ENTRY C2582 20201125 C200C258200000001 SUBENT C2582001 20201125 C200C258200100001 BIB 10 38 C258200100002 TITLE First inverse kinematics study of the 22Ne(p,gamma)23NaC258200100003 reaction and its role in AGB star and classical nova C258200100004 nucleosynthesis C258200100005 AUTHOR (M.Williams,A.Lennarz,A.M.Laird,U.Battino,J.Jose, C258200100006 D.Connolly,C.Ruiz,A.Chen,B.Davids,N.Esker,B.R.Fulton, C258200100007 R.Garg,M.Gay,U.Greife,U.Hager,D.Hutcheon,M.Lovely, C258200100008 S.Lyons,A.Psaltis,J.E.Riley,A.Tattersall) C258200100009 INSTITUTE (2UK YRK,1CANTMF,2UK EDG,2SPNUPC,1CANMCM,1CANSFU, C258200100010 1USACOL,1USACSM,1USAMSU) C258200100011 REFERENCE (J,PR/C,102,035801,2020) C258200100012 FACILITY (LINAC,1CANTMF) Experiment was performed using ISAC- C258200100013 1/DRAGON facility at TRIUMF C258200100014 SAMPLE Windowless gas target filled with H2 gas. Experiment C258200100015 was performed at several gas pressures between 2 and 5 C258200100016 Torr. The center of mass target thickness was in the C258200100017 range of 7 - 20 keV. C258200100018 DETECTOR (MAGSP) Selected reaction recoils (23Na) were C258200100019 transported through DRAGON recoil separator, C258200100020 consisting of two magnetic dipoles and two C258200100021 electrostatic dipoles complemented with focusing C258200100022 elements. C258200100023 (BGO) Windowless gas target is surrounded by a 4PI C258200100024 gamma detector array, coinsisting of 30 BGO C258200100025 scintillation detectors. Total solid angle coverage C258200100026 of the array was 92%. C258200100027 (MCPLT) A pair microchannel plate detectors were used C258200100028 for local time of flight measurement for recoil C258200100029 identification C258200100030 (SISD) A double-sided silicon strip detector placed C258200100031 in the DRAGON focal plane where the recoils were C258200100032 stopped and their kinetic energy measured. C258200100033 METHOD Inverse kinematics was used C258200100034 (COINC) Coincidence between gamma rays in BGO array C258200100035 and recoils detected in DRAGON focal plane detectors C258200100036 INC-SOURCE Isotopically pure beam of 22Ne was generated by the C258200100037 Multi Charge Ion Source and accelerated in ISAC-I C258200100038 accelerator complex (RFQ + DLT linac) C258200100039 HISTORY (20201125C) Compiled by S.H. C258200100040 ENDBIB 38 0 C258200100041 NOCOMMON 0 0 C258200100042 ENDSUBENT 41 0 C258200199999 SUBENT C2582002 20201125 C200C258200200001 BIB 4 14 C258200200002 REACTION (10-NE-22(P,G),,WID/STR) C258200200003 FLAG (1.) Reaction rate from singles measurement C258200200004 (2.) Reaction rate from coincidences measurement C258200200005 ERR-ANALYS (ERR-S) Statistical uncertainty C258200200006 (ERR-SYS,12.,16.) Systematic uncertainty for C258200200007 coincidence data C258200200008 (ERR-1,0.5,2.5) Uncertainty in beam normalization C258200200009 (ERR-2,2.,5.) Uncertainty in recoil charge-state C258200200010 fractions C258200200011 (ERR-3) Uncertainty in geometric efficiency of Si C258200200012 strip detectors C258200200013 (ERR-4,1.9,2.5) Uncertainty in the MCP detector C258200200014 (ERR-T) Total uncertainty C258200200015 STATUS (TABLE) Data taken from tab.2 of the reference C258200200016 ENDBIB 14 0 C258200200017 COMMON 2 3 C258200200018 ERR-S ERR-3 C258200200019 PER-CENT PER-CENT C258200200020 20. 0.6 C258200200021 ENDCOMMON 3 0 C258200200022 DATA 6 10 C258200200023 EN-RES-CM DATA ERR-T +ERR-T -ERR-T FLAG C258200200024 KEV EV EV EV EV NO-DIM C258200200025 149. 1.7E-7 +0.5E-7 -0.4E-7 2. C258200200026 181. 2.2E-6 0.4E-6 2. C258200200027 248. 8.5E-6 1.4E-6 2. C258200200028 458. 4.4E-1 0.2E-1 1. C258200200029 458. 4.4E-1 0.5E-1 2. C258200200030 610. 2.6 0.3 2. C258200200031 632. 4.8E-1 0.2E-1 1. C258200200032 632. 4.5E-1 0.3E-1 2. C258200200033 1222. 12.7 0.7 1. C258200200034 1222. 