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High-precision timing of millisecond pulsars. 3: Long-term monitoring of PSRs B1855+09 and B1937+21
Abstract
Biweekly timing observations of PSRs B1855+09 and B1937+21 have been made at the Arecibo Observatory for more than 7 and 8 year, respectively, with uniform procedures and only a few modest gaps. On each observing date we measure an equivalent pulse arrival time for PSR B1855+09 at 1.4 GHz, with typical accuracies of about 0.8 micrometers and for PSR B1937 + 21 at both 1.4 and 2.4 GHz, with accuracies around 0.2 micrometers. The pulse arrival times are fitted to a simple model for each pulsar, yielding high-precision astrometric, rotational, and orbital parameters, and a diverse range of conclusions. The celestial coordinates and proper motions of the two pulsars are determined with uncertainties less than or equal to 0.12 mas and less than or equal to 0.06 mas/year in the reference frame of the DE200 planetary ephemeris. The annual parallaxes are found to be pi=1.1 +/- 0.3 mas and pi less than 0.28 mas for PSRs B1855+09 and B1937+21, respectively. The general relativistic Shapiro delay is measured in the PSR B1855+09 system and used to obtain masses m1 = 1.50 +0.26 -0.14 solar mass and m (sub2) = 0.258 +0.028-0.016solar mass for the pulsar and its orbiting companion. The extremely stable orbital period of this system provides a phenomenological limit on the secular change of Newton's gravitational constant, dot-G/G=(-9 +/- 18) x 10-12/year. Variations in the dispersion measure of PSR B1937 + 21 indicate that the spectrum of electron-density fluctuations in the interstellar medi um has a power-law index beta = 3.874 +/- 0.011, slightly steeper than the Kolmogorov value of 11/3, and we find no strong evidence for an 'inner scale' greater than about 2 x 109cm. In the residual pulse arrival times for PSR B1937+21 we have observed small systematic trends not explained by our deterministic timing model. We discuss a number of possible causes; although the results are not yet conclusive, the most straightforward interpretation is that the unmodeled noise (a few microseconds over 8 yr, or Delta t/T approximately equals 10-14 is inherent to the pulsar itself. In the present data set, PSR B1855+09 exhibits no discernible timing noise. With conventional assumptions we derive a limit Omega g h2 less than 6 x 10-8 (95% confidence) for the energy density, per logarithmic frequency interval, in a cosmic background of stochastic gravitational waves. We discuss the feasibility of establishing a pulsar-based timescale that might be used to test the stabilities of the best available atomic clocks. In an Appendix, we propose guidelines for the archiving of pulsar timing observations. Instructions are provided for obtaining copies of our own archival data, via Internet.
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“If the electroweak and/or the chiral phase transitions occurred out of equilibrium they could be a significant source of primordial magnetic fields[117].”
From Phase Transitions in the Early and Present Universe (2006) · cites this paper as [117]
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Recycled Pulsars Discovered at High Radio Frequency
Edwards, R. T., & Bailes, M. (2001) · The Astrophysical Journal · doi:10.1086/320986 · Cited by 55
A Catalog of Potential Post–Common Envelope Binaries
Kruckow, M. U., Neunteufel, P., Stefano, R. D., Gao, Y., & Kobayashi, C. (2021) · The Astrophysical Journal · doi:10.3847/1538-4357/ac13ac · Cited by 54
Recycled Pulsars Discovered at High Radio Frequency
Edwards, R. T., & Bailes, M. (2001) · CERN Document Server (European Organization for Nuclear Research) · Cited by 54
Vijaykumar, A., Kapadia, S. J., & Ajith, P. (2021) · Physical Review Letters · doi:10.1103/physrevlett.126.141104 · Cited by 59
Dark energy, co-evolution of massive black holes with galaxies, and ASTROD-GW
Ni, W.-T. (2012) · Advances in Space Research · doi:10.1016/j.asr.2012.09.019 · Cited by 52
“For example, Jenet et al. (2004) ruled out the existence of a coalescing supermassive black-hole binary system (postulated in Sudou et al. (2003) from radio observations) at the centre of the radio galaxy 3C66B by using actual pulsar data from Kaspi et al. (1994).”
