requirements for space radiation dosimetrywrmiss.org/workshops/fourth/schimmerling.pdf · • ions...
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Requirements for Space Radiation DosimetryWalter Schimmerling, Francis A. Cucinotta, and John W. Wilson
Workshop on Radiation Monitoring for theInternational Space Station
Farnborough, UK3-5 November 1999
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Primaries and SecondariesInside 5 g/cm2 of Aluminum (all energies)
Different BiologyDifferent BiologyDifferent BiologyDifferent BiologyDifferent Biology
Proton13%
Alpha24%
21 • Z • 2824%
11 • Z • 2022% 3 • Z • 10
17%
C3H10T1/2 Cell DeathProton35%
21 • Z • 2813%11 • Z • 20
16%
3 • Z • 1014% Alpha
22%
C3H10T1/2 Cell Transformation
Proton21%
Alpha19%
21 • Z • 2821%
11 • Z • 2024%
3 • Z • 1015%
Dose Equivalent to SkinProton32%
21 • Z • 2815%
11 • Z • 2015%
3 • Z • 1012%
Alpha26%
Harderian Gland
Different Biology
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3
Annual Dose Equivalent Behind 5 g/cm2 of Aluminum
(1977 Solar Minimum)
SKIN
BFOdH
/ d(
ln E
)
0
2
4
6
8
10
E, MeV/amu10 100 1000 104 105
105
E, MeV/amu
dH /
d(ln
E)
2
4
6
8
10 100 1000 104
10
0
10 100 103 104 105
E, MeV/amu
0
5
10
15
20
25
H(<
E)
(cS
v)
30
3 • Z • 10
3 • Z • 10
3 • Z • 10
3 • Z • 10
21 • Z • 28
21 • Z • 28
21 • Z • 28
21 • Z • 28
11 • Z • 20
11 • Z • 20
11 • Z • 20
11 • Z • 20
10 100 103 104 105
E, MeV/amu
0
5
10
15
20
25
H(<
E)
(cS
v)
30
Protons
ProtonsProton
ProtonAlpha
Alpha
AlphaAlphas
SKIN
BFOdH
/ d(
ln E
)
0
2
4
6
8
10
E, MeV/amu10 100 1000 104 105
105
E, MeV/amu
dH /
d(ln
E)
2
4
6
8
10 100 1000 104
10
0
10 100 103 104 105
E, MeV/amu
0
5
10
15
20
25
H(<
E)
(cS
v)
30
Alpha
3 • Z • 10
3 • Z • 10
3 • Z • 10
3 • Z • 10
21 • Z • 28
21 • Z • 28
21 • Z • 28
21 • Z • 28
11 • Z • 20
11 • Z • 20
11 • Z • 20
11 • Z • 20
10 100 103 104 105
E, MeV/amu
0
5
10
15
20
25
H(<
E)
(cS
v)
30
Protons
Proton
Proton
Proton
Proton
Alpha
Alpha
Alpha
Alpha
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LET vs. Range
Range, cm
LE
T, k
eV/µ
m
50 A
MeV
100
A M
eV
200
A M
eV
400
A M
eV
650
A M
eV80
0 A
MeV
1200
A M
eV
2000
A M
eV
0.1
1
10
100
1000
10000
0.1 1 10 100
IronChromiumArgon
Silicon
OxygenCarbon
Magnesium
Alpha
Proton
1000
max RBE
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5
Critical QuestionsRelated to Space Dosimetry
• Space Radiation Environment– For a given mission, what are the fluxes of GCR in interplanetary space as a
function of particle energy, LET, and solar cycle?– What is the solar cycle dependence of space radiation?– What is the trapped radiation flux as a function of time, magnetic field
coordinates and geographical coordinates?– What are the doses related to heavy ions in deep space?
• Nuclear Interactions– What are the yields for nuclear interactions of HZE particles in tissue and space
shielding materials?– How are radiation fields transformed as a function of depth in different space
materials?– What are the optimal ways of shielding humans in space?
• Atomic Interactions– What is the precise energy deposition of heavy ions?– What are the yields and energy spectra of electrons?
