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 5
The agreement with the spectra involving 95 GHz and all the EE spectra, under the assumption that EE/BB = 2 for dust, is a validation of the model.
“The agreement with the spectra involving 95 GHz and all the EE spectra (under the assumption that EE/BB = 2 for dust) is therefore a validation of the model.”
Quote in the paperNot a substantial claim- The authors state this as an assumption: For dust, EE/BB = 2.
- Premisecitation§ 2. Likelihood Variation · p. 15
The Planck 2018 dust analysis did not show any evidence for dust decorrelation.
“The Planck 2018 dust analysis [24] did not show any evidence for dust decorrelation.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [24]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Study design and conductown data§ Appendix B: Internal Consistency Tests of New Data · p. 10
It was necessary to remove BICEP3 data from focal plane tile 1 in order to pass the tile jackknife.
“In addition we found it necessary to remove BICEP3 data from focal plane tile 1 in order to pass the tile jackknife.”
Quote in the paperNot a substantial claim - Premisecitation§ 2. Likelihood Variation · p. 15
In BK15 simulations with no decorrelation, allowing ∆d to vary freely resulted in 72% of the r curves peaking at zero.
“in BK15 it was found that allowing ∆ d to vary freely resulted in 72% of the r curves peaking at zero in simulations where there was no decorrelation.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites BK15
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisecitation§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 3
Ref. [31] analyzed S-PASS and WMAP 23 GHz data and found β_s=-3.22±0.06 in the BICEP2 sky patch.
“and that Ref. [31] analyzed the S-PASS and WMAP 23GHz data and found β s = -3 . 22 ± 0 . 06 in the BICEP2 sky patch.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [31]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Study design and conductown data§ Appendix C: 95 & 220 GHz Spectral Stability · p. 10
There is no evidence for inconsistency between the BK15 and BK18 220 GHz spectra.
“The lower panel again shows no evidence for inconsistency between the two spectra.”
Quote in the paperNot a substantial claim - Interpretationown data§ Appendix D: Multi Frequency Spectra · p. 12
The parametric model, including the approximation of Gaussian fluctuation of the dust and synchrotron sky patterns, remains an adequate description of the presently available data.
“The parametric model which we are using, including the approximation of Gaussian fluctuation of the dust (and synchrotron) sky patterns, remains an adequate description of the presently available data.”
Quote in the paperSubstantial claim- The authors state this as an assumption: The dust and synchrotron sky patterns have Gaussian fluctuations.
- Study design and conductown data§ Appendix B: Internal Consistency Tests of New Data · p. 10
Evidence for failure of the season split jackknife when including November 2016 Keck Array data led the authors to exclude that data.
“However, we found evidence for failure of the season split jackknife when including this data which lead us to exclude it.”
Quote in the paperSubstantial claim - Study design and conductown data§ Appendix C: 95 & 220 GHz Spectral Stability · p. 10
The consistency test comparing differences of real bandpowers to simulations sharing common input skies is passed for the 95 GHz BK15 vs BK18 spectra.
“The lower part of the figure shows that this (not very stringent) test is passed.”
Quote in the paperNot a substantial claim - Study design and conductown data§ 4. Exploration of Alternate Foreground Models · p. 19
Decorrelated simulations generated according to the paper's parameterization of decorrelation give unbiased results when re-fit with that extension.
“We also make decorrelated simulations according to our parameterization of decorrelation, and these are thus also expected to give unbiased results when re-fit with that extension to the parameterization-as we see they do in the second line of the table.”
Quote in the paperNot a substantial claim - Interpretationreasoning§ 3. Bandpass Uncertainty · p. 22
The most important non-additive systematic effect is spectral bandpass uncertainty.
“Given the importance of multi-frequency component separation to the current result, the most important non-additive systematic effect is spectral bandpass uncertainty.”
Quote in the paperSubstantial claim - Study design and conductreasoning§ 4. Exploration of Alternate Foreground Models · p. 19
The basic set of Gaussian dust simulations generated according to the parametric model used when re-fitting gives unbiased results.
“Our basic set of simulations includes Gaussian realizations of dust generated according to the parametric model which we use when re-fitting, and these are thus expected and to give unbiased results-as we see they do in the first row of the table.”
Quote in the paperNot a substantial claim
- May combine two claims. 53
- Classified as probably not a substantial claim. 34
May combine two claims.
Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 1The maximum likelihood search on simulations gives σ(r)=0.009 for BK18, reduced from σ(r)=0.020 for BK15.
“Running maximum likelihood search on simulations we obtain unbiased results and find that σ ( r ) = 0 . 009.”
- Also stated in: § BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 5 · plain
“The distributions of maximum likelihood r values in simulations where the true value of r is zero gave σ ( r 0 . 05 ) = 0 . 020 for BK15 which is reduced to σ ( r 0 . 05 ) = 0 . 009 for BK18”
Quote in the paperNot a substantial claim- Also stated in: § BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 5 · plain
May combine two claims.
Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 4The BK18 data shrinks the contours in the vertical r direction while the BAO data shrinks the contours in the horizontal n_s direction and shifts the centroid slightly to the right.
“The BK18 data shrinks the contours in the vertical ( r ) direction while the BAO data shrinks the contours in the horizontal ( n s ) direction and shifts the centroid slightly to the right.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 1The Q/U maps reach depths of 2.8, 2.8, and 8.8 μK_cmb arcmin at 95, 150, and 220 GHz respectively over an effective area of ≈600 square degrees at 95 GHz and ≈400 square degrees at 150 and 220 GHz.
“The Q/U maps now reach depths of 2.8, 2.8 and 8.8 µ K cmb arcmin at 95, 150 and 220 GHz respectively over an effective area of ≈ 600 square degrees at 95 GHz and ≈ 400 square degrees at 150 & 220GHz.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 4The value of A_d is very similar when evaluated over the larger BICEP3 sky coverage region and the smaller BICEP2/Keck sky region.
“We also find that the value of A d is very similar when evaluated over the larger BICEP3 sky coverage region and the smaller BICEP2 / Keck sky region.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 2BK18 improves the constraint on the tensor-to-scalar ratio r by more than a factor of two over the previous result, to r_{0.05}<0.036 at 95% confidence.
“This improves the constraint on primordial gravitational waves parameterized by the tensor-to-scalar ratio r by more than a factor of two over our previous result to r 0 . 05 < 0 . 036 at 95% confidence, setting important additional limits on inflationary models.”
Quote in the paperSubstantial claimMay combine two claims.
Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 3In BK15 the constraint on β_d was prior dominated, but for BK18 the data is able to constrain this parameter almost as well as the prior previously did.
“In the BK15 analysis the constraint on β d was prior dominated, but for BK18 we see that the data is able to constrain this parameter almost as well as the prior previously did.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 3Compared to BK15, the likelihood curve for r tightens considerably with the peak position shifting down slightly, and the A_d curve tightens slightly.
“As compared to the previous BK15 analysis, the likelihood curve for r tightens considerably with the peak position shifting down slightly, and the A d curve tightens slightly.”
Quote in the paperSubstantial claimMay combine two claims.
Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 4Freeing the amplitude of the lensing power gives A_BB_L=1.03^{+0.08}_{-0.09}, and the r constraint hardly changes.
“Freeing the amplitude of the lensing power we obtain A BB L = 1 . 03 +0 . 08 -0 . 09 , and the r constraint hardly changes.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Findingcitation§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 3The peak value of β_d selected is very close to the mean value from Planck 2018 analysis of larger regions of sky, β_d=1.53.
“Interestingly the peak value selected is very close to the mean value from Planck 2018 analysis of larger regions of sky β d = 1 . 53 [24].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [24]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
Findingown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 3The A_sync curve now peaks at zero; the weak evidence for synchrotron seen in BK15 is no longer present.
“In addition the A sync curve now peaks at zero-the weak evidence for synchrotron we saw in BK15 is no longer present.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Findingnone given§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 4The 95 GHz B map is approximately equal parts lensed-ΛCDM signal and noise.
“The 95GHz B map is approximately equal parts lensed-ΛCDM signal and noise.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown data§ 2. Likelihood Variation · p. 18The increase of 1.5 in -2 log(L) for the real data when removing synchrotron is smaller than the average increase in simulations, indicating no evidence that synchrotron is present.
“The increase of 1.5 for the real data is smaller than the average increase in the simulations indicating no evidence that synchrotron is present.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown data§ 2. Likelihood Variation · p. 17With a uniform prior on A_BB_L and marginalizing over all other parameters, the BK18 data yield A_BB_L = 1.03 +0.08 -0.09, showing no tension with ΛCDM.
“With a uniform prior on A BB L (and marginalizing over all other parameters) we obtain A BB L = 1 . 03 +0 . 08 -0 . 09 showing no tension with ΛCDM.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown data§ 2. Likelihood Variation · p. 17The r constraint hardly changes when freeing the lensing amplitude because the lensing amplitude preferred by BK18 data is very close to that predicted by Planck 2018 cosmological parameters.
“The r constraint hardly changes due to the fact that the lensing amplitude prefered by the BK18 data is very close to that predicted by the Planck 2018 cosmological parameters.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown data§ 1. Likelihood Evolution · p. 15Switching to the updated Planck 2018 lensing spectrum shifts the r constraint slightly up, indicating a marginally relevant change at BK18 sensitivity levels.
“In Fig. 17 switching to the updated Planck 2018 spectrum corresponds to the transition from red to black-the r constraint shifts slightly up indicating that this is a marginally relevant change at BK18 sensitivity levels.”
Quote in the paperNot a substantial claim- The authors state this as an assumption: The power spectrum of the polarized dust emission in the BICEP/Keck field follows a power law.
Probably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
Findingreasoning§ Appendix A: Maps · p. 10BICEP3 maps a larger area of sky than BICEP2/Keck because BICEP3 has a larger instantaneous field of view.
