ADOPTED LEVELS, GAMMAS for 33Cl
Authors: Jun Chen and Balraj Singh | Citation: Nucl. Data Sheets 199, 1 (2025) | Cutoff date: 30-Sep-2024
Full ENSDF file | Adopted Levels (PDF version)
| Q(β-)=-11619.0 keV 6 | S(n)= 15740.0 keV 7 | S(p)= 2276.8 keV 4 | Q(α)= -6475.4 keV 5 | ||
| Reference: 2021WA16 |
| References: | |||
| A | 33Ar ε decay (174.3 MS) | B | 35Ca ε2p decay (25.7 MS) |
| C | 2H(32S,nγ) | D | 32S(p,γ):RES |
| E | 32S(p,p),(pol p,p):RES | F | 32S(d,n) |
| G | 32S(3He,d) | H | 32S(3He,dγ) |
| I | 35Cl(p,t) | J | 36Ar(p,α) |
| E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
| 0.0 | ABCD FGHIJ | 3/2+ | 2.5059 s 23 % ε = 100 | |||||
| 810.57 15 | A CD FGHIJ | 1/2+ | 1.25 ps 24 | 810.57 16 | 100 | [M1] | 0.0 | 3/2+ |
| 1986.6 4 | D FG IJ | 5/2+ | 53 fs 12 | 1176.0? 1986.5 4 | <6 100 | [E2] M1+E2 | 810.57 0.0 | 1/2+ 3/2+ |
| 2352.02 26 | A D FG IJ | 3/2+ | 69 fs 21 | 1541.5 5 2351.9 3 | 100.0 27 35.1 27 | M1+E2 M1+E2 | 810.57 0.0 | 1/2+ 3/2+ |
| 2685.6 4 | D FG | (5/2)- | 9 ps +15-4 | 699.0 1875.0 2685.5 4 | 100 16 ≤14.5 45 9 | (E1) | 1986.6 810.57 0.0 | 5/2+ 1/2+ 3/2+ |
| 2839.13 30 | D | 5/2+ | 3 fs 1 | 2028.49 2839.0 3 | 1.0 4 100.0 4 | [E2] M1+E2 | 810.57 0.0 | 1/2+ 3/2+ |
| 2846.43 30 | D FG | 3/2- | ≤ 0.7 fs | 2035 15 2846.3 3 | 100 8 85 8 | E1 E1 | 810.57 0.0 | 1/2+ 3/2+ |
| 2975.54 30 | D G I | 7/2+ | 60 fs 14 | 988.9 2975.4 3 | 18 5 100 5 | M1+E2 E2 | 1986.6 0.0 | 5/2+ 3/2+ |
| 3816.34 30 | D | 5/2+ | 840.8 977.2 1464.3 1829.7 3005.62 3816.1 3 | 18.6 23 28 5 100 7 49 7 7.0 23 30 5 | M1+E2 M1+E2 M1+E2 M1+E2 | 2975.54 2839.13 2352.02 1986.6 810.57 0.0 | 7/2+ 5/2+ 3/2+ 5/2+ 1/2+ 3/2+ | |
| 3971.16 20 | A D I | 3/2+ | ≤ 0.3 keV | 1132.0 1619.10 1984.5 3160.43 3970.9 2 | 16 8 16 4 32 4 36 4 100 6 | (M1(+E2)) M1+E2 | 2839.13 2352.02 1986.6 810.57 0.0 | 5/2+ 3/2+ 5/2+ 1/2+ 3/2+ |
| 3979.06 20 | D | 5/2- | < 0.6 keV | 1003.5 1132.6 1139.9 1293.4 1992.4 3978.8 2 | 0.33 22 2.4 5 1.33 33 2.5 5 3.9 6 100.0 11 | M1+E2 (E1(+M2)) M1+E2 (E1(+M2)) | 2975.54 2846.43 2839.13 2685.6 1986.6 0.0 | 7/2+ 3/2- 5/2+ (5/2)- 5/2+ 3/2+ |
| E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
| 4099.5 11 | D | (1/2+,3/2,5/2+) | 1253.0 2112.8 3288.8 4099.2 | 6.7 17 100 7 30 5 30.0 33 | 2846.43 1986.6 810.57 0.0 | 3/2- 5/2+ 1/2+ 3/2+ | ||
| 4112.28 20 | A D | 3/2+ | ≤ 0.6 keV | 3301.53 4112.0 2 | 100 10 100 10 | M1+E2 | 810.57 0.0 | 1/2+ 3/2+ |
