ENTRY 14179 20140417 14011417900000001 SUBENT 14179001 20140417 14011417900100001 BIB 12 46 1417900100002 TITLE Parity violation in neutron resonances of antimony 1417900100003 and iodine 1417900100004 AUTHOR (Y.Matsuda,J.D.Bowman,B.E.Crawford,P.P.J.Delheij, 1417900100005 T.Haseyama, J.N.Knudsen,L.Y.Lowie,A.Masaike,Y.Masuda, 1417900100006 G.E.Mitchell, S.I.Penttila,H.Postma,N.R.Roberson, 1417900100007 S.J.Seestrom,E.I.Sharapov, S.L.Stephenson,Y.-F.Yen, 1417900100008 V.W.Yuan) 1417900100009 INSTITUTE (1USALAS,1USADKE,1USATNL,1CANTMF, 1417900100010 1USANCS,2JPNKEK,2NEDDEL,4ZZZDUB) 1417900100011 REFERENCE (J,PR/C,64,015501,2001) 1417900100012 FACILITY (LINAC,1USALAS)Measurements were performed at the 1417900100013 Manuel Lujan Jr. Neutron Scattering Center pulsed 1417900100014 spallation neutron source at Los Alamos Neutron 1417900100015 Science Center.The measurements were performed on 1417900100016 flight path 2, which views a gadolinium-poisoned water 1417900100017 moderator and has a cadmium/boron liner to reduce the 1417900100018 number of low-energy neutrons emerging in the tail of 1417900100019 the neutron pulse. After the moderator the neutrons are1417900100020 collimated to a 10-cm diameter beam inside a 4-m thick 1417900100021 biological shield. 1417900100022 SAMPLE The cylindrical sample of natural antimony had an 1417900100023 areal density of 3.67E23 atoms/cm2 of 121Sb and 1417900100024 2.74E23 atoms/cm2 of 123Sb. Enriched Sb sample 1417900100025 was enriched to 99.48% in 121Sb. The natural 1417900100026 crystalline iodine target had an areal density 1417900100027 of 7.24E23 atoms/cm2. 1417900100028 DETECTOR (SCIN) The 10B-loaded liquid scintillation neutron 1417900100029 detector was located 56.7 m from the neutron source. 1417900100030 The 55-cell segmented detector can handle 1417900100031 instantaneous counting rates up to 9 MHz per cell. 1417900100032 The neutron mean capture time in the detector 1417900100033 was 416+-5 ns 1417900100034 METHOD (TOF) Neutron energy was determined by time-of-flight 1417900100035 (TRN) Transmission method was used. 1417900100036 INC-SOURCE (POLNS,SPALL) The neutrons pass through a 1417900100037 polarized-proton spin filter where neutrons with one 1417900100038 of the two helicity states are preferentially scattered1417900100039 out of the beam, leaving a beam of longitudinally 1417900100040 polarized neutrons with polarization of 70%. 1417900100041 ANALYSIS (MLA) A multilevel, multichannel formalism of Reich 1417900100042 and Moore was used for the neutron cross sections, 1417900100043 which were convoluted with the TOF resolution function 1417900100044 ERR-ANALYS (DATA-ERR) No information given 1417900100045 HISTORY (20080824C) Compiled by S.H. 1417900100046 (20140417A) SD: Unnecessary "6" at the end of values 1417900100047 in col. DATA deleted in Subents 2,3. 