28P ADOPTED LEVELS, GAMMAS 13NDS 201310 28P H TYP=FUL$AUT=M. Shamsuzzoha Basunia$CIT=NDS 114, 1189 (2013)$ 28P 2 H CUT=1-Apr-2013$ 28P Q -1.122E4 1614497 262052.3 12-9525.0 15 2012WA38 28P cG E,RI$From (p,n|g), except otherwise noted 28P cG E(A)$From level energy differences. Recoil energy is subtracted. 28P cL E$From ({+3}He,t), except otherwise noted 28P cL E(B)$From (p,n|g) 28P cL J$From ({+3}He,t), based on L values, except otherwise noted 28P cL T$From (p,n|g),(p,n), except otherwise noted 28P XA28S B+ DECAY 28P XC28SI(P,NG),(P,N) 28P XB28SI(3HE,T) 28P PN 6 28P L 0.0 3+ 270.3 MS 5 28P X L XREF=ABC 28P B L MOMM1= 0.3115 34 28P cL MOMM1$From 2010MaZJ and 2011StZZ 28P cL J$From allowed {+28}P |b{++} decay to 2+ and 4+ states in {+28}Si at 28P 2cL 1779 keV and 4618 keV, respectively. 28P cL T$from 1968Ar03 28P 2 L %EC+%B+=100$%ECP=0.0013 4$%ECA=0.00086 25 28P cL %ECP,%ECA$from 1996Og01 28P L 105.64 10 (2+) B 28P X L XREF=BC 28P G 105.64 100 A 28P L 877 2 B 28P X L XREF=BC 28P G 773 3 100 28P L 1134.0 5 (3+) 1.0 PS LT B 28P X L XREF=BC 28P G 1028 4 67 18 28P G 1134 3 100 18 28P L 1313 2 (1+) B 28P X L XREF=BC 28P G 434 2 100 37 28P G 1207 85 37 A 28P L 1516 2 (2+) B 28P X L XREF=BC 28P G 1516 3 100 28P L 1567 3 (1+) B 28P X L XREF=BC 28P G 1461 100 A 28P L 2104 1 (2+) 87 FS LT B 28P X L XREF=BC 28P G 1227 15 LT A 28P G 1998 3 100 18 28P G 2104 5 67 18 28P L 2143 5 (1+) 28P X L XREF=B 28P L 2216 5 (3,4)+ 28P X L XREF=B 28P L 2406 5 (0,1,2)+ 28P X L XREF=B 28P L 2483 5 28P X L XREF=B 28P L 2628 5 (3,4)+ 28P X L XREF=B 28P L 2857 5 28P X L XREF=B 28P L 2896 5 (3,4)+ 28P X L XREF=B 28P L 2973 5 (1+) 28P X L XREF=B 28P L 3164 5 (3,4)+ 28P X L XREF=B 28P L 3200 5 28P X L XREF=B 28P L 3250 5 28P X L XREF=B 28P L 3512 5 (1+) 28P X L XREF=B 28P L 3558 5 28P X L XREF=B 28P L 3728 5 28P X L XREF=B 28P L 3806 5 28P X L XREF=B 28P L 3911 5 (2+) 28P X L XREF=B 28P L 4150 10 28P X L XREF=B 28P L 4180 10 28P X L XREF=B 28P L 4290 10 28P X L XREF=B 28P L 4500 28P X L XREF=B 28P L 4630 10 1+ 28P X L XREF=B 28P cL J$J|p=1+ is assigned in 1997Fu02 from a comparison of ({+3}He,t) 28P 2cL spectrum at 0|' with B(M1) strength in {+28}Si(e,e') experiment. 28P L 4940 10 6- 28P X L XREF=BC 28P cL J$from angular distribution and analyzing power in (p,n) 28P 2cL and (pol p,n). 28P L 4970 10 28P X L XREF=B 28P L 5190 10 28P X L XREF=B 28P L 5900 21 0+ 28P X L XREF=A 28P 2 L ISPIN=2 28P cL J$From {+28}S (J|p=0+) |b{++} Decay feeding (Superallowed transition). 28P 28S B+ DECAY 1989PO10 13NDS 201310 28P H TYP=FUL$AUT=M. Shamsuzzoha Basunia$CIT=NDS 114, 1189 (2013)$ 28P 2 H CUT=1-Apr-2013$ 28P H TYP=ERR$AUT=M.S. Basunia$DAT=1-Feb-2023$COM=Deleted 28P 2 H I(|e+|b{++}) branch to 5900 keV level. 28P c Sum of decay energies of this dataset is 5321 keV {i178} cf. 28P 2c 11220 keV {i160} obtained from {+28}S |b{++} decay Q(g.s.) and 28P xc branching. 28P c {+28}S obtained from {+39}Ar beam bombardment, 85 MeV/u, on a nickel 28P 2c target; isotope separator; heavy ions implanted and identified using a 28P 3c telescope, consists of six silicon detectors; measured |b{++} delayed 28P 4c proton spectrum, relative and absolute intensities, time of flight. 