| 4118 2 | DEFG | 3/2- | 9.3 keV 15 | 1272 3307 4118 | 1.5 7 100 6 29 6 | 2846.43 810.57 0.0 | 3/2- 1/2+ 3/2+ | |
| 4439.02 20 | A D G | 1/2+ | 2 keV 1 | 1592.6 2086.93 3628.24 4438.7 2 | 1.4 5 8.0 11 4.6 11 100.0 23 | 2846.43 2352.02 810.57 0.0 | 3/2- 3/2+ 1/2+ 3/2+ | |
| 4464.4 4 | A D G | 3/2+ | < 2 keV | 2477.7 3653.6 4464.1 4 | 55 6 57 6 100 9 | 1986.6 810.57 0.0 | 5/2+ 1/2+ 3/2+ | |
| 4516 4 | EF | 1/2- | 55 keV 5 | |||||
| 4746.8 15 | D | 5/2+ | < 2.3 fs | 1771.2 1907.6 2061.1 2394.7 2760.1 3936.0 4746.4 | 14.1 26 1.3 4 0.51 26 2.1 4 10.3 26 0.8 4 100.0 26 | [E2] | 2975.54 2839.13 2685.6 2352.02 1986.6 810.57 0.0 | 7/2+ 5/2+ (5/2)- 3/2+ 5/2+ 1/2+ 3/2+ |
| 4777 3 | DEFG | 7/2- | 0.25 keV 5 | 1801 1931 1938 2091 2790 | <5.7 17 4 100 10 72 10 <1.9 | E2 (E1(+M2)) M1+E2 | 2975.54 2846.43 2839.13 2685.6 1986.6 | 7/2+ 3/2- 5/2+ (5/2)- 5/2+ |
| 4835 2 | A D | 3/2+ | < 2 keV | 2848 4024 4835 | 3.8 21.3 100 | 1986.6 810.57 0.0 | 5/2+ 1/2+ 3/2+ | |
| E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
| 5002 2 | DE | 3/2- | 6.0 keV 20 | 2650 3015 4191 5002 | 19.6 8.7 89 100 | 2352.02 1986.6 810.57 0.0 | 3/2+ 5/2+ 1/2+ 3/2+ | |
| 5090 2 | DE G | 7/2- | ≤ 0.5 keV | 4279 5090 | 41 100 | [E3] | 810.57 0.0 | 1/2+ 3/2+ |
| 5106 2 | A DE | 3/2+ | 1.5 keV 5 | 2754 4295 5106 | 9.3 7 100 | 2352.02 810.57 0.0 | 3/2+ 1/2+ 3/2+ | |
| 5117 15 | EF | 1/2- | 298 keV 31 | |||||
| 5200 50 | I | |||||||
| 5276 2 | DEF | 5/2- | 0.34 keV 6 | 2924 3289 5276 | 22 25 100 | 2352.02 1986.6 0.0 | 3/2+ 5/2+ 3/2+ | |
| 5300 2 | A | (3/2)+ | < 10 keV | |||||
| 5374 2 | E | 5/2+ | 0.44 keV 8 | |||||
| 5448 1 | E | 1/2+ | 30 keV 2 | |||||
| 5548.4 5 | A DE I | 1/2+ | 105 eV 9 | 4737.5 5 5548.0 20 | 100 2 9.5 20 | 810.57 0.0 | 1/2+ 3/2+ | |
| 5555 1 | E G I | 7/2- | 0.73 keV 13 | |||||
| 5651 10 | A EF | 3/2- | 100 keV 10 | |||||
| 5694 9 | A D F | |||||||
| 5734 3 | A E | 1/2+ | 38 keV 5 | |||||
| 5867 3 | A | 1/2+,3/2+ | 1.4 keV 5 | |||||
| 5879 2 | DEFG | 5/2- | 1.50 keV 30 | |||||
| 6149 3 | A DE | 5/2+ | 0.40 keV 10 | |||||
| 6192 3 | DE | 3/2- | 1.0 keV 2 | |||||
| 6203 3 | DE | 3/2+ | 5.0 keV 5 | |||||
| 6247 5 | DE | (3/2-) | 6.5 keV 15 | |||||
| 6255 2 | A DE | 1/2+ | 2 keV 1 | |||||
| E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
| 6290 3 | EFG | 7/2- | 4.0 keV 10 | |||||
| 6314 2 | A D | 1/2,3/2 | ||||||
