161DY 161HO EC DECAY 1984VY01 11NDS 201111
161DY H TYP=FUL$AUT=C. W. Reich$CIT=NDS 112,2497 (2011)$CUT=1-Jun-2011$
161DY D DATA SET UPDATED (NOVEMBER, 2009) BY CW REICH TO INCLUDE REVISED QP
161DY2D VALUE, CC VALUES FROM BRICC AND SLIGHTLY MODIFIED COMMENTS.
161DY D DATA SET UPDATED (SEPT.-NOV.,1999) BY CW REICH TO INCLUDE ECK VALUES
161DY2D OF 1993Mu17, NEW Q+ VALUE AND RECALCULATED EC-RELATED INFORMATION
161DY3D AND NEW LEVEL ENERGY FOR 366.9 LEVEL AND QUESTIONABLE ASSIGNMENT
161DY4D FOR 84.86 G FEEDING IT. THE MR DATA HAVE BEEN EXTENSIVELY RE-DONE.
161DY D Experimental methods:
161DY D 1950Wi13: 161HO from TB(A,X) and DY(P,X). Half-life measured.
161DY D 1954Ha01: 161HO from ER(P,X) with chemistry to obtain 161ER, followed
161DY2D by its decay (Handley and Olson).
161DY D 1954HaAB: 161HO from (P,X) reactions with chemistry to obtain 161ER
161DY2D followed by its decay. Half-life measured (Handley).
161DY D 1959Ha09: 161HO from 162ER(P,2N) reaction and EC decay of 161TM and
161DY2D 161ER. CE studied in magnetic spectrographs.
161DY D 1961Ab04: 161HO from 660-MeV p spallation of tantalum target with
161DY2D chemical separation of 161ER followed by its decay. CE's measured
161DY D in magnetic spectrograph.
161DY D 1961Ba32: 161HO from p spallation of Ta target with chemistry. CE's
161DY2D measured in lens spectrometer. Only one line observed.
161DY D 1961Bj02: 161HO from ER(P,XN)161TM reaction followed by decay with
161DY2D chemical and isotope separation.
161DY D 1963Ra15: Measured p-induced cross sections; report 161HO half-life.
161DY D 1964Ma10: Measured p-induced cross sections; report several G lines.
161DY D 1964Bu09: Measured J of 161HO ground state by atomic-beam, magnetic
161DY2D resonance.
161DY c 1965Ab04: {+161}Ho from 660-MeV p spallation of Ta target with chemical
161DY2c separation. ce's studied in magnetic spectrograph with source
161DY3c containing Er, Ho, and their daughters. |g spectra measured
161DY4c with NaI detector and Ho sample. |a(K)exp values were normalized to
161DY5c the theoretical E2 value for the 175 |g, whose multipolarity was
161DY6c established from L subshell ratios.
161DY D 1965St08: 161HO from 75-MeV p bombardment of Ho target with chemical
161DY2D separation of 161ER followed by its decay. CE studied in
161DY3D magnetic spectrometer.
161DY D 1967HaAA: P. G. Hansen talk reported by 1984Vy01.
161DY D 1969Ve05: 161HO from ER(D,XN)TM reaction with E(D)=52 MeV and
161DY2D decay of 161TM and 161ER. Level half-life measured with NaI
161DY3D detectors.
161DY D 1973BuZR: Conference abstract. 161HO from 660-MeV p spallation of Ta
161DY2D target with chemical and isotope separation to provide source of
161DY3D 161ER and 161HO. G spectra measured.
161DY D 1975Gr44: Summary of laboratory program. No experimental details.
161DY D 1975VaYX: Half-lives of 44 and 103 levels in JINR-D6-8846 (1975).
161DY2D Have not seen copy, but values were given elsewhere. Are these
161DY3D data related to 1978AlZC?
161DY D 1978AlZC: Half-lives of several levels; probably 161HO EC decay.
161DY D 1981GrZV: Conference abstract. Report G multipolarities and level
161DY2D half-lives; the latter are assumed to be calculated. The
161DY3D evaluator assumes that the G data are superseded by 1984Vy01.
161DY D 1983VyZV: Conference abstract; see 1984Vy01 for published version.
161DY c 1984Vy01: {+161}Ho from 660-MeV p spallation of a Ta target with
161DY2c chemical and isotopic separation. |g's were measured with Ge detectors
161DY3c and ce with magnetic spectrometers. X-|g coincidences were
161DY4c measured.
