ENTRY F0769 20190814 F072F076900000001 SUBENT F0769001 20190814 F072F076900100001 BIB 9 34 F076900100002 TITLE Total cross sections for the 4,6He + 28Si reactions F076900100003 measured at 10 - 28 MeV/A F076900100004 AUTHOR (I.V.Kuznetsov,E.Byalkowski,M.P.Ivanov,R.Kalpakchieva, F076900100005 A.Kugler,I.N.Kukhtina,V.F.Kushniruk,V.A.Maslov, F076900100006 L.Mikhailov,F.Negoita,Yu.E.Penionzhkevich, F076900100007 N.O.Poroshin,N.K.Skobelev,V.I.Smirnov,Yu.G.Sobolev, F076900100008 V.Yu.Ugryumov) F076900100009 INSTITUTE (4ZZZDUB,3POLIFJ,3RUMBUC,4RUSMIF,3CZRUJF) F076900100010 REFERENCE (J,YF,65,1609,2002) F076900100011 (J,PAN,65,1569,2002) English translation F076900100012 FACILITY (CYCLO,4ZZZDUB) F076900100013 DETECTOR (TELES,SI)Silicon detector of sandwich type was used. F076900100014 The working area of the detector was ~ 3 cm2 and the F076900100015 total length of the telescope was 10 cm. Telescope F076900100016 detectors had different thicknesses from 400-1200 mu-m F076900100017 measured with the accuracy of 3 mu-m. F076900100018 SAMPLE Thick beryllium target (140 mg/cm2) was used to obtain F076900100019 the secondary beam of He-6 ions for silicon irradiationF076900100020 Telescope detectors served as a target; they detected F076900100021 reaction products and reduced the energy of 6He ions. F076900100022 ERR-ANALYS (EN-ERR) No source of uncertainty is given. F076900100023 (DATA-ERR) Error in cross section definition was F076900100024 determined by statistical errors, accuracy of F076900100025 detector thickness measurement and accuracy of F076900100026 discrimination of events related to nuclear reactions F076900100027 in the couple of detectors under study. F076900100028 HISTORY (20060420C) F076900100029 (20101001A) REACTION code in Sub 003,004 was changed. F076900100030 Target description in sub 001 was changed. MONITOR F076900100031 record was removed. METHOD code in Sub 003,004 was F076900100032 added. F076900100033 (20180705A) Reference code was added. F076900100034 (20190814A) SD: Ref. YF,80,33,2017 deleted (only F076900100035 analysis is given). Data in Subent 003 corrected. F076900100036 ENDBIB 34 0 F076900100037 NOCOMMON 0 0 F076900100038 ENDSUBENT 37 0 F076900199999 SUBENT F0769002 20060614 F025F076900200001 BIB 3 3 F076900200002 REACTION (14-SI-28(2-HE-6,X)2-HE-4,,SIG) F076900200003 ERR-ANALYS (DATA-ERR1)Error from the graphic bars F076900200004 STATUS (CURVE)Fig.3 F076900200005 ENDBIB 3 0 F076900200006 COMMON 3 3 F076900200007 DATA-ERR EN-ERR-DIG ERR-DIG F076900200008 PER-CENT MEV/A MB F076900200009 6. 0.08 1.56 F076900200010 ENDCOMMON 3 0 F076900200011 DATA 4 6 F076900200012 EN EN-ERR DATA DATA-ERR1 F076900200013 MEV/A MEV/A MB MB F076900200014 8.5586 1.6530 198.65 63.234 F076900200015 13.259 1.7978 298.97 71.480 F076900200016 14.981 1.7990 529.63 51.819 F076900200017 18.448 1.5812 356.29 55.624 F076900200018 21.431 1.7248 477.48 47.696 F076900200019 24.910 2.0827 342.83 52.137 F076900200020 ENDDATA 8 0 F076900200021 ENDSUBENT 20 0 F076900299999 SUBENT F0769003 20190814 F072F076900300001 BIB 4 17 F076900300002 REACTION (14-SI-28(A,NON),,SIG) F076900300003 METHOD (TRN) Method of attenuation of alpha particle beam F076900300004 was used. Telescope detectors were used as a target, F076900300005 a detector and an energy absorber of incident ions. F076900300006 Total cross section was determined by the following F076900300007 way. Events in which the studied nucleus passed F076900300008 through the telescope to the full stop due to the F076900300009 ionizing losses only were subtracted from the whole F076900300010 data array of particular nucleus. As a result in data F076900300011 array only the events related to the nuclear F076900300012 reactions and inelastic scattering of the studied F076900300013 nucleus on silicon were kept. F076900300014 (EDE) Particle determination was performed using the F076900300015 results of the energy losses in delta E counters. F076900300016 STATUS (TABLE) Data received from T.Zholdybayev, 2019-04-09 F076900300017 HISTORY (20190814A) SD: Values were corrected according to the F076900300018 according to data file received from T.Zholdybayev F076900300019 ENDBIB 17 0 F076900300020 NOCOMMON 0 0 F076900300021 DATA 4 2 F076900300022 EN EN-ERR DATA DATA-ERR F076900300023 MEV/A MEV/A MB MB F076900300024 23.2 0.5 1340. 40. F076900300025 26.5 0.3 1265. 50. F076900300026 ENDDATA 4 0 F076900300027 ENDSUBENT 26 0 F076900399999 SUBENT F0769004 20101001 F040F076900400001 BIB 3 15 F076900400002 REACTION (14-SI-28(2-HE-6,NON),,SIG) F076900400003 METHOD (TRN) Method of attenuation of alpha particle beam F076900400004 was used. Telescope detectors were used as a target, F076900400005 a detector and an energy absorber of incident ions. F076900400006 Total cross section was determined by the following F076900400007 way. Events in which the studied nucleus passed F076900400008 through the telescope to the full stop due to the F076900400009 ionizing losses only were subtracted from the whole F076900400010 data array of particular nucleus. As a result in data F076900400011 array only the events related to the nuclear F076900400012 reactions and inelastic scattering of the studied F076900400013 nucleus on silicon were kept. F076900400014 (EDE) Particle determination was performed using the F076900400015 results of the energy losses in delta E counters. F076900400016 STATUS (CURVE) Fig.4 F076900400017 ENDBIB 15 0 F076900400018 COMMON 3 3 F076900400019 DATA-ERR EN-ERR-DIG ERR-DIG F076900400020 PER-CENT MEV/A MB F076900400021 3. 0.1 1.37 F076900400022 ENDCOMMON 3 0 F076900400023 DATA 3 7 F076900400024 EN EN-ERR DATA F076900400025 MEV/A MEV/A MB F076900400026 8.731 1.7776 1.904E+03 F076900400027 13.348 1.8558 1.993E+03 F076900400028 15.143 1.8582 1.72E+03 F076900400029 18.643 1.7728 1.496E+03 F076900400030 21.597 1.7692 1.725E+03 F076900400031 25.102 2.0159 1.528E+03 F076900400032 27.522 1.6921 1.525E+03 F076900400033 ENDDATA 9 0 F076900400034 ENDSUBENT 33 0 F076900499999 ENDENTRY 4 0 F076999999999