26NA ADOPTED LEVELS, GAMMAS 16NDS 201604 26NA H TYP=FUL$AUT=M.S. Basunia and A.M. Hurst$CIT=NDS 134, 1 (2016)$ 26NA2 H CUT=1-Feb-2016$ 26NA Q 9354 4 5574 4 1.209E4 5 -12079 13 2012WA38 26NA cG E$From {+25}Na(d,p|g), except otherwise noted. 26NA cG E(A)$From {+26}Ne |b{+-} decay 26NA cG E(C)$From {+14}C({+14}C,d|g) 26NA cG RI$Relative photon branching from each level. 26NA cG M,MR$Deduced from angular distributions in {+14}C({+14}C,d|g) 2006Le17. 26NA2cG Measured D+Q assumed as M1+E2. 26NA cG M(B)$Deduced from differential cross sections and angular 26NA2cG distributions in {+25}Na(d,p|g) 2015Ca03. 26NA cL E$From least-squares fit to E|g data (by evaluators) yielding a 26NA2cL reduced |h{+2}=1.8 assuming |D(E|g)=1 keV for |g rays without 26NA3cL uncertainty, except where noted. 26NA cL J(D)$Based on observation of allowed |b{+-} decay from 0{++} g.s. in 26NA2cL {+26}Ne. 26NA cL J(G)$Based on differential cross section measurements compared to DWBA 26NA2cL calculations from charge-exchange (t,{+3}He) reaction and shell-model 26NA3cL analysis (1987Pe06). 26NA cL J(F)$Deduced by excitation energy, angular momentum transfer, 26NA2cL spectroscopic factor, comparison with shell-model calculations, and 26NA3cL measured |g-ray branching ratios from {+25}Na(d,p|g) in 2015Ca03 and 26NA4cL 2012WiZW. 26NA XA26NE B- DECAY 26NA XD14C(14C,DG) 26NA XE25NA(D,PG) 26NA XC26NE(D,2NG) 26NA XFCOULOMB EXCITATION 26NA XG26MG(N,P) 26NA XB26MG(T,3HE) 26NA XH26MG(7LI,7BE) 26NA XI26MG(11B,11C) 26NA PN 6 26NA L 0 3+ 1.07128 S 25 26NA2 L %B-=100$MOMM1=+2.851 2$ MOME2=-0.0053 2 26NA cL $Matter radius {+1/2}=2.92 fm {I3} and 2.93 fm {I4} (1998Su07). 26NA cL MOMM1$From 2014StZZ, 1978Hu12. 26NA cL MOME2$From 2014StZZ, 2000Ke09. Earlier value -0.08 b {I5} 1982To05. 26NAX L XREF=ACBDEFHI 26NA cL J$J(g.s.)=3 from Laser spectroscopy measurements (1978Hu12,2013Ma15); 26NA2cL |p=+ from log| {Ift}=4.71 to first 2+ in {+26}Mg from |b{+-} decay of 26NAxcL {+26}Na. 26NA cL T$From high-precision measurement 2005Gr07; a statistical uncertainty 26NA2cL of 0.00013 s combined with a systematic uncertainty of 0.00021 s 26NA3cL contribute to the overall uncertainty. Other values: 1.04 s {I3} 26NA4cL (1958Nu41); 1.03 s {I6} (1961Ro08); 1.070 s {I30} (1972Kl04); 26NA5cL 1.087 s {I12} (1973Al13); 1.05 s {I2} (1973Kl09); 26NA6cL 1.074 s {I6} (1992Te03). 26NA L 82.2 6 1+ 9 US 2 D 26NA2 L %IT=100 26NA cL J$82.5|g E2 to 3+ 26NA cL T$From 1987DuZU. 26NAX L XREF=ABCEF 26NA G 84 3 100 E2 A 26NA2 G FLAG=B 26NAB G BE2W=3.6 9 26NA L 232.7 6 2+ 0.9 NS +6-5 26NAX L XREF=ABCDEFH(210)I 26NA cL J$M1+E2 |g to 3+ and 1+. 26NA cL T$From Coulomb excitation 26NA G 153 3 75.1 25 M1+E2 +0.16 7 A 26NA cG RI$Other: 81 {i3} (Coulomb Excitation) 26NAB G BM1W=0.0030 +17-20$BE2W=19 +20-18 26NA G 232 2 100 4 M1+E2 -0.32 14 A 26NA cG M$M1 in {+25}Na(d,p|g) 2015Ca03. 26NAB G BM1W=0.0010 +6-7$BE2W=11 10 26NA L 406.7 5 2+ 0.18 NS +17-13 26NA cL J$M1+E2 |g to 3+ and 1+ 26NAX L XREF=AB(420)CDEFH 26NA G 174 2.8 4 26NA G 323 14.6 6 M1+E2 +0.14 9 26NAB G BM1W=0.0004 +2-3$BE2W=0.5 +7-4 26NA G 404 3 100.0 19 M1+E2 -0.25 12 A 26NA cG M$M1 in {+25}Na(d,p|g) 2015Ca03. 26NAB G BM1W=0.0015 +11-14$BE2W=3 +4-2 26NA L 840 40 26NA cL E$From {+26}Mg({+7}Li,{+7}Be) 1972Ba35. 26NAX L XREF=H 26NA L 1408.0 10 26NAX L XREF=DB(*) 26NA G 1408 100.0 26NA L 1509.0 11 (1+) D 26NAX L XREF=AB(*)CD(1514)E 26NA G 1102 10.00 LT 26NA G 1279 3 100.0 AP D A 26NA cG E$Other: 1274 in (d,p|g) 2015Ca03. 26NA L 1660.2 12 26NAX L XREF=D 26NA G 1578 100.0 C 26NA L 1808.0 6 (3+) F 26NAX L XREF=B(1860)E 26NA G 1402 8.8 19 26NA G 1577 24 4 26NA G 1806 100 6 26NA L 1996.5 7 (4+) F 26NAX L XREF=BCDE 26NA G 1590 54.8 AP C 26NA G 1764 100.0 AP C 26NA G 1996 100.0 AP C 26NA L 2045.2 7 26NAX L XREF=BDI(*) 26NA G 1639 100.0 C 26NA G 2044 100.0 & 26NAF G FLAG=C 26NA L 2118.2 8 (5+) F 26NAX L XREF=EI(*) 26NA G 2118 100.0 26NA L 2126.1 10 26NAX L XREF=D 26NA G 2126 100.0 C 26NA L 2182.3 8 26NAX L XREF=D 26NA G 1775 100.0 C 26NA G 2101 18.6 C 26NA L 2192.9 8 (2+) F 26NAX L XREF=BE 26NA G 1786 20.00 LT 26NA G 2193 100.0 AP 26NA L 2225.5 9 (4+) F 26NA cL J$2225|g to 3{++} g.s. rules out earlier (0+,1+) assignment. 