Comparison of Martian surface ionizing radiation measurements from MSL-RAD with Badhwar-O'Neill 2011/HZETRN model calculations
Open accessAbstract
Abstract Dose rate measurements from Mars Science Laboratory‐radiation assessment detector (MSL‐RAD) for 300 sols on Mars are compared to simulation results using the Badhwar‐O'Neill 2011 galactic cosmic ray (GCR) environment model and the high‐charge and energy transport (HZETRN) code. For the nuclear interactions of primary GCR through Mars atmosphere and Curiosity rover, the quantum multiple scattering theory of nuclear fragmentation is used. Daily atmospheric pressure is measured at Gale Crater by the MSL Rover Environmental Monitoring Station. Particles impinging on top of the Martian atmosphere reach RAD after traversing varying depths of atmosphere that depend on the slant angles, and the model accounts for shielding of the RAD “E” detector (used for dosimetry) by the rest of the instrument. Simulation of average dose rate is in good agreement with RAD measurements for the first 200 sols and reproduces the observed variation of surface dose rate with changing heliospheric conditions and atmospheric pressure. Model results agree less well between sols 200 and 300 due to subtleties in the changing heliospheric conditions. It also suggests that the average contributions of albedo particles (charge number Z < 3) from Martian regolith comprise about 10% and 42% of the average daily point dose and dose equivalent, respectively. Neutron contributions to tissue‐averaged effective doses will be reduced compared to point dose equivalent estimates because a large portion of the neutron point dose is due to low‐energy neutrons with energies <1 MeV, which do not penetrate efficiently to deep‐seated tissues. However the exposures from neutrons to humans on Mars should become an important consideration in radiobiology research and risk assessment.
Integrity signals
Registry
Cites
Statistics
Claims the paper makes
4 of 32 cited sources checked · 2 supported · 0 flagged · accuracy not yet measured
- Findingcitation
The simulated total dose rates using Badhwar-O'Neill 2011 and HZETRN reproduce the observed variation of surface dose rate with changing heliospheric conditions and atmospheric pressure.
“reproduces the observed variation of surface dose rate with changing heliospheric conditions and atmospheric pressure [Rafkin et al., 2014].”
- Also stated in: § 8. Summary and Conclusion · plain
“with the simulations reproducing the observed variation of surface dose rate with changing heliospheric conditions and atmospheric pressure.”
Quote in the paperSubstantial claim1 of 1 sources checked- cites Rafkin et al., 2014 source
The Summary and Conclusion (page unavailable) reports that measured surface dose rates vary with atmospheric pressure and that this effect is qualitatively consistent with scaled model results. The Data Analysis section also identifies heliospheric variability as a signal in the dose measurements. But the paper does not show that total-dose simulations using Badhwar–O’Neill 2011 and HZETRN reproduce the observed variation under both changing heliospheric conditions and atmospheric pressure. (LLM, conf=0.85)
Experimental — accuracy not yet measured
- Also stated in: § 8. Summary and Conclusion · plain
- Findingown data
The simulation reproduces the observed variation of surface dose rate with changing heliospheric conditions and atmospheric pressure.
“Simulation of average dose rate is in good agreement with RAD measurements for the first 200 sols and reproduces the observed variation of surface dose rate with changing heliospheric conditions and atmospheric pressure.”
Quote in the paperSubstantial claim- Rests on an assumption: The shielding by other RAD components (three Si detectors and two thin windows) is negligible compared to the shielding provided by the atmosphere and other detectors.
- Findingown data
Simulation of average dose rate is in good agreement with RAD measurements for the first 200 sols.
“Simulation of average dose rate is in good agreement with RAD measurements for the first 200 sols and reproduces the observed variation of surface dose rate with changing heliospheric conditions and atmospheric pressure.”
Quote in the paperSubstantial claim- Rests on an assumption: The shielding by other RAD components (three Si detectors and two thin windows) is negligible compared to the shielding provided by the atmosphere and other detectors.
- Findingown data
Average contributions of albedo particles (charge number Z < 3) from Martian regolith comprise about 42% of the average daily dose equivalent.
“It also suggests that the average contributions of albedo particles (charge number Z < 3) from Martian regolith comprise about 10% and 42% of the average daily point dose and dose equivalent, respectively.”
Quote in the paperSubstantial claim- Rests on an assumption: The shielding by other RAD components (three Si detectors and two thin windows) is negligible compared to the shielding provided by the atmosphere and other detectors.
- Findingreasoning
Model results agree less well between sols 200 and 300.
“Model results agree less well between sols 200 and 300 due to subtleties in the changing heliospheric conditions.”
- Also stated in: § 7. Dose and Dose Equivalent on Martian Surface · plain
“model results agree less well between sols 200 and 300”
Quote in the paperSubstantial claim- Rests on an assumption: The shielding by other RAD components (three Si detectors and two thin windows) is negligible compared to the shielding provided by the atmosphere and other detectors.
- Also stated in: § 7. Dose and Dose Equivalent on Martian Surface · plain
- Findingown data
Average contributions of albedo particles (charge number Z < 3) from Martian regolith comprise about 10% of the average daily point dose.
“It also suggests that the average contributions of albedo particles (charge number Z < 3) from Martian regolith comprise about 10% and 42% of the average daily point dose and dose equivalent, respectively.”
Quote in the paperNot a substantial claim- Rests on an assumption: The shielding by other RAD components (three Si detectors and two thin windows) is negligible compared to the shielding provided by the atmosphere and other detectors.
- Findingreasoning
As heliospheric condition changes from solar maximum to solar minimum, the relative contribution of albedo particles to the total dose and the dose equivalent increases regardless of atmospheric depth.
“As heliospheric condition changes from solar maximum to solar minimum, the relative contribution of albedo particles to the total dose and the dose equivalent increases regardless of atmospheric depth.”
Quote in the paperSubstantial claim - Findingown data
Without any atmospheric shielding, albedo neutrons contribute 2% of total point dose.
“Without any atmospheric shielding, the albedo neutrons contribute 2% and 8% of total point dose and total point-dose equivalent, respectively.”
Quote in the paperNot a substantial claim- Rests on an assumption: The shielding by other RAD components (three Si detectors and two thin windows) is negligible compared to the shielding provided by the atmosphere and other detectors.
- Findingown data
The RAD data and model calculations for the average daily dose rate are in good agreement.
“The RAD data and model calculations for the average daily dose rate are in good agreement.”
Quote in the paperSubstantial claim - Findingown data
The simulated total dose rates using Badhwar-O'Neill 2011 and HZETRN agree on average to within ±15% with the RAD measurements.
“The simulated total dose rates using Badhwar-O'Neill 2011 and HZETRN agrees on average to within ±15% with the RAD measurements”
- Also stated in: § 8. Summary and Conclusion · plain
“The resultant time series of dose rate simulation compared to the RAD measurement show relatively good agreement”
- Also stated in: § 8. Summary and Conclusion · plain
“The comparison here of the NASA computational models with the RAD data shows relatively good agreement in terms of total dose rate measurements.”
Quote in the paperSubstantial claim - Also stated in: § 8. Summary and Conclusion · plain
- Findingnone given
The average quality factor <Q> is predicted to be about 2.3 for the downward GCR and associated secondaries.
“The average quality factor, <Q> is predicted to be about 2.3 for the downward GCR and associated secondaries.”
