168RE    172IR A DECAY (2.19 S)        2004GOZZ,1996PA01,1992SC1610NDS    201008
168RE  H TYP=FUL$AUT=CORAL M. BAGLIN$CIT=NDS 111, 1807 (2010)$CUT=15-Jun-2010$
168RE C  2004GOZZ: 172IR SOURCES FROM |a-DECAY OF 176AU PRODUCED IN 84SR
168RE2C  BOMBARDMENT OF Mo; FRAGMENT MASS ANALYZER AND DOUBLE-SIDED SI STRIP
168RE3C  DETECTOR (FOR RECOILS AND DECAY |a PARTICLES) SURROUNDED BY 4 Ge
168RE4C  DETECTORS AND A LOW-ENERGY PHOTON SPECTROMETER; RECOIL DECAY TAGGING
168RE5C  TECHNIQUE; MEASURED EA, IA, RECOIL-|a-G COIN, |a(t), PARENT-DAUGHTER
168RE6C  |a CORRELATIONS.
168RE C  1992SC16: sources from 141PR(36AR,5n), E(36AR)=234 MEV PRIMARY BEAM,
168RE2C  helium-jet transport; monoisotopic targets; measured excitation
168RE3C  functions (175 MEV TO 204 MEV AT TARGET FACE), EA, EG, IA, IG,
168RE4C  AG coin, |a-(XK) coin.
168RE C  PARENT ^T{-1/2}: from ALPHA(T); WEIGHTED AVERAGE OF 2.26 S 5
168RE2C  (2004GOZZ), 2.0 S 1 (1992Sc16) AND 2.1 S 1 (1978Sc26).  OTHERS: 1.7 S 5
168RE3C  (1967Si02), 2.1 S 5 (1984SCZQ).
168RE CA HF        IF R0=1.5580 12, UNWEIGHTED AVERAGE OF R0(166W)=1.560 6
168RE2CA (2008BA14), R0(168W)=1.56 2 AND R0(168OS)=1.557 4 (THIS EVALUATION),
168RE3CA AND R0(170OS)=1.555 3 (2002BA93) (WEIGHTED AVERAGE IS 1.5564 22).
168RE4CA QA=5996 7 (FROM MEASURED EA FOR GS TO 349 LEVEL DECAY) HAS BEEN USED
168RE5CA FOR THE CALCULATION OF HF; 2003AU03 AND 2009AUZZ GIVE QA=5850 110 FROM
168RE6CA SYSTEMATICS.
168RE CG           RI(RE XK)=29 2 on same scale as RI (1992SC16).
168RE CG E,RI      FROM 1992SC16.
168RE CL E         FROM EG.
168RE CL J         FROM Adopted Levels.
172IR  P 133        8 (8+)             2.19 S    7              5996       7
172IR CP E         BECAUSE 1992ME10 REPORT NO EVIDENCE FOR AN ISOMERIC EXCITED
172IR2CP STATE IN 168RE, 1992SC16 CONCLUDE THAT BOTH THIS 5828A-162G CASCADE AND
172IR3CP THE 5515A-90G-123G-136G CASCADE FROM LOW-J 172IR TERMINATE AT THE 168RE
172IR4CP GS, IMPLYING E=133 8 FOR THE HIGH-J 172IR PARENT.  NOTE, HOWEVER, THAT
172IR5CP 2004GOZZ OBSERVE NEITHER THE 90G NOR THE 136G FROM THE LATTER CASCADE,
172IR6CP POSSIBLY DUE TO STATISTICALLY-LIMITED DATA.
168RE  N                       0.23     3
168RE CN BR        FROM 1992SC16. OTHERS: 0.22 6 (2004GOZZ), <32 (1984SCZQ).
168RE PN                                                                    C5
168RE2PN RELATIVE RI.  ALPHAS: PER 100 ALPHA DECAYS
168RE  L  0.0         (7+)
168RE  L  162.1     2 (8+)
168RE  A  5828      3 100      3.0      4                                   C
168RE CA E         5828 3 from 1982De11 (used for calibration by 1992Sc16).
168RE2CA OTHER DATA: 5810 5 (1967Si02 AND 1984SCZQ)), 5815 10 (1978Sc26),
168RE3CA 5822 12 (1996PA01), 5830 5 (2004GOZZ).
168RE CA           CORRELATED WITH 6080A, 6117A AND 6287A FROM 176AU(HIGH J)
168RE2CA (2004GOZZ).
168RE  G  162.1     2 44      4 M1+E2     0.99   16    0.99    6             C
168RES G KC=0.69 7$LC=0.226 10$MC=0.055 3$NC+=0.0152 8
168RES G NC=0.0132 7$OC=0.00202 8$PC=7.2E-5 9
168RE CG E         A 162G DEEXCITING THE LEVEL FED BY THE 5830A IS SHOWN IN
168RE2CG FIG. 6.4, IT APPEARS IN COINCIDENCE WITH THE 5830A IN FIG. 6.12, AND IS
168RE3CG MENTIONED IN TEXT (SECTION 6.4.1) OF 2004GOZZ.  HOWEVER,
168RE4CG IN TABLE 5.1, THE G COINCIDENT WITH THE 5830A HAS EG=136.3 5; THE
168RE5CG EVALUATOR ASSUMES THAT THE LATTER EG ENTRY IS ERRONEOUS.
168RE CG M,MR      from EKC=0.69 6, as deduced from RI and I(RE XK) (1992SC16).
168RE2CG MR=1.08 16 WAS DEDUCED BY 1992SC16 FROM BOTH EKC AND FROM THE RELATIVE
168RE3CG INTENSITIES OF THE 5828|a AND THE (5828|a+CEL(162)) SUM PEAK.