130TE 130TE(64NI,XG):XUNDL-1 1998ZH09,2004BR19 201206 130TE c Includes {+232}Th({+136}Xe,x|g) from 2004Br19. 130TE c Compiled (unevaluated) dataset from 1998Zh09: 130TE c Nucl Phys A 628, 386 (1998) and 2004Br19: Eur Phys J A 20, 145 (2004) 130TE c Compiled by J. Roediger and B. Singh (McMaster) September 9, 2004 130TE c Edited by B. Singh June 21, 2012 in response to email reply from 130TE2c R. Broda on June 15, 2012: 331 doublet |g rays reversed in placement 130TE3c and I|g. The GTOL code run again for least-squares fit. 130TE c 1998Zh09: E=275 MeV. Measured E|g, I|g, |g|g, |g|g(t), |g|g(|q) with 130TE2c the GASP multidetector |g-ray array. This reaction was performed in 130TE3c two seperate experiments. In the first, the beam was pulsed with 200 130TE4c ns intervals, and high statistics |g-ray coincidence data were 130TE5c collected with the 40 Ge detectors of the GASP array. Delayed 130TE6c |g-coincidences were measured with a seperate time-to-amplitude 130TE7c converter. The second experiment emphasized half-life determination 130TE8c for long-lived (t{-1/2}>100 ns) isomers. Off-beam |g-ray spectra were 130TE9c measured as a function of time using several beam-pulsing arrangements 130TExc covering a range from a few |ms to many ms. 130TE c 2004Br19: {+232}Th({+136}Xe,x|g) E=833 MeV. Measured E|g, I|g, |g|g, 130TE2c lifetimes with the GAMMASPHERE array of 73 large-volume 130TE3c Compton-suppressed Ge detectors. 130TE c All information taken from 1998Zh09 unless otherwise stated. 130TE cG RI$From 1998Zh09. Intensities were extracted from the 130TE2cG |g|g-coincidence data, mainly by gating on the yrast 2+ to 0+ |g-ray 130TE3cG in {+130}Te; the relative intensity of the 2+ to 0+ |g-ray itself was 130TE4cG obtained from cross coincidences with appropriate Ni |g-rays. 130TE5cG Uncertainties are <10%, as quoted in authors table 1. The compilers 130TE6cG have assigned a 10% uncertainty to each |g-ray from 1998Zh09. 130TE cG E(X)$From 2004Br19. 130TE cG E(A),RI(A)$ Placement and I|g values of 331-keV doublet reversed 130TE2cG as per email reply from one of the authors R. Broda on June 15, 2012. 130TE3cG The placements shown in 1998Zh09 were a print error 130TE cL E$From least-squares fit to E|g's (by compilers). Uncertainties for 130TE2cL |g-rays from 1998Zh09 are assigned by authors according to the 130TE3cL following criterion: 0.1 keV for I|g>3, and 0.3 keV for I|g<3. 130TE4cL For those transitions taken from 2004Br19 and the 46 keV transition 130TE5cL from the 7- isomer, a standard uncertainty of 1 keV is assumed. 130TE cL E$Yrast levels up to spins of 7 or 8 in {+130}Te are identified by 130TE2cL 1998Zh09 from previous |b-decay studies in literature. 130TE PN 5 130TE G 601.6 3 0.3 130TE cG E$Placement of transition belongs above the 7- isomer. 130TE L 0.0 0+ 130TE L 839.50 10 2+ 130TE G 839.5 1 5.3E2 5 130TE L 1588.46 14 2+ 130TE G 749.0 1 17.3 17 130TE L 1633.00 14 4+ 130TE G 793.5 1 100 10 130TE L 1815.70 17 6+ 10 NS 130TE cL $Configuration=(|pg{-7/2}{+2})6+ 130TE G 182.7 1 10.7 11 130TE L 1885.4 4 2+ 130TE G 1045.9 3 1.6 2 130TE L 1964.8 4 0+ 130TE G 1125.3 3 1.0 1 130TE L 1981.59 16 4+ 130TE G 348.6 1 4.6 5 130TE G 1142.0 3 2.8 3 130TE L 2101.30 17 5- 130TE G 468.3 1 13.7 14 130TE L 2138.82 21 3+ 130TE G 505.8 3 0.5 1 130TE G 550.8 3 1.4 2 130TE G 1298.9 3 2.8 3 130TE L 2146.72 19 7- 115 NS 130TE cL T$From ENSDF for {+130}Te 130TE cL $Configuration=(|nh{-11/2}d{-3/2})7- 130TE G 46 0.05 AP 130TE cG E$Existence required by |g|g coin data 130TE cG TI$Branching(46|g)|?4% 130TE G 331.0 1 4.8 5 A 130TE L 2331.2 4 4+ 130TE G 698.2 3 0.5 1 130TE L 2405.1 3 6- 130TE G 258.4 3 1.1 1 130TE G 303.7 3 1.0 1 130TE L 2432.2 3 7- 130TE G 285.5 3 1.7 2 130TE G 330.9 3 1.2 1 A 130TE L 2435.8 4 4- 130TE G 334.5 3 2.5 3 130TE L 2648.9 3 8+ 130TE G 502.0 3 0.9 1 130TE G 833.4 3 1.2 1 130TE L 2667.2 8 10+ 1.9 US 130TE cL T$From 2004Br19; 4.2 |ms 9 in 1998Zh09 (from observation of delayed 130TE2cL 6+ to 4+ to 2+ cascade between beam bursts). 130TE cL E$From 2004Br19; 2649+x in 1998Zh09, where x<90 keV. 130TE G 18.5 X S 130TE L 2878.8 4 130TE G 732.1 3 0.8 1 130TE L 3081.7 4 9- 130TE G 935.0 3 0.8 1 130TE L 3385.0 10 12+ 130TE G 718 X 130TE L 3540.1 5 11- 130TE G 458.3 3 0.3 130TE cG E$Placement from 2004Br19; this |g-ray is only defined as being 130TE2cG located above the 7- isomer in 1998Zh09 130TE G 873 X 130TE L 3951.6 8 130TE G 411 X 130TE G 870 X 130TE L 4250.9 8 13- 130TE G 299 X 130TE G 711 X 130TE G 866 X 130TE L 4377.9 13 15- 45 NS 130TE cL T$From 2004Br19. 130TE cL $Configuration=(h{-11/2}){+3}d{-3/2} (2004Br19). 130TE G 127 X 130TE COULOMB EXCITATION:XUNDL-2 2007ST24 200709 130TE c Compiled (unevaluated) dataset from 2007St24: 130TE2c Phys Rev C 76, 034306 (2007) 130TE c Compiled by S. Geraedts and B. Singh (McMaster): Sep 17, 2007 130TE C Reaction: 130TE(58NI,58NI'G) 130TE c E=195, {+58}Ni beam used to excite states of interest. Beam provided 130TE2c by ANU 14UD Pelletron accelerator. Backscattered particles were 130TE3c detected using two silicon detectors, and |g rays were detected with 130TE4c pairs of Ge detectors. Measured g factors by transient-field technique 130TE L 0 0+ 130TE L 839 2+ 130TE2 L G=+0.351 18 (2007ST24) 130TE G 839 130TE 130TE(N,N'G):XUNDL-3 2008HI17 200905 130TE c Compiled (unevaluated) dataset from 2008Hi17: 130TE2c Phys Rev C 78, 054320 (2008). 130TE c Compiled by A. MacDonald and B. Singh (McMaster); Dec 18, 2008. 130TE c Edited by B. Singh, May 27, 2009 in response to e-mail reply from 130TE2c of May 18, 2009 from the first author (S. Hicks) of 2008Hi17 130TE c E=2.0-3.3 MeV beam provided by accelerator at the University of 130TE2c Kentucky. Measured E|g, I|g, angular distributions using an n-type 130TE3c HPGe detector. Measured half-lives using Doppler-shift attenuation 130TE4c method. Study of 2+ states in connection with fragmentation 130TE5c of mixed-symmetry excitations 130TE cL T$ From DSAM (2008Hi17) unless otherwise stated 130TE PN 7 130TE L 0.0 0+ 130TE L 839.49 4 2+ 2.30 PS 5 130TE cL T$ from 'adopted levels, gammas' dataset for {+130}Te in ENSDF database 130TE G 839.49 4 100 E2 130TE2 G BE2W=15.1 3 130TE L 1588.17 8 2+ 2.1 PS GT 130TE cL T$ listed as <2.08 ps in table III and >2.01 ps in table IV of 130TE2cL 2008Hi17. It should be >2.01 ps according to e-mail reply of 130TE3cL May 18, 2009 from the first author of 2008Hi17 130TE G 748.76 4 98.1 3 E2+M1 130TE cG MR$+1.56 {I+23-19} or +0.16 {I10} 130TE cG $B(E2)(W.u.)<21 {I1} or 0.73 {I2} 130TE cG $B(M1)<1.3|*10{+-2} {I1} or 4.3|*10{+-2} {I+2-1} 130TE G 1588.09 2 1.9 1 E2 130TE2 G BE2W<1.3E-2 1 130TE L 1885.60 4 2+ 326 FS +28-21 130TE G 1046.11 2 98.5 4 E2+M1 130TE cG MR$+5.2 {I+24-13} or -0.26 {I+10-3} 130TE cG $B(E2)(W.u.)=34 {I3} or 2.2 {I+3-2} 130TE cG $B(M1)=3.7|*10{+-3} {I+3-4} or 9.7|*10{+-2} {I+8-11} 130TE G 1885.60 2 1.5 1 E2 130TE2 G BE2W=2.8E-2 4 130TE L 2190.21 4 2+ 409 FS 35 130TE G 1350.98 3 44.2 4 E2+M1 130TEF G FL=839.49 130TE cG MR$+6.2 {I+37-17} or -0.29 {I10} 130TE cG $B(E2)(W.u.)=3.4 {I4} or 0.27 {I+4-3} 130TE cG $B(M1)=4.4|*10{+-4} {I+5-4} or 1.6|*10{+-2} {I2} 130TE G 2190.48 3 55.8 6 E2 130TE2 G BE2W=0.39 4 130TE L 2282.43 4 2+ 104 FS 7 130TE cL T$105.4 fs {I14} in table IV of 2008Hi17 is incorrect. It should be 130TE2cL 104 fs {I7} according to e-mail reply of May 18, 2009 from the 130TE3cL first author of 2008Hi17 130TE G 1442.95 3 79.3 6 E2+M1 130TE cG MR$+3.5 {I+31-6} or -0.13 {I+13-14} 130TE cG $B(E2)(W.u.)=16 {I2} or 0.29 {I3} 130TE cG $B(M1)=7.7|*10{+-3} {I+8-9} or 9.8|*10{+-3} {I+10-9} 130TE G 2282.42 3 20.7 5 E2 130TE2 G BE2W=0.47 +5-4 130TE L 2300.14 7 (2+) 457 FS +42-35 130TE cL T$451 fs {I+42-35} in table IV of 2008Hi17 is a misprint, it should be 130TE2cL 457 fs {+42-35} according to e-mail reply of May 18, 2009 from the 130TE3cL first author of 2008Hi17 130TE G 1460.58 3 96.3 8 E2+M1 130TE cG MR$+7.6 {I+65-24} or -0.29 {I7} 130TE cG $B(E2)(W.u.)=4.5 {I5} or 0.36 {I4} 130TE cG $B(M1)=4.5|*10{+-4} {I4} or 2.5|*10{+-2} {I3} 130TE G 2300.20 6 3.7 4 E2 130TE2 G BE2W=1.8E-2 4 130TE 235U(N,FG):XUNDL-4 2012MU08 201207 130TE c Compiled (unevaluated) dataset from 2012Mu08: 130TE2c Phys Rev C 85, 064321 (2012) 130TE c Compiled by E. Thiagalingam and B. Singh (McMaster); July 12, 2012 130TE c E=thermal neutrons from the Canada India Research Utility Services 130TE2c (CIRUS) reactor facility, Bhabha Atomic Research Center (BARC), Mumbai. 130TE3c Target|?5.1 gm/cm{+3} UAl{-3} (17% enriched {+235}U). Gamma rays were 130TE4c detected by two clover HPGe detectors equipped with anti-Compton 130TE5c shields, in coincidence mode. Measured E|g, I|g, |g|g-coin. Deduced 130TE6c levels, J, |p, isotopic yield, angular momentum distribution. 130TE cG RI$ 2012Mu08 mention uncertainties of 5% to 25% depending on the 130TE2cG |g-ray intensity. Compilers assign 5% for |g rays with I|g|>50, 15% for 130TE3cG I|g=20-50 and 25% for I|g<20 130TE cL J$ From {+130}Te Adopted Levels in ENSDF database 130TE CL BAND(A)$ GS band 130TE PN 5 130TE L 0 0+ A 130TE L 840 2+ A 130TE G 840 100 GT 130TE L 1634 4+ A 130TE G 794 100 5 130TE L 1816 (6)+ A 130TE G 182 46 7 130TE L 2147 (7)- 130TE G 331 23 3 130TE L 2651 (8+) A 130TE G 835 130TE 238U(12C,FG):XUNDL-5 2014AS01 201402 130TE c Includes {+208}Pb({+18}O,F|g) 130TE c Compiled (unevaluated) dataset from 2014As01: 130TE2c Eur Phys J A 50, 2 (2014) 130TE c Compiled by M. Walters and B. Singh (McMaster), Jan 31, 2014 130TE c E({+12}C)=90 MeV, E({+18}O=85 MeV. Targets=47 mg/cm{+2} 130TE2c {+238}U and 100 mg/cm{+2} {+208}Pb. Measured E|g, I|g, |g|g-coin, 130TE3c level half-lives by delayed coincidence techniques using SAPhIR and 130TE4c Euroball arrays at Legnaro XTU accelerator for {+12}C beam and 130TE5c IReS Vivitron facility in Strasbourg. Deduced levels, J, |p. 130TE6c Comparison with shell-model calculations 130TE cG $R=angular correlation yield at different angles 130TE cG M$From |g|g(|q) data, mult=Q corresponds to |DJ=2, most likely E2. 130TE cG M(Y)$Mult=Q from |g|g(|q), RUL for E2 and M2 supports only E2 130TE cL E$From least-squares fit (by compilers) to E|g data 130TE cL J$As proposed in 2014As01; J|p assignments for low-lying levels are 130TE2cL from literature 130TE cL T(X)$From Adopted Levels of {+130}Te in ENSDF database 130TE CL BAND(A)$ |g cascade, yrast structure 130TE CL BAND(B)$ |g cascade based on 7- isomer 130TE CL BAND(C)$ |g cascade based on 10+ isomer 130TE PN 5 130TE L 0.0 0+ A 130TE L 839.2 3 2+ 2.30 PS 5 A 130TEF L FLAG=X 130TE G 839.2 3 100 E2 Y 130TE L 1632.4 5 4+ A 130TE G 793.2 3 74 15 Q 130TE L 1814.2 6 6+ 9.8 NS 5 A 130TEF L FLAG=X 130TE G 181.8 3 60 12 E2 0.208 Y 130TE cG $(181.8|g)(793.2|g)(|q): R(22|')=1.10 {I7}, R(46|')=1.05 {I5}, 130TE2cG R(75|')=1.00 130TE cG $(181.8|g)[793.2|g](839.2|g)(|q): R(22|')=1.09 {I7}, R(46|')=1.04 {I5}, 130TE2cG R(75|')=1.00 130TE L 2100.3 6 5- 130TE G 467.9 4 12 3 130TE L 2145.0 6 7- 110 NS 5 B 130TE cL T$from (458|g+935|g)(331|g+793|g)(t) (2014As01) 130TE G 330.7 3 43 11 D 130TE cG $(330.7|g)(181.2|g)(|q): R(22|')=0.89 {I8}, R(46|')=0.96 {I4}, 130TE2cG R(75|')=1.00 130TE cG $(330.7|g)[181.2|g][793.2|g](839.2)(|q): R(22|')=0.89 {I7}, 130TE2cG R(46|')=0.96 {I4}, R(75|')=1.00 130TE L 2646.8 6 8+ A 130TE G 501.5 5 4.5 10 130TE G 832.7 3 25 5 130TE L 2664.7 9 10+ 1.90 US 8 C 130TEF L FLAG=X 130TE G 17.9 S 130TE cG E$from level-energy difference; transition not observed due to its 130TE2cG low energy and consequential high internal conversion, 130TE3cG but expected from |g|g-coincidence observations 130TE L 2876.7 8 130TE G 731.7 5 9 3 130TE L 3079.5 7 9- B 130TE G 934.5 4 24 6 Q 130TE cG $(934.5|g)[330.7|g][181.2|g][793.2|g](839.2)(|q): R(22|')=1.11 {I8}, 130TE2cG R(46|')=1.04 {I4}, R(75|')=1.00 130TE cG $(934.5|g)(330.7|g)(|q): R(22|')=0.88 {I7}, R(46|')=0.96 {I5}, 130TE2cG R(75|')=1.00 130TE L 3382.4 9 (12+) C 130TE G 717.7 4 19 4 130TE L 3531.1 10 130TE G 654.4 5 8 3 130TE L 3537.5 8 11- B 130TE G 458.0 4 18 4 Q 130TE cG $(458.0|g)[934.5|g](330.7|g)(|q): R(22|')=0.85 {I9}, 130TE2cG R(46|')=0.90 {I7}, R(75|')=1.00 130TE G 872.9 5 6 2 130TE L 3948.8 9 (11-) 130TE G 411.4 5 3 1 130TE G 869.3 6 2 1 130TE L 4174.9 11 (13+) C 130TE G 792.5 5 8 3 130TE L 4247.7 9 (13-) B 130TE G 299.0 5 3 1 130TE G 710.1 4 13 4 130TE G 865.2 5 7 3 130TE L 4281.4 14 (14+) 130TE G 899 1 2 1 ? 