82KR 82RB EC DECAY (1.2575 M) 2016NI03,1983ME08 19NDS 201906
82KR H TYP=FUL$AUT=J. K. TULI, E. BROWNE$CIT=NDS 157, 260 (2019)$
82KR2 H CUT=1-Mar-2019$
82KR c Based on XUNDL compilation of 2016Ni03
82KR2c by E.A. McCutchan (NNDC,BNL), December 30, 2017 and
82KR3c 2012Gr03 compilation by
82KR4c J. Chen (NSCL, MSU): February 20, 2015
82KR c 2016Ni03: Source of {+82}Sr produced by irradiating thick RbCl
82KR2c targets with protons at the Brookhaven Linear Isotope Producer
82KR3c (BLIP), followed by
82KR3c chemical separation. Source for measurement was 100 |mCi. Measured
82KR4c E|g, I|g, |g|g, |g|g(|q) using the Gammasphere array consisting of 89
82KR5c Compton-suppressed HPGe detectors.
82KR c 2012Gr03: A technique developed to measure absolute intensity
82KR2c (photons/100 decays) of a gamma ray in {+82}Rb to {+82}Kr decay by
82KR3c ion-implantation
82KR c 2012Gr03: {+82}Rb ions were produced from the |e decay of the
82KR2c radioactive {+82}Sr beam, which was produced and accelerated above to
82KR3c 2.5 MeV/nucleon at the Holifield Radioactive Ion Beam Facility (HRIBF)
82KR4c at Oak Ridge National Laboratory. The beam was delivered to an
82KR5c ionization chamber for counting individual beam particles and measuring
82KR6c energy loss and then implanted into thin aluminum foils for
82KR7c subsequent offline |g-ray decay measurements with a Ge detector.
82KR8c Measured E|g, I|g, total count of decaying nuclei. Deduced the
82KR9c absolute |g-ray emission probability.
82KR c All data are from 2016Ni03, unless given otherwise. The decay scheme
82KR2c is from 2016Ni03 which has added additional levels to original
82KR3c scheme from 1983Me08
82KR c 1983Me08: Ge(Li), measured E|g, I|g, |g|g.
82KR c 1985Ze03: Measured ce, Magnetic spectrometer.
82KR c 1969Be74: Measured |b{++} spectrum
82KR c 2001Cr03: Measured |b{++}(E,|q,h), studied parity violation
82KR c 1969Ak03: Measured Internal Bremsstrahlung spectrum
82KR c Other: 1970Gr01.
82KR cG $All data are from 2016Ni03, unless given otherwise.
82KR cG M,MR$From |g|g(|q) in 2016Ni03.
82KR cG E(A)$Value from 2011Kr06 in 82Br |b{+-} decay
82KR cG E(B)$From E(level)
82KR cL E$From a least-squares fit to E|g
82KR cL J$As given in 2016Ni03, obtained from |g|g(|q) analysis (as noted),
82KR2cL previous literature values, and decay patterns.
82KR cL J(a)$J determined through |g|g(|q) analysis (2016Ni03). Unique
82KR2cL 0-2-0 pattern determined for 1395|g-775|g (2016Ni03,1970Hr02);
82KR3cL 2410|g-776|g, 2457|g-776|g, 2940|g-776|g, 975|g-1475|g, 1608|g-1956|g
82KR4cL cascades (2016Ni03)
82KR cE TI$From |g-ray intensity balance.
82KR DG CC$FROM BrIcc v2.3b (16-Dec-2014) 2008Ki07, "Frozen Orbitals" appr.
82KR cG MR$If no value given it was assumed |d=1.00 for E2/M1,
82KR2cG |d=1.00 for E3/M2 and |d=0.10 for the other multipolarities
82RB P 0 1+ 1.2575 M 2 4404 3
82RB cP J,T$From the Adopted Levels of {+82}Rb
82RB cP QP$From 2017Wa10
82KR N 0.1506 15 1.0 1.0 1.0
82KR cN NR$as given in 2016Ni03 based on weighted average of absolute
82KR2cN measurements of I|g(776): 0.149 {I4} (1987Ho06), 0.1512 {I18}
82KR3cN (1987Ju01), 0.1493 {I37} (2012Gr03).