1417900100048 ENDBIB 46 0 1417900100049 COMMON 1 3 1417900100050 POL-BM 1417900100051 NO-DIM 1417900100052 0.70 1417900100053 ENDCOMMON 3 0 1417900100054 ENDSUBENT 53 0 1417900199999 SUBENT 14179002 20140417 14011417900200001 BIB 3 5 1417900200002 REACTION 1(51-SB-121(N,0),,EN) 1417900200003 2(51-SB-121(N,EL),,WID,,G) 1417900200004 STATUS (TABLE) Data taken from Tab. 1 of PR/C,64,015501 1417900200005 HISTORY (20140417A) SD: Unnecessary "6" at the end of values 1417900200006 in col. DATA (1) deleted. 1417900200007 ENDBIB 5 0 1417900200008 NOCOMMON 0 0 1417900200009 DATA 3 171 1417900200010 DATA 1DATA 2DATA-ERR 2 1417900200011 EV MILLI-EV MILLI-EV 1417900200012 37.9 0.0085 0.0009 1417900200013 55.21 0.014 0.002 1417900200014 92.10 0.017 0.002 1417900200015 110.7 0.037 0.005 1417900200016 141.2 0.0081 0.0008 1417900200017 174.5 0.0054 0.0005 1417900200018 176.9 0.043 0.004 1417900200019 184.7 0.126 0.012 1417900200020 200.3 0.0054 0.0005 1417900200021 228.6 0.044 0.004 1417900200022 235.9 0.019 0.002 1417900200023 245.9 0.235 0.022 1417900200024 249.0 0.128 0.012 1417900200025 261.6 0.181 0.018 1417900200026 265.8 0.167 0.017 1417900200027 270.0 0.208 0.021 1417900200028 274.8 0.153 0.015 1417900200029 ENDDATA 19 0 1417900200030 ENDSUBENT 29 0 1417900299999 SUBENT 14179003 20140417 14011417900300001 BIB 3 5 1417900300002 REACTION 1(51-SB-123(N,0),,EN) 1417900300003 2(51-SB-123(N,EL),,WID,,G) 1417900300004 STATUS (TABLE) Data taken from Tab. 2 of PR/C,64,015501 1417900300005 HISTORY (20140417A) SD: Unnecessary "6" at the end of values 1417900300006 in col. DATA (1) deleted. SF3=G -> EL in REACTION code1417900300007 ENDBIB 5 0 1417900300008 NOCOMMON 0 0 1417900300009 DATA 3 5 1417900300010 DATA 1DATA 2DATA-ERR 2 1417900300011 EV MILLI-EV MILLI-EV 1417900300012 176.4 0.176 0.017 1417900300013 186.1 0.154 0.015 1417900300014 197.7 0.243 0.024 1417900300015 202.0 0.160 0.016 1417900300016 225.2 0.160 0.016 1417900300017 ENDDATA 7 0 1417900300018 ENDSUBENT 17 0 1417900399999 SUBENT 14179004 20080824 13511417900400001 BIB 2 3 1417900400002 REACTION 1(53-I-127(N,0),,EN) 1417900400003 2(53-I-127(N,EL),,WID,,G) 1417900400004 STATUS (TABLE) Data taken from Tab. 3 of the reference 1417900400005 ENDBIB 3 0 1417900400006 NOCOMMON 0 0 1417900400007 DATA 3 20 1417900400008 DATA 1DATA 2DATA-ERR 2 1417900400009 EV MILLI-EV MILLI-EV 1417900400010 7.51 0.00012 0.0001 1417900400011 10.34 0.0028 0.0003 1417900400012 13.93 0.0014 0.0001 1417900400013 24.63 0.00064 0.0006 1417900400014 52.20 0.00085 0.0008 1417900400015 53.82 0.019 0.002 1417900400016 64.04 0.008 0.001 1417900400017 85.84 0.0174 0.002 1417900400018 101.1 0.014 0.002 1417900400019 126.0 0.0021 0.0002 1417900400020 134.1 0.025 0.003 1417900400021 136.9 0.040 0.004 1417900400022 145.7 0.033 0.003 1417900400023 153.6 0.096 0.003 1417900400024 223.4 0.011 0.001 1417900400025 256.8 0.052 0.005 1417900400026 274.7 0.022 0.002 1417900400027 282.1 0.0045 0.0005 1417900400028 352.0 0.088 0.009 1417900400029 353.3 0.089 0.009 1417900400030 ENDDATA 22 0 1417900400031 ENDSUBENT 30 0 1417900499999 ENDENTRY 4 0 1417999999999