130TE L 4373.9 9 (15-) 53 NS 8 B 130TE cL T$from (710|g+458|g+935|g)(t) (2014As01) 130TE G 126.2 3 14 4 E2 0.747 130TEB G BE2W=4.9 7 130TE cG M$from |a(exp)=0.7 {I2} (2014As01) 130TE L 4535.0 12 (14+) C 130TE G 360.1 5 4 2 130TE L 5450.0 10 (16-) B 130TE G 1076.0 5 6 2 130TE L 5702.9 10 (17-) B 130TE G 252.8 5 4 2 130TE G 1329.1 6 2.5 12 130TE COULOMB EXCITATION:XUNDL-6 2013ST24 201501 130TE c Compiled (unevaluated) dataset from 2013St24: 130TE2c Phys Rev C 88, 051304(R) (2013). 130TE c Compiled by B. Singh (McMaster), Jan 6, 2015 130TE c Beam={+130}Te. Target=carbon 130TE c E({+130}Te)=342.8, 390 MeV beams were produced from the 130TE2c Holifield Radioactive Ion Beam Facility at ORNL and were Coulomb 130TE3c excited on a |?1 mg/cm{+2} natural carbon target. Recoiling 130TE4c target nuclei were detected in three rings of the "bare" HyBall array 130TE5c and |g rays were detected in three rings of the CLARION array 130TE6c configured with Compton-suppressed Clover detectors. Measured E|g, I|g, 130TE7c (particle)|g(|q), |g(t). Deduced B(E2) and level lifetime of 130TE8c the first 2+ state. 130TE L 0 0+ 130TE L 839 2+ 2.34 PS 8 130TE2 L BE2=0.291 10 (2013St24) 130TE cL $B(E2) is listed by 2013St24 as an average of two measurements: 130TE2cL 0.280 {I12} at 343 MeV and 0.292 {I10} at 390 MeV. But the compiler 130TE3cL obtains a weighted average of 0.287 {I8} and unweighted average of 130TE4cL 0.286 {I6} 130TE cL T$deduced by 2013St24 from B(E2) value 130TE G 839 E2 130TE 130TE 2B- HALF-LIFE:XUNDL-8 2018AL13 201905 130TE c Compiled (unevaluated) dataset from 2018Al13: 130TE2c Phys Rev Lett 120, 132501 (2018). 130TE c See also 2015Al20: Phys Rev Lett 115, 102502 (2015); and 2016Al11: 130TE2c Phys Rev C 93, 045503 (2016) for a description of CUORE-0 system. 130TE c Compiled by B. Singh (McMaster), Dec 29, 2018 130TE c 2018Al13: measurement of half-life limit for the 0|n|b|b decay mode of 130TE2c {+130}Te using CUORE (Cryogenic Underground Observatory for Rare 130TE3c Events, a prototype version was CUORE-0) bolometric detector apparatus 130TE4c located at the underground Gran Sasso laboratory of INFN-Italy. 130TE5c The CUORE apparatus consists of 988 5|*5|*5 cm{+3} TeO2 crystals, 130TE6c cooled to 7 mK, and each crystal is equipped with a thermistor to 130TE7c record thermal pulses, when a crystal absorbs energy. The crystals are 130TE8c arranged into 19 copper-framed towers, each tower consisting of 13 130TE9c floors with four crystals on each floor, and the towers thermally 130TEAc connected to a {+3}He-{+4}He dilution refrigerator. External |g-ray 130TEBc background was suppressed by two shields of ancient Roman lead. 130TECc Measured energy spectrum and reconstructed corresponding |g-ray 130TEDc spectrum. A background level of 0.014 {I2} counts/(keV kg yr) was 130TEEc achieved. Deduced lower limit of T{-1/2} and corresponding upper 130TEFc limit of the Majorana neutrino mass. 130TE c No events were observed for 0|n|b|b decay mode, close to the Q{-|b|b} 130TE2c window of 2527.51 keV {I1} (2017Wa10: AME-2016) corresponding to 130TE3c {+130}Te g.s. {+130}Xe g.s. |b|b transition, thus providing no 130TE4c evidence for 0|n|b|b decay of {+130}Te. 130TE L 0 0+ 1.3E+25 Y GT 130TE cL T$this value is for 0|n|b|b decay mode at 90% confidence level (C.L.), 130TE2cL and was derived from a Bayesian analysis (2018Al13). Authors' 130TE3cL frequentist analysis gave T{-1/2}>2.1|*10{+25} y at 90% C.L. and a 130TE4cL sensitivity of >0.76|*10{+25} y at 90% C.L. Combining the earlier 130TE5cL results of >2.7|*10{+24} y (CUORE-0 value from 2015Al20: 130TE6cL Phys. Rev. Lett. 115, 102502; and >2.8|*10{+24} y (CUORICINO value 130TE7cL from 2011An08: Astropart. Phys. 34, 822), authors obtain 130TE8cL T{-1/2}>1.5|*10{+25} y at 90% C.L. using profile likelihood or 130TE9cL Bayesian approach, and >2.2|*10{+25} y using frequentist technique. 130TE cL $Corresponding upper limit of Majorana neutrino mass 130TE2cL m{-|b|b}<0.11-0.52 eV (2018Al13) 130TE 130TE(N,N'G):XUNDL-9 2022HI01 202203 130TE c Compiled (unevaluated) dataset from 2022Hi01: 130TE2c Phys Rev C 105, 024329 (2022). 130TE c Compiled by B. Singh (McMaster); March 01, 2022. 130TE c 2022Hi01: E(n)=1.86-3.34 MeV neutron beam in 90 keV steps was 130TE2c provided by the 7 MV |eN Van de Graaff accelerator and the neutron 130TE3c production facility at the University of Kentucky Accelerator 130TE4c Laboratory (UKAL). Target was 48.6641 g {I5} g metallic sample, 130TE5c enriched to 99.47% {I1} in {+130}Te. Measured E|g, I|g, |g(|q), 130TE6c level lifetimes by Doppler-shift attenuation method (DSAM) from 130TE7c |g(|q) distributions using a single BGO Compton-suppressed n-type HPGe 130TE8c detector with 53% relative efficiency. For |g|g-coin measurements, 130TE9c natural Te sample was used and data were taken at E(n)=3.5 MeV, with 130TEAc the |g rays detected by four high-efficiency HPGe detectors. 130TEBc Theoretical cross sections were calculated using the statistical model 130TECc code CINDY with appropriate optical model parameters. Comparison with 130TEDc large-scale shell-model calculations using NuShellX@MSU code with two 130TEEc different effective interactions. Calculated Wave function composition 130TEFc and g factors for six 2+ states. Kumar-Cline sum rules were used to 130TEGc investigate rotational invariants for the 0+ g.s. and the first 2+, 4+ 130TEHc and 6+ states. See also a previous (n,n'|g) work by 2008Hi17 130TEIc (Phys. Rev. C 78, 054320) from the same laboratory, where results of 130TEJc level lifetime and gamma-transition measurements for the 1588-, 1886-, 130TEKc 2190-, 2282- and 2300-keV levels were reported. 2008Hi17 is considered 130TELc by compiler as superseded by authors' present detailed work in 2022Hi01 130TE cG $B(M1) values are in |m{-N}{+2} units in 2022Hi01 130TE cG $Transition probabilities are for the first spin listed when the spin 130TE2cG of the initial state is not definite, and multiple choices of spins 130TE3cG are given 130TE cG E,RI,M,MR$From 2022Hi01. When two values of mixing ratio |d are 130TE2cG given, first value listed in Table I of 2022Hi01 corresponds to a lower 130TE3cG value in |h{+2} fit. Second value here is listed in comments. 130TE4cG In addition, multipole-mixing ratios are for the first spin listed when 130TE5cG multiple choices of spins are given 130TE cG E(n)$New |g transition (2022Hi01) 130TE cG E(g)$Placement from |g|g-coin data (2022Hi01) 130TE cG E(d)$Doublet (2022Hi01) 130TE cG E(x)$2022Hi01 indicate probable missing strength from this level, 130TE2cG either possible unassigned decay path or the level itself is not well 130TE3cG described by statistical model calculations. 130TE cG RI(f)$Branching ratio from excitation function data (2022Hi01) 130TE cG RI(a)$|g branching ratio taken by 2022Hi01 from {+130}Te Adopted 130TE2cG Gammas in the ENSDF database (May 2001 update) 130TE cG RI(r)$|g branching ratio taken by 2022Hi01 from 1974Ke08 130TE cL $SMC=statistical model calculations 130TE cL E$Deduced by compiler from least-squares fit to E|g data, keeping 130TE2cL the energy of the first excited state as fixed. 130TE3cL Two |g rays were found to have somewhat poor fit: 1300.15 {I12} 130TE4cL from 2887.9 level, and 1414.14 {I10} from 3046.6 level. Increasing 130TE5cL the uncertainty to 0.2 keV for each of these |g rays gives a good 130TE6cL fit, with reduced |h{+2}=1.66 as compared to critical |h{+2}=1.34, 130TE7cL and with 12 |g rays out of a total of 169 |g rays deviating in energy 130TE8cL between 2 to 3 |s. Level energies given here are very close to the 130TE9cL values in Table I of 2022Hi01 130TE cL E(N)$New level proposed by 2022Hi01 130TE cL E(X)$2022Hi01 note that SMC calculations show missing |g-transition 130TE2cL strength indicated by listed branching ratios, while consistent, do 130TE3cL not agree with calculations for preferred spin from |g(|q) data. 130TE4cL Either there is another (presently missing) |g branch or the level is 130TE5cL not well described by SMC. 130TE cL J$As given in 2022Hi01, some from literature, others from |g(|q) data 130TE2cL and other arguments in the present work. 130TE cL T$From 2022Hi01, Doppler-shift attenuation method (DSAM) extracted from 130TE2cL |g(|q) distributions which were measured at E(n) closer to the level 130TE3cL threshold. Exceptions are noted. 130TE PN 7 130TE L 0.0 0+ 130TE L 839.49 5 2+ 2.30 PS 5 130TE cL E$level energy held fixed in least-squares adjustment 130TE cL T$2022Hi01 take value from {+130}Te Adopted Levels in the ENSDF 130TE2cL database (May 2001 update) 130TE G 839.49 5 100 E2 130TE2 G A2=+0.15 1 $ A4=-0.13 1 130TE cG $|g(|q) at E(n)=2.2 MeV. Note that authors give uncertainty of 0.00 130TE2cG for A{-2} and A{-4} 130TEB G BE2W=15.1 3 130TE cG $B(E2)(W.u.) taken by 2022Hi01 from {+130}Te Adopted Gammas in the 130TE2cG ENSDF database (May 2001 update). Also B(E2)(W.u.)=14.9 {I5} (2013St24) 130TE L 1588.206 21 2+ 908 FS GT 130TE cL T$measured mean lifetime |t>1310 fs (2022Hi01) 130TE G 748.73 6 98.12 3 M1+E2 +0.63 +27-33 130TE2 G A2=+0.33 1 $ A4=-0.06 1 130TE cG $|g(|q) at E(n)=2.2 MeV 130TEB G BM1<0.040 $ BE2W<19 (2022Hi01) 130TE G 1588.14 6 1.88 3 E2 130TE2 G A2=+0.22 7 $ A4=-0.15 10 130TE cG $|g(|q) at E(n)=2.2 MeV 130TEB G BE2W<0.030 (2022Hi01) 130TE L 1633.01 6 4+ 3.3 PS 7 130TE cL T$deduced by evaluators from preliminary B(E2)(W.u.)=14 {I3} 130TE2cL in 2020CoZY 130TE G 793.48 6 100 E2 130TE2 G A2=+0.34 1 $ A4=-0.05 1 130TE cG $|g(|q) at E(n)=2.2 MeV. Note that authors give uncertainty of 0.00 130TE2cG for A{-2} 130TEB G BE2W=14 3 130TE cG $B(E2)(W.u.) taken by 2022Hi01 from 2020CoZY, while noting that 130TE2cG B(E2)(W.u.)