“Due to the larger instantaneous field of view BICEP3 naturally maps a larger area of sky.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown data§ 2. Likelihood Variation · p. 18Removing synchrotron from the fit corresponds to a nominal reduction of 4 parameters, but the increase in mean -2 log(L) for simulations suggests only 2.5 effective free parameters.
“Removing synchrotron from the fit (i.e. fixing As = 0, β s = 0, α s = 0 and ϵ = 0) corresponds to a nominal reduction in the number of fit parameters of 4, but the increase in the mean -2 log( L ) for the simulations (which contain no synchrotron) suggests only 2.5 effective free parameters.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown data§ Appendix D: Multi Frequency Spectra · p. 12For the 594 bandpowers shown in Fig. 15, the maximum likelihood model gives χ2 = 541.6 with a PTE versus simulations of 0.94.
“For the 9 × 66 = 594 bandpowers shown in Fig. 15, χ 2 = ( d -m ) T C -1 ( d -m ) = 541 . 6, where d are the bandpower values, m are the model expectation values, and C is the bandpower covariance matrix for the maximum likelihood model. This has a PTE versus the simulations of 0 . 94.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown data§ 2. Likelihood Variation · p. 17Including EE spectra under the assumption that EE/BB ratios for dust and synchrotron are exactly 2 shifts the r peak position up, narrows the A_d curve, and makes the A_sync curve peak strongly away from zero.
“The effects are similar to those seen in BK15-the r peak position shifts up, the A d curve narrows, and the A sync curve peaks strongly away from zero.”
Quote in the paperNot a substantial claim- The authors state this as an assumption: The EE/BB ratios for dust and synchrotron are both exactly 2.
May combine two claims.
Findingreasoning§ Appendix B: Internal Consistency Tests of New Data · p. 10The χ2 and χ jackknife statistics do not have the nominal theory distributions because they are summations of bandpower values that are themselves χ2 rather than Gaussian distributed.
“The χ 2 and χ jackknife statistics do not actually have the nominal theory distributions since they are summations of bandpower values which are themselves χ 2 rather than Gaussian distributed.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Findingown data§ Appendix A: Maps · p. 10At 220 GHz, dust contamination becomes comparable in amplitude to the ΛCDM E-modes at the edges of the field.
“However, at 220 GHz we start to see dust contamination become comparable in amplitude to the ΛCDM E -modes at the edges of the field.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown data§ 2. Likelihood Variation · p. 17The peak position of A_d shifts only a very small amount under variations of sky coverage, showing no evidence for variation of the polarized dust amplitude as averaged across the BICEP3 coverage pattern versus the subset BICEP2/Keck field.
“Interestingly the peak position of A d only shifts a very small amount under these variations showing no evidence for variation of the polarized dust amplitude as averaged across the BICEP3 coverage pattern versus the subset BICEP2 / Keck fi eld.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown data§ 1. Likelihood Evolution · p. 15Dropping the β_d prior in the BK18 baseline analysis leaves r and A_sync nearly unchanged.
“In Fig. 17 dropping the β d prior corresponds to the transition from yellow to red curvesr and A sync show very little change while A d gets just slightly wider.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Findingown data§ 2. Likelihood Variation · p. 17The BICEP3 sky coverage is larger than the BICEP2/Keck region.
“As seen in Figures 8 and 9 the BICEP3 sky coverage is larger than the BICEP2 / Keck region.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Findingown data§ Appendix D: Multi Frequency Spectra · p. 12The sum of normalized deviations χ gives a PTE versus simulations of 0.22.
“If instead we take the sum of the normalized deviations χ = ∑ (( d -m ) /e ) where e is the square-root of the diagonal of C , we find that the PTE versus the simulations is 0.22.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown data§ 1. Likelihood Evolution · p. 15Residual uncertainty in the Planck 2018 cosmological parameters leads to a residual uncertainty in the predicted ΛCDM lensing BB spectrum of 2.2% within 20 < l < 500, with a distribution close to Gaussian.
“In a simple study we find this to be 2.2% within the multipole range 20 < ℓ < 500 (with a distribution close to Gaussian).”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Findingown data§ Appendix C: 95 & 220 GHz Spectral Stability · p. 10The BK18 220 GHz spectrum is sample variance limited out to l ∼ 200.
“The upper part of Fig. 14 compares the two BB spectra-a large improvement in sensitivity is again clear, and the BK18 220 GHz spectrum is sample variance limited out to ℓ ∼ 200.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingreasoning§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 4The E maps are dominated by ΛCDM signal and are highly correlated across all three bands.
“The E maps are dominated by ΛCDM signal, and hence are highly correlated across all three bands.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Findingreasoning§ Appendix A: Maps · p. 10In the T maps, the patterns at 95, 150, and 220 GHz are almost identical because the ΛCDM signal is dominant.
“Comparing the three frequencies we see almost identical patterns in the T maps since ΛCDM signal is dominant.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown data§ 2. Likelihood Variation · p. 17Dropping WMAP results in A_sync peaking strongly at zero, whereas dropping LFI results in A_sync peaking well above zero.
“Dropping WMAP results in A sync peaking strongly at zero whereas dropping LFI results in A sync peaking well above zero.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Findingnone given§ 2. Likelihood Variation · p. 17For the small field only version, the A_sync peak shifts above zero as it was in BK15.
“Note that for the small field only version the A sync peak shifts above zero as it was in BK15.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
Findingown data§ Appendix A: Maps · p. 10In the Q and U maps, the patterns at 95 and 150 GHz are extremely similar and dominated by the ΛCDM E-mode signal.
“For Q and U the patterns are again extremely similar between 95 and 150 GHz, and dominated by the ΛCDM E -mode signal.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown data§ 2. Likelihood Variation · p. 17BICEP/Keck alone constrains A_sync and β_d poorly, with the r constraint peaking hard at zero.
“BICEP/ Keck alone (blue) constrains A sync and β d poorly with the r constraint peaking hard at zero.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Findingown data§ 2. Likelihood Variation · p. 18The absolute goodness-of-fit of the baseline model to the data is adequate.
“In Appendix D above we saw that the absolute goodness-of-fit of the baseline model to the data is adequate.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown data§ 1. Likelihood Evolution · p. 14Switching from BK15 to BK18 data makes a substantial difference: the r constraint narrows and its peak position shifts down.
“We next switch from the BK15 data set to the BK18 one-i.e. including the improved sensitivity at 220 GHz and the improved sensitivity and sky area at 95 GHz (magenta to yellow). This makes a substantial difference: the r constraint narrows and its peak position shifts down.”
Quote in the paperSubstantial claim- The authors state this as an assumption: The power spectrum of the polarized dust emission in the BICEP/Keck field follows a power law.
Probably not a substantial claim: may not pass S3 (load-bearing).
Findingown data§ 1. Likelihood Evolution · p. 14Updating COSMOMC from Nov2016 to July2019 makes very little difference to the r constraint.
“Starting with the BK15 data set we first update the version of COSMOMC from Nov2016 to July2019 (green to magenta) which makes very little difference.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Findingown data§ Appendix D: Multi Frequency Spectra · p. 11The penalty from using different apodizations in reducing correlations of auto- and cross-spectra is negligible in the current case.
“Using different apodizations also in principle reduces the correlations of the auto- and cross-spectra which are key to the separation of foreground and CMB signals. However, in the current case the penalty turns out to be negligible.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Findingcitation§ 1. Likelihood Evolution · p. 15The peak value of β_d = 1.50 selected by the data is close to the mean value from Planck 2018 analysis of larger regions of sky β_d^P = 1.53 ± 0.02.
“Interestingly the peak value of β d = 1 . 50 selected by our data is close to the mean value from Planck 2018 analysis of larger regions of sky β P d = 1 . 53 ± 0 . 02 [24].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [24]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
Findingnone given§ Appendix B: Internal Consistency Tests of New Data · p. 10The two nominally 220 GHz receivers added before the 2015 season have passbands centered at ≈230 GHz, while the two added before the 2016 season have passbands centered at ≈220 GHz.
“The two nominally 220 GHz receivers added before the 2015 season actually have passbands centered at ≈ 230 GHz, whereas the two added before the 2016 season have passbands centered at ≈ 220 GHz.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown data§ 2. Likelihood Variation · p. 15Allowing the dust decorrelation parameter ∆d to vary freely shifts the r constraint down slightly and the A_sync constraint up slightly.
“We see that the r constraint shifts down slightly and the A sync constraint shifts up slightly.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown data§ 2. Likelihood Variation · p. 18Allowing decorrelation parameter ∆d to vary freely while fixing ε=0 leaves the nominal number of parameters unchanged and hardly changes the mean value of -2 log(L) for the simulations.
“Allowing decorrelation parameter ∆ d to vary freely while fixing ϵ = 0 leaves the nominal number of parameters unchanged and as expected hardly changes the mean value of -2 log( L ) for the simulations.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown data§ 2. Likelihood Variation · p. 17Dropping the 150 and 220 GHz bands does not substantially increase the width of the r constraint, but it does increase the widths of the A_d and β_d constraints.
“It is very interesting that dropping the 150 and 220 GHz bands does not substantially increase the width of the r constraint, although it is unsurprising that it does increase the widths of the A d and β d constraints.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown data§ Appendix D: Multi Frequency Spectra · p. 13Synchrotron is tightly limited in all multipole ranges and not detected in any of them.
“Synchrotron is tightly limited in all the multipole ranges, and not detected in any of them.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Findingown data§ 2. Likelihood Variation · p. 17Dropping the other HFI bands makes smaller additional changes.
“Dropping the other HFI bands makes smaller additional changes (red to green).”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown data§ 3. Bandpass Uncertainty · p. 22The shifts on dust parameters (A_d and β_d) due to bandpass nuisance parameters are a few percent, and still within statistical uncertainty and upper bounds predicted using maximum likelihood searches on simulations.
