project structure - nasa · 2395.780029 7616.859863 24216.09961 1.e-08 1.e-07 1.e-06 1.e-05 1.e-04...
TRANSCRIPT
![Page 1: Project Structure - NASA · 2395.780029 7616.859863 24216.09961 1.E-08 1.E-07 1.E-06 1.E-05 1.E-04 1.E-03 1.E-02 1.E-01 1.E+00 1E-05 1.100000024 3 18 65 140 Optical Photon Current](https://reader030.vdocuments.site/reader030/viewer/2022041111/5f10870a7e708231d4498ceb/html5/thumbnails/1.jpg)
Project Structure
1
Mark ChristlNASA/MSFCOct 23, 2015
Advanced Neutron Spectrometer on the International Space Station (ANS-ISS)
https://ntrs.nasa.gov/search.jsp?R=20150022206 2020-07-16T01:12:51+00:00Z
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Deep Space Radiation Environment• Radiation risk to crew includes charged and neutral
particle
• Sources of charged particles in LEO include: GCR, SEP, Trapped Belts
• Secondary neutrons are generated through the interaction of these charged particles with matter : spacecraft/habitats and planetary surface or atmosphere (e.g. albedo from Earth’s atmosphere)
• Mixed Radiation Field includes all of the above
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Properties of neutrons• Isolated neutrons have a half life of 13 minutes,
so no primary neutrons sources
• Penetrating: no energy loss through direct ionization (tissue, shielding)
• Estimated 25% of dose on ISS is due to neutrons
• Neutrons have high Q values
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ANS Technique: Gate and Capture
Thermal
neutron
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B10 technique
Li6 technique
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ANS GEN-II
Instrument (2014)
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ANS GEN-II
Instrument (2014)
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Waveforms for EM_Ver1 nPMT+nFEE
9
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Response to edge trig; 1”x1”x2”
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EM_Ver1 nPMT+nFEE signal separation
11
Neutron capture
signalBeta continuum
Alpha
peak
Noise peak
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Signal Response TRIUMF
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AmBe Source Exposure
Neutron Capture SignalProton Recoil Signaln-capture p-channelLate signal p-channel
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Comparison of 3 measured neutron source spectra
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Gamma ray rejection
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Gamma-ray Sensitivity (preliminary)
n & p rates over 2 days
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Comparison to Boron loaded detector
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p-recent dist for B10 and Li6May 15, 2013
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Comparison to NMS
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Neutron Spectrum
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Simulations
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Neutron Angular Production
10-6
10-5
10-4
10-3
10-2
0 50 100 150 200
9585756555453525155MeV500keV50keV5keV500eV50eV5eV5x5x5 cm
Angle (deg)
Ne
utr
on
Flu
x (
mm
-2)
200MeV p + Al n + X
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Neutron Spectra @ 45o – p + Al reaction
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Figure 1 ANS GEN-II diagram
ANS GEN-II Geant4 Simulations
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Figure B1 Fraction events versus energy deposited in the ANS GEN-II detector
volume for an incident neutron energy of 10 eV before neutron capture.
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Figure B2 Fraction events versus energy deposited in the ANS GEN-II detector
volume for an incident neutron energy of 0.5 MeV before neutron capture.
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Figure B3 Fraction events versus energy deposited in the ANS GEN-II detector
volume for an incident neutron energy of 10 MeV before neutron capture.
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Figure B4 Fraction events versus energy deposited in the ANS GEN-II detector
volume for an incident neutron energy of 20 MeV before neutron capture.
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Figure B7 ANS GEN-II optical photon response distribution for 0.5 MeV neutrons before
neutron capture.
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Figure B8 ANS GEN-II optical photon response distribution for 10 MeV neutrons before neutron
capture.
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Figure B9 ANS GEN-II optical photon response distribution for 20 MeV neutrons before neutron
capture.