=18 {I4} (2020CoZY) is also possible depending on the sign 130TE3cG of E2 matrix element in shell-model calculations 130TE L 1815.58 8 6+ 9.8 NS 5 130TE cL T$2022Hi01 take value from {+130}Te Adopted Levels in the ENSDF 130TE2cL database (May 2001 update) 130TE G 182.39 20 100 E2 0.206 130TE2 G A2=+0.37 25 $ A4=+0.34 39 130TE cG $|g(|q) at E(n)=2.2 MeV 130TEB G BE2W=6.1 3 130TE cG $B(E2)(W.u.) taken by 2022Hi01 from {+130}Te Adopted Gammas in the 130TE2cG ENSDF database (May 2001 update) 130TE L 1885.684 22 2+ 298 FS 28 130TE cL T$measured mean lifetime |t=430 fs {I40} (2022Hi01) 130TE G 1046.15 5 98.47 4 M1+E2 +3.9 +10-5 130TE2 G A2=+0.06 1 $ A4=-0.05 1 130TE cG $|g(|q) at E(n)=2.2 MeV 130TE cG $Branching ratios from 2008Hi17 in (n,n'|g) 130TE cG MR$other: -0.19 {I+11-4} (2022Hi01) 130TE cG $B(M1)=0.0070 {I+20-28}, B(E2)(W.u.)=36 {I+17-9} for 130TE2cG |d=+3.90 {I+10-5}; B(M1)=0.11 {I2}, B(E2)(W.u.)=1.3 {I2} for 130TE2cG |d=-0.19 {I+11-4} (2022Hi01) 130TE G 1885.70 9 1.53 4 E2 130TE2 G A2=+0.19 15 $ A4=-0.19 22 130TE cG $|g(|q) at E(n)=2.2 MeV 130TEB G BE2W=0.031 +5-4 (2022Hi01) 130TE L 1964.70 7 0+ 1.8 PS +17-6 130TE cL T$measured mean lifetime |t=2600 fs {I+2400-900} (2022Hi01); 130TE2cL Doppler shift from 1125.2|g(|q) distribution for E(n)=3.3 MeV 130TE G 1125.20 5 100 E2 1.12E-3 130TE2 G A2=-0.01 2 $ A4=-0.02 3 130TE cG $|g(|q) at E(n)=2.2 MeV 130TEB G BE2W=4.4 22 (2022Hi01) 130TE L 1981.43 7 4+ 1.9 PS +10-6 130TE cL T$measured mean lifetime |t=2800 fs {I+1500-800} (2022Hi01) 130TE G 348.5 2 53.4 3 M1+E2 +0.22 +48-17 d 130TE2 G A2=+0.38 3 $ A4=+0.04 4 130TE cG $|g(|q) at E(n)=2.2 MeV 130TEB G BM1=0.24 11 $ BE2W=35 +20-14 (2022Hi01) 130TE G 1141.93 5 46.6 3 E2 130TE2 G A2=+0.50 3 $ A4=-0.11 4 130TE cG $|g(|q) at E(n)=2.2 MeV 130TEB G BE2W=1.8 7 (2022Hi01) 130TE L 2101.16 9 5- 130TE G 468.3 2 100 E1 0.00310 130TE2 G A2=-0.23 4 $ A4=+0.09 5 130TE cG $|g(|q) at E(n)=2.2 MeV 130TE L 2138.54 6 3+ 3.1 PS +38-11 130TE cL T$measured mean lifetime |t=4400 fs {I+5500-1600} (2022Hi01) 130TE G 505.62 6 18 1 M1+E2 +1.1 8 130TE2 G A2=-0.60 12 $ A4=+0.19 17 130TE cG $|g(|q) at E(n)=2.2 MeV 130TEB G BM1=0.0080 +110-63 $ BE2W=15 +21-12 (2022Hi01) 130TE G 550.30 6 41 1 M1+E2 +1.3 6 130TE2 G A2=+0.80 4 $ A4=+0.36 9 130TE cG $|g(|q) at E(n)=2.2 MeV 130TEB G BM1=0.012 +15-9 $ BE2W=24 +28-18 (2022Hi01) 130TE G 1299.07 5 41 1 M1+E2 +0.51 +21-17 130TE2 G A2=+0.22 5 $ A4=-0.14 8 130TE cG $|g(|q) at E(n)=2.2 MeV 130TEB G BM1=0.0019 +15-12 $ BE2W=0.11 +9-7 (2022Hi01) 130TE L 2146.21 17 7- 115 NS 8 M 130TE2 L %IT=100 130TE cL T$2022Hi01 take value from {+130}Te Adopted Levels in the ENSDF 130TE2cL database (May 2001 update) 130TE cL J$|g(|q) data in 2022Hi01 consistent with J=7 or 5, the former 130TE2cL assignment is supported in authors' excitation function data and 130TE3cL comparison with SMC 130TE G 330.67 21 100 E1 d 130TE2 G A2=-0.34 3 $ A4=+0.04 4 130TEB G BE1W=6.4E-8 5 (2022Hi01) 130TE cG $|g(|q) data in 2022Hi01 give pure dipole with no mixing for J=7 for 130TE2cG 2146 level. 130TE L 2190.50 4 2+ 409 FS 28 130TE cL T$measured mean lifetime |t=590 fs {I40} (2022Hi01) 130TE G 1351.01 5 40 1 M1+E2 -2.0 +28-17 130TE2 G A2=+0.21 17 $ A4=-0.12 25 130TE cG $|g(|q) at E(n)=2.2 MeV 130TE2 G A2=+0.03 1 $ A4=-0.01 1 130TE cG $|g(|q) at E(n)=3.3 MeV 130TE cG $Second solution from |g(|q): |d(E2/M1)=-0.26 {I7} (2022Hi01) 130TEB G BM1W=0.0032 +58-31$ BE2W=2.5 +28-25 (2022Hi01) 130TE G 2190.45 10 60 1 E2 130TE2 G A2=+0.70 15 $ A4=+0.10 22 130TE cG $|g(|q) at E(n)=2.2 MeV 130TE2 G A2=+0.16 2 $ A4=-0.15 2 130TE cG $|g(|q) at E(n)=3.3 MeV 130TEB G BE2W=0.42 4 (2022Hi01) 130TE L 2282.52 5 2+ 83 FS 7 130TE cL T$measured mean lifetime |t=120 fs {I10} (2022Hi01) 130TE cL $|g branching ratio from excitation function data (2022Hi01) 130TE G 1443.02 5 84 1 M1+E2 +3.9 15 130TE2 G A2=+0.03 1 $ A4=-0.11 1 130TE cG MR$other: -0.16 {I11} (2022Hi01) 130TE cG $B(M1)=0.0084 {I+45-43}, B(E2)(W.u.)=23 {I+13-12} for 130TE2cG |d=+3.9 {I15}; B(M1)=0.13 {I7}, B(E2)(W.u.)=0.60 {I4} for 130TE3cG |d=-0.16 {I11} (2022Hi01) 130TE G 2282.51 10 16 1 E2 7.20E-4 130TE2 G A2=+0.19 3 $ A4=-0.18 4 130TEB G BE2W=0.46 +5-4 (2022Hi01) 130TE L 2300.10 5 (1+,2+) 464 FS +56-49 130TE cL T$measured mean lifetime |t=670 fs {I+80-70} (2022Hi01) 130TE cL J$|g(|q) data in 2022Hi01 consistent with J=1 or 2, the former 130TE2cL assignment is supported in authors' excitation function data and 130TE3cL comparison with SMC, but 2+ is not ruled out completely 130TE G 1460.62 5 96 1 M1+E2 -0.78 +85-76 130TE2 G A2=+0.02 1 $ A4=-0.01 2 130TE cG MR$-0.78 {I+85-76} for J|p(2300 level)=1+ (2022Hi01) 130TEB G BM1=0.016 +12-9 $ BE2W=1.7 +12-17 (2022Hi01) 130TE cG $B(M1) and B(E2)(W.u.) for J|p(2300 level)=1+ 130TE G 2300.16 12 4 1 M1 130TE2 G A2=-0.05 13 $ A4=-0.15 18 130TEB G BM1=0.00028 +11-9 (2022Hi01) 130TE cG $B(M1) for J|p(2300 level)=1+ 130TE L 2330.68 7 4+ 0.60 PS +14-10 130TE cL T$measured mean lifetime |t=860 fs {I+200-140} (2022Hi01) 130TE cL J$|g(|q) in (n,n'|g) rules out J=3 130TE cL $|g branching ratios deduced by 2022Hi01, using SMC iteratively 130TE2cL to obtain a consistency with |g(|q) and excitation functions data 130TE3cL and comparison with SMC for the 2330.7, 4+ level, since the 349.35|g 130TE4cL could not be resolved from the strong 348.5|g from 1981.4 keV level. 130TE G 349.35 22 13 2 (M1+E2) 0.0234 5 n 130TE2 G A2=+0.24 1 $ A4=-0.04 1 130TE cG RI$see comment for 2330.66 level for branching ratio 130TEF G FLAG=dg 130TE cG MR$<1.1 from RUL(E2)=300. 130TEB G BM1 LE 0.24 $ BE2W LE 820 (2022Hi01) 130TE cG $Note: RUL=300 for B(E2)(W.u.) 130TE G 697.68 5 70 5 M1(+E2) -0.03 +9-3 130TE2 G A2=+0.28 1 $ A4=+0.01 2 130TE cG $Other: |d(E2/M1)=+1.0 {I2} (2022Hi01) 130TE2 G BM1=0.13 4 $ BE2W=0.092 +26-92 (2022Hi01) 130TE G 1491.17 6 17 3 E2 130TE2 G A2=+0.34 3 $ A4=-0.03 5 130TEB G BE2W=0.56 +23-19 (2022Hi01) 130TE L 2405.02 15 6- X 130TE cL J$303.9|g(|q) allows J=3,4,6,(5); 258.8|g(|q) allows J=5,6. 130TE2cL Excitation function data compared with SMC strongly supports 6 130TE G 258.83 20 49 1 M1+E2 +5.2 +17-9 0.056 7 130TE2 G A2=-0.47 4 $ A4=+0.10 5 130TE cG MR$other: +0.25 {I+7-5} (2022Hi01) 130TE G 303.87 20 51 1 M1(+E2) +0.03 3 0.0330 130TE2 G A2=-0.16 2 $ A4=+0.04 4 130TE L 2432.41 24 (6+,7-) 130TE cL J$286.2|g(|q) supports J=5,6 and 331.1|g(|q) supports J=3,4,6; with 130TE2cL no multipole mixing for J=6 in both cases. Excitation functions data 130TE3cL compared with SMC give spin above 6 or 7. Systematics of even-A Te 130TE4cL isotopes support second 6+ near this energy. However, J=7 cannot be 130TE5cL ruled out 130TE G 286.23 20 26 3 a 130TE2 G A2=-0.12 3 $ A4=-0.01 4 130TE G 331.1 5 74 3 a 130TE2 G A2=-0.34 3 $ A4=+0.04 4 130TEF G FLAG=d 130TE L 2435.82 19 4- 130TE G 334.69 20 100 M1(+E2) -0.06 +6-3 0.0258 130TE2 G A2=-0.06 1 $ A4=-0.01 2 130TE L 2449.43 8 4+ 263 FS +35-28 130TE cL T$measured mean lifetime |t=380 fs {I+50-40} (2022Hi01) 130TE cL $An 861.6|g reported earlier in |b{+-} decay was weakly observed in 130TE2cL the present work but with a threshold of E(n)>2.6 MeV 130TE cL J$816.4|g(|q) consistent with 4+; excitation function of the 130TE2cL 816.4|g consistent with 4+ from SMC for an 80% branch 130TE G 467.90 23 20 4 [M1+E2] 0.0105 7 n 130TE2 G A2=-0.24 1 $ A4=-0.03 1 130TE cG $Note that authors give uncertainty of 0.00 for A{-2} 130TEF G FLAG=dg 130TE cG RI$467.9-keV is unresolved from the much stronger 468.3|g from the 130TE2cG 2101, 5- level 130TEB G BM1 LE 0.39 $ BE2W LE 650 (2022Hi01) 130TE G 816.42 5 80 4 M1+E2 -0.22 +10-8 130TE2 G A2=+0.18 2 $ A4=-0.01 2 130TE cG $Other |d(E2/M1)=+1.5 {I+3-2} (2022Hi01) 130TEB G BM1=0.21 4 $ BE2W=5.6 +10-9 (2022Hi01) 130TE L 2466.87 4 2+ 568 FS +90-69 X 130TE cL T$measured mean lifetime |t=820 fs {I+130-100} (2022Hi01) 130TE cL J$2+ supported by |g(|q) for all the transitions which are also seen 130TE2cL in appropriate |g|g-coin gates. 130TE G X x ? 130TE G 581.10 7 4.6 3 M1(+E2) -0.32 +45-56 n 130TE2 G A2=+0.10 18 $ A4=+0.20 25 130TE cG $Other |d(E2/M1)=+5.2 {I+540-98} (2022Hi01) 130TEB G BM1=0.015 +5-6 $ BE2W=1.6 +8-16 (2022Hi01) 130TE G 878.73 8 4.3 3 M1(+E2) -0.26 +33-37 n 130TE2 G A2=-0.10 15 $ A4=-0.28 22 130TE cG $Also, |d(E2/M1)=+5.2 {I+110-78} (2022Hi01) 130TEB G BM1=0.0041 +12-11 $ BE2W=0.13 +5-13 (2022Hi01) 130TE G 1627.37 5 80.1 4 M1+E2 -16 +25-28 130TE2 G A2=-0.07 2 $ A4=-0.02 2 130TE cG MR$other: -0.51 {I12} (2022Hi01) 130TE cG $B(M1)=0.000047 {I+120-47}, B(E2)(W.u.)=1.8 {I+50-18} for 130TE2cG |d=-16 {I+25-28}; B(M1)=0.010 {I3}, B(E2)(W.u.)=0.37 {I8} for 130TE3cG |d=-0.51 {I12} (2022Hi01) 130TE G 2466.91 11 11.0 2 E2 130TE2 G A2=+0.36 6 $ A4=-0.02 9 130TEB G BE2W=0.031 5 (2022Hi01) 130TE L 2476.02 7 0+ 1.2 PS +18-5 N 130TE cL T$measured mean lifetime |t=1800 fs {I+2600-700} (2022Hi01) 130TE cL J$from shell-model predictions (Fig. 13 in 2022Hi01) 130TE G 590.36 6 20.1 10E2 n 130TE2 G A2=+0.16 15 $ A4=+0.03 21 130TEB G BE2W=33 +24-21 (2022Hi01) 130TE G 887.81 6 28.8 6 E2 n 130TE2 G A2=+0.09 6 $ A4=+0.09 8 130TEB G BE2W=6.2 +42-38 (2022Hi01) 130TE G 1636.49 6 51.1 7 E2 n 130TE2 G A2=-0.02 4 $ A4=-0.10 5 130TEB G BE2W=0.52 +34-32 (2022Hi01) 130TE L 2527.12 6 3- 130TE G 425.86 22 0.8 3 n 130TE2 G A2=+0.56 27 $ A4=+0.45 38 130TE G 641.44 6 8.7 20 n 130TE2 G A2=-0.18 6 $ A4=-0.03 8 130TE G 894.10 6 3.1 5 130TE2 G A2=+0.60 34 $ A4=+0.38 30 130TE G 939.1 5 0.9 3 n 130TE2 G A2=-0.24 10 $ A4=-0.05 14 130TE G 1687.63 5 86.5 20 130TE2 G A2=-0.22 1 $ A4=-0.06 2 130TE L 2537.64 23 (7-,6) N 130TE G 436.48 21 100 n 130TE2 G A2=+0.15 14 $ A4=+0.07 19 130TE L 2575.03 7 3+ 0.51 PS +13-9 130TE cL T$measured mean lifetime |t=740 fs {I+180-130} (2022Hi01) 130TE cL J$|g(|q) forbid 4+, and J=5 and 6 less likely as large angular 130TE2cL momentum transfer not supported in the present work. 130TE G 942.01 5 68.0 3 M1(+E2) +0.03 +10-6 130TE2 G A2=-0.14 2 $ A4=-0.08 3 130TE cG $Negative A{-2} in |g(|q) forbids 4+ for 2575 level 130TEB G BM1=0.062 +14-13 $ BE2W=0.023 +5-23 (2022Hi01) 130TE G 986.74 6 24.1 3 M1+E2 -16 +17-9 n 130TE2 G A2=0.00 4 $ A4=+0.07 5 130TE cG MR$other: +0.13 {I+10-4} (2022Hi01) 130TE cG $B(M1)=0.00007 {I+15-6}, B(E2)(W.u.)=7.2 {I+84-72} for 130TE2cG |d=-16 {I+17-9}; B(M1)=0.019 {I+5-4}, B(E2)(W.u.)=0.12 {I3} for 130TE3cG |d=+0.13 {I+10-4} (2022Hi01) 130TE G 1735.67 7 7.9 3 M1+E2 -0.19 +11-13 130TE2 G A2=-0.33 11 $ A4=+0.02 15 130TE cG $Negative A{-2} in |g(|q) forbids 4+ for 2575 level 130TE cG MR$other: -2.5 {I+12-7} (2022Hi01) 130TE cG $B(M1)=0.0011 {I3}, B(E2)(W.u.)=0.0049 {I+13-12} for |d=-0.19 {+11-13} 130TE2cG B(M1)=0.00016 {I+10-11}, B(E2)(W.u.)=0.12 {I+12-6} for |d=-2.5 {+12-7} 130TE3cG (2022Hi01) 130TE L 2581.01 4 2+ 208 FS 14 130TE cL T$measured mean lifetime |t=300 fs {I20} (2022Hi01) 130TE cL J$993|g(|q) and 1742|g(|q) allow J=2,3,4; excitation 130TE2cL function data are above the SMC, but closest to J=2. 130TE G 992.77 6 10.2 3 M1+E2 +1.7 +8-14 130TE2 G A2=+0.18 7 $ A4=-0.03 10 130TE cG MR$other: +0.16 {I+35-20} (2022Hi01) 130TE cG $B(M1)=0.0051 {I+51-27}, B(E2)(W.u.)=5.5 {I+32-48} for 130TE2cG |d=+1.7 {I+8-14}; B(M1)=0.019 {I3}, B(E2)(W.u.)=0.19 {I+3-19} for 130TE2cG |d=+0.16 {I+35-20} (2022Hi01) 130TE G 1741.53 5 89.8 3 M1+E2 +0.68 +24-28 130TE2 G A2=+0.30 2 $ A4=-0.06 2 130TEB G BM1=0.022 +6-5 $ BE2W=1.3 3 (2022Hi01) 130TE L 2604.52 6 (0+) 0.35 PS +13-8 N 130TEF L FLAG=X 130TE cL T$measured mean lifetime |t=500 fs {I+190-110} (2022Hi01) 130TE cL J$from shell-model prediction (Fig. 13 in 2022Hi01) 130TE G X x ? 