• Human Radiation Protection– What should be the radiation dose limits for manned deep space missions?– What is the risk associated with each crew member at any time during a given
mission?
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6
Critical QuestionsRelated to Space Dosimetry
• Space Radiation Environment– For a given mission, what are the fluxes of GCR in interplanetary space as a
function of particle energy, LET, and solar cycle?– What is the solar cycle dependence of space radiation?– What is the trapped radiation flux as a function of time, magnetic field
coordinates and geographical coordinates?– What are the doses related to heavy ions in deep space?
• Nuclear Interactions– What are the yields for nuclear interactions of HZE particles in tissue and space
shielding materials?– How are radiation fields transformed as a function of depth in different space
materials?– What are the optimal ways of shielding humans in space?
• Atomic Interactions– What is the precise energy deposition of heavy ions?– What are the yields and energy spectra of electrons?
• Human Radiation Protection– What should be the radiation dose limits for manned deep space missions?– What is the risk associated with each crew member at any time during a given
mission?
![Page 7: Requirements for Space Radiation Dosimetrywrmiss.org/workshops/fourth/schimmerling.pdf · • Ions with differing M, Z, and E can have similar dE/dx over a substantial portion of](https://reader033.vdocuments.us/reader033/viewer/2022050405/5f826e1139e09d7c0d0b0293/html5/thumbnails/7.jpg)
7
Critical QuestionsRelated to Space Dosimetry
• Space Radiation Environment– For a given mission, what are the fluxes of GCR in interplanetary space as a
function of particle energy, LET, and solar cycle?– What is the solar cycle dependence of space radiation?– What is the trapped radiation flux as a function of time, magnetic field
coordinates and geographical coordinates?– What are the doses related to heavy ions in deep space?
• Nuclear Interactions– What are the yields for nuclear interactions of HZE particles in tissue and space
shielding materials?– How are radiation fields transformed as a function of depth in different space
materials?– What are the optimal ways of shielding humans in space?
• Atomic Interactions– What is the precise energy deposition of heavy ions?– What are the yields and energy spectra of electrons?
• Human Radiation Protection– What should be the radiation dose limits for manned deep space missions?– What is the risk associated with each crew member at any time during a given
mission?
![Page 8: Requirements for Space Radiation Dosimetrywrmiss.org/workshops/fourth/schimmerling.pdf · • Ions with differing M, Z, and E can have similar dE/dx over a substantial portion of](https://reader033.vdocuments.us/reader033/viewer/2022050405/5f826e1139e09d7c0d0b0293/html5/thumbnails/8.jpg)
8
Critical QuestionsRelated to Space Dosimetry
• Space Radiation Environment– For a given mission, what are the fluxes of GCR in interplanetary space as a
function of particle energy, LET, and solar cycle?– What is the solar cycle dependence of space radiation?– What is the trapped radiation flux as a function of time, magnetic field
coordinates and geographical coordinates?– What are the doses related to heavy ions in deep space?
• Nuclear Interactions– What are the yields for nuclear interactions of HZE particles in tissue and space
shielding materials?– How are radiation fields transformed as a function of depth in different space
materials?– What are the optimal ways of shielding humans in space?
• Atomic Interactions– What is the precise energy deposition of heavy ions?– What are the yields and energy spectra of electrons?
• Human Radiation Protection– What should be the radiation dose limits for manned deep space missions?– What is the risk associated with each crew member at any time during a given
mission?
![Page 9: Requirements for Space Radiation Dosimetrywrmiss.org/workshops/fourth/schimmerling.pdf · • Ions with differing M, Z, and E can have similar dE/dx over a substantial portion of](https://reader033.vdocuments.us/reader033/viewer/2022050405/5f826e1139e09d7c0d0b0293/html5/thumbnails/9.jpg)
9
Radiation Protection Model
SPACEFLIGHT
PREDICTRISK SUCCESS
DOSIMETRY:– Measure– Monitor– Record
GROUND-BASED RESEARCH
ReduceRisk
Y
N
ALARA?
