94PD 9BE(107AG,XG):XUNDL-6 2009GA40 201003 94PD c Compiled (unevaluated) dataset from 2009Ga40: 94PD2c Phys Rev C 80, 064303 (2009). 94PD c Compiled by A. MacDonald and B. Singh (McMaster); March 8, 2010. 94PD c {+107}Ag beam produced at E=750 MeV/nucleon by the SIS-18 Synchrotron 94PD2c at GSI. Reaction products were separated by the Fragment Separator 94PD3c (FRS). |g's were measured by the Rare Isotope Spectroscopic 94PD4c INvestigation (RISING) array, consisting of 105 hyperpure germanium 94PD5c detectors. Measured E|g,I|g, isomeric ratio, half-lives. Deduced 94PD6c levels, J, |p. 94PD c Level scheme is from Adopted dataset for {+94}Pd in ENSDF database. 94PD2c The |g-ray energies are from spectral figure 3 in 2009Ga40 94PD cL $The isomeric ratio is defined as R=N{-isomer}/(N{-ions}(fragment)|g), 94PD2cL N{-isomer}=number of ions observed in the isomeric state, 94PD3cL N{-ions}=total number of ions of that nuclear species, 94PD4cL F=correction factor for in-flight losses, g=correction factor 94PD5cL for finite measuring time period 94PD L 0 94PD L 814 2+ 94PD G 814 94PD L 1719 (4+) 94PD G 905 94PD L 2379 (6+) 94PD G 660 94PD L 2703 (8+) 94PD G 324 94PD L 3795 (10+) 94PD G 1092 94PD L 4788 (12+) 94PD G 993 94PD L 4884 (14+) 468 NS 19 94PD cL T$ measured in 2009Ga40. 94PD cL $ R=28 {I5} 94PD G 96 94PD 9BE(124XE,XG):XUNDL-7 2011BR01 201105 94PD c Compiled (unevaluated) dataset from 2011Br01: 94PD2c Phys Rev C 82, 061309(R) (2010) 94PD c Compiled by J. Chen and B. Singh (McMaster); Jan 14, 2011 94PD c Edited by B. Singh, May 17, 2011: 2010Br01 changed to 2011Br01. 94PD d Note that 2011Br01 in NSR database was incorrectly assigned to an 94PD2d article in 2010, but the NSR keynumbers once assigned, apparently, 94PD3d cannot be retracted 94PD c E=850 MeV/nucleon {+124}Xe beam produced from the SIS synchrotron at 94PD2c GSI and incident on a 4 g/cm{+2} {+9}Be target. Fragments separated by 94PD3c the Fragment Separator(FRS) and stopped by a stopper of nine double 94PD4c sided silicon strip detectors (DSSSD) surrounded by the RISING array 94PD5c of 105 Ge detectors for detecting |g-rays. Measured E|g, I|g, 94PD6c |g|g, ({+94}Pd ions)|g coin, isomer half-lives. Identified a 94PD7c high-spin isomeric state at 7212 keV. Comparison with shell-model 94PD8c calculations 94PD cL J$ 2011Br01 quote from previous work, except for the 7212 level. 94PD2cL The assignments are the same in Adopted Levels for {+94}Pd in ENSDF 94PD3cL database, except that most of these are given in parentheses 94PD cL E(A)$ Level shown in level-scheme figure 4 of 2011Br01, but no |g 94PD2cL transition from this level listed 94PD PN 7 94PD L 0 0+ 94PD L 814 2+ 94PD G 814 94PD L 1720 4+ 94PD G 906 94PD L 2380 6+ 94PD G 660 94PD L 2538 (5-) A 94PD L 2699 (6+) A 94PD L 2704 8+ 94PD G 324 94PD L 3051 (8+) 94PD G 347 94PD L 3065 (6+) A 94PD L 3796 10+ 94PD G 745 9 1 94PD cG RI$ from comparison of the intensities of the 347 and 745 keV peaks 94PD2cG to that of the 1092 keV peak. 94PD G 1092 91 1 94PD cG RI$ 100-branching for 745|g 94PD L 4790 12+ 94PD G 994 94PD L 4886 14+ 499 NS 13 94PD cL T$ from time distribution of |g rays