ENTRY F1529 20250818 F152900000001 SUBENT F1529001 20250818 20260228 F152900100001 BIB 13 48 F152900100002 TITLE Influence of deuteron breakup on d+6He elastic F152900100003 scattering F152900100004 AUTHOR (B.Zalewski,M.S.Golovkov,K.Rusek,S.G.Belogurov, F152900100005 A.A.Bezbakh,V.Chudoba,E.M.Gazeeva,A.V.Gorshkov, F152900100006 G.Kaminski,N.Keeley,S.A.Krupko,B.Mauyey, F152900100007 I.A.Muzalevskii,P.J.Napiorkowski,W.Piatek, F152900100008 A.Serikov,S.I.Sidorchuk,R.S.Slepnev,P.G.Sharov, F152900100009 N.Sokolowska,G.M.Ter-Akopian,A.Trzcinska,R.Wolski) F152900100010 INSTITUTE (3POLWWA) Heavy Ion Laboratory; F152900100011 Faculty of Physics F152900100012 (4ZZZDUB) Flerov Laboratory of Nuclear Reactions F152900100013 (3POLIPJ) National Centre for Nuclear Research, Otwock F152900100014 REFERENCE (J,PR/C,111,054616,2025) F152900100015 #doi:10.1103/PhysRevC.111.054616 F152900100016 FACILITY (CYCLO,4ZZZDUB) U-400M cyclotron and ACCULINA-2 F152900100017 fragment separator. F152900100018 INC-SOURCE The average intensity of the 6He beam was 10**4 F152900100019 particles per second with an energy of 156+-9 MeV and F152900100020 the beam spot at the target was about 20 mm in F152900100021 diameter. F152900100022 SAMPLE Primary 15N beam was focused onto a target of natural F152900100023 beryllium with the 2 mm thickness. The secondary beam F152900100024 of 6He ions was directed onto the deuterated polythene F152900100025 (CD2) targets with the thicknesses of 100 and 200 mu-mF152900100026 DETECTOR (TELES,SISD,CSICR) The reaction products were detected F152900100027 in two identical telescopes, each consisting of a 1 mm F152900100028 thick double-sided silicon detector (DSSD) and a F152900100029 cesium-iodide scintillator [CsI(Tl)]. The telescopes F152900100030 were placed on the left and right sides of the beam F152900100031 axis. The DSSD had 32 strips on the horizontal axis F152900100032 and 16 strips on the vertical axis. The CsI(Tl) F152900100033 detectors were thick enough to stop the reaction F152900100034 products and measure their remaining energy. F152900100035 (MWPC) Beam tracking was performed with two multiwire F152900100036 proportional chambers located 27 and 82 cm upstream F152900100037 of the secondary target. F152900100038 METHOD (EDE,TOF) F152900100039 (COINC) The elastic scattering events were identified F152900100040 by simultaneous registration of a 6He in the right F152900100041 telescope and a proton or deuteron in the left F152900100042 telescope. F152900100043 ADD-RES Effective potentials for the p+6He and d+6He systems F152900100044 were derived from optical model analyses of the data. F152900100045 ERR-ANALYS (ERR-S) Statistical error F152900100046 (ERR-SYS) Systematic error F152900100047 STATUS Data were presented by Dr. B.Zalewski. F152900100048 (APRVD) Entry was approved by Dr. B.Zalewski. F152900100049 HISTORY (20250818C) F152900100050 ENDBIB 48 0 F152900100051 COMMON 1 3 F152900100052 EN F152900100053 MEV/A F152900100054 26. F152900100055 ENDCOMMON 3 0 F152900100056 ENDSUBENT 55 0 F152900199999 SUBENT F1529002 20250818 20260228 F152900200001 BIB 3 3 F152900200002 REACTION ((1-H-1(2-HE-6,EL)1-H-1,,DA)=(2-HE-6(P,EL)2-HE-6,,DA)) F152900200003 PART-DET (2-HE-6,P) F152900200004 STATUS (TABLE,,B.Zalewski+,J,PR/C,111,054616,2025) F152900200005 ENDBIB 3 0 F152900200006 COMMON 1 3 F152900200007 ERR-SYS F152900200008 PER-CENT F152900200009 14. F152900200010 ENDCOMMON 3 0 F152900200011 DATA 3 46 F152900200012 ANG-CM DATA-CM ERR-S F152900200013 ADEG MB/SR MB/SR F152900200014 31.00 137.817 41.55340 F152900200015 33.00 148.973 32.50860 F152900200016 35.00 102.671 22.40460 F152900200017 37.00 100.077 18.27140 F152900200018 39.00 74.516 13.17270 F152900200019 41.00 77.186 11.91010 F152900200020 