“The shifts on dust parameters ( A d and β d ) are a few percent, and still within statistical uncertainty and upper bounds predicted using maximum likelihood searches on simulations.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown data§ 3. Likelihood Validation · p. 1960% of the lensed-ΛCDM+dust+noise simulations peak at zero, and 11% have a lower zero-to-peak ratio than the real data, i.e. show more evidence for r when the true value is zero.
“We find that 60% of the simulations peak at zero, and 11% have a lower zero-to-peak ratio than the real data-i.e. show more evidence for r when the true value is in fact zero.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown data§ 4. Exploration of Alternate Foreground Models · p. 20The PySM models 1, 2 and 3 have A_d in the BICEP/Keck sky region much greater than the actual level and modestly increase σ(r), by an amount fractionally less than the increase seen in BK15.
“They have A d in our sky region which is much greater that the actual level and this modestly increases σ ( r ), although interestingly by an amount that is fractionally less than the increase seen in BK15.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown data§ 4. Exploration of Alternate Foreground Models · p. 20Neither the MKD nor the Vansyngel model produces detectable bias on r.
“Neither of these models produces detectable bias on r .”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Findingcitation§ 1. Temperature-to-Polarization Leakage from Residual Beam Mismatch · p. 21The Keck 95 GHz, 150 GHz and 220 GHz beam map simulation spectra were found to be very similar to the BK15 results.
“The corresponding spectra for the Keck 95 GHz, 150 GHz and 220 GHz bands were found to be very similar to the BK15 results shown in Ref. [52].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [52]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
Findingown data§ 2. Likelihood Variation · p. 18The real data shows an increase almost exactly equal to that in the mean of simulations, i.e. the data is perfectly compatible with the lensed-ΛCDM expectation plus the simple 3 parameter dust model.
“The real data shows an increase almost exactly equal to that in the mean of simulations-i.e. the data is perfectly compatible with the lensed-ΛCDM expectation plus the simple 3 parameter dust model.”
Quote in the paperSubstantial claimMay combine two claims.
Findingown data§ 3. Likelihood Validation · p. 19In maximum likelihood validation on standard lensed-ΛCDM+dust+noise simulations, the input values are recovered in the mean, although there is a small detectable bias on A_d.
“The input values are recovered in the mean although formally there is a small bias detectable on A d .”
Quote in the paperNot a substantial claimMay combine two claims.
Findingcitation§ 2. Other Additive Systematics Effects · p. 22Uncertainties from polarized point source flux may yield an upward bias on r of 1-3 × 10^-3, and imperfections in noise bias estimates may yield a downward bias on r of 2 × 10^-3.
“More significant, but still subdominant for the current analysis, are uncertainties from the contributions of polarized flux from point sources in our field, which estimates suggest may yield an upward bias on r of 1-3 × 10 -3 [9, 64, and recent internal work], and imperfections in our noise bias estimates as they interact with leakage deprojection filtering, which recent preliminary work suggests”
Quote in the paperNot a substantial claim0 of 2 sources checked- cites [9]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites [64]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
Findingown data§ 1. Temperature-to-Polarization Leakage from Residual Beam Mismatch · p. 21The recovered bias on r from T→P leakage is ∆(r) = 1.5 ± 1.1 × 10^-3, which is subdominant compared to the statistical uncertainty σ(r) = 0.009.
“The recovered bias is ∆( r ) = 1 . 5 ± 1 . 1 × 10 -3 , which is subdominant compared to our statistical uncertainty σ ( r ) = 0 . 009.”
Quote in the paperSubstantial claimClassified as probably not a substantial claim.
Premisecitation§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 2A joint analysis using multifrequency data from Planck showed that most or all of the excess is due to polarized emission from dust in our own galaxy.
“In a joint analysis using multifrequency data from the Planck experiment it was shown that most or all of this is due to polarized emission from dust in our own galaxy [10, hereafter BKP].”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [10]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Classified as probably not a substantial claim.
Study design and conductcitation§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 4As part of standard data reduction, leading order temperature-to-polarization leakage is deprojected.
“As part of our standard data reduction we 'deproject' leading order temperature to polarization leakage [9, 34]-in Appendix F we quantify possible residual leakage and some other possible systematics.”
Quote in the paperSubstantial claim0 of 2 sources checked- cites [9]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites [34]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S3 (load-bearing).
Premisecitation§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 2The BICEP/Keck program first reported detection of an excess over the lensing B-mode expectation at 150 GHz.
“Our BICEP/ Keck program first reported detection of an excess over the lensing B -mode expectation at 150 GHz in Ref. [9].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [9]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
Premisecitation§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 2Under ΛCDM, the CMB polarization pattern is mostly E-mode, with a much smaller B-mode component arising from gravitational lensing of CMB photons after last scattering.
“Under the ΛCDM standard model the CMB polarization pattern is mostly E -mode, with a much smaller B -mode component which arises due to gravitational deflections (lensing) of the CMB photons after their last scattering [5].”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [5]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
Study design and conductcitation§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 3The EE spectra were not used to derive the model but agree well with it under the assumption that EE/BB = 2 for dust.
“The EE spectra were not used to derive the model but agree well with it under the assumption that EE/BB = 2 for dust, as is known to be close to the case [23, 24].”
Quote in the paperNot a substantial claim0 of 2 sources checked- cites [23]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites [24]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- The authors state this as an assumption: For dust, EE/BB = 2.
Probably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
Premisecitation§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 2At the South Pole the atmosphere is exceptionally transparent and stable at the observation frequencies.
“At the South Pole the atmosphere is exceptionally transparent and stable at the observation frequencies [17, Fig. 5].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [17, Fig. 5]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S3 (load-bearing).
Study design and conductown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 3Jackknife internal consistency null tests were carried out on the new 95 GHz and 220 GHz data.
“To test for systematic contamination we carry out our usual 'jackknife' internal consistency (null) tests on the new 95GHz and 220GHz data as described in Appendices B and C.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Premisecitation§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 3Planck analysis consistently finds approximate power law behavior of both the EE and BB dust spectra with exponents ≈ -0.4.
“Planck analysis consistently finds approximate power law behavior of both the EE and BB dust spectra with exponents ≈ -0 . 4 [23, 24].”
Quote in the paperNot a substantial claim0 of 2 sources checked- cites [23]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites [24]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
Premisecitation§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 2Since primordial gravitational waves produce E-modes and B-modes approximately equally, the best way to search for them is to look for an excess B-mode signal.
“Since primordial gravitational waves will produce E -modes and B -modes approximately equally it was realized in the late 1990's that the best way to search for them is to look for an excess B -mode signal [6-8].”
Quote in the paperSubstantial claim0 of 3 sources checked- cites [6]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites [7]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites [8]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
Premisecitation§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 3Using S-PASS data, the expectation is A_{sync,23}≈0.4 μK^2 in the BICEP/Keck field, consistent with the A_sync likelihood curve.
“(Using the S-PASS data [30] we estimate that the expectation is A sync , 23 ≈ 0 . 4 µ K 2 in the BICEP/ Keck fi eld, which is consistent with our A sync likelihood curve.)”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [30]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
Interpretationown data§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 4The φ^{2/3} model now lies outside the 95% contour, as does the band of natural inflation models.
“The φ 2 / 3 model now lies outside the 95% contour as does the band of natural inflation models.”
Quote in the paperSubstantial claimMay combine two claims.
Premisecitation§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 2If we can detect or set limits on primordial gravitational waves, we can set limits on inflationary models and probe physics at energy scales far higher than laboratory experiments.
“If we can detect or set limits on primordial gravitational waves we can set limits on these models [4], and probe physics at energy scales far higher than can ever be accessed in laboratory experiments.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [4]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S3 (load-bearing).
Premisecitation§ 2. Likelihood Variation · p. 17The Planck 2018 TT,TE,EE+lowE result is A_L = 1.18 ± 0.065.
“This is an interesting result given the Planck 2018 TT,TE,EE+lowE result A L = 1 . 18 ± 0 . 065 [2, Eqn. 36b].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [2]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
Interpretationown data§ 2. Likelihood Variation · p. 17There is very little degeneracy between r and A_BB_L, implying that all one needs from ΛCDM is the template shape of the lensing B-mode spectrum, not the amplitude.
“In addition in the right panel of Fig. 19 we see that there is very little degeneracy between r and A BB L implying that all one now needs from ΛCDM is the template shape of the lensing B -mode spectrum, and not the amplitude.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Study design and conductnone given§ Appendix B: Internal Consistency Tests of New Data · p. 10The authors did not look at the non-jackknife spectra until the data removals had been done and the null tests determined to be satisfactory.
“We note that we did not look at the non-jackknife spectra until the above data removals had been done and the null tests determined to be satisfactory.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Premisecitation§ 2. Likelihood Variation · p. 15Ref. [55] reported evidence for line-of-sight decorrelation in Planck data by using HI data to select sight lines which integrate over multiple dust clouds.
“Recently Ref. [55] reported evidence for line-of-sight decorrelation in Planck data by using HI data to select sight lines which integrate over multiple dust clouds.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [55]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S3 (load-bearing).
Study design and conductreasoning§ Appendix D: Multi Frequency Spectra · p. 12The other Planck bands were dropped because they provide a negligible amount of additional information.
“To keep down the total number of spectra we drop the other Planck bands since these provide a negligible amount of additional information.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
Premisecitation§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 3Analysis of 2.3 GHz data from S-PASS in conjunction with WMAP and Planck finds β_s=-3.2 with no detected trends with galactic latitude or angular scale.
