ENTRY C2235 20211007 C210C223500000001 SUBENT C2235001 20211007 C210C223500100001 BIB 10 40 C223500100002 TITLE Structure of 14C and 14B from the C223500100003 14,15C(d,3He)13,14B reactions C223500100004 AUTHOR (S.Bedoor,A.H.Wuosmaa,M.Albers,M.Alcorta, C223500100005 S.Almaraz-Calderon,B.B.Back,P.F.Bertone,C.M.Deibel, C223500100006 C.R.Hoffman,J.C.Lighthall,S.T.Marley,D.G.Mcneel, C223500100007 R.C.Pardo,K.E.Rehm,J.P.Schiffer,D.V.Shetty) C223500100008 INSTITUTE (1USAWMU,1USAANL,1USALSU) C223500100009 (1USAUSA) University of Connecticut,Storrs,Connecticut C223500100010 (1USAUSA) Grand Valley State University, C223500100011 Allendale,Michigan C223500100012 REFERENCE (J,PR/C,93,044323,2016) C223500100013 FACILITY (LINAC,1USAMSU) Experiment performed at ATLAS C223500100014 facility at Argonne National Laboratory using HELIOS C223500100015 solenoidal spectrometer C223500100016 SAMPLE Deuterated polyethylene (CD2)n foil target of areal C223500100017 density 140 mu-g/cm2 C223500100018 DETECTOR (MAGSP) The charged reaction products were separated C223500100019 in superconducting solenoid with a bore diameter of C223500100020 920 mm and length of 2350 mm. Polyethylene target was C223500100021 placed at the solenoid entrance, 550 mm upstream of C223500100022 the geometric center of the magnet. The 3He particles C223500100023 emerged in the forward hemisphere with laboratory C223500100024 angles less than 35 deg. Particles were transported in C223500100025 helical trajectories to detector array. C223500100026 (PS) An array of 24 position sensitive Si detectors C223500100027 placed on the beam axis in the downstream end of C223500100028 HELIOS was used to detect the 3He ions. C223500100029 (TELES,SI,SI) Recoil telescope consisted of dE and E C223500100030 detectors with thicknesses of 500 and 1000 mu-m, C223500100031 respectively C223500100032 (SIBAR) A silicon surface-barrier detector was C223500100033 mounted on the recoil-detector assembly at 0 deg to C223500100034 monitor incident beam flux. A Ta sheet 0.5 mm thick C223500100035 with regular holes with diameter of 80 mu-m was used C223500100036 to attenuate the incident flux to manageable level. C223500100037 METHOD (EDE) Inverse kinematics was used. C223500100038 ERR-ANALYS (ERR-S) Statistical uncertainties only which do not C223500100039 reflect the overall uncertainty in the absolute C223500100040 cross-section scale C223500100041 HISTORY (20211007C) Compiled by S.H. C223500100042 ENDBIB 40 0 C223500100043 NOCOMMON 0 0 C223500100044 ENDSUBENT 43 0 C223500199999 SUBENT C2235002 20211007 C210C223500200001 BIB 3 6 C223500200002 REACTION ((1-H-2(6-C-14,HE3)5-B-13,PAR,DA,RSD)= C223500200003 (6-C-14(D,HE3)5-B-13,PAR,DA)) C223500200004 INC-SOURCE The 14C(T1/2 = 5730+-40 year) beam was produced from C223500200005 enriched 14C material in a Cs sputter source. C223500200006 STATUS (CURVE) Data taken from figs.10,11 of the reference. C223500200007 Waiting for data from author C223500200008 ENDBIB 6 0 C223500200009 COMMON 1 3 C223500200010 