11.7 1.4 2. C258200200035 ENDDATA 12 0 C258200200036 ENDSUBENT 35 0 C258200299999 SUBENT C2582003 20201125 C200C258200300001 BIB 4 8 C258200300002 REACTION 1(10-NE-22(P,G)11-NA-23,DI,SIG) C258200300003 2(10-NE-22(P,G)11-NA-23,,SIG,,SFC) C258200300004 ERR-ANALYS (DATA-ERR) Origin of uncertainties not described C258200300005 ANALYSIS 1Direct part of cross section was obtained by C258200300006 subtracting the resonance contribution. It was made C258200300007 by Monte Carlo simulation. Branching ratios needed for C258200300008 simulations were obtained from direct capture model. C258200300009 STATUS (TABLE) Data taken from tab.3 of the reference C258200300010 ENDBIB 8 0 C258200300011 NOCOMMON 0 0 C258200300012 DATA 6 8 C258200300013 EN-CM EN-RSL DATA 1DATA-ERR 1DATA 2DATA-ERR 2C258200300014 KEV KEV MB MB B*KEV B*KEV C258200300015 511. 6.5 190.41 24.7 78.0 10.3 C258200300016 400. 5.6 31.7 4.9 60.0 9.9 C258200300017 397. 8.1 26.8 3.9 54.9 8.4 C258200300018 377. 8.5 21.4 3.1 61.2 9.4 C258200300019 353. 7.4 13.2 2.1 59.2 9.6 C258200300020 319. 9.7 6.6 1.1 56.6 10.0 C258200300021 309. 7.9 5.1 1.0 55.6 10.7 C258200300022 282. 7.9 2.4 0.7 50.8 15.0 C258200300023 ENDDATA 10 0 C258200300024 ENDSUBENT 23 0 C258200399999 SUBENT C2582004 20201125 C200C258200400001 BIB 4 7 C258200400002 REACTION (10-NE-22(P,G)11-NA-23,,SGV) C258200400003 MISC-COL (MISC1) Low reaction rate C258200400004 (MISC2) High reaction rate C258200400005 STATUS (TABLE) Data taken from tab.4 of the reference C258200400006 (DEP,C2582002) C258200400007 ANALYSIS Thermonuclear reaction rate determined from resonance C258200400008 parameters determined in present work C258200400009 ENDBIB 7 0 C258200400010 NOCOMMON 0 0 C258200400011 DATA 4 51 C258200400012 KT DATA MISC1 MISC2 C258200400013 K9 CM3/S/MOL CM3/S/MOL CM3/S/MOL C258200400014 0.010 6.75E-25 4.21E-25 1.08E-24 C258200400015 0.011 2.44E-23 1.58E-23 3.78E-23 C258200400016 0.012 4.81E-22 3.21E-22 7.21E-22 C258200400017 0.013 5.93E-21 4.03E-21 8.71E-21 C258200400018 0.014 5.08E-20 3.49E-20 7.37E-20 C258200400019 0.015 3.24E-19 2.23E-19 4.68E-19 C258200400020 0.016 1.62E-18 1.13E-18 2.35E-18 C258200400021 0.018 2.36E-17 1.63E-17 3.44E-17 C258200400022 0.020 1.98E-16 1.35E-16 2.90E-16 C258200400023 0.025 8.64E-15 5.69E-15 1.30E-14 C258200400024 0.030 1.02E-13 6.55E-14 1.57E-13 C258200400025 0.040 2.05E-12 1.25E-12 3.25E-12 C258200400026 0.050 1.16E-11 7.00E-12 1.89E-11 C258200400027 0.060 3.81E-11 2.36E-11 6.13E-11 C258200400028 0.070 1.34E-10 1.00E-10 1.87E-10 C258200400029 0.080 9.22E-10 8.25E-10 1.05E-09 C258200400030 0.090 7.10E-09 6.57E-09 7.71E-09 C258200400031 0.100 4.18E-08 3.90E-08 4.49E-08 C258200400032 0.110 1.86E-07 1.74E-07 1.98E-07 C258200400033 0.120 6.56E-07 6.20E-07 6.95E-07 C258200400034 0.130 1.93E-06 1.83E-06 2.03E-06 C258200400035 0.140 4.88E-06 4.65E-06 5.14E-06 C258200400036 0.150 1.10E-05 1.05E-05 1.15E-05 C258200400037 0.160 2.24E-05 2.14E-05 2.35E-05 C258200400038 0.180 7.44E-05 7.14E-05 7.77E-05 C258200400039 0.200 2.01E-04 1.93E-04 2.09E-04 C258200400040 0.250 1.88E-03 1.83E-03 1.94E-03 C258200400041 0.300 2.07E-02 2.00E-02 2.15E-02 C258200400042 0.350 1.64E-01 1.58E-01 1.70E-01 C258200400043 0.400 8.28E-01 7.98E-01 8.59E-01 C258200400044 0.450 2.96E+00 2.86E+00 3.07E+00 C258200400045 0.500 8.26E+00 7.98E+00 8.55E+00 C258200400046 0.600 3.92E+01 3.79E+01 4.04E+01 C258200400047 0.700 1.22E+02 1.18E+02 1.26E+02 C258200400048 0.800 2.92E+02 2.83E+02 3.02E+02 C258200400049 0.900 5.89E+02 5.68E+02 6.12E+02 C258200400050 1.000 1.05E+03 1.01E+03 1.10E+03 C258200400051 1.250 3.12E+03 2.94E+03 3.34E+03 C258200400052 1.500 6.72E+03 6.25E+03 7.32E+03 C258200400053 1.750 1.19E+04 1.09E+04 1.30E+04 C258200400054 2.000 1.83E+04 1.68E+04 2.02E+04 C258200400055 2.500 3.39E+04 3.10E+04 3.75E+04 C258200400056 3.000 5.10E+04 4.66E+04 5.63E+04 C258200400057 3.500 6.77E+04 6.22E+04 7.45E+04 C258200400058 4.000 8.29E+04 7.64E+04 9.08E+04 C258200400059 5.000 1.07E+05 9.95E+04 1.17E+05 C258200400060 6.000 1.23E+05 1.15E+05 1.33E+05 C258200400061 7.000 1.33E+05 1.24E+05 1.43E+05 C258200400062 8.000 1.38E+05 1.29E+05 1.48E+05 C258200400063 9.000 1.39E+05 1.31E+05 1.49E+05 C258200400064 10.000 1.38E+5 1.30E+05 1.48E+05 C258200400065 ENDDATA 53 0 C258200400066 ENDSUBENT 65 0 C258200499999 ENDENTRY 4 0 C258299999999