ENTRY D0545 20091222 D071D054500000001 SUBENT D0545001 20091222 D071D054500100001 BIB 12 47 D054500100002 TITLE Measurements of the breakup and neutron removal cross D054500100003 sections for 16C D054500100004 AUTHOR (N.I.Ashwood,M.Freer,J.C.Angelique,V.Bouchat, D054500100005 W.N.Catford,N.M.Clarke,N.Curtis,O.Dorvaux,F.Hanappe, D054500100006 Y.Kerckx,M.Labiche,J.L.Lecouey,F.M.Marques,T.Materna, D054500100007 A.Ninane,G.Normand,N.A.Orr,S.Pain,N.Soic,L.Stuttge, D054500100008 C.Timis,A.Unshakova,V.A.Ziman) D054500100009 INSTITUTE (2UK BIR,2FR CAE,2BLGBRU,2UK SUR,2FR ULP,2BLGLVN, D054500100010 4ZZZDUB) D054500100011 REFERENCE (J,PR/C,70,064607,2004) D054500100012 #doi:10.1103/PhysRevC.70.064607 D054500100013 FACILITY (ACCEL,2FR GAN) D054500100014 INC-SOURCE secondary beam of 14B was produced at 40.8 MeV/A by D054500100015 fragmentation of a 63 MeV/A 18O primary beam on a D054500100016 rotating 9Be target. At the same time, a secondary D054500100017 parasitic beam of 16C was produced at ~3% of beam D054500100018 purity with an energy of 46 MeV/A and intensity on D054500100019 the order of 300 particles per second. Particle D054500100020 identification was achieved via time-of-flight D054500100021 through the LISE spectrometer. D054500100022 SAMPLE The beam was tracked onto a 275 mg/cm2 carbon target D054500100023 using two drift chambers D054500100024 DETECTOR (CSICR) A zero degree telescope, consisting of two D054500100025 orthogonal strip detectors and a close packed array D054500100026 of 16 CsI detectors, was used to detect the beam and D054500100027 reaction products. D054500100028 (SCIN) Neutrons produced in the reactions were D054500100029 detected using the DeMoN array, which consists of D054500100030 ~100 liquid scintillators D054500100031 METHOD (EDE,TOF,COINC) Particle identification (PI) of D054500100032 reaction products was achieved using the EdE D054500100033 technique Rejection of particles resulting from the D054500100034 breakup of the 14B beam was achieved in software by D054500100035 gating on the 16C peak in the time-of-flight spectrum. D054500100036 The xLi+yBe, xHe+yBe, xLi+yLi, xHe+yLi, and xHe+yHe D054500100037 channels were measured by coincident detection of the D054500100038 two charged fragments, while the cross sections for D054500100039 the xC+1n channels were measured by detecting the D054500100040 fragment and the single neutron in coincidence. D054500100041 ERR-ANALYS (ERR-S) The uncertainties quoted are purely D054500100042 statistical. D054500100043 (ERR-SYS) Systematic errors in the determination of D054500100044 the cross section come from the uncertainty in the D054500100045 nature of the angular distributions used in the Monte D054500100046 Carlo simulations. These are estimated to be ~20%. D054500100047 STATUS (TABLE) Data from Tbl.1 of PR/C,70,064607,2004 D054500100048 HISTORY (20091222C) SD D054500100049 ENDBIB 47 0 D054500100050 COMMON 3 3 D054500100051 EN EN-ERR ERR-SYS D054500100052 MEV/A PER-CENT PER-CENT D054500100053 46. 3. 20. D054500100054 ENDCOMMON 3 0 D054500100055 ENDSUBENT 54 0 D054500199999 SUBENT D0545002 20091222 D071D054500200001 BIB 2 3 D054500200002 REACTION (6-C-12(6-C-16,X)ELEM/MASS,,SIG) D054500200003 ANALYSIS the xC+1n channels were measured by detecting the D054500200004 fragment and the single neutron in coincidence. D054500200005 ENDBIB 3 0 D054500200006 COMMON 1 3 D054500200007 ELEMENT D054500200008 NO-DIM D054500200009 6. D054500200010 ENDCOMMON 3 0 D054500200011 DATA 3 4 D054500200012 MASS DATA ERR-S D054500200013 NO-DIM B B D054500200014 15. 0.096 0.011 D054500200015 14. 0.094 0.011 D054500200016 13. 0.033 0.004 D054500200017 12. 0.011 0.001 D054500200018 ENDDATA 6 0 D054500200019 ENDSUBENT 18 0 D054500299999 SUBENT D0545003 20091222 D071D054500300001 BIB 1 1 D054500300002 REACTION (6-C-12(6-C-16,X)ELEM/MASS,,SIG) D054500300003 ENDBIB 1 0 D054500300004 NOCOMMON 0 0 D054500300005 DATA 6 28 D054500300006 ELEM1 MASS1 ELEM2 MASS2 DATA ERR-S D054500300007 NO-DIM NO-DIM NO-DIM NO-DIM B B D054500300008 4. 10. 3. 7. 70.E-06 100.E-06D054500300009 4. 10. 2. 6. 200.E-06 190.E-06D054500300010 4. 10. 2. 4. 0.015 0.004 D054500300011 4. 9. 3. 7. 270.E-06 230.E-06D054500300012 4. 9. 3. 6. 70.E-06 100.E-06D054500300013 4. 9. 2. 8. 70.E-06 100.E-06D054500300014 4. 9. 2. 6. 410.E-06 300.E-06D054500300015 4. 9. 2. 4. 0.013 0.004 D054500300016 3. 9. 2. 6. 200.E-06 190.E-06D054500300017 3. 9. 2. 4. 0.002 0.001 D054500300018 3. 8. 3. 7. 550.E-06 360.E-06D054500300019 3. 8. 3. 6. 140.E-06 150.E-06D054500300020 3. 8. 2. 6. 480.E-06 330.E-06D054500300021 3. 8. 2. 4. 0.010 0.003 D054500300022 3. 7. 3. 7. 680.E-06 420.E-06D054500300023 3. 7. 3. 6. 890.E-06 510.E-06D054500300024 3. 7. 2. 8. 340.E-06 270.E-06D054500300025 3. 7. 2. 6. 0.001 0.001 D054500300026 3. 7. 2. 4. 0.032 0.008 D054500300027 3. 6. 2. 8. 410.E-06 300.E-06D054500300028 3. 6. 2. 6. 340.E-06 270.E-06D054500300029 3. 6. 2. 4. 0.012 0.004 D054500300030 2. 8. 2. 8. 140.E-06 150.E-06D054500300031 2. 8. 2. 6. 820.E-06 480.E-06D054500300032 2. 8. 2. 4. 0.003 0.001 D054500300033 2. 6. 2. 6. 750.E-06 450.E-06D054500300034 2. 6. 2. 4. 0.010 0.003 D054500300035 2. 4. 2. 4. 0.131 0.025 D054500300036 ENDDATA 30 0 D054500300037 ENDSUBENT 36 0 D054500399999 ENDENTRY 3 0 D054599999999