ENTRY M0347 20180218 M095M034700000001 SUBENT M0347001 20180218 M095M034700100001 BIB 9 15 M034700100002 TITLE Photodisintegration of copper. M034700100003 AUTHOR (P.R.Byerly Jr,W.E.Stephens) M034700100004 REFERENCE (J,PR,83,(1),54,1951) M034700100005 INSTITUTE (1USAPEN) M034700100006 FACILITY (BETAT,1USAPEN) M034700100007 INC-SOURCE (BRST) M034700100008 SAMPLE A 0.0004 in. thick copper foil was used. M034700100009 REL-REF (M,,M.E.Toms+,J,PR,82,709,1951). M034700100010 The description of the setup. M034700100011 HISTORY (19870828C) Data were compiled in SCJAD of Saratov M034700100012 State University. M034700100013 (20180218U) Corrected by SD and VV: Updated to new M034700100014 date formats, lower case, REACTION, STATUS M034700100015 updated in all SUBENTs, SUBENTs 006 and 007 deleted M034700100016 because a single data point in arb. units. M034700100017 ENDBIB 15 0 M034700100018 NOCOMMON 0 0 M034700100019 ENDSUBENT 18 0 M034700199999 SUBENT M0347002 20180218 M095M034700200001 BIB 8 15 M034700200002 REACTION (29-CU-0(G,X)1-H-2,,DE,,BRA/REL) M034700200003 DETECTOR (PLATE) The 100 mu thick Ilford C-2 emulsions (1/2 M034700200004 in. x 1 in.) were used. M034700200005 CORRECTION The energy spectrum was corrected for the probability M034700200006 that deuteron tracks end outside the emulsion. M034700200007 ADD-RES (COMP) The evaporation model was used. M034700200008 COMMENT It was noted that the large number of observed M034700200009 deutrons cannot be explained within the evaporation M034700200010 model. M034700200011 (E-ERR) half of the range of the experimental M034700200012 histogram. M034700200013 ERR-ANALYS No information about sources of uncertainties. M034700200014 STATUS (CURVE) Data from Fig. 5 of PR,83,54,1981. M034700200015 HISTORY (20180218A) Corrected by SD and VV: PART-DET deleted, M034700200016 REACTION, STATUS. M034700200017 ENDBIB 15 0 M034700200018 COMMON 2 3 M034700200019 EN-MAX E-ERR M034700200020 MEV MEV M034700200021 24. 0.25 M034700200022 ENDCOMMON 3 0 M034700200023 DATA 2 9 M034700200024 E DATA M034700200025 MEV ARB-UNITS M034700200026 2.75 5. M034700200027 3.25 9. M034700200028 3.75 17. M034700200029 4.25 4. M034700200030 4.75 7. M034700200031 5.25 2. M034700200032 5.75 1. M034700200033 6.25 0. M034700200034 6.75 1. M034700200035 ENDDATA 11 0 M034700200036 ENDSUBENT 35 0 M034700299999 SUBENT M0347003 20180218 M095M034700300001 BIB 8 14 M034700300002 REACTION (29-CU-0(G,X)1-H-1,,DE,,BRA/REL) M034700300003 DETECTOR (PLATE) The 200 mu thick Ilford C-2 emulsions (1/2 M034700300004 in. x 1 in.) were used. M034700300005 CORRECTION The energy spectrum was corrected for the probability M034700300006 that proton tracks end outside the emulsion. M034700300007 ADD-RES (COMP) The evaporation model was used. M034700300008 COMMENT The part of the 'direct' protons was equal to about M034700300009 10%. M034700300010 (E-ERR) half of the range of the experimental M034700300011 histogram. M034700300012 ERR-ANALYS No information about sources of uncertainties. M034700300013 STATUS (CURVE) Data from Fig. 7 of PR,83,54,1981. M034700300014 HISTORY (20180218A) Corrected by SD and VV: PART-DET deleted, M034700300015 REACTION, STATUS. M034700300016 ENDBIB 14 0 M034700300017 COMMON 2 3 M034700300018 EN-MAX E-ERR M034700300019 MEV MEV M034700300020 24. 