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405 changes: 321 additions & 84 deletions exforall/A00/A0013.x4

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228 changes: 149 additions & 79 deletions exforall/A10/A1040.x4
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ENTRY A1040 19990319 19990505 20050926 0000
SUBENT A1040001 19990319 19990505 20050926 0000
BIB 12 24
INSTITUTE (1USANOT)
REFERENCE (J,PR/C,3,(6),2171,197106)
AUTHOR (J.T.KLOPCIC,S.E.DARDEN)
TITLE Cross section and polarisation measurements for the
ENTRY A1040 20240707 20240820 20240820 A113
SUBENT A1040001 20240707 20240820 20240820 A113
BIB 7 15
TITLE Cross section and polarization measurements for the
3He(He3,n)5Li reaction
FACILITY (VDG) Notre-Dame 4 MeV
SAMPLE Tritium targets consisted of thin copper disks
containing a layer of titanium into which tritium had
been absorbed
METHOD (PHD)
DETECTOR (SCIN) A liquid scintillator NC213 5cm*5cm DIAM.
MONIT-REF (C0004001,BAME+,J,PR,107,(6),1616,195709)
AUTHOR (J.T.Klopcic,S.E.Darden)
REFERENCE (J,PR/C,3,2171,1971)
INSTITUTE (1USANOT)
FACILITY (VDG,1USANOT) 4 MeV
CORRECTION Contributions from the three-body breakup channel
3H(He3,np)4He were removed by assuming these
neutrons to be unpolarized and to have a statistical
energy distribution in the high-energy portion of the
3H(He3,np)4He were removed by assuming these neutrons
to be unpolarized and to have a statistical energy
distribution in the high-energy portion of the
neutron spectrum
ERR-ANALYS (EN-ERR1) Scale error
(ANG-ERR) Angular resolution
(DATA-ERR2) The absolute uncertainty associated with
the normalization of the cross section appears to be
about 5% or less
HISTORY (19810311C) Compilation produced by Arzamas RFNC-VNIIEF
(19990115U)CNPD: corrected 4-dig. year and lower cases.
ENDBIB 24
COMMON 3 3
EN-ERR1 ANG-ERR DATA-ERR2
MEV ADEG PER-CENT
0.135 3. 5.
ENDCOMMON 3
ENDSUBENT 31
SUBENT A1040002 19990319 19990505 20050926 0000
BIB 3 7
REACTION (1-H-3(HE3,N)3-LI-5,,DA,,,EXP)
ERR-ANALYS (DATA-ERR) Order of 10%,arise from approximately equal
(20240707A) SD: Corrections in all Subents. Subent 005
was added.
ENDBIB 15
NOCOMMON 0 0
ENDSUBENT 18
SUBENT A1040002 20240707 20240820 20240820 A113
BIB 9 21
REACTION (1-H-3(HE3,N)3-LI-5,,DA)
SAMPLE Tritium targets consisted of thin copper disks
containing a layer of titanium into which tritium had
been absorbed.
For the cross-section measurements, the titanium was
270-keV thick to 3-MeV 3He+ ions.
DETECTOR (SCIN) A liquid scintillator Ne213 5 cm x 5 cm diam.
MONITOR (1-H-3(HE3,N)3-LI-5,,DA)
MONIT-REF (C0004001,S.J.Bame Jr+,J,PR,107,1616,1957)
METHOD (PHD,BCINT)
ERR-ANALYS (ERR-1) Order of 10%, arise from approximately equal
contributions from statistical uncertainties in the
data and from uncertainty in the separation of the
monoenergetic-neutron-recoil spectrum from the measured
spectrum.
STATUS (TABLE) Table 2
ENDBIB 7
NOCOMMON
(ERR-2,,5.) The absolute uncertainty associated with
the normalization of the cross section appears to be
about 5% or less.
STATUS (TABLE,,J.T.Klopcic+,J,PR/C,3,2171,1971) Table II
HISTORY (20240707A) SD: SF9=EXP deleted from REACTION code.
DATA-ERR -> ERR-1.
ENDBIB 21
COMMON 1 3
ANG-RSL
ADEG
3.