“We note that analysis of 2.3 GHz data from S-PASS in conjunction with WMAP and Planck fi nds β s = -3 . 2 with no detected trends with galactic latitude or angular scale [30]”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [30]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
Study design and conductcitation§ Appendix D: Multi Frequency Spectra · p. 11Using different apodizations suppresses the amplitude of cross-spectra relative to auto-spectra, but this is automatically taken into account in the bandpower window function calculations.
“Using different apodizations suppresses the amplitude of the cross-spectra as compared to the auto-spectra but this is automatically taken into account in the bandpower window function calculations [18, 53].”
Quote in the paperNot a substantial claim0 of 2 sources checked- cites [18]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites [53]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Classified as probably not a substantial claim.
Premisecitation§ 2. Likelihood Variation · p. 15In the BICEP/Keck region, one cloud dominates the column density in the majority of pixels.
“This study uses maps of the effective number of clouds taken from Ref. [56] which in Sec. 4.2 specifically examines the BICEP/ Keck patch and states that 'one cloud dominates the column density in the majority of pixels in the BICEP/ Keck region'.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [56]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S3 (load-bearing).
Study design and conductcitation§ Appendix B: Internal Consistency Tests of New Data · p. 10The jackknife tests of the new 2016, 2017, and 2018 data are the same as those performed on the previous BICEP/Keck data.
“In this section we perform tests of the new 2016, 2017 and 2018 data which are the same as those performed on the previous BICEP/ Keck data in Sec. VII.C of Ref. [9], Sec. 6.3 of Ref. [14], Appendix B of BK14, and Appendix B of BK15.”
Quote in the paperNot a substantial claim0 of 2 sources checked- cites [9]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites [14]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
Study design and conductown data§ 2. Likelihood Variation · p. 17Running maximum likelihood searches on simulations indicates that apodizing each map with its natural inverse variance coverage pattern results in σ(r) as low as any other option with no detectable bias on r.
“Running maximum likelihood searches on simulations indicates that this results in σ ( r ) as low as any other option with no detectable bias on r .”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Premisecitation§ BICEP / Keck XIII: Improved Constraints on Primordial Gravitational Waves using Planck , WMAP, and BICEP/ Keck Observations through the 2018 Observing Season · p. 3Ref. [30] finds a value at the bottom end of the range (≈ -1) from S-PASS data for BB at high galactic latitude.
“Ref. [30] finds a value at the bottom end of this range ( ≈ -1) from the S-PASS data for BB at high galactic latitude.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [30]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
Study design and conductown data§ Appendix F: Systematics · p. 21For all systematics effects considered, the magnitude of the estimated bias on r is significantly smaller than the statistical uncertainty, and not all biases have the same sign, which should lead to partial cancellation.
“For all effects considered, the magnitude of the estimated bias on r is significantly smaller than our statistical uncertainty, and not all of the biases have the same sign, which should lead to partial cancelation.”
Quote in the paperSubstantial claimClassified as probably not a substantial claim.
Study design and conductown data§ 1. Temperature-to-Polarization Leakage from Residual Beam Mismatch · p. 21In the BK18 leakage analysis, care was taken to minimize systematic contamination in the composite beam maps from the FFBM analysis pipeline itself.
“In this leakage analysis for BK18, care was taken to minimize systematic contamination in the composite beam maps from the FFBM analysis pipeline itself, e.g. by minimizing non-Gaussian noise and excess smoothing.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Interpretationreasoning§ 4. Exploration of Alternate Foreground Models · p. 19Variation of dust amplitude across the field can potentially produce bias on r given that the re-fit model assumes a single A_d value applies to both the smaller BICEP2/Keck field and the larger BICEP3 field.
“Such variation of the dust amplitude across the field can potentially produce bias on r given that our re-fit model assumes a single A d value applies to both the smaller BICEP2 / Keck fi eld and the larger BICEP3 fi eld.”
Quote in the paperNot a substantial claim- The authors state this as an assumption: The re-fit model assumes a single A_d value applies to both the smaller BICEP2/Keck field and the larger BICEP3 field.
May combine two claims.
Premisecitation§ 2. Other Additive Systematics Effects · p. 22Other additive systematic effects (EMI, magnetic, thermal, scan-synchronous sources, ghost beams) were studied in Ref. [34] and upper limits placed on their contributions equivalent to r < 10^-4, except EMI from the satellite uplink bounded at r < 1.7 × 10^-3 with 95% confidence.
“Other additive systematic effects including EMI, magnetic, thermal, and other scan-synchronous sources of residual contamination, and ghost beams, were studied in Ref. [34] and upper limits placed on their contributions equivalent to r < 10 -4 , except in the case of EMI contamination from the satellite uplink transmitter, which was bounded at r < 1 . 7 × 10 -3 with 95% confidence.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [34]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
Interpretationown data§ 1. Temperature-to-Polarization Leakage from Residual Beam Mismatch · p. 21The driving factor in the improvement in recovered T→P bias is the inclusion of BICEP3, which demonstrates lower differential beam power than Keck and BICEP2, both before and after deprojection.
“The driving factor in this improvement in the recovered bias is the inclusion of BICEP3 , which demonstrates lower differential beam power than Keck and BICEP2 , both before and after deprojection.”
Quote in the paperSubstantial claimMay combine two claims.
Study design and conductown data§ 2. Other Additive Systematics Effects · p. 22Levels of potential contamination from other additive systematic effects have been monitored throughout collection of the current dataset, and contributions from these effects remain negligible.
“Levels of these potential sources of contamination have been monitored throughout collection of the current dataset (including EMI reduction from additional shielding at the satellite uplink), and contributions from these effects remain negligible.”
Quote in the paperSubstantial claim
The authors state this as an assumption.
For dust, EE/BB = 2.
“under the assumption that EE/BB = 2 for dust, as is known to be close to the case [23, 24]”
“under the assumption that EE/BB = 2 for dust”
The authors state this as an assumption.
The synchrotron frequency spectrum is a simple power law A_sync ∝ ν^β_s.
“assuming a simple power law for the frequency spectral behavior A sync ∝ ν β s”
The authors state this as an assumption.
The dust spatial power spectrum is a power law D_ℓ ∝ ℓ^α_d.
“The spatial power spectrum is taken as a power law D ℓ ∝ ℓ α d marginalizing uniformly over the (generous) range -1 < α d < 0”
The authors state this as an assumption.
The synchrotron spatial power spectrum is a power law D_ℓ ∝ ℓ^α_s.
“The spatial power spectrum is taken as a power law D ℓ ∝ ℓ α s marginalizing over the range -1 < α s < 0 [32].”
The authors state this as an assumption.
The power spectrum of the polarized dust emission in the BICEP/Keck field follows a power law.
“We note that this figure offers empirical backing for an assumption which we make in our mainline analysis: that the power spectrum of the polarized dust emission in our field follows a power law.”
The authors state this as an assumption.
The dust and synchrotron sky patterns have Gaussian fluctuations.
“The parametric model which we are using, including the approximation of Gaussian fluctuation of the dust (and synchrotron) sky patterns, remains an adequate description of the presently available data.”
The paper relies on this without support.
Dust decorrelation exists in the BICEP/Keck sky patch at some level.
“Nonetheless, decorrelation surely exists in our sky patch at some level-the question is whether it is relevant as compared to the BK18 experimental noise.”
The authors state this as an assumption.
The EE/BB ratios for dust and synchrotron are both exactly 2.
“under the artificial assumption that the EE/BB ratios for dust and synchrotron are both exactly 2”
The authors state this as an assumption.
The re-fit model assumes a single A_d value applies to both the smaller BICEP2/Keck field and the larger BICEP3 field.
“given that our re-fit model assumes a single A d value applies to both the smaller BICEP2 / Keck fi eld and the larger BICEP3 fi eld.”
The paper relies on this without support.
When running on simulations generated according to the model being re-fit, the input parameter values should be recovered in the mean.
“we then have an a priori expectation that the input parameter values should be recovered in the mean.”
The paper relies on this without support.
The Planck 2018 cosmological parameters predict a specific lensing BB spectrum as used in the BK18 baseline analysis.
“The Planck 2018 cosmological parameters predict a specific lensing BB spectrum as used in the 'BK18 baseline' analysis described above.”
