107AG 107CD EC DECAY (6.50 H) 1974PA15 08NDS 200805
107AG H TYP=FUL$AUT=Jean Blachot$CIT=NDS 109, 1383 (2008)$CUT=1-Mar-2008$
107AG c Sources: {+107}Ag(p,n) E(p)=6.0,6.5,7.0 MeV, natural target (1974Pa15)
107AG c Unless otherwise noted, E|g, I|g are from 1974Pa15, semi,
107AG2c |g-singles analysis
107AG c |g|g-coin (see drawings): 1962La10, 1967Bl08, 1974Pa15; see 1974Bu15
107AG2c for analysis of anticoincidence spectra
107AG c |g|g(|q): 1967Bl08, 1969Be75, 1974Pa15
107AG c 1974Pa15 compared E(levels), |d, branching ratios, B(E2), B(M1) with
107AG2c calculation of 1973Pa10 using the model of a three-hole proton
107AG3c cluster coupled to quadrupole vibrations
107AG cE Q(|e)=1417 {I4} from E(|b{++})=302 {I4} to 93 level
107AG cG Unless otherwise noted, E|g, I|g are from 1974Pa15 semi |g
107AGxcG singles
107AG cG M$Based on |a(K)exp, |g|g(|q), and |g(|q) via Coul. ex.
107AG cG M(S)$D+Q from |g(|q). |D|p=no from known J|p's
107AG cG Except as noted, |a(K)exp=ce(K) (1962La10)/I|g(1974Pa15)
107AG2cG normalized to |a(K)(423|g)=0.0089 (E2 theory)
107AG cG I(|g{+|+})/I(829|g)=290 {I15} (1974Pa15). Others: 0.267 {I33}
107AG2cG (1962La10), 0.300 {I10} (1968Bu17)
107AG cG I(K| x ray)/I|g(93|g)=23 {I1} (1974Pa15), 22 {I1} (1962La10)
107AG cG I(K|a| x ray)/I(829|g)=542 {I38}, I(K|b| x ray)/I(829|g)=114
107AGxcG {I8} (1974Pa15)
107AG cL E$Level energy from least-squares adjustment
107CD P 0.0 5/2+ 6.50 H 2 1417 4
107AG N 0.00163 1.0 1.0
107AG cN NR$from I|g(93|g)=4.8% {I3}. This is consistent with I(|g+ce)=100% to
107AG2cN g.s. For log| {If{+1u}t}>8.5, expected for g.s. branch, one gets
107AGxcN I(|e+|b{++})(g.s.)<0.25%
107AG PN 3
107AG G 1264.5 8 0.085 17
107AG G 1294.0 8 0.012 3
107AG cG E$assignment to {+107}Cd decay is tentative.
107AG G 1297.0 4 0.035 5
107AG cG E$assignment to {+107}Cd decay is tentative.
107AG L 0.0 1/2- STABLE
107AG L 93.126197/2+ 44.3 S 2 M1
107AG E 1324 4 0.2 99.7 2 4.94
107AGS E EAV= 141.8 18$CK= 0.8603 $CL= 0.11032 $CM+= 0.02734 $
107AG cE E E|b+=302 {I4} (1962La10) s. Other: 320 {I10} (1945Br04) s
107AG cE |eK/|b{++} exp=320 {I30} (1945Br04) s
107AG G 93.124 202.87E+3 20 E3 20.4
107AG cG RI$I|g is the intensity in equilibrium
107AGS G KC= 9.39 $LC= 8.86 $MC= 1.797 $NC+= 0.322 $
107AG cG E from 1974HeYW. Others: 93.13 {I3} (1974Pa15), 93.16 {I2}
107AGxcG (1978Sh08)
107AG cG RI others: 2290 {I300} (1962La10), 2560 {I180} (1967Bl08),
107AG2cG 2400 {I250} (1974Bu15), 3510 {I300} (1974HeYW)
107AG cG M from |a(K)exp, K/L, L-subshell ratios; see {+107}Ag IT decay
107AGxcG (44.3 s)
107AG L 125.59 3(9/2)+ 2.85 NS 10
107AG cL T$from 1972Ja01 (796|g)(32|g,K| x ray)(t) scin. Others: 13 ns {I6}
107AG2cL (1962La10), <1 ns (1969Be75)
107AG G 32.46 2 2.9 3 M1+E2 0.074 14 11.6 2 C
107AGS G KC= 9.61 4$LC= 1.46 11$MC= 0.280 22$
107AG cG E from 1976Sv04. Others: 32.3 {I1} (1974Pa15), 32.6 {I4}
107AGxcG (1962La10)
107AG cG MR from L1:L2:L3=100 {I8}:17 {I4}: <14 (1976Sv04)
107AG cG |a(K)exp=10.1 {I4} from I(K| x ray)/I|g(32|g) via
107AGxcG (796|g)(32|g)-coin (1974Pa15)
107AG cG (796|g)(32|g)-coin: I(K| x ray)/I|g(32|g)=20 {I8}
107AG2cG (1962La10), 18.0 {I13} (1974Pa15)
107AG L 324.81 33/2-
107AG E 0.005 9.1
107AGS E CK= 0.8612 $CL= 0.11123 $CM+= 0.02759 $
107AG G 324.81 3 18.8 9 M1+E2 -0.207 10 0.0180 2 C
107AGS G KC=0.0157 $LC=0.00190 $MC=0.00036 $
107AG cG E$from 1974HeYW. Other: 324.8 {I1} (1974Pa15)
107AG cG RI$others: 18 {I1} (1967Bl08), 16 {I2} (1974Bu15), 20 {I2} (1974HeYW)
107AG cG MR$from 325|g(|q) Coul. ex. (1970RoZS). Other: 0.205 {I6} (1977Kr13)
107AG3 G EKC=0.0165 21
107AG L 423.150245/2-
107AG cL Branching: I|g(98|g)/I|g(423|g)=0.10 {I2} (1967Bl08), <0.11
107AG2cL (1974Pa15), 0.09 {I3} (1979Sc30) via ({+6}Li,3n|g); see Coul. ex.