130TE G 1016.3 8 8 6 E2 n 130TE2 G A2=-0.21 4 $ A4=-0.08 5 130TEF G FLAG=gf 130TEB G BE2W=3.1 +39-26 (2022Hi01) 130TE G 1765.02 6 92 6 E2 n 130TE2 G A2=-0.01 4 $ A4=0.00 5 130TEF G FLAG=f 130TEB G BE2W=2.3 +9-8 (2022Hi01) 130TE L 2607.23 6 1(+) 69 FS 7 130TE cL T$measured mean lifetime |t=100 fs {I10} (2022Hi01) 130TE cL J$positive parity is preferred from comparison of excitation function 130TE2cL data to SMC, and from systematics of stable Te isotopes 130TE G 1019.2 5 6 5 [M1,E2] n 130TE2 G A2=-0.21 4 $ A4=-0.08 5 130TEF G FLAG=f 130TEB G BM1 LE 0.061 $ BE2W LE 22 (2022Hi01) 130TE G 1767.77 6 31 6 [M1,E2] 130TE2 G A2=-0.04 5 $ A4=-0.10 7 130TEF G FLAG=f 130TEB G BM1 LE 0.040 $ BE2W LE 4.7 (2022Hi01) 130TE G 2607.05 11 63 4 M1 130TE2 G A2=-0.11 2 $ A4=-0.06 4 130TEF G FLAG=f 130TEB G BM1=0.020 3 (2022Hi01) 130TE L 2636.60 10 (5-,4-) 832 FS GE N 130TE cL T$measured mean lifetime |t|>1200 fs (2022Hi01) 130TE G 535.45 5 100 (M1+E2) +0.68 +18-9 130TE2 G A2=+0.36 2 $ A4=-0.04 3 130TE L 2688.64 5 1+ 33.3 FS 21 130TE cL T$measured mean lifetime |t=48 fs {I3} (2022Hi01) 130TE G 802.84 8 5.1 3 M1+E2 +1.0 64 n 130TE2 G A2=-0.33 26 $ A4=-0.45 35 130TEF G FL=1885.684 130TEB G BM1=0.053 +8-7 $ BE2W=36 +5-36 (2022Hi01) 130TE G 1101.07 25 23.5 2 [M1,E2] n 130TE2 G A2=+0.25 2 $ A4=-0.11 3 130TEF G FLAG=dg 130TEB G BM1 LE 0.23 $ BE2W LE 68 (2022Hi01) 130TE G 1849.17 7 6.8 2 M1+E2 +1.1 +35-31 130TE2 G A2=-0.28 11 $ A4=-0.30 16 130TE2 G BM1=0.0076 +23-21 $ BE2W=0.56 +18-56 130TE G 2688.61 10 64.6 4 M1 130TE2 G A2=-0.22 3 $ A4=-0.14 4 130TEB G BM1=0.039 3 (2022Hi01) 130TE L 2714.83 10 4- X 130TE cL J$614|g(|q) favors J=4 or 6, with non-zero mixing ratios. 576|g(|q) 130TE2cL consistent with J=2-5, with no mixing for J=4 130TE G X x ? 130TE G 576.23 12 3 2 n 130TE2 G A2=-0.54 21 $ A4=-0.64 30 130TE G 613.71 10 97 2 M1+E2 +1.7 +4-3 130TE2 G A2=-0.58 2 $ A4=+0.03 3 130TE cG MR$other: +0.68 {I+15-9} 130TE L 2733.46 7 4+ 152 FS +42-28 N 130TE cL E$two separate levels of 2733.4, 4+ and 2736.3, 5+ are proposed in the 130TE2cL present work based on excitation functions and |g|g-coin data, in 130TE3cL contrast to only one level 2736, 4+ in {+130}Te Adopted Levels in the 130TE4cL ENSDF database (2001 update) 130TE cL T$measured mean lifetime |t=220 fs {I+60-40} (2022Hi01) 130TE cL J$1145.2|g(|q) and 1894.0|g(|q) suggest J=4; positive parity from 130TE2cL population in |b decay. 130TE G 403.1 6 6 3 M1(+E2) +0.37 +47-40 n 130TE2 G A2=+0.48 15 $ A4=+0.14 21 130TEF G FLAG=f 130TEB G BM1=0.20 +19-13 $ BE2W=63 +58-63 (2022Hi01) 130TE G 1100.43 5 64 4 [M1,E2] n 130TEF G FLAG=fd 130TEB G BM1 LE 0.16 $ BE2W LE 49 (2022Hi01) 130TE G 1145.19 7 13 4 E2 n 130TE2 G A2=+0.40 9 $ A4=-0.29 13 130TEF G FLAG=f 130TEB G BE2W=6.2 +38-29 (2022Hi01) 130TE G 1894.03 6 17 3 E2 n 130TE2 G A2=+0.28 7 $ A4=-0.06 10 130TEF G FLAG=f 130TEB G BE2W=0.65 +30-23 (2022Hi01) 130TE L 2736.43 8 5+ 130TE cL E$two separate levels of 2733.4, 4+ and 2736.3, 5+ are proposed in the 130TE2cL present work based on excitation functions and |g|g-coin data, in 130TE3cL contrast to only one level 2736, 4+ in {+130}Te Adopted Levels in the 130TE4cL ENSDF database (2001 update) 130TE cL J$from 1103.4|g(|q) and excitation function for 920.9|g 1894.0|g(|q) 130TE G 920.89 6 69.3 7 M1+E2 +0.13 +7-8 130TE2 G A2=-0.30 5 $ A4=-0.06 7 130TE G 1103.35 7 30.7 7 M1+E2 +1.7 +18-2 130TE2 G A2=-0.64 9 $ A4=+0.44 10 130TE cG $|d=+1.70 {I+141-42} (2022Hi01) 130TE L 2743.79 8 1+ 104 FS 7 130TE cL T$measured mean lifetime |t=150 fs {I10} (2022Hi01) 130TE cL J$1155.8|g(|q) gives J=1,2,3, while the excitation function and SMC 130TE2cL slightly favor positive parity. 130TE G 1155.8 1 13.8 3 M1+E2 +1.4 24 n 130TE2 G A2=-0.07 6 $ A4=+0.22 9 130TE2 G BM1=0.012 +20-12 $ BE2W=6.0 +100-60 130TE G 2743.49 11 86.2 3 M1 130TE2 G A2=-0.12 2 $ A4=-0.04 2 130TEB G BM1=0.015 1 (2022Hi01) 130TE L 2744.82 6 3- 513 FS +97-76 130TE cL T$measured mean lifetime |t=740 fs {I+140-110} (2022Hi01) 130TE cL J$859.3|g(|q), 1111.7|g(|q) and 1905.3|g(|q) strongly support J=3. 130TE2cL Negative parity is from previous scattering experiments 130TE G 859.26 5 38.2 3 E1 130TE2 G A2=-0.24 2 $ A4=+0.01 3 130TEB G BE1W=3.1E-4 +5-6 (2022Hi01) 130TE G 1111.67 6 12.7 2 E1 130TE2 G A2=-0.14 5 $ A4=+0.02 6 130TEB G BE1W=4.8E-5 +9-8 (2022Hi01) 130TE G 1905.30 3 49.1 3 E1 130TE2 G A2=-0.26 2 $ A4=-0.03 3 130TEB G BE1W=3.7E-5 7 (2022Hi01) 130TE L 2747.99 8 5(-) 118 FS +21-14 N 130TE cL T$measured mean lifetime |t=170 fs {I+30-20} (2022Hi01) 130TE G 932.39 7 13 8 E1 n 130TE2 G A2=-0.10 15 $ A4=+0.06 21 130TEF G FLAG=f 130TEB G BE1W=3.6E-4 +31-24 (2022Hi01) 130TE G 1114.99 6 87 8 E1 n 130TE2 G A2=-0.23 3 $ A4=-0.06 5 130TEB G BE1W=0.0014 +4-3 (2022Hi01) 130TE L 2748.48 11 (5,6)- 0.6 PS +13-2 N 130TE cL T$measured mean lifetime |t=820 fs {I+1930-360} (2022Hi01) 130TE G 343.5 2 22 1 (M1+E2) -1.8 +36-9 n 130TE2 G A2=+0.27 14 $ A4=+0.30 20 130TEF G FLAG=f 130TEB G BM1=0.084 +210-80 $ BE2W LE 1900 (2022Hi01) 130TE cG $Note that RUL(E2)=300 for B(E2)(W.u.)|<2800 130TE cG $|d(E2/M1), B(M1) and B(E2)(W.u.) for J|p(2748 level)=(5)- 130TE G 647.31 7 78 1 (M1+E2) -0.22 +14-8 n 130TE2 G A2=+0.27 5 $ A4=+0.04 6 130TEB G BM1=0.19 +17-14$ BE2W=8.1 +67-58 (2022Hi01) 130TE cG $B(E2)(W.u.)=10.0 in author' Table I seems a misprint 130TE cG $|d(E2/M1), B(M1) and B(E2)(W.u.) for J|p(2748 level)=(5)- 130TE L 2759.36 13 (6,7)- 735 FS GT 130TE cL T$measured mean lifetime |t>1060 fs (2022Hi01) 130TE G 658.2 1 100 n 130TE2 G A2=+0.29 5 $ A4=-0.07 7 130TEF G FLAG=d 130TE L 2766.33 4 3+ 250 FS 28 130TE cL T$measured mean lifetime |t=360 fs {I40} (2022Hi01) 130TE cL J$no pure multipole decays from |g(|q) strongly support J|p=3+ 130TE cL $A previously assigned 949.8|g from this level is not observed 130TE2cL in the present experiment, except possibly with a threshold 130TE3cL above E(n)=3.1 MeV (2022Hi01). 130TE G 880.72 6 36 2 M1+E2 -0.85 +38-33 n 130TE2 G A2=-0.68 7 $ A4=-0.11 9 130TEF G FLAG=f 130TEB G BM1=0.048 +21-16$ BE2W=16 +7-6 (2022Hi01) 130TE cG $B(E2)(W.u.)=16.0 in author' Table I seems a misprint 130TE G 1133.36 7 12 4 M1+E2 +1.1 9 d 130TE2 G A2=-0.67 9 $ A4=-0.27 12 130TEF G FLAG=f 130TE cG MR$tentative value (2022Hi01) 130TEB G BM1=0.0056 +50-39 $ BE2W=2.1 +18-15 (2022Hi01) 130TE G 1178.06 6 39 1 M1+E2 +0.19 +8-7 130TE2 G A2=-0.01 3 $ A4=-0.04 5 130TEB G BM1=0.036 +6-5 $ BE2W=0.35 +6-5 (2022Hi01) 130TE G 1926.78 6 13 2 M1+E2 +1.2 7 130TE2 G A2=+0.44 7 $ A4=+0.02 9 130TEB G BM1=0.0011 +8-6 $ BE2W=0.16 +11-9 (2022Hi01) 130TE L 2770.82 9 (5,6,7)- 130TE cL J$669.7|g(|q) gives J=3-7 with preference for J=7, and then for J=5, 130TE2cL with negative parity supported for all the spin choices. 130TE2cL Excitation functions agree well with SMC for J=5 130TE cL $A previous tentatively assigned 1137|g from this level is not 130TE2cL supported in the present experiment, although a small contribution 130TE3cL cannot be excluded, while an 1135.6| is observed in this work with a 130TE4cL threshold above E(n)=3.1 MeV (2022Hi01). 130TE G 669.66 2 100 130TE2 G A2=+0.07 4 $ A4=-0.27 6 130TE L 2781.77 13 (7-) 130TE cL J$680.6|g(|q) gives J=3-7; excitation function and SMC support J=7 130TE cL $A previously assigned 635.6|g from this level is neither supported 130TE2cL by excitation function nor by the |g|g-coin data in 2022Hi01 130TE G 680.61 10 100 130TE2 G A2=+0.34 26 $ A4=+0.09 37 130TE L 2789.22 7 (2+) 173 FS +21-14 130TE cL T$measured mean lifetime |t=250 fs {I+30-20} from DSA for 130TE2cL 1949.7|g (2022Hi01) 130TE cL J$1949.7|g(|q) gives J=2,3,(1); 903.4|g(|q) and 1201.2|g(|q) 130TE2cL give J=0-4; excitation functions and SMC for 903.4|g and 1949.7|g 130TE3cL support J=2. 130TE G 903.42 6 28 6(M1+E2) +0.8 +11-15 n 130TE2 G A2=+0.43 3 $ A4=+0.19 4 130TEF G FLAG=f 130TE cG $|d=+0.83 {I+110-150} (2022Hi01) 130TEB G BM1=0.051 +63-43$ BE2W=16 16 (2022Hi01) 130TE G 1201.19 8 3 3[M1,E2] 0.0011012 n 130TE2 G A2=+0.04 18 $ A4=+0.23 25 130TEF G FLAG=df 130TEB G BM1 LE 0.0086$ BE2W LE 2.2 (2022Hi01) 130TE G 1949.72 6 69 7(M1+E2) -1.6 11 130TE2 G A2=-0.21 2 $ A4=-0.07 3 130TEF G FLAG=f 130TEB G BM1=0.0062 +52-45 $ BE2W=1.5 +13-11 (2022Hi01) 130TE L 2833.64 10 (5+) 130TE cL J$1018.0|g(|q) excludes J=4, pure E2 to 1815, 6+ level; excitation 130TE2cL function and SMC support J=5, using the listed branching ratios 130TE G 501.7 6 5.3 7 g ? 130TEF G FLAG=r 130TE G 1018.04 6 84.5 16 d 130TE2 G A2=-0.21 4 $ A4=-0.08 5 130TEF G FLAG=r 130TE G 1200.77 20 10.1 13 d 130TEF G FLAG=r 130TE L 2834.94 7 4+ 250 FS +83-56 N 130TEF L FLAG=X 130TE cL T$measured mean lifetime |t=360 fs {I+120-80} (2022Hi01) 130TE G X x ? 130TE G 853.51 6 71 2 M1+E2 +1.4 +3-4 n 130TE2 G A2=+0.18 5 $ A4=-0.10 7 130TEF G FLAG=d 130TEB G BM1=0.062 +35-26 $ BE2W=59 +33-25 (2022Hi01) 130TE G 1246.70 9 8 2 E2 n 130TE2 G A2=-0.12 27 $ A4=-1.50 35 130TEB G BE2W=1.5 +10-7 (2022Hi01) 130TE G 1995.47 7 21 3 E2 n 130TE2 G A2=+0.05 10 $ A4=-0.60 14 130TEB G BE2W=0.38 +18-14 (2022Hi01) 130TE L 2887.84 7 2+ N 130TEF L FLAG=X 130TE G X x ? 130TE G 587.85 10 11 1 M1+E2 -1.4 +43-28 n 130TE2 G A2=-0.30 33 $ A4=-0.07 46 130TE G 1300.15 12 42 4 n 130TEF G FLAG=dg 130TEF G FL=1588.206 130TE cG E$somewhat poor fit, level-energy difference=1299.75 130TE G 2048.11 11 35 1 M1+E2 -1.6 +11-10 n 130TE2 G A2=-0.40 3 $ A4=-0.16 8 130TE cG $|d=-1.56 {I+73-178} (2022Hi01) 130TE G 2887.72 13 12 1 E2 n 130TE2 G A2=+0.41 14 $ A4=0.00 22 130TE L 2926.57 16 5(-) N 130TEF L FLAG=X 130TE G X x ? 130TE G 490.8 3 14 LE(M1+E2) -0.29 +16-14 n 130TE2 G A2=-0.68 20 $ A4=-0.21 27 130TEF G FLAG=d 130TE cG RI$|<14 {I8} (2022Hi01) 130TE G 521.54 6 86 GE(M1(+E2)) +0.03 +13-3 n 130TE2 G A2=-0.23 4 $ A4=-0.02 5 130TE L 2945.65 5 2+ 201 FS 28 N 130TEF L FLAG=X 130TE cL T$measured mean lifetime |t=290 fs {I40} (2022Hi01) 130TE G X x ? 130TE G 807.18 7 12 3 M1(+E2) +0.19 +30-26 n 130TE2 G A2=-0.07 13 $ A4=+0.13 18 130TEF G FLAG=f 130TEB G BM1=0.044 +20-16 $ BE2W=0.89 +40-89 (2022Hi01) 130TE G 1059.87 7 16 1 M1+E2 +1.4 +9-32 n 130TE2 G A2=+0.19 12 $ A4=-0.12 17 130TEB G BM1=0.0093 +240-7 $ BE2W=5.7 +48-57 (2022Hi01) 130TE G 2106.24 11 46 2 M1+E2 -0.51 28 n 130TE2 G A2=-0.11 5 $ A4=-0.14 7 130TEB G BM1=0.0078 +26-21 $ BE2W=0.17 +6-5 (2022Hi01) 130TE G 2945.59 11 26 2 E2 n 130TE2 G A2=+0.28 6 $ A4=-0.22 8 130TEB G BE2W=0.086 +20-16 (2022Hi01) 130TE L 2953.28 9 3+ 152 FS +35-28 N 130TE cL T$measured mean lifetime |t=220 fs {I+50-40} (2022Hi01) 130TE G 1320.14 8 20 2 [M1,E2] n 130TE2 G A2=+0.31 19 $ A4=+1.09 16 130TEF G FLAG=d 130TEB G BM1 LE 0.030 $ BE2W LE 6.2 (2022Hi01) 130TE G 1365.85 37 14 3 [M1,E2] n 130TE2 G A2=-0.34 13 $ A4=+0.75 14 130TEF G FLAG=dg 130TEB G BM1 LE 0.021 $ BE2W LE 4.0 (2022Hi01) 130TE G 2113.93 11 66 3 M1+E2 -0.82 +32-26 n 130TE2 G A2=-0.60 4 $ A4=+0.03 6 130TEB G BM1=0.011 +5-4 $ BE2W=0.58 +29-20 (2022Hi01) 130TE L 2956.66 19 (4+) 0.51 PS +45-17 N 130TEF L FLAG=X 130TE cL T$measured mean lifetime |t=740 fs {I+650-250} (2022Hi01) 130TE cL J$1323.3|g(|q), 1368.6|g(|q), and 2117.2|g(|q) support J=4; |g to 2+ 130TE2cL suggests positive parity 130TE G X x ? 