ENTRY C2290 20180411 C175C229000000001 SUBENT C2290001 20180411 C175C229000100001 BIB 11 37 C229000100002 TITLE Probing the fusion of neutron-rich nuclei with C229000100003 re-accelerated radioactive beams C229000100004 AUTHOR (J.Vadas,Varinderjit Singh,B.B.Wiggins,J.Huston, C229000100005 S.Hudan,R.T.deSouza,Z.Lin,C.J.Horowitz,A.Chbihi, C229000100006 D.Ackermann,M.Famiano,K.W.Brown) C229000100007 INSTITUTE (1USAINU,2FR GAN,1USAWMU,1USAMSU) C229000100008 REFERENCE (J,PR/C,97,031601,2018) C229000100009 FACILITY (LINAC,1USAMSU) Experiment was performed using C229000100010 the ReA3 facility at Michigan State University's C229000100011 National Superconducting Cyclotron Laboratory. C229000100012 SAMPLE The 327 mu-g/cm2 -thick 28Si secondary emission foil C229000100013 of the microchannel plate (MCP) detector served as C229000100014 the target for the experiment. C229000100015 DETECTOR (MCPLT) Two microchannel plate detectors, one at the C229000100016 target position, the second one 1.3 m upstream C229000100017 provided a time-of-flight measurement of the beam C229000100018 particles. C229000100019 (IOCH) Two compact axial field ionization chambers C229000100020 were inserted in the beam path between the two MCP C229000100021 detectors for particle identification. C229000100022 (SI) Two annular silicon detectors which subtend the C229000100023 laboratory angles 1.0-7.3deg were used for detection C229000100024 of evaporation residui. C229000100025 METHOD (TOF) Time of flight allowed rejection of beam C229000100026 particles scattered or degraded prior to the target C229000100027 and provided a direct measure of the number of beam C229000100028 particles incident on the target. C229000100029 Particle identification was achieved by E-TOF C229000100030 method. C229000100031 INC-SOURCE Ions of 39 K from a source or 47 K from a thermalized C229000100032 radioactive beam were charge bred in an ion trap, C229000100033 injected into the ReA3 80-MHz linac, and C229000100034 re-accelerated to energies between 2 and 3 MeV/A. C229000100035 ERR-ANALYS (DATA-ERR) Uncertainty in the fusion cross sections C229000100036 includes both measurement statistics and systematic C229000100037 uncertainties. Sources of uncertainties not described. C229000100038 HISTORY (20180411C) Compiled by S.H. C229000100039 ENDBIB 37 0 C229000100040 NOCOMMON 0 0 C229000100041 ENDSUBENT 40 0 C229000199999 SUBENT C2290002 20180411 C175C229000200001 BIB 2 3 C229000200002 REACTION (19-K-39(14-SI-28,FUS),,SIG,ER) C229000200003 STATUS (CURVE) Data taken from fig. 3 of the reference, C229000200004 waiting for data from author C229000200005 ENDBIB 3 0 C229000200006 NOCOMMON 0 0 C229000200007 DATA 4 8 C229000200008 EN-CM EN-RSL DATA DATA-ERR C229000200009 MEV MEV MB MB C229000200010 36.75 0.11 7.240E+00 1.288E+00 C229000200011 37.47 0.11 2.091E+01 3.566E+00 C229000200012 37.75 0.10 2.895E+01 4.506E+00 C229000200013 38.43 0.11 4.877E+01 7.956E+00 C229000200014 39.41 0.13 1.255E+02 1.272E+01 C229000200015 40.74 0.15 1.755E+02 1.918E+01 C229000200016 41.53 0.15 1.998E+02 1.702E+01 C229000200017 42.57 0.17 2.613E+02 2.438E+01 C229000200018 ENDDATA 10 0 C229000200019 ENDSUBENT 18 0 C229000299999 SUBENT C2290003 20180411 C175C229000300001 BIB 2 3 C229000300002 REACTION (19-K-47(14-SI-28,FUS),,SIG,ER) C229000300003 STATUS (CURVE) Data taken from fig. 3 of the reference, C229000300004 waiting for data from author C229000300005 ENDBIB 3 0 C229000300006 NOCOMMON 0 0 C229000300007 DATA 4 7 C229000300008 EN-CM EN-RSL DATA DATA-ERR C229000300009 MEV MEV MB MB C229000300010 36.18 0.22 1.70E+01 4.33E+00 C229000300011 36.76 0.25 3.41E+01 6.07E+00 C229000300012 37.45 0.26 6.45E+01 1.19E+01 C229000300013 37.98 0.23 6.12E+01 1.31E+01 C229000300014 39.43 0.24 1.80E+02 3.00E+01 C229000300015 41.21 0.26 2.55E+02 4.45E+01 C229000300016 42.62 0.24 3.32E+02 3.23E+01 C229000300017 ENDDATA 9 0 C229000300018 ENDSUBENT 17 0 C229000399999 ENDENTRY 3 0 C229099999999