ENTRY C2808 20220821 C226C2808000 1 SUBENT C2808001 20220821 C226C2808001 1 BIB 8 29 C2808001 2 TITLE Direct measurement of the low-energy resonances in C2808001 3 22Ne(a,g)26Mg reaction C2808001 4 AUTHOR (Shahina,J.Gorres,D.Robertson,M.Couder,O.Gomez,A.Gula, C2808001 5 M.Hanhardt,T.Kadlecek,R.Kelmar,P.Scholz,A.Simon, C2808001 6 E.Stech,F.Strieder,M.Wiescher) C2808001 7 INSTITUTE (1USANOT,1USASRF) C2808001 8 (1USAUSA) South Dakota School of Mines and Technology, C2808001 9 Rapid City, South Dakota C2808001 10 REFERENCE (J,PR/C,106,025805,2022) C2808001 11 FACILITY (VDG,1USASRF) Experiment performed using 1-MV JN C2808001 12 positive ion accelerator at CASPAR (Compact AcceleratorC2808001 13 System for Performing Astrophysical Research), locatedC2808001 14 on the 4850-ft level of the Sanford Underground C2808001 15 Research Facility in Lead, South Dakota. C2808001 16 SAMPLE (10-NE-22,ENR=0.99) The 22Ne targets were produced by C2808001 17 implantation of enriched Ne onto think tantalum C2808001 18 backing with dimensions of 3.8 cm x 3.8 cm. The C2808001 19 implantation profile of the 22Ne targets was C2808001 20 investigated using the 1278-keV resonance in the C2808001 21 22Ne(p,g) 23Na reaction C2808001 22 DETECTOR (NAICR) Gamma rays were detected using HECTOR array, C2808001 23 consisting of 16 NaI(Tl) crystals with two phototubes C2808001 24 attached to each crystal. The crystals are arranged in C2808001 25 a frame to form a cube 16 x 16 x 16 in. in dimension. C2808001 26 The center of the detector array consists of a 60-mm C2808001 27 borehole that allows the target to be placed at the C2808001 28 center giving a 4Pi total coverage for the detection C2808001 29 of gamma rays. C2808001 30 HISTORY (20220821C) Compiled by S.H. C2808001 31 ENDBIB 29 0 C2808001 32 NOCOMMON 0 0 C2808001 33 ENDSUBENT 32 0 C280800199999 SUBENT C2808002 20220821 C226C2808002 1 BIB 4 7 C2808002 2 REACTION (10-NE-22(A,G),,WID/STR) C2808002 3 MONITOR (10-NE-22(P,G),,WID/STR) resonances at 479 and 851 keV C2808002 4 ERR-ANALYS (ERR-1) Uncertainty in alpha stopping power in Ta C2808002 5 (DATA-ERR) Origin of uncertainties not described C2808002 6 STATUS (TABLE,,Shahina+,J,PR/C,106,025805,2022) C2808002 7 Data taken from tab.1 and text p.6 of C2808002 8 the reference C2808002 9 ENDBIB 7 0 C2808002 10 NOCOMMON 0 0 C2808002 11 DATA 5 2 C2808002 12 EN-RES DATA DATA-ERR DATA-MAX ERR-1 C2808002 13 KEV MICRO-EV MICRO-EV MICRO-EV PER-CENT C2808002 14 650. 0.11 C2808002 15 830. 35. 4. 5. C2808002 16 ENDDATA 4 0 C2808002 17 ENDSUBENT 16 0 C280800299999 SUBENT C2808003 20220821 C226C2808003 1 BIB 4 5 C2808003 2 REACTION (10-NE-22(P,G),,WID/STR) C2808003 3 MONITOR (10-NE-22(P,G),,WID/STR) resonance at 479 keV C2808003 4 ERR-ANALYS (DATA-ERR) Origin of uncertainties not described C2808003 5 STATUS (TABLE,,Shahina+,J,PR/C,106,025805,2022) C2808003 6 Data taken from text p.6 of the reference C2808003 7 ENDBIB 5 0 C2808003 8 COMMON 1 3 C2808003 9 EN-RES-NRM C2808003 10 KEV C2808003 11 479. C2808003 12 ENDCOMMON 3 0 C2808003 13 DATA 5 1 C2808003 14 EN-RES DATA DATA-ERR MONIT MONIT-ERR C2808003 15 KEV EV EV EV EV C2808003 16 851. 9.2 0.7 0.594 0.038 C2808003 17 ENDDATA 3 0 C2808003 18 ENDSUBENT 17 0 C280800399999 ENDENTRY 3 0 C280899999999