161DY D 1986SoAA: Tallies LOGFT values for allowed, unhindered beta decays.
161DY c 1987BaZB: deduce |d values for 25.6 and 77.4 gammas from L-subshell
161DY2c ratios measured using a magnetic |b spectrograph.
161DY cG Data are from 1984Vy01, unless noted otherwise.
161DY cG E,RI From 1984Vy01. Others: 1965Ab04, 1965St08.
161DY cG RI I(K x ray)=2420 {I170}
161DY cG M,MR From the Adopted Gammas data set. The data types are |a,
161DY2cG L- and M-subshell ratios, |g(|q), and |g|g(|q). See the Adopted
161DY3cG Gammas data set for comments on specific cases.
161DY cG TI(W) Computed by evaluator from electron intensities (1984Vy01)
161DY2cG and conversion coefficients.
161DY cL Data are from 1984Vy01, unless noted otherwise. Level
161DY2cL structure is also known from the |b{+-} decay of {+161}Tb and reaction
161DY3cL studies.
161DY cL E From least-squares fit to |g energies.
161DY cL J From Adopted Levels. In this data set, the values are based
161DY2cL on the |g multipolarities, |g decay modes, and band-structure
161DY3cL considerations.
161DY cL T Information given here is only from this decay mode. See
161DY2cL Adopted Levels for results from all decay modes.
161DY DL Levels are 5/2(0), 7/2(43), 9/2(100), and 11/2(184).
161DY DL Levels are 5/2(25), 7/2(103), 9/2(200), and 11/2(320).
161DY DL Levels are 3/2(74), 5/2(131), 7/2(212), and 9/2(314).
161DY DL Levels are 1/2(366) and 5/2(451).
161DY DL Level is 5/2(790).
161DY CL BAND(A) GROUND-STATE BAND. CONF=5/2[642]
161DY CL BAND(B) 5/2[523] band
161DY CL BAND(C) 3/2[521] band
161DY CL BAND(D) 1/2[521] band
161DY CL BAND(F) BANDHEAD OF THE 5/2[512] BAND.
161HO P 0 7/2- 2.48 H 5 858.3 22
161HO DP J J measured by atomic-beam, magnetic resonance (1964Bu09).
161HO DP T From 161HO Adopted Levels. Weighted average of four values,
161HO2DP which is dominated by 2.48 H 5 (1965Ab04).
161HO DP QP From 2009AuZZ. 2003Au03 report this same value. From
161HO2DP K x ray-G coincidences to 790 level, 1984Vy01 report QP=863 6. Also
161HO3DP reported as 855 20 by 1975Gr44, but with no supporting data.
161DY N 0.039 6 0.039 6 1.00 1.00
161DY cN NR I|g normalization by 1984Vy01 to give 100% feeding to the
161DY2cN ground state, assuming no capture to the ground state. If the |e
161DY3cN transition to the g.s. has log| {Ift}|>5.9, the deduced I|e is <10%.
161DY PN 3
161DY G 252 0.005 LE
161DY G 728.2 0.025 LE
161DY L 0 5/2+ STABLE A
161DY L 25.656 3 5/2- 28.6 NS 4 B
161DY cL T weighted average of: 27.8 ns 15 (1969Ve05); 28.6 ns 5
161DY2cL (1978AlZC); and 29.0 ns 14 (1975VaYX). The 0.2 ns uncertainty from
161DY3cL 1978AlZC was increased to 0.5 ns (see the comment on this point in
161DY4cL the Adopted Levels data set).
161DY E 76 14 4.88 8 76 14
161DYS E CK=0.8250 $CL=0.1349 $CM+=0.04013
161DY cE 1993Mu17 measure |eK(exp) (i.e., P{-K}) to be 0.814 {I23},
161DY2cE in good agreement with the theoretical value of 0.825.
161DY G 25.655 3 7.0E+2 7 E1 2.29
161DYS G LC=1.79 3$MC=0.399 6$NC+=0.0984 14
161DYS G NC=0.0877 13$OC=0.01035 15$PC=0.000297 5
161DY L 43.806 18 7/2+ 0.99 NS 13 A
161DY cL T from 1975VaYX. Others: 1.0 ns 2 (1978AlZC) and 0.76 ns
161DY2cL (1981GrZV).
