ENTRY S0284 20251009 S028400000001 SUBENT S0284001 20251009 20260228 S028400100001 BIB 10 40 S028400100002 TITLE s- and d-wave intruder strengths in 13Bg.s. via the S028400100003 1H(13B, d)12B reaction S028400100004 AUTHOR (W.Liu, J.L.Lou, Y.L.Ye, Z.H.Li, Q.T.Li, H.Hua, S028400100005 X.F.Yang, J.Y.Xu, H.J.Ong, D.T.Tran, N.Aoi, S028400100006 E.Ideguchi, D.Y.Pang, C.X.Yuan, S.M.Wang, Y.Jiang, S028400100007 B.Yang, Y.Liu, J.G.Li, Z.Q.Chen, J.X.Han, S.W.Bai, S028400100008 G.Li, K.Ma, Z.W.Tan, H.Y.Zhu, B.L.Xia) S028400100009 INSTITUTE (3CPRBJG,2JPNOSA,3CPRIMP,3CPRUCA,3VN IPH,3CPRBHN, S028400100010 3CPRSZH,3CPRFUD,1USAMSU) S028400100011 REFERENCE (J,PR/C,104,064605,2021) S028400100012 #doi:10.1103/PhysRevC.104.064605 S028400100013 FACILITY (CYCLO,2JPNOSA) Exotic Nuclear (EN) beam line at S028400100014 Research Center for Nuclear Physics (RCNP) S028400100015 INC-SOURCE 9Be(18O,13B). A 23-MeV/nucleon 13B secondary beam S028400100016 was produced from a 58-MeV/nucleon 18O primary beam S028400100017 impinging on a 3.8-mm-thick 9Be target. The secondary S028400100018 beam purity and intensity were 98% and about 2.0E4 S028400100019 particles per second, respectively. S028400100020 SAMPLE A 6.76-mg/cm2 polyethylene target (CH2)n S028400100021 DETECTOR (SCIN) TOF provided by two plastic scintillation S028400100022 detectors S028400100023 (PPAC) Two position-sensitive parallel plate S028400100024 avalanche chambers (PPACs) were employed to track the S028400100025 13B beam before the physical target. The position S028400100026 resolution of two PPACs was about 1.5 mm [full width S028400100027 at half maximum (FWHM)] S028400100028 (TELES,SISD,SI,CSICR) Four sets of charged-particle S028400100029 telescopes (T0, T1, T2, TA) were employed in the S028400100030 large scattering chamber. T0, consisting of a double- S028400100031 sided silicon strip (DSSD) detector with a thickness S028400100032 of 1000 um, two large size silicon detectors (SSDs), S028400100033 and a layer of 4-cm-thick CsI(Tl) crystals. T1, same S028400100034 as T2, was composed of a 60-mm-thick DSSD, a SSD and S028400100035 an array of 4-cm-thick CsI(Tl) crystals. TA is a set S028400100036 of the annular double-sided silicon strip detector S028400100037 composed of six sectors. S028400100038 METHOD (TOF,EDE) The secondary beam was identified by the S028400100039 time of flight. S028400100040 HISTORY (20250220R) Data received from J.L.Lou S028400100041 (20251009C) Liu Yangyang S028400100042 ENDBIB 40 0 S028400100043 COMMON 2 3 S028400100044 EN EN-RSL-FW S028400100045 MEV/A KEV S028400100046 23. 776. S028400100047 ENDCOMMON 3 0 S028400100048 ENDSUBENT 47 0 S028400199999 SUBENT S0284002 20251009 20260228 S028400200001 BIB 3 8 S028400200002 REACTION ((1-H-1(5-B-13,EL)1-H-1,,DA,,RTH)= S028400200003 (5-B-13(P,EL)5-B-13,,DA,,RTH)) S028400200004 ERR-ANALYS (ERR-S) The statistical error S028400200005 (ERR-SYS,,0.09) The systematic error is less than 9%, S028400200006 considering the uncertainties in the geometrical S028400200007 efficiency determination, the thickness of the target,S028400200008 and the cuts on the particle identification spectra. S028400200009 STATUS (TABLE,,W.Liu+,J,PR/C,104,064605,2021) Fig.6 S028400200010 ENDBIB 8 0 S028400200011 COMMON 1 3 S028400200012 ANG-RSL-FW S028400200013 ADEG S028400200014 2.00 S028400200015 ENDCOMMON 3 0 S028400200016 DATA 3 7 S028400200017 ANG-CM DATA-CM ERR-S S028400200018 ADEG NO-DIM NO-DIM S028400200019 58.00 9.76 0.78 S028400200020 54.00 6.36 0.43 S028400200021 50.00 6.70 0.37 S028400200022 46.00 8.75 0.37 S028400200023 42.00 11.29 0.37 S028400200024 38.00 13.62 0.35 S028400200025 34.00 14.63 0.31 S028400200026 ENDDATA 9 0 S028400200027 ENDSUBENT 26 0 S028400299999 SUBENT S0284003 20251009 20260228 S028400300001 BIB 4 10 S028400300002 REACTION ((1-H-1(5-B-13,D)5-B-12,PAR,DA,RSD)= S028400300003 (5-B-13(P,D)5-B-12,PAR,DA)) S028400300004 EN-SEC (E-LVL,5-B-12) S028400300005 ERR-ANALYS (ERR-S) The statistical error S028400300006 (ERR-SYS,,0.11) The systematic error is less than S028400300007 11%,taking into consideration the uncertainties in S028400300008 the geometrical efficiency determination, the S028400300009 thickness of the target, and the cuts of deuterons S028400300010 and borons on the particle identification spectra. S028400300011 STATUS (TABLE,,W.Liu+,J,PR/C,104,064605,2021) Fig.9 S028400300012 ENDBIB 10 0 S028400300013 NOCOMMON 0 0 S028400300014 DATA 6 20 S028400300015 E-LVL ANG-CM -ANG-RSL +ANG-RSL DATA-CM ERR-S S028400300016 MEV ADEG ADEG ADEG MB/SR MB/SR S028400300017 0.000 16.66 1.74 1.91 2.49 0.43S028400300018 0.000 20.68 2.12 2.41 2.21 0.31S028400300019 0.000 25.93 2.84 3.50 1.24 0.19S028400300020 0.000 34.17 4.74 8.62 0.80 0.10S028400300021 0.953 18.02 1.91 2.11 4.02 0.50S028400300022 0.953 22.51 2.37 2.75 2.93 0.33S028400300023 0.953 28.56 3.30 4.26 1.24 0.17S028400300024 0.953 39.32 6.49 11.68 0.68 0.07S028400300025 1.674 19.16 2.06 2.29 0.10 0.07S028400300026 1.674 24.05 2.60 3.05 0.14 0.07S028400300027 1.674 30.87 3.77 5.13 0.27 0.07S028400300028 2.723 20.99 2.31 2.60 0.50 0.15S028400300029 2.723 26.59 3.00 3.63 0.52 0.11S028400300030 2.723 34.95 4.73 7.50 0.27 0.06S028400300031 3.389 22.28 2.50 2.83 0.45 0.13S028400300032 3.389 28.44 3.32 4.12 0.26 0.07S028400300033 3.389 38.23 5.68 12.42 0.12 0.03S028400300034 4.523 24.78 2.87 3.33 0.22 0.08S028400300035 4.523 32.16 4.05 5.36 0.15 0.05S028400300036 4.523 46.75 9.23 8.25 0.04 0.01S028400300037 ENDDATA 22 0 S028400300038 ENDSUBENT 37 0 S028400399999 ENDENTRY 3 0 S028499999999