130TE G 1323.3 5 16 2 [M1,E2] n 130TE2 G A2=+0.03 41 $ A4=+0.36 34 130TEF G FLAG=d 130TEB G BM1 LE 0.0091 $ BE2W LE 1.9 (2022Hi01) 130TE G 1368.6 9 9 1 E2 n 130TE2 G A2=+0.41 19 $ A4=+1.90 15 130TEF G FLAG=d 130TEB G BE2W=0.53 +37-29 (2022Hi01) 130TE G 2117.2 2 75 4 E2 n 130TE2 G A2=+0.30 6 $ A4=-0.24 8 130TEB G BE2W=0.50 +30-25 (2022Hi01) 130TE L 3006.4 4 7- N 130TE G 905.2 3 100 n 130TE2 G A2=+0.44 15 $ A4=0.00 22 130TEF G FLAG=g 130TE L 3021.21 9 5+ 1.04 PS GE N 130TE cL T$measured mean lifetime |t|>1500 fs (2022Hi01) 130TE G 1039.78 6 100 M1+E2 +0.37 +25-15 n 130TE2 G A2=+0.19 9 $ A4=-0.23 12 130TEB G BM1 LE 0.032 $ BE2W LE 1.6 (2022Hi01) 130TE L 3036.64 10 (5,6)- 208 FS GE N 130TE cL T$measured mean lifetime |t|>300 fs (2022Hi01) 130TE G 400.21 21 52 2 (M1+E2) -0.73 +45-53 n 130TE2 G A2=-0.04 12 $ A4=+0.06 16 130TEB G BM1 LE 1.3 $ BE2W LE 1700 (2022Hi01) 130TE cG $|d(E2/M1), B(M1) and B(E2)(W.u.) for J|p(3036 level)=(5)-. Note 130TE2cG that RUL(E2)=300 130TE G 935.46 6 48 2 (M1+E2) +3.1 14 n 130TE2 G A2=-0.43 10 $ A4=+0.07 14 130TE cG $|d=+3.11 {I+236-99} (2022Hi01) 130TEB G BM1 LE 0.016 $ BE2W LE 67 (2022Hi01) 130TE cG $|d(E2/M1), B(M1) and B(E2)(W.u.) for J|p(3036 level)=(5)- 130TE L 3046.66 10 (5) N 130TE G 1231.03 6 71 3 n 130TE2 G A2=-0.26 5 $ A4=-0.26 6 130TE G 1414.14 10 29 3 n 130TEF G FL=1633.01 130TE cG E$somewhat poor fit, level-energy difference=1413.63 130TE L 3055.43 21 (4,2,3) N 130TEF L FLAG=X 130TE G X x ? 130TE G 289.1 2 100 D(+Q) -0.06 +19-14 n 130TE2 G A2=-0.18 15 $ A4=+0.14 19 130TE cG $|d(Q/D) for J(3055 level)=(4) 130TE L 3083.12 12 (0:4) 132 FS +42-28 N 130TEF L FLAG=X 130TE cL T$measured mean lifetime |t=190 fs {I+60-40} (2022Hi01) 130TE G X x ? 130TE G 2243.61 11 n 130TE2 G A2=0.00 8 $ A4=-0.15 11 130TE L 3094.85 4 2+ 125 FS 14 N 130TE cL T$measured mean lifetime |t=180 fs {I20} (2022Hi01) 130TE G 956.34 7 7.4 3 M1(+E2) +0.16 +23-17 n 130TE2 G A2=-0.09 12 $ A4=+0.10 17 130TEB G BM1=0.026 5 $ BE2W=0.27 +6-27 (2022Hi01) 130TE G 1209.35 50 3.1 3 [M1,E2] n 130TE2 G A2=-0.14 29 $ A4=-0.62 43 130TEF G FLAG=d 130TEB G BM1 LE 0.0070 $ BE2W LE 1.4 +4-3 (2022Hi01) 130TE G 1461.70 8 27.6 2 E2 n 130TE2 G A2=+0.02 1 $ A4=-0.01 2 130TEF G FLAG=d 130TEB G BE2W=4.9 +7-6 (2022Hi01) 130TE G 1506.68 6 18.2 6 M1+E2 -1.6 +13-12 n 130TE2 G A2=-0.30 7 $ A4=-0.05 10 130TEB G BM1 LE 0.0086 $ BE2W=2.0 +20-17 (2022Hi01) 130TE G 2255.32 11 26.5 8 M1+E2 -1.5 +7-8 n 130TE2 G A2=-0.37 5 $ A4=-0.02 7 130TEB G BM1=0.0024 +13-21 $ BE2W=0.37 +26-19 (2022Hi01) 130TE G 3094.8 5 17.2 6 E2 n 130TE2 G A2=+0.37 7 $ A4=-0.18 11 130TEB G BE2W=0.072 +12-10 (2022Hi01) 130TE L 3103.56 10 6- 277 FS GE N 130TEF L FLAG=X 130TE cL T$measured mean lifetime |t|>400 fs (2022Hi01) 130TE G X x ? 130TE G 1002.40 6 100 M1+E2 -0.68 +28-65 n 130TE2 G A2=-0.87 8 $ A4=+0.05 11 130TE L 3110.03 6 1 270 FS +83-56 N 130TEF L FLAG=X 130TE cL T$measured mean lifetime |t=390 fs {I+120-80} (2022Hi01) 130TE G X x ? 130TE G 1521.74 6 21 2 n 130TE2 G A2=+0.14 6 $ A4=+0.08 9 130TEF G FLAG=d 130TE G 2270.94 14 16 1 n 130TE2 G A2=+0.17 17 $ A4=+0.05 24 130TE G 3110.08 51 63 2 n 130TE2 G A2=-0.18 7 $ A4=-0.10 10 130TE L 3128.80 4 2+ 471 FS GE N 130TEF L FLAG=X 130TE cL T$measured mean lifetime |t|>680 fs (2022Hi01) 130TE G X x ? 130TE G 938.28 6 14.2 8 M1+E2 -1.5 13 n 130TE2 G A2=-0.24 10 $ A4=-0.05 14 130TEF G FLAG=d 130TE G 990.49 10 11.9 8 M1(+E2) +0.09 320 n 130TE2 G A2=-0.21 21 $ A4=-0.29 30 130TE G 1243.08 6 17.4 6 M1(+E2) +0.73 +86-97 n 130TE2 G A2=-0.03 12 $ A4=-0.58 15 130TE G 1540.39 11 11.1 7 M1(+E2) +0.59 +81-77 n 130TE2 G A2=+0.47 18 $ A4=+0.25 26 130TE G 2289.30 12 21.9 8 M1+E2 -1.5 +17-18 n 130TE2 G A2=-0.23 12 $ A4=-0.12 17 130TE G 3128.78 51 23.5 9 E2 n 130TE2 G A2=+0.21 12 $ A4=-0.40 18 130TE L 3132.04 10 (6-,7-) 0.4 PS +11-2 N 130TEF L FLAG=X 130TE cL T$measured mean lifetime |t=630 fs {I+1600-280} (2022Hi01) 130TE G 1030.88 6 100 (M1+E2) +1.7 +7-9 n 130TE2 G A2=+0.58 9 $ A4=+0.17 12 130TEB G BM1=0.021 +37-18 $ BE2W=21 +32-18 (2022Hi01) 130TE cG $Mult, B(M1) and B(E2)(W.u.) for J|p(3132.1 level)=(6-) 130TE L 3138.01 13 (5+) N 130TE G 1322.42 10 100 (M1+E2) +0.9 +13-11 n 130TE2 G A2=+0.03 41 $ A4=+0.36 34 130TEF G FLAG=d 130TE cG $|d=+0.93 {I+130-110} (2022Hi01) 130TE L 3144.92 21 (5,6,7) N 130TE G 998.71 12 100 n 130TE2 G A2=+0.38 23 $ A4=-0.06 35 130TEF G FLAG=d 130TE L 3154.55 8 4+ 194 FS +49-35 130TE cL T$measured mean lifetime |t=280 fs {I+70-50} (2022Hi01) 130TE cL J$2314.8|g(|q) gives J=4,(2,3); 1566.0|g(|q) gives J=1,2,3,(4); 130TE2cL 1521.6|g(|q) gives J=2-5; excitation function and SMC support J=4; 130TE3cL |g to 2+ suggests positive parity. 130TE G 1521.64 6 27 2 M1+E2 -0.36 +25-29 d 130TE2 G A2=+0.14 6 $ A4=+0.08 9 130TE cG RI$intensity for the doublet assigned from |g|g-coin data (2022Hi01) 130TEB G BM1=0.014 +6-5 $ BE2W=0.28 +12-9 (2022Hi01) 130TE G 1566.04 15 13 1 E2 6.79E-4 n 130TE2 G A2=-0.14 24 $ A4=+0.23 34 130TEB G BE2W=1.0 +4-3 (2022Hi01) 130TE G 2314.83 11 60 2 E2 7.28E-4 n 130TE2 G A2=+0.05 8 $ A4=-0.18 11 130TEB G BE2W=0.67 +18-16 (2022Hi01) 130TE L 3163.40 13 (5,3) N 130TEF L FLAG=X 130TE G X x ? 130TE G 1181.97 11 100 (D+Q) -2.3 +18-10 n 130TE2 G A2=-0.60 24 $ A4=+0.11 32 130TE cG MR$for J(3163 level)=5. Other |d=-0.36 {I+25-29} (2022Hi01) 130TE L 3176.91 8 3- 0.5 PS +49-3 N 130TE cL T$measured mean lifetime |t=660 fs {I+7000-340} (2022Hi01) 130TE cL J$from 1291.2|g(|q) and excitation function compared with SMC; 130TE2cL |g to 5- 130TE G 1075.76 6 28 1 E2 1.23E-3 n 130TE2 G A2=+0.11 10 $ A4=-0.03 14 130TEB G BE2W=6.2 +72-57 (2022Hi01) 130TE G 1291.21 6 61 1 E1 4.65E-4 n 130TE2 G A2=-0.30 6 $ A4=+0.08 9 130TEB G BE1W=1.6E-4 +18-15 (2022Hi01) 130TE G 2337.34 14 11 1 E1 9.75E-4 n 130TE2 G A2=-0.72 20 $ A4=-0.92 33 130TEB G BE1W=5.0E-6 +54-46 (2022Hi01) 130TE L 3181.06 11 (5-,7-) N 130TE G 1079.90 7 100 (M1+E2) +0.40 +40-38 n 130TE2 G A2=+0.60 13 $ A4=-0.27 19 130TE cG $|d(E2/M1) for J|p(3181)=(5-) 130TE L 3187.60 10 4- 0.8 PS +27-4 N 130TE cL T$measured mean lifetime |t=1100 fs {I+3900-600} (2022Hi01) 130TE G 1086.44 6 100 M1+E2 +1.1 +5-6 n 130TE2 G A2=-0.64 5 $ A4=+0.09 7 130TEB G BM1=0.018 +32-15 $ BE2W=7.2 +120-62 (2022Hi01) 130TE L 3195.32 12 0:4 N 130TEF L FLAG=X 130TE G X x ? 130TE G 1309.66 14 38 4 n 130TE2 G A2=-0.33 33 $ A4=-0.75 47 130TE G 1607.04 21 62 4 n 130TE2 G A2=+0.11 10 $ A4=-0.07 15 130TEF G FLAG=dg 130TE L 3196.31 7 2+ 90 FS 14 N 130TE cL T$measured mean lifetime |t=130 fs {I20} (2022Hi01) 130TE G 1057.61 22 4 1 [M1+E2] 0.0014517 n 130TEF G FLAG=dg 130TEB G BM1 LE 0.022 $ BE2W LE 7.1 (2022Hi01) 130TE G 1608.16 8 24 4 [M1+E2] 0.000715 n 130TE2 G A2=+0.11 10 $ A4=-0.07 15 130TEF G FLAG=dg 130TEB G BM1 LE 0.035 $ BE2W LE 4.9 (2022Hi01) 130TE G 2356.60 16 16 5 M1+E2 +0.59 +77-64 n 130TE2 G A2=+0.78 17 $ A4=+0.50 24 130TE cG $|d=+0.59 {I+138-53} (2022Hi01) 130TEB G BM1=0.0041 +29-26 $ BE2W=0.094 +73-94 (2022Hi01) 130TE G 3196.13 51 56 8 E2 1.01E-3 n 130TE2 G A2=+0.41 7 $ A4=0.00 8 130TEB G BE2W=0.28 8 (2022Hi01) 130TE L 3204.62 8 3,(2) N 130TEF L FLAG=X 130TE G X x ? 130TE G 369.95 22 n 130TE2 G A2=+0.26 28 $ A4=+0.56 38 130TEF G FLAG=d 130TE G 1066.04 6 n 130TE2 G A2=+0.24 9 $ A4=+0.05 13 130TEF G FLAG=d 130TE G 1318.84 14 n 130TE2 G A2=+0.31 19 $ A4=+1.09 16 130TEF G FLAG=d 130TE G 1616.56 12 n 130TE2 G A2=+2.12 50 $ A4=+1.54 41 130TEF G FLAG=d 130TE L 3236.32 19 (1:4) N 130TE G X x ? 130TE G 2396.81 18 100 n 130TE2 G A2=+0.27 30 $ A4=-0.87 45 130TE L 3236.71 10 (4,6)- N 130TE G 1135.55 6 100 (M1+E2) +1.1 6 n 130TE2 G A2=-0.65 6 $ A4=+0.22 7 130TE cG $|d(E2/M1) for J|p(3237)=(4-) 130TE L 3241.8 5 1 159 FS +35-28 N 130TEF L FLAG=X 130TE cL T$measured mean lifetime |t=230 fs {I+50-40} (2022Hi01) 130TE G X x ? 130TE G 3241.73 51 100 n 130TE2 G A2=-0.30 5 $ A4=-0.15 8 130TE L 3243.51 11 3- 97 FS +28-21 N 130TE cL T$measured mean lifetime |t=140 fs {I+40-30} (2022Hi01) 130TE G X x ? 130TE G 1142.2 3 n 130TE2 G A2=+0.28 1 $ A4=-0.05 1 130TEF G FLAG=d 130TE G 1357.95 15 19.4 LE n 130TE2 G A2=-0.10 29 $ A4=+0.02 34 130TE G 2403.94 12 80.6 LE n 130TE2 G A2=+0.35 9 $ A4=0.00 13 130TE L 3287.4 3 (5) N 130TE G 851.6 2 n 130TEF G FLAG=d 130TE L 3319.17 9 (4,3,2) 0.21 PS +53-10 N 130TEF L FLAG=X 130TE cL T$measured mean lifetime |t=300 fs {I+760-150} (2022Hi01) 130TE G X x ? 130TE G 1433.46 8 n 130TEF G FLAG=g 130TE G 1731.2 5 n 130TEF G FLAG=g 130TE G 2479.7 2 n 130TE2 G A2=+0.66 17 $ A4=+0.63 24 130TE L 3340.67 15 (3+) 0.12 PS +24-6 N 130TEF L FLAG=X 130TE cL T$measured mean lifetime |t=180 fs {I+340-90} (2022Hi01) 130TE G X x ? 130TE G 1752.2 2 45 5 M1+E2 -0.83 +86-80 n 130TE2 G A2=-1.20 78 $ A4=-0.54 81 130TE G 2501.4 2 55 5 M1(+E2) +0.09 +36-32 n 130TE2 G A2=+0.13 26 $ A4=+0.48 42 130TE L 3342.92 15 (3,4) N 130TEF L FLAG=X 130TE G X x ? 130TE G 1710.2 2 28 3 n 130TE2 G A2=-0.70 43 $ A4=-0.08 56 130TE G 1754.4 2 72 3 D+Q -1.2 +16-15 n 130TE2 G A2=+0.50 20 $ A4=-0.22 34 130TE cG $|d(Q/D) for J(3342 level)=(3) 130TE 130TE 2B-:T1/2:XUNDL-10 2019AL27 202208 130TE c Compiled (unevaluated) dataset from 2019Al27: 130TE2c Eur. Phy. J C 79, 795 (2019) 130TE c Compiled by E.A. McCutchan (NNDC,BNL) July 7, 2022 130TE c Search for 2|b{+-} decay of {+130}Te with CUORE-0 130TE c CUURE-0 consists of 52 natural TeO{-2} crystals. 130TE2c Combined mass of 39 kg with 10.8 kg of {+130}Te. 130TE3c Crystals operated at 10 mK using a dilution refrigerator. 130TE4c Results here are from {+130}Te exposure of 9.8 kg y. 130TE5c Measured energy spectrum; deduced lower limit for neutrinoless 130TE6c double beta decay to the first excited state in {+130}Xe. 130TE L 0.0 2.4E23 Y GT 130TE cL T$at 90% confidence level for 2|n decay to first excited 130TE2cL 0+ state in {+130}Xe (2019Al27). For 0|n decay mode, 130TE3cL T{-1/2} > 7.9|*10{+23} y for decay to first excited 0+ 130TE4cL state in {+130}Xe (2019Al27). Authors also combine their 130TE5cL results with those from CUORICINO experiment to obtain 130TE6cL T{-1/2}{+0|n} > 1.4|*10{+24} y and T{-1/2}{+2|n} > 130TE7cL 2.5|*10{+23} y, both for decay to the first excited state 130TE8cL in {+130}Xe. 130TE 130SB B- DECAY:T1/2:XUNDL-11 2022KU31 202210 130TE c Includes {+130m}Te IT decay (1.90 |ms) 130TE c Compiled (unevaluated) dataset from 2022Ku31: 130TE2c Phys Rev C 106, 034306 (2022) 130TE c Compiled by B. Singh (McMaster), Sept 16, 2022 130TE c 2022Ku31: measured level lifetimes by |g|g(t) and |g(t) using 130TE2c Generalized Centroid Difference (GCD) method for lifetimes in 130TE3c ps region, slope method for lifetimes in the ns region up to |?30 ns, 130TE4c and delayed gamma-decay curves for longer lifetimes using four 130TE5c LaBr{-3}(Ce) detectors, two clover HPGe detectors, and an ionization 130TE6c chamber. Levels in {+130}Te were populated in |b{+-} decay of {+130}Sb, 130TE7c and decay of micro-second isomer in {+130}Te. The {+130}Sb and {+130}Te 130TE8c activities were formed in {+233}U(n,F),E=thermal at ILL-Grenoble, and 130TE9c recoiling fission fragments were separated in mass and kinetic energy 130TEAc using the Lohengrin recoil fragment separator. Deduced B(E2) values. 130TEBc Comparison with previous experimental results, and with large-basis 130TECc shell-model (LBSM) calculations 130TE cL J$As listed in Fig. 1 of 2022Ku31, based on assignments in literature 130SB P 0.0 (8-) 39.5 M 8 5067 14 130SB cP J,T$From {+130}Sb Adopted Levels in the ENSDF database 130SB2cP (May 2001 update) 130SB cP QP$From 2021Wa16 (AME2020). 