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BICEP2. II. EXPERIMENT AND THREE-YEAR DATA SET
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Self-citationAdam, R., Ade, P. A. R., Aghanim, N., Arnaud, M., Aumont, J., Baccigalupi, C., Banday, A. J., Barreiro, R. B., Bartlett, J. G., Bartolo, N., et al. (2015) · Astronomy and Astrophysics · doi:10.1051/0004-6361/201425034 · Cited by 219 · see citing works
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Self-citationDegree Angular Scale Interferometer 3 Year Cosmic Microwave Background Polarization Results
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Self-citationPlanck constraints on the tensor-to-scalar ratio
Tristram, M., Banday, A. J., Gorski, K. M., Keskitalo, R., Lawrence, C. R., Andersen, K. J., Barreiro, R. B., Borrill, J., Eriksen, H. K., Fernández-Cobos, R., et al. (2021) · Astronomy and Astrophysics · doi:10.1051/0004-6361/202039585 · Cited by 164 · see citing works
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Self-citationImplications of the Cosmic Background Imager Polarization Data
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Self-citationANTENNA-COUPLED TES BOLOMETERS USED IN BICEP2,Keck Array, AND SPIDER
Ade, P. A. R., Aikin, R. W., Amiri, M., et al. (2015) · The Astrophysical Journal · doi:10.1088/0004-637x/812/2/176 · Cited by 94 · see citing works
Self-citationBICEP Array: a multi-frequency degree-scale CMB polarimeter
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Self-citationSayre, J. T., Reichardt, C. L., Henning, J. W., Ade, P. A. R., Anderson, A. J., Austermann, J. E., Avva, J. S., Beall, J. A., Bender, A. N., Benson, B. A., et al. (2020) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.101.122003 · Cited by 92 · see citing works
Self-citationS–PASS view of polarized Galactic synchrotron at 2.3 GHz as a contaminant to CMB observations
Krachmalnicoff, N., Carretti, E., Baccigalupi, C., Bernardi, G., Brown, S., Gaensler, B., Haverkorn, M., Kesteven, M., Perrotta, F., Poppi, S., et al. (2018) · Astronomy & Astrophysics · doi:10.1051/0004-6361/201832768 · Cited by 86 · see citing works
Prospects for polarized foreground removal
Dunkley, J., Amblard, A., Baccigalupi, C., et al. (2009) · AIP conference proceedings · doi:10.1063/1.3160888 · Cited by 83 · see citing works
New Measurements of Fine‐Scale CMB Polarization Power Spectra from CAPMAP at Both 40 and 90 GHz
Bischoff, C. A., Hyatt, L., McMahon, J. J., Nixon, G. W., Samtleben, D. F. E., Smith, K. M., Vanderlinde, K., Barkats, D., Farese, P. C., Gaier, T., et al. (2008) · The Astrophysical Journal · doi:10.1086/590487 · Cited by 78 · see citing works
Self-citationThe structure and statistics of interstellar turbulence
Kritsuk, A. G., Ustyugov, S. D., & Norman, M. L. (2017) · New Journal of Physics · doi:10.1088/1367-2630/aa7156 · Cited by 78 · see citing works
A Measurement of the Degree-scale CMB B-mode Angular Power Spectrum with Polarbear
Adachi, S., Faúndez, M. A. O. A., Arnold, K., Baccigalupi, C., Barron, D. R., Beck, D., Beckman, S., Bianchini, F., Boettger, D., Borrill, J., et al. (2020) · The Astrophysical Journal · doi:10.3847/1538-4357/ab8f24 · Cited by 71 · see citing works
Self-citationDEGREE-SCALE COSMIC MICROWAVE BACKGROUND POLARIZATION MEASUREMENTS FROM THREE YEARS OF BICEP1 DATA
Barkats, D., Aikin, R. W., Bischoff, C. A., et al. (2014) · The Astrophysical Journal · doi:10.1088/0004-637x/783/2/67 · Cited by 66 · see citing works
Self-citationBicep2. III. INSTRUMENTAL SYSTEMATICS
Ade, P. A. R., Aikin, R. W., Barkats, D., et al. (2015) · The Astrophysical Journal · doi:10.1088/0004-637x/814/2/110 · Cited by 63 · see citing works
Self-citationAghanim, N., Ashdown, M., Aumont, J., et al. (2016) · Astronomy and Astrophysics · doi:10.1051/0004-6361/201629164 · Cited by 63 · see citing works
SPATIAL VARIATIONS IN THE SPECTRAL INDEX OF POLARIZED SYNCHROTRON EMISSION IN THE 9 yr WMAP SKY MAPS
Fuskeland, U., Wehus, I., Eriksen, H., & Naess, S. (2014) · The Astrophysical Journal · doi:10.1088/0004-637x/790/2/104 · Cited by 61 · see citing works
Assessments of Ali, Dome A, and Summit Camp for mm-wave Observations Using MERRA-2 Reanalysis
Kuo, C.-L. L. (2017) · The Astrophysical Journal · doi:10.3847/1538-4357/aa8b74 · Cited by 61 · see citing works
Self-citationPolarized galactic synchrotron and dust emission and their correlation
Choi, S. K., & Page, L. A. (2015) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2015/12/020 · Cited by 59 · see citing works
Statistical simulations of the dust foreground to cosmic microwave background polarization
Vansyngel, F., Boulanger, F., Ghosh, T., Wandelt, B. D., Aumont, J., Bracco, A., Levrier, F., Martin, P. G., & Montier, L. (2017) · Astronomy and Astrophysics · doi:10.1051/0004-6361/201629992 · Cited by 57 · see citing works
Results from the Atacama B-mode Search (ABS) experiment
Kusaka, A., Appel, J. W., Essinger-Hileman, T., Beall, J. A., Campusano, L. E., Cho, H.-M., Choi, S. K., Crowley, K., Fowler, J. W., Gallardo, P., et al. (2018) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2018/09/005 · Cited by 56 · see citing works
Self-citationEvidence for line-of-sight frequency decorrelation of polarized dust emission in Planck data
Pelgrims, V., Clark, S. E., Hensley, B. S., Panopoulou, G. V., Pavlidou, V., Tassis, K., Eriksen, H. K., & Wehus, I. K. (2021) · Astronomy and Astrophysics · doi:10.1051/0004-6361/202040218 · Cited by 55 · see citing works
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Self-citationBattye, R. A., Browne, I. W. A., Peel, M., et al. (2011) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2010.18115.x · Cited by 50 · see citing works
Receiver development for BICEP Array, a next-generation CMB polarimeter at the South Pole
Moncelsi, L., Ade, P. A. R., Ahmed, Z., Amiri, M., Barkats, D., Thakur, R. B., Bischoff, C. A., Bock, J. J., Buza, V., Cheshire, J. R., et al. (2020) · Millimeter, Submillimeter, and Far-Infrared Detectors and Instrumentation for Astronomy XI · doi:10.1117/12.2561995 · Cited by 48 · see citing works
Self-citationDust-Polarization Maps for Local Interstellar Turbulence
Kritsuk, A. G., Flauger, R., & Ustyugov, S. D. (2018) · Physical Review Letters · doi:10.1103/physrevlett.121.021104 · Cited by 47 · see citing works
A 3D model of polarized dust emission in the Milky Way
Martínez-Solaeche, G., Karakci, A., & Delabrouille, J. (2018) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sty204 · Cited by 46 · see citing works
A demonstration of improved constraints on primordial gravitational waves with delensing
Ade, P. A. R., Ahmed, Z., Amiri, M., Anderson, A. J., Austermann, J. E., Avva, J. S., Barkats, D., Thakur, R. B., Beall, J. A., Bender, A. N., et al. (2021) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.103.022004 · Cited by 43 · see citing works
Self-citationBICEP2/KECK ARRAY. VII. MATRIX BASED E/B SEPARATION APPLIED TO BICEP2 AND THE KECK ARRAY
Ade, P. A. R., Ahmed, Z., Aikin, R. W., et al. (2016) · The Astrophysical Journal · doi:10.3847/0004-637x/825/1/66 · Cited by 25 · see citing works
Self-citationMaps of the Number of H i Clouds along the Line of Sight at High Galactic Latitude
Panopoulou, G. V., & Lenz, D. (2020) · The Astrophysical Journal · doi:10.3847/1538-4357/abb6f5 · Cited by 24 · see citing works
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Self-citationFuskeland, U., Andersen, K. J., Aurlien, R., et al. (2020) · Astronomy and Astrophysics · doi:10.1051/0004-6361/202037629 · Cited by 22 · see citing works
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Probing cosmic inflation with the LiteBIRD cosmic microwave background polarization survey
Allys, E., Arnold, K., Aumont, J., Aurlien, R., Azzoni, S., Baccigalupi, C., Banday, A. J., Banerji, R., Barreiro, R. B., Bartolo, N., et al. (2022) · Progress of Theoretical and Experimental Physics · doi:10.1093/ptep/ptac150 · Cited by 374 · see citing works
Self-citationCosmology with the Laser Interferometer Space Antenna
Auclair, P., Bacon, D., Baker, T., Barreiro, T., Bartolo, N., Belgacem, E., Bellomo, N., Ben-Dayan, I., Bertacca, D., Besançon, M., et al. (2023) · Living Reviews in Relativity · doi:10.1007/s41114-023-00045-2 · Cited by 342 · see citing works
Valentino, E. D., Said, J. L., Riess, A. G., Pollo, A., Poulin, V., Gómez-Valent, A., Weltman, A., Palmese, A., Huang, C. D., van de Bruck, C., et al. (2025) · Physics of the Dark Universe · doi:10.1016/j.dark.2025.101965 · Cited by 366 · see citing works
Self-citationImproved limits on the tensor-to-scalar ratio using BICEP and P l a n c k data
Tristram, M., Banday, A. J., Gorski, K. M., Keskitalo, R., Lawrence, C. R., Andersen, K. J., Barreiro, R. B., Borrill, J., Colombo, L. P. L., Eriksen, H. K., et al. (2022) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.105.083524 · Cited by 266 · see citing works
The Atacama Cosmology Telescope: DR6 power spectra, likelihoods and ΛCDM parameters
Louis, T., Posta, A. L., Atkins, Z., Jense, H. T., Abril-Cabezas, I., Addison, G. E., Ade, P. A. R., Aiola, S., Alford, T., Alonso, D., et al. (2025) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2025/11/062 · Cited by 239 · see citing works
Self-citationCosmological parameters derived from the final Planck data release (PR4)
Tristram, M., Banday, A. J., Douspis, M., Garrido, X., Gorski, K. M., Versillé, S., Hergt, L. T., Ilić, S., Keskitalo, R., Lagache, G., et al. (2023) · Astronomy and Astrophysics · doi:10.1051/0004-6361/202348015 · Cited by 217 · see citing works
The Atacama Cosmology Telescope: DR6 constraints on extended cosmological models
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Self-citationVagnozzi, S. (2023) · Journal of High Energy Astrophysics · doi:10.1016/j.jheap.2023.07.001 · Cited by 175 · see citing works
New physics from the polarized light of the cosmic microwave background
Komatsu, E. (2022) · Nature Reviews Physics · doi:10.1038/s42254-022-00452-4 · Cited by 164 · see citing works
“C ` = cos 2(2β )CEE ` + sin 2(2β )CBB ` , (21)”
Cosmic Birefringence from thePlanckData Release 4
Diego-Palazuelos, P., Eskilt, J. R., Minami, Y., Tristram, M., Sullivan, R. M., Banday, A. J., Barreiro, R. B., Eriksen, H. K., Gorski, K. M., Keskitalo, R., et al. (2022) · Physical Review Letters · doi:10.1103/physrevlett.128.091302 · Cited by 157 · see citing works
Harlow, D., Heidenreich, B., Matthew Reece, B., & Rudelius, T. (2023) · Reviews of Modern Physics · doi:10.1103/revmodphys.95.035003 · Cited by 156 · see citing works
String cosmology: From the early universe to today
Cicoli, M., Conlon, J. P., Maharana, A., Parameswaran, S., Quevedo, F., & Ivonne Zavala, C. (2024) · Physics Reports · doi:10.1016/j.physrep.2024.01.002 · Cited by 172 · see citing works
Eskilt, J. R., & Komatsu, E. (2022) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.106.063503 · Cited by 132 · see citing works
The Science of the Einstein Telescope
Abac, A., Abramo, L. R., Albanesi, S., Albertini, A., Agapito, A., Agathos, M., Albertus, C., Andersson, N., Andrade, T., Andreoni, I., et al. (2026) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2026/03/081 · Cited by 172 · see citing works
Cosmological Background Interpretation of Pulsar Timing Array Data
Figueroa, D. G., Pieroni, M., Ricciardone, A., et al. (2024) · Physical Review Letters · doi:10.1103/physrevlett.132.171002 · Cited by 116 · see citing works
Anatomy of single-field inflationary models for primordial black holes
Καράμ, Α., Koivunen, N., Tomberg, E., Vaskonen, V., & Veermäe, H. (2023) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2023/03/013 · Cited by 112 · see citing works
Cosmological gravitational particle production and its implications for cosmological relics
Kolb, E. W., & Long, A. J. (2024) · Reviews of Modern Physics · doi:10.1103/revmodphys.96.045005 · Cited by 106 · see citing works
Camphuis, E., Quan, W., Balkenhol, L., Khalife, A. R., Ge, F., Guidi, F., Huang, N., Lynch, G. P., Omori, Y., Trendafilova, C., et al. (2026) · Physical review. D/Physical review. D. · doi:10.1103/7wt3-9v2y · Cited by 84 · see citing works
Self-citationBaryogenesis via relativistic bubble expansion
Baldes, I., Blasi, S., Mariotti, A., Sevrin, A., & Turbang, K. (2021) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.104.115029 · Cited by 1 · see citing works
Hybrid α-attractors, primordial black holes and gravitational wave backgrounds
Braglia, M., Linde, A. D., Каллош, Р., & Finelli, F. (2023) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2023/04/033 · Cited by 82 · see citing works
Implications of stochastic effects for primordial black hole production in ultra-slow-roll inflation
Figueroa, D. G., Raatikainen, S., Räsänen, S., & Tomberg, E. (2022) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2022/05/027 · Cited by 78 · see citing works
“(This would also be needed in the solar case to fit the latest CMB data [184].”