161DY E 2.5 9 6.34 16 2.5 9
161DYS E CK=0.8246 $CL=0.1351 $CM+=0.04023
161DY G 18.15 5 E1 5.93 10 24 6 W
161DYS G L/T=0.668 7$M/T=0.151 3$N+/T=0.0364 8
161DYS G N/T=0.0327 7$O/T=0.00360 8$P/T=9.00E-5 19
161DY cG RI measured value is |<7 (1984Vy01). The value computed from
161DY2cG I(ce) is 3.3 {I9}.
161DY G 43.80 3 10 2 M1+E2 0.216 8 7.7 3
161DY3 G M1/M3=1.65 17 (1984Vy01) $ M1/M2=1.91 21 (1984Vy01)
161DY4 G L1/L2=1.8 5 (1984Vy01)
161DYS G LC=5.95 21$MC=1.36 5$NC+=0.352 13
161DYS G NC=0.310 12$OC=0.0409 14$PC=0.001340 20
161DY cG MR$1984Vy01 report %E2=4.5 {I2} from L- and M-subshell ratios.
161DY L 74.566 8 3/2- C
161DY G 48.86 2 3.0 9 M1+E2 -0.056 1 3.20
161DYS G LC=2.50 4$MC=0.552 8$NC+=0.1468 21
161DYS G NC=0.1273 18$OC=0.0184 3$PC=0.001006 15
161DY cG M deduced penetration parameter is |l=+2.5 {I23}
161DY2cG (1982Bh07,1985Bh08). These authors derive |d{+2}=0.0036 {I2} in their
161DY3cG analysis.
161DY G 74.577 9 3.0 3 E1 0.672
161DYS G KC=0.556 8$LC=0.0909 13$MC=0.0200 3$NC+=0.00514 8
161DYS G NC=0.00451 7$OC=0.000603 9$PC=2.46E-5 4
161DY cG MR |d=0.00 {I3}; average of -0.006 {I20} (1983Ri15), 0.06
161DY2cG {I+3-6} (1966Su03), and +0.08 {I10} (1971Kr19).
161DY L 100.41 3 9/2+ 0.1 NS A
161DY cL T from 1981GrZV.
161DY E 0.117 19 7.61 8 0.117 19
161DYS E CK=0.8233 $CL=0.1361 $CM+=0.04058
161DY G 56.64 3 M1+E2 0.22 3 12.91 254.0 9 W ?
161DYS G K/T=0.715 10$L/T=0.166 13$M/T=0.038 4$N+/T=0.0098 10
161DYS G N/T=0.0086 9$O/T=0.00117 10$P/T=4.54E-5 12
161DY cG RI measured value is |<0.7 (1984Vy01). The value computed from
161DY2cG I(ce) is 0.28 {I6}
161DY cG MR computed by the evaluator from the L-subshell ratios of
161DY2cG 1984Vy01. The listed |d value implies a %E2 value somewhat different
161DY3cG from that reported by these authors.
161DY G 100.39 5 1.4 LE(E2) 2.67
161DYS G KC=1.112 16$LC=1.201 17$MC=0.287 4$NC+=0.0723 11
161DYS G NC=0.0645 10$OC=0.00775 11$PC=4.61E-5 7
161DY cG RI value includes the contribution from the 100.64 |g.
161DY L 103.067 14 7/2- 0.60 NS 4 B
161DY cL T weighted average of 0.64 ns 3 (1978AlZC) and 0.55 ns 3
161DY2cL (1975VaYX); other: 0.61 ns (1981GrZV).
161DY E 19 4 5.39 10 19 4
161DYS E CK=0.8232 $CL=0.1362 $CM+=0.04060
161DY cE 1993Mu17 measure |eK(exp) (i.e.,P{-K}) to be 0.84 {I4}, in
161DY2cE good agreement with the theoretical value of 0.823.
161DY G 59.23 30 15.5 13E1 1.221 24
161DYS G KC=0.999 19$LC=0.173 4$MC=0.0381 8$NC+=0.00975 20
161DYS G NC=0.00858 18$OC=0.001126 23$PC=4.32E-5 8
161DY cG M from L-subshell ratios (1984Vy01)
161DY G 77.42 4 49 4 M1+E2 -1.050 8 6.15
161DYS G KC=3.03 5$LC=2.41 4$MC=0.572 9$NC+=0.1444 22
161DYS G NC=0.1285 20$OC=0.01569 24$PC=0.0001691 25
161DY3 G L1/L2=0.368 22 $ L1/L3=0.35 2 $ L2/L3=0.95 4
161DY cG L1/L2,L1/L3,L2/L3 $subshell ratios are from 1984Vy01.