130TE N 1.0 130TE L 0 0+ 130TE L 840 2+ 3.5 PS 21 130TE cL $Measured mean lifetime |t=5 ps {I3} from 794|g-840|g(t) (2022Ku31). 130TE2cL Compared with T{-1/2}=2.30 ps {I5} (|t=3.32 {I7}) in the ENSDF 130TE3cL database; and measured B(E2)(up)=0.291 e{+2}b{+2} {I10} from Coulomb 130TE4cL excitation, which translates to |t=3.38 ps {I12} (2013St24: 130TE5cL Phys. Rev. C 88, 051304(R) (2013)) 130TE G 840 E2 130TEB G BE2W=10.0 +150-40 (2022Ku31) 130TE L 1633 4+ 4.2 PS 28 130TE cL $Measured mean lifetime |t=6 ps {I4}, from combined lifetimes for the 130TE2cL first 2+ and 4+ states |t=11 ps {I3} and 14 ps {I3} from 130TE3cL 182|g-840|g(t), subtracting lifetime of the first 2+ state (2022Ku31). 130TE4cL Authors compared their result to |t=4.7 ps {I10} (from B(E2) in 130TE5cL Coul. Ex. in 2020CoZY: EPJ Web of Conf. Vol. 232 (2020)); and 130TE6cL tau=1.395 {I+342-237} (stat) {I+150-124} (syst) (from DSA in 2022Pr02: 130TE7cL Phys. Rev. C 105, 034319) 130TE G 794 E2 130TEB G BE2W=11.0 +220-40 (2022Ku31) 130TE L 1815 6+ 9.4 NS 6 130TE cL $Measured mean lifetime |t=13.5 ns {I8} and 14.5 ns {I2} from 130TE2cL 331|g-182|g(t) (2022Ku31). Compared with T{-1/2}=9.8 ns {I5} 130TE3cL (|t=14.1 ns {I7}) in the ENSDF database. 130TE G 182 E2 0.207 5 130TE cG CC$for E|g=182 {I1} 130TEB G BE2W=6.4 4 (2022Ku31) 130TE L 2147 7- 107 NS 17 M1 130TE cL $Measured mean lifetime |t=155 ns {I24} from 502|g-331|g(t) (2022Ku31). 130TE2cL Compared with T{-1/2}=115 ns {I8} (|t=166 ns {I11}) in the ENSDF 130TE3cL database. Newer measurement: T{-1/2}=186 ns {I11} (2004Va03: 130TE4cL Phys. Rev. C 69, 024316); 110 ns {I5} (2014As01: 130TE5cL Eur. Phys. Jour. A50, 2) 130TE G 331 E1+M2 +0.070 6 130TEB G BE1W=6.8E-8 +13-10 $BM2W=0.0139 +38-29 130TE L 2648.3 1 8+ 83 NS LT 130TE cL E$from 2004Br19 (Eur. Phys. Jour. A20, 145); and 130TE2cL 2014As01 (Eur. Phys Jour. A50, 2) 130TE cL $Measured mean lifetime |t<120 ns (2022Ku31). 130TE G 502 130TE G 833 130TEB G BE2W>0.00025 (2022Ku31) 130TE L 2666.7 3 10+ 1.91 US 8 M2 130TE cL E$from 2004Br19 and 2014As01. 130TE cL $Measured mean lifetime |t=2.76 |ms {I12} from (794|g+840|g)(t) 130TE2cL (2022Ku31). Compared with T{-1/2}=1.90 |ms {I8} (|t=2.74 |ms {I11}) in 130TE3cL the ENSDF database. 130TE G 18.4 3 [E2] 1.66E3 15 S 130TE cG E$from level-energy difference (compiler) 130TEB G BE2W=2.2 1 (2022Ku31) 130TE 130TE 2B-:T1/2:XUNDL-12 2020NU01 202212 130TE c Compiled (unevaluated) dataset from 2020Nu01 130TE c J. Low Temp. Phys. 199, 519 (2020) 130TE c Compiled by S. Ota (NNDC,BNL). Aug. 26, 2022 130TE c The cryogenic calorimeteric detector located underground at the 130TE2c Laboratori Nazionali del Gran Sasso was used to search for the 130TE3c 0|n|b|b decay of {+130}Te (CUORE experiment). The detector consists 130TE4c of {+nat}TeO{-2} crystals arranged into 19 towers of 13 floors with 4 130TE5c crystals per floor (988 crystals in total). Each crystal weighs 750 g 130TE6c (containing 208 g of {+130}Te) and its size is 5|*5|*5 cm{+3}, and 130TE7c thus the total mass of TeO{-2} in the detector is 742 kg, 130TE8c corresponding to 206 kg of {+130}Te. This setup allows to have the 130TE9c {+130}Te |b|b emitters within the detector absorber itself. The 130TEac detector's average energy resolution in the run was 7.7 {I5} keV 130TEbc (FWHM) at 2527 keV (=Q{-|b|b}). The events corresponding to 0|n|b|b 130TEcc decay were looked for after applying basic quality cuts, rejection of 130TEdc spurious signals by pulse shape analysis and anti-coincidence 130TEec selections to the raw data. As of the publication date (86.3 130TEfc kg(TeO{-2}) year exposure), no evidence was found for the 0|n|b|b 130TEgc decay of {+130}Te, and the lower limit of T{-1/2} and the upper limit 130TEhc of the effective Majorana neutrino mass ({Im}{-|b|b}) were deduced. 130TEic T{-1/2} of the {+130}Te 2|n|b|b decay was obtained most precisely 130TEjc among the past experiments and consistent with previous measurements. 130TE L 0.0 0+ 1.3E25 Y GT 130TE cL T$For 0|n|b|b from 2020Nu01 with a 90% C.L. The authors stated that 130TE2cL T{-1/2} > 1.5|*10{+25} yrs (90% C. L.), combined with the CUORE-0 130TE3cL (2015Al20, 2016Al11) and Cuoricino (2011An08) results. 130TE cL T$7.9 {I1} (stat) {I2} (syst) |* 10{+20} yrs for 2|n|b|b from 130TE2cL 2020Nu01. 130TE 130TE(POL G,G'):XUNDL-15 2021IS05 202309 130TE c Includes {+130}Te(|g,|g') 130TE c Compiled (unevaluated) dataset from 2021Is05: 130TE2c Phys Rev C 103, 044317 (2021) + Supplemental Material 130TE c Compiled by B. Singh (McMaster), January 23, 2023. 130TE c 2021Is05: two experiments were performed: 1. at S-DALINAC facility in 130TE2c Darmstadt, using continuous-energy bremsstrahlung photon beam of 130TE3c endpoint energy of 6.0 and 9.13 MeV from Darmstadt high-intensity 130TE4c photon setup (DHIPS) and 99.8 enriched {+128}Te target. Measured E|g, 130TE4c I|g, |g(|q) using BGO-shielded three HPGe detectors at 90|' and 130|' 130TE5c with respect to the beam direction. 2. at TUNL using the High Intensity 130TE6c |g-ray Source (HI|gS) facility providing fully linearly polarized and 130TE7c quasimonochromatic photon beams of 2.76-8.92 MeV. Measured E|g, I|g, 130TE8c |g(linear polarization) using four HPGe detectors. Comparison with 130TE9c predictions of quasiparticle phonon model. 130TE cL E(a)$Level is previously known. 130TE CL T$LABEL=|G{-0}{+2}/|G (eV) 130TE CL S$LABEL=B(E1)|^ (e{+2}b) 130TE L 0.0 0+ 130TE L 2606.4 7 1 0.0026 EV 4 0.68E-5 17a 130TE G 2606.4 7 130TE L 2688.0 6 1 0.0063 EV 5 0.93E-5 7 a 130TE G 2688.0 6 130TE L 2742.7 6 1 0.0051 EV 5 0.71E-5 7 a 130TE G 2742.7 6 130TE L 3566.7 7 1 0.0123 EV 6 0.78E-5 4 a 130TE G 3566.7 7 130TE L 3681.8 8 1 0.0121 EV 7 0.70E-5 4 130TE G 3681.8 8 130TE L 3982.2 8 1 0.0093 EV 8 0.42E-5 4 130TE G 3982.2 8 130TE L 4531.3 6 1 0.062 EV 3 1.91E-5 9 130TE G 4531.3 6 130TE L 4733.9 8 1 0.0090 EV 14 0.24E-5 4 130TE G 4733.9 8 130TE L 4744.5 7 1 0.0384 EV 24 1.03E-5 7 130TE G 4744.5 7 130TE L 4811.0 6 1 0.129 EV 4 3.32E-5 10 130TE G 4811.0 6 130TE L 4979.5 8 1 0.034 EV 8 0.79E-5 19 130TE G 4979.5 8 130TE L 4984.3 9 1 0.049 EV 5 1.13E-5 12 130TE G 4984.3 9 130TE L 5099.2 10 1 0.020 EV 5 0.43E-5 11 130TE G 5099.2 10 130TE L 5116.2 11 1 0.031 EV 4 0.66E-5 9 130TE G 5116.2 11 130TE L 5181.6 7 1 0.053 EV 5 1.09E-5 10 130TE G 5181.6 7 130TE L 5247.4 7 1 0.045 EV 4 0.89E-5 8 130TE G 5247.4 7 130TE L 5359.8 8 1- 0.044 EV 15 0.82E-5 27 130TE G 5359.8 8 130TE L 5369.2 9 1- 0.043 EV 16 0.79E-5 29 130TE G 5369.2 9 130TE L 5420.0 10 1- 0.050 EV 6 0.90E-5 10 130TE G 5420.0 10 130TE L 5451.1 8 1- 0.048 EV 5 0.84E-5 9 130TE G 5451.1 8 130TE L 5472.5 11 1- 0.035 EV 5 0.61E-5 9 130TE G 5472.5 11 130TE L 5483.8 9 1- 0.070 EV 6 1.23E-5 10 130TE G 5483.8 9 130TE L 5581.3 9 1- 0.092 EV 10 1.52E-5 16 130TE G 5581.3 9 130TE L 5606.0 7 1- 0.315 EV 10 5.13E-5 17 130TE G 5606.0 7 130TE L 5612.9 8 1- 0.087 EV 17 1.41E-5 27 130TE G 5612.9 8 130TE L 5619.9 7 1- 0.171 EV 8 2.77E-5 12 130TE G 5619.9 7 130TE L 5630.3 9 1- 0.066 EV 14 1.05E-5 22 130TE G 5630.3 9 130TE L 5641.3 9 1- 0.057 EV 5 0.92E-5 8 130TE G 5641.3 9 130TE L 5652.3 9 1- 0.152 EV 8 2.41E-5 13 130TE G 5652.3 9 130TE L 5694.3 8 1- 0.419 EV 26 6.5E-5 4 130TE G 5694.3 8 130TE L 5700.8 7 1- 0.355 EV 25 5.5E-5 4 130TE G 5700.8 7 130TE L 5714.1 7 1- 0.205 EV 8 3.16E-5 13 130TE G 5714.7 7 130TE L 5743.7 6 1- 0.306 EV 9 4.63E-5 14 130TE G 5743.7 6 130TE L 5757.9 9 1- 0.157 EV 12 2.35E-5 18 130TE G 5757.9 9 130TE L 5765.5 6 1- 0.484 EV 14 7.24E-5 21 130TE G 5765.5 6 130TE L 5809.8 11 1- 0.070 EV 8 1.02E-5 12 130TE G 5809.8 11 130TE L 5824.1 7 1- 0.124 EV 8 1.81E-5 12 130TE G 5824.1 7 130TE L 5835.4 8 1- 0.188 EV 11 2.71E-5 17 130TE G 5835.4 8 130TE L 5840.9 8 1- 0.161 EV 12 2.32E-5 18 130TE G 5840.9 8 130TE L 5859.3 9 1- 0.076 EV 16 1.08E-5 22 130TE G 5859.3 9 130TE L 5866.9 8 1- 0.134 EV 8 1.90E-5 11 130TE G 5866.9 8 130TE L 5875.8 8 1- 0.166 EV 11 2.34E-5 15 130TE G 5875.8 8 130TE L 5884.9 9 1- 0.086 EV 15 1.20E-5 20 130TE G 5884.9 9 130TE L 5899.0 6 1- 0.438 EV 11 6.13E-5 16 130TE G 5899.0 6 130TE L 5917.3 2 1- 0.154 EV 8 2.14E-5 11 130TE G 5917.3 2 130TE L 5986.4 9 1- 0.126 EV 10 1.68E-5 14 130TE G 5986.4 9 130TE L 6005.5 12 1- 0.063 EV 11 0.83E-5 14 130TE G 6005.5 12 130TE L 6006.8 15 1- 0.087 EV 16 1.16E-5 22 130TE G 6006.8 15 130TE L 6013.9 13 1- 0.140 EV 18 1.84E-5 24 130TE G 6013.9 13 130TE L 6020.0 10 1- 0.069 EV 10 0.91E-5 13 130TE G 6020.0 10 130TE L 6032.0 11 1- 0.156 EV 21 2.04E-5 27 130TE G 6032.0 11 130TE L 6038.4 8 1- 0.359 EV 21 4.68E-5 28 130TE G 6038.4 8 130TE L 6046.9 10 1- 0.103 EV 9 1.34E-5 11 130TE G 6046.9 10 130TE L 6067.9 8 1- 0.187 EV 8 2.40E-5 11 130TE G 6067.9 8 130TE L 6087.8 6 1- 0.608 EV 14 7.73E-5 18 130TE G 6087.8 6 130TE L 6104.8 7 1- 0.263 EV 11 3.31E-5 14 130TE G 6104.8 7 130TE L 6133.1 10 1- 0.100 EV 18 1.25E-5 23 130TE G 6133.1 10 130TE L 6150.9 7 1- 0.307 EV 13 3.79E-5 16 130TE G 6150.9 7 130TE L 6182.7 7 1- 0.306 EV 13 3.72E-5 16 130TE G 6182.7 7 130TE L 6202.7 8 1- 0.255 EV 12 3.06E-5 14 130TE G 6202.7 8 130TE L 6209.9 8 1- 0.267 EV 14 3.20E-5 17 130TE G 6209.9 8 130TE L 6216.8 9 1- 0.160 EV 14 1.91E-5 16 130TE G 6216.8 9 130TE L 6228.6 7 1- 0.353 EV 15 4.19E-5 18 130TE G 6228.6 7 130TE L 6238.2 9 1- 0.210 EV 14 2.49E-5 17 130TE G 6238.2 9 130TE L 6258.0 9 1- 0.073 EV 6 0.86E-5 6 130TE G 6258.0 9 130TE L 6274.0 8 1- 0.218 EV 13 2.53E-5 15 130TE G 6274.0 8 130TE L 6291.4 11 1- 0.154 EV 15 1.78E-5 17 130TE G 6291.4 11 130TE L 6299.4 12 1- 0.116 EV 13 1.33E-5 15 130TE G 6299.4 12 130TE L 6308.4 7 1- 0.585 EV 18 6.69E-5 20 130TE G 6308.4 7 130TE L 6324.0 12 1- 0.158 EV 21 1.79E-5 24 130TE G 6324.0 12 130TE L 6333.4 8 1- 0.278 EV 16 3.15E-5 18 130TE G 6333.4 8 130TE L 6341.0 9 1- 0.224 EV 15 2.52E-5 17 130TE G 6341.0 9 130TE L 6352.2 9 1- 0.433 EV 27 4.85E-5 30 130TE G 6352.2 9 130TE L 6370.3 10 1- 0.145 EV 14 1.61E-5 16 130TE G 6370.3 10 130TE L 6378.0 8 1- 0.307 EV 16 3.40E-5 18 130TE G 6378.0 8 130TE L 6402.6 7 1- 0.225 EV 14 2.47E-5 16 130TE G 6402.6 7 130TE L 6412.4 7 1- 0.440 EV 15 4.79E-5 16 130TE G 6412.4 7 130TE L 6433.7 8 1- 0.192 EV 13 2.07E-5 14 130TE G 6433.7 8 130TE L 6447.2 13 1- 0.936 EV 18 10.03E-5 20 130TE G 6447.2 13 130TE L 6474.4 7 1- 0.327 EV 15 3.46E-5 15 130TE G 6474.4 7 130TE L 6492.8 9 1- 0.161 EV 14 1.69E-5 14 130TE G 6492.8 9 130TE L 6505.5 8 1- 0.229 EV 14 2.39E-5 15 130TE G 6505.5 8 130TE L 6519.6 13 1- 0.113 EV 14 1.17E-5 15 130TE G 6519.6 13 130TE L 6528.5 6 1- 0.662 EV 18 6.83E-5 19 130TE G 6528.5 6 130TE L 6540.2 11 1- 0.147 EV 16 1.51E-5 16 130TE G 6540.2 11 130TE L 6558.2 7 1- 0.439 EV 17 4.47E-5 17 130TE G 6558.2 7 130TE L 6578.6 6 1- 1.079 EV 23 10.88E-5 23 130TE G 6578.6 6 130TE L 6590.6 10 1- 0.175 EV 17 1.75E-5 17 130TE G 6590.6 10 130TE L 6600.8 9 1- 0.800 EV 40 8.0E-5 4 130TE G 6600.8 9 130TE L 6613.6 8 1- 0.580 EV 27 5.76E-5 27 130TE G 6613.6 8 130TE L 6620.4 10 1- 0.173 EV 17 1.71E-5 16 130TE G 6620.4 10 130TE L 6631.3 8 1- 0.257 EV 16 2.53E-5 16 130TE G 6631.3 8 130TE L 6678.4 10 1- 0.123 EV 10 1.18E-5 10 130TE G 6678.4 10 