Quote in the paperNot a substantial claim - Findingown data
Contributions of backscattered neutrons and light ions to dose increase to 10% for CO2 shielding depths between 50 and 150 g/cm2.
“The contributions of backscattered neutrons and light ions to dose and dose equivalent increase to 10% and 45%, respectively, for CO 2 shielding depths between 50 and 150 g/cm 2 and then decrease beyond those depths.”
Quote in the paperNot a substantial claim- Rests on an assumption: The shielding by other RAD components (three Si detectors and two thin windows) is negligible compared to the shielding provided by the atmosphere and other detectors.
- Findingown data
Contributions of backscattered neutrons and light ions to dose and dose equivalent decrease beyond CO2 shielding depths of 150 g/cm2.
“The contributions of backscattered neutrons and light ions to dose and dose equivalent increase to 10% and 45%, respectively, for CO 2 shielding depths between 50 and 150 g/cm 2 and then decrease beyond those depths.”
Quote in the paperNot a substantial claim- Rests on an assumption: The shielding by other RAD components (three Si detectors and two thin windows) is negligible compared to the shielding provided by the atmosphere and other detectors.
- Findingown data
The largest contribution to backscattered dose is from albedo neutrons.
“Here, the largest contribution is from albedo neutrons.”
Quote in the paperNot a substantial claim- Rests on an assumption: The shielding by other RAD components (three Si detectors and two thin windows) is negligible compared to the shielding provided by the atmosphere and other detectors.
- Findingnone given
The RAD data and model calculations for the average daily dose rate are in relatively good agreement for the first 200 sols.
“The RAD data and model calculations for the average daily dose rate are in relatively good agreement for the first 200 sols.”
Quote in the paperSubstantial claim - Findingnone given
The remaining contribution to backscattered dose is from protons and helium ions.
“The remaining contribution to the backscattered dose is from protons and helium ions, but contributions to dose equivalent are largely from backscattered helium ions.”
Quote in the paperNot a substantial claim- Rests on an assumption: The shielding by other RAD components (three Si detectors and two thin windows) is negligible compared to the shielding provided by the atmosphere and other detectors.
- Findingown data
Contributions of backscattered neutrons and light ions to dose equivalent increase to 45% for CO2 shielding depths between 50 and 150 g/cm2.
“The contributions of backscattered neutrons and light ions to dose and dose equivalent increase to 10% and 45%, respectively, for CO 2 shielding depths between 50 and 150 g/cm 2 and then decrease beyond those depths.”
Quote in the paperNot a substantial claim- Rests on an assumption: The shielding by other RAD components (three Si detectors and two thin windows) is negligible compared to the shielding provided by the atmosphere and other detectors.
- Findingown data
Without any atmospheric shielding, albedo neutrons contribute 8% of total point-dose equivalent.
“Without any atmospheric shielding, the albedo neutrons contribute 2% and 8% of total point dose and total point-dose equivalent, respectively.”
Quote in the paperNot a substantial claim- Rests on an assumption: The shielding by other RAD components (three Si detectors and two thin windows) is negligible compared to the shielding provided by the atmosphere and other detectors.
- Findingreasoning
Inclusion of the albedo contribution increases the average quality factor to 3.5.
“inclusion of this contribution increases the average quality factor to 3.5.”
Quote in the paperNot a substantial claim - Findingreasoning
Above 150 g/cm2, the albedo contributions decline.
“Above 150 g/cm 2 , the albedo contributions decline due to the decreasing rate of production of new particles beyond this depth.”
Quote in the paperNot a substantial claim - Findingcitation
On the Mars surface, during ~300 sol period near the maximum of solar cycle 24, the average total GCR dose rate at Gale Crater was 0.21 ± 0.01 mGy/sol from the simulation, compared to 0.21 ± 0.05 mGy/sol by the RAD measurement using the E-detector.
“On the Mars surface, during ~300 sol period near the maximum of solar cycle 24, an average total GCR dose rate at Gale Crater (À4.4 km Mars orbital laser altimeter) was found to be 0.21 ± 0.01 mGy/sol from the simulation, compared to 0.21 ± 0.05 mGy/sol by the RAD measurement using the E-detector [Hassler et al., 2014].”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Hassler et al., 2014 source
- Findingnone given
Contributions to dose equivalent are largely from backscattered helium ions.
“The remaining contribution to the backscattered dose is from protons and helium ions, but contributions to dose equivalent are largely from backscattered helium ions.”
Quote in the paperNot a substantial claim- Rests on an assumption: The shielding by other RAD components (three Si detectors and two thin windows) is negligible compared to the shielding provided by the atmosphere and other detectors.
- Findingcitation
The average quality factor <Q> on the Martian surface was estimated as 3.5 ± 0.02 from the simulation, compared to 3.05 ± 0.3 by the RAD measurement.
“The average quality factor <Q> on the Martian surface was estimated as 3.5 ± 0.02 from the simulation, compared to 3.05 ± 0.3 by the RAD measurement [Hassler et al., 2014].”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Hassler et al., 2014 source
- Interpretationnone given
The less good agreement between sols 200 and 300 is due to subtleties in the changing heliospheric conditions.
“Model results agree less well between sols 200 and 300 due to subtleties in the changing heliospheric conditions.”
Quote in the paperSubstantial claim - Premisecitation
Low-energy neutrons with energies <1 MeV do not penetrate efficiently to deep-seated tissues.
“which do not penetrate efficiently to deep-seated tissues.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites ICRP, 2013
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationcitation
The estimates here of neutron contributions to point dose equivalents of more than 40% likely over-estimate the neutron contributions to effective dose equivalents or risks because of the large contributions from neutrons with energies below 1 MeV, which do not penetrate efficiently to deep-seated tissues.
“The estimates here of neutrons contributions to point dose equivalents of more than 40% likely over-estimate the neutron contributions to effective dose equivalents or risks because of the large contributions from neutrons with energies below 1 MeV, which do not penetrate efficiently to deep-seated tissues [ICRP, 2013].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites ICRP, 2013
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisecitation
The addition of tissue shielding will greatly reduce low-energy (<1 MeV) neutron contributions to tissue averaged doses or effective dose equivalents.
“the addition of tissue shielding will greatly reduce low-energy (<1 MeV) neutron contributions to tissue averaged doses or effective dose equivalents [ICRP, 2013].”
Quote in the paperSubstantial claim0 of 1 sources checked- cites ICRP, 2013
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationreasoning
The increase in relative albedo contribution from solar maximum to solar minimum occurs because GCR energy spectra at solar minimum are populated at low energies compared to solar maximum, and a larger share of primary GCRs fail to penetrate the atmosphere.
“This is because the GCR energy spectra at solar minimum are populated at low energies compared to solar maximum, and a larger share of primary GCRs fail to penetrate the atmosphere.”
Quote in the paperSubstantial claim - Interpretationreasoning
The decline in albedo contributions above 150 g/cm2 is due to the decreasing rate of production of new particles beyond this depth.
“Above 150 g/cm 2 , the albedo contributions decline due to the decreasing rate of production of new particles beyond this depth.”
Quote in the paperNot a substantial claim - Interpretationcitation
Calculations made here for point doses, which are defined as without tissue shielding, will overestimate the percent contribution of neutrons to tissue averaged doses or effective dose equivalent.