161DY cG MR from the L-subshell ratio data of 1984Vy01, the evaluator
161DY2cG calculates |d{+2}=1.106 {I21}, in agreement with their reported
161DY3cG %E2=53.7 {I43}. From the L-subshell ratios of 1987BaZB, the evaluator
161DY4cG calculates |d{+2}=1.094 {I36}, giving essentially the same %E2 value as
161DY5cG that given by them. From the L-subshell ratios of 1965Ab04, the
161DY6cG evaluator calculates |d{+2}=1.1 {I7}. 1986GrZQ report %E2=48.0 {I13},
161DY7cG but do not show the data from which this value was derived.
161DY G 103.05 2 100 E1 0.285
161DYS G KC=0.238 4$LC=0.0368 6$MC=0.00806 12$NC+=0.00209 3
161DYS G NC=0.00183 3$OC=0.000250 4$PC=1.102E-5 16
161DY L 131.764 9 5/2- 0.13 NS C
161DY cL T from 1981GrZV
161DY E 0.60 20 6.86 15 0.60 20
161DYS E CK=0.8224 $CL=0.1368 $CM+=0.04080
161DY G 28.68 3 M1+E2 0.036 +8-10 15.6 5 4.9 8 W
161DYS G L/T=0.734 15$M/T=0.162 7$N+/T=0.0431 18
161DYS G N/T=0.0374 16$O/T=0.00540 21$P/T=0.000293 10
161DY cG RI measured value is |<2 (1984Vy01). The value computed from
161DY2cG I(ce) is 0.31 {I5}.
161DY cG MR this value is somewhat different from the value derived
161DY2cG from %E2=0.25 {I+15-11}, which is that reported by 1984Vy01 from
161DY3cG L-subshell ratios.
161DY G 57.200 5 1.4 3 M1+E2 -0.187 16 12.39 19
161DYS G KC=9.78 15$LC=2.03 10$MC=0.459 23$NC+=0.120 6
161DYS G NC=0.105 5$OC=0.0145 6$PC=0.000619 10
161DY cG M deduced penetration parameter is |l=-5 {I5} (1965Su04,
161DY2cG 1966Su03, and 1983Hn01) from
161DY3cG |l=-7 {I+6-8} (1965Su04,1966Su03) and |l=-4.0 {I42} (1983Hn01).
161DY4cG Values of |d=-0.22 and |d=-0.20, respectively, were used in these
161DY5cG authors' analyses.
161DY cG MR from L-subshell ratios, 1984Vy01 report %E2=3.2 {I13}. This
161DY2cG is somewhat different from that implied by |d{+2}=0.038 {I11},
161DY3cG computed by the evaluator from their reported L-subshell ratios.
161DY G 87.93 3 0.31 15(E1) 0.435
161DYS G KC=0.362 5$LC=0.0573 8$MC=0.01257 18$NC+=0.00325 5
161DYS G NC=0.00285 4$OC=0.000385 6$PC=1.638E-5 23
161DY G 106.23 5 M1+E2 -0.85 35 2.08 5 0.33 6 W
161DYS G K/T=0.45 3$L/T=0.17 4$M/T=0.041 12$N+/T=0.010 3
161DYS G N/T=0.009 3$O/T=0.0012 3$P/T=2.5E-5 5
161DY cG RI measured value is |<0.25 (1984Vy01). The value computed
161DY2cG from I(ce) is 0.11 {I2}.
161DY G 131.8 0.03 LE ?
161DY cG E placement doubtful, since J|p value requires E1, while the
161DY2cG data suggest otherwise.
161DY L 184.23 5 11/2+ A
161DY G 83.83 5 M1+E2 -0.25 7 4.05 8 0.24 6 W
161DYS G K/T=0.643 6$L/T=0.124 14$M/T=0.028 4$N+/T=0.0073 10
161DYS G N/T=0.0064 9$O/T=0.00089 10$P/T=3.97E-5 13
161DY cG RI measured value is |<0.25 (1984Vy01). The value computed
161DY2cG from I(ce) is 0.05 {I1}.