26NAX L XREF=AC(2230)EH 26NA G 418 6.2 6 26NA G 2219 4 100 5 A 26NA cG E$Other: 2225 {+25}Na(d,p|g) 2015Ca03. 26NA L 2230.4 8 26NAX L XREF=D 26NA G 1996 70.5 & 26NAF G FLAG=C 26NA G 2232 100.0 C 26NA L 2284.1 10 (5+) 26NA cL J$Assignment is compatible with 2284|g decay to 3+ g.s. from 26NA2cL {+14}C({+14}C,d|g) 2006Le17. 26NA3cL Other assignment (3+,4+); best fit as 4+ in DWBA analysis although the 26NA4cL 3+ prediction gives a good account of all data other than the most 26NA5cL forward-angle measurement in (t,{+3}He) charge-exchange reaction 26NA6cL (1987Pe06). 26NAX L XREF=BD 26NA G 2284 100.0 26NA L 2422.5 8 (2+) F 26NAX L XREF=E 26NA G 2015 1.0E2 4 26NA G 2423 9.E1 3 26NA L 2452.7 8 26NAX L XREF=BD 26NA G 2044 37.9 & 26NAF G FLAG=C 26NA cG E$2045 in Figure 4 of 2006Le17 26NA G 2371 100.0 C 26NA L 2712.3 12 26NAX L XREF=B(2697)D 26NA G 2630 100.0 C 26NA L 2720 3 (1+) D 26NAX L XREF=A(2721)D 26NA G 1212 3 100.0 A 26NA G 2486 4 92.0 A 26NA cG E$Other: 2493 ({+14}C,d|g) 26NA L 2803.9 8 26NAX L XREF=B(2815)D 26NA G 350 24.1 C 26NA cG E$351 in Figure 4 of 2006Le17 26NA G 2805 100.0 C 26NA L 2853.1 7 (2-) F 26NAX L XREF=EG(2860) 26NA G 2620 81 8 26NA G 2771 100 8 26NA G 2853 60 6 26NA L 2937.8 8 (1+,2+) G 26NAX L XREF=B(2933)D 26NA G 2855 76.2 26NA G 2938 100.0 26NA L 3134.0 8 (3)- F 26NA cL J$L=1 in {+25}Na(d,p|g) 2015Ca03. 26NAX L XREF=B(3123)E 26NA G 2727 51 6 26NA G 3134 100 7 26NA L 3222.8 10 (2+) 26NAX L XREF=B(3232)D 26NA cL J$Based on differential cross section measurements compared to DWBA 26NA2cL calculations from charge-exchange (t,{+3}He) reaction and shell-model 26NA3cL analysis (1987Pe06). Hypothesis supported by angular distributions 26NA4cL measured in {+14}C({+14}C,d) (2006Le17). 26NA G 1041 100.0 C 26NA G 1177 42.6 C 26NA L 3304.6 12 26NAX L XREF=B(3310)D 26NA G 1308 100.0 C 26NA L 3417.4 12 26NAX L XREF=B(3400)D 26NA G 3335 100.0 C 26NA L 3509.3 8 (4)- F 26NA cL J$L=1 in {+25}Na(d,p|g) 2015Ca03. 26NAX L XREF=E 26NA G 3509 100.0 26NA L 3603.4 12 26NAX L XREF=B(3618)D 26NA G 3521 100.0 C 26NA L 3814 15 26NA cL E$From {+26}Mg(t,{+3}He) 1974Fl01. 26NAX L XREF=B 26NA L 3966 15 26NA cL E$From {+26}Mg(t,{+3}He) 1974Fl01. 26NAX L XREF=B 26NA L 4090.1 12 (2)- 26NA cL J$Based on 2282|g to 3+ state at 1807.8 keV; assumed E1 transition 26NA2cL according to systematics in this mass region (2015Ca03). L=1 in 26NA3cL {+25}Na(d,p|g) 2015Ca03. 26NAX L XREF=BE 26NA G 2282 100.0 D 26NAF G FLAG=B 26NA cG M$based on systematics in mass region 2015Ca03. 26NA L 4188.1 15 26NAX L XREF=B(4190)D 26NA cL E$Probable doublet in 1974Fl01. 26NA G 2679 100.0 C 26NA L 4303.4 8 (5-) F 26NAX L XREF=E 26NA G 794 100 7 26NA G 2078 70 6 26NA G 2185 43 4 26NA L 4440 15 26NA cL E$From {+26}Mg(t,{+3}He) 1974Fl01. 26NAX L XREF=B 26NA L 4702 15 26NA cL E$From {+26}Mg(t,{+3}He) 1974Fl01. 26NA cL E$Probable doublet in 1974Fl01. 26NAX L XREF=BI 26NA L 4915.4 9 (6-) F 26NAX L XREF=EH(4910) 26NA G 612 100 6 D 26NAF G FLAG=B 26NA G 1406 39 4 26NA G 2797 63 5 26NA L 4970 40 (4+) G 26NA cL E$From {+26}Mg(t,{+3}He) 1974Fl01. 26NAX L XREF=B 26NA L 5013.2 12 (3-,4-) F 26NAX L XREF=E 26NA G 3205 100.0 26NA L 5080 60 (2+) 26NA2 L XREF=B 26NA L 5480 G 26NAX L XREF=G 26NA L 7200 26NA cL E$From {+26}Mg(t,{+3}He) 1974Fl01. 26NAX L XREF=B 26NA L 9000 26NA cL E$From {+26}Mg(t,{+3}He) 1974Fl01. 