“The calculations made here for point doses, which are defined as without tissue shielding, will overestimate the percent contribution of neutrons to tissue averaged doses or effective dose equivalent”
Quote in the paperSubstantial claim- Rests on an assumption: The shielding by other RAD components (three Si detectors and two thin windows) is negligible compared to the shielding provided by the atmosphere and other detectors.
- Premisecitation
Since Curiosity's landing, the RAD has been measuring the energetic particle radiation environment on the surface of Mars with roughly 30 min cadence.
“Since Curiosity's landing, the RAD has been measuring the energetic particle radiation environment [Hassler et al., 2012[Hassler et al., , 2014] ] on the surface of Mars with roughly 30 min cadence.”
Quote in the paperSubstantial claim0 of 2 sources checked - Premisecitation
The Badhwar-O'Neill model accurately accounts for solar modulation of each element from hydrogen to nickel by propagating the local interstellar spectrum of each element through the heliosphere.
“This model accurately accounts for solar modulation of each element (from hydrogen to nickel) by propagating the local interstellar spectrum (LIS) of each element through the heliosphere by solving the Fokker-Planck diffusion, convection, and energy loss boundary value problem.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Badhwar and O'Neill, 1992 source
- Interpretationreasoning
The comparisons made possible by the RAD instrument so far improve confidence in the application of the NSCR-2012 model for mission design considerations.
“The NSCR-2012 incorporates the computational models used herein and the comparisons made possible by the RAD instrument so far improve confidence in the application of the NSCR-2012 model for mission design considerations.”
Quote in the paperSubstantial claim- Rests on an assumption: NSCR-2012 incorporates the computational models used herein.
- Interpretationreasoning
The larger value of <Q> predicted by the simulation is likely due to the fact that RAD E-detector is insensitive to neutrons with energies below about 5 MeV.
“The larger value of <Q> predicted by the simulation is likely due to the fact that RAD E-detector is insensitive to neutrons with energies below about 5 MeV.”
Quote in the paperSubstantial claim- Rests on an assumption: RAD E-detector is insensitive to neutrons with energies below about 5 MeV.
- Premisecitation
Backscattered neutrons and other light particles from the Martian regolith contribute significantly along with the GCR components.
“Backscattered neutrons and other light particles from the Martian regolith contribute significantly along with the GCR components [Wilson et al., 2004].”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Wilson et al., 2004 source
- Classified as probably not a substantial claim. 20
- May combine two claims. 7
Probably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationThe recent solar minimum is by far the deepest minimum since space-based measurements began.
“which is by far the deepest minimum since space-based measurements began [Mewaldt et al., 2010].”
Quote in the paperNot a substantial claim1 of 1 sources checked- cites Mewaldt et al., 2010 source
The Introduction describes the 2008–2010 minimum as prolonged, with unusually weak magnetic fields, and the Summary reports record cosmic-ray intensities relative to earlier space-era minima. The paper does not establish that the solar minimum itself was “by far the deepest” since space-based measurements began; its record-setting comparison concerns cosmic-ray intensities. (LLM, conf=0.84)
Experimental — accuracy not yet measured
May combine two claims.
PremisecitationThe atmosphere of Mars attenuates the intensity of the heavy ion component of the primary GCR but increases the fluence of secondary particles (neutrons, and hydrogen and helium isotopes) because of particle production processes in nuclear interactions.
“The atmosphere of Mars attenuates the intensity of the heavy ion component of the primary GCR but increases the fluence of secondary particles (neutrons, and hydrogen and helium isotopes) because of particle production processes in nuclear interactions [Cucinotta et al., 2007].”
Quote in the paperSubstantial claim1 of 1 sources checked- cites Cucinotta et al., 2007 source
Probably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationThe QMSFRG model is shown to be in excellent agreement with available experimental data for nuclear fragmentation cross sections.
“The QMSFRG model is shown to be in excellent agreement with available experimental data for nuclear fragmentation cross sections [Cucinotta et al., 2007].”
Quote in the paperNot a substantial claim1 of 1 sources checked- cites Cucinotta et al., 2007 source
May combine two claims.
FindingcitationThe resultant average GCR dose equivalent rate on the Mars surface is 0.72 ± 0.02 mSv/sol from the simulation, compared to 0.66 ± 0.10 mSv/sol from combining the tissue dose-rate measurement with <Q> measurement by the RAD.
“The resultant average GCR dose equivalent rate on the Mars surface is 0.72 ± 0.02 mSv/sol from the simulation, compared to 0.66 ± 0.10 mSv/sol from combining the tissue dose-rate measurement with <Q> measurement by the RAD [Hassler et al., 2014].”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Hassler et al., 2014 source
May combine two claims.
Findingnone givenThe albedo contributions peak at atmospheric depths between 50 and 150 g/cm2 and are nearly constant in that range.
“atmospheric depths between 50 and 150 g/cm 2 , and are nearly constant in that range.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingnone givenThe mean values of the albedo contribution at the RAD detector comprise 10% of the dose and 42% of the dose equivalent.
“values of the albedo contribution at the RAD detector comprise 10% of the dose and 42% of the dose equivalent”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationLarge health risks from space radiation are a limitation to the number of days astronauts could be exposed to galactic cosmic rays for interplanetary missions.
“The large health risks from space radiation are a limitation to the number of days astronauts could be exposed to galactic cosmic rays (GCR) for interplanetary missions”
Quote in the paperNot a substantial claim0 of 2 sources checked- cites Cucinotta et al., 2013a
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites Cucinotta et al., 2013b
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 conductnone givenIn the current simulation, any effects of the GCR dose rate due to short-term heliospheric structure variability due to solar activity and rotation are not included.
“In the current simulation, any effects of the GCR dose rate due to short-term heliospheric structure variability due to solar activity and rotation are not included.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationParker [1965] showed that the steady-state, spherically symmetric Fokker-Planck equation accurately accounts for diffusion, convection, and adiabatic deceleration of these particles.
“Parker [1965] showed that the steady-state, spherically symmetric Fokker-Planck equation accurately accounts for diffusion, convection, and adiabatic deceleration of these particles.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Parker, 1965 source
Probably not a substantial claim: may not pass S3 (load-bearing).
Interpretationnone givenSuch gamma rays increase absorbed doses by a few percent.
“but such gamma rays increase absorbed doses by a few percent and should be investigated.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Study design and conductnone givenNeutrons produced in the rover have not been included in the calculation.
“Also, the contributions of neutrons produced in the rover have not been included at this time.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
InterpretationreasoningThe less good agreement between sols 200 and 300 is thought to be due to subtleties in the changing heliospheric conditions which are not adequately modeled using the modulation parameter (Φ).
“which is thought to be due to subtleties in the changing heliospheric conditions which are not adequately modeled using the modulation parameter (Φ).”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationThe most recent model BO'11 utilizes a large number of GCR measurements from 1955 to 2012, spanning solar cycle 19 to 24 including the recent solar minimum.
“The most recent model of BO'11 [O'Neill and Foster, 2013] utilizes a large number of GCR measurements from 1955 to 2012, spanning solar cycle 19 to 24 including the recent solar minimum”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites O'Neill and Foster, 2013
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 conductnone givenParticles produced in the shielding provided by the rover and by those components in the geometry of the RAD instrument were not modeled.