130TE L 6689.4 11 1- 0.079 EV 17 0.75E-5 16 130TE G 6689.4 11 130TE L 6707.2 11 1- 0.194 EV 21 1.85E-5 20 130TE G 6707.2 11 130TE L 6714.7 8 1- 0.915 EV 51 8.7E-5 5 130TE G 6714.7 8 130TE L 6736.7 8 1- 0.420 EV 19 3.94E-5 18 130TE G 6736.7 8 130TE L 6770.2 7 1- 0.499 EV 18 4.62E-5 17 130TE G 6770.2 7 130TE L 6787.9 9 1- 0.292 EV 22 2.68E-5 21 130TE G 6787.9 9 130TE L 6808.3 10 1- 0.255 EV 23 2.32E-5 21 130TE G 6808.3 10 130TE L 6815.9 7 1- 0.893 EV 30 8.10E-5 27 130TE G 6815.9 7 130TE L 6827.7 8 1- 0.682 EV 32 6.15E-5 29 130TE G 6827.7 8 130TE L 6836.2 10 1- 0.528 EV 42 4.8E-5 4 130TE G 6836.2 10 130TE L 6842.6 10 1- 0.415 EV 42 3.7E-5 4 130TE G 6842.6 10 130TE L 6852.0 18 1- 0.158 EV 35 1.41E-5 31 130TE G 6852.0 18 130TE L 6858.4 14 1- 0.212 EV 33 1.89E-5 29 130TE G 6858.4 14 130TE L 6870.2 8 1- 0.286 EV 18 2.53E-5 16 130TE G 6870.2 8 130TE L 6907.4 9 1- 0.136 EV 23 1.18E-5 20 130TE G 6907.4 9 130TE L 6927.8 8 1- 0.470 EV 26 4.06E-5 22 130TE G 6927.8 8 130TE L 6937.9 8 1- 0.542 EV 27 4.66E-5 24 130TE G 6937.9 8 130TE L 6956.2 10 1- 0.329 EV 25 2.80E-5 21 130TE G 6956.2 10 130TE L 6968.3 14 1- 0.118 EV 24 1.00E-5 20 130TE G 6968.3 14 130TE L 6971.4 8 1- 0.333 EV 18 2.83E-5 15 130TE G 6971.4 8 130TE L 6986.9 7 1- 0.856 EV 30 7.20E-5 25 130TE G 6986.9 7 130TE L 6996.6 11 1- 0.283 EV 26 2.37E-5 22 130TE G 6996.6 11 130TE L 7000.2 12 1- 0.90 EV 23 0.75E-5 19 130TE G 7000.2 12 130TE L 7007.4 11 1- 0.252 EV 23 2.10E-5 19 130TE G 7007.4 11 130TE L 7012.7 11 1- 0.88 EV 22 0.73E-5 18 130TE G 7012.7 11 130TE L 7018.8 10 1- 0.179 EV 21 1.49E-5 18 130TE G 7018.8 10 130TE L 7024.0 12 1- 0.115 EV 23 0.95E-5 19 130TE G 7024.0 12 130TE L 7038.0 19 1- 0.390 EV 34 3.21E-5 28 130TE G 7038.0 19 130TE L 7043.3 19 1- 0.286 EV 40 2.35E-5 33 130TE G 7043.3 19 130TE L 7068.5 10 1- 0.286 EV 22 2.33E-5 18 130TE G 7068.5 10 130TE L 7085.2 8 1- 0.370 EV 21 2.98E-5 17 130TE G 7085.2 8 130TE L 7100.8 8 1- 0.676 EV 34 5.42E-5 27 130TE G 7100.8 8 130TE L 7110.1 11 1- 0.390 EV 33 3.11E-5 27 130TE G 7110.1 11 130TE L 7118.9 11 1- 0.313 EV 30 2.49E-5 24 130TE G 7118.9 11 130TE L 7145.3 10 1- 0.283 EV 25 2.23E-5 20 130TE G 7145.3 10 130TE L 7155.8 8 1- 0.206 EV 27 1.61E-5 21 130TE G 7155.8 8 130TE L 7162.4 4 1- 0.398 EV 29 3.11E-5 23 130TE G 7162.4 4 130TE L 7173.1 7 1- 0.899 EV 34 6.99E-5 26 130TE G 7173.1 7 130TE L 7184.4 9 1- 0.170 EV 43 1.31E-5 33 130TE G 7184.4 9 130TE L 7190.6 8 1- 0.706 EV 32 5.45E-5 25 130TE G 7190.6 8 130TE L 7200.0 10 1- 0.534 EV 42 4.11E-5 33 130TE G 7200.0 10 130TE L 7208.1 9 1- 0.688 EV 44 5.28E-5 34 130TE G 7208.1 9 130TE L 7223.0 10 1- 0.196 EV 41 1.49E-5 31 130TE G 7223.0 10 130TE L 7230.5 11 1- 0.572 EV 50 4.3E-5 4 130TE G 7230.5 11 130TE L 7235.5 13 1- 0.283 EV 36 2.15E-5 27 130TE G 7235.5 13 130TE L 7246.4 12 1- 0.266 EV 25 2.01E-5 19 130TE G 7246.4 12 130TE L 7306.4 8 1- 0.621 EV 34 4.57E-5 25 130TE G 7306.4 8 130TE L 7316.7 10 1- 0.346 EV 32 2.54E-5 23 130TE G 7316.7 10 130TE L 7328.9 12 1- 0.282 EV 30 2.06E-5 22 130TE G 7328.9 12 130TE L 7442.3 8 1- 0.522 EV 32 3.64E-5 22 130TE G 7442.3 8 130TE L 7450.9 10 1- 0.398 EV 29 2.76E-5 20 130TE G 7450.9 10 130TE L 7461.9 6 1- 0.133 EV 25 0.92E-5 17 130TE G 7461.9 6 130TE L 7475.8 6 1- 0.242 EV 34 1.67E-5 23 130TE G 7475.8 6 130TE L 7484.7 9 1- 0.876 EV 45 6.00E-5 31 130TE G 7484.7 9 130TE L 7536.9 11 1- 0.211 EV 48 1.41E-5 32 130TE G 7536.9 11 130TE L 7561.5 10 1- 0.536 EV 38 3.56E-5 25 130TE G 7561.5 10 130TE L 7577.5 11 1- 0.210 EV 46 1.38E-5 30 130TE G 7577.5 11 130TE L 7585.7 12 1- 0.386 EV 35 2.54E-5 23 130TE G 7585.7 12 130TE L 7597.8 12 1- 0.302 EV 34 1.98E-5 22 130TE G 7597.8 12 130TE L 7617.6 14 1- 0.239 EV 32 1.55E-5 21 130TE G 7617.6 14 130TE L 7661.0 12 1- 0.232 EV 62 1.5E-5 4 130TE G 7661.0 12 130TE L 7679.2 11 1- 0.575 EV 45 3.65E-5 29 130TE G 7679.2 11 130TE L 7688.9 11 1- 0.553 EV 44 3.49E-5 28 130TE G 7688.9 11 130TE L 7698.7 11 1- 0.457 EV 43 2.87E-5 27 130TE G 7698.7 11 130TE L 7713.9 14 1- 0.270 EV 50 1.69E-5 31 130TE G 7713.9 14 130TE L 7723.0 9 1- 1.089 EV 62 6.8E-5 4 130TE G 7723.0 9 130TE L 7734.7 11 1- 0.657 EV 45 4.07E-5 28 130TE G 7734.7 11 130TE L 7755.0 13 1- 0.386 EV 39 2.37E-5 24 130TE G 7755.0 13 130TE L 7775.8 23 1- 0.108 EV 36 0.66E-5 22 130TE G 7775.8 23 130TE L 7780.9 12 1- 0.248 EV 41 1.51E-5 25 130TE G 7780.9 12 130TE L 7793.2 11 1- 0.290 EV 40 1.76E-5 24 130TE G 7793.2 11 130TE L 7807.3 12 1- 0.194 EV 42 1.17E-5 25 130TE G 7807.3 12 130TE L 7816.5 18 1- 0.148 EV 35 0.89E-5 21 130TE G 7816.5 18 130TE L 7823.9 10 1- 0.222 EV 52 1.34E-5 32 130TE G 7823.9 10 130TE L 7838.7 12 1- 0.222 EV 46 1.32E-5 27 130TE G 7838.7 12 130TE L 7845.6 10 1- 0.401 EV 49 2.38E-5 29 130TE G 7845.6 10 130TE L 7856.8 9 1- 0.587 EV 49 3.47E-5 29 130TE G 7856.8 9 130TE L 7884.0 9 1- 0.106 EV 36 0.62E-5 21 130TE G 7884.0 9 130TE L 7897.5 10 1- 0.551 EV 49 3.21E-5 29 130TE G 7897.5 10 130TE L 7920.1 9 1- 0.609 EV 59 3.51E-5 34 130TE G 7920.1 9 130TE L 7929.6 10 1- 0.590 EV 60 3.39E-5 34 130TE G 7929.6 10 130TE L 7949.7 11 1- 0.532 EV 58 3.04E-5 33 130TE G 7949.7 11 130TE L 7965.2 12 1- 0.50 EV 11 2.9E-5 6 130TE G 7965.2 12 130TE L 7993.2 12 1- 0.244 EV 78 1.4E-5 4 130TE G 7993.2 12 130TE L 8004.6 14 1- 0.347 EV 67 1.9E-5 4 130TE G 8004.6 14 130TE L 8013.3 15 1- 0.293 EV 69 1.6E-5 4 130TE G 8013.3 15 130TE L 8022.2 14 1- 0.203 EV 64 1.1E-5 4 130TE G 8022.2 14 130TE L 8063.2 18 1- 0.183 EV 35 1.00E-5 19 130TE G 8063.2 18 130TE L 8109.1 15 1- 0.198 EV 34 1.06E-5 18 130TE G 8109.1 15 130TE L 8138.9 14 1- 0.158 EV 30 0.84E-5 16 130TE G 8138.9 14 130TE L 8158.8 15 1- 0.121 EV 28 0.64E-5 15 130TE G 8158.8 15 130TE L 8194.3 14 1- 0.126 EV 27 0.66E-5 14 130TE G 8194.3 14 130TE L 8206.1 14 1- 0.241 EV 34 1.25E-5 18 130TE G 8206.1 14 130TE L 8276.7 12 1- 0.316 EV 51 1.60E-5 26 130TE G 8276.7 12 130TE L 8298.6 21 1- 0.284 EV 58 1.43E-5 29 130TE G 8298.6 21 130TE L 8310.6 17 1- 0.186 EV 53 0.93E-5 26 130TE G 8310.6 17 130TE 130TE(P,P'G):DSAM:XUNDL-13 2022PR02 202212 130TE c Compiled (unevaluated) dataset from 2022Pr02: 130TE2c Phys Rev C 105, 034319 (2022) 130TE c Compiled by B. Singh (McMaster), October 26, 2022 130TE c 2022Pr02: E(p)=10 MeV beam from 10 MV FN-Tandem accelerator of the 130TE2c University of Cologne. Measured E|g, p|g-coin, |g(|q), level lifetimes 130TE3c by Doppler-shift attenuation method (DSAM) using SONIC@HORUS array of 130TE4c 12 passivated implanted planar silicon (PIPS) detectors for protons, 130TE5c and 14 HPGe detectors, six of which had BGO Compton suppressors, 130TE6c positioned at five different angles with respect to the beam direction. 130TE7c Target was 99.3% enriched {+130}Te, with aerial density of 0.5 mg/cm 130TE8c evaporated on 1.0 mg/cm Ta stopper foil. Deduced B(E2) and B(M1). 130TE9c Comparison with earlier measurements in literature, and with 130TEAc shell-model calculations. 130TE cG $B(E2) values listed here are in e{+2}b{+2} units. 2022Pr02 130TE2cG list these values in e{+2}fm{+2} units. B(M1) values are in 130TE3cG |m{+2}{-N} units. 130TE cG E,RI,M,MR$From {+130}Te Adopted Levels, Gammas in the ENSDF database 130TE2cG (May 2001 update), unless otherwise indicated. 130TE cG E(n)$New |g transition proposed by 2022Pr02; branching ratio is not 130TE2cG given by the authors. 130TE cL E,J$From {+130}Te Adopted Levels in the ENSDF database (May 2001 130TE2cL update), unless otherwise indicated 130TE cL T$From DSAM (2022Pr02). Literature mean lifetimes |t values from 130TE2cL DSAM in (n,n'|g) (2008Hi17) are listed in comments 130TE PN 6 130TE L 0.0 0+ 130TE L 839.49 1 2+ 2.30 PS 5 130TE cL T$from Adopted Levels 130TE G 839.49 2 100 E2 130TE L 1588.26 3 2+ 2.01 PS GT 130TE cL T$from DSAM in (n,n'|g) (2008Hi17) 130TE G 748.76 2 100 14 M1+E2 +0.65 15 130TE G 1588.19 8 1.6 3 E2 130TE L 1633.00 2 4+ 0.97 PS +26-19 130TE cL $Measured mean lifetime |t=1395 fs {I+342-237}(stat) {I+150-124}(syst) 130TE2cL from DSA for 794|g (2022Pr02). Deduced mean lifetime=1395 fs 130TE3cL {I+373-268} or T{-1/2}=967 fs {I+259-186}. 130TE G 793.53 2 100 E2 130TE2 G BE2=0.1859 +422-408 (2022Pr02) 130TE L 1815.336 25 (6)+ 130TE G 182.335 11 100 E2 130TE L 1885.70 3 2+ 196 FS +68-49 130TE cL $Measured mean lifetime |t=283 fs {I+93-65}(stat) {I+30-26}(syst) 130TE2cL from DSA for 1046|g (2022Pr02). Deduced mean lifetime=283 fs {I+98-70} 130TE3cL or T{-1/2}=196 fs {I+68-49}. Literature |t=470 fs {I+40-30} (2008Hi17) 130TE G 1046.21 2 100 14 M1+E2 -0.175 10 130TE2 G BE2=0.0067 +27-22 $ BM1=0.17 +6-5 (2022Pr02) 130TE G 1885.69 18 2.0 4 E2 130TE L 1964.76 4 (0+) 0.30 PS +18-10 130TE cL $Measured mean lifetime |t=439 fs {I+255-135}(stat) {I+46-42}(syst) 130TE2cL from DSA for 1125|g (2022Pr02). Deduced mean lifetime=439 fs 130TE3cL {I+259-141} or T{-1/2}=304 fs {I+180-98}. 130TE G 1125.26 3 100 [E2] 130TE2 G BE2=0.1030 +470-391 130TE L 1981.55 3 4+ 0.67 PS +15-12 130TE cL $Measured mean lifetime |t=960 fs {I+186-139}(stat) {I+99-89}(syst) 130TE2cL from DSA for 1142|g (2022Pr02). Deduced mean lifetime=960 fs 130TE3cL {I+211-165} or T{-1/2}=665 fs {I+146-114}. 130TE G 348.58 2 100 11 M1+E2 -0.12 3 0.0232 130TE G 1142.02 2 70 9 E2 130TE2 G BE2=0.0180 +45-43 (2022Pr02) 130TE L 2101.25 3 5- 130TE G 468.27 2 100 E1(+M2) +0.03 2 130TE L 2190.62 3 (2+) 399 FS +81-65 130TE cL $Measured mean lifetimes |t=523 fs {I+145-100}(stat) {I+55-48}(syst) 130TE2cL from DSA for 1351|g; 615 fs {I+151-107}(stat) {I+65-67}(syst) from DSA 130TE3cL for 2191|g, with weighted averaged |t=576 fs {I+100-78}(stat) 130TE4cL {I+61-53}(syst) (2022Pr02). Deduced averaged mean lifetime=576 fs 130TE5cL {I+117-94} or T{-1/2}=399 fs {I+81-65}. Literature |t=590 fs {I50} 130TE6cL (2008Hi17) 130TE G 1351.11 3 94 13(M1+E2) -0.27 2 130TE2 G BE2=0.0010 3 $ BM1=0.018 +5-4 (2022Pr02) 130TE G 2190.60 3 100 15(E2) 130TE2 G BE2=0.0014 4 (2022Pr02) 130TE L 2282.59 3 (2+) 59 FS +13-10 130TE cL $Measured mean lifetimes |t=90 fs {I+20-18}(stat) {I+9-8}(syst) 130TE2cL from DSA for 1443|g; 79 fs {I+24-20}(stat) {I+8-7}(syst) from DSA 130TE3cL for 2283|g, with weighted averaged |t=85 fs {I+15-13}(stat) 130TE4cL {I+9-8}(syst) (2022Pr02). Deduced averaged mean lifetime=85 fs 130TE5cL {I+18-15} or T{-1/2}=59 fs {I+13-10}. Literature |t=150 fs {I10} 130TE6cL (2008Hi17) 130TE G 1443.09 2 100 15(M1+E2) -0.10 2 130TE2 G BE2=0.0013 +4-3 $ BM1=0.18 5 (2022Pr02) 130TE G 2282.60 7 21 3 (E2) 130TE2 G BE2=0.0027 +8-7 (2022Pr02) 130TE L 2435.59 4 4- 130TE G 334.34 2 100 M1+E2 -0.052 7 0.0261 130TE L 2449.48 4 4+ 309 FS +56-46 130TE cL $Measured mean lifetime |t=446 fs {I+64-52}(stat) {I+48-40}(syst) 130TE2cL from DSA for 816|g (2022Pr02). Deduced mean lifetime=446 fs {I+80-66} 130TE3cL or T{-1/2}=309 fs {I+56-46}. 130TE G 816.48 3 100 8 M1+E2 -0.21 2 130TE2 G BE2=0.0206 +41-40 $ BM1=0.22 4 (2022Pr02) 130TE G 861.6 4 3.3 17 130TE L 2466.89 4 (2+) 403 FS +67-58 130TE cL $Measured mean lifetime |t=581 fs {I+76-63}(stat) {I+60-55}(syst) 130TE2cL from DSA for 1627|g (2022Pr02). Deduced mean lifetime=581 fs {I+97-84} 130TE3cL or T{-1/2}=403 fs {I+67-58}. 130TE G 1627.38 3 100 14 [E2] 130TE cG M$(M1+E2) in ENSDF, with |d=-0.48 {I4} or 1/|d=-0.02 {I3} 130TE G 2466.94 18 11 2 (E2) 130TE L 2527.06 3 3- 1.2 PS +14-5 130TE cL $Measured mean lifetime |t=1749 fs {I+2058-651}(stat) {I+184-162}(syst) 130TE2cL from DSA for 1688|g (2022Pr02). Deduced mean lifetime=1749 fs 130TE3cL {I+2066-671} or T{-1/2}=1212 fs {I+1432-465}. 