26NAX L XREF=B 26NA 26NE B- DECAY 2007SU05,2004WE11,1987DUZU16NDS 201604 26NA H TYP=FUL$AUT=M.S. Basunia and A.M. Hurst$CIT=NDS 134, 1 (2016)$ 26NA2 H CUT=1-Feb-2016$ 26NA c 2007Su05: {+26}Ne radioactive beam produced from a primary 26NA2c beam of {+48}Ca at 140 MeV/nucleon bombarding a {+9}Be target at NSCL 26NA3c facility. The fragments were separated by A1900 fragment separator 26NA4c on the basis of magnetic rigidities. The beam of {+26}Ne was used 26NA5c in a pulsed mode of 300 ns timing. The detection system consisted 26NA6c of implantation detector, an array of 16 neutron time-of-flight 26NA7c detectors and eight |g-ray detectors of SeGA array. Particle ({+26}Na) 26NA8c identification was achieved by time-of-flight and energy loss 26NA9c information in silicon detectors. Measured E|g, I|g, |g|g, 26NAAc (particle)|g coin, |b, |g|b coin, isotopic 26NABc half-life by timing of |g rays. Comparisons with shell-model 26NACc calculations. 26NA c 2004We11: Mass separated {+26}Ne beam from the ISOLDE facility 26NA2c obtained from fission of uranium by 1.4 GeV protons. Measured 26NA3c E|g, I|g, |g|g, |b|g coin using Ge detector for |g rays and plastic 26NA4c scintillator for |b rays. 26NA c 1987DuZU: Projectile-fragment isotopic separation technique used to 26NA2c produce {+26}Ne. Partial decay scheme of {+26Na} deduced from |b decay; 26NA3c |g-ray energies, but not intensities, reported. Measured T{-1/2}. 26NA cB LOGFT$ Deduced by evaluators using log| {Ift} code at 26NA2cB www.nndc.bnl.gov. These values are nearly the same as in 2007Su05 26NA cG E,RI$Taken from 2007Su05. 26NA cL E$Taken from 2007Su05. 26NA cL J$From Adopted Levels. 26NE P 0.0 0+ 197 MS 2 7340 19 26NA N 1 1 1 1 26NA PN 3 26NA L 0.0 3+ 26NA L 82.0 23 1+ 9 US 2 26NA cL T$From 1987DuZu 26NA B 91.6 2 3.87 6 26NAS B EAV=3397.0 96 26NA G 84 3 84.2 15 0.128 20 95 26NA cG RI$deduced by evaluators from I(|g+ce) and |a=0.128 {I20} (from BrIcc 26NAxcG code) 26NA cG TI$2007Su05 quote intensity from 2004We11. Evaluators note that 26NA2cG 2004We11 give I(|g+ce)(82.5|g)=100 but |b feeding=92 {i5} for 82.5-keV 26NA3cG level. The latter value implies I(|g+ce)(82.5|g)=95, which has been 26NA4cG used by 2007Su05. 26NA L 232.9 18 2+ 26NA B 1.7 4 5.6 1 26NAS B EAV=3322.5 95 26NA cB LOGFT$ too low for |DJ=2, |D|p=no transition (evaluator's note). 26NA G 153 3 3.4 2 26NA G 232 2 4.4 2 26NA L 404 3 2+ 26NA cL J$Reported as (0+,1+,2+) in 2007Su05. 26NA B 0.4 1 6.1 1 26NAS B EAV=3238.1 95 26NA G 404 3 0.4 1 26NA L 1511 4 (1+) 26NA cL J$Reported as (0+,1+) in 2007Su05. 26NA B 4.2 4 4.8 1 26NAS B EAV=2692.5 96 26NA G 1279 3 5.4 2 26NA L 2219 4 (4+) 26NA cL J$Reported as (0+,1+) in 2007Su05. 26NA B 0.6 2 5.4 2 26NAS B EAV=2345.0 96 26NA G 2219 4 0.6 2 26NA L 2721 4 (1+) 26NA cL J$Reported as (0+,1+) in 2007Su05. 26NA B 1.9 4 4.7 1 26NAS B EAV=2098.9 95 26NA G 1212 3 1.2 3 26NA G 2486 4 0.7 2 26NA 26MG(T,3HE) 1974FL01,1987PE06,2006ZE0116NDS 201604 26NA H TYP=FUL$AUT=M.S. Basunia and A.M. Hurst$CIT=NDS 134, 1 (2016)$ 26NA2 H CUT=1-Feb-2016$ 26NA c 1974Fl01: Triton beam E=23.5 MeV provided by Los Alamos Van de Graff 26NA2c facility impinged upon {+26}Mg target. Reaction products measured from 26NA3c 15 to 30|' at 5|' intervals using E-|DE silicon 26NA4c surface-barrier-detector telescope with a 50 |mm |DE detector. Excited 26NA5c states in {+26}Na were populated using charge-exchange (t,{+3}He) 26NA6c reaction and relative d|s/d|W measured. 26NA c 1987Pe06: {+3}H{+-} ions accelerated to 36 MeV by tandem Van de Graff 26NA2c accelerator with average beam intensity of 200 nA and incident upon 26NA3c self-supporting foils of {+26}Mg with thicknesses of 0.20 mg/cm{+2} and 26NA4c 1.50 mg/cm{+2}. Recoiling particles measured using Daresbury 1 m 26NA5c scattering chamber in conjunction with five |DE-E semiconductor 26NA6c telescopes. |DE detectors were between 118 and 155 |mm thick and E 26NA7c detectors 5 mm thick. Particle-energy spectra and differential cross 26NA8c sections obtained over angular range 15 to 50|'. Results compared 26NA9c to DWBA calculations. 