–Forecast–Warn
Operational and Flight Rule LimitationsOperational and Flight Rule Limitations
(ALARA)
CURRENTKNOWLEDGE
Radiation Limits (Dose Equivalent, proportional to acceptable risk) Radiation Limits (Dose Equivalent, proportional to acceptable risk)
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107
Risk Prediction Model
Current
γ-rays A-bomb survivors Quality Factor (LET) cancer,
neutrons (ICRP 60,1990) genetic effectsacute effects
Low-LET radiobiology D, DREF, (LET), riskage, gender (UNSCEAR,
BEIR V)
PPA, LBL, BNL (USA) ϕ(A,Z,Ω,m,B, …) RBE cancer, CNS,GSI(Germany), HIMAC(Japan) cataracts, etc.
FutureSpace radiation environment shielding, risk
radiation biology countermeasures
Quality Factor (LET)
(LET),D,
ϕ(A,Z,Ω,m,B, …)
Space radiation environment
Space Radiation Dosimetry
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11
Risk Issues Related to Space Dosimetry
What is risk?• a priori vs. a posteriori probabilities• probability of defined effect (e.g., excess leukemia)• architecture-dependent (trip duration, spacecraft, EVA's, etc.)
Prospective risk assessment:• radiation monitoring
– identify radiation in sufficient detail to understand results, i.e.,spectral information may be required in addition to ionizationchambers; area monitors to define radiation field
• risk assessment vs. risk estimate• architecture issues
Archival risk assessment:• legal
– evidence of causation (or lack of causation) of an effect by exposureto space radiation
• medical history– acute effects: treatment, record– late effects: how?
• epidemiological– evaluate effects of cumulative population exposures
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12
Risk Issues Related to Space Dosimetry
What is risk?• a priori vs. a posteriori probabilities• probability of defined effect (e.g., excess leukemia)• architecture-dependent (trip duration, spacecraft, EVA's, etc.)
Prospective risk assessment:• radiation monitoring
– identify radiation in sufficient detail to understand results, i.e.,spectral information may be required in addition to ionizationchambers; area monitors to define radiation field
• risk assessment vs. risk estimate• architecture issues
Archival risk assessment:• legal
– evidence of causation (or lack of causation) of an effect by exposureto space radiation
• medical history– acute effects: treatment, record– late effects: how?
• epidemiological– evaluate effects of cumulative population exposures
![Page 13: Requirements for Space Radiation Dosimetrywrmiss.org/workshops/fourth/schimmerling.pdf · • Ions with differing M, Z, and E can have similar dE/dx over a substantial portion of](https://reader033.vdocuments.us/reader033/viewer/2022050405/5f826e1139e09d7c0d0b0293/html5/thumbnails/13.jpg)
13
Risk Issues Related to Space Dosimetry
What is risk?• a priori vs. a posteriori probabilities• probability of defined effect (e.g., excess leukemia)• architecture-dependent (trip duration, spacecraft, EVA's, etc.)
Prospective risk assessment:• radiation monitoring
– identify radiation in sufficient detail to understand results, i.e.,spectral information may be required in addition to ionizationchambers; area monitors to define radiation field
• risk assessment vs. risk estimate• architecture issues
Archival risk assessment:• legal
– evidence of causation (or lack of causation) of an effect by exposureto space radiation
• medical history– acute effects: treatment, record– late effects: how?