107AG E 0.021 8.4
107AGS E CK= 0.8607 $CL= 0.11161 $CM+= 0.02770 $
107AG G 98.2 5 0.83 10(M1+E2) -0.059 18 0.449 3 S
107AGS G KC= 0.3892 20$LC= 0.0488 7$MC=0.00925 13$NC+=0.00185 $
107AG cG E$from Coul. ex. (1970Ro14). Other: 98.2 (1974Pa15)
107AG cG RI$from branching: I|g(98|g)/I|g(423|g)=0.046 {I5} (1970Ro14, Coul.
107AGxcG ex.)
107AG cG MR$from 98|g(|q) Coul. ex. (1970Ro14)
107AG G 423.150 25 18.0 9 E2 0.0104 C
107AGS G KC=0.00893 $LC=0.00118 $MC=0.00023 $
107AG cG E$from 1974HeYW. Other: 423.0 {I1} (1974Pa15)
107AG cG RI$others: 18.1 {I30} (1962La10), 18.6 {I17} (1974HeYW)
107AG cG |a(K)exp=0.0095 {I12} if normalized to |a(K)(93|g)=9.4 (E3
107AGxcG theory)
107AG L 786.4713 3/2-
107AG cL Branching: I|g(786|g)/I|g(462|g)/I|g(364|g)=100/40 {I7}/<15
107AG2cL (1974Pa15), 100/44 {I9}/12 {I6} (1970Ro14, Coul. ex.)
107AG E 0.002 9.0
107AGS E CK= 0.8574 $CL= 0.11414 $CM+= 0.02843 $
107AG G 364.0 0.15 LT ?
107AG G 461.7 4 0.40 6 (M1+E2) -0.01 8 C
107AG3 G FLAG=S
107AG cG MR$|d from |g(|q) in Coul. ex. (1974Ro14)
107AGS G KC=0.00649 $LC=0.00077 $MC=0.00015 $
107AG G 786.45 15 1.0 1 (M1+E2) -0.057 10 S
107AG cG MR$|d from |g(|q) in Coul. ex. (1974Ro14)
107AGS G KC=0.00185 $LC=0.00022 $
107AG cG E from 1974HeYW. Other: 786.7 {I1} (1974Pa15)
107AG L 922.06 35/2+ 0.6 NS LE
107AG cL T from 1969Be75 (K| x ray)(829|g)(t)
107AG cL Branching: I|g(829|g)/I|g(797|g)/I|g(597|g)=100/40 {I1}/4.6
107AG2cL {I3} (1974Pa15), 100/40 {I4}/5.3 {I6} (1974HeYW), 100/38 {I14}/4.6
107AGxcL {I8} (1962La10)
107AG E 0.23 6.7
107AGS E CK= 0.8549 $CL= 0.11609 $CM+= 0.02899 $
107AG G 597.27 6 4.65 25 E1 C
107AGS G KC=0.00116 $LC=0.00013 $
107AG cG E$from 1974HeYW. Other: 597.3 {I1} (1974Pa15)
107AG3 G EKC=0.00135 26
107AG G 796.462 25 39.8 12 (E2) C
107AG cG M$|a(K)exp is consistent with M1 or E2; level scheme requires E2.
107AGS G KC=0.00159 $LC=0.00019 $
107AG cG E$from 1974HeYW. Other: 796.7 {I1} (1974Pa15)
107AG3 G EKC=0.0018 2
107AG G 828.934 30 100 M1 C
107AGS G KC=0.00164 $LC=0.00019 $
107AG cG E$from 1974HeYW. Other: 829.0 {I1} (1974Pa15)
107AG3 G EKC=0.0018 2
107AG L 949.70 75/2-
107AG cL Branching: I|g(950|g)/I|g(856|g)/I|g(625|g)/I|g(526|g)=29
107AG2cL {I3}/2.0 {I4}/78 {I7}/100 (1974Pa15), 24 {I2}/1.8 {I8}/78 {I5}/100
107AGxcL (1970Ro14, Coul. ex.)