| 6392 5 | EF | 3/2- | 69 keV 7 | |||||
| 6593 5 | A G | 1/2,3/2 | ||||||
| 6626 3 | DE | 5/2+ | 5 keV 2 | |||||
| 6630 5 | DEF | (5/2)- | 25 keV 3 | |||||
| 6672 9 | D | |||||||
| 6698 3 | E | 5/2+ | 5.5 keV 9 | |||||
| 6850 | DEF | 3/2+ | 0.36 keV 15 | |||||
| 6855 3 | DEF | 3/2+,5/2+ | 30 keV 10 | |||||
| 6901 | D | |||||||
| 6920 3 | E | 5/2- | 20 keV 2 | |||||
| 6949 2 | A D I | 1/2(+),3/2(+) | ||||||
| 6983 3 | DE I | 3/2+ | 10 keV 1 | |||||
| 6993 3 | EF | 5/2- | 7.0 keV 7 | |||||
| 7094 3 | E | 5/2+ | 18 keV 2 | |||||
| 7142 5 | A | 1/2,3/2 | ||||||
| 7178 8 | E | 3/2- | 13.0 keV 13 | |||||
| 7211 4 | DE | 5/2+ | 2.6 keV 5 | |||||
| 7230 40 | D G | 5/2-,7/2- | ||||||
| 7265 6 | DE | 3/2+ | 30 keV 3 | |||||
| 7275 4 | DE | 3/2- | 20 keV 3 | |||||
| 7289 6 | A | (3/2)+ | 10 keV 5 | |||||
| 7301 3 | EF | 9/2+ | 4.0 keV 4 | |||||
| 7323 50 | DEF I | 7/2- | 3.0 keV 3 | |||||
| 7392 2 | DE I | 5/2+ | 108 eV 7 | |||||
| 7399 3 | DE I | 5/2+ | 11.0 keV 11 | |||||
| 7404 10 | A | 1/2,3/2 | ||||||
| 7449 4 | DE | 3/2- | 35.0 keV 35 | |||||
| 7471 3 | DE | 7/2+ | 1.50 keV 15 | |||||
| E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
| 7482 2 | A DE | 1/2+ | 6.5 keV 20 | |||||
| 7490 | F | (1/2-,3/2-) | ||||||
| 7540 4 | A | 1/2+,3/2+ | < 4 keV | |||||
| 7551 2 | A | 1/2+,3/2+ | < 10 keV | |||||
| 7667 4 | A | 1/2+,3/2+ | 8 keV 4 | |||||
| 7720 | D F | (5/2-,7/2-) | ||||||
| 7766 5 | A | (1/2)+ | 10 keV 6 | |||||
| 7930 | F | (5/2-,7/2-) | ||||||
| 8077 3 | A I | 1/2+,3/2+ | 34 keV 6 | |||||
| 8110 | FG I | (5/2-,7/2-) | ||||||
| 8130 3 | A I | 1/2+,3/2+ | ||||||
| 8183 5 | A | (1/2)+ | 22 keV 6 | |||||
| 8290 | FG | (5/2-,7/2-) | ||||||
| 8316 6 | A | 1/2+,3/2+ | ||||||
| 8490 6 | A F | (1/2)+ | ||||||
| 8558 5 | A | (3/2)+ | ||||||
| 8710 50 | G | 5/2-,7/2- | ||||||
| 8813 8 | A | 1/2,3/2 | ||||||
| 8849 5 | A F | 1/2+,3/2+ | ||||||
| 8864 10 | A F | 1/2,3/2 | ||||||
| 8964 8 | A | (1/2)+ | ||||||
| 9117 6 | A | (3/2)+ | ||||||
| 9154 6 | A | (3/2)+ | ||||||
| 9193 9 | A | 1/2+,3/2+ | ||||||
| 9560 | F | (5/2-,7/2-) | ||||||
| 9583 6 | A | 1/2+,3/2+ | ||||||
| 9780 | F | (5/2-,7/2-) | ||||||
E(level): From a least-squares fit to Eγ values with ΔEγ up to 5548 level, from Ep in (p,γ):res or (p,p):res for levels up to 7471 level, and from 33Ar ε+β+ decay for levels above that, unless otherwise noted.