• epidemiological– evaluate effects of cumulative population exposures
![Page 14: Requirements for Space Radiation Dosimetrywrmiss.org/workshops/fourth/schimmerling.pdf · • Ions with differing M, Z, and E can have similar dE/dx over a substantial portion of](https://reader033.vdocuments.us/reader033/viewer/2022050405/5f826e1139e09d7c0d0b0293/html5/thumbnails/14.jpg)
14
Detector Considerations
AccuracySignal-to-noise ratioCalibration, pre-experiment testingDetection artifactsTiming and location
PrecisionSensitivity adequate for statistically significant resultsGeometry factors and acceptance
Dynamic rangeSpectrum of particles and energiesSpectrum of LETDoses, dose rates and flux
Data acquisitionOn-line vs. off-lineStability of data, especially for integrating detectorsAvailability of records
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15
Detector Considerations
AccuracySignal-to-noise ratioCalibration, pre-experiment testingDetection artifactsTiming and location
PrecisionSensitivity adequate for statistically significant resultsGeometry factors and acceptance
Dynamic rangeSpectrum of particles and energiesSpectrum of LETDoses, dose rates and flux
Data acquisitionOn-line vs. off-lineStability of data, especially for integrating detectorsAvailability of records
![Page 16: Requirements for Space Radiation Dosimetrywrmiss.org/workshops/fourth/schimmerling.pdf · • Ions with differing M, Z, and E can have similar dE/dx over a substantial portion of](https://reader033.vdocuments.us/reader033/viewer/2022050405/5f826e1139e09d7c0d0b0293/html5/thumbnails/16.jpg)
16
Detector Considerations
AccuracySignal-to-noise ratioCalibration, pre-experiment testingDetection artifactsTiming and location
PrecisionSensitivity adequate for statistically significant resultsGeometry factors and acceptance
Dynamic rangeSpectrum of particles and energiesSpectrum of LETDoses, dose rates and flux
Data acquisitionOn-line vs. off-lineStability of data, especially for integrating detectorsAvailability of records
![Page 17: Requirements for Space Radiation Dosimetrywrmiss.org/workshops/fourth/schimmerling.pdf · • Ions with differing M, Z, and E can have similar dE/dx over a substantial portion of](https://reader033.vdocuments.us/reader033/viewer/2022050405/5f826e1139e09d7c0d0b0293/html5/thumbnails/17.jpg)
17
Detector Considerations
AccuracySignal-to-noise ratioCalibration, pre-experiment testingDetection artifactsTiming and location
PrecisionSensitivity adequate for statistically significant resultsGeometry factors and acceptance
Dynamic rangeSpectrum of particles and energiesSpectrum of LETDoses, dose rates and flux
Data acquisitionOn-line vs. off-lineStability of data, especially for integrating detectorsAvailability of records
![Page 18: Requirements for Space Radiation Dosimetrywrmiss.org/workshops/fourth/schimmerling.pdf · • Ions with differing M, Z, and E can have similar dE/dx over a substantial portion of](https://reader033.vdocuments.us/reader033/viewer/2022050405/5f826e1139e09d7c0d0b0293/html5/thumbnails/18.jpg)
18(*) R.H. Thomas,Passive Detectors. In: Advances in Radiation Protection and DosimetryIn Medicine (R.H. Thomas and V. Perez-Mendez, Eds.) Plenum Press, New York, 1980, p. 218
TLD Efficiency(*)
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19
Separating Species
0
500
1000
1500
0 2 4 6 8 10Detector Number
350AMeV Fe295AMeV Cr320AMeV Mn
• Ions with differing M, Z, and E canhave similar dE/dx over asubstantial portion of their paths.
• Need good energy calibration (< 3%or so) and information from manydetectors.
• Measure efficiencies of triggers• Using these efficiencies, apply
corrections.
