ENTRY C2624 20210912 C209C262400000001
SUBENT C2624001 20210912 C209C262400100001
BIB 7 11 C262400100002
TITLE Comparison of the 12C(p,n)12N and 12C(p,p') reactions C262400100003
at Ep = 62 and 120 MeV C262400100004
AUTHOR (C.A.Goulding,M.B.Greenfield,C.C.Foster,T.E.Ward, C262400100005
J.Rapaport,D.E.Bainum,C.D.Goodman) C262400100006
INSTITUTE (1USAFSU,1USAINU,1USAOHO,1USAORL) C262400100007
REFERENCE (J,NP/A,331,29,1979) C262400100008
#doi:10.1016/0375-9474(79)90298-7 C262400100009
FACILITY (CYCLO,1USAINU) C262400100010
METHOD (TOF) The proton beam flux was measured using a C262400100011
Faraday cup. C262400100012
HISTORY (20210912C) OG C262400100013
ENDBIB 11 0 C262400100014
NOCOMMON 0 0 C262400100015
ENDSUBENT 14 0 C262400199999
SUBENT C2624002 20210913 C209C262400200001
BIB 5 9 C262400200002
REACTION (3-LI-7(P,N)4-BE-7,PAR,DA) These measurements were doneC262400200003
for determination of the absolute efficiency of the C262400200004
neutron detector. The efficiency was determined using C262400200005
a method similar to that described by Schery et al. C262400200006
REL-REF (M,B0127003,S.D.Schery+,J,NIM,147,399,1977) C262400200007
SAMPLE A target 93 +/- 5 mg/cm2 thick of natural Li was used. C262400200008
ERR-ANALYS (DATA-ERR) No information on source of uncertainties. C262400200009
STATUS (CURVE) Fig.2 (p.32) in Nucl.Phys.A,331,29,1979 was C262400200010
digitized by GSYS2.4.7. C262400200011
ENDBIB 9 0 C262400200012
COMMON 3 3 C262400200013
EN E-LVL E-LVL C262400200014
MEV MEV MEV C262400200015
119.8 0.0 0.43 C262400200016
ENDCOMMON 3 0 C262400200017
DATA 3 5 C262400200018
ANG-CM DATA-CM DATA-ERR C262400200019
ADEG MB/SR MB/SR C262400200020
0.932 3.079E+01 C262400200021
6.708 2.293E+01 C262400200022
12.792 1.044E+01 C262400200023
18.491 4.527E+00 C262400200024
24.112 1.932E+00 1.869E-01 C262400200025
ENDDATA 7 0 C262400200026
ENDSUBENT 25 0 C262400299999
SUBENT C2624003 20210913 C209C262400300001
BIB 6 7 C262400300002
REACTION (3-LI-7(P,N)4-BE-7,,SIG) C262400300003
DECAY-DATA (4-BE-7,53.4D,DG,478.) C262400300004
SAMPLE A target 93 +/- 5 mg/cm2 thick of natural Li was used. C262400300005
METHOD (ACTIV) C262400300006
ERR-ANALYS (DATA-ERR)No information on source of uncertainties. C262400300007
STATUS (TABLE) Text on p.32 in Nucl.Phys.A,331,29,1979. C262400300008
(DEP,C2624002) C262400300009
ENDBIB 7 0 C262400300010
NOCOMMON 0 0 C262400300011
DATA 3 1 C262400300012
EN DATA DATA-ERR C262400300013
MEV MB MB C262400300014
119.8 5.40 0.17 C262400300015
ENDDATA 3 0 C262400300016
ENDSUBENT 15 0 C262400399999
SUBENT C2624004 20210913 C209C262400400001
BIB 7 24 C262400400002
REACTION (6-C-12(P,INL)6-C-12,PAR,DA) C262400400003
EN-SEC (E-LVL,6-C-12) C262400400004
LEVEL-PROP (6-C-12,E-LVL=15.11,SPIN=1.,PARITY=+1.) C262400400005
(6-C-12,E-LVL=16.11,SPIN=2.,PARITY=+1.) C262400400006
DETECTOR (MAGSP,SCIN) Quadrupole-dipole-dipole-multipole C262400400007
magnetic spectrograph. C262400400008
The focal plane detection system was composed of C262400400009
an intrinsic delay-line helical gas counter for C262400400010
position measurement followed by one 1.27 cm thick and C262400400011
another 0.635 cm thick pilot B plastic scintillator. C262400400012
Threefold coincidences from these detectors were C262400400013
required. C262400400014
SAMPLE A 37.6 mg/cm2 thick polystyrene target was used. C262400400015
ERR-ANALYS (ERR-1,,4.) The relative uncertainties are +/-4% or C262400400016
less for all points in each angular distribution. C262400400017
Statistical and fitting uncertainties were the largest C262400400018
