ENTRY F1345 20180709 F068F134500000001 SUBENT F1345001 20180709 F068F134500100001 BIB 10 25 F134500100002 TITLE Non-Rutherford cross-sections for alpha elastic F134500100003 scattering off Z=28-38 elements in the energy range F134500100004 up to 10 MeV. F134500100005 AUTHOR (A.F.Gurbich, M.V.Bokhovko) F134500100006 INSTITUTE (4RUSFEI) F134500100007 REFERENCE (J,NIM/B,420,1,2018) F134500100008 #doi:10.1016/j.nimb.2018.01.026 F134500100009 FACILITY (VDGT,4RUSFEI) The IPPE 3MV Tandetron accelerator. F134500100010 DETECTOR (SI) Ion implanted silicon charged particle detectors F134500100011 were used. F134500100012 SAMPLE The targets were 10**18 atoms/cm2 thick and were F134500100013 prepared by thermal evaporation in vacuum of F134500100014 chemically pure materials on silicon substrates. F134500100015 ERR-ANALYS (DATA-ERR) A dominant contribution in the uncertainty F134500100016 comes from counting statistics. Systematic errors F134500100017 were mainly defined by the reproducibility of the F134500100018 measurement of the accumulated charge and by a F134500100019 possible non-uniformity of the deposited films F134500100020 combined with a possible lateral variation of the F134500100021 beam density. tion of the beam density. The absolute F134500100022 errors in the obtained cross section ratios were F134500100023 estimated to be around 2.0 %. F134500100024 STATUS Data were taken from SigmaCalc on-line calculator. F134500100025 (APRVD) Entry was approved by Dr. A.F. Gurbich. F134500100026 HISTORY (20180709C) F134500100027 ENDBIB 25 0 F134500100028 COMMON 1 3 F134500100029 EN-ERR F134500100030 PER-CENT F134500100031 0.06 F134500100032 ENDCOMMON 3 0 F134500100033 ENDSUBENT 32 0 F134500199999 SUBENT F1345002 20180709 F068F134500200001 BIB 2 2 F134500200002 REACTION (28-NI-0(A,EL)28-NI-0,,DA,,RTH) F134500200003 STATUS (TABLE) Data from Fig. 2 F134500200004 ENDBIB 2 0 F134500200005 COMMON 2 3 F134500200006 ANG DATA-ERR F134500200007 ADEG NO-DIM F134500200008 170. 0.02 F134500200009 ENDCOMMON 3 0 F134500200010 DATA 2 6 F134500200011 EN DATA F134500200012 KEV NO-DIM F134500200013 6000. 1.000 F134500200014 6500. 0.995 F134500200015 7200. 0.967 F134500200016 7600. 0.940 F134500200017 8000. 0.895 F134500200018 8500. 0.840 F134500200019 ENDDATA 8 0 F134500200020 ENDSUBENT 19 0 F134500299999 SUBENT F1345003 20180709 F068F134500300001 BIB 2 2 F134500300002 REACTION (29-CU-0(A,EL)29-CU-0,,DA,,RTH) F134500300003 STATUS (TABLE) Data from Fig. 4, 5 F134500300004 ENDBIB 2 0 F134500300005 NOCOMMON 0 0 F134500300006 DATA 4 20 F134500300007 ANG EN DATA DATA-ERR F134500300008 ADEG KEV NO-DIM NO-DIM F134500300009 150. 6500. 0.997 0.020 F134500300010 150. 7000. 0.990 0.020 F134500300011 150. 7500. 0.971 0.019 F134500300012 150. 7600. 0.965 0.019 F134500300013 150. 7700. 0.958 0.019 F134500300014 150. 7800. 0.950 0.019 F134500300015 150. 7900. 0.940 0.019 F134500300016 150. 8000. 0.930 0.019 F134500300017 150. 8500. 0.857 0.017 F134500300018 150. 9000. 0.750 0.015 F134500300019 170. 6500. 1.000 0.015 F134500300020 170. 7000. 0.984 0.014 F134500300021 170. 7500. 0.971 0.014 F134500300022 170. 7600. 0.947 0.014 F134500300023 170. 7700. 0.958 0.014 F134500300024 170. 7800. 0.922 0.013 F134500300025 170. 7900. 0.952 0.013 F134500300026 170. 8000. 0.919 0.013 F134500300027 170. 8500. 0.813 0.012 F134500300028 170. 9000. 0.716 0.011 F134500300029 ENDDATA 22 0 F134500300030 ENDSUBENT 29 0 F134500399999 SUBENT F1345004 20180709 F068F134500400001 BIB 2 2 F134500400002 REACTION (39-Y-89(A,EL)39-Y-89,,DA,,RTH) F134500400003 STATUS (TABLE) Data from Fig. 9 F134500400004 ENDBIB 2 0 F134500400005 COMMON 2 3 F134500400006 ANG DATA-ERR F134500400007 ADEG NO-DIM F134500400008 170. 0.02 F134500400009 ENDCOMMON 3 0 F134500400010 DATA 2 21 F134500400011 EN DATA F134500400012 KEV NO-DIM F134500400013 7000. 1.000 F134500400014 7100. 0.975 F134500400015 7200. 0.990 F134500400016 7300. 1.021 F134500400017 7400. 1.016 F134500400018 7500. 0.978 F134500400019 7600. 1.014 F134500400020 7700. 1.006 F134500400021 7800. 1.005 F134500400022 7900. 1.009 F134500400023 8000. 1.016 F134500400024 8100. 1.018 F134500400025 8200. 0.979 F134500400026 8300. 0.978 F134500400027 8400. 1.023 F134500400028 8500. 0.987 F134500400029 8600. 1.023 F134500400030 8700. 1.003 F134500400031 8800. 1.022 F134500400032 8900. 1.030 F134500400033 9000. 1.023 F134500400034 ENDDATA 23 0 F134500400035 ENDSUBENT 34 0 F134500499999 ENDENTRY 4 0 F134599999999