26NA c 2006Ze01,2007Ze04: E=115 MeV/nucleon. Triton beam produced from 26NA2c 140 MeV/nucleon |a beam impinging on a Be target. Measured {+3}He 26NA3c spectrum, |s(|q) using the s800 spectrometer of two two-dimensional 26NA4c cathode-readout drift detectors (CRDCs). FWHM=300 keV, DWBA analysis. 26NA5c Deduced Gamow-Teller transition strengths. 26NA cL E$From measured particle-energy spectra in 1974Fl01 except where noted. 26NA cL E(A)$From measured particle-energy spectra in 1987Pe06. 26NA cL J$From DWBA analysis in 1987Pe06 except where noted. 26NA cL E(B),J(B)$Based on Gamow-Teller strengths in 2006Ze01. 26NA cL $L,B(>): Based on Gamow-Teller strengths in 2006Ze01. 26NA cL E(C),L(C)$From spectrum in Figure 1 of 2006Ze01. 26NA cL E(D)$Level observed as part of multiplet centered on 2600 keV {i200} 26NA2cL in 2006Ze01 listing J|p=1{++}, L=0, and B(>)=0.13 {i2}. 26NA cL E(E)$Level observed as part of multiplet centered on 5100 keV {i400} 26NA2cL in 2006Ze01 listing J|p=1{++}, L=0, and B(>)=0.22 {i4}. 26NA CL S$LABEL=^B(^GT) 26NA L 0 3+ 26NA L 88 15 1+ 0 0.41 5 26NA L 241 15 2+ 26NA L 420 15 2+ 26NA L 1.4E3 2 1+ 0 0.09 2 B 26NA cL E$A group of unresolved levels between 1450 and 1650 keV is also 26NA2cL reported in 1987Pe06. 26NA L 1860 60 A 26NA L 1996 30 26NA L 2048 15 26NA L 2186 15 26NA L 2290 15 (3+,4+) 26NA cL J$Best fit as 4+ in DWBA analysis although the 3+ prediction gives a 26NA2cL good account of all data other than the most forward-angle measurement 26NA2cL in 1987Pe06. 26NA L 2456 15 D 26NA L 2697 15 D 26NA L 2815 15 26NA L 2933 15 (1+,2+) 26NA L 3123 15 26NA L 3232 15 (2+) 26NA L 3310 15 26NA L 3400 15 26NA L 3618 15 26NA L 3814 15 26NA L 3966 15 26NA L 4083 15 26NA L 4190 15 26NA cL E$Probably doublet (1974Fl01) 26NA L 4200 2- 1 C 26NA cL J$From Figure 4 of 2006Ze01 26NA L 4440 15 26NA L 4702 15 E 26NA cL E$Probably doublet (1974Fl01) 26NA L 4970 40 (4+) E 26NA L 5080 60 (2+) E 26NA L 7200 1 C 26NA L 9000 1 C 26NA 2H(25NA,26NAG) 2004SC43,2015CA03 16NDS 201604 26NA H TYP=FUL$AUT=M.S. Basunia and A.M. Hurst$CIT=NDS 134, 1 (2016)$ 26NA2 H CUT=1-Feb-2016$ 26NA c 2004Sc43: A post-accelerated {+25}Na beam provided by the REX-ISOLDE 26NA2c facility at CERN was delivered to a 10-|mm thick deuterated 26NA3c polyethylene target with a beam energy of 2.2 MeV/nucleon and an 26NA4c intensity of about 1|*10{+6} s{+-1} (inverse kinematics). Recoiling 26NA5c nuclei were detected in a segmented 24|*4 annular and 16|*4 radial 26NA6c Cd-type charged-particle detector telescope comprising a |? 500-|mm 26NA7c thick |DE followed by a|?500-|mm thick E detector and covers a 26NA8c laboratory range from 15|' to 50|'. Coincident |g rays were 26NA9c measured using the MINIBALL array of 24 {I6}-fold segmented, 26NAAc individually encapsulated, HPGe detectors arranged in 8 triple-cluster 26NABc cryostats. Measured E|g, |g(ions) coincidence. Preliminary report as 26NACc stated in 2004Sc43. 26NA c 2015Ca03: A 5-MeV/nucleon {+25}Na beam was provided by ISAC2 at TRIUMF 26NA2c to impinge a 0.5-mg/cm{+2} Cd{-2} target with an intensity of 26NA3c 3|*10{+7} pps. Recoiling nuclei were detected in the silicon array 26NA4c SHARC in coincidence with deexcitation |g rays recorded in the HPGe 26NA5c clover array TIGRESS. Deduced levels, E|g, J|p, measured angular 26NA6c distributions and extracted differential cross sections. Results 26NA7c compared with shell model calculations and previous work. See also 26NA8c 2012WiZW, 2012Wi13. 26NA cG E,RI$Measured in 2012WiZW except where noted. 26NA cG E(A)$Taken from 2015Ca03. 26NA cG RI(B)$Taken from 2012WiZW. 26NA cG M$Assignment in 2015Ca03, based on measured angular distributions. 26NA cL E$From least-squares fit (by evaluators) to E|g data yielding a reduced 26NA2cL |h{+2} of |?1. An uncertainty of 1 keV is assumed for each E|g. 26NA cL J$Assignments in 2015Ca03 and 2012WiZW, based on excitation energy, 26NA2cL angular momentum transfer, spectroscopic factor, comparison with 26NA3cL shell-model calculations, and measured |g-ray branching ratios. 