205PO    209RN A DECAY                 1971GO35                  20NDS    202006
205PO  H TYP=FUL$AUT=F.G. KONDEV$CIT=NDS 166, 1 (2020)$CUT=20-Apr-2020$
205PO CA HF$Using R0(205PO)=1.467 10, unweighted average value deduced from
205PO2CA values for neighboring even-even 204PO (R0=1.476 5) and 206PO
205PO3CA (R0=1.4569 22) nuclei and HF{-|a}=1.
205PO CA E,IA$ From 1971Go35
205PO CL E$ From the measured E|a.
205PO CL J,T$ From adopted levels, unless otherwise stated.
205PO CL E(A)$CONF=|n(f{-5/2}{+-1})
205PO CL E(B)$CONF=|n(p{-1/2}{+-1})
205PO CL E(C)$CONF=|n(p{-3/2}{+-1})
209RN  P 0.0          5/2-             28.8 M    10              6155.4   20
209RN CP $1971Go35: Mass separated source was produced in bombardment of a
209RN2CP metallic thorium target with 660 MEV proton beams. Detectors: magnetic
209RN3CP spectrograph with energy resolution of 4-6 KEV; Measured: EA, IA, T1/2,
209RN4CP and %A. Others: 1955Mo68, 1955Mo69, 1971Jo19 and 1993Wa04
209RN cP $J|p, T{-1/2}, and %|a from 2015Ch30. Q(|a) from 2017Wa10. Note, that
209RN2cP %|a= 9% {I2} in 2017Lo13, but the authors do not exclude a {+209}Rn
209RN3cP diffusion out of the detector material that could result in lower %|a.
205PO  N 1.0         1.0        0.17    2
205PO PN                                                                     1
205PO  L 0.0          5/2-             1.74 H    8                          A
205PO  A 6039       3 99.62  3   1.30  17
205PO CA E$Others: 6037 KEV 3 (1955Mo69) and 6036 KEV 3 (1993Wa04)
205PO  L    144     4 1/2-             310 NS    60                         BM1
205PO cL T$ From |a|g(t) in 1971Jo19.
205PO  A 5898       3 0.139  20  209   41
205PO  L    155     4 3/2-                                                  C
205PO  A 5887       3 0.219  20  118   19
205PO  L    386     4 (3/2)-
205PO  A 5660       3 0.0239 20   86   14