0.25 M034700300021 ENDCOMMON 3 0 M034700300022 DATA 2 28 M034700300023 E DATA M034700300024 MEV ARB-UNITS M034700300025 2.75 17. M034700300026 3.25 41. M034700300027 3.75 70. M034700300028 4.25 103. M034700300029 4.75 141. M034700300030 5.25 163. M034700300031 5.75 135. M034700300032 6.25 119. M034700300033 6.75 125. M034700300034 7.25 76. M034700300035 7.75 67. M034700300036 8.25 65. M034700300037 8.75 59. M034700300038 9.25 46. M034700300039 9.75 29. M034700300040 10.25 25. M034700300041 10.75 17. M034700300042 11.25 9. M034700300043 11.75 13. M034700300044 12.25 7. M034700300045 12.75 5. M034700300046 13.25 1. M034700300047 13.75 3. M034700300048 14.25 3. M034700300049 14.75 1. M034700300050 15.25 2. M034700300051 15.75 0. M034700300052 16.25 1. M034700300053 ENDDATA 30 0 M034700300054 ENDSUBENT 53 0 M034700399999 SUBENT M0347004 20180218 M095M034700400001 BIB 9 19 M034700400002 REACTION (29-CU-0(G,X)0-NN-1,,DE,,BRA/REL) M034700400003 METHOD (REC) M034700400004 DETECTOR (PLATE) The 100 mu thick Ilford C-2 emulsions (1 in. M034700400005 x 3 in.) were used. M034700400006 CORRECTION The energy spectrum was corrected for M034700400007 (a) the dependence of the (n,p) cross section on M034700400008 neutron energy, M034700400009 (b) the probability that proton tracks end outside M034700400010 the emulsion, M034700400011 (c) the background. M034700400012 ADD-RES (COMP) The evaporation model was used. M034700400013 COMMENT The part of the 'direct' neutrons was equal to about M034700400014 10%. M034700400015 (E-ERR) half of the range of the experimental M034700400016 histogram. M034700400017 ERR-ANALYS No information about sources of uncertainties. M034700400018 STATUS (CURVE) Data from Fig. 10 of PR,83,54,1981. M034700400019 HISTORY (20180218A) Corrected by SD and VV: PART-DET deleted, M034700400020 REACTION, STATUS. M034700400021 ENDBIB 19 0 M034700400022 COMMON 2 3 M034700400023 EN-MAX E-ERR M034700400024 MEV MEV M034700400025 24. 0.25 M034700400026 ENDCOMMON 3 0 M034700400027 DATA 2 21 M034700400028 E DATA M034700400029 MEV ARB-UNITS M034700400030 0.75 34.0 M034700400031 1.25 59.6 M034700400032 1.75 41.9 M034700400033 2.25 29.9 M034700400034 2.75 32.0 M034700400035 3.25 20.0 M034700400036 3.75 16.0 M034700400037 4.25 6.0 M034700400038 4.75 4.9 M034700400039 5.25 10.0 M034700400040 5.75 6.4 M034700400041 6.25 6.8 M034700400042 6.75 5.3 M034700400043 7.25 2.9 M034700400044 7.75 0.0 M034700400045 8.25 0.0 M034700400046 8.75 0.8 M034700400047 9.25 1.1 M034700400048 9.75 0.0 M034700400049 10.25 0.0 M034700400050 10.75 1.1 M034700400051 ENDDATA 23 0 M034700400052 ENDSUBENT 51 0 M034700499999 SUBENT M0347005 20180218 M095M034700500001 BIB 9 12 M034700500002 REACTION (29-CU-0(G,X)2-HE-4,,DE,,BRA/REL) M034700500003 PART-DET (A) M034700500004 DETECTOR (PLATE) The 200 mu thick Ilford C-2 emulsions (1/2 M034700500005 in. x 1 in.) were used. M034700500006 CORRECTION The energy spectrum was corrected for the probability M034700500007 that