ENTRY F0899 20160423 F062F089900000001 SUBENT F0899001 20160423 F062F089900100001 BIB 6 12 F089900100002 TITLE Energy dependence of the cross-section and polarizationF089900100003 of protons in elastic scattering by 27Al F089900100004 AUTHOR (I.R.Gulamov,T.N.Mikhaleva,E.A.Romanovskii, F089900100005 D.L.Chuprunov) F089900100006 INSTITUTE (4RUSMOS) F089900100007 REFERENCE (J,IZV,38,130,1974) F089900100008 (J,BAS,38,(1),114,1974) Engl.transl.of IZV,38,130,1974 F089900100009 FACILITY (CYCLO,4RUSMOS) F089900100010 HISTORY (20080202C) F089900100011 (20160423A) SD: Issue numb. was added to ref. BAS,38. F089900100012 Small corrections in all Subents. Subent 004 was F089900100013 deleted (see ADD-RES in Subent 003). F089900100014 ENDBIB 12 0 F089900100015 NOCOMMON 0 0 F089900100016 ENDSUBENT 15 0 F089900199999 SUBENT F0899002 20160423 F062F089900200001 BIB 5 5 F089900200002 REACTION (13-AL-27(P,EL)13-AL-27,,DA,,REL) F089900200003 DETECTOR (SCIN) F089900200004 SAMPLE Al target of 0.5 mu-m thicknesses was used. F089900200005 STATUS (CURVE)Fig.1 of IZV,38,130,1974 F089900200006 HISTORY (20160423A) SD: SF8=AV deleted from REACTION code. F089900200007 ENDBIB 5 0 F089900200008 COMMON 3 3 F089900200009 EN-ERR-DIG ERR-DIG EN-RSL F089900200010 MEV ARB-UNITS KEV F089900200011 0.002 15. 10. F089900200012 ENDCOMMON 3 0 F089900200013 DATA 3 94 F089900200014 ANG EN DATA F089900200015 ADEG MEV ARB-UNITS F089900200016 70. 6.212 3549. F089900200017 70. 6.217 3382. F089900200018 70. 6.222 3265. F089900200019 70. 6.233 2904. F089900200020 70. 6.245 3156. F089900200021 70. 6.253 2951. F089900200022 70. 6.273 3144. F089900200023 70. 6.285 3124. F089900200024 70. 6.292 2830. F089900200025 70. 6.298 2489. F089900200026 70. 6.308 2215. F089900200027 70. 6.324 2370. F089900200028 70. 6.331 2535. F089900200029 70. 6.344 2544. F089900200030 70. 6.353 2426. F089900200031 70. 6.362 2211. F089900200032 70. 6.373 2015. F089900200033 70. 6.382 1946. F089900200034 70. 6.391 2023. F089900200035 70. 6.401 2227. F089900200036 70. 6.413 2441. F089900200037 70. 6.432 2273. F089900200038 70. 6.449 2067. F089900200039 70. 6.462 2359. F089900200040 70. 6.492 2366. F089900200041 70. 6.510 2023. F089900200042 70. 6.523 1974. F089900200043 70. 6.534 2002. F089900200044 70. 6.543 2099. F089900200045 70. 6.554 2137. F089900200046 70. 6.564 2194. F089900200047 70. 6.584 2066. F089900200048 70. 6.591 1841. F089900200049 70. 6.612 1635. F089900200050 70. 6.639 1886. F089900200051 70. 6.651 2285. F089900200052 70. 6.661 2479. F089900200053 70. 6.668 2420. F089900200054 70. 6.670 2527. F089900200055 70. 6.682 2331. F089900200056 70. 6.700 2388. F089900200057 70. 6.701 2320. F089900200058 70. 6.722 2318. F089900200059 70. 6.731 2395. F089900200060 70. 6.740 2492. F089900200061 90. 6.208 1641. F089900200062 90. 6.216 1485. F089900200063 90. 6.230 1434. F089900200064 90. 6.239 1491. F089900200065 90. 6.250 1558. F089900200066 90. 6.262 1498. F089900200067 90. 6.270 1380. F089900200068 90. 6.280 1165. F089900200069 90. 6.288 989. F089900200070 90. 6.298 871. F089900200071 90. 6.312 996. F089900200072 90. 6.322 1179. F089900200073 90. 6.332 1401. F089900200074 90. 6.340 1574. F089900200075 90. 6.349 1729. F089900200076 90. 6.359 1698. F089900200077 90. 6.372 1531. F089900200078 90. 6.379 1375. F089900200079 90. 6.390 1334. F089900200080 90. 6.402 1352. F089900200081 90. 6.410 1419. F089900200082 90. 6.419 1544. F089900200083 90. 6.429 1951. F089900200084 90. 6.445 2230. F089900200085 90. 6.459 2102. F089900200086 90. 6.470 1955. F089900200087 90. 6.481 1720. F089900200088 90. 6.489 1632. F089900200089 90. 6.506 1629. F089900200090 90. 6.519 1618. F089900200091 90. 6.527 1539. F089900200092 90. 6.529 1442. F089900200093 90. 6.538 1295. F089900200094 90. 6.539 1402. F089900200095 90. 6.550 1381. F089900200096 90. 6.561 1525. F089900200097 90. 6.577 1290. F089900200098 90. 6.588 1055. F089900200099 90. 6.603 1072. F089900200100 90. 6.610 1149. F089900200101 90. 6.629 1137. F089900200102 90. 6.637 1058. F089900200103 90. 6.650 1124. F089900200104 90. 6.668 1122. F089900200105 90. 6.697 991. F089900200106 90. 6.709 1077. F089900200107 90. 6.717 1358. F089900200108 90. 6.726 1560. F089900200109 90. 6.739 1792. F089900200110 ENDDATA 96 0 F089900200111 ENDSUBENT 110 0 F089900299999 SUBENT F0899003 20160423 F062F089900300001 BIB 8 10 F089900300002 REACTION (13-AL-27(P,EL)13-AL-27,,POL/DA) F089900300003 DETECTOR (PLATE,SCIN) Carbon polarimeters were employed both F089900300004 with photographic detection of the twice-scattered F089900300005 protons and with semiconductor detectors. F089900300006 SAMPLE Al target of 1.08 mg/cm2 thickness was used. F089900300007 METHOD (DSCAT) F089900300008 ADD-RES Sample thickness dependence of polarization was given.F089900300009 ERR-ANALYS (DATA-ERR) No information on source of uncertainties F089900300010 STATUS (CURVE) Fig.2 of IZV,38,130,1974 F089900300011 HISTORY (20160423A) SD: Data divided by 100. F089900300012 ENDBIB 10 0 F089900300013 COMMON 5 3 F089900300014 ANG EN-ERR-DIG ERR-DIG DATA-ERR EN-RSL F089900300015 ADEG MEV NO-DIM NO-DIM KEV F089900300016 60. 0.006 0.05 0.01 30. F089900300017 ENDCOMMON 3 0 F089900300018 DATA 2 8 F089900300019 EN DATA F089900300020 MEV NO-DIM F089900300021 6.238 0.10 F089900300022 6.284 0.11 F089900300023 6.331 0.07 F089900300024 6.361 0.09 F089900300025 6.407 -0.04 F089900300026 6.430 -0.10 F089900300027 6.451 -0.03 F089900300028 6.481 -0.06 F089900300029 ENDDATA 10 0 F089900300030 ENDSUBENT 29 0 F089900399999 NOSUBENT F0899004 20160423 F062F089900400001 ENDENTRY 4 0 F089999999999