T1/2(level): LABEL=T1/2 or Γ
T1/2(level): Half-lives by DSAM and widths up to 4835 level are from (p,γ):res, widths for levels up to 7471 level are from (p,p):res, and widths for levels above that are from 33Ar ε+β+ decay, unless otherwise noted
| E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
| 810.57 | 1/2+ | 1.25 ps 24 | 810.57 16 | [M1] | B(M1)(W.u.)=0.0331 +75-53 | ||
| 1986.6 | 5/2+ | 53 fs 12 | 1176.0 | [E2] | 4.51×10-5 | B(E2)(W.u.)<55, α=4.51E-5 6 | |
| 5/2+ | 53 fs 12 | 1986.5 4 | M1+E2 | +0.53 6 | 2.68×10-4 | B(E2)(W.u.)=11.7 +41-29, B(M1)(W.u.)=0.040 +12-8, α=2.68E-4 5 | |
| 2352.02 | 3/2+ | 69 fs 21 | 1541.5 5 | M1+E2 | +0.44 4 | 9.99×10-5 | B(E2)(W.u.)=18.0 +83-49, B(M1)(W.u.)=0.054 +23-13, α=9.99E-5 16 |
| 3/2+ | 69 fs 21 | 2351.9 3 | M1+E2 | -1.3 4 | 4.62×10-4 | B(E2)(W.u.)=3.0 +13-11, B(M1)(W.u.)=0.0024 +17-9, α=4.62E-4 18 | |
| 2685.6 | (5/2)- | 9 ps +15-4 | 699.0 | (E1) | B(E1)(W.u.)=1.41E-4 +72-92 | ||
| 2839.13 | 5/2+ | 3 fs 1 | 2028.49 | [E2] | 3.41×10-4 | B(E2)(W.u.)=8.6 +58-37, α=3.41E-4 5 | |
| 5/2+ | 3 fs 1 | 2839.0 3 | M1+E2 | -0.10 2 | 6.06×10-4 | B(E2)(W.u.)=1.6 +11-6, B(M1)(W.u.)=0.31 +15-8, α=6.06E-4 9 | |
| 2846.43 | 3/2- | ≤ 0.7 fs | 2035 15 | E1 | 6.74×10-4 | B(E1)(W.u.)≥0.054, α=6.74E-4 14 | |
| 3/2- | ≤ 0.7 fs | 2846.3 3 | E1 | 1.17×10-3 | B(E1)(W.u.)≥0.017, α=1.17E-3 2 | ||
| 2975.54 | 7/2+ | 60 fs 14 | 988.9 | M1+E2 | +0.31 3 | B(E2)(W.u.)=21.2 +96-71, B(M1)(W.u.)=0.053 +21-16 | |
| 7/2+ | 60 fs 14 | 2975.4 3 | E2 | 7.77×10-4 | B(E2)(W.u.)=5.4 +21-14, α=7.77E-4 15 | ||
| 3816.34 | 5/2+ | 977.2 | M1+E2 | +0.47 16 | |||
| 5/2+ | 1464.3 | M1+E2 | +0.17 4 | 7.51×10-5 | α=7.51×10-5 11 | ||
| 5/2+ | 1829.7 | M1+E2 | -0.22 3 | 1.94×10-4 | α=1.94×10-4 3 | ||
| 5/2+ | 3816.1 3 | M1+E2 | -2.5 3 | 1.09×10-3 | α=1.09×10-3 2 | ||
| 3971.16 | 3/2+ | ≤ 0.3 keV | 3160.43 | (M1(+E2)) | -0.00 2 | ||
| 3/2+ | ≤ 0.3 keV | 3970.9 2 | M1+E2 | +0.50 4 | 1.06×10-3 | α=1.06×10-3 2 | |
| 3979.06 | 5/2- | < 0.6 keV | 1132.6 | M1+E2 | -0.23 8 | ||
| 5/2- | < 0.6 keV | 1139.9 | (E1(+M2)) | -0.03 15 | |||
| 5/2- | < 0.6 keV | 1293.4 | M1+E2 | -0.9 3 | |||
| 5/2- | < 0.6 keV | 3978.8 2 | (E1(+M2)) | -0.01 2 | 1.68×10-3 | α=1.68×10-3 2 | |
| 4112.28 | 3/2+ | ≤ 0.6 keV | 3301.53 | M1+E2 | -0.10 5 | ||
| 4746.8 | 5/2+ | < 2.3 fs | 3936.0 | [E2] | 1.15×10-3 | B(E2)(W.u.)>0.12, α=1.15E-3 2 | |
| 4777 | 7/2- | 0.25 keV 5 | 1938 | (E1(+M2)) | -0.02 2 | ||
| 7/2- | 0.25 keV 5 | 2091 | M1+E2 | +0.21 4 | |||
| E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
Additional Level Data and Comments:
| E(level) | Jπ(level) | T1/2(level) | Comments |
| 810.57 | 1/2+ | 1.25 ps 24 | Γγ=3.7×10-4 eV 6. |
| 1986.6 | 5/2+ | 53 fs 12 | Γγ=0.011 eV 3. |
| 2352.02 | 3/2+ | 69 fs 21 | Γγ=0.007 eV 2. |
| 2685.6 | (5/2)- | 9 ps +15-4 | (2J+1)ΓγΓp/Γ=9×10-5 eV 4 (1976Al01). |
| 2839.13 | 5/2+ | 3 fs 1 | (2J+1)ΓγΓp/Γ=0.08 eV 1 (1976Al01). |