below the 14+ isomer 94PD2cL (2011Br01) using ROOT implementation of MINUIT 94PD2cL computer code and one exponential fit.. 94PD G 96 100 E2 1.62 7 94PD cG RI$ 2011Br01 quote 100 including internal conversion, but the 94PD2cG compilers give it as photon intensity while giving the total 94PD3cG conversion coefficient 94PD2 G ECC=1.7 1 (2011Br01) 94PDB G BE2W=2.09 14 94PD cG $B(E2)(W.u.) deduced by the compilers, 2011Br01 give 2.1 {I1} 94PD L 5294 (15+) 94PD G 408 94PD L 5561 (16+) 94PD G 267 94PD L 7106 (18+) 94PD G 1545 94PD L 7212 (19-) 197 NS 22 94PD cL J$tentative assignment based on Weisskopf estimates 94PD cL T$ from time distribution of 1651|g using ROOT implementation of MINUIT 94PD2cL computer code (2011Br01). 94PD cL $Dominant configuration=|p[(p{-1/2}{+-1}g{-9/2}{+-3})]{-11}~# 94PD2cL |n[g{-9/2}{+-2}]{-8} 94PD G 106 18 4 E1 0.129 4 94PD cG RI$ 2011Br01 quote 20 {I4} including internal conversion, but the 94PD2cG compilers give it as photon intensity while giving the total 94PD3cG conversion coefficient 94PDB G BE1W=2.5E-7 7 94PD cG $B(E1)(W.u.) deduced by the compilers, 2011Br01 give 3|*10{+-7} {I1} 94PD G 1651 82 4 E3 94PD cG RI$ 80 {I4} adjusted to 82 {I4} by the compilers so that the 94PD2cG total photon intensities from the 7212 level adds to 100 94PDB G BE3W=0.28 4 94PD L 7703 (20+) A 94PD 9BE(124XE,XG):XUNDL-8 2017PA35 201712 94PD c Compiled (unevaluated) dataset from 2017Pa35: 94PD2c Phys Rev C 96, 044311 (2017) 94PD c Compiled by Y. Ichikawa (RIKEN) and F.G. Kondev (ANL); 94PD2c November 9, 2017 94PD c 2017Pa35: The {+94}Pd nucleus was produced by fragmentation reaction 94PD2c using {+124}Xe beam at E=345 MeV/nucleon incident on a 740 mg/cm{+2} 94PD3c thick {+9}Be target at the RIKEN-RIBF facility. The identification of 94PD4c the nuclide of interest was made through the BigRIPS separator and the 94PD5c ZeroDegree spectrometer by determining the atomic number and the 94PD6c mass-to-charge ratio of the ion using the tof-B|r-|DE method. The 94PD7c secondary beam was stopped in the double-sided silicon strip detector 94PD8c of the WAS3ABi spectrometer. The |g rays were detected by EURICA array 94PD9c comprising of 84 HP Ge detectors. Measured: E|g, I|g and T{-1/2}. 94PD D ------------------------------------------------------ 94PD cL E$From least-squares fit to E|g. 94PD cL J,T$From adopted levels in ENSDF, unless otherwise stated 94PD cG E,RI,M$From adopted gammas in ENSDF, unless otherwise stated 94PD L 0 0+ 94PD L 813.80 102+ 94PD G 813.8 1 100 94PD L 1719.11 15(4+) 94PD G 905.3 1 100 94PD L 2378.21 18(6+) 94PD G 659.1 1 100 94PD L 2702.21 20(8+) 94PD G 324.0 1 100 94PD L 3049.21 23(8+) 94PD G 347.0 1 100 94PD L 3794.12 23(10+) 94PD G 745 94PD G 1091.9 1 100 94PD L 4787.6 3(12+) 94PD G 993.5 2 100 94PD L 4883.2 4(14+) 495 NS 7 94PD cL E$Isomeric ratio R=30 % {I1} (2017Pa35) 94PD cL T$From |g(t) in 2017Pa35, but the gating |g-ray transitions were not 94PD2cL given by the authors 94PD G 95.6 2 100 E2 1.64 3 94PD cG $B(E2)(W.u.)