43.00 53.1343 8.61952 F152900200021 45.00 46.2728 7.14005 F152900200022 47.00 50.7001 2.98753 F152900200023 49.00 38.5006 2.24923 F152900200024 51.00 29.2739 1.81549 F152900200025 53.00 22.9727 1.51808 F152900200026 55.00 16.9194 1.22424 F152900200027 57.00 12.7210 1.01524 F152900200028 59.00 9.16211 0.80668 F152900200029 61.00 8.02180 0.72038 F152900200030 63.00 6.67403 0.62784 F152900200031 65.00 5.26951 0.53504 F152900200032 67.00 4.46727 0.47621 F152900200033 69.00 3.52127 0.40660 F152900200034 71.00 3.65123 0.40321 F152900200035 73.00 2.29935 0.31004 F152900200036 75.00 2.37427 0.30652 F152900200037 77.00 2.82721 0.32430 F152900200038 79.00 2.03164 0.26910 F152900200039 81.00 1.61833 0.23861 F152900200040 83.00 2.01113 0.18436 F152900200041 85.00 1.75129 0.15186 F152900200042 87.00 1.72770 0.14602 F152900200043 89.00 1.65279 0.14173 F152900200044 91.00 1.85160 0.14969 F152900200045 93.00 1.63202 0.13943 F152900200046 95.00 1.70882 0.14046 F152900200047 97.00 1.54708 0.12937 F152900200048 99.00 1.27006 0.11643 F152900200049 101.00 1.16880 0.11247 F152900200050 103.00 1.10285 0.10920 F152900200051 105.00 1.08850 0.10940 F152900200052 107.00 1.14462 0.11278 F152900200053 109.00 0.74754 0.09133 F152900200054 111.00 0.88715 0.10045 F152900200055 113.00 0.73957 0.09469 F152900200056 115.00 0.66508 0.09313 F152900200057 117.00 0.55636 0.09025 F152900200058 119.00 0.72561 0.10939 F152900200059 121.00 0.47529 0.09321 F152900200060 ENDDATA 48 0 F152900200061 ENDSUBENT 60 0 F152900299999 SUBENT F1529003 20250818 20260228 F152900300001 BIB 3 3 F152900300002 REACTION ((1-H-2(2-HE-6,EL)1-H-2,,DA)=(2-HE-6(D,EL)2-HE-6,,DA)) F152900300003 PART-DET (2-HE-6,D) F152900300004 STATUS (TABLE,,B.Zalewski+,J,PR/C,111,054616,2025) F152900300005 ENDBIB 3 0 F152900300006 COMMON 1 3 F152900300007 ERR-SYS F152900300008 PER-CENT F152900300009 13. F152900300010 ENDCOMMON 3 0 F152900300011 DATA 3 47 F152900300012 ANG-CM DATA-CM ERR-S F152900300013 ADEG MB/SR MB/SR F152900300014 25. 131.017 17.2034 F152900300015 27. 74.168 8.50765 F152900300016 29. 46.9887 5.2535 F152900300017 31. 30.1779 3.37399 F152900300018 33. 25.6087 2.53564 F152900300019 35. 28.7161 2.31401 F152900300020 37. 24.8854 1.86002 F152900300021 39. 25.6918 1.68312 F152900300022 41. 22.0815 1.41653 F152900300023 43. 19.269 1.21625 F152900300024 45. 18.3133 1.10635 F152900300025 47. 14.4294 0.93336 F152900300026 49. 12.7745 0.836884 F152900300027 51. 10.4614 0.739733 F152900300028 53. 7.33707 0.611423 F152900300029 55. 5.82082 0.542794 F152900300030 57. 4.44305 0.476345 F152900300031 59. 3.82636 0.450941 F152900300032 61. 2.95595 0.185839 F152900300033 63. 2.11583 0.153498 F152900300034 65. 1.6285 0.132967 F152900300035 67. 1.39358 0.121295 F152900300036 69. 1.09139 0.106508 F152900300037 71. 0.775564 0.0889633 F152900300038 73. 0.725734 0.0855285 F152900300039 75. 0.674977 0.081853 F152900300040 77. 0.508509 0.0712055 F152900300041 79. 0.52028 0.0714659 F152900300042 81. 0.507278 0.0710331 F152900300043 83. 0.299066 0.0546018 F152900300044 85. 0.271604 0.0380322 F152900300045 87. 0.286018 0.0346847 F152900300046 89. 0.174447 0.0251792 F152900300047 91. 0.194761 0.0255734 F152900300048 93. 0.119488 0.0196436 F152900300049 95. 0.100783 0.0178161 F152900300050 97. 0.0985483 0.0174211 F152900300051 99. 0.0843306 0.015937 F152900300052 101. 0.0647463 0.013804 F152900300053 103. 0.0480793 0.0120198 F152900300054 105. 0.0206535 0.0078063 F152900300055 107. 0.0360327 0.0104017 F152900300056 109. 0.0210315 0.00794915 F152900300057 111. 0.0149975 0.00670709 F152900300058 113. 0.00607569 0.00429616 F152900300059 115. 0.0122594 0.00612972 F152900300060 117. 0.00946494 0.00546459 F152900300061 ENDDATA 49 0 F152900300062 ENDSUBENT 61 0 F152900399999 ENDENTRY 3 0 F152999999999