of the relative uncertainties. C262400400019
(ERR-2) A +/-5% uncertainty in the thickness of the C262400400020
2.08 mg/cm2 natural carbon target is the major factor C262400400021
in a +/-7% uncertainty in the absolute normalization. C262400400022
(ERR-3) Uncertainty in the absolute normalization of C262400400023
each cross section angular distribution. C262400400024
STATUS (CURVE) Fig.5 (p.36) in Nucl.Phys.A,331,29,1979 was C262400400025
digitized by GSYS2.4.7. C262400400026
ENDBIB 24 0 C262400400027
COMMON 3 3 C262400400028
EN ERR-2 ERR-3 C262400400029
MEV PER-CENT PER-CENT C262400400030
61.8 5. 7. C262400400031
ENDCOMMON 3 0 C262400400032
DATA 3 38 C262400400033
E-LVL ANG-CM DATA-CM C262400400034
MEV ADEG MB/SR C262400400035
15.11 5.932 1.374E+00 C262400400036
15.11 8.271 1.278E+00 C262400400037
15.11 10.891 1.153E+00 C262400400038
15.11 12.791 1.024E+00 C262400400039
15.11 15.018 9.594E-01 C262400400040
15.11 17.252 8.421E-01 C262400400041
15.11 19.319 7.448E-01 C262400400042
15.11 21.721 6.413E-01 C262400400043
15.11 23.900 5.628E-01 C262400400044
15.11 25.966 5.017E-01 C262400400045
15.11 28.090 4.335E-01 C262400400046
15.11 30.268 3.835E-01 C262400400047
15.11 32.400 3.067E-01 C262400400048
15.11 34.908 2.777E-01 C262400400049
15.11 37.086 2.466E-01 C262400400050
15.11 39.491 2.058E-01 C262400400051
15.11 41.283 1.772E-01 C262400400052
15.11 43.356 1.462E-01 C262400400053
15.11 45.430 1.210E-01 C262400400054
16.11 6.026 1.755E-01 C262400400055
16.11 8.403 1.943E-01 C262400400056
16.11 10.913 1.746E-01 C262400400057
16.11 13.056 2.170E-01 C262400400058
16.11 15.213 2.366E-01 C262400400059
16.11 17.253 2.732E-01 C262400400060
16.11 19.316 2.512E-01 C262400400061
16.11 21.857 2.868E-01 C262400400062
16.11 24.010 3.237E-01 C262400400063
16.11 25.848 3.069E-01 C262400400064
16.11 27.960 3.014E-01 C262400400065
16.11 30.180 3.029E-01 C262400400066
16.11 32.294 2.917E-01 C262400400067
16.11 34.959 2.909E-01 C262400400068
16.11 37.026 2.573E-01 C262400400069
16.11 39.365 2.393E-01 C262400400070
16.11 41.494 1.974E-01 C262400400071
16.11 43.338 1.767E-01 C262400400072
16.11 45.742 1.486E-01 C262400400073
ENDDATA 40 0 C262400400074
ENDSUBENT 73 0 C262400499999
SUBENT C2624005 20210913 C209C262400500001
BIB 5 8 C262400500002
REACTION (6-C-12(P,N)7-N-12,PAR,DA) C262400500003
DETECTOR The large volume neutron detector (15 cm x 15 cm and C262400500004
100 cm long). C262400500005
SAMPLE A 37.6 mg/cm2 thick polystyrene target was used at 62 C262400500006
MeV and a 475 mg/cmZ carbon target was used at 120 MeV.C262400500007
ERR-ANALYS (DATA-ERR)No information on source of uncertainties. C262400500008
STATUS (CURVE) Figs.5-6 (p.36-37) in Nucl.Phys.A,331,29,1979 C262400500009
was digitized by GSYS2.4.7. C262400500010
ENDBIB 8 0 C262400500011
NOCOMMON 0 0 C262400500012
DATA 6 12 C262400500013
EN E-LVL E-LVL ANG-CM DATA-CM DATA-ERR C262400500014
MEV MEV MEV ADEG MB/SR MB/SR C262400500015
61.8 0.0 1.168 3.368E+00 C262400500016
61.8 0.0 6.285 3.051E+00 C262400500017
61.8 0.0 12.112 2.116E+00 1.256E-01C262400500018
61.8 0.0 23.155 1.164E+00 7.899E-02C262400500019
61.8 1.0 0.782 3.117E-01 3.331E-02C262400500020
61.8 1.0 5.987 3.365E-01 3.596E-02C262400500021
61.8 1.0 11.450 3.465E-01 4.964E-02C262400500022
61.8 1.0 22.996 5.737E-01 7.631E-02C262400500023
119.8 0.0 1.0 6.631 5.082E+00 C262400500024
119.8 0.0 1.0 8.730 4.180E+00 C262400500025
119.8 0.0 1.0 15.624 1.634E+00 1.607E-01C262400500026
119.8 0.0 1.0 21.737 7.763E-01 1.014E-01C262400500027
ENDDATA 14 0 C262400500028
ENDSUBENT 27 0 C262400599999
ENDENTRY 5 0 C262499999999