=2.14 {I5} (by compilers) 94PD L 5291.4 5(15+) 94PD G 408.2 2 100 94PD L 5559.0 5(16+) 94PD G 267.6 2 100 94PD L 7103.6 6(18+) 94PD G 1544.5 3 100 94PD L 7209.8 9(19-) 225 NS 32 94PD cL E$Isomeric ratio R=6.8 % {I29} (2017Pa35) 94PD cL J$From 2011Br11 94PD cL T$From |g(t) in 2017Pa35, but the gating |g-ray transitions were not 94PD2cL given by the authors 94PD G 106 1 23 5 [E1] 0.129 4 94PD cG E$From 2017Pa35, but the uncertainty is assigned by the compilers 94PD cG RI$From reported I(|g+ce) in 2017Pa35 and |a (by compilers) 94PD cG $B(E1)(W.u.)=2.2|*10{+-7} {I5} (by compilers) 94PD G 1651 1 100 5 [E3] 7.00E-4 94PD cG E$From 2017Pa35, but the uncertainty is assigned by the compilers 94PD cG RI$From reported I(|g+ce) in 2017Pa35 and |a (by compilers) 94PD cG $B(E3)(W.u.)=0.24 {I4} (by compilers) 94PD 9BE(124XE,XG):T1/2,B+P:XUNDL-92019PA16 202006 94PD c Compiled (unevaluated) dataset from 2019Pa16: 94PD2c Phys Rev C 99, 034313 (2019) 94PD c Compiled by E.A. McCutchan (NNDC,BNL) August 16, 2019 94PD c {+94}Pd produced from fragmentation of a {+124}Xe beam at E=345 94PD2c MeV/nucleon on a 740 mg/cm{+2} {+9}Be target at RIKEN, Japan. 94PD3c Fragments separated by B|r-|DE-B|r method in the first stages 94PD4c of BigRIPS and then B|r-tof-B|r measurements using later stage of 94PD5c BigRIPS and the ZeroDegree spectrometer. Ions were implanted in 94PD6c WAS3ABi consisting of three double-sided silicon strip detectors 94PD7c and ten single-sided silicon strip detectors. Gamma rays were 94PD8c detected using the Euroball-RIKEN Cluster Array (EURICA) consisting 94PD9c of 84 HPGe crystals arranged in 12 clusters. 94PDac Measured E|g, I|g, |b spectra, E(p), I(p), |b|g-coin, |bp-coin, 94PDbc |g|bp-coin, half-life, |b-delayed proton emission probability. 94PD L 0.0 0+ 9.1 S 4 94PD2 L %B+P LT 0.13 (2019Pa16) 94PD cL T$from implant-|b(t) using 94PD2cL multiparameter fit 94PD3cL to total decay time distribution with a Bateman equation (2019Pa16). 94PD cL %B+P$from the number of |bp events divided by the total number of 94PD2cL decays as determined from the T{-1/2} analysis (2019Pa16). 94PD 9BE(124XE,XG):XUNDL-10 2019HA26 202404 94PD c Compiled (unevaluated) dataset from 2019Ha26: 94PD2c Phys Rev C 100, 024302 (2019) 94PD c Compiled by E.A. McCutchan (NNDC,BNL) February 21, 2024 94PD c {+94}Pd nucleus was produced in fragmentation of a 94PD2c {+124}Xe beam at E=345 MeV/nucleon incident on a 4-mm 94PD3c thick {+9}Be target at the RIKEN-RIBF facility. Identification of 94PD4c the nuclei of interest was made through the BigRIPS separator and the 94PD5c ZeroDegree spectrometer. The secondary ions were implanted into 94PD6c modified SIMBA active stopper detector. 94PD7c |g rays were measured by EURICA array 94PD8c consisting of 84 HP Ge detectors. Measured: E|g, I|g and T{-1/2}. 94PD L 0 0+ 94PD L 814 2+ 94PD G 814 94PD L 1719 (4+) 94PD G 905 94PD L 2378 (6+) 94PD G 659 94PD L 2702 (8+) 94PD G 324 94PD L 3049 (8+) 94PD G 347 94PD L 3794 (10+) 94PD G 745 94PD G 1092 94PD L 4788 (12+) 94PD G 994 94PD L 4883 (14+) 515 NS 1 94PD cL T$From 95|g(t) (2019Ha26) 94PD G 95 94PD L 5291 (15+) 94PD G 408 94PD L 5559 (16+) 94PD G 268 94PD L 7104 (18+) 94PD G 1544 94PD L 7210 (19-) 230 NS 20 94PD cL T$From 106|g(t) (2019Ha26) 94PD G 106 94PD BE(124XE,XG):XUNDL-11 