MethodRecycling of neutron stars in common envelopes and hypernova explosions
Barkov, M. V., & Komissarov, S. S. (2011) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2011.18762.x · Cited by 52
“It is rather difficult to measure the mass of a millisecond pulsar, but the few available results agree with this prediction of the accretion model (Kaspi et al. 1994; Jacoby et al. 2005; Demorest et al. 2010).”
ResultStudying the Solar system with the International Pulsar Timing Array
Caballero, R. N., Guo, Y. J., Lee, K., et al. (2018) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sty2632 · Cited by 52
Arzoumanian, Z., Baker, P. T., Brazier, A., et al. (2020) · The Astrophysical Journal · doi:10.3847/1538-4357/ababa1 · Cited by 52
“It was the first object targeted for continuous wave detection, as reported by Jenet et al. (2004) (hereafter J04), in which seven years of Arecibo timing data from PSR B1855+09 (Kaspi et al. 1994) was used to search the Fourier domain timing residuals (commonly referred to as a Lomb-Scargle periodogram), using harmon…”
MethodTiming Observations of Four Millisecond Pulsars with the Arecibo and Effelsberg Radio Telescopes
Wolszczan, A., Doroshenko, O. V., Konacki, M., et al. (2000) · The Astrophysical Journal · doi:10.1086/308206 · Cited by 52
“…lack of a comparable timing noise in other millisecond pulsars with spin parameters and ages similar to those of PSR B1257]12 (e.g., PSR B1855]09 ; Kaspi et al. 1994) and the presence of three planets around the pulsar make it much more likely that the observed TOA variations are caused by…”
BackgroundResultInfluentialSelf-citationKrämer, M., Janssen, G. H., Harding, A. K., et al. (n.d.) · NASA STI Repository (National Aeronautics and Space Administration) · Cited by 52
Model-based asymptotically optimal dispersion measure correction for pulsar timing
Lee, K. J., Bassa, C., Janssen, G. H., et al. (2014) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stu664 · Cited by 51
“Based on the five examples, we also compare the reconstructed DM variation waveform with the results from three other methods: polynomial smoothing (Kaspi et al. 1994; Freire et al. 2012); piecewise linear function fitting (Keith et al. 2013); and point-to-point fitting.”
MethodDetecting cosmic strings in the CMB with the Canny algorithm
Amsel, S., Berger, J., & Brandenberger, R. (2007) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2008/04/015 · Cited by 58
THEORETICAL TOOLS FOR CMB PHYSICS
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Jofré, P., Reisenegger, A., & Fernández, R. (2006) · Physical Review Letters · doi:10.1103/physrevlett.97.131102 · Cited by 50
The impact of element diffusion on the formation and evolution of helium white dwarf stars
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Searching for Primordial Black Hole Dark Matter with Pulsar Timing Arrays
Seto, N., & Cooray, A. R. (2007) · The Astrophysical Journal · doi:10.1086/516570 · Cited by 50
“This is because we cannot separate TOA residuals due to gravitational waves from secular effects such as the long-term spin evolution of pulsars (Kaspi et al. 1994, see also Damour & Taylor 1991).”