82KR PN 3
82KR L 0 0+
82KR E 81.8 4 3.00 3 4.576 3 84.8 4
82KRS E EAV=1536.0 15$CK=0.03108 8$CL=0.003593 10$CM+=0.0007375 1
82KR L 776.523 8 2+
82KR E 13.0 4 1.05 3 4.863 13 14.1 4
82KRS E EAV=1169.0 14$CK=0.06547 22$CL=0.007577 25$CM+=0.001555 5
82KR G 776.511 10 100.0 20 Q A
82KR L 1474.904 8 2+ a
82KR E 0.158 5 0.0332 11 6.178 14 0.191 6
82KRS E EAV=844.6 14$CK=0.1523 7$CL=0.01766 8$CM+=0.003625 15
82KR G 698.361 10 0.95 3 A
82KR G 1474.895 10 0.63 2 Q A
82KR L 1487.70 5 0+
82KR E 0.0416 11 0.0089224 6.744 12 0.0505 13
82KRS E EAV=838.7 14$CK=0.1550 7$CL=0.01796 8$CM+=0.003689 15
82KR G 711.09 7 0.358 8
82KR G 1488 E0 6.2E-6 6 B
82KR cG $K/K+L+=0.76$L/K+L+=0.07
82KR cG $ce(K)(1488|g)/ce(K)(1475|g)=0.31 {I3};
82KR2cG ce(K)(1488|g)=4.7|*10{+-6} {I5} per 100 {+82}Rb decays (1985Ze03)
82KR L 1820.538 13 4+
82KR E 0.0003211 0.000135 8.48 16 0.00045 16
82KRS E EAV=686.8 14$CK=0.2476 11$CL=0.02873 13$CM+=0.00590 3
82KR G 1044.005 10 0.008 1 A
82KR L 1956.771 16 (2+) a
82KR E 0.0026 7 0.0014 4 7.40 12 0.0040 11
82KRS E EAV=625.3 14$CK=0.3022 14$CL=0.03509 16$CM+=0.00721 4
82KR G 1180.209 24 0.112 6 D+Q -0.52 16 A
82KR G 1956.740 21 0.043 2 Q A
82KR L 2094.018 10 3+
82KR G 619.105 10 0.0103 8 A
82KR G 1317.485 10 0.0063 7 A
82KR L 2171.81 5 0+ a
82KR E 0.32 2 0.28 1 5.010 22 0.60 3
82KRS E EAV=529.0 14$CK=0.4131 18$CL=0.04802 21$CM+=0.00986 5
82KR G 696.85 7 0.176 4
82KR G 1395.26 7 3.81 19 Q
82KR G 2172 E0 5E-5 1 B
82KRS G K/T=0.3$L/T=0.03
82KR cG $ce(K)(2172|g)/ce(K)(2168|g)=4.1 {I10};
82KR2cG ce(K)(2172|g)=1.4|*10{+-5} {I3} per 100 {+82}Rb decays (1985Ze03)
82KR L 2450.19 5 0+ a
82KR E 0.0048820 0.0103 4 6.331 18 0.0152 6
82KRS E EAV=406.1 14$CK=0.5952 21$CL=0.06930 25$CM+=0.01424 5
82KR G 975.22 7 0.056 2
82KR G 1673.70 7 0.045 3
82KR L 2480.06 3 2+ a
82KR E 0.0298 12 0.070 3 5.485 18 0.100 4
82KRS E EAV=393.0 14$CK=0.6158 21$CL=0.07170 25$CM+=0.01473 5
82KR G 523.24 7 0.062 2
82KR G 659.38 7 0.0050 3
82KR G 992.27 9 0.0139 4
82KR G 1703.54 7 0.36 2 D+Q 1.03 10
82KR G 2480.23 7 0.24 1
82KR L 2547.468 13 (3-)
82KR E 4.E-5 3 0.0001111 8.2 4 0.00015 14
82KRS E EAV=363.6 13$CK=0.6614 20$CL=0.07705 24$CM+=0.01583 5
82KR G 1072.554 10 0.0081 7 A
82KR L 2655.96 4 2+ a
