ENTRY L0210 20160105 L028L021000000001 SUBENT L0210001 20160105 L028L021000100001 BIB 10 33 L021000100002 TITLE 2H(p,gamma)He3 reaction using polarized and L021000100003 unpolarized protons L021000100004 AUTHOR (D.M.Skopik,H.R.Weller,N.R.Roberson,S.A.Wender) L021000100005 REFERENCE (J,PR/C,19,(3),601,1979) L021000100006 #doi:10.1103/PhysRevC.19.601 L021000100007 INSTITUTE (1CANSAS,1USAFLA,1USADKE,1USATNL) L021000100008 FACILITY (ACCEL,1USATNL) The capture gamma-ray facility at the L021000100009 Triangle Universities Nuclear Laboratory L021000100010 DETECTOR (NAICR) 25.4 x 25.4 cm NaI crystal having a plastic L021000100011 anticoincidence shield. L021000100012 SAMPLE (1-H-2,ENR=0.92) CD2 ~1 mg/cm2 and ~0.2 mg/cm2 L021000100013 deuterium gas targets. L021000100014 METHOD Measured was the energy distribution over an L021000100015 excitation range in 3He of Ex=7.5 to 15.4 MeV or directL021000100016 absolute cross section from E = 3.0 to 14.8 MeV. The L021000100017 energy distribution was to 12 MeV with the CD2 target, L021000100018 while for the higher energies a deuterium gas cell L021000100019 was used and normalized to the solid target results L021000100020 at several overlapping energies. Since the L021000100021 spectrometer efficiency was determined at 15.1 MeV, L021000100022 the efficiencies at other energies have been obtained L021000100023 by correcting for the experimentally determined L021000100024 energy dependence of (1) the crystal response L021000100025 function, (2) the attenuation of the gamma-rays by L021000100026 the shielding in front of the crystal, and (3) the L021000100027 rejection rate due to the anticoincidence shield. For L021000100028 the lowest energy the efficiency was taken as 14.5% L021000100029 (a 15% correction relative to the calibration point). L021000100030 The energy loss of the primary proton beam in the L021000100031 target was also taken into account. L021000100032 ANALYSIS (DTBAL) The cross sections have been converted to L021000100033 that for photo disintegration using detailed balance. L021000100034 HISTORY (20160105C) BP L021000100035 ENDBIB 33 0 L021000100036 NOCOMMON 0 0 L021000100037 ENDSUBENT 36 0 L021000199999 SUBENT L0210002 20160105 L028L021000200001 BIB 3 3 L021000200002 REACTION (2-HE-3(G,P)1-H-2,,DA,,,DERIV) L021000200003 ERR-ANALYS (DATA-ERR) No information on sources of uncertainties. L021000200004 STATUS (CURVE) Fig. 8, page 607. L021000200005 ENDBIB 3 0 L021000200006 COMMON 1 3 L021000200007 ANG L021000200008 ADEG L021000200009 90.0 L021000200010 ENDCOMMON 3 0 L021000200011 DATA 3 13 L021000200012 EN DATA DATA-ERR L021000200013 MEV MB/SR MB/SR L021000200014 7.404 40.798 8.282 L021000200015 8.080 63.497 9.202 L021000200016 8.664 108.589 6.442 L021000200017 9.401 113.497 7.055 L021000200018 9.708 107.975 5.521 L021000200019 10.108 119.325 3.067 L021000200020 10.722 116.564 3.067 L021000200021 11.398 115.337 3.374 L021000200022 11.982 112.577 4.601 L021000200023 12.688 115.644 4.908 L021000200024 13.272 102.454 5.215 L021000200025 14.009 98.160 4.601 L021000200026 15.269 88.344 7.669 L021000200027 ENDDATA 15 0 L021000200028 ENDSUBENT 27 0 L021000299999 SUBENT L0210003 20160105 