EN C223500200011 MEV/A C223500200012 17.1 C223500200013 ENDCOMMON 3 0 C223500200014 DATA 5 37 C223500200015 E-LVL ANG-CM ANG-ERR DATA-CM ERR-S C223500200016 MEV ADEG ADEG MB/SR MB/SR C223500200017 0.0 21.3 1.7 1.500 C223500200018 0.0 24.3 1.3 0.700 C223500200019 0.0 28.5 1.2 0.500 C223500200020 0.0 30.9 1.0 0.700 C223500200021 0.0 34.4 1.0 1.100 C223500200022 0.0 36.4 1.0 1.100 C223500200023 0.0 39.7 2.0 1.000 C223500200024 0.0 41.5 1.5 0.700 C223500200025 0.0 44.2 1.3 0.800 C223500200026 0.0 45.9 1.0 0.600 0.100 C223500200027 0.0 48.5 1.0 0.400 0.100 C223500200028 3.8 23.0 1.6 0.095 C223500200029 3.8 26.0 1.5 0.103 C223500200030 3.8 30.0 1.5 0.087 0.011 C223500200031 3.8 33.0 1.8 0.089 0.011 C223500200032 3.8 36.5 1.2 0.098 0.013 C223500200033 3.8 39.0 1.2 0.109 0.014 C223500200034 3.8 41.9 1.0 0.149 0.021 C223500200035 3.8 44.0 1.0 0.151 0.023 C223500200036 4.8 24.0 1.5 0.116 0.008 C223500200037 4.8 27.5 1.7 0.118 0.009 C223500200038 4.8 32.0 1.3 0.117 0.009 C223500200039 4.8 34.5 1.3 0.098 0.008 C223500200040 4.8 38.5 1.1 0.083 0.013 C223500200041 4.8 40.5 1.0 0.081 0.010 C223500200042 5.3 17.0 1.6 0.065 0.011 C223500200043 5.3 21.0 1.7 0.037 0.007 C223500200044 5.3 26.1 1.3 0.044 0.007 C223500200045 5.3 29.0 1.3 0.044 0.007 C223500200046 5.3 33.0 1.1 0.044 0.008 C223500200047 5.3 36.0 1.1 0.039 0.008 C223500200048 6.3 13.2 2.0 0.045 0.008 C223500200049 6.3 18.0 2.0 0.038 0.007 C223500200050 6.3 24.0 1.6 0.070 0.009 C223500200051 6.3 26.4 1.5 0.087 0.011 C223500200052 6.3 30.6 1.5 0.128 0.016 C223500200053 6.3 34.3 1.6 0.115 0.015 C223500200054 ENDDATA 39 0 C223500200055 ENDSUBENT 54 0 C223500299999 SUBENT C2235003 20211007 C210C223500300001 BIB 3 9 C223500300002 REACTION ((1-H-2(6-C-15,HE3)5-B-14,PAR,DA,RSD)= C223500300003 (6-C-15(D,HE3)5-B-14,PAR,DA)) C223500300004 INC-SOURCE The 14C beam bombarded a cryogenic D2 gas cell held at C223500300005 a pressure of 1400 mbar and at a temperature of C223500300006 -184 deg C. The 15C beam was made from d(14C,15C)p C223500300007 reactions in the cell. The resulting 15C beam had C223500300008 intensity approx. 5E+05 part/s C223500300009 STATUS (CURVE) Data taken from fig.12 of the reference. C223500300010 Waiting for data from author C223500300011 ENDBIB 9 0 C223500300012 COMMON 1 3 C223500300013 EN C223500300014 MEV/A C223500300015 15.7 C223500300016 ENDCOMMON 3 0 C223500300017 DATA 5 12 C223500300018 E-LVL ANG-CM ANG-ERR DATA-CM ERR-S C223500300019 MEV ADEG ADEG MB/SR MB/SR C223500300020 0.0 21.4 3.0 0.868 0.262 C223500300021 0.0 28.5 3.5 0.671 0.182 C223500300022 0.0 34.8 2.5 1.058 0.231 C223500300023 0.0 40.3 2.5 1.256 0.321 C223500300024 0.0 45.7 2.1 0.568 0.176 C223500300025 0.0 50.0 2.1 0.439 0.202 C223500300026 1.8 10.7 3.0 0.639 0.289 C223500300027 1.8 18.6 3.5 0.348 0.159 C223500300028 1.8 26.0 2.5 0.328 0.139 C223500300029 1.8 32.7 2.6 0.100 0.070 C223500300030 1.8 38.2 2.1 0.050 0.050 C223500300031 1.8 43.4 2.0 0.070 0.069 C223500300032 ENDDATA 14 0 C223500300033 ENDSUBENT 32 0 C223500399999 ENDENTRY 3 0 C223599999999