ENTRY C2812 20220926 C226C2812000 1 SUBENT C2812001 20220926 C226C2812001 1 BIB 10 43 C2812001 2 TITLE Experimental measurement of 12C+16O fusion at stellar C2812001 3 energies C2812001 4 AUTHOR (X.Fang,W.P.Tan,M.Beard,R.J.Deboer,G.Gilardy,H.Jung, C2812001 5 Q.Liu,S.Lyons,D.Robertson,K.Setoodehnia,C.Seymour, C2812001 6 E.Stech,B.Vande Kolk,M.Wiescher,R.T.deSouza,S.Hudan, C2812001 7 V.Singh,X.D.Tang,E.Uberseder) C2812001 8 INSTITUTE (1USANOT,3CPRSZH,1USAINU,3CPRIMP,1USATAM) C2812001 9 REFERENCE (J,PR/C,96,045804,2017) C2812001 10 FACILITY (VDG,1USANOT) Experiment was made using a 5 MV single- C2812001 11 ended Pelletron accelerator at the Nuclear Science C2812001 12 Laboratory of the University of Notre Dame C2812001 13 SAMPLE Highly ordered pyrolytic graphite with a dimension of C2812001 14 2 cm x 2 cm x 1 mm was used as a target. It was C2812001 15 attached to a water-cooled aluminum holder and fixed C2812001 16 by a round graphite disk with a rectangular hole in C2812001 17 the center C2812001 18 DETECTOR (SISD) The silicon detector array consisted of six C2812001 19 YY1-type silicon detectors and one S2-type silicon C2812001 20 detector, covering angles from 102 to 146 deg and 151 C2812001 21 to 170 deg in the laboratory frame. Each wedge shaped C2812001 22 YY1 is segmented into 16 strips on the front junction C2812001 23 side. Six detectors formed a lampshade C2812001 24 configuration. The S2 detector was doubled sided and C2812001 25 has 48 rings on the front junction side and 16 C2812001 26 segments on the back ohmic side. The solid angle C2812001 27 covered by the detectors was 4.1% of 4Pi for each YY1 C2812001 28 detector and 5.4% of 4Pi for the S2 detector. C2812001 29 (HPGE) For the measurement of the gamma transitions, C2812001 30 high purity germanium detectors was used. C2812001 31 ANALYSIS Cross sections at given incident energy was obtained C2812001 32 from thick target yields measurement. It was C2812001 33 extracted from the derivative of thick target C2812001 34 yields measured in multiple small energy steps. C2812001 35 ERR-ANALYS (DATA-ERR) Systematic uncertainty up to 17% dominate C2812001 36 uncertainties at high energy end and include C2812001 37 contributions from C2812001 38 - detector geometry and efficiency, C2812001 39 - angular distributions, C2812001 40 - summing effects C2812001 41 - thick target approach C2812001 42 Main contribution to uncertainties at low energy end C2812001 43 was lower statistics and relatively higher background C2812001 44 HISTORY (20220926C) Compiled by S.H. C2812001 45 ENDBIB 43 0 C2812001 46 NOCOMMON 0 0 C2812001 47 ENDSUBENT 46 0 C281200199999 SUBENT C2812002 20220926 C226C2812002 1 BIB 