26NA cL S$Corrected for forward focusing of emitted |g rays. Extracted from 26NA2cL measured and calculated differential cross sections in 2012WiZW. 26NA cL L$Deduced from measured differential cross sections and theoretical 26NA2cL angular distributions in 2012WiZW. 26NA PN 5 26NA L 0 3+ 26NA L 81.8 8 1+ 26NA L 232.1 6 2+ 0 0.144 26NA G 151 42.9 14 26NA G 232 57.1 18 M1 A 26NA L 405.8 5 2+ 0 0.337 26NA G 174 2.4 3 26NA G 323 12.4 5 26NA G 405 85.2 16 M1 A 26NA L 1507.0 9 1+ 26NA G 1102 10 LT 26NA G 1274 100 AP 26NA L 1807.6 6 3+ 2 0.216 26NA G 1402 6.6 14 A 26NA G 1577 18.3 26 A 26NA G 1806 75.1 45 26NA L 1996.1 8 4+ 26NA cL E,J$only reported in 2015Ca03. 26NA G 1764 50 AP A 26NAF G FLAG=B 26NA G 1996 50 AP A 26NAF G FLAG=B 26NA L 2118.2 8 5+ 2 0.216 26NA cL J$reported as 4+ in 2012WiZW. 26NA G 2118 100 26NA L 2192.5 8 2+ 26NA G 1786 20 LT 26NA G 2193 100 AP 26NA L 2225.3 7 4+ 2 0.432 26NA G 418 5.8 5 A 26NA G 2225 94.2 39 26NA L 2422.0 8 2+ 26NA G 2015 52 18 A 26NA G 2423 48 16 A 26NA L 2852.8 7 2- 26NA G 2620 33.5 30 26NA G 2771 41.5 33 26NA G 2853 25.0 25 26NA L 3133.6 8 3- 1 0.0983 26NA G 2727 33.6 40 26NA G 3134 66.4 46 26NA L 3509.3 8 4- 1 0.540 26NA G 3509 100 26NA L 4089.7 12 2- 26NA cL E,J$only reported in 2015Ca03. 26NA G 2282 100 [E1] A 26NAF G FLAG=B 26NA cG M$based on systematics in this mass region (2015Ca03). 26NA L 4303.3 8 (5-) 26NA G 794 46.9 32 26NA G 2078 32.7 25 26NA G 2185 20.4 19 26NA L 4915.3 9 (6-) 26NA G 612 49.4 28 [M1] 26NA G 1406 19.2 16 26NA G 2797 31.3 21 26NA L 5012.8 12 (3-,4-) 26NA G 3205 100 26NA 14C(14C,DG) 2006LE17 16NDS 201604 26NA H TYP=FUL$AUT=M.S. Basunia and A.M. Hurst$CIT=NDS 134, 1 (2016)$ 26NA2 H CUT=1-Feb-2016$ 26NA c 2006Le17: E=22 MeV. Measured E|g, I|g, d|g coin, |g|g|g coin, |g(|q), 26NA2c using an array of three (four crystal) Compton-suppressed 'clover' 26NA3c detectors and seven Compton-suppressed single Ge crystals. The three 26NA4c 'clovers' and one single Ge detectors were placed at 90|', two single 26NA5c crystals at 35|' and four at 145|' relative to the beam direction. 26NA6c Charged particles were detected with Si detector (E-|DE) telescope 26NA7c at 0|'. Comparisons with shell-model calculations. Detailed 26NA8c discussion of a missing 1+ state below 3 MeV, and possible 26NA9c candidates. 26NA cL E$ From least-squares fit to E|g data, assuming |D(E|g)=1 keV for each 26NA2cL |g ray 26NA PN 5 26NA L 0 3+ 26NA L 82.3 6 1+ 26NA G 82.5 26NA L 233.6 6 2+ 26NA G 150.9 82 M1+E2 +0.16 7 26NA G 233.3 100 M1+E2 -0.32 14 26NA L 407.0 6 2+ 26NA G 324.1 16 M1+E2 +0.14 9 26NA G 406.5 87 M1+E2 -0.25 12 26NA L 1408.0 10 26NA G 1408 33 26NA L 1514.0 8 1+ 26NA G 1107 6.5 26NA G 1280 45 M1(+E2) +0.07 10 26NA L 1660.4 12 26NA G 1578 15 26NA L 1996.9 7 26NA G 1590 17 26NA G 1764 31 26NA G 1996 31 & 26NA cG E$1997 in Figure 4 of 2006Le17 26NA L 2045.4 7 26NA G 1639 7.2 26NA G 2044 7.2 & 26NA cG E$2045 in Figure 4 of 2006Le17 26NA L 2126.1 10 26NA G 2126 147 26NA L 2182.5 8 26NA G 1775 14 26NA G 2101 2.6 26NA L 2230.9 8 26NA G 1996 31 & 26NA G 2232 44 26NA L 2284.1 10 5+ 26NA G 2284 14 26NA L 2452.9 8 26NA G 2044 7.2 & 26NA G 2371 19 26NA L 2712.5 12 26NA G 2630 19 26NA L 2726.4 10 1+ 26NA G 1212 25 26NA G 2493 23 26NA L 2804.0 8 26NA G 350 13 26NA cG E$351 in Figure 4 of 2006Le17 26NA G 2805 54 26NA L 2937.8 8 26NA G 2855 9.9 26NA G 2938 13 26NA L 3222.9 10 (2+) 26NA G 1041 19 26NA G 1177 8.1 26NA L 3305.0 12 26NA G 1308 3.2 26NA L 3417.5 12 26NA G 3335 20 26NA L 3603.6 12 26NA G 3521 41 26NA L 4193.1 13 26NA G 2679 24 26NA 25NA(D,PG) 2004SC43,2015CA03 16NDS 201604 26NA H TYP=FUL$AUT=M.S. Basunia and A.M. Hurst$CIT=NDS 134, 1 (2016)$ 26NA2 H CUT=1-Feb-2016$ 26NA c 2004Sc43: Inverse kinematics reaction: A post-accelerated {+25}Na beam 26NA2c provided by the REX-ISOLDE facility at CERN was delivered to a 10-|mm 26NA3c thick