67AS 40CA(32S,APG):XUNDL-2 2009OR02 200907 67AS c Compiled (unevaluated) dataset from 2009Or02: 67AS2c Phys Rev Lett 103, 052501 (2009). 67AS c Compiled by A. MacDonald and B. Singh (McMaster); July 30, 2009. 67AS c {+32}S beam produced at E=90 MeV by the ATLAS accelerator at Argonne 67AS2c National Lab. |g spectra were measured using the Gammasphere array, 67AS3c consisting of 77 HPGe detectors. Evaporated particles were detected 67AS4c by the Microball array and the 30-element liquid-scintillator neutron 67AS5c shell. Half-lives were determined from measurements of the centroid 67AS6c shifts of the relative-time spectra. Measured E|g, I|g, |g|g-coin, 67AS7c half-lives, angular distributions. Deduced levels, J, |p, B(E1), B(M2). 67AS cG $ ADO=I{-|g}(162.7|')/I{-|g}(90|') 67AS cL E$ From least-squares fit to E|g's (by compilers), assuming uncertainty 67AS2cL of 1 keV for each |g ray 67AS cL $ No evidence was found by 2009Or02 for a 12-ns isomer reported in 67AS2cL 2001Je10: Phys Rev C64, 064311 (2001) 67AS CL BAND(A)$ Band based on 9/2+ 67AS CL BAND(a)$ Band based on 11/2+ 67AS PN 7 67AS L 0 5/2- 67AS L 69.0 13 3/2- 67AS L 697.0 8 7/2- 67AS G 697 67AS L 1103.0 8 7/2- 67AS G 1034 67AS G 1103 67AS L 1422.0 7 9/2+ 0.49 NS 14 A 67AS cL T$ half-life measured by 2009Or02 67AS G 319 30 1 E1(+M2) +0.05 +10-14 67AS cG $ ADO=0.50 {I11} 67AS2 G BE1=8.3E-8 +24-25 67AS2 G BM2=0.3 +21-3 67AS G 725 59 2 E1+M2 -0.16 +8-13 67AS cG $ ADO=0.28 {I4} 67AS2 G BE1=1.4E-8 4 67AS2 G BM2=0.08 +16-6 67AS G 1422 12 2 M2 67AS cG $ ADO=1.1 {I6} 67AS2 G BM2=0.022 7 67AS L 2281.0 11 11/2+ a 67AS G 859 67AS L 2364.0 11 13/2+ A 67AS G 942 67AS L 3179.0 12 13/2+ a 67AS G 815 67AS G 898 67AS L 3591.0 14 17/2+ A 67AS G 1227 67AS L 3882.0 13 15/2+ a 67AS G 703 67AS G 1518 67AS L 4520.0 14 19/2+ a 67AS G 638 67AS G 929 67AS L 4948.0 15 21/2+ A 67AS G 428 67AS G 1357 67AS L 5721.0 19 25/2+ A 67AS G 773 67AS L 6704.1 21 29/2+ A 67AS G 983 67AS 9BE(67AS,67AS'G):XUNDL-3 2013CO23 201410 67AS c Compiled (unevaluated) data set from 2013Co23: 67AS2c Phys Rev C 88, 044311 (2013) 67AS c Compiled by C. Smith (ORNL/UTK) and C. D. Nesaraja (ORNL), 67AS2c October 10, 2014 67AS d Edited by B. Singh (McMaster), Oct 10, 2014 67AS c Inelastic scattering experiment. 67AS c Beam and target: {+67}As at 70 MeV/nucleon produced by fragmentation 67AS2c of {+78}Kr primary beam at 150 MeV/nucleon on 329 mg/cm{+2} thick 67AS3c {+9}Be production target at the NSCL-MSU facility. The secondary beam 67AS4c of {+67}As impinged a 188 mg/cm{+2} thick secondary {+9}Be target. 