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Requirements for Space Radiation Dosimetry Walter Schimmerling, Francis A. Cucinotta, and John W. Wilson Workshop on Radiation Monitoring for the International Space Station Farnborough, UK 3-5 November 1999

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Page 1: 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

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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2

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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4

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?

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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?

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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?

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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

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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

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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

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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

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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

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(*)

Page 19: 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

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

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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

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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

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

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

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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

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30

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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31

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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32

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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33

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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34

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?

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35

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?

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36

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