130TE G 894.06 14 4.3 7 130TE G 1687.56 2 100 16 E1(+M2) +0.030 6 130TE L 2575.2 4 78 FS +92-48 130TE cL $Measured mean lifetime |t=112 fs {I+132-68}(stat) {I+12-10}(syst) 130TE2cL from DSA for 942|g (2022Pr02). Deduced mean lifetime=112 fs {I+133-69} 130TE3cL or T{-1/2}=78 fs {I+92-48}. 130TE G 942.2 4 100 [E2] 130TE2 G BE2=0.98 +152-54 (2022Pr02) 130TE cG M$E2 assumed in 2022Pr02 130TE L 2581.15 5 (2+) 193 FS +31-26 130TE cL $Measured mean lifetime |t=279 fs {I+33-28}(stat) {I+30-26}(syst) 130TE2cL from DSA for 1741|g (2022Pr02). Deduced mean lifetime=279 fs {I+45-38} 130TE3cL or T{-1/2}=193 fs {I+31-26}. 130TE G 992.95 13 12.1 19 130TE G 1741.64 4 100 15 M1+E2 +0.18 2 130TE cG M$D+Q in ENSDF database, M1+E2 assigned here 130TE L 2689.12 5 1 46 FS +22-18 130TE cL $Measured mean lifetime |t=66 fs {I+31-25}(stat) {I+6-6}(syst) 130TE2cL from DSA for 2689|g (2022Pr02). Deduced mean lifetime=66 fs {I+32-26} 130TE3cL or T{-1/2}=46 fs {I+22-18}. 130TE G 2689.09 5 100 130TE L 2743.14 4 1 76 FS +71-42 130TE cL $Measured mean lifetime |t=109 fs {I+102-59}(stat) {I+11-10}(syst) 130TE2cL from DSA for 2743|g (2022Pr02). Deduced mean lifetime=109 fs {I+103-60} 130TE3cL or T{-1/2}=76 fs {I+71-42}. 130TE G 2743.11 4 100 130TE L 2744.97 4 (2+,3) 471 FS +64-57 130TE cL $Measured mean lifetimes |t=811 fs {I+283-177}(stat) {I+83-74}(syst) 130TE2cL from DSA for 859|g; 664 fs {I+63-55}(stat) {I+68-60}(syst) from DSA 130TE3cL for 1905|g, with weighted averaged |t=679 fs {I+61-53}(stat) 130TE4cL {I+69-62}(syst) (2022Pr02). Deduced averaged mean lifetime=679 fs 130TE5cL {I+92-82} or T{-1/2}=471 fs {I+64-57}. 130TE G 309.1 5 n 130TE G 462.0 5 n 130TE G 553.6 5 n 130TE G 859.30 4 91 13 130TE G 1112.01 9 29 4 130TE G 1905.43 4 100 14 130TE L 2765.26 22 (4+) 36 FS LT 130TE cL $Measured mean lifetime |t<52 fs from DSA for 1177|g (2022Pr02). 130TE G 481.6 5 n 130TE G 949.8 4 46 9 130TE G 1131.9 4 59 14 130TE G 1177.3 4 100 10 [E2] 130TE2 G BE2>0.3059 (2022Pr02) 130TE G 1925.7 8 18 9 130TE L 2789.26 5 205 FS +42-34 130TE cL $Measured mean lifetimes |t=165 fs {I+159-79}(stat) {I+18-15}(syst) 130TE2cL from DSA for 1156|g; 307 fs {I+55-44}(stat) {I+33-28}(syst) from DSA 130TE3cL for 1950|g, with weighted averaged |t=296 fs {I+51-41}(stat) 130TE4cL {I+32-27}(syst) (2022Pr02). Deduced averaged mean lifetime=296 fs 130TE5cL {I+60-49} or T{-1/2}=205 fs {I+42-34}. 130TE G 1156.21 14 25 4 [E2] 130TE2 G BE2=0.0267 +51-47 (2022Pr02) 130TE cG M$E2 assumed in 2022Pr02 130TE G 1949.76 5 100 14 130TE L 3177.0 20 (3-,4+) 130TE cL E$from 2022Pr02. Other: 3180 {I20} in ENSDF from (|a,|a') 130TE cL J$tentative assignment in 2022Pr02 130TE G 1075.3 2 n 130TE G 1290.6 1 n 130TE L 3194.0 10 (1,2+) 130TE cL E$from 2022Pr02. Other: 3180 {I20} in ENSDF from (|a,|a') 130TE cL J$tentative assignment in 2022Pr02 130TE G 3193.7 4 n 130TE L 3364.1 5 3- 173 FS +22-17 130TE cL $Measured mean lifetime |t=250 fs {I+13-12}(stat) {I+28-22}(syst) 130TE2cL from DSA for 1478|g (2022Pr02). Deduced mean lifetime=250 fs {I+31-25} 130TE3cL or T{-1/2}=173 fs {I+22-17}. 130TE cL E$from 2022Pr02. Other: 3360 {I10} in ENSDF from (p,p') 130TE G 619.2 1 n 130TE G 1081.0 3 n 130TE G 1173.5 1 n 130TE G 1262.3 2 n 130TE G 1382.6 2 n 130TE G 1478.4 1 130TE G 1776.2 1 n 130TE L 3567.7 3 (1,2) 14 FS LT 130TE cL $Measured mean lifetime |t<20 fs from DSA for 3568|g (2022Pr02) 130TE G 2728 25 LT 130TE G 3567.6 3 100 130TE 130TE 2B- HALF-LIFE:XUNDL-14 2023AD01,2022AD14 202302 130TE c Compiled (unevaluated) dataset from 2023Ad01: 130TE c Nuova Cim C 46, 7 (2023). 130TE c Also from 2022Ad14: 130TE c Nature 604, 53 (2022) 130TE c Compiled by G. G~urdal, Dec 23, 2022 130TE c 2023Ad01: measurement of half-life limit for the 0|n|b|b decay mode 130TE2c of {+130}Te using CUORE (Cryogenic Underground Observatory for Rare 130TE3c Events) bolometric detector apparatus located at the underground 130TE4c Laboratori Nazionali del Gran Sasso (LNGS) in Italy. The CUORE 130TE5c consists of 988 5|*5|*5 cm{+3} natural crystals of TeO{-2}, arranged 130TE6c in 19 towers packed inside a multistage cryogen-free cryostat. 15 130TE7c tons of material was cooled down below 4K (3 tons of which below 130TE8c 5mK). A cryogenics sensor which is Neutron Doped Transmutation 130TE9c germanium (NTD-Ge) thermistor, connected to each crystal to convert 130TEac the thermal photons into electrical signals. 1 ton|*yr data of 130TEbc |J1800kg|*yr of exposure have been analysed. The callibration data 130TEcc were taken using an external {+232}Th-{+60}Co source. Measured energy 130TEdc spectrum with a range of interest between 2490 keV and 2570 keV. 130TEec Deduced lower limit of T{-1/2} and corresponding upper limit of the 130TEfc Majorana neutrino mass. 130TE c No events were observed for 0|n|b|b decay mode, close to the Q{-|b|b} 130TE2c window of 2527.51 keV {I1} (2017Wa10: AME-2016) corresponding to 130TE3c {+130}Te g.s. {+130}Xe g.s. |b|b transition, thus providing no 130TE4c evidence for 0|n|b|b decay of {+130}Te. 130TE L 0 0+ 2.2E+25 Y GT 130TE cL T$this value is for 0|n|b|b decay mode at 90% credibility interval 130TE2cL (C.I.), and was derived using Bayesian analysis. The authors also 130TE3cL reported the same half-life limit at an earlier publication 130TE4cL (2022Ad14). 130TE cL $Corresponding upper limit of Majorana neutrino mass 130TE2cL m{-|b|b}<0.090-0.305 eV. s 130TE 130TE 2B- HALF-LIFE:XUNDL-16 2019CA21 202310 130TE c Compiled (unevaluated) dataset from 2019Ca21: Universe 130TE2c 5, 10 (2019) 130TE c Compiled by E.A. McCutchan (NNDC,BNL) October 26, 2023 130TE c 2019Ca21: measurement of half-life limit for the 2|n|b|b decay mode 130TE2c of {+130}Te using CUORE (Cryogenic Underground Observatory for Rare 130TE3c Events) bolometric detector apparatus located at the underground 130TE4c Laboratori Nazionali del Gran Sasso (LNGS) in Italy. CUORE 130TE5c consists of 988 5|*5|*5 cm{+3} natural crystals of TeO{-2}, arranged 130TE6c in 19 towers packed inside a multistage cryogen-free cryostat. 15 130TE7c tons of material was cooled down below 4K (3 tons of which below 130TE8c 5mK). A cryogenics sensor which is Neutron Doped Transmutation 130TE9c germanium (NTD-Ge) thermistor, connected to each crystal to convert 130TEac the thermal photons into electrical signals. Total exposure of 130TEbc 86.3 kg/r. 130TEcc Measured energy 130TEdc spectrum; 130TEec Deduced of T{-1/2} 2|n|b|b decay and limit for 0|n|b|b decay. 130TE L 0 0+ 7.9E20 Y 2 130TE cL T$this value is for 2|n|b|b decay mode and reported as 130TE2cL 7.9|*10{+20} y {I1} (stat) {I2} (syst) (2019Ca21). Authors 130TE3cL also report limit for 0|n|b|b decay mode as 130TE4cL T{-1/2} > 1.3|*10{+25} y at 90% C.L. (2019Ca21) 130TE 130TE 2B-:T1/2:XUNDL-17 2020AD04 202403 130TE c Compiled (unevaluated) dataset from 2020Ad04 130TE c Phys. Rev. Lett. 124, 122501 (2020) 130TE c Compiled by E.A. McCutchan (NNDC,BNL) February 25, 2024 130TE c The cryogenic calorimeteric detector located underground at the 130TE2c Laboratori Nazionali del Gran Sasso was used to search for the 130TE3c 0|n|b|b decay of {+130}Te (CUORE experiment). The detector consists 130TE4c of {+nat}TeO{-2} crystals arranged into 19 towers of 13 floors with 4 130TE5c crystals per floor (988 crystals in total). 130TE6c Total mass of TeO{-2} in the detector is 750 kg 130TE7c corresponding to 206 kg of {+130}Te. 130TE8c This setup allows to have the 130TE9c {+130}Te |b|b emitters within the detector absorber itself. The 130TEac detector's average energy resolution in the run was 7.7 {I5} keV 130TEbc (FWHM) at 2527 keV (=Q{-|b|b}). The events corresponding to 0|n|b|b 130TEcc decay were looked for after applying basic quality cuts, rejection of 130TEdc spurious signals by pulse shape analysis and anti-coincidence 130TEec selections to the raw data. As of the publication date (372.5 130TEfc kg(TeO{-2}) year exposure), no evidence was found for the 0|n|b|b 130TEgc decay of {+130}Te, and the lower limit of T{-1/2} and the upper limit 130TEhc of the effective Majorana neutrino mass ({Im}{-|b|b}) were deduced. 130TE L 0.0 0+ 3.2E25 Y GT 130TE cL T$For 0|n|b|b from 2020Ad04 with a 90% C.L. 130TE 130TE:2B-:T1/2:XUNDL-7 2016EB03 201612 130TE c Compiled (unevaluated) dataset from 2016Eb03: Phys. Rev. C 94, 024603 130TE2c (2016) 130TE c Compiled by G. G~urdal (Millsaps College), October 1, 2016 130TE c The COBRA demonstrator located at the Laboratori Nazionali del Gran 130TE2c Sasso was used to search for the 0|n|b|b decay of {+130}Te. The COBRA 130TE3c demonstrator consisted of 64 CdZnTe coplanar-grid semiconductor 130TE4c detectors arranged in four layers of 4|*4 detectors. Each detector 130TE5c had a mass of 5.9 g. The detectors were supported by a 130TE6c polyoxymethylene frame installed in a support structure made of 130TE7c electroformed copper. The detectors were constantly flushed with 130TE8c evaporated nitrogen to suppress radon-induced background and shielded 130TE9c by ultralow-activity and standard lead. To reduce the neutron flux, a 130TEac 5-cm borated polyethylene layer was used. After the data-quality 130TEbc selection and the applied energy thresholds, the data corresponding 130TEcc to an exposure of 216.1 kg d were analyzed. The effective FWHM for 130TEdc the full demonstrator was measured as 15 keV at 238 keV and 30 keV at 130TEec 2.6 MeV by modeling the |g-peaks of the calibration sources using 130TEfc double-Gaussian functions. The average detection efficiency of the 130TEgc COBRA detector array was determined as 89 % {I1}. Measured energy 130TEhc deposited into detectors. Deduced lower limit of T{-1/2} using 130TEic Bayesian analysis. No identification for 0|n|b|b decay has been found. 130TE L 0.0 0+ 6.1E21 Y GT 130TE cL T$From 2016Eb03 with a 90 % C.L. The authors stated that switching to 130TE2cL a prior uniform effective neutrino Majorana mass increased the limits 130TE3cL on the T{-1/2}. 130TE 130TE 2B-:T1/2:XUNDL-18 2025AD05 202509 130TE c Compiled (unevaluated) dataset from 2025Ad05 130TE c Phys. Rev. Lett. 135, 082501 (2025) 130TE c Compiled by E.A. McCutchan (NNDC,BNL) September 4, 2025 130TE c The cryogenic calorimeteric detector located underground at the 130TE2c Laboratori Nazionali del Gran Sasso was used to measure 130TE3c 2|n|b|b decay of {+130}Te (CUORE experiment). The detector consists 130TE4c of {+nat}TeO{-2} crystals arranged into 19 towers of 13 floors with 4 130TE5c crystals per floor (988 crystals in total). 130TE6c Total mass of TeO{-2} in the detector is 750 kg 130TE7c corresponding to 206 kg of {+130}Te. 130TE8c This new measurement used first complete model of CUORE data, 130TE9c based on 1038 kg yr of collected exposure. 130TEac Precise determination of T{-1/2} and measurement of shape of 130TEbc |b spectrum. 130TE L 0.0 0+ 9.32E20 Y +9-8 130TE cL T$for 2|n|b|b with a 90% C.L. (2025Ad05). 130TE2cL Value is reported as 9.32 |*10{+20} y {I+5-4} (stat) {I7} (syst), 130TE3cL uncertainty combined in quadrature by compiler.