ENTRY C2053 20130908 C135C205300000001 SUBENT C2053001 20130908 C135C205300100001 BIB 14 48 C205300100002 TITLE First observation of 15Be C205300100003 AUTHOR (J.Snyder,T.Baumann,G.Christian,R.A.Haring-Kaye, C205300100004 P.A.DeYoung,Z.Kohley,B.Luther,M.Mosby,S.Mosby,A.Simon, C205300100005 J.K.Smith,A.Spyrou,S.Stephenson,M.Thoennessen) C205300100006 INSTITUTE (1USAMSU,1USAHPE) C205300100007 (1USAUSA) Ohio Wesleyan University, Delaware, Ohio C205300100008 (1USAUSA) Concordia College, Moorhead, Minnesota C205300100009 (1USAUSA) Gettysburg College, Gettysburg, Pennsylvania C205300100010 REFERENCE (J,PR/C,88,031303,2013) C205300100011 FACILITY (CYCTM,1USAMSU) Experiment was performed at the C205300100012 National Superconducting Cyclotron Laboratory at C205300100013 Michigan State University C205300100014 SAMPLE Deuterated polyethylene target with thickness of C205300100015 435 mg/cm2 C205300100016 DETECTOR (MAGSP)14Be reaction products were deflected by a C205300100017 large-gap dipole magnet set to a magnetic rigidity of C205300100018 3.55 Tm. C205300100019 (DRFTC) Two cathode readout drift chambers with C205300100020 dimensions of 30cm x 30 cm separated by 1.88 m was C205300100021 used to determine position and angle of charged C205300100022 particles. C205300100023 (SCIN) Energy loss and total energy of charged C205300100024 particles were measured in 5 mm and 150 mm thick C205300100025 plastic scintillators, respectively. C205300100026 (SCIN) Coincident neutrons were measured with the C205300100027 Modular Neutron Array. The 144 plastic scintillator C205300100028 detectors of the array were arranged into 18 walls C205300100029 each 80 cm tall. The walls were assembled into two C205300100030 close-packed blocks located at 0deg and 23deg from C205300100031 the secondary beam direction, with their respective C205300100032 distances from the target being 650 cm and 470 cm. C205300100033 METHOD (COINC,EDE) C205300100034 INC-SOURCE A 120 MeV/u 18-O primary beam from the Coupled C205300100035 Cyclotron Facility bombarded a 3196 mg/cm2 C205300100036 9Be production target. The A1900 fragment separator C205300100037 in conjunction with a 1050 mg/cm2 aluminum achromatic C205300100038 wedge degrader was used to separate and select for C205300100039 the 14Be secondary beam. The final energy of the beam C205300100040 was 59 MeV/u with a momentum spread of 2%, an C205300100041 intensity of approximately 1000 pps, and a purity of C205300100042 96.5%. C205300100043 ANALYSIS The energy and momentum vector of the fragments were C205300100044 reconstructed from a transformation matrix based on C205300100045 the magnetic field map. C205300100046 ERR-ANALYS (DATA-ERR) No information given C205300100047 HISTORY (20130908C) Compiled by S.H. C205300100048 EN-SEC (E-LVL,4-BE-15) C205300100049 LEVEL-PROP (4-BE-15,E-LVL=1.8,SPIN=2.5,PARITY=+1.) C205300100050 ENDBIB 48 0 C205300100051 COMMON 3 3 C205300100052 EN EN-RSL E-LVL C205300100053 MEV/A PER-CENT MEV C205300100054 59.0 2.0 1.8 C205300100055 ENDCOMMON 3 0 C205300100056 ENDSUBENT 55 0 C205300199999 SUBENT C2053002 20130908 C135C205300200001 BIB 2 3 C205300200002 REACTION ((1-H-2(4-BE-14,P)4-BE-15,PAR,SIG)= C205300200003 (4-BE-14(D,P)4-BE-15,PAR,SIG)) C205300200004 STATUS (TABLE) Data taken from text, p3.of the reference C205300200005 ENDBIB 3 0 C205300200006 NOCOMMON 0 0 C205300200007 DATA 2 1 C205300200008 DATA DATA-ERR C205300200009 MB MB C205300200010 1.1 0.6 C205300200011 ENDDATA 3 0 C205300200012 ENDSUBENT 11 0 C205300299999 SUBENT C2053003 20130908 C135C205300300001 BIB 2 2 C205300300002 REACTION (6-C-12(4-BE-14,6-C-11)4-BE-15,PAR,SIG) C205300300003 STATUS (TABLE) Data taken from text, p3. of the reference C205300300004 ENDBIB 2 0 C205300300005 NOCOMMON 0 0 C205300300006 DATA 2 1 C205300300007 DATA DATA-ERR C205300300008 MB MB C205300300009 0.7 0.5 C205300300010 ENDDATA 3 0 C205300300011 ENDSUBENT 10 0 C205300399999 ENDENTRY 3 0 C205399999999