ENDCOMMON 3
DATA 4 25
EN ANG-CM DATA-CM DATA-ERR
EN ANG-CM DATA-CM ERR-1
MEV ADEG MB/SR MB/SR
2.7 0. 1.05 0.07
2.7 0.0 1.05 0.07
2.7 11.5 1.06 0.12
2.7 23. 1.17 0.13
2.7 23.0 1.17 0.13
2.7 34.4 1.36 0.15
2.7 45.6 1.37 0.15
2.7 56.7 1.39 0.15
Expand All @@ -61,62 +66,80 @@ MEV ADEG MB/SR MB/SR
2.7 127.6 0.89 0.13
2.7 136.7 0.83 0.14
2.7 145.6 0.7 0.14
3.55 0. 1.38 0.15
3.55 0.0 1.38 0.15
3.55 17.5 1.67 0.19
3.55 34.9 1.98 0.22
3.55 46.3 1.89 0.21
3.55 68.5 1.76 0.2
3.55 68.5 1.76 0.20
3.55 84.5 1.56 0.18
3.55 100. 1.41 0.16
3.55 100.0 1.41 0.16
3.55 114.5 1.29 0.15
3.55 128.5 1.24 0.17
3.55 141.9 1.06 0.2
ENDDATA 27
ENDSUBENT 39
SUBENT A1040003 19990319 19990505 20050926 0000
BIB 3 5
REACTION (1-H-3(HE3,N)3-LI-5,,DA,,,EXP)
ERR-ANALYS (EN-ERR) Digitizing error
(DATA-ERR1) From graphic bars (definition at DATA-ERR)
and digitizing error
STATUS (CURVE) FIG 5
ENDBIB 5
ENDSUBENT 57
SUBENT A1040003 20240707 20240820 20240820 A113
BIB 9 21
REACTION (1-H-3(HE3,N)3-LI-5,,DA)
SAMPLE Tritium targets consisted of thin copper disks
containing a layer of titanium into which tritium had
been absorbed.
For the cross-section measurements, the titanium was
270-keV thick to 3-MeV 3He+ ions.
DETECTOR (SCIN) A liquid scintillator NE213 5 cm x 5 cm diam.
MONITOR (1-H-3(HE3,N)3-LI-5,,DA)
MONIT-REF (C0004001,S.J.Bame Jr+,J,PR,107,1616,1957)
METHOD (PHD,BCINT)
ERR-ANALYS (ERR-1) Order of 10%, arise from approximately equal
contributions from statistical uncertainties in the
data and from uncertainty in the separation of the
monoenergetic-neutron-recoil spectrum from the measured
spectrum.
(ERR-2,,5.) The absolute uncertainty associated with
the normalization of the cross section appears to be
about 5% or less.
STATUS (CURVE,,J.T.Klopcic+,J,PR/C,3,2171,1971) Fig.5
HISTORY (20240707A) SD: SF9=EXP deleted from REACTION code.
EN-ERR -> EN-ERR-DIG; DATA-ERR1 -> ERR-1.
ENDBIB 21
COMMON 1 3
EN-ERR
EN-ERR-DIG
MEV
0.01
ENDCOMMON 3
DATA 4 15
EN ANG DATA DATA-ERR1
MEV ADEG MB/SR MB/SR
1. 40. 0.3468 0.0631
1.301 40. 0.5871 0.0946
1.583 0. 0.7895 0.1072
1.592 40. 0.8526 0.1261
1.893 40. 0.9794 0.1261
2.194 0. 1.075 0.1325
2.194 40. 1.175 0.145
2.486 40. 1.466 0.1766
2.777 40. 1.7 0.1955
2.787 0. 1.442 0.1766
3.088 40. 1.903 0.3342
3.379 0. 1.96 0.2397
3.389 40. 2.301 0.2775
3.624 0. 1.891 0.1955
3.69 40. 2.402 0.2964
ANG EN DATA ERR-1
ADEG MEV MB/SR MB/SR
0. 1.58 0.789 0.107
0. 2.19 1.075 0.133
0. 2.79 1.442 0.177
0. 3.38 1.960 0.240
0. 3.62 1.891 0.196
40. 1.00 0.347 0.063
40. 1.30 0.587 0.095
40. 1.59 0.853 0.126
40. 1.89 0.979 0.126
40. 2.19 1.175 0.145
40. 2.49 1.466 0.177
40. 2.78 1.700 0.196
40. 3.09 1.903 0.334
40. 3.39 2.301 0.278
40. 3.69 2.402 0.296
ENDDATA 17
ENDSUBENT 31
SUBENT A1040004 19990319 19990505 20050926 0000
BIB 3 7
REACTION (1-H-3(HE3,N+P)2-HE-4,,DA,N,,EXP)
ERR-ANALYS (DATA-ERR) Order of 10%,arise from approximately equal
ENDSUBENT 47
SUBENT A1040004 20240707 20240820 20240820 A113
BIB 5 9
REACTION (1-H-3(HE3,N+P)2-HE-4,,DA,N)
DETECTOR (SCIN) A liquid scintillator NE213 5 cm x 5 cm diam.
