ENTRY D6262 20170307 D110D626200000001 SUBENT D6262001 20170307 D110D626200100001 BIB 9 25 D626200100002 TITLE Understanding the two neutron transfer reaction D626200100003 mechanism in 206Pb(18O,16O)208Pb D626200100004 AUTHOR (A.Parmar, Sonika, B.J.Roy, V.Jha, U.K.Pal, T.Sinha, D626200100005 S.K.Pandit, V.V.Parkar, K.Ramachandran, K.Mahata, D626200100006 S.Santra, A.K.Mohanty) D626200100007 INSTITUTE (3INDTRM,3INDSAH) D626200100008 REFERENCE (J,NP/A,940,167,2015) D626200100009 FACILITY (VDGT,3INDTRM) Pelletron-Linac facility D626200100010 SAMPLE 206PB target isotopically enriched (>99%) evaporated D626200100011 on 12C foil. The target and carbon backing D626200100012 thicknesses are 250 ug/cm2 and 30 ug/cm2 respectively. D626200100013 DETECTOR (TELES,SIBAR,SIBAR) Four silicon surface barrier D626200100014 detector telescopes in dE-E configuration mounted on D626200100015 two movable arms inside the General Purpose D626200100016 Scattering Chamber at 0 degree beam line of the D626200100017 Pelletron beam hall. Thickness of the delta E D626200100018 detectors is ~ 25 um and E detectors are above 300 D626200100019 um. Each telescope subtended a solid angle of ~ 0.5 D626200100020 msr. D626200100021 (SIBAR) Two monitor detectors (SSB detector of D626200100022 thickness 1 mm) are placed at forward angle +-25 D626200100023 degree with respect to the beam direction for cross D626200100024 section normalization. D626200100025 METHOD (EDE) D626200100026 HISTORY (20170307C) Compiled by JITHEESH GANGADHARAN K, NITC D626200100027 ENDBIB 25 0 D626200100028 NOCOMMON 0 0 D626200100029 ENDSUBENT 28 0 D626200199999 SUBENT D6262002 20170307 D110D626200200001 BIB 3 7 D626200200002 REACTION (82-PB-206(8-O-16,EL)82-PB-206,,DA,,RTH) D626200200003 ERR-ANALYS (ERR-SYS) An overall systematic uncertainty of ~10% D626200200004 (mostly for the large angles daa mainly due to the D626200200005 fitting procedure to extract the area under the D626200200006 elastic peak) D626200200007 STATUS (TABLE) Fig.2 of Nuclear Physics A,940(2015)167 D626200200008 "Error-bar values were not available from the author" D626200200009 ENDBIB 7 0 D626200200010 COMMON 2 3 D626200200011 EN ERR-SYS D626200200012 MEV PER-CENT D626200200013 79. 10. D626200200014 ENDCOMMON 3 0 D626200200015 DATA 2 14 D626200200016 ANG-CM DATA D626200200017 ADEG NO-DIM D626200200018 90.00 1.000 D626200200019 109.84 0.978 D626200200020 119.54 0.978 D626200200021 124.34 1.050 D626200200022 129.10 0.945 D626200200023 133.84 0.963 D626200200024 138.54 0.870 D626200200025 143.22 0.885 D626200200026 147.87 0.741 D626200200027 152.50 0.707 D626200200028 157.12 0.661 D626200200029 161.71 0.573 D626200200030 166.30 0.537 D626200200031 170.87 0.540 D626200200032 ENDDATA 16 0 D626200200033 ENDSUBENT 32 0 D626200299999 SUBENT D6262003 20170307 D110D626200300001 BIB 4 7 D626200300002 REACTION (82-PB-206(8-O-18,8-O-16)82-PB-208,PAR,DA) D626200300003 EN-SEC (E-LVL1,8-O-16) D626200300004 (E-LVL2,82-PB-208) D626200300005 ERR-ANALYS (ERR-1) Uncertainty in the solid angle measurement is D626200300006 estimated to be ~3% D626200300007 STATUS (TABLE) Fig.3 of Nuclear Physics A,940(2015)167 D626200300008 "Error-bar values were not available from the author" D626200300009 ENDBIB 7 0 D626200300010 COMMON 4 3 D626200300011 EN E-LVL1 E-LVL2 ERR-1 D626200300012 MEV MEV MEV PER-CENT D626200300013 79. 0. 0. 3. D626200300014 ENDCOMMON 3 0 D626200300015 DATA 2 12 D626200300016 ANG-CM DATA-CM D626200300017 ADEG MB/SR D626200300018 119.54 0.039 D626200300019 124.34 0.110 D626200300020 129.10 0.092 D626200300021 133.84 0.160 D626200300022 138.54 0.158 D626200300023 143.22 0.211 D626200300024 147.87 0.190 D626200300025 152.50 0.158 D626200300026 157.12 0.217 D626200300027 161.71 0.170 D626200300028 166.30 0.160 D626200300029 170.87 0.111 D626200300030 ENDDATA 14 0 D626200300031 ENDSUBENT 30 0 D626200399999 ENDENTRY 3 0 D626299999999