BackgroundThe Parallax and Proper Motion of PSR J0030+0451
Lommen, A. N., Kipphorn, R. A., Nice, D. J., et al. (2006) · The Astrophysical Journal · doi:10.1086/501067 · Cited by 50
Pulsars as gravitational wave detectors
Hobbs, G. B. (2010) · Astrophysics and space science proceedings · doi:10.1007/978-3-642-17251-9_20 · Cited by 49
Review of Options for Autonomous Cislunar Navigation
Christian, J. A., & Lightsey, E. G. (2009) · Journal of Spacecraft and Rockets · doi:10.2514/1.42819 · Cited by 49
CANNY ALGORITHM, COSMIC STRINGS AND THE COSMIC MICROWAVE BACKGROUND
Danos, R. J., & Brandenberger, R. (2010) · International Journal of Modern Physics D · doi:10.1142/s0218271810016324 · Cited by 50
The Green Bank Northern Sky Survey for Fast Pulsars
Sayer, R. W., Nice, D. J., & Taylor, J. H. (1997) · The Astrophysical Journal · doi:10.1086/303446 · Cited by 49
Self-citationGravitational wave detection using pulsars: status of the Parkes Pulsar Timing Array projectPreprint
Hobbs, G. B., Bailes, M., Bhat, N. D. R., et al. (2009) · Cited by 48
On Pulse Phase Estimation and Tracking of Variable Celestial X-ray Sources
Golshan, A., & Sheikh, S. I. (2007) · Cited by 47
Relic gravitational waves with a running spectral index and its constraints at high frequencies
Tong, M., & Zhang, Y. (2009) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.80.084022 · Cited by 49
Measurement uncertainty in pulsar timing array experiments
Verbiest, J. P. W., & Shaifullah, G. M. (2018) · Classical and Quantum Gravity · doi:10.1088/1361-6382/aac412 · Cited by 47
A new white dwarf constraint on the rate of change of the gravitational constant
Biesiada, M., & Malec, B. (2003) · CERN Document Server (European Organization for Nuclear Research) · Cited by 47
CHECKING THE VARIABILITY OF THE GRAVITATIONAL CONSTANT WITH BINARY PULSARS
Бисноватый-Коган, Г. С. (2006) · International Journal of Modern Physics D · doi:10.1142/s0218271806008747 · Cited by 51
A 24 HR GLOBAL CAMPAIGN TO ASSESS PRECISION TIMING OF THE MILLISECOND PULSAR J1713+0747
Dolch, T., Lam, M. T., Cordes, J. M., et al. (2014) · The Astrophysical Journal · doi:10.1088/0004-637x/794/1/21 · Cited by 45
“In contrast, the first MSP discovered, PSR B1937+21, is well known to be extremely stable on the order of weeks to months, but its residuals show a significant red noise power spectrum visible on timescales of years (Kaspi et al. 1994).”
BackgroundNoise analysis for X-ray navigation systems
Hanson, J., Sheikh, S. I., Graven, P., et al. (2008) · IEEE/ION Position Location and Navigation Symposium · doi:10.1109/plans.2008.4570028 · Cited by 45
“A unique aspect of this rotation is that it can be extremely stable and predictable [12, 13].”
BackgroundThe Nature and Evolutionary History of GRO J1744−28
Rappaport, S., & Joss, P. C. (1997) · The Astrophysical Journal · doi:10.1086/304506 · Cited by 45
The search for gravitational wave bursts in data from the second LIGO science run
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Constraining the Evolution of ZZ Ceti
Mukadam, A. S., Kepler, S. O., Winget, D. E., et al. (2003) · The Astrophysical Journal · doi:10.1086/377044 · Cited by 44
“It has a period of 5.36 ms and a measured _P ¼ 1:78363 10 20 s s 1 (Kaspi et al. 1994), which implies that the stability timescale is s 9:5 Gyr.”
BackgroundInfluentialOptimal filters for the construction of the ensemble pulsar time
Rodin, A. E. (2008) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2008.13270.x · Cited by 43
The NANOGrav Nine-year Data Set: Excess Noise in Millisecond Pulsar Arrival Times
Lam, M. T., Cordes, J. M., Chatterjee, S., et al. (2016) · Repository of the Academy's Library (Library of the Hungarian Academy of Sciences) · Cited by 42
The NANOGrav 11 yr Data Set: Evolution of Gravitational-wave Background Statistics
Hazboun, J. S., Simon, J., Taylor, S. R., et al. (2020) · The Astrophysical Journal · doi:10.3847/1538-4357/ab68db · Cited by 42
“It has long been known that this pulsar has a great deal of red noise (Kaspi et al. 1994), so much that it was not included in the analysis by Arzoumanian et al. (2016).”