“We have not modeled particles produced in the shielding provided by the rover and by those components in the geometry of the RAD instrument, which should be considerations for future investigations.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationAtmospheric pressure has been measured by the MSL Rover Environmental Monitoring Station (REMS).
“The atmospheric pressure has been measured by the MSL Rover Environmental Monitoring Station (REMS) [Gómez-Elvira et al., 2012].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Gómez-Elvira et al., 2012
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).
PremisecitationBadhwar and O'Neill [1992] developed a self-consistent solution to the Fokker-Plank equation for particle transport in the heliosphere that has been fit to available GCR data.
“Badhwar and O'Neill [1992] developed a self-consistent solution to the Fokker-Plank equation for particle transport in the heliosphere that has been fit to available GCR”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Badhwar and O'Neill, 1992 source
May combine two claims.
InterpretationreasoningHigh-energy, highly penetrating particles that generate albedo particles are largely unaffected by changing heliospheric conditions, so their contribution remains nearly constant.
“The high-energy, highly penetrating particles that generate albedo particles are largely unaffected by the changing heliospheric conditions; hence, their contribution remains nearly constant.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationThe intensity of the GCR flux varies over the approximately 11 year solar cycle due to changes in the interplanetary plasma that originates in the expanding solar corona.
“The intensity of the GCR flux varies over the approximately 11 year solar cycle due to changes in the interplanetary plasma that originates in the expanding solar corona [Babcock, 1961;Badhwar and O'Neill, 1992].”
Quote in the paperNot a substantial claim0 of 2 sources checkedMay combine two claims.
InterpretationcitationThe present results provide the first step in validating accurate estimates of organ dose, and the resultant biological risks can be made to evaluate radiation shielding requirements for varying space scenarios using the NSCR-2012 model.
“The present results provide the first step in validating accurate estimates of organ dose, and the resultant biological risks can be made to evaluate radiation shielding requirements for varying space scenarios using the NASA's space radiation evaluation tool, the NSCR-2012 model [Cucinotta et al., 2013a[Cucinotta et al., , 2013b]].”
Quote in the paperSubstantial claim0 of 2 sources checked- cites Cucinotta et al., 2013a
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites Cucinotta et al., 2013b
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).
PremisecitationInter-comparisons of some radiation transport codes using matched configurations and environments have showed very good agreement.
“Inter-comparisons of some radiation transport codes using matched configurations and environments have showed very good agreement [Heinbockel et al., 2011a[Heinbockel et al., , 2011b]].”
Quote in the paperNot a substantial claim0 of 2 sources checked- cites Heinbockel et al., 2011a
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites Heinbockel et al., 2011b
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Classified as probably not a substantial claim.
PremisecitationThe solar modulation parameter has been derived directly from the sunspot number, with propagation delay taken into account, to determine the modulated GCR flux.
“The solar modulation parameter has been derived directly from the sunspot number, with propagation delay taken into account, to determine the modulated GCR flux [O'Neill and Foster, 2013].”
Quote in the paperSubstantial claim0 of 1 sources checked- cites O'Neill and Foster, 2013
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 conductnone givenDose contributions from gamma rays produced by albedo neutrons have not been estimated.
“Dose contributions from gamma rays produced by albedo neutrons have not been estimated.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationPrevious comparisons of transport models to dosimetry measurements show agreement to within ±15% for dose and dose equivalent on the International Space Station or in transit to Mars.
“Previous comparisons of transport models to dosimetry measurements show agreement to within ±15% for dose and dose equivalent on the International Space Station [Cucinotta et al., 2008] or in transit to Mars [Zeitlin et al., 2013].”
Quote in the paperNot a substantial claim0 of 2 sources checkedClassified as probably not a substantial claim. May combine two claims.
PremisecitationRadiation transport codes have been validated by extensive comparisons to measurements, and they have been combined with detailed descriptions of the space environment to enable accurate simulations behind spacecraft shielding or on planetary surfaces.
“radiation transport codes have been validated by extensive comparisons to measurements, and they have been combined with detailed descriptions of the space environment to enable accurate simulations behind spacecraft shielding or on planetary surfaces [Cucinotta et al., 2011;Kim et al., 2012].”
Quote in the paperSubstantial claim0 of 2 sources checkedProbably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationSunspot number is well correlated with many observable quantities to indicate the temporal variation of solar modulation of GCR.
“sunspot number is well correlated with many observable quantities to indicate the temporal variation of solar modulation of GCR [Kim et al., 2006].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Kim et al., 2006 source
Probably not a substantial claim: may not pass S3 (load-bearing).
InterpretationreasoningGamma ray contribution to dose equivalent is likely to be small because of their low quality factors.
“Their contribution to dose equivalent is likely to be small because of their low quality factors”
Quote in the paperNot a substantial claim
The paper relies on this without support.
The shielding by other RAD components (three Si detectors and two thin windows) is negligible compared to the shielding provided by the atmosphere and other detectors.
“The shielding by other components, including three 300 micron thick Si detectors, and two very thin windows is not modeled; these pieces are negligible compared to the shielding provided by the atmosphere and other detectors.”
The paper relies on this without support.
No comparisons of radiation models to Martian surface measurements were possible prior to Curiosity's landing.
“no comparisons were possible prior to the successful landing of Curiosity on Mars.”
The paper relies on this without support.
RAD E-detector is insensitive to neutrons with energies below about 5 MeV.
“RAD E-detector is insensitive to neutrons with energies below about 5 MeV.”
The paper relies on this without support.
NSCR-2012 incorporates the computational models used herein.
“The NSCR-2012 incorporates the computational models used herein”
Cites
The passage of energetic charged particles through interplanetary space
Parker, E. N. (1965) · Planetary and Space Science · doi:10.1016/0032-0633(65)90131-5 · Cited by 1,607 · see citing works
The Topology of the Sun's Magnetic Field and the 22-YEAR Cycle.
Babcock, H. W. (1961) · The Astrophysical Journal · doi:10.1086/147060 · Cited by 1,479 · see citing works
Mars' surface radiation environment measured with the Mars Science Laboratory's Curiosity rover
Hassler, D. M., Zeitlin, C., Wimmer-Schweingruber, R. F., Ehresmann, B., Rafkin, S., Eigenbrode, J. L., Brinza, D. E., Weigle, G., Böttcher, S., Böhm, E., et al. (2014) · Science · doi:10.1126/science.1244797 · Cited by 690 · cited 10× · see citing works
“…rate enhancement from onemoderately hard Solar Energetic Particle event on sol 242 (12–13 April 2013), and several dose rate decreases from Forbush decreases [Cane, 2000] resulting from soft event-related interplanetary coronal mass ejections on sols 50, 97, 208, and 259 [Hassler et al., 2014].”