82KR E 0.0024712 0.0122 6 6.160 21 0.0147 7
82KRS E EAV=316.6 13$CK=0.7296 18$CL=0.08507 21$CM+=0.01748 5
82KR G 699.41 13 0.0042 6
82KR G 1168.23 7 0.0060 3
82KR G 1181.05 7 0.0091 8
82KR G 1879.61 7 0.068 4 D+Q -0.71 21
82KR G 2655.56 8 0.0141 3
82KRF G FL=0
82KR L 2676.0 3
82KR E 0.00016122 0.0008812 7.29 6 0.00104 14
82KRS E EAV=308.0 13$CK=0.7411 18$CL=0.08642 21$CM+=0.01776 5
82KR G 1899.5 3 0.0069 9
82KR L 2684.45 12
82KR E 0.00040525 0.0023114 6.87 3 0.00271 16
82KRS E EAV=304.3 13$CK=0.7459 17$CL=0.08698 20$CM+=0.01787 4
82KR G 1907.90 12 0.018 1
82KR L 2944.52 4 2 a
82KR E 0.001538 0.0471 20 5.417 19 0.0486 21
82KRS E EAV=193.2 13$CK=0.8489 7$CL=0.09925 9$CM+=0.02040 2
82KR G 396.93 20 0.0029 5
82KR G 850.37 7 0.0026 2
82KR G 987.60 21 0.0031 5
82KR G 1469.64 9 0.016 1
82KR G 2168.06 7 0.262 13 D+Q 0.06 LT
82KR G 2944.61 12 0.0358 18
82KR L 2964.81 16
82KR E 1.5E-5 3 0.0005511 7.34 9 5.6E-4 11
82KRS E EAV=184.5 13$CK=0.8532 7$CL=0.09979 8$CM+=0.02051 2
82KR G 2188.26 16 0.0037 7
82KR L 2993.43 18
82KR E 8.4E-6 14 0.000407 7.46 8 0.00041 7
82KRS E EAV=172.4 13$CK=0.8585 6$CL=0.10044 7$CM+=0.02065 2
82KR G 2217.7 3 0.0010 4
82KR G 2992.97 21 0.0017 2
82KR L 3131.35 17
82KR E 3.1E-6 5 0.0008413 7.05 7 8.4E-4 13
82KRS E EAV=113.9 13$CK=0.8729 2$CL=0.10232 3$CM+=0.021040 5
82KR G 1656.47 22 0.0021 5
82KR G 2354.73 24 0.0035 7
82KR L 3187.15 5 (0)+ a
82KR E 3.8E-5 3 0.0288 13 5.471 20 0.0288 13
82KRS E EAV=90.1 13$CK=0.8749$CL=0.10265 2$CM+=0.021110 3
82KR G 1230.35 7 0.0134 7
82KR G 1712.24 7 0.013 1
82KR G 2410.65 17 0.165 8 Q
82KR L 3207.1 3
82KR E 4.8E-4 8 7.23 8 4.8E-4 8
82KRS E CK=0.8753$CL=0.10273 2$CM+=0.021127 3
82KR G 2430.5 3 0.0032 5
82KR L 3217.2 3
82KR E 4.1E-4 8 7.30 9 4.1E-4 8
82KRS E CK=0.8755$CL=0.1028$CM+=0.021135 3
82KR G 1742.23 30 0.0027 5
82KR L 3234.06 10 (0+) a
82KR E 0.0022317 6.55 4 0.00223 17
82KRS E CK=0.8756$CL=0.1028$CM+=0.02115
82KR G 754.03 16 0.0050 6
82KR G 1276.93 19 0.0048 8
82KR G 2457.69 15 0.0050 5 Q
82KR L 3285.81 5
82KR E 0.0040517 6.248 19 0.00405 17
82KRS E CK=0.8758$CL=0.1029$CM+=0.02118
82KR G 805.76 7 0.0043 4
82KR G 1113.71 15 0.0007 2
82KR G 1191.61 18 0.0048 3
82KR G 2509.31 7 0.0171 9
82KR L 3355.99 7 1,2(+)
82KR E 0.001399 6.66 3 0.00139 9