BackgroundChen, Z.-C., Wu, Y.-M., & Huang, Q.-G. (2022) · Communications in Theoretical Physics · doi:10.1088/1572-9494/ac7cdf · Cited by 41
“In this work, we use the VersionB data release by choosing only pulsars with a timing baseline greater than three years in our analyses and excluding the pulsar J1939 +2134 because of its complicated DM variation and timing noise [18, 35, 36].”
Pulsed X‐Ray Emission from the Fastest Millisecond Pulsar: PSR B1937+21 withASCA
Takahashi, M., Shibata, S., Torii, K., et al. (2001) · The Astrophysical Journal · doi:10.1086/321330 · Cited by 41
CONSTRAINING THE COALESCENCE RATE OF SUPERMASSIVE BLACK-HOLE BINARIES USING PULSAR TIMING
Wen, Z. L., Jenet, F. A., Yardley, D. R. B., et al. (2011) · The Astrophysical Journal · doi:10.1088/0004-637x/730/1/29 · Cited by 40
“Previous work (Romani & Taylor 1983; Kaspi et al. 1994; Lommen 2002; Jenet et al. 2006) placed upper limits on a stochastic background of GWs.”
BackgroundKhurshudyan, M., Pourhassan, B., & Pasqua, A. (2015) · Canadian Journal of Physics · doi:10.1139/cjp-2014-0283 · Cited by 37
Systematic And Stochastic Variations In Pulsar Dispersion Measures
Lam, M. T., Cordes, J. M., Chatterjee, S., et al. (2016) · The Research Repository @ WVU (West Virginia University) · Cited by 40
On detection of the stochastic gravitational-wave background using the Parkes pulsar timing array
Yardley, D. R. B., Coles, W. A., Hobbs, G. B., et al. (2024) · Figshare · doi:10.25916/sut.26242943.v1 · Cited by 40
PSR J1022+1001: profile stability and precision timing
Hotan, A. W., Bailes, M., & Ord, S. M. (2004) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2004.08376.x · Cited by 40
“The discovery of the millisecond pulsars PSR B1937+21 and B1855+09 (Backer et al. 1982; Segelstein et al. 1986) and their subsequent timing (Kaspi et al. 1994) revealed that millisecond pulsars were very rotationally stable, rivaling the best atomic clocks.”
BackgroundBinary pulsars as detectors of ultralow-frequency gravitational waves
Kopeikin, S. M. (1997) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.56.4455 · Cited by 40
Temperature and cooling age of the white dwarf companion of PSR J0218+4232
Bassa, C., van Kerkwijk, M. H., & Kulkarni, S. R. (2003) · Astronomy and Astrophysics · doi:10.1051/0004-6361:20030384 · Cited by 40
VANISHING DIMENSIONS AND PLANAR EVENTS AT THE LHC
Anchordoqui, L. A., DAI, D. C., FAIRBAIRN, M., LANDSBERG, G., & STOJKOVIC, D. (2012) · Modern Physics Letters A · doi:10.1142/s0217732312500216 · Cited by 64
Single‐Pulse Characteristics of the Millisecond Radio Pulsar PSR B1937+21 at 430 MHz
Jenet, F. A., Anderson, S. B., & Prince, T. A. (2001) · The Astrophysical Journal · doi:10.1086/318256 · Cited by 39
“This pulsarÏs timing noise is extremely small (Kaspi et al. 1994), the linear polarization angle is nearly constant across both proÐles (Thorsett & Stinebring 1990), and the giant pulses occur in a restricted region of pulse phase (Kinkhabwala & Thorsett 2000).”