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20
Radial Energy Deposition
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21
Biodosimetry
• Biological monitoring of radiation exposure:– record accumulated radiation exposure for individuals– supplement area monitors– weigh components of environmental radiation according to
their biological efficacy– desired goal: predict risk
• Different types:– intrinsic biological dosimeters: biomarkers for genetic or
metabolic changes– extrinsic biological dosimeters/indicators for radiation and
other genotoxic substances and agents
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22
Biomarker Requirements
• sensitivity to the levels of radiation exposure of concern– unequivocal: not sensitive to confounding factors (high signal-to-
noise ratio)• accuracy of predictions
– predict risk and health care decisions at a well-defined level ofconfidence
• specificity of prediction– plausible causal relationship based on testable mechanisms of
radiation action, rather than just a contingent correlation withradiation exposure
• precision: the results are not significantly distorted by individual orcircumstantial variations in radiation response
• lead to diagnostic procedures that are:– practical under actual circumstances of exposure rather than
only under highly restricted laboratory conditions– cost-effective , to screen large populations where required
![Page 23: Requirements for Space Radiation Dosimetrywrmiss.org/workshops/fourth/schimmerling.pdf · • Ions with differing M, Z, and E can have similar dE/dx over a substantial portion of](https://reader033.vdocuments.us/reader033/viewer/2022050405/5f826e1139e09d7c0d0b0293/html5/thumbnails/23.jpg)
23
Biomarker Requirements
• sensitivity to the levels of radiation exposure of concern– unequivocal: not sensitive to confounding factors (high signal-to-
noise ratio)• accuracy of predictions
– predict risk and health care decisions at a well-defined level ofconfidence
• specificity of prediction– plausible causal relationship based on testable mechanisms of
radiation action, rather than just a contingent correlation withradiation exposure
• precision: the results are not significantly distorted by individual orcircumstantial variations in radiation response
• lead to diagnostic procedures that are:– practical under actual circumstances of exposure rather than
only under highly restricted laboratory conditions– cost-effective , to screen large populations where required
![Page 24: Requirements for Space Radiation Dosimetrywrmiss.org/workshops/fourth/schimmerling.pdf · • Ions with differing M, Z, and E can have similar dE/dx over a substantial portion of](https://reader033.vdocuments.us/reader033/viewer/2022050405/5f826e1139e09d7c0d0b0293/html5/thumbnails/24.jpg)
24
Biomarker Requirements
• sensitivity to the levels of radiation exposure of concern– unequivocal: not sensitive to confounding factors (high signal-to-
noise ratio)• accuracy of predictions
– predict risk and health care decisions at a well-defined level ofconfidence
• specificity of prediction– plausible causal relationship based on testable mechanisms of
radiation action, rather than just a contingent correlation withradiation exposure
• precision: the results are not significantly distorted by individual orcircumstantial variations in radiation response
• lead to diagnostic procedures that are:– practical under actual circumstances of exposure rather than
only under highly restricted laboratory conditions– cost-effective , to screen large populations where required
![Page 25: Requirements for Space Radiation Dosimetrywrmiss.org/workshops/fourth/schimmerling.pdf · • Ions with differing M, Z, and E can have similar dE/dx over a substantial portion of](https://reader033.vdocuments.us/reader033/viewer/2022050405/5f826e1139e09d7c0d0b0293/html5/thumbnails/25.jpg)
25
Biomarker Requirements
• sensitivity to the levels of radiation exposure of concern– unequivocal: not sensitive to confounding factors (high signal-to-
noise ratio)• accuracy of predictions
– predict risk and health care decisions at a well-defined level ofconfidence
• specificity of prediction– plausible causal relationship based on testable mechanisms of