BackgroundMethodInfluentialSelf-citationCREME96: A Revision of the Cosmic Ray Effects on Micro-Electronics Code
Tylka, A. J., Adams, J. H., Boberg, P. R., Brownstein, B., Dietrich, W. F., Flueckiger, E. O., Petersen, E. L., Shea, M. A., Smart, D. F., & Smith, E. C. (1997) · IEEE Transactions on Nuclear Science · doi:10.1109/23.659030 · Cited by 643 · see citing works
Measurements of energetic particle radiation in transit to Mars on the Mars Science Laboratory
Zeitlin, C., Hassler, D. M., Cucinotta, F. A., Ehresmann, B., Wimmer-Schweingruber, R. F., Brinza, D. E., Kang, S., Weigle, G., Böttcher, S., Böhm, E., et al. (2013) · Science · doi:10.1126/science.1235989 · Cited by 641 · see citing works
Self-citationCoronal Mass Ejections and Forbush Decreases
Cane, H. V. (2000) · Space Science Reviews · doi:10.1023/a:1026532125747 · Cited by 491 · see citing works
REMS: The Environmental Sensor Suite for the Mars Science Laboratory Rover
Gómez‐Elvira, J., Armiens, C., Castañer, L., Domínguez-Pumar, M., Genzer, M., Gómez, F., Haberle, R. M., Harri, A., Jimenez, V., Kahanpää, H., et al. (2012) · Space Science Reviews · doi:10.1007/s11214-012-9921-1 · Cited by 310 · see citing works
Self-citationCoronal Mass Ejections and Forbush Decreases
Cane, H. V. (2000) · Space Sciences Series of ISSI · doi:10.1007/978-94-017-1187-6_4 · Cited by 292 · see citing works
How Safe Is Safe Enough? Radiation Risk for a Human Mission to Mars
Cucinotta, F. A., Kim, M.-H. Y., Chappell, L. J., & Huff, J. L. (2013) · PLoS ONE · doi:10.1371/journal.pone.0074988 · Cited by 250 · see citing works
Self-citationThe Radiation Assessment Detector (RAD) Investigation
Hassler, D. M., Zeitlin, C., Wimmer-Schweingruber, R. F., Böttcher, S., Martin, C., Andrews, J., Böhm, E., Brinza, D. E., Bullock, M. A., Burmeister, S., et al. (2012) · Space Science Reviews · doi:10.1007/s11214-012-9913-1 · Cited by 247 · see citing works
Self-citationICRP Publication 123: Assessment of Radiation Exposure of Astronauts in Space
Dietze, G., Bartlett, D. T., Cool, D. A., Cucinotta, F. A., Jia, X., McAulay, I. R., Pelliccioni, M., Petrov, V., Reitz, G., & Sato, T. (2013) · Annals of the ICRP · doi:10.1016/j.icrp.2013.05.004 · Cited by 239 · see citing works
Self-citationSpace Radiation Cancer Risk Projections and Uncertainties – 2012
Cucinotta, F. A., Y.Kim, M.-H., & Chappell, L. J. (2013) · NASA · doi:10.13140/rg.2.1.1413.3528 · Cited by 218 · see citing works
Self-citationPhysical and biological organ dosimetry analysis for international space station astronauts
Cucinotta, F. A., Kim, M.-H. Y., Willingham, V., & George, K. A. (2008) · Radiation Research · doi:10.1667/rr1330.1 · Cited by 196 · cited 1× · see citing works
“Previous comparisons of transport models to dosimetry measurements show agreement to within ±15% for dose and dose equivalent on the International Space Station [Cucinotta et al., 2008] or in transit to Mars [Zeitlin et al., 2013].”
ResultSelf-citationRECORD-SETTING COSMIC-RAY INTENSITIES IN 2009 AND 2010
Mewaldt, R. A., Davis, A. J., Lave, K. A., Leske, R. A., Stone, E. C., Wiedenbeck, M. E., Binns, W. R., Christian, E. R., Cummings, A. C., de Nolfo, G. A., et al. (2010) · The Astrophysical Journal · doi:10.1088/2041-8205/723/1/l1 · Cited by 178 · see citing works
Badhwar–O'Neill 2010 Galactic Cosmic Ray Flux Model—Revised
O'Neill, P. M. (2010) · IEEE Transactions on Nuclear Science · doi:10.1109/tns.2010.2083688 · Cited by 167 · see citing works
An improved model of galactic cosmic radiation for space exploration missions
Badhwar, G. D., & O'Neill, P. M. (1992) · International Journal of Radiation Applications and Instrumentation. Part D. Nuclear Tracks and Radiation Measurements · doi:10.1016/1359-0189(92)90024-p · Cited by 149 · see citing works
MCNPX benchmark for cosmic ray interactions with the Moon
McKinney, G. W., Lawrence, D. J., Prettyman, T. H., Elphic, R. C., Feldman, W. C., & Hagerty, J. J. (2006) · Journal of Geophysical Research Atmospheres · doi:10.1029/2005je002551 · Cited by 116 · see citing works
The physics of the FLUKA code: Recent developments
Ballarini, F., Battistoni, G., Brugger, M., Campanella, M., Carboni, M., Cerutti, F. M., Empl, A., Fasso, A., FERRARI, A., Gadioli, E., et al. (2007) · Advances in Space Research · doi:10.1016/j.asr.2007.05.031 · Cited by 81 · see citing works
Coupled neutron transport for HZETRN
Slaba, T. C., Blattnig, S. R., Aghara, S. K., Townsend, L. W., Handler, T., Gabriel, T. A., Pinsky, L. S., & Reddell, B. (2010) · Radiation Measurements · doi:10.1016/j.radmeas.2010.01.005 · Cited by 80 · see citing works
Rafkin, S. C. R., Zeitlin, C., Ehresmann, B., Hassler, D., Guo, J., Köhler, J., Wimmer‐Schweingruber, R., Gomez‐Elvira, J., Harri, A., Kahanpää, H., et al. (2014) · Journal of Geophysical Research: Planets · doi:10.1002/2013je004525 · Cited by 56 · see citing works
Self-citationNuclear interactions in heavy ion transport and event-based risk models
Cucinotta, F. A., Plante, I., Ponomarev, A. L., & Kim, M.-H. Y. (2011) · Radiation Protection Dosimetry · doi:10.1093/rpd/ncq512 · Cited by 52 · see citing works
Self-citationNUCFRG3: Light ion improvements to the nuclear fragmentation model
Adamczyk, A. M., Norman, R. B., Sriprisan, S., Townsend, L. W., Norbury, J. W., Blattnig, S. R., & Slaba, T. C. (2012) · Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment · doi:10.1016/j.nima.2012.02.021 · Cited by 46 · see citing works
Slaba, T. C., Blattnig, S. R., Reddell, B., Bahadori, A., Norman, R. B., & Badavi, F. F. (2013) · Advances in Space Research · doi:10.1016/j.asr.2013.02.015 · Cited by 46 · see citing works
Galactic cosmic ray transport methods: Past, present, and future
Wilson, J. W., Townsend, L. W., Shinn, J. L., Cucinotta, F. A., Costen, R. C., Badavi, F. F., & Lamkin, S. L. (1994) · Advances in Space Research · doi:10.1016/0273-1177(94)90549-5 · Cited by 46 · see citing works
Self-citationComparison of the transport codes HZETRN, HETC and FLUKA for galactic cosmic rays
Heinbockel, J. H., Slaba, T. C., Tripathi, R. K., Blattnig, S. R., Norbury, J. W., Badavi, F. F., Townsend, L. W., Handler, T., Gabriel, T. A., Pinsky, L. S., et al. (2010) · Advances in Space Research · doi:10.1016/j.asr.2010.11.013 · Cited by 39 · see citing works