deuterated polyethylene target with a beam energy of 26NA4c 2.2 MeV/nucleon and an intensity of about 1|*10{+6} s{+-1}. Recoiling 26NA5c nuclei were detected in a segmented 24|*4 annular and 16|*4 radial 26NA6c Cd-type charged-particle detector telescope comprising an |?500-|mm 26NA7c thick |DE followed by an |?500-|mm thick E detector and covers a 26NA8c laboratory range from 15|' to 50|'. Coincident |g rays were 26NA9c measured using the MINIBALL array of 24 {I6}-fold segmented, 26NAAc individually encapsulated, HPGe detectors arranged in 8 triple-cluster 26NABc cryostats. Measured E|g, |g(ions) coincidence. Preliminary report as 26NACc stated in 2004Sc43. 26NA c 2015Ca03: Inverse kinematics reaction: A 5-MeV/nucleon {+25}Na beam 26NA2c was provided by ISAC2 at TRIUMF to impinge a 0.5-mg/cm{+2} Cd{-2} 26NA3c target with an intensity of 3|*10{+7} pps. Recoiling nuclei were 26NA4c detected in the silicon array SHARC in coincidence with deexcitation 26NA5c |g rays recorded in the HPGe clover array TIGRESS. Deduced levels, 26NA6c E|g, J|p, measured angular distributions and extracted differential 26NA7c cross sections. Results compared with shell model calculations and 26NA8c previous work. See also 2012WiZW, 2012Wi13. 26NA cG E,RI$Measured in 2012WiZW except where noted. 26NA cG E(A)$Taken from 2015Ca03. 26NA cG RI(B)$Taken from 2012WiZW. 26NA cG M$Assignment in 2015Ca03, based on measured angular distributions. 26NA cL E$From least-squares fit (by evaluators) to E|g data yielding a reduced 26NA2cL |h{+2} of |?1. An uncertainty of 1 keV is assumed for each E|g. 26NA cL J$Assignments in 2015Ca03 and 2012WiZW, based on excitation energy, 26NA2cL angular momentum transfer, spectroscopic factor, comparison with 26NA3cL shell-model calculations, and measured |g-ray branching ratios. 26NA cL S$Corrected for forward focusing of emitted |g rays. Extracted from 26NA2cL measured and calculated differential cross sections in 2012WiZW. 26NA cL L$Deduced from measured differential cross sections and theoretical 26NA2cL angular distributions in 2012WiZW. 26NA PN 5 26NA L 0 3+ 26NA L 81.8 8 1+ 26NA L 232.1 6 2+ 0 0.144 26NA G 151 42.9 14 26NA G 232 57.1 18 M1 A 26NA L 405.8 5 2+ 0 0.337 26NA G 174 2.4 3 26NA G 323 12.4 5 26NA G 405 85.2 16 M1 A 26NA L 1507.0 9 1+ 26NA G 1102 10 LT 26NA G 1274 100 AP 26NA L 1807.6 6 3+ 2 0.216 26NA G 1402 6.6 14 A 26NA G 1577 18.3 26 A 26NA G 1806 75.1 45 26NA L 1996.1 8 4+ 26NA cL E,J$only reported in 2015Ca03. 26NA G 1764 50 AP A 26NAF G FLAG=B 26NA G 1996 50 AP A 26NAF G FLAG=B 26NA L 2118.2 8 5+ 2 0.216 26NA cL J$reported as 4+ in 2012WiZW. 26NA G 2118 100 26NA L 2192.5 8 2+ 26NA G 1786 20 LT 26NA G 2193 100 AP 26NA L 2225.3 7 4+ 2 0.432 26NA G 418 5.8 5 A 26NA G 2225 94.2 39 26NA L 2422.0 8 2+ 26NA G 2015 52 18 A 26NA G 2423 48 16 A 26NA L 2852.8 7 2- 26NA G 2620 33.5 30 26NA G 2771 41.5 33 26NA G 2853 25.0 25 26NA L 3133.6 8 3- 1 0.0983 26NA G 2727 33.6 40 26NA G 3134 66.4 46 26NA L 3509.3 8 4- 1 0.540 26NA G 3509 100 26NA L 4089.7 12 2- 26NA cL E,J$only reported in 2015Ca03. 26NA G 2282 100 [E1] A 26NAF G FLAG=B 26NA cG M$based on systematics in this mass region (2015Ca03). 26NA L 4303.3 8 (5-) 26NA G 794 46.9 32 26NA G 2078 32.7 25 26NA G 2185 20.4 19 26NA L 4915.3 9 (6-) 26NA G 612 49.4 28 [M1] 26NA G 1406 19.2 16 26NA G 2797 31.3 21 26NA L 5012.8 12 (3-,4-) 26NA G 3205 100 26NA 26NE(D,2NG) 2006OB05 16NDS 201604 26NA H TYP=FUL$AUT=M.S. Basunia and A.M. Hurst$CIT=NDS 134, 1 (2016)$ 26NA2 H CUT=1-Feb-2016$ 26NA c 2006Ob05: Inverse kinematic reaction: Beam={+26}Ne, target={+2}H 26NA c E({+26}Ne)=9.7 MeV/nucleon secondary beam produced by ISOL method 26NA2c using SPIRAL facility at GANIL. The primary beam of {+36}S at 26NA3c E=77.5 MeV/nucleon was fragmented on a Carbon SPIRAL target. 