82KRS E CK=0.8757$CL=0.1031$CM+=0.02121
82KR G 1399.31 23 0.0010 2
82KR G 2579.18 11 0.0063 5
82KR G 3356.09 10 0.0019 1
82KR L 3438.15 12
82KR E 9.9E-4 10 6.73 5 9.9E-4 10
82KRS E CK=0.8755$CL=0.1033$CM+=0.02125
82KR G 1963.21 20 0.0020 5
82KR G 2661.58 14 0.0046 4
82KR L 3457.21 14 1,2(+)
82KR E 0.000426 7.09 7 0.00042 6
82KRS E CK=0.8754$CL=0.1033$CM+=0.02126
82KR G 2681.5 4 0.0019 4
82KR G 3457.03 14 0.000895
82KR L 3565.12 5 (0)+ a
82KR E 0.0057 3 5.847 23 0.0057 3
82KRS E CK=0.8750$CL=0.1036$CM+=0.021336 3
82KR G 908.85 22 0.004 1
82KR G 1085.08 11 0.0032 4
82KR G 1608.21 7 0.0194 10 Q
82KR G 2090.00 29 0.0044 7
82KR G 2788.81 9 0.0071 5
82KR L 3716.15 6 (2+) a
82KR cL J$From adopted levels; 0+ in 2016Ni03 from |g|g(|q)
82KR E 0.0052418 5.708 16 0.00524 18
82KRS E CK=0.8743$CL=0.10423 2$CM+=0.021479 4
82KR G 1168.40 8 0.0032 2
82KR G 1621.99 13 0.0020 2
82KR G 1759.25 25 0.0026 4
82KR G 2940.09 10 0.027 1 Q
82KRF G FL=776.523
82KR L 3742.76 6
82KR E 0.0050522 5.689 20 0.00505 22
82KRS E CK=0.8741$CL=0.10436 2$CM+=0.021511 4
82KR G 1195.72 16 0.0010 1
82KR G 1570.88 15 0.0014 2
82KR G 1648.76 23 0.0022 3
82KR G 1785.85 7 0.018 1
82KR G 2255.02 31 0.0026 3
82KR G 2268.24 21 0.0041 7
82KR G 2966.17 14 0.0042 4
82KR L 3815.23 7 1,2(+)
82KR E 6.8E-4 4 6.46 3 6.8E-4 4
82KRS E CK=0.8736$CL=0.10480 2$CM+=0.021613 5
82KR G 3038.3 4 0.0009 2
82KR G 3815.15 7 0.0036 1
82KR L 3836.13 6 1,2
82KR E 0.0022314 5.91 3 0.00223 14
82KRS E CK=0.8734$CL=0.10494 3$CM+=0.021647 6
82KR G 1741.73 18 0.0039 3
82KR G 2360.96 21 0.0042 7
82KR G 3059.47 12 0.0053 4
82KR G 3836.18 8 0.001418
82KR L 3881.00 7 1,2(+)
82KR E 1.25E-310 6.09 4 1.25E-3 10
82KRS E CK=0.8730$CL=0.10530 3$CM+=0.021731 7
82KR G 1400.82 10 0.0039 5
82KR G 1786.7 3 0.0017 2
82KR G 2405.95 13 0.0009 2
82KR G 3104.60 23 0.0014 2
82KR G 3881.47 19 0.000415
82KR L 3910.85 12 1,2(+)
82KR E 0.00014311 6.98 4 0.000143 11
82KRS E CK=0.8726$CL=0.10557 3$CM+=0.021795 7
82KR G 3910.75 12 0.000957
82KR L 3920.01 24
82KR E 6.0E-5 15 7.34 11 6.0E-5 15
82KRS E CK=0.8725$CL=0.10566 3$CM+=0.021817 8
82KR G 3143.42 24 0.0004 1
82KR L 3958.05 14 1,2(+)
82KR E 1.22E-410 6.96 4 1.22E-4 10
82KRS E CK=0.8720$CL=0.10608 4$CM+=0.021916 9
82KR G 3957.95 14 0.000816