ENTRY C0466 19990331 0000C046600000001 SUBENT C0466001 19990331 0000C046600100001 BIB 12 29 C046600100002 INSTITUTE (1USAWIS,2SWTZUR) C046600100003 REFERENCE (J,PR/C,40,1586,198910) C046600100004 AUTHOR (W.Zhenjie,R.A.Bigelow,P.A.Quin,J.Liechti) C046600100005 TITLE Production of polarized 8Li with the C046600100006 7Li(d-pol,8Li-pol)p reaction. C046600100007 FACILITY (VDGT,1USAWIS) C046600100008 INC-SOURCE (POLIS) Polarized ion source used to provide a C046600100009 momentum analyzed,variable energy, beam of C046600100010 vector polarized deuterons with polarization C046600100011 py or pz = 0.59 (0.01). The maximum py or pz C046600100012 for a purely vector polarized beam is +-2/3. C046600100013 The tenzor polarization of the beams were C046600100014 pyy and pzz < 0.05. C046600100015 SAMPLE Targets were typically 1-mm thick Li metal wafers, C046600100016 enriched to 99.9 % in 7Li, and held near C046600100017 liquid-nitrogen temperature (77 K). C046600100018 METHOD (ACTIV) Target was activated for 1 s and activity C046600100019 counted as function of time for 4 s. The sign of C046600100020 the deuteron polarization was reversed, and the C046600100021 cycle repeated. C046600100022 DETECTOR (TELES,SCIN) Plastic scintillators or detector C046600100023 telescopes sufficiently thick to stop 16-MeV C046600100024 electrons for detecting of beta-particles. C046600100025 DECAY-DATA (3-LI-8,,B) Nominal endpoint energy is 13 MeV with C046600100026 2.94-MeV level of 8Be rapidly decaying into two alpha C046600100027 particles. C046600100028 STATUS Data taken from Table 1 of reference. C046600100029 (APRVD) ZApproved by R.A. Bigelow, 31 March 1999 C046600100030 HISTORY (19990225C) VV C046600100031 ENDBIB 29 0 C046600100032 NOCOMMON 0 0 C046600100033 ENDSUBENT 32 0 C046600199999 SUBENT C0466002 20010307 0000C046600200001 BIB 4 7 C046600200002 REACTION 1(3-LI-7(D,P)3-LI-8,NN,POL/DA,,K) C046600200003 2(3-LI-7(D,P)3-LI-8,LL,POL/DA,,K) C046600200004 CORRECTION Since transient depolarization contributions were not C046600200005 included in analysis, results are more precisely C046600200006 lower bounds on polarization transfer coefficients. C046600200007 ERR-ANALYS (DATA-ERR) No information on source of uncertainties. C046600200008 HISTORY (20010307A) Date on subentry record corrected. C046600200009 ENDBIB 7 0 C046600200010 COMMON 2 3 C046600200011 ANG-MIN ANG-MAX C046600200012 ADEG ADEG C046600200013 0.0 180.0 C046600200014 ENDCOMMON 3 0 C046600200015 DATA 5 13 C046600200016 EN DATA 1DATA-ERR 1DATA 2DATA-ERR 2 C046600200017 MEV NO-DIM NO-DIM NO-DIM NO-DIM C046600200018 1.5 0.308 0.009 0.243 0.011 C046600200019 1.8 0.294 0.005 C046600200020 2.0 0.281 0.013 0.249 0.007 C046600200021 2.5 0.236 0.012 0.238 0.009 C046600200022 3.0 0.239 0.011 0.243 0.012 C046600200023 3.5 0.229 0.012 0.245 0.017 C046600200024 4.0 0.220 0.016 0.249 0.005 C046600200025 5.0 0.233 0.012 0.252 0.016 C046600200026 6.0 0.230 0.009 0.231 0.007 C046600200027 7.0 0.228 0.013 0.238 0.008 C046600200028 8.0 0.196 0.012 0.229 0.014 C046600200029 9.0 0.205 0.007 0.231 0.008 C046600200030 10.0 0.214 0.019 0.235 0.008 C046600200031 ENDDATA 15 0 C046600200032 ENDSUBENT 31 0 C046600299999 ENDENTRY 2 0 C046699999999