gamma spectroscopy
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Gamma Spectroscopy. 4/26/12 H . Herrmann (LANL ). Next Steps. Cherenkov detectors Energy thresholded Gas limited to >2.5 MeV Solid limited to 0.1 MeV ?). - PowerPoint PPT PresentationTRANSCRIPT
Gamma Spectroscopy
4/26/12
H. Herrmann (LANL)
- 2 -
e-
Next Steps• Cherenkov detectors
Energy thresholdedGas limited to >2.5 MeVSolid limited to <~0.2 MeVAerogel might span the gap
• Real g-ray spectroscopy (Energy resolved)
X-ray framing camera + CCDX-ray framing camera + CCDSourceSource
θBragg=12oθBragg=12o
Sagittally Bent HOPG crystal
M. Moran, RSI 56, 1066 (1985)
Compton Spect. (>2 MeV) Pixelated Single-Hit “Furlong” (>0.1 MeV?)
Bent Crystal(<1.5 MeV)
Energy resolution would provide valuable information to the Ignition Campaign
1.E-07
1.E-06
1.E-05
1.E-04
1.E-03
0 5 10 15 20
Gam
mas
/Neu
tron
/(0.
1 M
eV b
in)
Gamma-Ray Energy (MeV)
DT
Fu
sio
nD
(n,
)
12C
(n,
)
12 C
(n,n
’)
12C
(n,
)
Hohlraum/TMP n-
Calculated DT Gamma-Ray Spectrum
•Spectral uncertainties call for energy resolution- GRH is only energy thresholding, not resolving
•Be Ablator R from impurity 16O(n,n’) at 6.1, 6.9, 7.1 MeV
• Spectral lines may provide:- 16.75 MeV fusion DT yield- 4.44 MeV 12C(n,n’) CH Ablator R- 15.58 MeV D(n,) Fuel R
DT Fusion -ray spectrum needs to be mapped out better
D + T 5He*
5He*16.75 MeV
4.5 MeV
0 MeV
-0.96 MeV 4He + n5He
1
0
1/0 2.3 ± 0.4
0 5 10 15 200
0.2
0.4
0.6
0.8
1
Gamma-Ray Energy (MeV)
Inte
ns
ity
(a
. u
.)
1
0
G-total/Gn = (4.2 ± 2.0) × 10-5
10-5
10-4
101 102 103 104
Buss '63Kosiara '70Bezotosnyi '70Cecil '84 ( only)Morgan '86 ( only)Kammeraad '93Balbes '94Parker '2011Present Work
D-T
Bra
nch
ing
Rat
io
Deuteron Beam Energy (keV)
Center of Mass Energy (MeV)6 60 6 102 6 103
presentwork
0
0
Y. Kim (LANL), C. Horsfield (AWE)
• GCD mapping of spectrum at OMEGA used assumed line shapes determined by R-Matrix analysis (G. Hale, LANL
• Needs to be verified by spectroscopy
0.0E+00
5.0E-06
1.0E-05
1.5E-05
2.0E-05
2.5E-05
3.0E-05
10 15 20
Gam
mas
/Sou
rce_
neut
ron/
MeV
Gamma-Ray Energy (MeV)
DT
D
C
Hohl/TMP
Total
0.5 MeV binning
Slide 5
0.5 MeV resolution (E/E 3%) at high energy is adequate
Slide 6
0.0E+00
5.0E-06
1.0E-05
1.5E-05
2.0E-05
2.5E-05
3.0E-05
10 15 20
Gam
mas
/Sou
rce_
neut
ron/
MeV
Gamma-Ray Energy (MeV)
DT
D
C
Hohl/TMP
Total
0.5 MeV binning
0.5 MeV resolution (E/E 3%) at high energy is adequate
1.0E-04
1.0E-02
2.0E-02
3.0E-02
4.0E-02
5.0E-02
0 5 10
Gam
mas
/Sou
rce_
neut
ron/
MeV
Gamma-Ray Energy (MeV)
DT
D
C
Hohl/TMP
Total
0.5 MeV binning
Slide 7
0.5 MeV resolution at low energy (adequate, but GCS will do better at 3%)
Operated by Los Alamos National Security, LLC for NNSA
U N C L A S S I F I E D
Mix-dependant -ray lines could aid Ignition Campaign
reaction E (g MeV) Application13C(d,n)14N* 4.91, 5.69 13C layers in CH or doped in Be
9Be(d,n)10B* 2.8, 3.4 , 4.49, 6.03 Be Capsule
9Be(a,n)12C* 4.4 Be Capsule
• MeV alpha-particles born in the DT burn and MeV knockon deuterons and tritons interacting with ablator material (C or Be)
• Reactions emitting gammas sensitive to stopping power with sg>~10 mb/sr/gamma-ray:
A. Hayes, LANL
• 2-Temp LPI x-rays spectrum (Kruer model)– 3 orders-of-mag more x-ray energy below 300
keV than above– Nearly 4 orders-of-mag more energy in LPI x-
rays than Prompt Nuclear -rays– Comparable energy in x-rays & -rays above
~300 keV• Empirically, there’s ~3x more FFLEX signal
from -rays than x-rays at >250 keV• GRH background is dominated by <250 keV
x-rays
Challenge: measure high energy -ray in background of other -rays & LPI x-rays
1.E+08
1.E+09
1.E+10
1.E+11
1.E+12
1.E+13
1.E+14
1.E+15
1.E+16
1.E-02 1.E-01 1.E+00 1.E+01 1.E+02
keV
/keV
/sr
Ex (MeV)
LPI x-rays(Kruer)
Prompt -raysYDTn = 5e14(DT, D,C,Al,Si,Au)
1.E-05
1.E-04
1.E-03
1.E-02
1.E-01
1.E+00
1.E+01
1.E+02
1.E+03
1.E-02 1.E-01 1.E+00 1.E+01 1.E+02
E (
J) a
bove E
x
Ex (MeV)
LPI x-rays
Prompt -rays-rays of interest:
12C(n,n’)
DT- D(n,)
Slide 10
Physics-based Requirements:
Topic Requirement
Resolution E/E 5%
Sensitivity Req’d n Yield
100 e- in bins of interest:Y > 3e14 for 12C- (at R12C 200 mg/cm2)
Y > 3e15 for DT-0
Y > 1e16 for DT-1 and D(n,g)
Binning 12 energy bins
Temporal Response <1ns
SNR >5
Energy Range Total: 2-25 MeVSingle Shot: 2/3Ehigh to Ehigh (e.g., 12-18 MeV)
04/19/2023 11
Option: FURLONG, does not need high neutron yield…
Each detector records less than one gamma ray, many detectors.
Build a spectrum by summing over many detectors.
Painful, but very high quality data.
LaBr3 “Brilliance” detectors. The Best…. But VERY expensive. Need to build factory, share with GSI / FAIR plans
Very good energy resolution Detector array planned at FAIRW. Stoeffl (LLNL)