ENTRY F0005 20190717 F072F000500000001
SUBENT F0005001 20190717 F072F000500100001
BIB 10 32 F000500100002
TITLE Absolute cross sections for the Li-6(p,He-3)He-4 F000500100003
reaction at energies below 1 MeV F000500100004
AUTHOR (T.Shinozuka,Y.Tanaka,K.Sugiyama) F000500100005
INSTITUTE (2JPNTOH) F000500100006
REFERENCE (J,NP/A,326,47,1979) F000500100007
SAMPLE The layer of 6Li (thickness 10 mu-g/cm**2) was F000500100008
evaporated onto the thin backing of nickel and copper F000500100009
(total thickness 30 mu-g/cm**2) or aluminium (total F000500100010
thickness 20 mu-g/cm**2) F000500100011
METHOD (PHD,BCINT) F000500100012
MONITOR (3-LI-6(P,EL)3-LI-6,,DA,,RTH) - F000500100013
The target thickness was monitored by observing the F000500100014
Rutherford scattered protons from the target. F000500100015
The energy resolution of the monitoring detector F000500100016
was about 10 keV for 400 keV protons F000500100017
FACILITY (CCW,2JPNTOH) For hydrogen ion beams below 400 keV. F000500100018
Energy resolution 5 keV. F000500100019
(DYNAM,2JPNTOH) For ion beams above 400 keV. F000500100020
Energy resolution 2 keV. F000500100021
DETECTOR (SIBAR) Two silicon surface-barrier detectors for F000500100022
detecting the reaction products,3He and 4He, were F000500100023
mounted on a turntable at distances of 8.8 cm and F000500100024
9.5 cm from the center of the scattering chamber. F000500100025
The third silicon surface-barrier detector was placed F000500100026
at a distance of 14 cm from the axis of the chamber at F000500100027
an angle of 150 degr. with respect to the proton beam. F000500100028
The energy resolution of the monitoring detector was F000500100029
about 10 keV for 400 keV protons. F000500100030
HISTORY (19820108C) F000500100031
(19971212U) Added Monitor in Subent 002 F000500100032
(19990407A) CNPD: corrected 4-dig. year F000500100033
(20190717A) SD:Corrections in all Subents.MONITOR addedF000500100034
ENDBIB 32 0 F000500100035
NOCOMMON 0 0 F000500100036
ENDSUBENT 35 0 F000500199999
SUBENT F0005002 20190717 F072F000500200001
BIB 4 8 F000500200002
REACTION (3-LI-6(P,HE3)2-HE-4,,DA,,RSD) F000500200003
ERR-ANALYS (DATA-ERR) From graphic bars and digitizing error F000500200004
No any other information about uncertainties F000500200005
STATUS (CURVE) Fig 3 from Nucl.Phys.A326(1979)47 F000500200006
HISTORY (20190717A) SD: SF8=RSD added; SF9=EXP deleted from F000500200007
REACTION code. MONITOR deleted. Units in DATA/ERR were F000500200008
changed MB/SR -> NO-DIM. COS-ERR -> COS-ERR-D; F000500200009
ANG-NRM deleted. F000500200010
ENDBIB 8 0 F000500200011
COMMON 1 3 F000500200012
COS-ERR-D F000500200013
NO-DIM F000500200014
0.02 F000500200015
ENDCOMMON 3 0 F000500200016
DATA 4 53 F000500200017
EN COS-CM DATA-CM DATA-ERR F000500200018