Monte Carlo analysis of pion contribution to absorbed dose from Galactic cosmic rays
Aghara, S., Blattnig, S. R., Norbury, J. W., & Singleterry, R. C. (2009) · Nuclear Instruments and Methods in Physics Research Section B Beam Interactions with Materials and Atoms · doi:10.1016/j.nimb.2009.01.136 · Cited by 37 · see citing works
Cucinotta, F. A., Kim, M.-H., Schneider, S. I., & Hassler, D. M. (2007) · Radiation and Environmental Biophysics · doi:10.1007/s00411-007-0099-y · Cited by 35 · see citing works
Self-citationComparison of the transport codes HZETRN, HETC and FLUKA for a solar particle event
Heinbockel, J. H., Slaba, T. C., Blattnig, S. R., Tripathi, R. K., Townsend, L. W., Handler, T., Gabriel, T. A., Pinsky, L. S., Reddell, B., Clowdsley, M. S., et al. (2010) · Advances in Space Research · doi:10.1016/j.asr.2010.11.012 · Cited by 35 · see citing works
Sato, T., Endo, A., & Niita, K. (2010) · Physics in Medicine and Biology · doi:10.1088/0031-9155/55/8/008 · Cited by 34 · see citing works
Badhwar - O'Neill 2014 Galactic Cosmic Ray Flux Model Description
O'Neill, P. M. (2015) · NASA Technical Reports Server (NASA) · Cited by 32 · see citing works
Ныммик, Р. А. (2000) · Advances in Space Research · doi:10.1016/s0273-1177(99)01242-9 · Cited by 27 · see citing works
A solar cycle statistical model for the projection of space radiation environment
Kim, M. Y., Wilson, J. W., & Cucinotta, F. A. (2006) · Advances in Space Research · doi:10.1016/j.asr.2004.11.036 · Cited by 25 · see citing works
Self-citationAbrasion-ablation model for neutron production in heavy ion collisions
Cucinotta, F. A., Wilson, J. W., & Townsend, L. W. (1997) · Nuclear Physics A · doi:10.1016/s0375-9474(97)00130-9 · Cited by 23 · see citing works
Self-citationSato, T., Endo, A., Sihver, L., & Niita, K. (2010) · Radiation and Environmental Biophysics · doi:10.1007/s00411-010-0330-0 · Cited by 20 · see citing works
The Radiation Assessment Detector (RAD) Investigation
Hassler, D. M., Zeitlin, C. J., Wimmer-Schweingruber, R. F., Böttcher, S. I., Martı́n, C., Andrews, J., Böhm, E., Brinza, D. E., Bullock, M. A., Burmeister, S., et al. (2012) · Springer eBooks · doi:10.1007/978-1-4614-6339-9_15 · Cited by 19 · see citing works
Self-citationREMS: The Environmental Sensor Suite for the Mars Science Laboratory Rover
Gómez‐Elvira, J., Armiens, C., Castañer, L., Domínguez-Pumar, M., Genzer, M., Gómez, F., Haberle, R. M., Harri, A., Jimenez, V., Kahanpää, H., et al. (2012) · Springer eBooks · doi:10.1007/978-1-4614-6339-9_17 · Cited by 19 · see citing works
Self-citationA space radiation transport method development
Wilson, J. W., Tripathi, R. K., Qualls, G. D., Cucinotta, F. A., Prael, R. E., Norbury, J. W., Heinbockel, J. H., & Tweed, J. (2004) · Advances in Space Research · doi:10.1016/j.asr.2003.10.048 · Cited by 14 · see citing works
Self-citationDescription of Transport Codes for Space Radiation Shielding
Kim, M.-H. Y., Wilson, J. W., & Cucinotta, F. A. (2012) · Health Physics · doi:10.1097/hp.0b013e318266732f · Cited by 8 · see citing works
Self-citation
Flagged first, then by citations
Cited by
Sorted by citations
Space radiation risks to the central nervous system
Cucinotta, F. A., Alp, M., Sulzman, F. M., & Wang, M. (2014) · Life Sciences in Space Research · doi:10.1016/j.lssr.2014.06.003 · Cited by 262 · see citing works
“, 2013a, 2013b) as shown in previous reports comparing to flight measurements (Cucinotta et al., 2008; Cucinotta et al., 2013a; Zeitlin et al., 2013; Kim et al., 2014).”
BackgroundResultSelf-citationCancer Risk of Low Dose Ionizing Radiation
Ali, Y. F., Cucinotta, F. A., Liu, N., & Zhou, G. (2020) · Frontiers in Physics · doi:10.3389/fphy.2020.00234 · Cited by 97 · see citing works
Self-citationThe Martian surface radiation environment – a comparison of models and MSL/RAD measurements
Matthiä, D., Ehresmann, B., Lohf, H., Köhler, J., Zeitlin, C., Appel, J., Sato, T., Slaba, T., Martin, C., Berger, T., et al. (2016) · Journal of Space Weather and Space Climate · doi:10.1051/swsc/2016008 · Cited by 91 · see citing works
“…the radiation exposure in interplanetary space during a cruise to Mars (e.g. McKenna-Lawlor et al. 2012b), in the atmosphere and on the surface of Mars (e.g. Simonsen et al. 1990; Townsend et al. 2011; Kim et al. 2014; Gronoff et al. 2015), few data are available on predicted particle spectra.”
BackgroundSelf-citationCucinotta, F. A., & Cacao, E. (2017) · Scientific Reports · doi:10.1038/s41598-017-02087-3 · Cited by 85 · see citing works
Self-citationMatthiä, D., Hassler, D. M., de Wet, W., Ehresmann, B., Firan, A., Flores-McLaughlin, J., Guo, J., Heilbronn, L. H., Lee, K., Ratliff, H., et al. (2017) · Life Sciences in Space Research · doi:10.1016/j.lssr.2017.06.003 · Cited by 75 · see citing works
Self-citationGuo, J., Zeitlin, C., Wimmer-Schweingruber, R. F., Hassler, D. M., Ehresmann, B., Rafkin, S., Freiherr von Forstner, J. L., Khaksarighiri, S., Liu, W., & Wang, Y. (2021) · The Astronomy and Astrophysics Review · doi:10.1007/s00159-021-00136-5 · Cited by 73 · see citing works
Self-citationSafe days in space with acceptable uncertainty from space radiation exposure
Cucinotta, F. A., Alp, M., Rowedder, B., & Kim, M.-H. Y. (2015) · Life Sciences in Space Research · doi:10.1016/j.lssr.2015.04.002 · Cited by 71 · see citing works
“These methods agree with spaceflight data in low Earth orbit, in transit to Mars and on the Mars surface to within 15% for dose and dose equivalent (Cucinotta et al., 2013a; Kim et al., 2014; ICRP, 2013).”
MethodSelf-citationSlaba, T. C., Blattnig, S. R., Norbury, J. W., Rusek, A., & Tessa, C. L. (2016) · Life Sciences in Space Research · doi:10.1016/j.lssr.2016.01.001 · Cited by 69 · see citing works
Kim, M.-H. Y., Rusek, A., & Cucinotta, F. A. (2015) · Frontiers in Oncology · doi:10.3389/fonc.2015.00122 · Cited by 61 · see citing works
“The HZETRN code has been compared to extensive flight measurements for dose and dose equivalent on space shuttle, ISS, and Mars transit and Mars surface measurements and generally agree with these measurements to within ±15% (9, 12, 13, 17).”