InfluentialCosmology from CMB lensing and delensed E E power spectra using 2019–2020 SPT-3G polarization data
Ge, F., Millea, M., Camphuis, E., Daley, C., Huang, N., Omori, Y., Quan, W., Anderes, E., Anderson, A. J., Ansarinejad, B., et al. (2025) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.111.083534 · Cited by 76 · see citing works
“…allow for powerful tests of the standard cosmological model, ΛCDM, via the primary and CMB lensing signals [3], improved constraints on primordial gravitational waves via de-lensing of the degree-scale observations of the BICEP/Keck Collaboration [4], and many other science applications [5–11].”
Self-citationUpdated constraints on amplitude and tilt of the tensor primordial spectrum
Galloni, G., Bartolo, N., Matarrese, S., Migliaccio, M., Ricciardone, A., & Vittorio, N. (2023) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2023/04/062 · Cited by 75 · see citing works
Recent Developments in Warm Inflation
Kamali, V., Motaharfar, M., & Ramos, R. O. (2023) · Universe · doi:10.3390/universe9030124 · Cited by 82 · see citing works
“036, from the combined BICEP/Keck and Planck results [94].”
BackgroundPerturbativity in the presence of ultraslow-roll dynamics
Franciolini, G., Iovino, A. J., Marco Taoso, A., & Alfredo Urbano, A. (2024) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.109.123550 · Cited by 73 · see citing works
Primordial black holes from multifield inflation with nonminimal couplings
Geller, S. R., Qin, W., McDonough, E., & Kaiser, D. I. (2022) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.106.063535 · Cited by 69 · see citing works
Haque, M. R., & Maity, D. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.107.043531 · Cited by 69 · see citing works
Progress of the TianQin project
Luo, J. B., Bai, S., Bai, Y., Cai, L., Dang, H., Dong, Q., Duan, H., Du, Y., Lei, F., Fu, X., et al. (2025) · Classical and Quantum Gravity · doi:10.1088/1361-6382/adda8a · Cited by 75 · see citing works
“At the lower end of the GW spectrum, efforts are being made to look for possible signatures of primordial GWs through CMB observations (see, e.g., [10, 11]).”
BICEP/ Keck constraints on attractor models of inflation and reheating
Ellis, J. R., García, M. A. G., Nanopoulos, D. V., Olive, K. A., & Verner, S. (2022) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.105.043504 · Cited by 68 · see citing works
Lattice simulations of axion-U(1) inflation
Caravano, A., Komatsu, E., Lozanov, K. D., & Weller, J. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.108.043504 · Cited by 68 · see citing works
Analytic extensions of Starobinsky model of inflation
Ivanov, V. R., Ketov, S. V., Pozdeeva, E. O., & Vernov, S. Y. (2022) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2022/03/058 · Cited by 67 · see citing works
Refined predictions for Starobinsky inflation and post-inflationary constraints in light of ACT
Drees, M., & Xu, Y. (2025) · Physics Letters B · doi:10.1016/j.physletb.2025.139612 · Cited by 67 · see citing works
“5 × 10 15 GeV from the upper bound on the inflationary scale as measured by BICEP/KecK 2018 [30], shown in light blue.”
Measurement of gravitational lensing of the cosmic microwave background using SPT-3G 2018 data
Pan, Z., Bianchini, F., Wu, W. L. K., Ade, P. A. R., Ahmed, Z., Anderes, E., Anderson, A. J., Ansarinejad, B., Archipley, M., Aylor, K., et al. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.108.122005 · Cited by 72 · see citing works
“With SPT-3G ’s full-survey lensing map, we expect to improve BICEP Array’s r uncertainty by a factor of about 2.5, reaching σ ( r ) of about 0.003.”
InfluentialSelf-citationPrimordial gravitational waves from excited states
Fumagalli, J., Palma, G. A., Renaux‐Petel, S., Sypsas, S., Witkowski, L. T., & Zenteno, C. (2022) · Hispana · doi:10.1007/jhep03(2022)196 · Cited by 65 · see citing works
“To date, CMB observations [14] have constrained the power spectrum of primordial GWs to be far below the signal sensitivity available to the next generation of detectors (one order of magnitude for SKA, three orders of magnitude for LISA) leaving essentially no possibility for a direct detection of the SGWB’s primordi…”
BackgroundImproved Planck Constraints on Axionlike Early Dark Energy as a Resolution of the Hubble Tension
Efstathiou, G., Rosenberg, E., & Poulin, V. (2024) · Physical Review Letters · doi:10.1103/physrevlett.132.221002 · Cited by 65 · see citing works
Revisiting small-scale fluctuations in α-attractor models of inflation
Iacconi, L., Assadullahi, H., Fasiello, M., & Wands, D. (2022) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2022/06/007 · Cited by 64 · see citing works
Gravitational dark matter: Free streaming and phase space distribution
Haque, M. R., & Maity, D. (2022) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.106.023506 · Cited by 60 · see citing works
Isotropic cosmic birefringence from early dark energy
Murai, K., Naokawa, F., Namikawa, T., & Komatsu, E. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.107.l041302 · Cited by 58 · see citing works
Self-citationConstant-roll and primordial black holes in f ( Q , T ) gravity
Bourakadi, K. E., Koussour, M., Otalora, G., Bennai, M., & Ouali, T. (2023) · Physics of the Dark Universe · doi:10.1016/j.dark.2023.101246 · Cited by 58 · see citing works
PBHs and GWs from 𝕋2-inflation and NANOGrav 15-year data
Mansoori, S. A. H., Felegary, F., Talebian, A., & Sami, M. (2023) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2023/08/067 · Cited by 57 · see citing works
Bianchini, F., & Fabbian, G. (2022) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.106.063527 · Cited by 57 · see citing works
Keeping the relation between the Starobinsky model and no-scale supergravity ACTive
Gialamas, I. D., Katsoulas, T., & Tamvakis, K. (2025) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2025/09/060 · Cited by 56 · see citing works
“Recent data from the Atacama Cosmology Telescope (ACT) [5, 6] in combination with the first-year DESI measurements of baryon acoustic oscillations (BAO) [7] as well as CMB observations from BICEP/Keck [8] and Planck [9] turned out to give a value of the spectral index n s = 0 .”
Gravitational wave from graviton Bremsstrahlung during reheating
Barman, B., Bernal, N., Xu, Y., et al. (2023) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2023/05/019 · Cited by 55 · see citing works
Ye, G., Jiang, J.-Q., & Yun-song Piao, A. (2022) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.106.103528 · Cited by 53 · see citing works
Inflation in metric-affine quadratic gravity
Gialamas, I. D., & Tamvakis, K. (2023) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2023/03/042 · Cited by 53 · see citing works
“Furthermore, the combination of WMAP, Planck and BICEP/Keck data constrains the spectral index to the range 0.958 ns 0.975 again at the 95% C.L. for r = 0.004.”
BackgroundMethodInfluentialBerera, A. (2023) · Universe · doi:10.3390/universe9060272 · Cited by 53 · see citing works
“However this model required inflation at a very high energy at the GUT scale, which has been ruled out by CMB Planck data [70] and further constrained by more recent BICEP data [71].”
