coulomb excitation data analysis codes; gosia 2007 - Physics and ...

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13 7 8 6.56100 5.00000 9.0000014 8 8 -5.56500 COUPLED TO 1315 8 9 6.81600 5.00000 9.0000016 9 9 -5.75300 COUPLED TO 1517 9 10 6.88000 5.00000 9.0000018 10 10 -5.78500 COUPLED TO 1719 10 11 7.20900 5.00000 9.0000020 11 11 -6.04200 COUPLED TO 19203 EXPERIMENTAL YIELDS 10 MATRIX ELEMENTS TO BE VARIEDLEVEL LIFETIME ERRORLIFETIMES(PSEC)The experimental lifetime data,if it is provided by the user.3 112.00 1.00LIFETIMES ARE TAKEN WITH WEIGHT 0.100000E+01*** CHISQ= 0.277172E+02 ****** CHISQ= 0.965818E+01 ****** CHISQ= 0.594594E+01 ****** CHISQ= 0.403621E+01 ***MATRIX ELEMENT 1 LOCKED!*** CHISQ= 0.209903E+01 ****** CHISQ= 0.202990E+01 ****** CHISQ= 0.160540E+01 ****** CHISQ= 0.160194E+01 ****** CHISQ= 0.159863E+01 ****** CHISQ= 0.159805E+01 ****** CHISQ= 0.158588E+01 ***The progress of chi-squared is printed at eachstep. When a matrix element can be locked bythe fit routine, this is reported as well.MATRIX ELEMENT 9 LOCKED!*** CHISQ= 0.156263E+01 ****** CHISQ= 0.153814E+01 ***MATRIX ELEMENT 17 LOCKED!*** CHISQ= 0.153532E+01 ****** CHISQ= 0.153465E+01 ****** CHISQ= 0.153271E+01 ****** CHISQ= 0.153266E+01 ***MATRIX ELEMENT 15 LOCKED!*** CHISQ= 0.143361E+01 ****** CHISQ= 0.138014E+01 ****** CHISQ= 0.136744E+01 ***MATRIX ELEMENT 7 LOCKED!*** CHISQ= 0.135145E+01 ***180
*** CHISQ= 0.134003E+01 ***MATRIX ELEMENT 13 LOCKED!*** CHISQ= 0.133839E+01 ****** CHISQ= 0.133774E+01 ****** CHISQ= 0.130050E+01 ****** CHISQ= 0.128192E+01 ****** CHISQ= 0.109960E+01 ****** CHISQ= 0.101986E+01 ****** CHISQ= 0.101761E+01 ***MATRIX ELEMENT 5 LOCKED!*** CHISQ= 0.100682E+01 ****** CHISQ= 0.100057E+01 ***MATRIX ELEMENT 3 LOCKED!*** CHISQ= 0.999197E+00 ****** CHISQ= 0.995206E+00 ***Convergence is reported with the number of steps and theconvergence criterion (CONV) in parentheses. Refer tosections 4.5 and 5.17 for details on the minimization procedure.MATRIX ELEMENT 19 LOCKED!*** CHISQ= 0.984981E+00 ***AT STEP 34CONVERGENCE ACHIEVED( 0.768053E-07)*** CHISQ= 0.984981E+00 ***NORMALIZATION CONSTANTSEXPERIMENT DETECTORS(1-32)1 0.35E+032 0.22E+033 0.15E+034 0.10E+035 0.75E+026 0.56E+027 0.43E+028 0.35E+029 0.31E+0210 0.28E+0211 0.25E+0212 0.22E+0213 0.20E+0214 0.18E+0215 0.16E+0216 0.14E+0217 0.13E+0218 0.11E+0219 0.10E+0220 0.92E+0121 0.83E+0122 0.75E+0123 0.67E+0124 0.61E+0125 0.54E+0126 0.49E+0127 0.44E+01Normalization constants between the experiments, eitherspecified by the user (as in g1demo.inp) or fit by GOSIA,followed by the recommended relative gamma-raydetector efficiencies. Refer to section 4.5.2.181
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COULOMB EXCITATION DATA ANALYSIS CO
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10 MINIMIZATION BY SIMULATED ANNEAL
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1 INTRODUCTION1.1 Gosia suite of Co
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104 Ru, 110 Pd, 165 Ho, 166 Er, 186
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Figure 1: Coordinate system used to
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Cλ E =1.116547 · (13.889122) λ (
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Figure 2: The orbital integrals R 2
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2.2 Gamma Decay Following Electroma
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where :d 2 σ= σ R (θ p ) X R kχ
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Formula 2.49 is valid only for t mu
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Ã XK(α) =exp−iτ i (E γ )x i (
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important to have an accurate knowl
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3 APPROXIMATE EVALUATION OF EXCITAT
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with the reduced matrix element M c
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q (20)s (0 + → 2 + ) · M 1 ζ (2
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esults of minimization and error ru
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adjustment of the stepsize accordin
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approximation reliability improves
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Zd 2 σ(I → I f )Y (I → I f )=s
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4.5 MinimizationThe minimization, i
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X(CC k Yk c − Yk e ) 2 /σ 2 k =m
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However, estimation of the stepsize
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It can be shown that as long as the
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een exceeded; third, the user-given
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where f k stands for the functional
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x i + δx i Rx iexp ¡ − 1 2 χ2
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method used for the minimization, i