BackgroundMethodInfluentialSelf-citationRisks of cognitive detriments after low dose heavy ion and proton exposures
Cucinotta, F. A., & Cacao, E. (2019) · International Journal of Radiation Biology · doi:10.1080/09553002.2019.1623427 · Cited by 58 · see citing works
Self-citationPlanetary space weather: scientific aspects and future perspectives
Plainaki, C., Lilensten, J., Radioti, A., Andriopoulou, M., Milillo, A., Nordheim, T. A., Dandouras, I., Coustenis, A., Grassi, D., Mangano, V., et al. (2016) · Journal of Space Weather and Space Climate · doi:10.1051/swsc/2016024 · Cited by 55 · see citing works
“…in-situ measurements at the Martian surface by the RAD instrument (Hassler et al. 2012) on board the Mars Science Laboratory rover agree relatively well with the quiet-time GCR predictions made by these computational modelling efforts (Hassler et al. 2014; Kim et al. 2014; Gronoff et al. 2015).”
BackgroundMethodRisk of defeats in the central nervous system during deep space missions
Kokhan, V. S., Матвеева, М. И., Mukhametov, A., & Shtemberg, A. S. (2016) · Neuroscience & Biobehavioral Reviews · doi:10.1016/j.neubiorev.2016.10.006 · Cited by 46 · see citing works
Gronoff, G., Norman, R. B., & Mertens, C. J. (2015) · Advances in Space Research · doi:10.1016/j.asr.2015.01.028 · Cited by 42 · see citing works
Cacao, E., Hada, M., Saganti, P. B., George, K. A., & Cucinotta, F. A. (2016) · PLoS ONE · doi:10.1371/journal.pone.0153998 · Cited by 38 · see citing works
Self-citationA proposed change to astronaut exposures limits is a giant leap backwards for radiation protection
Cucinotta, F. A., Schimmerling, W., Blakely, E. A., & Hei, T. K. (2021) · Life Sciences in Space Research · doi:10.1016/j.lssr.2021.07.005 · Cited by 35 · see citing works
Self-citationSolar energetic particle warnings from a coronagraph
Cyr, O. C. S., Posner, A., & Burkepile, J. R. (2017) · Space Weather · doi:10.1002/2016sw001545 · Cited by 34 · see citing works
“…summary of the radiation risks in spaceflight and recommendations to address them were compiled by the National Research Council [2008], and many researchers have already been thinking about this hazard to human interplanetary space travel [e.g.,McKenna-Lawlor et al., 2012; Kim et al., 2014].”
BackgroundSelf-citationGuo, J., Guo, J., Dobynde, M. I., Wang, Y., & Wimmer-Schweingruber, R. F. (2022) · Journal of Geophysical Research Planets · doi:10.1029/2021je007157 · Cited by 30 · see citing works
Self-citationGalactic Cosmic-Ray Bombardment of Europa’s Surface
Nordheim, T. A., Jasinski, J. M., & Hand, K. P. (2019) · The Astrophysical Journal Letters · doi:10.3847/2041-8213/ab3661 · Cited by 26 · see citing works
The First Ground Level Enhancement Seen on Three Planetary Surfaces: Earth, Moon, and Mars
Guo, J., Li, X., Zhang, J., Dobynde, M. I., Wang, Y., Xu, Z., Berger, T., Semkova, J., Wimmer-Schweingruber, R. F., Hassler, D. M., et al. (2023) · Geophysical Research Letters · doi:10.1029/2023gl103069 · Cited by 24 · see citing works
“The interaction of particles with the lunar or martian environment has been studied via particle transport modeling through the planetary atmosphere and regolith (e.g., Banjac et al., 2018; Kim et al., 2014; Matthiä et al., 2016, 2017; Mesick et al., 2018; Naito et al., 2020).”
Self-citationCancer and circulatory disease risks for a human mission to Mars: Private mission considerations
Cucinotta, F. A., Cacao, E., Kim, M. Y., & Saganti, P. B. (2018) · Acta Astronautica · doi:10.1016/j.actaastro.2018.08.022 · Cited by 22 · see citing works
Self-citationMcKenna-Lawlor, S. M. P., Bhardwaj, A., Ferrari, F., Kuznetsov, N. V., Lal, A. K., Li, Y., Nagamatsu, A., Ныммик, Р. А., Panasyuk, M., Petrov, V., et al. (2014) · Acta Astronautica · doi:10.1016/j.actaastro.2014.11.009 · Cited by 21 · see citing works
Self-citationCucinotta, F. A. (2023) · Life Sciences in Space Research · doi:10.1016/j.lssr.2023.08.003 · Cited by 19 · see citing works
Self-citationBaqué, M., Dobrijévic, M., Postollec, A. L., et al. (2016) · International Journal of Astrobiology · doi:10.1017/s1473550415000555 · Cited by 16 · see citing works
“…of an actual mission to Mars as it was monitored by the Radiation Assessment Detector instrument on-board theMars science laboratory spacecraft on cruise to Mars and continue to be recorded by the rover Curiosity directly on its surface (Hassler et al. 2013; Zeitlin et al. 2013; Kim et al. 2014).”