| 2846.43 | 3/2- | ≤ 0.7 fs | (2J+1)ΓγΓp/Γ=0.21 eV 3 (1976Al01). |
| 2975.54 | 7/2+ | 60 fs 14 | XREF: I(2950). |
| 3816.34 | 5/2+ | Γγ>8.8E-3 EV (2J+1)ΓγΓp/Γ=0.053 eV 7 (1976Al01). | |
| 3971.16 | 3/2+ | ≤ 0.3 keV | Γγ=0.23 4 XREF: I(3990). |
| 3979.06 | 5/2- | < 0.6 keV | (2J+1)ΓγΓp/Γ=0.38 keV 4 in (p,γ):res (1976Al01). |
| 4099.5 | (1/2+,3/2,5/2+) | (2J+1)ΓγΓp/Γ=0.019 eV 8. | |
| 4112.28 | 3/2+ | ≤ 0.6 keV | (2J+1)ΓγΓp/Γ=0.07 eV 2 (1976Al01). |
| 4118 | 3/2- | 9.3 keV 15 | XREF: F(4130). Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 4439.02 | 1/2+ | 2 keV 1 | (2J+1)ΓγΓp/Γ=0.30 eV 4 (1976Al01). |
| 4464.4 | 3/2+ | < 2 keV | (2J+1)ΓγΓp/Γ=0.14 eV 2 (1976Al01). T1/2(level): From the measured peak shape of delayed-proton and the calculated recoil broadening in 33Ar ε+β+ decay (1993Sc16). |
| 4516 | 1/2- | 55 keV 5 | XREF: F(4550). Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 4777 | 7/2- | 0.25 keV 5 | XREF: F(4790). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 4835 | 3/2+ | < 2 keV | T1/2(level): From the measured peak shape of delayed-proton and the calculated recoil broadening in 33Ar ε+β+ decay (1993Sc16). |
| 5002 | 3/2- | 6.0 keV 20 | Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 5090 | 7/2- | ≤ 0.5 keV | Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 5106 | 3/2+ | 1.5 keV 5 | Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 5117 | 1/2- | 298 keV 31 | XREF: F(5090). Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 5276 | 5/2- | 0.34 keV 6 | Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 5300 | (3/2)+ | < 10 keV | T1/2(level): From the measured peak shape of delayed-proton and the calculated recoil broadening in 33Ar ε+β+ decay (1993Sc16). |
| 5374 | 5/2+ | 0.44 keV 8 | Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| E(level) | Jπ(level) | T1/2(level) | Comments |
| 5448 | 1/2+ | 30 keV 2 | Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 5548.4 | 1/2+ | 105 eV 9 | T=3/2 IAS of 1/2+ g.s. in 33Ar. E(level): IAS of 1/2+ g.s. in 33Ar. Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 5555 | 7/2- | 0.73 keV 13 | Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 5651 | 3/2- | 100 keV 10 | Jπ,Γ: from R-matrix analysis of σ(θ) data in (p,p). E(level): Jπ,Γ: from R-matrix analysis of σ(θ) data in (p,p). Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 5734 | 1/2+ | 38 keV 5 | Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 5867 | 1/2+,3/2+ | 1.4 keV 5 | T1/2(level): From the measured peak shape of delayed-proton and the calculated recoil broadening in 33Ar ε+β+ decay (1993Sc16). |