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OP,ERRO (ERRORS) (5.6):Activates th
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-----OP,SIXJ (SIX-j SYMBOL) (5.25):
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5.3 CONT (CONTROL)This suboption of
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I,I1 Ranges of matrix elements to b
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CODE DEFAULT OTHER CONSEQUENCES OF
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5.4 OP,CORR (CORRECT )This executio
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5.6 OP,ERRO (ERRORS)ThemoduleofGOSI
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5.7 OP,EXIT (EXIT)This option cause
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M AControls the number of magnetic
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5.10 OP,GDET (GE DETECTORS)This opt
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5.12 OP,INTG (INTEGRATE)This comman
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¡ dE¢dx1 ..¡ dEdx¢Stopping powe
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NI1, NI2 Number of subdivisions of
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5.13 LEVE (LEVELS)Mandatory subopti
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5.15 ME (OP,COUL)Mandatory suboptio
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Figure 10: Model system having 4 st
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ME =< INDEX2||E(M)λ||INDEX1 > The
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When entering matrix elements in th
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There are no restrictions concernin
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5.18 OP,POIN (POINT CALCULATION)Thi
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5.20 OP,RAW (RAW UNCORRECTED γ YIE
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5.21 OP,RE,A (RELEASE,A)This option
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5.25 OP,SIXJ (SIXJ SYMBOL)This stan
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5.27 OP,THEO (COLLECTIVE MODEL ME)C
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2,5,1,-2,23,5,1,-2,23,6,1,-2,2Matri
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5.29 OP,TROU (TROUBLE)This troubles
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to that of the previous experiment,
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To reduce the unnecessary input, on
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OP,STAR or OP,POIN under OP,GOSI. N
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5.31 INPUT OF EXPERIMENTAL γ-RAY Y
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6 QUADRUPOLE ROTATION INVARIANTS -
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*½P 5 (J) = s(E2 × E2) J ×¯h¾
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The expectation value of cos3δ can
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where ē is an arbitratry vector. D
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achieved using “mixed“ calculat
Page 129 and 130: TAPE9 Contains the parameters neede
Page 131 and 132: TAPE18 Input file, containing the i
Page 133 and 134: 7.4.4 CALCULATION OF THE INTEGRATED
Page 135 and 136: OP,EXITInput: TAPE4,TAPE7,TAPE9Outp
Page 137 and 138: OP,ERRO0,MS,MEND,1,0,RMAXand the fi
Page 139 and 140: 8 SIMULTANEOUS COULOMB EXCITATION:
Page 141 and 142: 4, 3, 1kr88.corKr corrected yields
Page 143 and 144: 0 Correction for in-flight decay ch
Page 145 and 146: OP, ERRO Estimation of errors of fi
Page 147 and 148: 9 COULOMB EXCITATION OF ISOMERIC ST
Page 149 and 150: configurations with a probability e
Page 151 and 152: The average range covered by each m
Page 153 and 154: SFX,NTOTI1(1),I2(1),RSIGN(1)I1(2),I
Page 155 and 156: 11.2 LearningtoWriteGosiaInputsThe
Page 157 and 158: (1.6 MeV)1.1 MeV0.75 MeV0.4 MeV0.08
Page 159 and 160: Define the germaniumdetector geomet
Page 161 and 162: Figure 15: Flow diagram for Gosia m
Page 163 and 164: gosia < 2-make-correction-factors.i
Page 165 and 166: Issue the commandgosia < 9-diag-err
Page 167 and 168: At this point, it is suggested to c
Page 169 and 170: calculation.) In this case, a copy
Page 171 and 172: 4,-4, -3.705, 3,44,5, 4.626, 3.,7.5
Page 173 and 174: 90145901459014590145901459014590145
Page 175 and 176: .10.028921.10.026031.10.023431.10.0
Page 177 and 178: 5,5,634,650,82.000,84.000634,638,64
Page 179: ***********************************
Page 183 and 184: CALCULATED AND EXPERIMENTAL YIELDS
Page 185 and 186: 11.7 Annotated excerpt from a Coulo
Page 187 and 188: 11.8 Accuracy and speed of calculat
Page 189 and 190: 18,10.056,0.068,0.082,0.1,0.12,0.15
Page 191 and 192: line 152 Eu 182 Tanumber (keV) (keV
Page 193 and 194: 1.6 Normalization between data sets
Page 195 and 196: 13 GOSIA 2007 RELEASE NOTESThese no
Page 197 and 198: Matrix elements 500(April 1990, T.
Page 199 and 200: 14 GOSIA Manual UpdatesDATE UPDATE2
Page 201 and 202: [KIB08]T.Kibédi,T.W.Burrows,M.B.Tr
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