alpha-particle tracks end outside the emulsion. M034700500008 ADD-RES (COMP) The evaporation model was used. M034700500009 COMMENT (E-ERR) half of the range of the experimental M034700500010 histogram. M034700500011 ERR-ANALYS No information about sources of uncertainties. M034700500012 STATUS (CURVE) Data from Fig. 9 of PR,83,54,1981. M034700500013 HISTORY (20180218U) Corrected by SD and VV: REACTION, STATUS. M034700500014 ENDBIB 12 0 M034700500015 COMMON 2 3 M034700500016 EN-MAX E-ERR M034700500017 MEV MEV M034700500018 24. 0.25 M034700500019 ENDCOMMON 3 0 M034700500020 DATA 2 9 M034700500021 E DATA M034700500022 MEV ARB-UNITS M034700500023 5.75 2.3 M034700500024 6.25 6.9 M034700500025 6.75 2.3 M034700500026 7.25 8.9 M034700500027 7.75 6.6 M034700500028 8.25 10.3 M034700500029 8.75 5.1 M034700500030 9.25 2.9 M034700500031 9.75 2.4 M034700500032 ENDDATA 11 0 M034700500033 ENDSUBENT 32 0 M034700599999 NOSUBENT M0347006 20180218 M095M034700600001 NOSUBENT M0347007 20180218 M095M034700700001 SUBENT M0347008 20180218 M095M034700800001 BIB 6 7 M034700800002 REACTION (29-CU-0(G,X)ELEM/MASS,,SIG,,BRA/REL) M034700800003 COMMENT Arb. units = 10**6* particles/mole/roentgen. M034700800004 ANALYSIS The yield was determined from the solid angles of M034700800005 observed tracks. M034700800006 ERR-ANALYS (DATA-ERR) The uncertainties of the yield. M034700800007 STATUS (TABLE) Data from the text on p.59 of PR,83,54,1951. M034700800008 HISTORY (20180218U) Corrected by SD and VV: REACTION, STATUS. M034700800009 ENDBIB 7 0 M034700800010 COMMON 2 3 M034700800011 EN-MAX DATA-ERR M034700800012 MEV PER-CENT M034700800013 24. 50. M034700800014 ENDCOMMON 3 0 M034700800015 DATA 3 3 M034700800016 ELEMENT MASS DATA M034700800017 NO-DIM NO-DIM ARB-UNITS M034700800018 1. 1. 1.07 M034700800019 1. 2. 0.34 M034700800020 2. 4. 0.04 M034700800021 ENDDATA 5 0 M034700800022 ENDSUBENT 21 0 M034700899999 SUBENT M0347009 20180218 M095M034700900001 BIB 6 12 M034700900002 REACTION (29-CU-63(G,N)29-CU-62,,SIG,,BRS) M034700900003 METHOD (ACTIV) M034700900004 ANALYSIS The excitation curve of Cu-62 was taken by varying M034700900005 the produced radioactivity.The cross-section curve M034700900006 was calculated from this excitation curve and the M034700900007 X-ray photon energy distribution. M034700900008 REL-REF (M,,H.E.Johns+,J,PR,80,1062,1950) M034700900009 The description of the method of the cross-section M034700900010 calculation. M034700900011 STATUS (CURVE) Data from Fig. 11 of PR,83,54,1951. M034700900012 HISTORY (20180218A) Corrected by SD and VV: SF9 = EXP deleted M034700900013 from REACTION, STATUS. M034700900014 ENDBIB 12 0 M034700900015 NOCOMMON 0 0 M034700900016 DATA 2 13 M034700900017 EN DATA M034700900018 MEV B M034700900019 12. 0.008 M034700900020 13. 0.017 M034700900021 14. 0.032 M034700900022 15. 0.046 M034700900023 16. 0.069 M034700900024 17. 0.095 M034700900025 18. 0.091 M034700900026 19. 0.087 M034700900027 20. 0.065 M034700900028 21. 0.021 M034700900029 22. 0.037 M034700900030 23. 0.008 M034700900031 24. 0.030 M034700900032 ENDDATA 15 0 M034700900033 ENDSUBENT 32 0 M034700999999 ENDENTRY 9 0 M034799999999