93-Np-236 JAEA+ EVAL-FEB10 O.Iwamoto,T.Nakagawa,K.Furutaka,+
DIST-MAY10 20100318
----JENDL-4.0 MATERIAL 9343
-----INCIDENT NEUTRON DATA
------ENDF-6 FORMAT
History
07-07 New theoretical calculation was made with CCONE code.
07-09 Resolved resonance parameters were replaced.
07-10 Theoretical calculation was made with CCONE code.
Data were compiled as JENDL/AC-2008/1/.
09-02 (3,102) below 0.2 eV, (1,452), (1,455) and (1,456) were
revised.
10-02 Data of prompt gamma rays due to fission were given.
10-03 Covariance data were given.
MF= 1 General information
MT=452 Number of Neutrons per fission
Sum of MT's=455 and 456.
MT=455 Delayed neutron data
Determined from systematics by Tuttle/2/, Benedetti et al./3/
and Waldo et al./4/, and partial fission cross sections
calculated with CCONE code /5/.
MT=456 Number of prompt neutrons per fission
Based on the data measured by Lindner and Seegmiller/6/ and
Ohsawa's systematics/7/.
MF= 2 Resonance parameters
MT=151
Resolved resonance parameters (MLBW: 1.0e-5 - 21.5 eV)
Evaluated by Furutaka /8/ with SAMMY-7 code/9/.
Experimental data used are fission cross-section data measured
by Danon et al./10/ Their data were normalized to 2815 b at
0.0253 eV. The capture width was fixed to 40 meV.
Doppler as well as resolution broadenings were taken into
account in the analysis: temperature was assumed to be 298 K.
For resolution broadening, parameters of SAMMY's original
resolution-broadening function were chosen to approximately
reproduce the experimental resolution function described by
equation (11) of ref./10/.
The 8 fictitious resonances in the energy range 24 to 33 eV
were adopted from ENDF/B-VII.0/11/
Un-resolved resonance parameters (21.5 eV - 10 keV)
Parameters (URP) were determined with ASREP code/12/ so as to
reproduce the cross sections in this energy region. URP are
used only for self-shielding calculations.
Thermal cross sections and resonance integrals (at 300K)
-------------------------------------------------------
0.0253 eV reson. integ.(*)
(barns) (barns)
-------------------------------------------------------
total 2938.9
elastic 9.657
fission 2808.0 1170
capture 121.3 100
-------------------------------------------------------
(*) In the energy range from 0.5 eV to 10 MeV.
MF= 3 Neutron cross sections
All the cross-section data above 21.5 eV were calculated with
CCONE code/5/.
MT= 1 Total cross section
The cross section was calculated with CC OMP of Soukhovitskii
et al./13/.
MT=18 Fission cross section
Calculated with CCONE code. The simulated (n,f) cross section
of Britt and Wilhelmy/14/ and the experimental data of
Danon et al./10/ and Val'skiy et al./15/ were used to
determine the parameters in the CCONE calculation.
MF= 4 Angular distributions of secondary neutrons
MT=2 Elastic scattering
Calculated with CCONE code.
MT=18 Fission
Isotropic distributions in the laboratory system were assumed.
MF= 5 Energy distributions of secondary neutrons
MT=18 Prompt neutrons
Calculated with CCONE code/5/.
MF= 6 Energy-angle distributions
Calculated with CCONE code.
Distributions from fission (MT=18) are not included.
MF=12 Photon production multiplicities
MT=18 Fission
Calculated from the total energy released by the prompt
gamma-rays due to fission which was estimated from its
systematics, and the average energy of gamma-rays.
MF=14 Photon angular distributions
MT=18 Fission
Isotoropic distributions were assumed.
MF=15 Continuous photon energy spectra
MT=18 Fission
Experimental data measured by Verbinski et al./16/ for
Pu-239 thermal fission were adopted.
MF=31 Covariances of average number of neutrons per fission
MT=452 Number of neutrons per fission
Sum of covariances for MT=455 and MT=456.
MT=455
Error of 15% was assumed.
MT=456
Covariance was obtained by fitting a linear function to the
data at 0.0 and 5.0 MeV with an uncertainty of 30% which was
estimated from the experimental data of Lindner and
Seegmiller/6/.
MF=32 Covariances of resonance parameters
MT=151 Resolved resonance parameterss
Format of LCOMP=1 was adopted.
Covariances of parameters were taken from the results of SAMMY
analysis/8/. The covariances were multiplied by a factor
of 10 because they were too small.
MF=33 Covariances of neutron cross sections
Covariances were given to all the cross sections by using
KALMAN code/17/ and the covariances of model parameters
used in the cross-section calculations.
Covariances of the fission cross section were determined by
considering the experimental data (see MF=3).
In the resolved resonance region, the following standard
deviations were added to the contributions from resonance
parameters:
Elastic scattering 20 %
Capture 50 %
MF=34 Covariances for Angular Distributions
MT=2 Elastic scattering
Covariances were given only to P1 components.
MF=35 Covariances for Energy Distributions
MT=18 Fission spectra
Estimated with CCONE and KALMAN codes.
*****************************************************************
Calculation with CCONE code
*****************************************************************
Models and parameters used in the CCONE/5/ calculation
1) Coupled channel optical model
Levels in the rotational band were included. Optical model
potential and coupled levels are shown in Table 1.
2) Two-component exciton model/18/
* Global parametrization of Koning-Duijvestijn/19/
was used.
* Gamma emission channel/20/ was added to simulate direct
and semi-direct capture reaction.
3) Hauser-Feshbach statistical model
* Moldauer width fluctuation correction/21/ was included.