107AG E 0.009 8.1
107AGS E CK= 0.8542 $CL= 0.11664 $CM+= 0.02915 $
107AG G 526.5 1 2.75 16 M1+E2 -0.24 3 C
107AGS G KC=0.00472 $LC=0.00056 $
107AG cG MR$from 526|g(|q) Coul. ex. (1970Ro14). Others: -0.25 {I3}
107AG2cG (1969Ro03), -0.17 +7 -10 (1974Pa15), -0.18 {I3} (1977Kr13)
107AG3 G EKC=0.0058 9
107AG G 624.91 10 2.15 13 M1+E2 -0.28 3 C
107AGS G KC=0.00313 $LC=0.00037 $
107AG cG E$from 1974HeYW. Other: 625.0 {I1} (1974Pa15)
107AG cG MR$from 625|g(|q) Coul. ex. (1970Ro14). Other: 0.24 {I3} (1977Kr13),
107AG2cG -0.09 {I6} (1974Pa15) via (625|g)(325|g)(|q)
107AG3 G EKC=0.0048 8
107AG cG M$the |a(K)exp is discrepant with M1 or E2 theory values.
107AG G 856.5 4 0.055 10
107AG G 949.8 2 0.80 8 E2
107AGS G KC=0.00105 $LC=0.00013 $
107AG cG M consistent with 950|g(|q) Coul. ex. (1970Ro14)
107AG cG |a(K)exp=0.0019 {I5}
107AG L 973.1 3 (7/2)-
107AG E 0.001 9.0
107AGS E CK= 0.8535 $CL= 0.11716 $CM+= 0.02930 $
107AG G 549.9 4 0.55 6 C
107AG G 648.4 4 0.11 2
107AG L 1143.06 7(5/2)-
107AG E 0.006 7.7
107AGS E CK= 0.8448 $CL= 0.1239 3$CM+= 0.03126 8$
107AG G 356.4 4 0.21 3
107AG G 719.93 10 2.20 15 M1+E2 -1.1 2 C
107AGS G KC=0.00214 $LC=0.00026 $
107AG cG E$from 1974HeYW. Other: 720.0 {I1} (1974Pa15)
107AG cG MR$(720|g)(423|g)(|q): -1.1 {I2} (1974Pa15), -0.9 {I4} (1967Bl08).
107AG2cG Other: 1977Kr13
107AG3 G EKC=0.0029 6
107AG G 818.23 10 1.25 15 (M1+E2) C
107AG3 G FLAG=S
107AG cG E from 1974HeYW. Other: 818.5 {I4} (1974Pa15)
107AG cG MR +2.0 {I+2-5} or +0.26 {I+14-11} (1974Pa15)
107AG2cG via (818|g)(325|g)(|q)
107AG cG Doublet |a(K)exp=0.007 {I3}, E(ce(K) 818|g)=E(ce(L) 796|g)
107AG G 1050.0 4 0.12 2
107AG G 1143.0 4 0.015 LT
107AG L 1223.00 5(5/2)+
107AG cL $Branching: I|g(1130|g)/I|g(1097|g)/I|g(898|g)/I|g(800|g)/
107AG2cL I|g(\437|g)/I|g(301|g)= 74 {I4}/20 {I2}/100/20 {I2}/2.7 {I4}/27 {I2}
107AG3cL (1974Pa15), 72 {I11}/20 {I3}/100/30 {I5}/--/30 {I4} (1974HeYW)
107AG E 0.024 6.8
107AGS E CK= 0.8345 $CL= 0.1319 6$CM+= 0.03360 18$
107AG G 300.9 1 1.6 1 M1(+E2) 0.63 LT 0.022 C
107AG cG E other: 300.88 {I10} (1974HeYW)
107AG3 G EKC=0.018 3
107AG G 436.6 4 0.16 2
107AG G 799.92 15 1.2 1 C
107AG cG E from 1974HeYW. Other: 800.0 {I4} (1974Pa15)
107AG G 898.17 6 5.95 25 E1 C
107AGS G KC=0.00049 $
107AG cG E from 1974HeYW. Other: 898.3 {I1} (1974Pa15)
107AG3 G EKC=0.00058 20
107AG G 1097.5 2 1.2 1
107AG G 1129.9 1 4.4 2 M1,E2
107AG3 G EKC=0.0010 3
107AG G 1223.0 4 0.001 LT
107AG L 1258.8924(3/2)+
107AG E 0.0005 8.3
107AGS E CK= 0.8257 13$CL= 0.1387 10$CM+= 0.0356 3$
107AG G 934.0 4 0.045 10
107AG G 1165.7 4 0.25 4
107AG G 1259.0 4 0.030 6
107AG L 1325.8 3(3/2)+
107AG E 0.0005 7.7
107AGS E CK= 0.783 6$CL= 0.172 5$CM+= 0.0454 13$
107AG G 1232.6 4 0.29 6
107AG G 1325.8 4 0.050 8