ENTRY C2092 20140910 C150C209200000001 SUBENT C2092001 20140910 C150C209200100001 BIB 11 30 C209200100002 TITLE Measuring the fusion cross-section of light nuclei C209200100003 with low-intensity beams C209200100004 AUTHOR (T.K.Steinbach,M.J.Rudolph,Z.Q.Gosser,K.Brown,B.Floyd, C209200100005 S.Hudan,R.T.deSouza,J.F.Liang,D.Shapira,M.Famiano) C209200100006 INSTITUTE (1USAINU,1USAORL,1USAWMU) C209200100007 REFERENCE (J,NIM/A,743,5,2014) C209200100008 FACILITY (VDGT,1USAWMU) Experiment was carried out at Western C209200100009 Michigan University tandem Van de Graaff accelerator C209200100010 SAMPLE Natural carbon foil with thickness of (93+-0.5)mu-g/cm2C209200100011 DETECTOR (SCIN) The setup consisted of active collimator, C209200100012 constructed from a 1/8in. plastic scintillator 3in. C209200100013 in diameter with a 0.511in. diameter hole in the C209200100014 center. The scintillator was coupled to a fast PMT. C209200100015 (SI) Two segmented n-type silicon detectors with C209200100016 annular rings on the junction side and pie shaped C209200100017 sectors on the ohmic side 249 mu-m and 305 mu-m thick C209200100018 covered the angular region of 11.3 deg - 21.8deg and C209200100019 3.53deg - 10.8deg. C209200100020 (IOCH) The final detector in the setup was the zero C209200100021 degree gas ionization chamber (ZDIC) that measured C209200100022 the energy loss of the beam as well as fusion C209200100023 residues in the angular region of theta lab less than C209200100024 3.52 deg. C209200100025 METHOD (TOF) Reaction residues were identified using C209200100026 energy x time of flight method C209200100027 CORRECTION Corrected for charge trapping in segmented Si detector C209200100028 ERR-ANALYS (DATA-ERR) No information given C209200100029 (ERR-1) Uncertainty associated with correction for C209200100030 charge trapping. C209200100031 HISTORY (20140910C) Compiled by S.H. C209200100032 ENDBIB 30 0 C209200100033 COMMON 1 3 C209200100034 ERR-1 C209200100035 PER-CENT C209200100036 2.0 C209200100037 ENDCOMMON 3 0 C209200100038 ENDSUBENT 37 0 C209200199999 SUBENT C2092002 20140910 C150C209200200001 BIB 3 17 C209200200002 REACTION 1(6-C-12(8-O-16,FUS),,SIG,ER) C209200200003 2(6-C-12(8-O-16,FUS),,SIG,ER) C209200200004 STATUS (TABLE) data presented in fig.13 of the reference C209200200005 sent by author (R.T.deS.) C209200200006 DETECTOR 1(MCPLT) Two electrostatic micro-channel plate C209200200007 detectors were used for time of flight measurement. C209200200008 First detector utilizes a conventional electrostatic C209200200009 mirror to reflect secondary emission electrons C209200200010 generated by the passage of the beam through a carbon C209200200011 foil to MCP. The 18mm MCP detector also served as an C209200200012 active target in the experiment. C209200200013 2(MCPLT) Two electrostatic micro-channel plate C209200200014 detectors were used for time of flight measurement. C209200200015 Gridless detector utilizes a crossed electric and C209200200016 magnetic fields to transport secondary electrons C209200200017 to the MCP detector, which served as an active. C209200200018 target in the experiment. C209200200019 ENDBIB 17 0 C209200200020 NOCOMMON 0 0 C209200200021 DATA 6 8 C209200200022 EN-CM EN-RSL DATA 1DATA-ERR 1DATA 2DATA-ERR 2C209200200023 MEV MEV MB MB MB MB C209200200024 7.046 0.016 92.07 36.83 C209200200025 8.007 0.016 91.00 16.61 C209200200026 8.212 0.030 124.48 12.45 C209200200027 8.968 0.016 192.73 15.53 C209200200028 9.944 0.030 348.18 34.82 C209200200029 11.962 0.016 541.76 38.70 C209200200030 12.118 0.031 564.75 56.48 C209200200031 14.713 0.031 737.51 73.75 C209200200032 ENDDATA 10 0 C209200200033 ENDSUBENT 32 0 C209200299999 ENDENTRY 2 0 C209299999999