BackgroundSmashing the Guitar: An Evolving Neutron Star Bow Shock
Chatterjee, S., & Cordes, J. M. (2003) · CERN Document Server (European Organization for Nuclear Research) · Cited by 39
High energy physics and the very early universe with LISA
Ungarelli, C., & Vecchio, A. (2001) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.63.064030 · Cited by 39
New mechanism for the generation of primordial seeds for the cosmic magnetic fields
Gasperini, M. (2001) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.63.047301 · Cited by 38
Low frequency gravitational waves from black hole MACHO binaries
Ioka, K., Tanaka, T., & Nakamura, T. (1999) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.60.083512 · Cited by 37
The Parkes Pulsar Timing Array
Manchester, R. N. (2006) · 天文和天体物理学研究:英文版 · doi:10.1088/1009-9271/6/s2/27 · Cited by 38
Lai, D. (1998) · The Astrophysical Journal · doi:10.1086/305938 · Cited by 38
“In particular, the 5.4 ms recycled pulsar B1855+09, which is thought to have gone through a LMXB phase (Phinney & Kulkarni 1994), has a mass 1.50 ± 0.26 0.14 M ⊙ (Kaspi et al. 1994).”
MethodInfluentialAnswers to frequently asked questions about the pulsar timing array Hellings and Downs curve
Romano, J. D., & Allen, B. (2024) · Classical and Quantum Gravity · doi:10.1088/1361-6382/ad4c4c · Cited by 37
“Indeed, in the early days of pulsar timing, upper limits were set on the amplitude of GWs by examining the timing residuals from single pulsars [19].”
BackgroundThe minimally extended Varying Speed of Light (meVSL)
Lee, S. (2021) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2021/08/054 · Cited by 43
The parallax, mass and age of the PSR J2145-0750 binary system
Lohmer, O., Krämer, M., Driebe, T. M., et al. (2004) · Astronomy and Astrophysics · doi:10.1051/0004-6361:20041031 · Cited by 37
A baseband recorder for radio pulsar observations
Stairs, I. H., Splaver, E. M., Thorsett, S. E., et al. (2000) · Monthly Notices of the Royal Astronomical Society · doi:10.1046/j.1365-8711.2000.03306.x · Cited by 37
Self-citationPulsar timing array observations of gravitational wave source timing parallax
Deng, X., & Finn, L. S. (2011) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2010.17913.x · Cited by 36
“…has been used to bound the gravitational wave power associated with stochastic gravitational waves of cosmological origin (Romani & Taylor 1983; Kaspi et al. 1994; Lommen 2002); timing residual correlations among pulsar pairs have been used to bound the power in an isotropic stochastic…”
MethodSpacecraft Navigation and Timing Using X-ray Pulsars
Sheikh, S. I., Hanson, J., Graven, P., et al. (2011) · NAVIGATION Journal of the Institute of Navigation · doi:10.1002/j.2161-4296.2011.tb01799.x · Cited by 36
VANISHING DIMENSIONS AND PLANAR EVENTS AT THE LHC
Anchordoqui, L. A., Dai, D.-C., Fairbairn, M., et al. (2012) · Research Portal (King's College London) · Cited by 36
Pogosian, L., Wyman, M., & Wasserman, I. (2004) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2004/09/008 · Cited by 36
Constraining a Possible Variation of G with Type Ia Supernovae
Mould, J. R., & Uddin, S. A. (2014) · Publications of the Astronomical Society of Australia · doi:10.1017/pasa.2014.9 · Cited by 56
A detailed study of giant pulses from PSR B1937+21 using the Large European Array for Pulsars
McKee, J. W., Stappers, B. W., Bassa, C., et al. (2018) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sty3058 · Cited by 35
“It is one of the few MSPs that is presently known to exhibit significant timing noise (Kaspi et al. 1994, Shannon et al. 2013, Caballero et al. 2016), in addition to large variations in dispersion measure (DM) and scattering (Ramachandran et al. 2006, Keith et al. 2013, Levin et al. 2016), all of…”
BackgroundPULSAR TIMING ERRORS FROM ASYNCHRONOUS MULTI-FREQUENCY SAMPLING OF DISPERSION MEASURE VARIATIONS
Lam, M. T., Cordes, J. M., Chatterjee, S., et al. (2015) · The Astrophysical Journal · doi:10.1088/0004-637x/801/2/130 · Cited by 34
“…DM variations are well known, e.g., for the Crab Pulsar (Isaacman & Rankin 1977), for B1937+21 (Rawley et al. 1988; Cordes et al. 1990; Kaspi et al. 1994; Ramachandran et al. 2006), for B1821–24 (Cognard & Lestrade 1997), and numerous other cases (Phillips & Wolszczan 1991; Backer et…”
BackgroundDeneva, J. S., Ray, P. S., Lommen, A., et al. (2019) · The Astrophysical Journal · doi:10.3847/1538-4357/ab0966 · Cited by 34
“This is equivalent to the approach taken by Taylor (1991) and Kaspi et al. (1994).”