67AS c Experimental arrangement: the target were placed at the pivot point of 67AS2c the S800 spectrometer and surrounded by the SeGA array composed of 67AS3c 17 HPGe segmented detectors positioned at 20cm from the target and 67AS4c arranged in a configuration of two rings in a cylindrical symmetry 67AS5c around the beam axis: seven detectors at 37|' in the forward direction 67AS6c and ten detectors at 90|' relative to the beam axis. Incoming particle 67AS7c identification was performed by a time-of-flight measurement between 67AS8c two plastic scintillators located at the image point of the A1900 67AS9c fragment separator and at the object point of the S800 magnetic 67ASAc spectrometer. Outgoing particles were identified via a correlation 67AScc of |DE in the ionization chamber at the focal plane of the S800 67ASdc spectrometer and A/q from the time-of-flight measurements between 67ASec scintillators at the object point and at the focal plane of S800. 67AS c Measured: E|g, ({+67}As)|g coincidence. Deduced levels 67AS c Theory: comparison of measured low lying levels with theoretical values 67AS2c via shell model calculations with JUN45 interaction, and via beyond 67AS3c mean-field calculations using five-dimensional collective Hamiltonian 67AS4c (5DCH) method with the Gogny D1S interaction. 67AS G 639 6 67AS G 862 6 67AS G 942 6 67AS L 0 5/2- 67AS L 720 6 (7/2-) 67AS G 720 6 67AS L 1242 9 (9/2-) 67AS G 1242 9 67AS COULOMB EXCITATION:XUNDL-4 2013CO23 201410 67AS c Compiled (unevaluated) data set from 2013Co23: 67AS2c Phys Rev C 88, 044311 (2013) 67AS c Compiled by C. Smith (ORNL/UTK) and C. D. Nesaraja (ORNL), 67AS2c October 10, 2014 67AS c Edited by B. Singh (McMaster), Oct 10, 2014 67AS c Beam={+67}As, target={+197}Au 67AS c Beam and target: {+67}As at 70 MeV/nucleon produced by fragmentation 67AS2c of {+78}Kr primary beam at 150 MeV/nucleon on 329 mg/cm{+2} thick 67AS3c {+9}Be production target at the NSCL-MSU facility. The secondary beam 67AS4c of {+67}As impinged a 257 mg/cm{+2} thick {+197}Au target. 67AS c Experimental arrangement: the target were placed at the pivot point of 67AS2c the S800 spectrometer and surrounded by the SeGA array composed of 67AS3c 17 HPGe segmented detectors positioned at 20cm from the target and 67AS4c arranged in a configuration of two rings in a cylindrical symmetry 67AS5c around the beam axis: seven detectors at 37|' in the forward direction 67AS6c and ten detectors at 90|' relative to the beam axis. Incoming particle 67AS7c identification was performed by a time-of-flight measurement between 67AS8c two plastic scintillators located at the image point of the A1900 67AS9c fragment separator and at the object point of the S800 magnetic 67ASAc spectrometer. Outgoing particles were identified via a correlation 67AScc of |DE in the ionization chamber at the focal plane of the S800 67ASdc spectrometer and A/q from the time-of-flight measurements between 67ASec scintillators at the object point and at the focal plane of S800. 67AS c Measured: E|g, ({+67}As)|g coincidence. Deduced levels, Coulomb 67AS2c excitation yields, B(E2) 67AS c Theory: comparison of measured low lying levels with theoretical values 67AS2c via shell model calculations with JUN45 interaction, and via beyond 67AS3c mean-field calculations using five-dimensional collective Hamiltonian 67AS4c (5DCH) method with the Gogny D1S interaction. 