ERR-ANALYS (DATA-ERR) Order of 10%, arise from approximately equal
contributions from statistical uncertainties in the
data and from uncertainty in the separation of the
monoenergetic-neutron-recoil spectrum from the measured
spectrum.
STATUS (TABLE) Table 2
ENDBIB 7
NOCOMMON
STATUS (TABLE,,J.T.Klopcic+,J,PR/C,3,2171,1971) Table 2
HISTORY (20240707A) SD: SF9=EXP deleted from REACTION code.
ENDBIB 9
NOCOMMON 0 0
DATA 4 25
EN ANG-CM DATA-CM DATA-ERR
MEV ADEG MB/SR MB/SR
Expand Down Expand Up @@ -146,5 +169,52 @@ MEV ADEG MB/SR MB/SR
3.55 128.5 0.35 0.15
3.55 141.9 0.36 0.16
ENDDATA 27
ENDSUBENT 39
ENDENTRY 4
ENDSUBENT 41
SUBENT A1040005 20240707 20240820 20240820 A113
BIB 7 16
REACTION (1-H-3(HE3,N)3-LI-5,,POL/DA)
SAMPLE Tritium targets consisted of thin copper disks
containing a layer of titanium into which tritium had
been absorbed.
For the polarization measurements, a relatively thick
target (600 keV for 3-MeV 3He+ ions) was used.
DETECTOR (COIN,SCIN) The gas scintillator, paraffin and
W-Ni shielding, and two neutron detectors were mounted
on a movable table which could be pivoted about the
position of the tritium target. Rectangular plastic
scintillators 5 cm x 7.5 cm x 15 cm were used as
neutron detectors.
METHOD 4He used as an analyzer
ERR-ANALYS (DATA-ERR) No information about source of uncertainty
STATUS (TABLE,,J.T.Klopcic+,J,PR/C,3,2171,1971) Table II
HISTORY (20240707C) SD
ENDBIB 16
NOCOMMON 0 0
DATA 4 22
EN ANG-CM DATA DATA-ERR
MEV ADEG NO-DIM NO-DIM
2.7 11.5 -0.012 0.046
2.7 23.0 -0.073 0.031
2.7 34.4 -0.125 0.025
2.7 45.6 -0.081 0.025
2.7 51.2 -0.094 0.030
2.7 56.7 -0.093 0.049
2.7 67.6 -0.099 0.031
2.7 78.3 -0.134 0.062
2.7 88.7 -0.098 0.031
2.7 98.8 -0.158 -0.036
2.7 108.7 -0.182 0.029
2.7 118.3 -0.253 0.032
2.7 127.6 -0.262 0.031
2.7 136.7 -0.200 0.040
3.5 23.4 -0.105 0.044
3.5 34.9 -0.109 0.036
3.5 51.9 -0.088 0.028
3.5 68.5 -0.058 0.029
3.5 84.5 -0.085 0.028
3.5 99.8 -0.118 0.035
3.5 114.5 -0.207 0.028
3.5 128.5 -0.149 0.029
ENDDATA 24
ENDSUBENT 45
ENDENTRY 5
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