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010.5
23.4493007774.55190277
237.0220032753.559021
2395.7800297616.859863
24216.09961
1.E-08
1.E-07
1.E-06
1.E-05
1.E-04
1.E-03
1.E-02
1.E-01
1.E+00
1E-05
1.100000024
3
18
65
140
Optical Photon Current
Freq
uen
ct
Neutron Energy (MeV)
1.E-01-1.E+00
1.E-02-1.E-01
1.E-03-1.E-02
1.E-04-1.E-03
1.E-05-1.E-04
1.E-06-1.E-05
1.E-07-1.E-06
1.E-08-1.E-07
Figure 11 Geant4 simulation of ANS GEN-II neutron response versus energy and PMT optical
photon current.
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Figure 17 ANS GEN-II response for high-rate 98 MeV protons at 950 V. The fit is 1.09x106E-1.16.
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Figure 22 ANS GEN-II response for AmBe source 30 mV at 950 V. The normalization is 7.11x107.
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Current Status• NASA has not yet selected a neutron spectrometer for
manned exploration• Current state-of-the-art is based on boron loaded
scintillator (cf. Lithium-6)• ANS is a competing technique: advantages: positive
neutron identification, better background rejection and cleaner spectral measurements in mixed radiation fields; disadvantage: lower neutron cross section, no commercial detector available
• ISS will provide the space flight environment to test ANS-ISS and mature the technique and design
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ANS-ISS SummaryObjectives
• The ISS provides a relevant spaceflight environment for testing hardware
• Mature the ANS measurement technique and design
• Deploy to ISS for 6 month mission
• Transmit data to ground for analysis
• Analyze data to determine the fast neutron spectrum on the ISS
• Compare with FND (soon)
• Evaluate environment background
ANS-ISS Allocation• Mass: 5 kgs• Volume: 5”x9”x10”• Power: 7.5 W• Voltage: 28 VDC• Data Link: USB to ISS laptop• Data Rate: 100 kbits/sec• Attachment location: Internal • Attachment method: Velcro • Mission
• Primary: 6 months• Secondary: ISS duratiuon
• Launch configuration: Soft stow• Payload readiness date:
June/July2016
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Next Steps
• Evaluate and test the response matrix with mono-energetic beams of neutrons:
E = 0.024, 0.14, 0.25, 0.57, 1.2, 2.5, 5, 8 , 14, 19 MeV• Conduct flight test on ISS to evaluate trigger efficiency and
susceptibility in a real space environment• Compare derived spectrum with historical results and Boron
loaded detector• Finalize design and qualify:
Tech-demo → Operational instrument5 year mission durationVerify de-convolution approachPotential alterations:
single set of 4 PMTsspheres replacing fibers
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Backup Material
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Space Exposure
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SPE Peak and Average values
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Relevance of the accelerator exposures
Example calculation of the proton intensity for a deep space exposure to neutrons produced by to
solar energetic protons interacting on a spacecraft/habitat sized shhelter:
Assumptions:
Area of spacecraft/habitat right circular cylinder: 5m x5m = 118 m2 (=1.18x10
6 cm
2)
Wall thickness: 10 g/cm2 (based on ISS and including more than such the spacecraft wall)
Incident flux: 1cps/cm2-sr (particle event threshold is 10 Hz/cm
2-sr at >10 MeV)
Total incident proton intensity (p+Al=> X) = 1.2x106 p/s-sr
For an average daily fluence of 104 /cm
2-sr => 10
4x1.2x10
6/(24x3600)=1.3x10
5 p/s
(peak flux probably is several factors higher than daily average)
For frustum 5x3.3=> 62.5 m2 surface area; mass 9000kgs => 14.4 g/cm
2
Incident flux: 1cps/cm2-sr
Total incident proton intensity (p+Al=> X) = 0.625x106 p/s-sr
For an average daily fluence of 104/cm
2 => 10
4x1.25x10
6/(24x3600)= 0.7x10
5 p/s
(peak flux probably is several factors higher than daily average)
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Rate comparison
Threshold > 10 MeV >30 MeV >60 MeV >100 MeVRate in protons/sec 1.4X1011 2.3X1010 2.6X109 6.0X108
SPE intensity
IUCF intensity