MEV NO-DIM NO-DIM NO-DIM F000500200019
0.125 0.7817 1.043 0.1495 F000500200020
0.125 0.5681 1.043 0.1495 F000500200021
0.125 0.3352 1.024 0.1401 F000500200022
0.125 -0.4218 0.9668 0.1401 F000500200023
0.125 -0.6356 1.013 0.1308 F000500200024
0.125 -0.7907 0.9477 0.1401 F000500200025
0.225 0.7781 1.014 0.1152 F000500200026
0.225 0.5453 1.034 0.1248 F000500200027
0.225 0.3323 1.082 0.1248 F000500200028
0.225 0.2152 1.025 0.1248 F000500200029
0.225 -0.3693 0.8442 0.1057 F000500200030
0.225 -0.4647 0.998 0.1055 F000500200031
0.225 -0.6398 0.9697 0.1152 F000500200032
0.225 -0.8349 0.8838 0.1056 F000500200033
0.325 0.5484 1.033 0.1347 F000500200034
0.325 0.3155 1.139 0.1347 F000500200035
0.325 0.2184 1.072 0.1154 F000500200036
0.325 -0.3644 0.8798 0.1058 F000500200037
0.325 -0.4616 0.8222 0.1058 F000500200038
0.325 -0.6557 0.8415 0.077 F000500200039
0.325 -0.8305 0.803 0.077 F000500200040
0.4 0.7316 1.066 0.0871 F000500200041
0.4 0.4799 1.116 0.087 F000500200042
0.4 0.2855 1.097 0.0968 F000500200043
0.4 0.1493 1.078 0.087 F000500200044
0.4 -0.3993 0.7612 0.058 F000500200045
0.4 -0.477 0.7608 0.0775 F000500200046
0.4 -0.673 0.6462 0.0485 F000500200047
0.4 -0.8493 0.5404 0.0388 F000500200048
0.5 0.7599 1.158 0.0855 F000500200049
0.5 0.5322 1.1 0.076 F000500200050
0.5 0.3042 1.061 0.0665 F000500200051
0.5 0.1901 1.052 0.076 F000500200052
0.5 -0.3792 0.9069 0.0569 F000500200053
0.5 -0.4733 0.8305 0.0475 F000500200054
0.5 -0.6435 0.7538 0.038 F000500200055
0.5 -0.8145 0.7247 0.0474 F000500200056
0.6 0.7917 1.262 0.0864 F000500200057
0.6 0.5822 1.261 0.0863 F000500200058
0.6 0.3354 1.184 0.0767 F000500200059
0.6 0.2227 1.049 0.0768 F000500200060
0.6 -0.3643 0.7309 0.048 F000500200061
0.6 -0.4595 0.7312 0.0672 F000500200062
0.6 -0.6299 0.6342 0.0288 F000500200063
0.6 -0.7813 0.5474 0.0479 F000500200064
0.7 0.7735 1.174 0.0865 F000500200065
0.7 0.5452 1.213 0.0769 F000500200066
0.7 0.3164 1.184 0.0769 F000500200067
0.7 0.1823 1.089 0.0577 F000500200068
0.7 -0.354 0.731 0.0268 F000500200069
0.7 -0.4687 0.672 0.0384 F000500200070
0.7 -0.6589 0.712 0.0384 F000500200071
0.7 -0.8121 0.609 0.0288 F000500200072
ENDDATA 55 0 F000500200073
ENDSUBENT 72 0 F000500299999
SUBENT F0005003 20190717 F072F000500300001
BIB 5 9 F000500300002
REACTION (3-LI-6(P,HE3)2-HE-4,,DA,,LEG/RS) F000500300003
REL-REF (A,,H.Beaumevieille,R,CEA-R-2624,1964) F000500300004
COMMENT Coefficients (b1) and (b2) normalized to (b0) F000500300005
STATUS (CURVE) fig.4 from Nucl.Phys.A326(1979)47 F000500300006
(DEP,F0005002) F000500300007
HISTORY (19990405A) Added STATUS in SAN=3 F000500300008
(20190717A) SD: SF9=EXP deleted from REACTION code. F000500300009
REL-REF corrected. STATUS updated. EN-ERR -> EN-ERR-DIGF000500300010
DATA-ERR -> ERR-DIG. F000500300011