Constraining an exact Brans–Dicke gravity theory with recent observations
Amirhashchi, H., & Yadav, A. K. (2020) · Physics of the Dark Universe · doi:10.1016/j.dark.2020.100711 · Cited by 40
Local constraints on cosmic string loops from photometry and pulsar timing
Pshirkov, M. S., & Tuntsov, A. V. (2010) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.81.083519 · Cited by 34
TWO MILLISECOND PULSARS DISCOVERED BY THE PALFA SURVEY AND A SHAPIRO DELAY MEASUREMENT
Deneva, J. S., Freire, P. C. C., Cordes, J. M., et al. (2012) · The Astrophysical Journal · doi:10.1088/0004-637x/757/1/89 · Cited by 33
“In this respect, they are very similar to PSR B1855+09 (z ∼ 50 pc; Kaspi et al. 1994) and PSR J1903+0327 (z < 270 pc; Freire et al. 2011), which are also close to the Galactic plane.”
ResultSelf-citationObservable gravitational waves in pre-big bang cosmology: an update
Gasperini, M. (2016) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2016/12/010 · Cited by 33
Discovery of the Young, Energetic Radio Pulsar PSR J1105−6107
Kaspi, V. M., Bailes, M., Manchester, R. N., et al. (1997) · The Astrophysical Journal · doi:10.1086/304462 · Cited by 33
Self-citationScalar and tensor inhomogeneities from dimensional decoupling
Massimo Giovannini, A. (1997) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.55.595 · Cited by 33
Inflation, string theory and cosmic strings
Chernoff, D. F., & Tye, S.-H. H. (2015) · International Journal of Modern Physics D · doi:10.1142/s0218271815300104 · Cited by 32
“results for experiments involving lensing [83, 84, 85, 86, 87, 88, 89, 90, 91], gravitational wave background and bursts [92, 93, 94, 95, 96, 97, 98, 99, 100, 101, 102, 103, 104, 105], pulsar timing [106, 84, 107, 108, 109, 110, 111] and cosmic microwave background radiation [9, 75, 112, 113, 114, 115, 116, 117, 76, 1…”
BackgroundThe Temperature and Cooling Age of the White Dwarf Companion to the Millisecond Pulsar PSR B1855+09
van Kerkwijk, M. H., Bell, J. F., Kaspi, V. M., et al. (2000) · The Astrophysical Journal · doi:10.1086/312478 · Cited by 32
“…for which braking indices have been measured, values less than 3 have been found: n = 2.51 ± 0.01 for PSR B0531+21 (Lyne, Pritchard, & Smith 1993); 2.28 ± 0.02 for PSR B0540−69 (Boyd et al. 1995); 1.4 ± 0.2 for PSR B0833−45 (Lyne et al. 1996); and 2.837± 0.001 for PSR B1509−58 (Kaspi et al. 1994).”
InfluentialSelf-citationFundamental constants: from measurement to the universe, a window on gravitation and cosmology
Uzan, J.-P. (2025) · Living Reviews in Relativity · doi:10.1007/s41114-025-00059-y · Cited by 36
Validation of Pulsar Phase Tracking for Spacecraft Navigation
Anderson, K. D., Pines, D. J., & Sheikh, S. I. (2015) · Journal of Guidance Control and Dynamics · doi:10.2514/1.g000789 · Cited by 31
“In fact, a specific subset called millisecond period pulsars (MSPs) have been shown tomatch the stabilities of today’s atomic clocks [10,11].”
BackgroundPerera, B. B. P., Stappers, B. W., Babak, S., et al. (2018) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sty1116 · Cited by 31
“Due to their high rotational stability, the timing measurements of MSPs can be obtained with a significant accuracy (e.g. Kaspi et al. 1994).”