161DY G 140.4 1 0.06 LE[E2] 0.795
161DYS G KC=0.448 7$LC=0.267 4$MC=0.0634 10$NC+=0.01604 23
161DYS G NC=0.01427 21$OC=0.00175 3$PC=1.97E-5 3
161DY L 201.077 19 9/2- 0.17 NS B
161DY cL T from 1981GrZV; others: |<0.3 ns (1975VaYX,1978AlZC)
161DY E 1.8 3 6.29 8 1.8 3
161DYS E CK=0.8203 $CL=0.1384 $CM+=0.04136
161DY G 69.29 5 (E2) 11.19 1.5 4 W
161DYS G K/T=0.191 4$L/T=0.559 7$M/T=0.1343 25$N+/T=0.0336 7
161DYS G N/T=0.0300 6$O/T=0.00356 7$P/T=8.70E-6 17
161DY cG RI measured value is |<0.1 (1984Vy01). The value computed
161DY2cG from I(ce) is 0.12 {I4}.
161DY G 98.02 2 3.9 3 M1+E2 0.9 2 2.71 6
161DYS G KC=1.71 12$LC=0.77 13$MC=0.18 3$NC+=0.046 8
161DYS G NC=0.041 7$OC=0.0052 8$PC=9.5E-5 10
161DY cG MR computed by the evaluator from L1/L2=0.67 {I20}, as reported
161DY2cG by 1984Vy01. 1965Ab04 report L1/L2=0.65, which leads to |d=0.96.
161DY G 100.64 5 1.4 LE(E1) 0.303
161DYS G KC=0.253 4$LC=0.0393 6$MC=0.00861 13$NC+=0.00223 4
161DYS G NC=0.00196 3$OC=0.000267 4$PC=1.169E-5 17
161DY cG RI value includes the contribution from the 100.39 |g.
161DY G 157.26 6 12.5 10E1 0.0919
161DYS G KC=0.0773 11$LC=0.01142 16$MC=0.00250 4$NC+=0.000653 10
161DYS G NC=0.000570 8$OC=7.95E-5 12$PC=3.80E-6 6
161DY G 175.42 5 11.1 10E2 0.368
161DYS G KC=0.234 4$LC=0.1030 15$MC=0.0243 4$NC+=0.00617 9
161DYS G NC=0.00548 8$OC=0.000684 10$PC=1.082E-5 16
161DY L 212.940 24 7/2- 0.066 NS C
161DY cL T from 1981GrZV
161DY E 0.35 7 6.98 9 0.35 7
161DYS E CK=0.8199 $CL=0.1387 $CM+=0.04147
161DY G 81.23 4 1.4 2 M1+E2 0.18 3 4.40
161DYS G KC=3.60 6$LC=0.62 3$MC=0.139 8$NC+=0.0368 19
161DYS G NC=0.0320 17$OC=0.00454 19$PC=0.000224 4
161DY cG MR from L-subshell ratios (1984Vy01).
161DY G 109.83 4 (M1) 1.83 0.18 6 W
161DYS G K/T=0.544 5$L/T=0.0800 13$M/T=0.0176 3$N+/T=0.00470 8
161DYS G N/T=0.00407 7$O/T=0.000595 10$P/T=3.39E-5 6
161DY cG RI measured value is |<0.038 (1984Vy01). The value computed
161DY2cG from I(ce) is 0.06 {I2}.
161DY G 112.52 5 0.090 15E1 0.225
161DYS G KC=0.188 3$LC=0.0288 4$MC=0.00631 9$NC+=0.001639 23
161DYS G NC=0.001434 21$OC=0.000197 3$PC=8.84E-6 13
161DY G 138.39 5 0.45 4 E2 0.836
161DYS G KC=0.467 7$LC=0.285 4$MC=0.0676 10$NC+=0.01709 24
161DYS G NC=0.01520 22$OC=0.00186 3$PC=2.04E-5 3
161DY G 187.3 2 0.043 7 M1,E2 0.35 6
161DYS G KC=0.27 8$LC=0.064 15$MC=0.015 4$NC+=0.0038 9
161DYS G NC=0.0034 9$OC=0.00045 8$PC=1.5E-5 7
161DY G 212.80 15 0.024 8 E1 0.0413
161DYS G KC=0.0349 5$LC=0.00504 8$MC=0.001101 16$NC+=0.000290 4
161DYS G NC=0.000252 4$OC=3.56E-5 5$PC=1.78E-6 3
161DY L 314.77 10 9/2- C
161DY E 0.0082 19 8.45 11 0.0082 19
161DYS E CK=0.8154 $CL=0.1420 $CM+=0.04263
161DY G 102.0 ?
