ENTRY E1931 20091026 E059E193100000001 SUBENT E1931001 20091026 E059E193100100001 BIB 12 37 E193100100002 TITLE Quasielastic scattering of 6He on 9Be at 25 E193100100003 MeV/nucleon E193100100004 AUTHOR (Y.L.Ye, D.Y.Pang, D.X.Jiang, T.Zheng, Q.J.Wang, E193100100005 Z.H.Li, X.Q.Li, Y.C.Ge, C.Wu, G.L.Zhang, Q.Y.Hu, E193100100006 J.Wang, Z.Q.Chen, A.Ozawa, Y.Yamaguchi, R.Kanungo, E193100100007 I.Tanihata) E193100100008 INSTITUTE (3CPRBJG) School of Physics and MOE Key Laboratory of E193100100009 Heavy Ion Physics E193100100010 (2JPNIPC) E193100100011 REFERENCE (J,PR/C,71,(1),014604,200501) Main reference E193100100012 Main reference. See also TITLE and AUTHOR. E193100100013 (W,YE,20050723) E193100100014 Influence of inelastic scattering to the data given E193100100015 (J,JP/G,31,(10),S1647,200510) E193100100016 PART-DET (2-HE-6) E193100100017 SAMPLE - Chemical-form of target is element. E193100100018 - Physical-form of target is solid. E193100100019 - Target-thickness: 100 micro-meter (tilted 45 deg E193100100020 with respect to beam direction) E193100100021 METHOD (TOF) To eliminate the contamination of 6He beam E193100100022 FACILITY (CYCLO,2JPNIPC) Secondary beam produced by E193100100023 fragmentation of 70 MeV/nucleon 13C E193100100024 primary beam on thick 9Be target E193100100025 (PRJFS,2JPNIPC) RIKEN Projectile Fragment Separator E193100100026 (RIPS) E193100100027 DETECTOR (TELES,SCIN,SIBAR,CSICR) To detect outgoing particles E193100100028 ERR-ANALYS (ERR-SYS) Uncertainties in determining the E193100100029 quasielastic peak in energy spectrum, solid E193100100030 angle and number of incident 6He ions (-15%) E193100100031 ADD-RES E1931.003:4-BE-9(2-HE-6,EL)4-BE-9 E193100100032 Optical potential parameter E193100100033 See NRDF D1931 DATA,2 for detail. E193100100034 (COMP) Optical model (Code ECIS97 [J. Raynal, E193100100035 coupled-channel code ECIS97 (unpublished)]) E193100100036 HISTORY (20050711C) Kc + On E193100100037 (20061004A) On. Reference (NUSTAR'05) added E193100100038 (20090823U) Nf. REFERENCE: JP/S -> JP/G E193100100039 ENDBIB 37 0 E193100100040 COMMON 2 3 E193100100041 EN ERR-SYS E193100100042 MEV/A PER-CENT E193100100043 25. 15. E193100100044 ENDCOMMON 3 0 E193100100045 ENDSUBENT 44 0 E193100199999 SUBENT E1931002 20060411 E036E193100200001 BIB 4 13 E193100200002 REACTION 1(4-BE-9(2-HE-6,EL)4-BE-9,,DA) E193100200003 Quasielastic scattering (Elastic + Little influence of E193100200004 5/2- state at 2.43 MeV and7/2- state at 6.76 MeV) E193100200005 2(4-BE-9(2-HE-6,EL)4-BE-9,,DA,,RTH) E193100200006 Quasielastic scattering (Elastic + Little influence of E193100200007 5/2- state at 2.43 MeV and7/2- state at 6.76 MeV) E193100200008 EN-SEC ANG-CM is polar angle between beam and 6He in center E193100200009 of mass system E193100200010 ERR-ANALYS (ERR-S) Statistical uncertainty E193100200011 STATUS (TABLE) Data (Fig.7, p014604-5 in reference for E193100200012 Rutherford ratio, not shown for absolute cross E193100200013 section) received from Y.L.Ye by e-mail E193100200014 (2005.05.07) E193100200015 ENDBIB 13 0 E193100200016 NOCOMMON 0 0 E193100200017 DATA 5 10 E193100200018 ANG-CM ANG-RSL DATA-CM 1ERR-S 1DATA-CM 2 E193100200019 ADEG ADEG MB/SR MB/SR NO-DIM E193100200020 2.500E+00 2.500E+00 2.550E+05 6.940E+04 2.190E+00 E193100200021 5.000E+00 2.500E+00 2.650E+04 5.120E+03 7.560E+00 E193100200022 7.500E+00 2.500E+00 3.150E+03 7.800E+02 5.120E+00 E193100200023 1.000E+01 2.500E+00 1.160E+03 1.690E+02 6.180E+00 E193100200024 1.250E+01 2.500E+00 2.650E+02 1.080E+02 3.510E+00 E193100200025 1.370E+01 4.570E+00 2.170E+02 1.080E+01 3.920E+00 E193100200026 2.070E+01 8.180E+00 6.890E+01 4.640E+00 6.120E+00 E193100200027 2.640E+01 4.560E+00 2.820E+01 5.090E-01 7.350E+00 E193100200028 3.320E+01 7.850E+00 1.230E+01 2.350E-01 7.650E+00 E193100200029 4.970E+01 7.760E+00 1.790E+00 5.280E-02 5.330E+00 E193100200030 ENDDATA 12 0 E193100200031 ENDSUBENT 30 0 E193100299999 NOSUBENT E1931003 20060411 E036E193100300001 ENDENTRY 3 0 E193199999999