| 5879 | 5/2- | 1.50 keV 30 | Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 6149 | 5/2+ | 0.40 keV 10 | XREF: α(6118?). Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 6192 | 3/2- | 1.0 keV 2 | Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 6203 | 3/2+ | 5.0 keV 5 | Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 6247 | (3/2-) | 6.5 keV 15 | Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 6255 | 1/2+ | 2 keV 1 | T1/2(level): From the measured peak shape of delayed-proton and the calculated recoil broadening in 33Ar ε+β+ decay (1993Sc16). |
| 6290 | 7/2- | 4.0 keV 10 | XREF: γ(6250). Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 6314 | 1/2,3/2 | XREF: d(6308). | |
| 6392 | 3/2- | 69 keV 7 | XREF: F(6440). Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 6593 | 1/2,3/2 | XREF: γ(6580). | |
| 6626 | 5/2+ | 5 keV 2 | Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 6630 | (5/2)- | 25 keV 3 | XREF: F(6660). Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 6698 | 5/2+ | 5.5 keV 9 | Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 6850 | 3/2+ | 0.36 keV 15 | T=3/2 Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 6855 | 3/2+,5/2+ | 30 keV 10 | Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 6920 | 5/2- | 20 keV 2 | Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 6949 | 1/2(+),3/2(+) | XREF: d(6938). | |
| 6983 | 3/2+ | 10 keV 1 | T=3/2 Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 6993 | 5/2- | 7.0 keV 7 | XREF: F(6970). Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| E(level) | Jπ(level) | T1/2(level) | Comments |
| 7094 | 5/2+ | 18 keV 2 | Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 7178 | 3/2- | 13.0 keV 13 | Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 7211 | 5/2+ | 2.6 keV 5 | Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 7265 | 3/2+ | 30 keV 3 | Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 7275 | 3/2- | 20 keV 3 | Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 7289 | (3/2)+ | 10 keV 5 | T1/2(level): From the measured peak shape of delayed-proton and the calculated recoil broadening in 33Ar ε+β+ decay (1993Sc16). |
| 7301 | 9/2+ | 4.0 keV 4 | Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 7323 | 7/2- | 3.0 keV 3 | XREF: d(7343). Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 7392 | 5/2+ | 108 eV 7 | T=3/2 (2J+1)ΓγΓp/Γ=1.50 eV 37 (1972Es02). Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 7399 | 5/2+ | 11.0 keV 11 | Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 7449 | 3/2- | 35.0 keV 35 | Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 7471 | 7/2+ | 1.50 keV 15 | Jπ(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). T1/2(level): From analysis of σ(θ) data in (p,p):res using dispersion theory (up to 5448 level) or R-matrix theory (above 5448 level). |
| 7482 | 1/2+ | 6.5 keV 20 | T1/2(level): From the measured peak shape of delayed-proton and the calculated recoil broadening in 33Ar ε+β+ decay (1993Sc16). |
| 7540 | 1/2+,3/2+ | < 4 keV | T1/2(level): From the measured peak shape of delayed-proton and the calculated recoil broadening in 33Ar ε+β+ decay (1993Sc16). |