MethodPrimordial Black Holes from Null Energy Condition Violation during Inflation
Cai, Y., Zhu, M., & Yun-song Piao, A. (2024) · Physical Review Letters · doi:10.1103/physrevlett.133.021001 · Cited by 53 · see citing works
“035 at 95% confidence level [92], the rich phenomenology of our scenario occurs mainly on smaller scales, including the observational windows of Pulsar Timing Array (PTA) and space-borne GW detectors.”
BackgroundThe Road to Precision Cosmology
Turner, M. S. (2022) · Annual Review of Nuclear and Particle Science · doi:10.1146/annurev-nucl-111119-041046 · Cited by 58 · see citing works
Campeti, P., & Komatsu, E. (2022) · The Astrophysical Journal · doi:10.3847/1538-4357/ac9ea3 · Cited by 52 · see citing works
Primordial black hole formation in Starobinsky's linear potential model
Pi, S., & Wang, J. (2023) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2023/06/018 · Cited by 54 · see citing works
Rubiño-Martín, J. A., Guidi, F., Génova-Santos, R., Harper, S., Herranz, D., Hoyland, R. J., Lasenby, A. N., Poidevin, F., Rebolo, R., Ruiz-Granados, B., et al. (2023) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stac3439 · Cited by 51 · see citing works
Large-field inflation and the cosmological collider
Matthew Reece, B., Wang, L.-T., & Zhong-zhi Xianyu, A. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.107.l101304 · Cited by 51 · see citing works
Zhang, F. (2022) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.105.063539 · Cited by 50 · see citing works
“[103] V. Poulin, P. D. Serpico, F. Calore, S. Clesse, and K. Kohri, CMB bounds on disk-accreting massive primordial black holes, Phys.”
BackgroundInfluentialLin, J., Gao, S., Gong, Y., Lu, Y., Wang, Z., & Zhang, F. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.107.043517 · Cited by 56 · see citing works
Inflationary Butterfly Effect: Nonperturbative Dynamics from Small-Scale Features
Caravano, A., Inomata, K., & Renaux‐Petel, S. (2024) · Physical Review Letters · doi:10.1103/physrevlett.133.151001 · Cited by 50 · see citing works
BICEP/Keck and cosmological attractors
Каллош, Р., & Linde, A. D. (2021) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2021/12/008 · Cited by 50 · see citing works
On the present status of inflationary cosmology
Каллош, Р., & Linde, A. D. (2025) · General Relativity and Gravitation · doi:10.1007/s10714-025-03470-6 · Cited by 49 · see citing works
“3 shows that many models allowed by Planck 2018 (green area) have been ruled out by a combination of Planck data and the results obtained by BICEP/Keck [42].”
Coupling metric-affine gravity to a Higgs-like scalar field
Rigouzzo, C., & Zell, S. (2022) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.106.024015 · Cited by 49 · see citing works
“6) agree excellently with current observations [130, 131].”
BackgroundResultInfluentialACT observations, reheating, and Starobinsky and Higgs inflation
Zharov, D. S., Sobol, O. O., & Vilchinskiĭ, S. I. (2025) · Physical review. D/Physical review. D. · doi:10.1103/km3q-rm34 · Cited by 49 · see citing works
Enhancement of primordial curvature perturbations in R 3 -corrected Starobinsky-Higgs inflation
Kim, J., Wang, X., Zhang, Y.-L., & Ren, Z. (2025) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2025/09/011 · Cited by 47 · see citing works
“036 (95% C.L.), is put by the latest analysis of the Planck and BICEP/Keck data [6, 7].”
InfluentialPrimordial black hole dark matter from inflation: The reverse engineering approach
Franciolini, G., & Alfredo Urbano, A. (2022) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.106.123519 · Cited by 48 · see citing works
Stochastic constant-roll inflation and primordial black holes
Tomberg, E. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.108.043502 · Cited by 46 · see citing works
Inflation, the Hubble tension, and early dark energy: An alternative overview
Giarè, W. (2024) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.109.123545 · Cited by 46 · see citing works
Jiang, J.-Q., Cai, Y., Ye, G., & Yun-song Piao, A. (2024) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2024/05/004 · Cited by 46 · see citing works
“039, slightly higher than that of Planck+BK18 [8] In Figure 3 Ref.”
BackgroundMethodResultInfluentialКаллош, Р., & Linde, A. D. (2022) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2022/04/017 · Cited by 44 · see citing works
Probing reheating with graviton bremsstrahlung
Bernal, N., Cléry, S., Mambrini, Y., et al. (2024) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2024/01/065 · Cited by 44 · see citing works
“035, obtained from BICEP/Keck 2018 [52], to derive an upper bound on the inflationary scale, denoted by H I 2 .”
MethodAspects of the dark dimension in cosmology
Anchordoqui, L. A., Ignatios Antoniadis, A., & Lüst, D. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.107.083530 · Cited by 43 · see citing works
García-Bellido, J., Papageorgiou, A., Peloso, M., et al. (2024) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2024/01/034 · Cited by 43 · see citing works
“Moreover, the red tilt of its spectrum plus the current limit at CMB scales [1], implies that this SGWB is below the reach of current (LIGO, Virgo, KAGRA) or upcoming (LISA, Einstein Telescope, Cosmic Explorer) laser interferometers.”
BackgroundReheating in models with non-minimal coupling in metric and Palatini formalisms
Cheong, D. Y., Lee, S. M., & Park, S. C. (2022) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2022/02/029 · Cited by 43 · see citing works
Cosmological implications of n ≈ 1 in light of the Hubble tension
Takahashi, F., & Yin, W. (2022) · Physics Letters B · doi:10.1016/j.physletb.2022.137143 · Cited by 43 · see citing works
General double monodromy inflation
D’Amico, G., Kaloper, N., & Westphal, A. (2022) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.105.103527 · Cited by 43 · see citing works
“Figure 2: Tensor-to-scalar ratio versus spectral index for double monodromy with quartic (left) and sextic (right) kinetic terms, compared to the data of [4].”
MethodPaoletti, D., Finelli, F., Väliviita, J., et al. (2022) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.106.083528 · Cited by 42 · see citing works
“The recent release of BICEP-Keck Array (BK18) [7] in combination with Planck 2018 data has set a 95% CL upper limit on the tensor-to-scalar ratio r < 0.”
BackgroundMethodInfluentialChakraborty, A., Haque, M. R., Maity, D., et al. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.108.023515 · Cited by 42 · see citing works
Quantum effects on the evaporation of PBHs: contributions to dark matter
Haque, M. R., Maity, S., Maity, D., & Mambrini, Y. (2024) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2024/07/002 · Cited by 42 · see citing works
“036 from CMB data [78].”
MethodInfluentialPalatini R 2 quintessential inflation
Dimopoulos, K., Karam, A., López, S. S., & Tomberg, E. (2022) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2022/10/076 · Cited by 44 · see citing works
“036) [15] suggests that the inflaton potential has to be sufficiently flat at large field values.”
BackgroundMethodInfluentialQuintessential Inflation: A Tale of Emergent and Broken Symmetries
Bettoni, D., & Rubio, J. (2021) · Galaxies · doi:10.3390/galaxies10010022 · Cited by 49 · see citing works
“The tensor-to-scalar ratio following from this flow equation turns out to exceed, however, the current observational constraints [5].”
BackgroundMethodResultInfluentialReturn of Harrison–Zeldovich spectrum in light of recent cosmological tensions
Jiang, J.-Q., Ye, G., & Yun-song Piao, A. (2023) · Monthly Notices of the Royal Astronomical Society Letters · doi:10.1093/mnrasl/slad137 · Cited by 43 · see citing works
Inflationary interpretation of the nHz gravitational-wave background
Frosina, L., & Alfredo Urbano, A. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.108.103544 · Cited by 46 · see citing works
Numerical 1-loop correction from a potential yielding ultra-slow-roll dynamics
Davies, M., Iacconi, L., & Mulryne, D. J. (2024) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2024/04/050 · Cited by 41 · see citing works
Gravitational waves from inflation in LISA: reconstruction pipeline and physics interpretation
Braglia, M., Calcagni, G., Franciolini, G., Fumagalli, J., Germano Nardini, B., Peloso, M., Pieroni, M., Renaux‐Petel, S., Ricciardone, A., Gianmassimo Tasinato, C., et al. (2024) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2024/11/032 · Cited by 41 · see citing works
GW170817 Viable Einstein-Gauss-Bonnet inflation compatible with the atacama cosmology telescope data
Odintsov, S. D., & Oikonomou, V. K. (2025) · Physics Letters B · doi:10.1016/j.physletb.2025.139779 · Cited by 41 · see citing works
Independent connection in action during inflation
Salvio, A. (2025) · Physical review. D/Physical review. D. · doi:10.1103/tq3v-vy3y · Cited by 41 · see citing works
“Lower plot : the predictions of pseudoscalaron inflation in the ( n s , r ) plane together with the bounds from [3, 4] (in blue) and the more recent ones from [1, 2].”
InfluentialRevealing the cosmic history with gravitational waves
Ringwald, A., & Tamarit, C. (2022) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.106.063027 · Cited by 41 · see citing works
“002 Mpc −1, together with the newest CMB constraints at the 95% confidence level arising from a combination of Planck and BICEP/KECK results [40], as well as the projected 95% reach of the Simons Observatory (r < 0.”
BackgroundMethodInfluentialMassive neutrino self-interactions and inflation
Choudhury, S. R., Hannestad, S., & Tram, T. (2022) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2022/10/018 · Cited by 40 · see citing works
Probing the early Universe cosmology with NANOGrav: Possibilities and limitations
Ben-Dayan, I., Kumar, U., Thattarampilly, U., et al. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.108.103507 · Cited by 39 · see citing works
“007 which is much closer to the upper bound given from the joint analysis of Planck, WMAP, BICEP2, and BICEP3 [93], r 0 .”