28P cL E,J,T$From Adopted Levels 28S P 0.0 0+ 125 MS 10 1.122E4 16 28P N 1.0 1.0 28P L 0.0 3+ 270.3 MS 5 28P 2 L %EC+%B+=100 28P L 5900 2 0+ 28P 28SI(3HE,T) 1979RA07 13NDS 201310 28P H TYP=FUL$AUT=M. Shamsuzzoha Basunia$CIT=NDS 114, 1189 (2013)$ 28P 2 H CUT=1-Apr-2013$ 28P c J|p({+28}Si)=0+ 28P c Others: 1997Fu02, 1984Ta11, 1982Ta05, 1977Pe02, and 1966Ma18 28P c 1979Ra07: {+28}Si({+3}He,t) E=35 MeV. Measured |s(E,|q), magnetic 28P 2c spectrometer, FWHM 15 keV. 28P cL E$From 1979Ra07 28P cL J$Authors' value in 1979Ra07, except otherwise noted 28P cL L$From angular distribution measurement and DWBA analysis in 1979Ra07 28P L 0 3+ 270.3 MS 5 4 28P cL T$from Adopted Levels 28P L 106 5 2+ 2 28P L 877 5 28P L 1133 5 3+ 4 28P L 1313 5 1+ 0+2 28P L 1516 5 2+ 2 28P L 1569 5 1+ 0+2 28P L 2104 5 2+ 2 28P L 2143 5 1+ 0+2 28P L 2216 5 (3,4)+ 2+4 28P L 2406 5 (0,1,2)+ 2 28P L 2483 5 28P L 2628 5 (3,4)+ 2+4 28P L 2857 5 28P L 2896 5 (3,4)+ 4 28P L 2973 5 1+ 0+2 28P L 3164 5 (3,4)+ 4 28P L 3200 5 28P L 3250 5 28P L 3512 5 1+ 0+2 28P L 3558 5 28P L 3728 5 28P L 3806 5 28P L 3911 5 2+ 2 28P L 4150 10 28P L 4180 10 28P L 4290 10 28P L 4500 28P cL E$Multiplet 28P L 4630 10 1+ 28P cL E,J$4610 keV {i50} in 1997Fu02. J|p=1+ is assigned in 1997Fu02 from a 28P 2cL comparison of ({+3}He,t) spectrum at 0|' with B(M1) strength in 28P 3cL {+28}Si(e,e') experiment. 28P L 4940 10 6- 28P cL J$from 1985Fa06 28P L 4970 10 28P L 5190 10 28P 28SI(P,NG),(P,N) 1977MI01,1972MO02 13NDS 201310 28P H TYP=FUL$AUT=M. Shamsuzzoha Basunia$CIT=NDS 114, 1189 (2013)$ 28P 2 H CUT=1-Apr-2013$ 28P c J|p({+28}Si)=0+ 28P c Others: 1992Ta04, 1991Po05, 1987Ra23, 1985Fa06, 1980Go07, 1976Fr13, 28P 2c 1974Mo06, and 1971Be46 28P c 1977Mi01: {+28}Si(p,n|g), E=23 MeV; two Ge(Li) and NE213 liquid 28P 2c scintillator; Measured E|g, I|g, n-|g coin; deduced excited level 28P 3c energy, upper limit of mean-lifetime using Doppler Shift Attenuation 28P xc method. 28P c 1972Mo02: {+28}Si(p,n|g), E=16, 23 MeV; Ge(Li) detector; measured E|g, 28P 2c I|g, n-|g coin; deduced excited level energy, |g-ray branching ratio. 28P cG E$From 1972Mo02, except otherwise noted 28P cG E(A)$From level energy differences. Recoil energy is subtracted. 28P cG RI$From 1977Mi01, except otherwise noted 28P cG RI(B)$Weighted average of data from 1977Mi01 and 1972Mo02 28P cL E$Level energies are from 1977Mi01, except otherwise noted 28P cL E(C)$From 1972Mo02 28P cL J$From Adopted Levels, except otherwise noted. 28P cL T$From 1977Mi01 using Doppler Shift Attenuation method, 28P 2cL except otherwise noted. 28P PN 6 28P L 0 3+ 270.3 MS 5 28P cL T$from Adopted Levels 28P L 105.64 10 (2+) C 28P G 105.64 100 A 28P L 877 2 28P G 773 3 100 28P L 1134.0 5 (3+) 1.0 PS LT 28P G 1028 4 67 18 B 28P G 1134 3 100 18 B 28P L 1313 2 (1+) 28P G 434 2 100 37 28P G 1207 85 37 A 28P L 1516 2 (2+) 28P G 1516 3 100 28P L 1567 3 (1+) 28P G 1461 100 A 28P L 2104 1 (2+) 87 FS LT 28P G 1227 15 LT A 28P G 1998 3 100 18 B 28P G 2104 5 67 18 B 28P L 4940 10 6- 28P cL E$From Adopted Levels 28P cL J$From angular distribution and analyzing power studies in (p,n) and 28P 2cL (pol p,n) reactions (1985Fa06).