26NA c Measured E|g, I|g, ({+26}Na)|g coin using 11 'Clovers' (8 EXOGAM and 26NA2c 3 EUROGAM). The {+26}Na ejectiles were analyzed in the focal 26NA3c plane of the VAMOS magnetic spectrometer using time-of-flight and 26NA4c E-|DE method. 26NA c Level scheme is taken from 2006Le17 - ({+14}C,d|g) 26NA G 368 2 26NA L 0 3+ 26NA L 82 4 26NA L 232 3 26NA G 150 2 26NA G 232 3 26NA L 407 2 26NA G 407 2 26NA L 1516 9 26NA G 1284 9 26NA L 1998 8 26NA G 1998 8 * 26NA L 2230 9 26NA G 1998 8 * 26NA COULOMB EXCITATION 2015SI01 16NDS 201604 26NA H TYP=FUL$AUT=M.S. Basunia and A.M. Hurst$CIT=NDS 134, 1 (2016)$ 26NA2 H CUT=1-Feb-2016$ 26NA c 2015Si01: Beam=2.82 MeV/nucleon {+26}Na produced in bombardment of 26NA2c UC{-x} target by 1.4 GeV protons provided by the CERN PS Booster and 26NA3c {+26}Na ions separated by ISOLDE General Purpose separator. 26NA c Coulomb excitation target=enriched {+104}Pd 26NA c A radioactive-beam Coulomb-excitation experiment with {+26}Na 26NA2c (T{-1/2}=1.07 s) performed using the REX-ISOLDE facility at CERN. 26NA3c {+26}Na ions (q=6{++}) were post accelerated to 2.82 MeV/nucleon and 26NA4c impinged upon a 3.6-mg/cm{+2} thick {+104}Pd target with an average 26NA5c beam intensity of 6.4|*10{+4} {i5} ions/s for an irradiation period of 26NA6c 73 h. Scattered beam and target nuclei were detected using the 500-|mm 26NA7c double-sided silicon strip detector. Deexcitation |g rays following 26NA8c Coulomb excitation of projectile and target nuclei were detected using 26NA9c the MINIBALL |g-ray spectrometer comprising eight triple-cluster 26NAAc detectors, each consisting of three six-fold-segmented HPGe crystals. 26NABc Measured E|g, I|g, (scattered particle)|g-coin. 26NABc The coupled-channels Coulomb-excitation code GOSIA2 was used to obtain 26NACc transition matrix elements from observed |g-ray yields and known 26NADc spectroscopic data (branching ratios, multipole mixing ratios and half 26NAEc lives). Deduced B(E2) and B(M1) values are compared to {Isd} 26NAFc shell-model calculations using various interactions: universal {Isd} 26NAGc (USD), universal {Isd}-A (USDA), and universal {Isd}-B (USDB) 26NAHc interaction. 26NA cG M,MR$From Adopted Gammas 26NA cL E$From least-squares fit to E|g data, assuming 0.5 keV uncertainty 26NA2cL for 82.5-keV transition 26NA cL J(B)$From Adopted Levels 26NA cL J(A)$Deduced from best fit to (t,{+3}He) angular distributions in 26NA2cL 1987Pe06, although these assignments were not adopted in Endt's 26NA3cL 1990En08 evaluation. 2006Le17 in their {+14}C({+14}C,d|g) claim 26NA4cL to confirm 2+ assignment for both the 233- and 407-keV levels. 26NA PN 6 26NA L 0 3+ B 26NA L 82.4 6 1+ B 26NA G 84 3 [E2] 0.137 4 26NAB G BE2W=3.10 26NA cG E$From Adopted Gammas 26NA cG $B(E2)(W.u.) deduced by 2015Si01 from known half-life of 82.4 level 26NA2cG and theoretical conversion coefficient for 82.5|g from BrIcc code. 26NA3cG Shell-model predictions (2015Si01) for corresponding B(E2)(W.u.) 26NA4cG values are 8.66 (USD), 8.39 (USDA) and 6.88 (USDB) 26NA L 233.2 8 2+ 0.7 NS +6-5 A 26NA2 L BE2=0.00421 +46-41 26NA cL $B(E2) from 3+ g.s. to 233 level deduced by evaluators from 26NA2cL experimental B(E2)(W.u.)=12.9 {I+14-13}, branching ratio and 26NA3cL mixing ratio for 233|g 26NA cL T$deduced by evaluators from B(E2)(W.u.) and adopted 233|g properties 26NA G 151 1 81.0 32 M1+E2 +0.16 7 26NA2 G BM1W=0.44 +73-22 $BE2W=26 +67-19 26NA cG $Shell-model predictions for corresponding B(M1)(W.u.) in 2015Si01: 26NA2cG 0.0002 (USD), 0.011 (USDA) and 0.023 (USDB) 26NA cG $Shell-model predictions for corresponding B(E2)(W.u.) in 2015Si01: 26NA2cG 3.09 (USD); 1.23 (USDA); 1.84 (USDB) 26NA cG RI$corrected number of counts reported as 3279 {I131} in 2015Si01. 26NA G 233 1 100 4 M1+E2 -0.32 14 26NA2 G BM1W=0.13 +28-7 $BE2W=12.9 +14-13 26NA cG $Shell-model predictions for corresponding B(M1)(W.u.) in 2015Si01: 26NA2cG 0.14 (USD), 0.04 (USDA) and 0.07 (USDB) 26NA cG $Shell-model predictions for corresponding B(E2)(W.u.) in 2015Si01: 26NA2cG 6.25 (USD), 10.06 (USDA) and 10.04 (USDB) 26NA cG RI$corrected number of counts reported as 4046 {I162} in 2015Si01. 