53NI 9BE(54NI,53NIG):XUNDL-3 2016MI05 201604 53NI c Compiled (unevaluated) dataset from 2016Mi05: 53NI c Phys Rev C 93, 024318 (2016) 53NI c Compiled by G. G~urdal (Millsaps College) 53NI c March 25, 2016 53NI c The secondary beam {+54}Ni was produced via fragmentation of a 160 53NI2c MeV/nucleon {+58}Ni primary beam. The {+58}Ni beam impinged on a 802 53NI3c mg/cm{+2} {+9}Be target and the resulting fragments were separated by 53NI4c the A1900 separator and transferred to S800 spectrometer. The 53NI5c secondary beam fragments were identified from their time-of-flight 53NI6c measured between two scintillators. The excited states of {+53}Ni 53NI7c were populated by the one-nucleon knockout reaction from the |?87 53NI8c MeV/nucleon secondary {+54}Ni beam on a 188 mg/cm{+2} {+9}Be target 53NI9c located at the secondary target position in S800 spectrometer. SeGA 53NIac detector array was used to detect in-flight |g-rays. Particle 53NIbc identification was done using energy loss and time-of-flight 53NIcc measurements. Measured: E|g, branching ratio, |g|g-coin, T{-1/2} 53NIdc using Doppler-correction and lineshape analysis and relative |s for 53NIec knockout to the ground state and all the observed excited states from 53NIfc the measured beam rate by using the efficiency and feeding corrected 53NIgc |g-ray intensities. 53NI cL $Relative one-neutron knockout cross sections are given in Figure 5 53NI2cL of 2016Mi05. Values included in the comments here are approximated by 53NI3cL compiler from this figure. 53NI cG E,RI$From Figure 2 in 2016Mi05. 53NI cL E$From E|g. 53NI cL J$Tentative assignments from mirror-symmetry arguments in 2016Mi05. 53NI PN 6 53NI L 0.0 (7/2-) 53NI cL $|s{-exp}=60%. |s{-theory}=50% using Shell Model. 53NI L 320 3 (5/2-) 198 PS 12 53NI cL T$From simulated lineshape analysis to the experimental data 53NI2cL determined by using a reduced |h{+2} at both 37{+|o} and 90{+|o} of 53NI3cL SeGA rings. The uncertainty includes the statistical error (198 ps 53NI4cL {I8}) and an overall systematic error of 4.6% from uncertainties due 53NI5cL to ambiguities in the geometry of the setup (3%), |g-ray anisotropy 53NI6cL effects (1.5%), assumptions in the background (3%) and effects due to 53NI7cL the feeding of the 5/2- state from short-lived states (1%). 53NI cL $|s{-exp}|?12%. Shell Model predicts a very small cross section. 53NI G 320 3 53NI cG E$From the energy difference between prompt 972|g and 1292|g 53NI2cG transitions. Other: 320.5 {I2} from minimization of |h{+2} fitting of 53NI3cG both E|g and T{-1/2} 53NI L 1292 2 (3/2-) 53NI cL $|s{-exp}|?5%. Shell Model predicts a very small cross section. 53NI G 972 2 90 9 53NI G 1292 2 100 9 53NI L 1456 4 (11/2-) 53NI G 1456 4 53NI L 2391 3 (3/2-) 53NI cL $|s{-exp}|?2%. Shell Model predicts a very small cross section. 53NI G 1099 3 53NI L 2842 3 (1/2+) 53NI cL $|s{-exp}|?12%. |s{-theory}|?12% using Shell Model. 53NI G 1550 2 53NI L 3010 4 (5/2+) 4 PS LT 53NI cL T$From |b=0.416 {I6} determined by aligning 1718|g in both 37{+|o} 53NI2cL and 90{+|o} SeGA rings (using Doppler-correction analysis). Authors 53NI3cL stated that time for beam to traverse the target thickness was |?8 ps 53NI4cL therefore the measured |b indicated the average point of decay was 53NI5cL inside the target volume. 53NI cL $|s{-exp}|?5%. |s{-theory}=10% using Shell Model. 53NI G 1718 3 53NI 9BE(58NI,X):T1/2:XUNDL-3 2016SU10 201604 53NI c Compiled (unevaluated) dataset from: 53NI2c Phys Lett B756, 323 (2016) 53NI c See also 2013Su07: Phys Rev C87, 024312 (2013) from the same group 53NI c Compiled by B. Singh (McMaster), March 29, 2016 53NI c 2016Su10: {+58}Ni{+25+} primary beam at E=68.3 MeV/nucleon provided by 53NI2c the Heavy Ion Research Facility in Lanzhou (HIRFL). Target=503 |mm 53NI3c thick {+9}Be. The {+53}Ni fragments were separated and focused using 53NI3c the Radioactive Ion Beam Line, Lanzhou (RIBLL) facility. Measured 53NI4c |b-delayed protons, half-life of {+53}Ni decay, (proton)|g-coin, E|g, 53NI5c I|g, |g|g-coin using double-sided silicon strip detectors (DSSSDs) 53NI6c for particle detection and four segmented clover Ge detectors for 53NI7c |g rays. 53NI L 0 7/2- 57 MS 3 53NI2 L %ECP=22 1 (2016Su10) 53NI cL T$from decay-time spectra fitted with exponential curves (2016Su10), 53NI2cL same procedure as in authors' previous paper 2013Su07. 53NI3cL This value can be compared with 56 ms {I8} in 2013Su07 and 55.2 ms {I7} 53NI4cL in {+53}Ni Adopted Levels in the ENSDF database (June 2013 update), 53NI5cL a value taken from 2007Do17 (Nucl. Phys. A792, 18). 53NI6cL 2016Su10 quote 55.2 ms in decay-scheme Fig. 5. Compiler obtains 53NI7cL weighted average of the three values as 55.3 ms {I7}, almost the 53NI8cL same as that in 2007Do17 53NI cL J$From the Adopted Levels of {+53}Ni in the ENSDF database.