161DY G 183.0 1 0.21 3
161DY L 320.69 6 11/2- 0.125 NS B
161DY cL T from 1981GrZV
161DY DL If this level has no G feeding, the LOGFT to it is 9.1.
161DY2DL This is much too small for a 2nd-forbidden transition.
161DY G 107.74 5 0.01 LE ?
161DY G 119.61 5 0.025 8 M1,E2 1.421 25
161DYS G KC=1.0 3$LC=0.36 19$MC=0.08 5$NC+=0.022 12
161DYS G NC=0.019 10$OC=0.0024 11$PC=5.3E-5 23
161DY G 217.6 1 0.003 LE E2 0.179 ?
161DYS G KC=0.1236 18$LC=0.0427 6$MC=0.00998 14$NC+=0.00255 4
161DYS G NC=0.00226 4$OC=0.000288 4$PC=6.01E-6 9
161DY cG M 1984Vy01 report M1,E2. J|p assignments require E2.
161DY L 366.969 11 1/2- D
161DY G 292.401 7
161DY G 341.38 5
161DY L 451.34 19 5/2- D
161DY G 84.86 5 ?
161DYF G FL=366.969
161DY cG E the energy fit of this |g is poor and it is not reported in
161DY2cG (n,|g). So, we show it as questionable here.
161DY G 238.40 25 0.018 6
161DY G 319.6 3 0.017 6
161DY G 348.2
161DY cG E |g is in decay scheme, but not in |g list (1984Vy01).
161DY G 376.5
161DY cG E |g is in decay scheme, but not in |g list (1984Vy01).
161DY G 425.8
161DY cG E |g is in decay scheme, but not in |g list (1984Vy01).
161DY L 772.18 10 5/2+,7/2,9/2+
161DY cL There is also a level reported at 772.7 keV, with J|p=1/2+
161DY2cL (see the Adopted Levels).
161DY cL J possible bandhead of 7/2[633]. If this is correct, then
161DY2cL J|p=7/2+.
161DY E 0.0008 3 7.35 17 0.0008 3
161DYS E CK=0.48 3 $CL=0.388 19 $CM+=0.135 8
161DY G 669.0 3 0.0030 15 ?
161DY G 672.5 3 0.0045 15
161DY G 772.1 1 0.017 6
161DY L 790.70 4 5/2- F
161DY E 0.048 8 5.17 10 0.048 8
161DYS E CK=0.23 6 $CL=0.56 4 $CM+=0.206 16
161DY G 577.9 2 0.013 5
161DY G 658.95 10 0.061 7 M1,E2 0.011 4
161DYS G KC=0.009 4$LC=0.0014 4$MC=0.00031 8$NC+=8.2E-5 21
161DYS G NC=7.1E-5 18$OC=1.0E-5 3$PC=5.6E-7 21
161DY G 687.5 1 0.125 10 M1,E2 0.010 4
161DYS G KC=0.008 3$LC=0.0013 4$MC=0.00028 7$NC+=7.4E-5 19
161DYS G NC=6.4E-5 16$OC=9.3E-6 25$PC=5.1E-7 18
161DY G 716.09 8 0.096 10 M1,E2 0.009 3
161DYS G KC=0.0077 25$LC=0.0011 3$MC=0.00025 7$NC+=6.7E-5 17
161DYS G NC=5.8E-5 15$OC=8.4E-6 23$PC=4.6E-7 16
161DY G 746.98 5 0.122 12E1 0.00219
161DYS G KC=0.00187 3$LC=0.000252 4$MC=5.47E-5 8$NC+=1.455E-5 21
161DYS G NC=1.261E-5 18$OC=1.84E-6 3$PC=1.038E-7 15
161DY G 764.96 8 0.437 35M1,E2 0.0078 24
161DYS G KC=0.0066 21$LC=0.00096 25$MC=0.00021 6$NC+=5.6E-5 15
161DYS G NC=4.9E-5 13$OC=7.1E-6 19$PC=3.9E-7 14
161DY G 790.68 8 0.361 30E1 0.00196
161DYS G KC=0.001673 24$LC=0.000224 4$MC=4.87E-5 7$NC+=1.296E-5 19
161DYS G NC=1.124E-5 16$OC=1.636E-6 23$PC=9.29E-8 13