radiation action, rather than just a contingent correlation withradiation exposure
• precision: the results are not significantly distorted by individual orcircumstantial variations in radiation response
• lead to diagnostic procedures that are:– practical under actual circumstances of exposure rather than
only under highly restricted laboratory conditions– cost-effective , to screen large populations where required
![Page 26: Requirements for Space Radiation Dosimetrywrmiss.org/workshops/fourth/schimmerling.pdf · • Ions with differing M, Z, and E can have similar dE/dx over a substantial portion of](https://reader033.vdocuments.us/reader033/viewer/2022050405/5f826e1139e09d7c0d0b0293/html5/thumbnails/26.jpg)
26
Biomarker Requirements
• sensitivity to the levels of radiation exposure of concern– unequivocal: not sensitive to confounding factors (high signal-to-
noise ratio)• accuracy of predictions
– predict risk and health care decisions at a well-defined level ofconfidence
• specificity of prediction– plausible causal relationship based on testable mechanisms of
radiation action, rather than just a contingent correlation withradiation exposure
• precision: the results are not significantly distorted by individual orcircumstantial variations in radiation response
• lead to diagnostic procedures that are:– practical under actual circumstances of exposure rather than
only under highly restricted laboratory conditions– cost-effective , to screen large populations where required
![Page 27: Requirements for Space Radiation Dosimetrywrmiss.org/workshops/fourth/schimmerling.pdf · • Ions with differing M, Z, and E can have similar dE/dx over a substantial portion of](https://reader033.vdocuments.us/reader033/viewer/2022050405/5f826e1139e09d7c0d0b0293/html5/thumbnails/27.jpg)
27
Single Instrument Specificationsϕ(A,Z, LET, … ), D(LET), QF(LET), …
• Particle identification:Positive charges vs. neutrons,
electrons, γ-rays(1,1) • (A,Z) • (56,26) [p to Fe]∆Z/Z • 0.2]∆A/A • 1
• Energies:10 • εHZE • 1000 MeV/nucleon10 keV • εn • 100 MeV700 keV • εx,γ,β • 10 MeV
• LET range:0.1 • LET • 2000 keV/µm
• Acceptance– Solid angle (statistics) • 2•– detection efficiency • 10%– ∆ø/ø (angular resolution) • 3°
• Rate DependenceR • 105 particles/sec; N • 104
particles/cm2
0.01 µGy/min • • D/• t • 1 Gy/min• Localization
– Portability» Personnel dosimetry» Area monitoring
– Shielding: traceable to mass distributions• Data acquisition and recording
– Telemetry and on-board readout– Coincidence and correlation w/other
instruments– Autonomy > 90 days– Availability and distribution < 30 days– Stability: 50 yrs
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28
Single Instrument Specificationsϕ(A,Z, LET, … ), D(LET), QF(LET), …
• Particle identification:Positive charges vs. neutrons,
electrons, γ-rays(1,1) • (A,Z) • (56,26) [p to Fe]∆Z/Z • 0.2]∆A/A • 1
• Energies:10 • εHZE • 1000 MeV/nucleon10 keV • εn • 100 MeV700 keV • εx,γ,β • 10 MeV
• LET range:0.1 • LET • 2000 keV/µm
• Acceptance– Solid angle (statistics) • 2•– detection efficiency • 10%– ∆ø/ø (angular resolution) • 3°
• Rate DependenceR • 105 particles/sec; N • 104
particles/cm2
0.01 µGy/min • • D/• t • 1 Gy/min• Localization
– Portability» Personnel dosimetry» Area monitoring
– Shielding: traceable to mass distributions• Data acquisition and recording
– Telemetry and on-board readout– Coincidence and correlation w/other
instruments– Autonomy > 90 days– Availability and distribution < 30 days– Stability: 50 yrs
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29
Single Instrument Specificationsϕ(A,Z, LET, … ), D(LET), QF(LET), …
• Particle identification:Positive charges vs. neutrons,
electrons, γ-rays(1,1) • (A,Z) • (56,26) [p to Fe]∆Z/Z • 0.2]∆A/A • 1
• Energies:10 • εHZE • 1000 MeV/nucleon10 keV • εn • 100 MeV700 keV • εx,γ,β • 10 MeV
• LET range:0.1 • LET • 2000 keV/µm
• Acceptance– Solid angle (statistics) • 2•– detection efficiency • 10%– ∆ø/ø (angular resolution) • 3°
• Rate DependenceR • 105 particles/sec; N • 104
particles/cm2
0.01 µGy/min • • D/• t • 1 Gy/min• Localization
– Portability» Personnel dosimetry» Area monitoring
– Shielding: traceable to mass distributions• Data acquisition and recording