4 6 C2812002 2 REACTION (6-C-12(8-O-16,P)13-AL-27,,SIG) C2812002 3 PART-DET (P,G) C2812002 4 ADD-RES 12C(16O,p)27Al cross sections determined by proton and C2812002 5 gamma detections in Table II C2812002 6 STATUS (TABLE,,X.Fang+,J,PR/C,96,045804,2017) C2812002 7 Data taken from tab.3 of the reference C2812002 8 ENDBIB 6 0 C2812002 9 NOCOMMON 0 0 C2812002 10 DATA 3 21 C2812002 11 EN-CM DATA DATA-ERR C2812002 12 MEV MB MB C2812002 13 3.64 5.06E-10 3.71E-10 C2812002 14 3.73 1.64E-9 1.11E-9 C2812002 15 3.81 4.32E-9 2.17E-9 C2812002 16 3.90 8.57E-9 3.65E-9 C2812002 17 4.03 2.25E-8 0.87E-8 C2812002 18 4.11 3.15E-8 1.13E-8 C2812002 19 4.20 5.63E-8 1.60E-8 C2812002 20 4.29 1.19E-7 0.28E-7 C2812002 21 4.37 1.93E-7 0.42E-7 C2812002 22 4.46 2.87E-7 0.66E-7 C2812002 23 4.54 4.18E-7 0.88E-7 C2812002 24 4.63 9.36E-7 2.21E-7 C2812002 25 4.67 1.28E-6 0.31E-6 C2812002 26 4.71 1.51E-6 0.37E-6 C2812002 27 4.76 2.27E-6 0.62E-6 C2812002 28 4.80 3.72E-6 0.81E-6 C2812002 29 4.84 4.79E-6 1.01E-6 C2812002 30 4.88 4.64E-6 0.96E-6 C2812002 31 4.93 5.96E-6 1.23E-6 C2812002 32 4.97 1.29E-5 0.26E-5 C2812002 33 5.01 1.36E-5 0.28E-5 C2812002 34 ENDDATA 23 0 C2812002 35 ENDSUBENT 34 0 C281200299999 SUBENT C2812003 20220926 C226C2812003 1 BIB 3 4 C2812003 2 REACTION (6-C-12(8-O-16,A)12-MG-24,,SIG) C2812003 3 PART-DET (G) C2812003 4 STATUS (TABLE,,X.Fang+,J,PR/C,96,045804,2017) C2812003 5 Data taken from tab.3 of the reference C2812003 6 ENDBIB 4 0 C2812003 7 NOCOMMON 0 0 C2812003 8 DATA 3 13 C2812003 9 EN-CM DATA DATA-ERR C2812003 10 MEV MB MB C2812003 11 3.90 2.20E-9 0.45E-9 C2812003 12 4.03 1.67E-8 0.38E-8 C2812003 13 4.11 4.19E-8 1.23E-8 C2812003 14 4.20 3.49E-8 0.93E-8 C2812003 15 4.29 8.65E-7 0.23E-7 C2812003 16 4.37 1.56E-7 0.22E-7 C2812003 17 4.46 2.28E-7 0.33E-7 C2812003 18 4.54 3.94E-7 0.40E-7 C2812003 19 4.63 7.28E-7 1.02E-7 C2812003 20 4.67 9.18E-7 1.18E-7 C2812003 21 4.71 1.06E-6 0.16E-6 C2812003 22 4.76 1.31E-6 0.18E-6 C2812003 23 4.80 1.60E-6 0.19E-6 C2812003 24 ENDDATA 15 0 C2812003 25 ENDSUBENT 24 0 C281200399999 SUBENT C2812004 20220926 C226C2812004 1 BIB 3 4 C2812004 2 REACTION (6-C-12(8-O-16,N)14-SI-27,,SIG) C2812004 3 PART-DET (G) C2812004 4 STATUS (TABLE,,X.Fang+,J,PR/C,96,045804,2017) C2812004 5 Data taken from tab.3 of the reference C2812004 6 ENDBIB 4 0 C2812004 7 NOCOMMON 0 0 C2812004 8 DATA 3 12 C2812004 9 EN-CM DATA DATA-ERR C2812004 10 MEV MB MB C2812004 11 4.03 4.38E-9 1.00E-9 C2812004 12 4.11 9.13E-9 2.69E-9 C2812004 13 4.20 8.44E-9 2.26E-9 C2812004 14 4.29 2.66E-8 0.71E-8 C2812004 15 4.37 4.94E-8 0.68E-8 C2812004 16 4.46 5.69E-8 0.82E-8 C2812004 17 4.54 1.16E-7 0.12E-7 C2812004 18 4.63 8.15E-8 1.14E-8 C2812004 19 4.67 1.71E-7 0.22E-7 C2812004 20 