ENTRY            C2771   20241030                             C247C277100000001 
SUBENT        C2771001   20241030                             C247C277100100001 
BIB                 10         23                                 C277100100002 
TITLE      Revised decay properties of the key 93-keV resonance   C277100100003 
           in the 25Mg(p,gamma) reaction and its influence on     C277100100004 
           the MgAl cycle in astrophysical environments           C277100100005 
AUTHOR     (G.Lotay,D.T.Doherty,R.V.F.Janssens,D.Seweryniak,      C277100100006 
           H.M.Albers,S.Almaraz-Calderon,M.P.Carpenter,           C277100100007 
           A.E.Champagne,C.J.Chiara,C.R.Hoffman,C.Iliadis,        C277100100008 
           A.Kankainen,T.Lauritsen,S.Zhu)                         C277100100009 
REFERENCE  (J,PR/C,105,L042801,2022)                              C277100100010 
           #doi:10.1103/PhysRevC.105.L042801                      C277100100011 
REL-REF    (O,C2595002,A.Kankainen+,J,PL/B,813,136033,2021)       C277100100012 
INSTITUTE  (2UK SUR,1USANCA,1USATNL,1USAANL,1USAMRY,2SF JYV)      C277100100013 
FACILITY   (LINAC,1USAANL) The Argonne ATLAS accelerator.         C277100100014 
DETECTOR   (HPGE) The Gammasphere detector array which, in this   C277100100015 
           instance, consisted of 99 detectors operated in        C277100100016 
           stand-alone mode.                                      C277100100017 
SAMPLE     ~300 mu-g/cm2-thick target of 11B.                     C277100100018 
METHOD     ~5 pnA, 19-MeV beam of 16O ions, delivered by the      C277100100019 
           Argonne ATLAS accelerator, was used to bombard 11B     C277100100020 
           target for ~100 hr, in order to populate excited       C277100100021 
           states in 26Al via the one-neutron evaporation         C277100100022 
           channel. The resulting gamma-ray transitions were      C277100100023 
           detected using the Gammasphere array.                  C277100100024 
HISTORY    (20241030C) BP                                         C277100100025 
ENDBIB              23          0                                 C277100100026 
COMMON               1          3                                 C277100100027 
EN                                                                C277100100028 
MEV                                                               C277100100029 
19.                                                               C277100100030 
ENDCOMMON            3          0                                 C277100100031 
ENDSUBENT           30          0                                 C277100199999 
SUBENT        C2771002   20241030                             C247C277100200001 
BIB                  4          8                                 C277100200002 
REACTION   (5-B-11(8-O-16,N)13-AL-26,PAR,DA,G,LEG/RS)             C277100200003 
ANALYSIS   For strong transitions, an angular distribution        C277100200004 
           analysis was performed by fitting gamma-ray intensitiesC277100200005 
            as a function of detection angle with respect to the  C277100200006 
           beam axis with the customary function                  C277100200007 
           W(theta) = A0 [1 + a2P2(cos theta) + a4P4(cos theta)]. C277100200008 
ERR-ANALYS (DATA-ERR) No details on sources of uncertainties.     C277100200009 
STATUS     (TABLE,,G.Lotay+,J,PR/C,105,L042801,2022) Table I.     C277100200010 
ENDBIB               8          0                                 C277100200011 
NOCOMMON             0          0                                 C277100200012 
DATA                 4         26                                 C277100200013 
E          NUMBER     DATA       DATA-ERR                         C277100200014 
KEV        NO-DIM     NO-DIM     NO-DIM                           C277100200015 
      1744.         2.      -0.34       0.06                      C277100200016 
      1744.         4.       0.08       0.08                      C277100200017 
      1894.         2.      -0.36       0.11                      C277100200018 
      1894.         4.       0.21       0.14                      C277100200019 
      3239.         2.       0.34       0.15                      C277100200020 
      3239.         4.      -0.03       0.17                      C277100200021 
      3999.         2.       0.32       0.11                      C277100200022 
      3999.         4.       0.20       0.14                      C277100200023 
      4130.         2.       0.22       0.06                      C277100200024 
      4130.         4.      -0.16       0.09                      C277100200025 
      4273.         2.      -0.49       0.08                      C277100200026 
      4273.         4.       0.05       0.08                      C277100200027 
      4328.         2.       0.50       0.11                      C277100200028 
      4328.         4.      -0.04       0.14                      C277100200029 
      4749.         2.       0.13       0.20                      C277100200030 
      4749.         4.       0.38       0.24                      C277100200031 
      4806.         2.       0.39       0.07                      C277100200032 
      4806.         4.       0.11       0.11                      C277100200033 
      4851.         2.      -0.49       0.16                      C277100200034 
      4851.         4.      -0.05       0.21                      C277100200035 
      5743.         2.       0.34       0.08                      C277100200036 
      5743.         4.      -0.07       0.10                      C277100200037 
      6018.         2.       0.29       0.06                      C277100200038 
      6018.         4.      -0.33       0.09                      C277100200039 
      6193.         2.       0.18       0.04                      C277100200040 
      6193.         4.       0.10       0.05                      C277100200041 
ENDDATA             28          0                                 C277100200042 
ENDSUBENT           41          0                                 C277100299999 
ENDENTRY             2          0                                 C277199999999