ENTRY F1355 20180702 F068F135500000001 SUBENT F1355001 20180702 F068F135500100001 BIB 10 17 F135500100002 TITLE The stripping process in the interactions of F135500100003 accelerated N-14 ions with the nuclei of some elements.F135500100004 AUTHOR (V.V.Volkov,A.S.Pasyuk,G.N.Flerov) F135500100005 REFERENCE (J,ZET,33,595,1957) F135500100006 (J,JET,6,459,1958) English translation F135500100007 (C,57MOSCOW,,513,1957) F135500100008 INSTITUTE (4RUSKUR) F135500100009 FACILITY (CYCLO,4RUSKUR) F135500100010 DETECTOR (GEMUC) Magnetic analyzer was used to determine the F135500100011 sign of the beta particles. F135500100012 ANALYSIS (DECAY) F135500100013 DECAY-DATA (7-N-13,10.MIN,B) F135500100014 SAMPLE Targets made of Al, Ni, Cu, Ag, Cd, Sn, Pt, Au, and F135500100015 Pb were used. The target thickness was such that the F135500100016 particle energy after traversing the target did not F135500100017 exceed 70 Mev. F135500100018 HISTORY (20180702C) F135500100019 ENDBIB 17 0 F135500100020 NOCOMMON 0 0 F135500100021 ENDSUBENT 20 0 F135500199999 SUBENT F1355002 20180702 F068F135500200001 BIB 4 11 F135500200002 REACTION (28-NI-0(7-N-14,X)7-N-13,,DA,,REL) F135500200003 No explanation of relative units is given. F135500200004 METHOD N-13 were stopped in the collector made of 3.5 mu-m F135500200005 lead foil. Lead collector was put into the form of a F135500200006 cylindrical surface which included all angles from + F135500200007 60 to -60 degrees. After irradiation the collector F135500200008 was cut into equal strips for measurement of the F135500200009 beta-activity decay curve. F135500200010 ERR-ANALYS (DATA-ERR) Statistical errors and the angular spread F135500200011 due to the finite size of the strips are given. F135500200012 STATUS (CURVE) Fig.2 a F135500200013 ENDBIB 11 0 F135500200014 COMMON 4 3 F135500200015 EN EN-ERR ANG-ERR-D ERR-DIG F135500200016 MEV MEV ADEG ARB-UNITS F135500200017 56. 6. 0.416 0.0057 F135500200018 ENDCOMMON 3 0 F135500200019 DATA 4 12 F135500200020 ANG-CM ANG-ERR DATA-CM DATA-ERR F135500200021 ADEG ADEG ARB-UNITS ARB-UNITS F135500200022 -78.827 7.041 0.0917 0.0888 F135500200023 -66.576 5.281 0.1868 0.0888 F135500200024 -57.283 7.041 0.6803 0.1110 F135500200025 -45.988 7.921 1.9747 0.1555 F135500200026 -34.320 8.802 2.8027 0.1333 F135500200027 -23.930 10.562 1.9192 0.1110 F135500200028 -15.708 10.562 1.5457 0.1110 F135500200029 21.188 9.682 1.6533 0.0888 F135500200030 29.547 8.802 2.2130 0.1110 F135500200031 39.525 7.921 2.9512 0.1555 F135500200032 49.371 7.921 1.6454 0.2887 F135500200033 66.258 6.161 0.3431 0.0888 F135500200034 ENDDATA 14 0 F135500200035 ENDSUBENT 34 0 F135500299999 SUBENT F1355003 20180702 F068F135500300001 BIB 4 11 F135500300002 REACTION (79-AU-197(7-N-14,X)7-N-13,,DA,,REL) F135500300003 No explanation of relative units is given. F135500300004 METHOD N-13 were stopped in the collector made of 3.5 mu-m F135500300005 lead foil. Lead collector was put into the form of a F135500300006 cylindrical surface which included all angles from + F135500300007 60 to -60 degrees. After irradiation the collector F135500300008 was cut into equal strips for measurement of the F135500300009 beta-activity decay curve. F135500300010 ERR-ANALYS (DATA-ERR) Statistical errors and the angular spread F135500300011 due to the finite size of the strips are given. F135500300012 STATUS (CURVE) Fig.2 b F135500300013 ENDBIB 11 0 F135500300014 COMMON 4 3 F135500300015 EN EN-ERR ANG-ERR-D ERR-DIG F135500300016 MEV MEV ADEG ARB-UNITS F135500300017 64. 