195TL    199BI A DECAY (24.70 M)       1950NE77,1964SI11,1966MA5114NDS    201408
195TL  H TYP=FUL$AUT=Huang Xiaolong and Kang Mengxiao$CIT=NDS 121, 395 (2014)$
195TL2 H CUT=1-Mar-2014$
195TL c  Sources produced by {+208}Pb(d,{+11}N) (1950Ne77) and
195TL2c  {+208}Pb(p,{+10}N) (1964Si11,1966Ma51).
195TL c  1950Ne77: {+208}Pb(d,{+11}N), E(d)=180 MeV;
195TL2c  identification based upon excitation function, chemistry, and
195TL3c  growth of {+199}Tl daughter.
195TL c  1964Si11, 1966Ma51: {+208}Pb(p,{+10}N), E(p)=100-160 MeV;
195TL2c  identification based upon mass separator.
195TL c  For analysis, see 1978Va21.
195TL C  THE IDENTIFICATION OF THE 5.486-MEV ALPHA WITH A 199BI
195TL2C  EXCITED STATE CANNOT be MADE WITH COMPLETE CONFIDENCE SINCE SYSTEMATIC
195TL3C  GIVES 4820 KEV 1000 (1975BoYG) FOR THE GROUND-STATE Q-VALUE, AND THIS I
195TL4C  NOT NECESSARILY INCONSISTENT WITH THE OBSERVED QA OF 5599 KEV 6.
195TL5C  FURTHER, THE T=27 M 1 REPORTED FOR CE DECAY (1964Si11) LIES RELATIVELY
195TL6C  CLOSE TO THE MORE ACCURATELY DETERMINED T(ALPHA)=24.70 M 15. HOWEVER,
195TL7C  ALPHA DECAY FROM A (9/2-) 199BI GROUND STATE WOULD BE EXPECTED
195TL8C  TO POPULATE THE 483-KEV (9/2-) LEVEL IN 195TL WITH A CONSEQUENTLY
195TL9C  EVEN SMALLER ENERGY RELEASE.
195TL c  For the evaluations, see 1988Sc02 and 1986BrZQ.
195TL cL J(A),T(A)$From adopted levels
195TL  N 1                     0.0001  AP
195TL cN BR        |e/a|?8|*10{+3} (1950Ne77), K| x ray/a|?1|*10{+4}
195TL2cN (1964Si11); |e/a< 0.028 (1970DaZM). Value from 1988Sc02
199BI  P 667       4 (1/2+)            24.70 M   15             4933      7
195TL  L 0.0         1/2+               1.16 H   5
195TL3 L FLAG=A$
195TL  A 5484       5100          65   AP
195TL cA E         from weighted average of 5.49 MeV {I2} (1970DaZM), 5.49 {I1}
195TL2cA (1967Ti04), 5.481 {I6} (1966Ma51), 5.52 {I2} (1964Si11), 5.47 {I6}
195TLxcA (1950Ne77)
195TL cA HF        r{-0}=1.45
195TL cA           The |a decay of {+199}Bi(24.7 min) may be compared with that
195TL2cA of the 846(1/2+) level in {+201}Bi.