L028L021000300001 BIB 7 14 L021000300002 REACTION (2-HE-3(G,P)1-H-2,,SIG,,,DERIV) L021000300003 COMMENT At the paper was given the coefficient a0, and L021000300004 sigma(total)=4*pi*a0 calculated by compiler L021000300005 MISC-COL (MISC) a0 coefficient L021000300006 FLAG (0.) Standard description L021000300007 (1.) The cross section is nearly zero at 0 and 180 deg.L021000300008 A second fit was performed in which the cross section L021000300009 was constrained to be essentially zero at these angles L021000300010 but with errors taken to be indicative of the errors inL021000300011 the present experiment. L021000300012 ERR-ANALYS (ERR-S) Statistical error in text on page 608 is L021000300013 consistent with the data plotted in Fig.9 L021000300014 STATUS (TABLE) Table 1, plotted also in Fig.9 L021000300015 HISTORY (20160105T) Numerical data moved from A1186.002 L021000300016 ENDBIB 14 0 L021000300017 NOCOMMON 0 0 L021000300018 DATA 6 6 L021000300019 EN DATA ERR-S MISC MISC-ERR FLAG L021000300020 MEV MB MB MICRO-B MICRO-B NO-DIM L021000300021 8.83 0.9664 0.0189 76.8 1.5 0. L021000300022 8.83 1.038 0.0101 82.5 0.8 1. L021000300023 9.83 1.072 0.0315 85.2 2.5 0. L021000300024 9.83 1.087 0.0138 86.4 1.1 1. L021000300025 10.83 1.091 0.0176 86.7 1.4 0. L021000300026 10.83 1.083 0.0076 86.1 0.6 1. L021000300027 ENDDATA 8 0 L021000300028 ENDSUBENT 27 0 L021000399999 SUBENT L0210004 20160218 L028L021000400001 BIB 5 11 L021000400002 REACTION (2-HE-3(G,P)1-H-2,,DA,,LEG/RS,DERIV) L021000400003 FLAG (0.) Standard description L021000400004 (1.) The cross section is nearly zero at 0 and 180 deg.L021000400005 a second fit was performed in which the cross section L021000400006 was constrained to be essentially zero at these angles L021000400007 but with errors taken to be indicative of the errors inL021000400008 the present experiment. L021000400009 ERR-ANALYS (DATA-ERR) Error includes statistical error and error L021000400010 of fitting procedure L021000400011 STATUS (TABLE) Table 1 L021000400012 HISTORY (20160105T) Numerical data moved from A1186.003 L021000400013 ENDBIB 11 0 L021000400014 NOCOMMON 0 0 L021000400015 DATA 5 24 L021000400016 EN NUMBER DATA-CM DATA-ERR FLAG L021000400017 MEV NO-DIM NO-DIM NO-DIM NO-DIM L021000400018 8.83 1. 0.08 0.03 0. L021000400019 8.83 1. 0.14 0.02 1. L021000400020 8.83 2. -0.79 0.07 0. L021000400021 8.83 2. -0.8 0.03 1. L021000400022 8.83 3. -0.27 0.06 0. L021000400023 8.83 3. -0.15 0.02 1. L021000400024 8.83 4. -0.16 0.08 0. L021000400025 8.83 4. -0.2 0.03 1. L021000400026 9.83 1. 0.04 0.07 0. L021000400027 9.83 1. 0.08 0.02 1. L021000400028 9.83 2. -0.63 0.12 0. L021000400029 9.83 2. -0.77 0.02 1. L021000400030 9.83 3. -0.13 0.09 0. L021000400031 9.83 3. -0.09 0.02 1. L021000400032 9.83 4. -0.11 0.09 0. L021000400033 9.83 4. -0.24 0.03 1. L021000400034 10.83 1. 0.25 0.03 0. L021000400035 10.83 1. 0.24 0.02 1. L021000400036 10.83 2. -0.69 0.06 0. L021000400037 10.83 2. -0.75 0.03 1. L021000400038 10.83 3. -0.18 0.05 0. L021000400039 10.83 3. -0.24 0.02 1. L021000400040 10.83 4. -0.15 0.07 0. L021000400041 10.83 4. -0.25 0.03 1. L021000400042 ENDDATA 26 0 L021000400043 ENDSUBENT 42 0 L021000499999 ENDENTRY 4 0 L021099999999