26NA L 407.0 20 2+ 0.18 NS +17-13 A 26NA2 L BE2=0.001039 96 26NA cL $B(E2) from 3+ g.s. to 407 level deduced by evaluators from 26NA2cL experimental B(E2)(W.u.)=3.18 {I29}, branching ratio and 26NA3cL mixing ratio for 407|g 26NA cL T$deduced by evaluators from B(E2)(W.u.) and adopted 407|g properties 26NA G 324 18 S 26NA cG E,RI$from {+14}C({+14}C,d|g) (2006Le17) 26NA G 407 2 100 10 M1+E2 -0.25 12 26NA2 G BM1W=0.15 +42-8 $BE2W=3.18 29 26NA cG $Shell-model predictions for corresponding B(M1)(W.u.) in 2015Si01: 26NA2cG 0.34 (USD), 0.34 (USDA) and 0.32 (USDB) 26NA cG $Shell-model predictions for corresponding B(E2)(W.u.) in 2015Si01: 26NA2cG 11.27 (USD), 7.91 (USDA) and 7.89 (USDB) 26NA cG RI$corrected number of counts reported as 1374 {I137} in 2015Si01. 26NA 26MG(N,P) 1987YE03 16NDS 201604 26NA H TYP=FUL$AUT=M.S. Basunia and A.M. Hurst$CIT=NDS 134, 1 (2016)$ 26NA2 H CUT=1-Feb-2016$ 26NA c 1987Ye03: Primary proton beam from TRIUMF cyclotron was delivered to a 26NA2c {+7}Li production target at the TRIUMF nucleon charge-exchange 26NA3c facility. Breakup neutrons then impinged a {+26}Mg target at 198 MeV 26NA4c and recoiling nuclei were measured at 0|', 5|', 10|', and 15|'. Excited 26NA5c states in {+26}Na observed as distinct groups in the particle-energy 26NA6c spectra. Results compared to Gamow-Teller strength predictions. 26NA7c See also 1986AlZJ. 26NA L 160 26NA cL E$Level is not adopted by evaluators; it is possibly the centroid of a 26NA2cL doublet corresponding to the first two excited states at around 82 and 26NA3cL 233 keV. 26NA L 2860 26NA L 5480 26NA 26MG(7LI,7BE) 1972BA35,1985DO14 16NDS 201604 26NA H TYP=FUL$AUT=M.S. Basunia and A.M. Hurst$CIT=NDS 134, 1 (2016)$ 26NA2 H CUT=1-Feb-2016$ 26NA c 1972Ba35: E({+7}Li)=36 MeV from Chalk River MP tandem accelerator 26NA2c incident upon |?100-|mg/cm{+2} thick {+26}Mg target. Reaction products 26NA3c detected in two solid-state |DE-E detectors positioned at forward 26NA4c (|q<20|') angles. |DE counters of thicknesses 11 |mm and 33 |mm were 26NA5c used together with 100 |mm E and a 2000 |mm anti-coincidence counter. 26NA6c Measured excited states in {+26}Na from particle-energy spectra. 26NA c 1985Do14: E({+7}Li)=88 MeV measured at the Harwell Variable Energy 26NA2c Cyclotron using silicon |DE-E telescopes. Measured differential cross 26NA3c sections compared to one-step DWBA angular distribution predictions 26NA4c using microscopic form factors. 26NA cL E$From particle-energy spectra measured in 1972Ba35. 26NA cL E(A)$From particle-energy spectra measured in 1985Do14. 26NA cL J$From angular distributions and DWBA analysis in 1985Do14. 26NA L 0 3+ 26NA L 210 40 26NA L 430 70 3+ A 26NA cL E$An energy resolution of about 70 keV is quoted in 1985Do14. 26NA L 840 40 26NA L 2210 40 26NA L 4910 40 26NA 26MG(11B,11C) 1974SC26 16NDS 201604 26NA H TYP=FUL$AUT=M.S. Basunia and A.M. Hurst$CIT=NDS 134, 1 (2016)$ 26NA2 H CUT=1-Feb-2016$ 26NA c 1974Sc26: a 750 |mg/cm{+2} {+26}Mg target bombarded by an 86-MeV 26NA2c {+11}B beam at the 88-Inch Cyclotron of the Lawrence Berkeley National 26NA3c Laboratory. Reaction products identified from their time-of-flight 26NA4c (tof) and energy loss using QSD spectrometer. Magnetic rigidity and 26NA5c energy loss measured with position sensitive Borkowski-Kopp 26NA6c proportional counters, TOF measured using a 250-|mg/cm{+2} thick NE 26NA7c 111 scintillator foil. Energy levels deduced in {+26}Na from measured 26NAxc particle spectra. 26NA L 0 26NA L 2.3E+2 15 26NA L 2.10E+3 15 ? 26NA cL E$Ambiguous assignment due to close proximity of excited state in 26NA2cL {+11}C at 1995 keV. 26NA L 4.79E+3 15 ? 26NA cL E$Ambiguous assignment due to close proximity of excited state in 26NA2cL {+11}C at 4794 keV.