ENTRY F1364 20181030 F070F136400000001 SUBENT F1364001 20181030 F070F136400100001 BIB 11 20 F136400100002 TITLE Energy distribution of neutrons emitted from F136400100003 beryllium bombarded by 680 MeV protons. F136400100004 AUTHOR (V.Kiselev,V.B.Fliagin) F136400100005 INSTITUTE (4ZZZDUB) F136400100006 REFERENCE (J,ZET,32,962,1957) F136400100007 (J,JET,5,786,1957) English translation F136400100008 FACILITY (SYNCY,4ZZZDUB) F136400100009 SAMPLE Berillium target of 2.5 cm thickness was used. F136400100010 DETECTOR (SCIN,TELES) Telescope of four scintillation F136400100011 detectors (three were connected for coincidence, the F136400100012 fourth for anticoincidence) was used. F136400100013 METHOD (DSCAT) The measurements were performed principally F136400100014 by differential method. The neutron energy F136400100015 distribution was investigated by determining the F136400100016 energy spectra of the recoil protons, emitted at a 30 F136400100017 degr. laboratory angle, as a result of elastic n-p F136400100018 scattering. F136400100019 ERR-ANALYS (ERR-S) Statistical error F136400100020 STATUS (CURVE) Figure from ZET,32,962,1957. F136400100021 HISTORY (20181030C) F136400100022 ENDBIB 20 0 F136400100023 COMMON 3 3 F136400100024 EN E-ERR-DIG ERR-DIG F136400100025 MEV MEV ARB-UNITS F136400100026 680. 0.86 0.0029 F136400100027 ENDCOMMON 3 0 F136400100028 ENDSUBENT 27 0 F136400199999 SUBENT F1364002 20181030 F070F136400200001 BIB 1 2 F136400200002 REACTION (4-BE-9(P,X)0-NN-1,,DA/DE,,REL) F136400200003 No explanation of relative units is given. F136400200004 ENDBIB 2 0 F136400200005 NOCOMMON 0 0 F136400200006 DATA 5 34 F136400200007 ANG E E-ERR DATA ERR-S F136400200008 ADEG MEV MEV ARB-UNITS ARB-UNITS F136400200009 0. 123.28 19.24 1.0138 0.1519 F136400200010 0. 165.34 20.45 0.8196 0.0970 F136400200011 0. 201.46 26.46 1.0347 0.1476 F136400200012 0. 224.32 26.46 1.0388 0.1139 F136400200013 0. 284.52 20.45 1.3635 0.1434 F136400200014 0. 294.14 15.64 1.3972 0.1055 F136400200015 0. 325.33 15.64 0.9753 0.0844 F136400200016 0. 328.92 14.43 0.8657 0.0886 F136400200017 0. 360.17 19.24 0.7348 0.2025 F136400200018 0. 376.96 16.84 0.4859 0.0886 F136400200019 0. 435.88 22.85 0.4140 0.0886 F136400200020 0. 480.38 20.45 0.4392 0.0675 F136400200021 0. 527.26 20.45 0.2831 0.0633 F136400200022 0. 576.69 18.04 0.8988 0.0675 F136400200023 0. 617.61 20.45 1.0042 0.0675 F136400200024 0. 664.44 19.24 0.6160 0.0675 F136400200025 0. 691.99 18.04 0.0465 0.1055 F136400200026 18. 114.05 10.86 0.8519 0.1008 F136400200027 18. 118.96 18.10 0.9527 0.0966 F136400200028 18. 158.82 16.89 1.0195 0.1050 F136400200029 18. 169.94 31.36 1.3640 0.1429 F136400200030 18. 198.75 14.48 1.1788 0.1219 F136400200031 18. 207.25 13.27 1.2544 0.1218 F136400200032 18. 218.12 28.96 1.2711 0.1302 F136400200033 18. 256.55 14.48 1.0354 0.1303 F136400200034 18. 278.37 26.54 1.1739 0.1513 F136400200035 18. 338.31 24.13 0.6859 0.0966 F136400200036 18. 377.92 26.54 0.4251 0.1051 F136400200037 18. 449.29 21.71 0.6807 0.0924 F136400200038 18. 483.30 20.51 0.9787 0.0882 F136400200039 18. 544.79 20.51 0.9319 0.0924 F136400200040 18. 595.21 20.51 0.6121 0.0798 F136400200041 18. 639.55 16.89 0.2210 0.0798 F136400200042 18. 687.72 18.10 0.1155 0.1008 F136400200043 ENDDATA 36 0 F136400200044 ENDSUBENT 43 0 F136400299999 ENDENTRY 2 0 F136499999999