67AS cG RI(A)$Predicted from shell model calculation as well as from limit of 67AS2cG experimental observation of transition from (9/2-) to (7/2-) 67AS PN 7 67AS L 0 5/2- 67AS L 720 6 (7/2-) 3.4 PS +9-6 67AS2 L BE2=0.116 +24-26 (2013Co23) 67AS cL $B(E2) deduced by 2013Co23 from Coulomb excitation yields; 67AS2cL listed here in e{+2}b{+2} units 67AS cL $B(E2)=0.1162 {I236}(stat) {I+0-90} (syst, due to <10% branching ratio 67AS2cL for (9/2-) to (7/2-) transition) (2013Co23). Compilers have 67AS3cL quadratically summed the two uncertainties 67AS cL T$deduced by compilers from B(E2)|^, assuming pure E2 for 720 67AS2cL transition. Dominant E2 is suggested by shell-model calculations 67AS G 720 6 [E2] 67AS L 1240 9 (9/2-) 0.66 PS +15-10 67AS2 L BE2=0.046 +9-7 (2013Co23) 67AS cL $B(E2) deduced by 2013Co23 from Coulomb excitation yields; 67AS2cL listed here in e{+2}b{+2} units 67AS cL $B(E2)(from 0,5/2-)=0.0460 {I70} (stat) {I+50-0} (syst, due to <10% 67AS2cL branching ratio for (9/2-) to (7/2-) transition) (2013Co23). Compilers 67AS3cL have quadratically summed the two uncertainties 67AS cL T$deduced by compilers from B(E2)|^ 67AS G 522 5 5 A ? 67AS cG RI$<10% branching from theory and experiment 67AS G 1240 9 95 5 A 67AS cG RI$listed as >90 from theory 67AS 40CA(36AR,2APG):XUNDL-5 2018WA22 202001 67AS c Compiled (unevaluated) dataset from 2018Wa22: 67AS2c Phys Rev C 98, 024313 (2018) 67AS c Compiled by J. Chen (NSCL, MSU), September 1, 2018 67AS c 2018Wa22: E=145 MeV {+36}Ar beam was produced from the ATLAS facility 67AS2c at ANL. Target was a 390 |mg/cm{+2} thick {+40}Ca foils with 113 and 97 67AS3c |mg/cm{+2} flashes of gold in front and behind, respectively. |g rays 67AS4c were detected with the Gammashpere array and evaporated charged 67AS5c particles were detected with the MICROBALL CsI detector array. Measured 67AS6c E|g, I|g, |g|g-coin, |g|g|g-coin, particle-|g-coin, |g|g(DCO). Deduced 67AS7c levels, J, |p, band structures, |g-ray multipolarities. Comparisons 67AS8c with theoretical calculations. 67AS cG E(X)$Newly observed transitions in 2018Wa22 67AS cG E(Y)$It was not possible to determine how and exactly where the 67AS2cG floating band feeds into the 4523, 19/2+ state (2018Wa22). 67AS cG E(A)$ DCO ratios from gating on 775-keV E2 transition 67AS cG E(B)$DCO ratios from sum of gates on 943, 1228, 1357, and 983 keV E2 67AS2cG transitions 67AS cG E(C),RI(C)$Contaminated by 697 keV transition 67AS cG M$As given in 2018Wa22, based on measured DCO ratios. Expected values 67AS2cG of DCO ratios are |?1.1 for stretched quadrupole transitions and |?0.8 67AS3cG for stretched dipole transitions when gating on stretched quadrupole 67AS4cG transitions (2018Wa22). 67AS cL E$From a least-squares fit to |g-ray energies (by compiler), unless 67AS2cL otherwise noted. 