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