8. 0.524 0.0073 F135500300018 ENDCOMMON 3 0 F135500300019 DATA 4 9 F135500300020 ANG-CM ANG-ERR DATA-CM DATA-ERR F135500300021 ADEG ADEG ARB-UNITS ARB-UNITS F135500300022 -75.263 6.015 1.5554 0.1123 F135500300023 -62.834 6.015 4.3701 0.1796 F135500300024 -51.797 6.874 2.3316 0.1123 F135500300025 -41.038 6.874 0.6525 0.0898 F135500300026 -30.570 8.592 0.4559 0.0898 F135500300027 30.383 6.874 0.5556 0.0898 F135500300028 39.665 6.015 1.8859 0.1347 F135500300029 49.523 6.015 2.4752 0.1572 F135500300030 59.520 5.155 2.8849 0.2695 F135500300031 ENDDATA 11 0 F135500300032 ENDSUBENT 31 0 F135500399999 SUBENT F1355004 20180702 F068F135500400001 BIB 4 11 F135500400002 REACTION (82-PB-0(7-N-14,X)7-N-13,,DA,,REL) F135500400003 No explanation of relative units is given. F135500400004 METHOD N-13 were stopped in the collector made of 3.5 mu-m F135500400005 lead foil. Lead collector was put into the form of a F135500400006 cylindrical surface which included all angles from + F135500400007 60 to -60 degrees. After irradiation the collector F135500400008 was cut into equal strips for measurement of the F135500400009 beta-activity decay curve. F135500400010 ERR-ANALYS (DATA-ERR) Statistical errors and the angular spread F135500400011 due to the finite size of the strips are given. F135500400012 STATUS (CURVE) Fig.2 c F135500400013 ENDBIB 11 0 F135500400014 COMMON 4 3 F135500400015 EN EN-ERR ANG-ERR-D ERR-DIG F135500400016 MEV MEV ADEG ARB-UNITS F135500400017 60. 7. 0.159 0.0055 F135500400018 ENDCOMMON 3 0 F135500400019 DATA 4 9 F135500400020 ANG-CM ANG-ERR DATA-CM DATA-ERR F135500400021 ADEG ADEG ARB-UNITS ARB-UNITS F135500400022 -72.804 5.2836 2.5235 0.2695 F135500400023 -62.054 4.4030 4.4168 0.2920 F135500400024 -51.949 7.0447 1.8158 0.2021 F135500400025 -40.085 7.0447 0.2718 0.0898 F135500400026 -30.417 7.9253 0.2995 0.1123 F135500400027 31.469 7.0447 0.0411 0.0898 F135500400028 40.106 7.0447 0.2480 0.2471 F135500400029 51.454 6.1641 2.4788 0.2471 F135500400030 57.750 4.4030 2.3249 0.5390 F135500400031 ENDDATA 11 0 F135500400032 ENDSUBENT 31 0 F135500499999 SUBENT F1355005 20180702 F068F135500500001 BIB 4 11 F135500500002 REACTION (78-PT-0(7-N-14,X)7-N-13,,DA,,REL) F135500500003 No explanation of relative units is given. F135500500004 METHOD N-13 were stopped in the collector made of 3.5 mu-m F135500500005 lead foil. Lead collector was put into the form of a F135500500006 cylindrical surface which included all angles from + F135500500007 60 to -60 degrees. After irradiation the collector F135500500008 was cut into equal strips for measurement of the F135500500009 beta-activity decay curve. F135500500010 ERR-ANALYS (DATA-ERR) Statistical errors and the angular spread F135500500011 due to the finite size of the strips are given. F135500500012 STATUS (CURVE) Fig.2 d F135500500013 ENDBIB 11 0 F135500500014 COMMON 4 3 F135500500015 EN EN-ERR ANG-ERR-D ERR-DIG F135500500016 MEV MEV ADEG ARB-UNITS F135500500017 81. 7. 