ENTRY C2231 20160718 C162C223100000001 SUBENT C2231001 20160718 C162C223100100001 BIB 8 30 C223100100002 TITLE Measurement of the Plasma Astrophysical S Factor for C223100100003 the 3He(d,p)4He Reaction in Exploding Molecular C223100100004 Clusters C223100100005 AUTHOR (M.Barbui,W.Bang,A.Bonasera,K.Hagel,K.Schmidt, C223100100006 J.B.Natowitz,R.Burch,G.Giuliani,M.Barbarino,H.Zheng, C223100100007 G.Dyer,H.J.Quevedo,E.Gaul,A.C.Bernstein,M.Donovan, C223100100008 S.Kimura,M.Mazzocco,F.Consoli,R.De Angelis,P.Andreoli, C223100100009 T.Ditmire) C223100100010 INSTITUTE (1USATAM,1USATEX,2ITYLNS,2ITYMIL,2ITYPAD,2ITYEFR) C223100100011 REFERENCE (J,PRL,111,082502,2013) C223100100012 FACILITY (LASER,1USATEX)The experiment was performed using C223100100013 Texas Petawatt Laser at the Center for High Energy C223100100014 Density Science at The University of Texas at Austin. C223100100015 METHOD D2 or CD4 molecular clusters were produced in the C223100100016 adiabatic expansion of a high-pressure (52.5 bars) C223100100017 and low-temperature gas into vacuum through a C223100100018 supersonic nozzle. The temperature of the gas was 86 K C223100100019 in the case of D2 and 200 - 260 K in the case of CD4. C223100100020 Different concentrations of 3He gas were introduced C223100100021 into the reservoir in order to study collisions C223100100022 between fast d ions and 3He. For each laser shot, a C223100100023 residual gas analyzer measured the partial pressures C223100100024 of D2 or CD4 and 3He in the reaction chamber. C223100100025 Images of the plasma were taken by different cameras C223100100026 in order to measure the dimensions and calculate the C223100100027 plasma volume. C223100100028 DETECTOR (SCIN) The yield of 14.7 MeV protons was measured C223100100029 with three thin plastic scintillators placed at 45, 90,C223100100030 and 135deg with respect to the laser beam direction. C223100100031 HISTORY (20160718C) Compiled by S.H. C223100100032 ENDBIB 30 0 C223100100033 NOCOMMON 0 0 C223100100034 ENDSUBENT 33 0 C223100199999 SUBENT C2231002 20160718 C162C223100200001 BIB 3 15 C223100200002 REACTION (2-HE-3(D,P)2-HE-4,,SIG,,MXW) C223100200003 STATUS (TABLE) Data presented in fig. 1 of the reference C223100200004 sent by author (M.B.) C223100200005 ERR-ANALYS (ERR-T) Total uncertainties, dominant contribution is C223100200006 uncertainty of measured proton yield C223100200007 (ERR-S) Statistical uncertainty in number of detected C223100200008 protons C223100200009 (ERR-1,3.0,5.0) Systematic uncertainty related to C223100200010 plasma temperature C223100200011 (ERR-2,3.0,5.0) Systematic uncertainty related to C223100200012 number of ions C223100200013 (ERR-3,3.0,5.0) Systematic uncertainty related to C223100200014 concentration ratio C223100200015 (ERR-4,3.0,5.0) Systematic uncertainty related to C223100200016 plasma dimensions C223100200017 ENDBIB 15 0 C223100200018 COMMON 1 3 C223100200019 ERR-S C223100200020 PER-CENT C223100200021 45.0 C223100200022 ENDCOMMON 3 0 C223100200023 DATA 4 7 C223100200024 KT KT-ERR DATA ERR-T C223100200025 KEV KEV B B C223100200026 4.77 0.15 2.23E-05 8.2E-06 C223100200027 5.18 0.15 4.02E-05 1.0E-05 C223100200028 5.59 0.15 4.76E-05 1.1E-05 C223100200029 6.0 0.15 6.46E-05 1.9E-05 C223100200030 6.57 0.15 1.1E-04 3.0E-05 C223100200031 8.84 0.15 4.6E-04 2.9E-04 C223100200032 9.54 0.15 6.99E-04 3.1E-04 C223100200033 ENDDATA 9 0 C223100200034 ENDSUBENT 33 0 C223100299999 SUBENT C2231003 20160718 C162C223100300001 BIB 4 8 C223100300002 REACTION (2-HE-3(D,P)2-HE-4,,SIG,,SFC,DERIV) C223100300003 ANALYSIS Through parametrization of S(E) expressed by a C223100300004 polynomial function used by H.-S.Bosch et al. C223100300005 REL-REF (N,,H.-S.Bosch+,J,NF,32,611,1992) C223100300006 Functional form of S(E) given C223100300007 STATUS (TABLE) Data presented in fig. 2 of the reference C223100300008 sent by author (M.B.) C223100300009 (DEP,C2231002) Maxwellian cross sections given C223100300010 ENDBIB 8 0 C223100300011 NOCOMMON 0 0 C223100300012 DATA 2 7 C223100300013 EN-CM DATA C223100300014 KEV B*KEV C223100300015 29.96 6861.82 C223100300016 31.65 6923.35 C223100300017 33.30 6984.2 C223100300018 34.91 7044.47 C223100300019 37.08 7127.46 C223100300020 45.20 7451.45 C223100300021 47.55 7549.96 C223100300022 ENDDATA 9 0 C223100300023 ENDSUBENT 22 0 C223100399999 ENDENTRY 3 0 C223199999999