* Neutron, gamma and fission decay channel were included.
* Transmission coefficients of neutrons were taken from
coupled channel calculation in Table 1.
* The level scheme of the target is shown in Table 2.
* Level density formula of constant temperature and Fermi-gas
model were used with shell energy correction and collective
enhancement factor. Parameters are shown in Table 3.
* Fission channel:
Double humped fission barriers were assumed.
Fission barrier penetrabilities were calculated with
Hill-Wheler formula/22/. Fission barrier parameters were
shown in Table 4. Transition state model was used and
continuum levels are assumed above the saddles. The level
density parameters for inner and outer saddles are shown in
Tables 5 and 6, respectively.
* Gamma-ray strength function of Kopecky et al/23/,/24/
was used. The prameters are shown in Table 7.
------------------------------------------------------------------
Tables
------------------------------------------------------------------
Table 1. Coupled channel calculation
--------------------------------------------------
* rigid rotor model was applied
* coupled levels = 0,1,5 (see Table 2)
* optical potential parameters /13/
Volume:
V_0 = 49.97 MeV
lambda_HF = 0.01004 1/MeV
C_viso = 15.9 MeV
A_v = 12.04 MeV
B_v = 81.36 MeV
E_a = 385 MeV
r_v = 1.2568 fm
a_v = 0.633 fm
Surface:
W_0 = 17.2 MeV
B_s = 11.19 MeV
C_s = 0.01361 1/MeV
C_wiso = 23.5 MeV
r_s = 1.1803 fm
a_s = 0.601 fm
Spin-orbit:
V_so = 5.75 MeV
lambda_so = 0.005 1/MeV
W_so = -3.1 MeV
B_so = 160 MeV
r_so = 1.1214 fm
a_so = 0.59 fm
Coulomb:
C_coul = 1.3
r_c = 1.2452 fm
a_c = 0.545 fm
Deformation:
beta_2 = 0.213
beta_4 = 0.066
beta_6 = 0.0015
* Calculated strength function
S0= 0.90e-4 S1= 2.70e-4 R'= 9.46 fm (En=1 keV)
--------------------------------------------------
Table 2. Level Scheme of Np-236
-------------------
No. Ex(MeV) J PI
-------------------
0 0.00000 6 - *
1 0.05600 7 - *
2 0.06000 1 +
3 0.07600 2 +
4 0.10000 3 +
5 0.12000 8 - *
6 0.13200 4 +
-------------------
*) Coupled levels in CC calculation
Table 3. Level density parameters
--------------------------------------------------------
Nuclide a* Pair Eshell T E0 Ematch
1/MeV MeV MeV MeV MeV MeV
--------------------------------------------------------
Np-237 18.3022 0.7795 2.4371 0.3963 -0.9739 3.1569
Np-236 18.2358 0.0000 2.1332 0.2999 -0.7994 1.1664
Np-235 18.1694 0.7828 2.2924 0.3973 -0.9417 3.1303
Np-234 18.1029 0.0000 2.1332 0.2844 -0.6773 1.0000
Np-233 18.0364 0.7861 2.3620 0.4163 -1.1454 3.3864
--------------------------------------------------------
Table 4. Fission barrier parameters
----------------------------------------
Nuclide V_A hw_A V_B hw_B
MeV MeV MeV MeV
----------------------------------------
Np-237 6.000 0.950 5.570 0.600
Np-236 6.100 0.600 6.080 0.600
Np-235 6.250 0.950 5.630 0.600
Np-234 6.200 0.460 5.850 0.370
Np-233 4.300 0.800 3.300 0.520
----------------------------------------
Table 5. Level density above inner saddle
--------------------------------------------------------
Nuclide a* Pair Eshell T E0 Ematch
1/MeV MeV MeV MeV MeV MeV
--------------------------------------------------------
Np-237 21.9626 0.9094 2.6000 0.3162 -1.4591 2.9094
Np-236 22.2477 0.0000 2.6000 0.3139 -2.3586 2.0000
Np-235 20.3497 0.9133 2.6000 0.3299 -1.4981 2.9133
Np-234 20.2753 0.0000 2.6000 0.3306 -2.4114 2.0000
Np-233 20.2008 0.9172 2.6000 0.3312 -1.4942 2.9172
--------------------------------------------------------
Table 6. Level density above outer saddle
--------------------------------------------------------
Nuclide a* Pair Eshell T E0 Ematch
1/MeV MeV MeV MeV MeV MeV
--------------------------------------------------------
Np-237 22.3287 0.9094 0.2400 0.3268 -0.5253 2.6094
Np-236 22.2477 0.0000 0.2000 0.3977 -2.2734 2.7000
Np-235 22.1666 0.9133 0.1600 0.3517 -0.7691 2.9133
Np-234 20.2753 0.0000 0.1200 0.3712 -1.6997 2.0000
Np-233 20.2008 0.9172 0.0800 0.3724 -0.7819 2.9172
--------------------------------------------------------
Table 7. Gamma-ray strength function for Np-237
--------------------------------------------------------
K0 = 1.300 E0 = 4.500 (MeV)
* E1: ER = 10.98 (MeV) EG = 2.17 (MeV) SIG = 311.00 (mb)
ER = 14.08 (MeV) EG = 4.66 (MeV) SIG = 540.00 (mb)
* M1: ER = 6.63 (MeV) EG = 4.00 (MeV) SIG = 2.08 (mb)
* E2: ER = 10.18 (MeV) EG = 3.27 (MeV) SIG = 6.65 (mb)
--------------------------------------------------------
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