– Telemetry and on-board readout– Coincidence and correlation w/other
instruments– Autonomy > 90 days– Availability and distribution < 30 days– Stability: 50 yrs
![Page 30: Requirements for Space Radiation Dosimetrywrmiss.org/workshops/fourth/schimmerling.pdf · • Ions with differing M, Z, and E can have similar dE/dx over a substantial portion of](https://reader033.vdocuments.us/reader033/viewer/2022050405/5f826e1139e09d7c0d0b0293/html5/thumbnails/30.jpg)
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Single Instrument Specificationsϕ(A,Z, LET, … ), D(LET), QF(LET), …
• Particle identification:Positive charges vs. neutrons,
electrons, γ-rays(1,1) • (A,Z) • (56,26) [p to Fe]∆Z/Z • 0.2]∆A/A • 1
• Energies:10 • εHZE • 1000 MeV/nucleon10 keV • εn • 100 MeV700 keV • εx,γ,β • 10 MeV
• LET range:0.1 • LET • 2000 keV/µm
• Acceptance– Solid angle (statistics) • 2•– detection efficiency • 10%– ∆ø/ø (angular resolution) • 3°
• Rate DependenceR • 105 particles/sec; N • 104
particles/cm2
0.01 µGy/min • • D/• t • 1 Gy/min• Localization
– Portability» Personnel dosimetry» Area monitoring
– Shielding: traceable to mass distributions• Data acquisition and recording
– Telemetry and on-board readout– Coincidence and correlation w/other
instruments– Autonomy > 90 days– Availability and distribution < 30 days– Stability: 50 yrs
![Page 31: Requirements for Space Radiation Dosimetrywrmiss.org/workshops/fourth/schimmerling.pdf · • Ions with differing M, Z, and E can have similar dE/dx over a substantial portion of](https://reader033.vdocuments.us/reader033/viewer/2022050405/5f826e1139e09d7c0d0b0293/html5/thumbnails/31.jpg)
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Single Instrument Specificationsϕ(A,Z, LET, … ), D(LET), QF(LET), …
• Particle identification:Positive charges vs. neutrons,
electrons, γ-rays(1,1) • (A,Z) • (56,26) [p to Fe]∆Z/Z • 0.2]∆A/A • 1
• Energies:10 • εHZE • 1000 MeV/nucleon10 keV • εn • 100 MeV700 keV • εx,γ,β • 10 MeV
• LET range:0.1 • LET • 2000 keV/µm
• Acceptance– Solid angle (statistics) • 2•– detection efficiency • 10%– ∆ø/ø (angular resolution) • 3°
• Rate DependenceR • 105 particles/sec; N • 104
particles/cm2
0.01 µGy/min • • D/• t • 1 Gy/min• Localization
– Portability» Personnel dosimetry» Area monitoring
– Shielding: traceable to mass distributions• Data acquisition and recording
– Telemetry and on-board readout– Coincidence and correlation w/other
instruments– Autonomy > 90 days– Availability and distribution < 30 days– Stability: 50 yrs
![Page 32: Requirements for Space Radiation Dosimetrywrmiss.org/workshops/fourth/schimmerling.pdf · • Ions with differing M, Z, and E can have similar dE/dx over a substantial portion of](https://reader033.vdocuments.us/reader033/viewer/2022050405/5f826e1139e09d7c0d0b0293/html5/thumbnails/32.jpg)
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Single Instrument Specificationsϕ(A,Z, LET, … ), D(LET), QF(LET), …
• Particle identification:Positive charges vs. neutrons,
electrons, γ-rays(1,1) • (A,Z) • (56,26) [p to Fe]∆Z/Z • 0.2]∆A/A • 1
• Energies:10 • εHZE • 1000 MeV/nucleon10 keV • εn • 100 MeV700 keV • εx,γ,β • 10 MeV
• LET range:0.1 • LET • 2000 keV/µm
• Acceptance– Solid angle (statistics) • 2•– detection efficiency • 10%– ∆ø/ø (angular resolution) • 3°
• Rate DependenceR • 105 particles/sec; N • 104
particles/cm2
0.01 µGy/min • • D/• t • 1 Gy/min• Localization
– Portability» Personnel dosimetry» Area monitoring
– Shielding: traceable to mass distributions• Data acquisition and recording
– Telemetry and on-board readout– Coincidence and correlation w/other
instruments– Autonomy > 90 days– Availability and distribution < 30 days– Stability: 50 yrs
![Page 33: Requirements for Space Radiation Dosimetrywrmiss.org/workshops/fourth/schimmerling.pdf · • Ions with differing M, Z, and E can have similar dE/dx over a substantial portion of](https://reader033.vdocuments.us/reader033/viewer/2022050405/5f826e1139e09d7c0d0b0293/html5/thumbnails/33.jpg)
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Single Instrument Specificationsϕ(A,Z, LET, … ), D(LET), QF(LET), …
• Particle identification:Positive charges vs. neutrons,