MethodCucinotta, F. A., Cacao, E., Kim, M.-H. Y., & Saganti, P. B. (2020) · Life Sciences in Space Research · doi:10.1016/j.lssr.2020.07.008 · Cited by 16 · see citing works
Self-citationIkeda, H., Souda, H., Puspitasari, A., Held, K. D., Hidema, J., Nikawa, T., Yoshida, Y., Kanai, T., & Takahashi, A. (2016) · Biological Sciences in Space · doi:10.2187/bss.30.8 · Cited by 15 · see citing works
Directionality of the Martian Surface Radiation and Derivation of the Upward Albedo Radiation
Guo, J., Khaksarighiri, S., Wimmer‐Schweingruber, R. F., Hassler, D. M., Ehresmann, B., Zeitlin, C., Löffler, S., Matthiä, D., Berger, T., Reitz, G., et al. (2021) · Geophysical Research Letters · doi:10.1029/2021gl093912 · Cited by 14 · see citing works
Self-citationRace and ethnic group dependent space radiation cancer risk predictions
Cucinotta, F. A., & Saganti, P. B. (2022) · Scientific Reports · doi:10.1038/s41598-022-06105-x · Cited by 14 · see citing works
Self-citationZaman, M. A. A., & Kunja, L. A. (2023) · AIP Advances · doi:10.1063/5.0163306 · Cited by 14 · see citing works
Cucinotta, F. A., Cacao, E., Kim, M.-H. Y., & Saganti, P. B. (2019) · Radiation Protection Dosimetry · doi:10.1093/rpd/ncy264 · Cited by 12 · see citing works
Self-citationMars science laboratory radiation assessment detector (MSL/RAD) modeling workshop proceedings
Hassler, D. M., Norbury, J. W., & Reitz, G. (2017) · Life Sciences in Space Research · doi:10.1016/j.lssr.2017.06.004 · Cited by 11 · see citing works
Self-citationFlores-McLaughlin, J. (2017) · Life Sciences in Space Research · doi:10.1016/j.lssr.2017.07.007 · Cited by 11 · see citing works
Semkova, J., Benghin, V. V., Guo, J., Zhang, J., Pieve, F. D., Krastev, K., Matviichuk, Y. N., Tomov, B., Shurshakov, V., Drobyshev, S., et al. (2022) · Life Sciences in Space Research · doi:10.1016/j.lssr.2022.08.007 · Cited by 6 · see citing works
Self-citationCancer and circulatory disease risks for the largest solar particle events in the space age
Cucinotta, F. A., & Pak, S. (2023) · Life Sciences in Space Research · doi:10.1016/j.lssr.2023.10.003 · Cited by 5 · see citing works
Self-citationLiu, W. M., Guo, J., Zhang, J., & Semkova, J. (2023) · The Astrophysical Journal · doi:10.3847/1538-4357/acce3c · Cited by 5 · see citing works
Self-citationKim, M. Y., Blattnig, S. R., Clowdsley, M. C., & Norman, R. B. (2017) · Space Weather · doi:10.1002/2016sw001552 · Cited by 4 · see citing works
Self-citationCucinotta, F. A., & Saganti, P. B. (2023) · Life Sciences in Space Research · doi:10.1016/j.lssr.2023.09.001 · Cited by 3 · see citing works
Self-citationYoshida, K., Hada, M., Hayashi, M., Kizu, A., Kitada, K., Eguchi-Kasai, K., Kokubo, T., Teramura, T., Suzuki, H., Watanabe, H., et al. (2024) · International Journal of Molecular Sciences · doi:10.3390/ijms25063283 · Cited by 3 · see citing works
“…the biological effect that is calculated physical dose measurement, are about 0.5–0.62 mSv/day on the International Space Station (ISS) [11,12], 1.15 mSv/day on the surface of the moon of the Earth [13,14], 0.5 mSv/day on the surface of Mars [15], and 1.84 mSv/day during the flight from the Earth…”
BackgroundInfluentialSelf-citationRace and Ethnic Group Dependent Space Radiation Cancer Risk PredictionsPreprint
Cucinotta, F. A., & Saganti, P. B. (2021) · Research Square · doi:10.21203/rs.3.rs-871085/v1 · Cited by 1 · see citing works
Self-citationRace and Ethnic Group Dependent Space Radiation Cancer Risk PredictionsPreprint
Cucinotta, F. A., & Saganti, P. B. (2021) · medRxiv · doi:10.1101/2021.09.08.21263281 · Cited by 1 · see citing works
Self-citationThe ionizing radiation environment and shielding in pit craters and cave skylights on Mars
Millán, A. V., & Viúdez‐Moreiras, D. (2026) · Life Sciences in Space Research · doi:10.1016/j.lssr.2026.02.002
Non-DSB clustered damage is much more frequent than DSBs in galactic cosmic ray exposures
Cucinotta, F. A. (2026) · Life Sciences in Space Research · doi:10.1016/j.lssr.2026.02.009
Self-citationGuo, J., Tian, C., Charpentier, G., Wimmer-Schweingruber, R. F., Khaksarighiri, S., Pan, L., Löwe, J. L., Ehresmann, B., Hassler, D. M., Zeitlin, C. J., et al. (2026) · Journal of Geophysical Research Planets · doi:10.1029/2026je009704
“…radiation environment can be studied via particle transport modeling through the Martian atmosphere and surface (Charpentier et al., 2024; De Angelis et al., 2006; Gronoff et al., 2015; Guo et al., 2019; Keating et al., 2005; Kim et al., 2014; Saganti et al., 2004; Zhang et al., 2022, etc.).”
Self-citation
- Authors
- Kim, M. Y., Cucinotta, F. A., Nounu, H. N., Zeitlin, C., Hassler, D. M., Rafkin, S. C. R., Wimmer‐Schweingruber, R. F., Ehresmann, B., Brinza, D. E., Böttcher, S., Böhm, E., Burmeister, S., Guo, J., Köhler, J., Martin, C., Reitz, G., Posner, A., Gómez‐Elvira, J., Harri, A., & the MSL Science Team
- Affiliations
- Wyle (United States) (US)
- University of Nevada, Las Vegas (US)
- Southwest Research Institute (US)
- Christian Albrechts University Kiel Germany
- Jet Propulsion Laboratory (US)
- Christian-Albrechts-Universität zu Kiel (DE)
- Deutsches Zentrum für Luft- und Raumfahrt e. V. (DLR) (DE)
- National Aeronautics and Space Administration (US)
- Consejo Superior de Investigaciones Científicas (ES)
- Finnish Meteorological Institute (FI)
- Corresponding author
- Kim, Myung‐Hee Y.
- ORCID
- Venue
- Journal of Geophysical Research: Planets
- Publisher
- American Geophysical Union (AGU)
- Published
- 2014-06
- Volume
- 119
- Issue
- 6
- Pages
- 1311-1321
- ISSN
- 2169-9097 (ISSN-L)
- 2169-9100
- OpenAlex
- W2156168145
- Cited by
- 42
- References
- 35
- Citations by year
- 2026: 3 · 2024: 1 · 2023: 6 · 2022: 3 · 2021: 5 · 2020: 2 · 2019: 2 · 2018: 2 · 2017: 6 · 2016: 7 · 2015: 3 · 2014: 2
- FWCI
- 3.23
- Type
- journal article
- Language
- en
- Open access
- bronze
- doi.org
- Locations
- Journal of Geophysical Research Planets (publishedVersion)
- DIGITAL.CSIC (Spanish National Research Council (CSIC)) (submittedVersion)
- elib (German Aerospace Center) (submittedVersion)
- Funders
- National Aeronautics and Space Administration (50QM1201, 50QM0501, 1273039)
- California Institute of Technology
- Southwest Research Institute
- Deutsches Zentrum für Luft- und Raumfahrt (50QM0501, 50QM1201)
- Jet Propulsion Laboratory (1273039)
- Langley Research Center
- Johnson Space Center
- University of California, Los Angeles
- NASA Headquarters
- Human Exploration and Operations Mission Directorate
- Topics
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Planetary Science and Exploration
- Health Sciences › Medicine › Pulmonary and Respiratory Medicine › Radiation Therapy and Dosimetry
- Physical Sciences › Engineering › Electrical and Electronic Engineering › Radiation Effects in Electronics
- Keywords
- galactic cosmic rays, HZETRN, radiation dose rate, atmospheric pressure dependence, neutron dose, dose equivalent, nuclear fragmentation, Gale Crater, Curiosity rover, Martian regolith
About these checks
Registry, retraction, Cites and statistics results are computed, not judged, with one exception: a printed reference that no index lists is read once by a model before it counts as a citation error. Claims are extracted by a model and kept only when their quote appears verbatim in the text; each cited source is then checked, with a model’s help, for whether it says what the claim relies on. Those verdicts can be wrong — read the claim’s quote and the cited source before relying on one.
Claims read by deepseek-v4.1-flash under definition version 3 (extract-v3) on 2026-10-11.
Classified by jev-1.13-20260917 (gold-guideline-v0.2) on 2026-10-11.
Cited sources are checked by gpt-6-sol.
Statistics and arithmetic are recomputed, not judged.
Confidence bands are shown only for fields calibrated on our annotated test set. None is calibrated yet, so no band is shown.
What counts as a claim ›How we measure confidence ›How we check this ›
Are you an author, or do you see a problem with this page? Request a review