0.335 0.0094 F135500500018 ENDCOMMON 3 0 F135500500019 DATA 4 9 F135500500020 ANG-CM ANG-ERR DATA-CM DATA-ERR F135500500021 ADEG ADEG ARB-UNITS ARB-UNITS F135500500022 -68.666 4.297 3.4541 0.2246 F135500500023 -58.847 5.156 2.3376 0.1797 F135500500024 -47.261 5.156 0.3910 0.1123 F135500500025 -37.563 6.875 0.1735 0.1123 F135500500026 -28.822 8.594 0.0451 0.0674 F135500500027 25.959 7.735 0.2882 0.1572 F135500500028 36.199 6.875 0.3633 0.0898 F135500500029 46.364 4.297 0.5057 0.0898 F135500500030 54.618 4.297 2.3997 0.1123 F135500500031 ENDDATA 11 0 F135500500032 ENDSUBENT 31 0 F135500599999 SUBENT F1355006 20180702 F068F135500600001 BIB 4 14 F135500600002 REACTION (28-NI-0(7-N-14,X)7-N-13,,SIG) F135500600003 METHOD The number of N-13 nuclei was determined by F135500600004 separation of the ten-minute activity in the lead F135500600005 collectors. The efficiency of the beta particle F135500600006 detection was determined by means of a radioactive F135500600007 source of known intensity. F135500600008 ERR-ANALYS (DATA-ERR1) The error in determining the absolute F135500600009 value of the cross section was caused principally F135500600010 by lack of accurate knowledge concerning the F135500600011 efficiency of detection of the beta particles. F135500600012 (DATA-ERR2) Error of the relative measurements as F135500600013 well as the energy spread due to the finite target F135500600014 thickness are given. F135500600015 STATUS (CURVE) Fig.5 from J,JET,6,459,1958 F135500600016 ENDBIB 14 0 F135500600017 COMMON 3 3 F135500600018 DATA-ERR1 EN-ERR-DIG ERR-DIG F135500600019 PER-CENT MEV PER-CENT F135500600020 30. 0.296 1.8 F135500600021 ENDCOMMON 3 0 F135500600022 DATA 4 7 F135500600023 EN EN-ERR DATA DATA-ERR2 F135500600024 MEV MEV B B F135500600025 30.592 4.679 4.8480E-04 1.9396E-04 F135500600026 45.066 3.509 9.7403E-03 8.3986E-04 F135500600027 55.101 2.924 1.8241E-02 1.5728E-03 F135500600028 70.347 3.509 2.3768E-02 2.0493E-03 F135500600029 82.080 7.604 3.0093E-02 2.5947E-03 F135500600030 98.513 5.849 4.4201E-02 5.0071E-03 F135500600031 106.660 3.509 3.2623E-02 6.9726E-03 F135500600032 ENDDATA 9 0 F135500600033 ENDSUBENT 32 0 F135500699999 SUBENT F1355007 20180702 F068F135500700001 BIB 4 14 F135500700002 REACTION (13-AL-27(7-N-14,X)7-N-13,,SIG) F135500700003 METHOD The number of N-13 nuclei was determined by F135500700004 separation of the ten-minute activity in the lead F135500700005 collectors. The efficiency of the beta particle F135500700006 detection was determined by means of a radioactive F135500700007 source of known intensity. F135500700008 ERR-ANALYS (DATA-ERR1) The error in determining the absolute F135500700009 value of the cross section was caused principally F135500700010 by lack of accurate knowledge concerning the F135500700011 efficiency of detection of the beta particles. F135500700012 (DATA-ERR2) Error of the relative measurements as F135500700013 well as the energy spread due to the finite target F135500700014 thickness are given. F135500700015 STATUS (CURVE) Fig.5 from J,JET,6,459,1958 F135500700016 ENDBIB 14 0 F135500700017 COMMON 3 3 F135500700018 DATA-ERR1 EN-ERR-DIG ERR-DIG F135500700019 PER-CENT MEV PER-CENT F135500700020 30. 0.109 0.6 F135500700021 ENDCOMMON 3 0 F135500700022 DATA 4 9 F135500700023 EN EN-ERR DATA DATA-ERR2 F135500700024 MEV MEV B B F135500700025 26.668 4.524 1.0222E-03 3.3019E-04 F135500700026 38.103 3.231 4.2576E-03 3.0746E-04 F135500700027 48.119 2.585 7.6688E-03 4.4633E-04 F135500700028 66.811 2.908 1.2498E-02 1.0751E-03 F135500700029 74.195 2.900 1.1326E-02 1.1282E-03 F135500700030 80.586 2.585 9.8228E-03 1.1101E-03 F135500700031 84.891 3.231 1.1879E-02 1.6536E-03 F135500700032 90.934 3.231 9.8529E-03 2.5523E-03 F135500700033 97.106 2.585 1.0388E-02 3.7624E-03 F135500700034 ENDDATA 11 0 F135500700035 ENDSUBENT 34 0 F135500799999 ENDENTRY 7 0 F135599999999