electrons, γ-rays(1,1) • (A,Z) • (56,26) [p to Fe]∆Z/Z • 0.2]∆A/A • 1
• Energies:10 • εHZE • 1000 MeV/nucleon10 keV • εn • 100 MeV700 keV • εx,γ,β • 10 MeV
• LET range:0.1 • LET • 2000 keV/µm
• Acceptance– Solid angle (statistics) • 2•– detection efficiency • 10%– ∆ø/ø (angular resolution) • 3°
• Rate DependenceR • 105 particles/sec; N • 104
particles/cm2
0.01 µGy/min • • D/• t • 1 Gy/min• Localization
– Portability» Personnel dosimetry» Area monitoring
– Shielding: traceable to mass distributions• Data acquisition and recording
– Telemetry and on-board readout– Coincidence and correlation w/other
instruments– Autonomy > 90 days– Availability and distribution < 30 days– Stability: 50 yrs
![Page 34: Requirements for Space Radiation Dosimetrywrmiss.org/workshops/fourth/schimmerling.pdf · • Ions with differing M, Z, and E can have similar dE/dx over a substantial portion of](https://reader033.vdocuments.us/reader033/viewer/2022050405/5f826e1139e09d7c0d0b0293/html5/thumbnails/34.jpg)
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When is a dosimeter not a dosimeter?
• Not every measurement is ISS dosimetry– Have the instruments been calibrated at a recognized facility?
» How accurately does the calibration site simulate the component of spaceradiation for which the instrument is designed?
– Can the results of the measurement be interpreted in terms of othermeasurements?
» Has an intercomparison been performed with other dosimetry instruments?» Have previous flight data been published in refereed journals?
• Not every ISS dosimetry measurement will necessarily be used for implementingALARA
– Are the data available during the mission?» Are they available in real time?» Are they available to the crew in flight?» Is privacy of individual data safeguarded?» Is there a protocol for use by mission operations?
– Are the data available after the mission?» Is there a protocol for incorporation into medical records?» Is there a protocol for interpretation of the data in terms of crew member
radiation history?» Can the data be interpreted in terms of crew member risk?
![Page 35: Requirements for Space Radiation Dosimetrywrmiss.org/workshops/fourth/schimmerling.pdf · • Ions with differing M, Z, and E can have similar dE/dx over a substantial portion of](https://reader033.vdocuments.us/reader033/viewer/2022050405/5f826e1139e09d7c0d0b0293/html5/thumbnails/35.jpg)
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When is a dosimeter not a dosimeter?
• Not every measurement is ISS dosimetry– Have the instruments been calibrated at a recognized facility?
» How accurately does the calibration site simulate the component of spaceradiation for which the instrument is designed?
– Can the results of the measurement be interpreted in terms of othermeasurements?
» Has an intercomparison been performed with other dosimetry instruments?» Have previous flight data been published in refereed journals?
• Not every ISS dosimetry measurement will necessarily be used for implementingALARA
– Are the data available during the mission?» Are they available in real time?» Are they available to the crew in flight?» Is privacy of individual data safeguarded?» Is there a protocol for use by mission operations?
– Are the data available after the mission?» Is there a protocol for incorporation into medical records?» Is there a protocol for interpretation of the data in terms of crew member
radiation history?» Can the data be interpreted in terms of crew member risk?
![Page 36: Requirements for Space Radiation Dosimetrywrmiss.org/workshops/fourth/schimmerling.pdf · • Ions with differing M, Z, and E can have similar dE/dx over a substantial portion of](https://reader033.vdocuments.us/reader033/viewer/2022050405/5f826e1139e09d7c0d0b0293/html5/thumbnails/36.jpg)
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Ground Research:Simulate Space Radiation
Determine Biological Factors of Risk
ACCELERATOREXPOSUREFACILITIES
ValidateHZE
Loma Linda
Brookhaven
Uncertainties Basic Knowledge
protons
Countermeasures
operationalshielding
biomedicalROBOTICPRECURSOR
MISSIONS
RelativeBiologicalEfficiency
Flight Rules
Space Radiation Research ProgramRoad Map
Doses andDose Rates
Enable HumanPresence in Space
EnvironmentShielding