2024YA19 202503 94PD c Compiled (unevaluated) dataset from 2024Ya19: Phys Lett B 855 {I138805} 94PD2c (2024) 94PD c Compiled by V. Cheung (LLNL) on January 24, 2025 94PD c E=982 MeV/nucleon {+124}Xe beam produced from the SIS18 synchrotron 94PD2c at GSI and incident on a 4 g/cm{+2} {+9}Be target. Fragments 94PD3c separated by the Fragment Separator (FRS). The |g rays emitted in the 94PD4c deexcitation of the 14{++} isomeric state in {+94}Pd were registered 94PD5c in FATIMA using 6 triple cluster HPGe (GALILEO) and 36 LaBr{-3}(Ce) 94PD6c detectors. Measured E|g and isomer half-lives. Compared B(E2)with 94PD7c shell-model calculations. 94PD DG CC$FROM BrIcc v2.3e (17-Jun-2020) 2008Ki07, "Frozen Orbitals" appr. 94PD L 0 0 94PD L 814 (2+) 94PD G 814 (E2) 1.63E-32 94PDS G KC=0.001421 20$LC=0.0001705 24$MC=3.20E-5 4$NC=5.36E-6 8 94PD L 1719 (4+) 94PD G 905 (E2) 1.27E-32 94PDS G KC=0.001105 15$LC=0.0001314 18$MC=2.463E-5 34$NC=4.13E-6 6 94PD L 2379 (6+) 40 PS LT 94PD cL T$from direct 324|g and 660|g coincidences and indirect 324|g and 94PD2cL 818|g coincidences 94PD G 660 (E2) 0.002774 94PDS G KC=0.002410 34$LC=0.000295 4$MC=5.55E-5 8$NC=9.27E-6 13 94PDB G BE2W GT 4.4 94PD L 2703 (8+) 7.6E2 PS 11 94PD cL T$from direct 1092|g and 324|g coincidences and indirect coincidences 94PD2cL of 1092|g and 660 |g, 994|g and 324|g, 994|g and 660|g, 994|g and 94PD3cL 905|g, 96|g and 324|g, 96|g and 660|g, 96|g and 905|g, 96|g and 814|g. 94PD G 324 (E2) 0.0229532 94PDS G KC=0.01965 28$LC=0.00270 4$MC=0.000511 7$NC=8.39E-5 12 94PDB G BE2W=8.03 17 94PD L 3795 (10+) 94PD G 1092 (E2) 8.28E-412 94PDS G KC=0.000724 10$LC=8.49E-5 12$MC=1.591E-5 22$NC=2.67E-6 4 94PD L 4789 (12+) 94PD G 994 (E2) 1.02E-31 94PDS G KC=0.000892 12$LC=0.0001052 15$MC=1.972E-5 28$NC=3.31E-6 5 94PD L 4884 (14+) 515 NS 1 94PD cL T$taken from 2019Ha26 94PD G 96 (E2) 1.616 23 94PDS G KC=1.238 17$LC=0.309 4$MC=0.0597 8$NC=0.00931 13 94PDB G BE2W=2.03 11 94PD 9BE(124XE,XG):XUNDL-12 2025AP05 202510 94PD c Compiled (unevaluated) dataset from 2025Ap05: 94PD2c Phys. Rev. C 112, 034310 (2025) 94PD c Compiled by E.A. McCutchan (NNDC,BNL) October 14, 2025 94PD c {+94}Pd produced from fragmentation of a {+124}Xe beam at E=345 94PD2c MeV/nucleon on a 740 mg/cm{+2} {+9}Be target at RIKEN, Japan. 94PD3c Fragments separated by BigRIPS separator 94PD4c and then |DE-B|r-tof measurements using 94PD5c plastic scintillators and MUSIC. Ions implanted into 94PD6c AIDA an array of six DSSDs. 94PD7c Gamma rays were detected 94PD8c using the Decay Total Absorption Spectrometer (DTAS) 94PD9c consisting of 16 NaI detectors. 94PDac Measured E|g, I|g, |b spectra, E(p), I(p), |b|g-coin, |bp-coin, 94PDbc |g|bp-coin, half-life, |b-delayed proton emission probability. 94PD L 0.0 0+ 9.0 S 2 94PD2 L %B+P=0.3 1 (2025Ap05) 94PD cL T$weighted average of 9.0 s {I2} from implant-|b(t) and 9 s {I3} 94PD2cL from implant-|bp(t); both analyses used multiparameter fits 94PD3cL to total decay time distribution with a Bateman equation (2025Ap05). 94PD cL %B+P$from the number of |bp events divided by the total number of 94PD2cL decays as determined from the T{-1/2} analysis (2025Ap05).