4.71 2.63E-7 0.39E-7 C2812004 21 4.76 4.03E-7 0.55E-7 C2812004 22 4.80 8.69E-7 1.03E-7 C2812004 23 ENDDATA 14 0 C2812004 24 ENDSUBENT 23 0 C281200499999 SUBENT C2812005 20220926 C226C2812005 1 BIB 3 4 C2812005 2 REACTION (6-C-12(8-O-16,FUS),,SIG) C2812005 3 ANALYSIS Sum of (16O,p), (16O,a) and (16O,n) cross sections C2812005 4 STATUS (TABLE,,X.Fang+,J,PR/C,96,045804,2017) C2812005 5 Data taken from tab.3 of the reference C2812005 6 ENDBIB 4 0 C2812005 7 NOCOMMON 0 0 C2812005 8 DATA 3 21 C2812005 9 EN-CM DATA DATA-ERR C2812005 10 MEV MB MB C2812005 11 3.64 1.13E-9 0.83E-9 C2812005 12 3.73 3.62E-9 2.46E-9 C2812005 13 3.81 9.50E-9 4.78E-9 C2812005 14 3.90 1.87E-8 0.48E-8 C2812005 15 4.03 4.88E-8 0.83E-8 C2812005 16 4.11 8.40E-8 1.54E-8 C2812005 17 4.20 9.83E-8 1.52E-8 C2812005 18 4.29 2.32E-7 0.33E-7 C2812005 19 4.37 4.36E-7 0.32E-7 C2812005 20 4.46 6.41E-7 0.55E-7 C2812005 21 4.54 1.03E-6 0.06E-6 C2812005 22 4.63 1.84E-6 0.16E-6 C2812005 23 4.67 2.58E-6 0.20E-6 C2812005 24 4.71 3.04E-6 0.27E-6 C2812005 25 4.76 4.23E-6 0.36E-6 C2812005 26 4.80 6.02E-6 0.43E-6 C2812005 27 4.84 9.86E-6 2.08E-6 C2812005 28 4.88 9.53E-6 1.98E-6 C2812005 29 4.93 1.22E-5 0.25E-5 C2812005 30 4.97 2.64E-5 0.54E-5 C2812005 31 5.01 2.79E-5 0.57E-5 C2812005 32 ENDDATA 23 0 C2812005 33 ENDSUBENT 32 0 C281200599999 SUBENT C2812006 20220926 C226C2812006 1 BIB 4 7 C2812006 2 REACTION (6-C-12(8-O-16,FUS),,SIG,,SFC) C2812006 3 ANALYSIS The S(E) factor was calculated from measured C2812006 4 partial cross sections. C2812006 5 ADD-RES S-factor derived with (16O,p) cross section from C2812006 6 proton-gamma coincidence detection in Table IV C2812006 7 STATUS (TABLE,,X.Fang+,J,PR/C,96,045804,2017) C2812006 8 Data taken from tab.4 of the reference C2812006 9 ENDBIB 7 0 C2812006 10 NOCOMMON 0 0 C2812006 11 DATA 3 21 C2812006 12 EN-CM DATA DATA-ERR C2812006 13 MEV B*MEV B*MEV C2812006 14 3.64 8.19E+19 6.00E+19 C2812006 15 3.73 1.27E+20 0.86E+20 C2812006 16 3.81 1.64E+20 0.83E+20 C2812006 17 3.90 1.64E+20 0.42E+20 C2812006 18 4.03 1.60E+20 0.27E+20 C2812006 19 4.11 1.47E+20 0.27E+20 C2812006 20 4.20 9.37E+19 1.44E+19 C2812006 21 4.29 1.22E+20 0.17E+20 C2812006 22 4.37 1.30E+20 0.09E+20 C2812006 23 4.46 1.10E+20 0.09E+20 C2812006 24 4.54 1.03E+20 0.06E+20 C2812006 25 4.63 1.09E+20 0.09E+20 C2812006 26 4.67 1.18E+20 0.09E+20 C2812006 27 4.71 1.08E+20 0.10E+20 C2812006 28 4.76 1.17E+20 0.10E+20 C2812006 29 4.80 1.30E+20 0.09E+20 C2812006 30 4.84 1.67E+20 0.35E+20 C2812006 31 4.88 1.28E+20 0.27E+20 C2812006 32 4.93 1.30E+20 0.27E+20 C2812006 33 4.97 2.22E+20 0.46E+20 C2812006 34 5.01 1.87E+20 0.38E+20 C2812006 35 ENDDATA 23 0 C2812006 36 ENDSUBENT 35 0 C281200699999 ENDENTRY 6 0 C281299999999