67AS cL E(F)$Rounded value from Adopted Levels of {+67}As in ENSDF database 67AS cL J$As given in 2018Wa22, based on |g-ray multipolarities deduced from 67AS2cL measured |g|g(DCO), band assignments and known spin-parities for 67AS3cL low-lying states. 67AS CL BAND(B)$Band 1b. 67AS CL BAND(A)$Band 1a, based on 9/2+. 67AS CL BAND(C)$Band 2a, based on 27/2+. 67AS CL BAND(D)$Band 2b. 67AS CL BAND(E)$Floating band. Feeding into the 4523,19/2+ level. 67AS PN 5 67AS L 0 5/2- 67AS L 68.6 3/2- F 67AS DL E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 67AS L 697.13 24 7/2- 67AS G 697.4 3 71.4 25M1+E2 67AS2 G DCO=0.87 1 67AS L 1103.0 3 7/2- 67AS G 1034.1 5 28.2 57E2 67AS2 G DCO=1.03 4 67AS G 1103.3 5 10 3 M1+E2 67AS2 G DCO=0.99 13 67AS L 1422.86 22 9/2+ A 67AS G 319.8 3 35.4 26E1 67AS2 G DCO=0.84 2 67AS G 726.0 3 72.0 25E1 67AS2 G DCO=0.79 1 67AS G 1422.6 3 6.7 3 M2 67AS2 G DCO=0.99 7 67AS L 2281.6 4 11/2+ 67AS G 858.3 3 9.7 17M1+E2 67AS2 G DCO=0.97 5 67ASF G FL=1422.86 67AS L 2365.0 5 13/2+ A 67AS G 943.2 5 100 E2 A 67AS2 G DCO=1.07 2 67AS L 3180.2 4 13/2+ 67AS G 815.4 3 9.1 14M1+E2 67AS2 G DCO=0.93 5 67AS G 898.2 3 9.7 14M1+E2 A 67AS2 G DCO=0.89 6 67AS L 3593.4 6 17/2+ A 67AS G 1228.4 5 70.0 45E2 67AS2 G DCO=1.12 2 67AS L 3883.8 5 15/2+ 67AS G 703.4 3 26.0 23M1+E2 C 67ASF G FL=3180.2 67AS G 1520.2 7 3.0 5 M1+E2 67AS2 G DCO=1.0 1 67AS L 4523.2 6 19/2+ 67AS G 639.4 3 39.1 26E2 67AS2 G DCO=0.95 6 67AS G 930.2 5 12.6 14M1+E2 67AS2 G DCO=0.93 4 67AS L 4950.6 5 21/2+ A 67AS G 427.6 3 15.4 11M1+E2 A 67AS2 G DCO=0.78 1 67AS G 1356.6 5 26.3 8 E2 67AS2 G DCO=1.11 3 67AS L 5725.1 7 25/2+ A 67AS G 774.5 3 42.0 11E2 67AS2 G DCO=1.09 2 67AS L 4523+X E 67AS G X Y ? 67ASF G FL=4523.2 67AS L 5297+X E ? 67AS G 774 1 X ? 67AS L 6708.3 8 29/2+ A 67AS G 983.3 5 40.3 20E2 67AS2 G DCO=1.10 3 67ASF G FL=5725.1 67AS L 6803.2 8 27/2+ C 67AS G 1078.0 5 4.1 4 M1+E2 A 67ASF G FLAG=X 67ASF G FL=5725.1 67AS2 G DCO=0.91 3 67AS L 6377+X E 67AS G 1080 1 X 67AS L 8053.6 9 31/2+ C 67AS G 1250 1 3.8 4 E2 A 67ASF G FLAG=X 67AS2 G DCO=1.03 6 67AS G 1345.4 7 10.9 9 M1+E2 X 67AS2 G DCO=0.83 4 67AS L 8311.9 9 33/2+ A 67AS G 1603.6 5 17.7 8 E2 X 67AS2 G DCO=1.08 5 67AS L 7578+X E 67AS G 1201 1 X 67AS L 9694.4 10 35/2+ C 67AS G 1382.4 5 4 1 (M1+E2) X 67AS G 1640.8 7 8.8 7 E2 X 67AS2 G DCO=1.27 9 67AS L 9073+X E 67AS G 1495 1 X 67AS L 10530.0 12 37/2+ A 67AS G 2218.0 7 8.6 9 E2 B 67ASF G FLAG=X 67AS2 G DCO=1.13 9 67AS L 11713.2 12 39/2+ C 67AS G 2018.8 7 7.9 6 E2 B 67ASF G FLAG=X 67AS2 G DCO=1.12 6 67AS L 10570+X E ? 67AS G 1497 1 X ? 67AS L 12964.0 16 (41/2+) B 67AS G 2434 1 1.5 3 X 67AS L 13199.0 16 (41/2+) A 67AS G 2669 1 1.3 2 X 67AS L 13599.9 14 (43/2+) D 67AS G 1886.6 7 2.2 3 B 67ASF G FLAG=X 67AS2 G DCO=1.1 2 67AS L 13798.0 15 (43/2+) C 67AS G 2085 1 2.8 3 X 67AS L 15861.8 15 (47/2+) D 67AS G 2261.7 7 1 LT X 67AS L 15875 3 (45/2+) B 67AS G 2911 2 1 LT X 67AS L 16007.3 16 (47/2+) C 67AS G 2209.4 7 1.3 3 X 67AS L 16176 3 (45/2+) A ? 67AS G 2977 2 1 LT X ? 67AS L 18647.1 16 (51/2+) C 67AS G 2640 1 1.0 2 X 67AS G 2785 1 1 LT X