BackgroundLutz-Kelker bias in pulsar parallax measurements
Verbiest, J. P. W., Lorimer, D. R., & McLaughlin, M. A. (2010) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2010.16488.x · Cited by 30
“T 0.14+0.06−0.04 – Kaspi et al. (1994) (B1937+21) 0.13 ± 0.065 2.0 0.01 ± 0.10 – 0.14+0.05−0.03 0.0 ± 0.08 Verbiest et al. (2009) J2018+2839 0.9 ± 3.6 0.3 –”
InfluentialConstraints on pre-big-bang models for seeding large-scale anisotropy by massive Kalb-Ramond axions
Gasperini, M., & VENEZIANO, G. (1998) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.59.043503 · Cited by 28
Effect of evolving physical constants on type Ia supernova luminosity
Gupta, R. P. (2022) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stac254 · Cited by 29
Measuring neutron star mass and radius with three mass-radius relations
Zhang, C. M., Yin, H. X., Kojima, Y., et al. (2006) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2006.11133.x · Cited by 29
Evolution of white dwarfs as a probe of theories of gravitation: the case of Brans—Dicke
Benvenuto, O. G., Althaus, L. G., & Torres, D. F. (1999) · Monthly Notices of the Royal Astronomical Society · doi:10.1046/j.1365-8711.1999.02486.x · Cited by 28
The minimum and maximum gravitational-wave background from supermassive binary black holes
Zhu, X. J., Cui, W., & Thrane, E. (2018) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sty2849 · Cited by 28
“The proposed binary system, with inferred total mass of 5.4 × 1010M and mass ratio of 0.1, was subsequently ruled out with 95% confidence by Jenet et al. (2004) using timing observations of PSR B1855+09 presented in Kaspi et al. (1994).”
MethodInfluentialConstraining cosmic superstrings with dilaton emission
Babichev, E., & Kachelrieß, M. (2005) · Physics Letters B · doi:10.1016/j.physletb.2005.03.053 · Cited by 28
“8 wave background [ 15 ]. However, this bounds is modified only by a factor < 3 in the range of dilaton masses m� < 150 TeV and cosmic string parameters, 10 3 < p ≤ 1 and 104 < ǫ < 10 6, therefore the Figs.”
BackgroundKrastev, P. G., & Li, B.-A. (2007) · Physical Review C · doi:10.1103/physrevc.76.055804 · Cited by 28
Dehant, V., & Capitaine, N. (1997) · Celestial Mechanics and Dynamical Astronomy · doi:10.1007/bf00049506 · Cited by 28
MERGERS OF LUMINOUS EARLY-TYPE GALAXIES IN THE LOCAL UNIVERSE AND GRAVITATIONAL WAVE BACKGROUND
Wen, Z. L., Liu, F. S., & Han, J. L. (2009) · The Astrophysical Journal · doi:10.1088/0004-637x/692/1/511 · Cited by 27
“(18) Using the eight year timing data of PSR B1855+09, Kaspi et al. (1994) obtainedΩh2 < 6× 10−8 for the cosmic GW background.”
MethodTemperature and cooling age of the white dwarf companion of PSR J0218+4232
Bassa, C., van Kerkwijk, M. H., & Kulkarni, S. R. (2003) · Springer Link (Chiba Institute of Technology) · doi:10.1051/0004-6361:20030384/pdf · Cited by 27
Pulse Arrival Times from Binary Pulsars with Rotating Black Hole Companions
Laguna, P., & Wolszczan, A. (1997) · The Astrophysical Journal · doi:10.1086/310835 · Cited by 27
Wolszczan, A., Hoffman, I. M., Konacki, M., et al. (2000) · The Astrophysical Journal · doi:10.1086/312872 · Cited by 27
The refractive index of relic gravitons
Massimo Giovannini, A. (2016) · Classical and Quantum Gravity · doi:10.1088/0264-9381/33/12/125002 · Cited by 27
Sensitivity of wideband detectors to quintessential gravitons
Babusci, D., & Giovannini, M. (1999) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.60.083511 · Cited by 27
The NANOGrav 11-year Data Set: Pulse Profile Variability
Brook, P. R., Karastergiou, A., McLaughlin, M. A., et al. (2018) · The Astrophysical Journal · doi:10.3847/1538-4357/aae9e3 · Cited by 26
“Suggested interpretations of the red noise include intrinsic changes in the spindown rate of the pulsar (Kaspi et al. 1994), interstellar propagation effects (Armstrong 1984; Rickett 1990; Kaspi et al. 1994; Cognard et al. 1995) and the presence of a circumpulsar asteroid belt (Shannon et al. 2013).”