ENDBIB 9 0 F000500300012
COMMON 1 3 F000500300013
EN-ERR F000500300014
MEV F000500300015
0.04 F000500300016
ENDCOMMON 3 0 F000500300017
DATA 4 21 F000500300018
EN NUMBER-CM DATA-CM ERR-DIG F000500300019
MEV NO-DIM NO-DIM NO-DIM F000500300020
0.1132 1. 0.0543 0.4739E-02 F000500300021
0.1619 1. 0.1219 0.4739E-02 F000500300022
0.1633 2. -0.0516 0.2524E-02 F000500300023
0.216 1. 0.1005 0.4739E-02 F000500300024
0.2183 2. -0.0316 0.2524E-02 F000500300025
0.2648 1. 0.1749 0.4739E-02 F000500300026
0.2667 2. -0.4846E-02 0.2524E-02 F000500300027
0.3132 1. 0.222 0.4739E-02 F000500300028
0.3191 2. -0.073 0.2524E-02 F000500300029
0.3663 2. -0.0869 0.2524E-02 F000500300030
0.3699 1. 0.3646 0.4739E-02 F000500300031
0.383 2. -0.2125 0.2524E-02 F000500300032
0.3839 1. 0.3849 0.4739E-02 F000500300033
0.4827 2. -0.0607 0.2524E-02 F000500300034
0.4907 1. 0.2601 0.4739E-02 F000500300035
0.5367 2. -0.0746 0.2524E-02 F000500300036
0.5479 1. 0.4369 0.4739E-02 F000500300037
0.5842 2. -0.0784 0.2524E-02 F000500300038
0.5964 1. 0.4908 0.4739E-02 F000500300039
0.6902 1. 0.4004 0.4739E-02 F000500300040
0.6929 2. -0.0826 0.2524E-02 F000500300041
ENDDATA 23 0 F000500300042
ENDSUBENT 41 0 F000500399999
SUBENT F0005004 20190717 F072F000500400001
BIB 5 16 F000500400002
REACTION (3-LI-6(P,HE3)2-HE-4,,SIG) F000500400003
REL-REF (A,A1409001,J.B.Marion+,J,PR,104,1402,1956) F000500400004
(A,A1513006,F.Bertrand+,R,CEA-R-3428,1968) F000500400005
(D,,H.Beaumevieille,R,CEA-R-2624,1964) F000500400006
(D,A1367002,W.Gemeinhardt+,J,ZP,197,58,1966) F000500400007
(A,A1445004,H.Spinka+,J,NP/A,164,1,1971) F000500400008
ERR-ANALYS (ERR-T) Total error F000500400009
(ERR-1,8.,10.) The main error sources in the F000500400010
measurements are due to the determination of the numberF000500400011
of target nuclei and the correction for effects of beamF000500400012
charge exchange and of multiple scattering of the F000500400013
proton beam by the target nuclei F000500400014
STATUS (TABLE) Table 1 from Nucl.Phys.A326(1979)47 F000500400015
HISTORY (20190717A) SD: SF9=EXP deleted from REACTION code. F000500400016
REL-REF corrected. STATUS updated. DATA-ERR1 and F000500400017
DATA-ERR2 were included into ERR-1. F000500400018
ENDBIB 16 0 F000500400019
NOCOMMON 0 0 F000500400020
DATA 3 11 F000500400021
EN DATA ERR-T F000500400022
MEV MB MB F000500400023
0.125 5.31 0.82 F000500400024
0.175 15.61 2.21 F000500400025
0.225 24.61 3.25 F000500400026
0.275 40.52 5.53 F000500400027
0.325 53.35 6.81 F000500400028
0.375 67.74 6.07 F000500400029
0.4 79.64 6.57 F000500400030
0.5 84.52 5.81 F000500400031
0.55 92.73 8.78 F000500400032
0.6 97.67 8.06 F000500400033
0.7 106.8 11.13 F000500400034
ENDDATA 13 0 F000500400035
ENDSUBENT 34 0 F000500499999
ENDENTRY 4 0 F000599999999