| 7551 | 1/2+,3/2+ | < 10 keV | T1/2(level): From the measured peak shape of delayed-proton and the calculated recoil broadening in 33Ar ε+β+ decay (1993Sc16). |
| 7667 | 1/2+,3/2+ | 8 keV 4 | T1/2(level): From the measured peak shape of delayed-proton and the calculated recoil broadening in 33Ar ε+β+ decay (1993Sc16). |
| 7720 | (5/2-,7/2-) | XREF: d(7706). | |
| 7766 | (1/2)+ | 10 keV 6 | T1/2(level): From the measured peak shape of delayed-proton and the calculated recoil broadening in 33Ar ε+β+ decay (1993Sc16). |
| 8077 | 1/2+,3/2+ | 34 keV 6 | T=1/2+3/2 T1/2(level): From the measured peak shape of delayed-proton and the calculated recoil broadening in 33Ar ε+β+ decay (1993Sc16). |
| 8110 | (5/2-,7/2-) | XREF: γ(8150). | |
| 8183 | (1/2)+ | 22 keV 6 | T=1/2+3/2 T1/2(level): From the measured peak shape of delayed-proton and the calculated recoil broadening in 33Ar ε+β+ decay (1993Sc16). |
| 8290 | (5/2-,7/2-) | XREF: γ(8350). |
| E(level) | E(gamma) | Comments |
| 810.57 | 810.57 | E(γ): weighted average of 810.6 2 from 33Ar ε+β+ decay, 810.7 3 from (p,γ):res, and 810.51 16 from (3He,dγ) |
| 2352.02 | 1541.5 | E(γ): from 33Ar ε+β+ decay. I(γ): other: 100 9 from 33Ar ε+β+ decay | 2351.9 | E(γ): weighted average of 2352.4 6 from 33Ar ε+β+ decay and 2351.8 3 from (p,γ):res I(γ): other: 35 4 from 33Ar ε+β+ decay |
| 2685.6 | 699.0 | M(γ): d(+Q) with δ=-0.0 6 from γ(θ) in (p,γ):res; Δπ=yes from level scheme; M2 ruled out by RUL. |
| 2846.43 | 2035 | M(γ): from γ(θ) in 1958Va22 and γ(lin pol) in (p,γ):res (1959Su55) | 2846.3 | M(γ): from γ(θ) in 1958Va22 and γ(lin pol) in (p,γ):res (1959Su55) |
| 2975.54 | 2975.4 | M(γ): Q(+O) with δ=-0.09 9 from γ(θ) in (p,γ):res; M2(+E3) and M3 component in E2+M3 ruled out by RUL |
| 3971.16 | 3160.43 | M(γ): d(+Q) from γ(θ) in (p,γ):res; Δπ=no from level scheme |
| 3979.06 | 1139.9 | M(γ): d(+Q) from γ(θ); Δπ=yes from level scheme | 3978.8 | M(γ): d(+Q) from γ(θ); Δπ=yes from level scheme |
| 4746.8 | 3936.0 | M(γ): M2 ruled out by RUL and T1/2<2.3 fs from Γ>0.2 eV of 4747 level deduced from (2J+1)ΓγΓp/Γ=1.4 eV 2 |
| 4777 | 1938 | M(γ): d(+Q) from γ(θ) in (p,γ):res; Δπ=yes from level scheme |
| 5548.4 | 4737.5 | E(γ): weighted average of 4734 3 from 33Ar ε+β+ decay and 4737.6 4 from (p,γ):res |
33Cl first identified and produced in 32S(d,n) reaction at 8 MeV bombarding energy (1940Ho01)
Mass measurement: 2011Tu09, 2003Bl17
Theoretical calculations:
2023Se01: calculated ft value of β decay and magnetic moment.
2008Pe13: calculated magnetic moment, β-decay half-life, gyromagnetic ratio
1974Wi04: calculated σ(θ) and spectroscopic factors of two-nucleon transfer
1970Ba14: calculated levels, J, π, B(E2), B(M1), magnetic and quadrupole moments using vibration-particle coupling model
Q-value: S(2n)=30111 3, S(2p)=11140.7 4, Q(ε)=5582.5 4 (2021Wa16)