BackgroundLutz-Kelker bias in pulsar parallax measurements
Verbiest, J. ;. H. O.-0.-4.-8., Lorimer, D. R., & McLaughlin, M. A. (2010) · The Research Repository @ WVU (West Virginia University) · Cited by 26
Beskin, V. S., Чернов, С. В., Gwinn, C. R., et al. (2015) · Space Science Reviews · doi:10.1007/s11214-015-0173-8 · Cited by 26
Siklér, F., Ray, P. S., Lommen, A. N., et al. (2019) · Repository of the Academy's Library (Library of the Hungarian Academy of Sciences) · Cited by 26
Secondary graviton spectra and waterfall-like fields
Giovannini, M. (2010) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.82.083523 · Cited by 26
Pulsars and Gravitational Wave Detection
Hobbs, G. (2005) · Publications of the Astronomical Society of Australia · doi:10.1071/as04063 · Cited by 26
“This work was generalized for multiple pulsar data sets by Kaspi et al. (1994), but was criticized by Thorsett & Dewey (1996), who developed a technique based on the Neyman–Pearson test.”
MethodPulsar Timing Arrays: Status and Techniques
Hobbs, G. B. (2012) · Proceedings of the International Astronomical Union · doi:10.1017/s1743921312023526 · Cited by 25
The confrontation between general relativity and experiment
Will, C. M. (2004) · Pramana · doi:10.1007/bf02705195 · Cited by 29
Bayesian estimation of non-Gaussianity in pulsar timing analysis
Lentati, L., Hobson, M., & Alexander, P. (2014) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stu1721 · Cited by 24
Gravitational wave detection using high precision pulsar observations
Hobbs, G. B. (2008) · Classical and Quantum Gravity · doi:10.1088/0264-9381/25/11/114032 · Cited by 24
“In contrast with earlier techniques (e.g. Kaspi et al 1994) this method used the TEMPO2 software package (Hobbs et al 2006a) to account for all the fitting procedures undertaken during the pulsar timing process.”
Method
Metadata
- Authors
- Kaspi, V. M., Taylor, J. H., & Ryba, M. F.
- ORCID
- Kaspi, V. M.
- Venue
- The Astrophysical Journal
- Publisher
- American Astronomical Society
- Published
- 1994-06
- Volume
- 428
- Pages
- 713
- ISSN
- 0004-637X (ISSN-L)
- 1538-4357
- OpenAlex
- W2025727932
- Cited by
- 595
- References
- 0
- Citations by year
- 2026: 8 · 2025: 16 · 2024: 21 · 2023: 13 · 2022: 9 · 2021: 17 · 2020: 13 · 2019: 14 · 2018: 33 · 2017: 7 · 2016: 20 · 2015: 21 · 2014: 17 · 2013: 17 · 2012: 22
- FWCI
- 25.02
- Type
- journal article
- Language
- en
- Open access
- closed
- Locations
- The Astrophysical Journal (publishedVersion)
- Topics
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Pulsars and Gravitational Waves Research
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Astrophysical Phenomena and Observations
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Stellar, planetary, and galactic studies
- Keywords
- millisecond pulsars, PSR B1937+21, pulsar timing, proper motions, annual parallax, Shapiro delay, varying gravitational constant, dispersion measure, Kolmogorov spectrum, pulsar astrometry, orbital elements, Arecibo Observatory
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