MethodResultDahal, S., Appel, J. W., Datta, R., Brewer, M. K., Ali, A., Bennett, C. L., Bustos, R., Chan, M., Chuss, D. T., Cleary, J., et al. (2022) · The Astrophysical Journal · doi:10.3847/1538-4357/ac397c · Cited by 39 · see citing works
Qin, W., Geller, S. R., Balaji, S., McDonough, E., & Kaiser, D. I. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.108.043508 · Cited by 39 · see citing works
Kinetically modified Palatini inflation meets ACT data
Pallis, C. (2025) · Physics Letters B · doi:10.1016/j.physletb.2025.139739 · Cited by 38 · see citing works
Has ACT measured radiative corrections to the tree-level Higgs-like inflation?
Gialamas, I. D., Καράμ, Α., Racioppi, A., & Raidal, M. (2025) · Physical review. D/Physical review. D. · doi:10.1103/6fpc-67s1 · Cited by 38 · see citing works
Abdalla, E., Abellán, G. F., Aboubrahim, A., Agnello, A., Akarsu, Ö., Akrami, Y., Alestas, G., Aloni, D., Amendola, L., Anchordoqui, L. A., et al. (2022) · Journal of High Energy Astrophysics · doi:10.1016/j.jheap.2022.04.002 · Cited by 37 · see citing works
Improved cosmic microwave background (de-)lensing using general spherical harmonic transforms
Reinecke, M., Belkner, S., & Carron, J. (2023) · Astronomy and Astrophysics · doi:10.1051/0004-6361/202346717 · Cited by 37 · see citing works
CMB-S4: Iterative Internal Delensing and r Constraints
Belkner, S., Carron, J., Legrand, L., et al. (2024) · The Astrophysical Journal · doi:10.3847/1538-4357/ad2351 · Cited by 37 · see citing works
“[82], and which has been used in all BICEP/Keck analyses up to the most recent [10].”
BackgroundMethodSelf-citationNonminimal coupling in light of ACT data
Gao, Q., Gong, Y., Yi, Z., et al. (2025) · Physics of the Dark Universe · doi:10.1016/j.dark.2025.102106 · Cited by 37 · see citing works
Natural inflation after Planck 2018
Stein, N. K., & Kinney, W. H. (2022) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2022/01/022 · Cited by 37 · see citing works
Simons Observatory: Constraining inflationary gravitational waves with multitracer B -mode delensing
Namikawa, T., Lizancos, A. B., Robertson, N., Sherwin, B. D., Challinor, A. D., Alonso, D., Azzoni, S., Baccigalupi, C., Calabrese, E., Carron, J., et al. (2022) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.105.023511 · Cited by 37 · see citing works
Self-citationLimits on the cosmic neutrino background
Bauer, M., & Shergold, J. D. (2023) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2023/01/003 · Cited by 36 · see citing works
“025, which is currently constrained using combined measurements from Planck [92] and BICEP [93] to rTS ă 0.”
MethodInfluentialHeydari, S., & Karami, K. (2024) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2024/02/047 · Cited by 37 · see citing works
Ade, P. A. R., Ahmed, Z., Amiri, M., et al. (2023) · The Astrophysical Journal · doi:10.3847/1538-4357/acc85c · Cited by 36 · see citing works
Self-citationPrimordial black holes and gravitational waves from nonminimally coupled supergravity inflation
Kawai, S., & Kim, J. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.107.043523 · Cited by 36 · see citing works
Observational constraints on warm natural inflation
Montefalcone, G., Aragam, V., Visinelli, L., & Katherine Freese, B. (2023) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2023/03/002 · Cited by 36 · see citing works
- Authors
- Ade, P. A. R., Ahmed, Z., Amiri, M., Barkats, D., Thakur, R. B., Bischoff, C. A., Beck, D., Bock, J. J., Boenish, H., Bullock, E., Buza, V., Cheshire, J. R., Connors, J., Cornelison, J., Crumrine, M., Cukierman, A., Denison, E. V., Dierickx, M., Duband, L., Eiben, M., Fatigoni, S., Filippini, J. P., Fliescher, S., Goeckner-Wald, N., Goldfinger, D. C., Grayson, J., Grimes, P., Hall, G., Halal, G., Halpern, M., Hand, E., Harrison, S., Henderson, S., Hildebrandt, S. R., Hilton, G. C., Hubmayr, J., Hui, H., Irwin, K. D., Kang, J., Karkare, K. S., Karpel, E., Kefeli, S., Kernasovskiy, S. A., Kovac, J. M., Kuo, C. L., Lau, K., Leitch, E. M., Lennox, A., Megerian, K. G., Minutolo, L., Moncelsi, L., Nakato, Y., Namikawa, T., Nguyen, H. T., O’Brient, R., Ogburn, R. W., Palladino, S., Prouve, T., Pryke, C., Racine, B., Reintsema, C. D., Richter, S., Schillaci, A., Schwarz, R., Schmitt, B. L., Sheehy, C. D., Soliman, A., Germaine, T. S., Steinbach, B., Sudiwala, R. V., Teply, G. P., Thompson, K. L., Tolan, J. E., Tucker, C., Turner, A. D., Umiltà, C., Vergès, C., Vieregg, A. G., Wandui, A., Weber, A. C., Wiebe, D. V., Willmert, J., Wong, C. L., Wu, W. L. K., Yang, H., Yoon, K. W., Young, E., Yu, C., Zeng, L., Zhang, C., Zhang, S., & BICEP/<i>Keck</i> Collaboration
- Affiliations
- Cardiff University (GB)
- SLAC National Accelerator Laboratory (US)
- University of British Columbia (CA)
- Center for Astrophysics Harvard & Smithsonian (US)
- California Institute of Technology (US)
- University of Cincinnati (US)
- University of Minnesota (US)
- University of Chicago (US)
- National Institute of Standards and Technology (US)
- Commissariat à l'Énergie Atomique et aux Énergies Alternatives (FR)
- University of Illinois Urbana-Champaign (US)
- Stanford University (US)
- Harvard University (US)
- Jet Propulsion Laboratory (US)
- Kavli Institute for the Physics and Mathematics of the Universe (JP)
- Service des Basses Températures, Commissariat à l’Energie Atomique, 38054 Grenoble, France
- Centre National de la Recherche Scientifique (FR)
- Brookhaven National Laboratory (US)
- ORCID
- Ade, P. A. R.
- Ahmed, Z.
- Barkats, D.
- Bischoff, C. A.
- Beck, D.
- Bock, J. J.
- Buza, V.
- Cheshire, J. R.
- Cukierman, A.
- Dierickx, M.
- Eiben, M.
- Filippini, J. P.
- Goldfinger, D. C.
- Grimes, P.
- Halal, G.
- Halpern, M.
- Henderson, S.
- Hildebrandt, S. R.
- Irwin, K. D.
- Karkare, K. S.
- Kovac, J. M.
- Kuo, C. L.
- Leitch, E. M.
- Nakato, Y.
- Namikawa, T.
- Ogburn, R. W.
- Pryke, C.
- Racine, B.
- Schillaci, A.
- Sudiwala, R. V.
- Thompson, K. L.
- Tolan, J. E.
- Vergès, C.
- Vieregg, A. G.
- Wandui, A.
- Wiebe, D. V.
- Willmert, J.
- Wu, W. L. K.
- Young, E.
- Yu, C.
- Zeng, L.
- Venue
- Physical Review Letters
- Publisher
- American Physical Society (APS)
- Published
- 2021-10-04
- Volume
- 127
- Issue
- 15
- Pages
- 151301-151301
- ISSN
- 0031-9007 (ISSN-L)
- 1079-7114
- OpenAlex
- W3202102945
- Semantic Scholar
- 93637369c8e398b920a6f82f83adf5ffc4fbba76
- Cited by
- 1,014
- References
- 57
- Citations by year
- 2026: 163 · 2025: 253 · 2024: 218 · 2023: 203 · 2022: 162 · 2021: 15
- FWCI
- 80.49
- Type
- journal article
- Language
- en
- Open access
- green
- arxiv.org
- Licence
- Locations
- Physical Review Letters (publishedVersion)
- PubMed (publishedVersion)
- arXiv (Cornell University) (submittedVersion)
- CaltechAUTHORS (California Institute of Technology) (submittedVersion)
- HAL AMU (submittedVersion)
- OSTI OAI (U.S. Department of Energy Office of Scientific and Technical Information) (submittedVersion)
- arXiv (Cornell University)
- Funders
- National Science Foundation (0742818, 0742592, 1044978, 1110087, 1145172, 1145143, 1145248, 1639040, 1638957, 1638978, 1638970)
- W. M. Keck Foundation
- Jet Propulsion Laboratory
- National Aeronautics and Space Administration (06-ARPA206-0040, 10-SAT10-0017, 12-SAT12-0031, 14-SAT14-0009, 16-SAT-16-0002)
- Gordon and Betty Moore Foundation
- Canada Foundation for Innovation
- University of British Columbia
- Science and Technology Facilities Council (ST/N000706/1)
- Faculty of Arts and Sciences, Harvard University
- U.S. Department of Energy
- Office of Science
- Topics
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Cosmology and Gravitation Theories
- Physical Sciences › Physics and Astronomy › Nuclear and High Energy Physics › Dark Matter and Cosmic Phenomena
- Physical Sciences › Physics and Astronomy › Statistical and Nonlinear Physics › Noncommutative and Quantum Gravity Theories
- Keywords
- primordial gravitational waves, BICEP2, Keck Array, CMB polarization, tensor-to-scalar ratio, foreground modeling, polarized dust emission, synchrotron radiation, Planck, WMAP
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