CODE	NUCLIDE	ORIGINAL DATA TAKEN FROM	MODIFICATION	ADDITIONAL FILE MODIFICATIONS	ORIGINAL DATA TAKEN FROM	MODIFICATION	ADDITIONAL FILE MODIFICATIONS	COMMENTS
1082208	082_Pb_208	ENDF/B-VII	Covariances - BNL, July, 2011: Covariances were adopted from COMMARA-2.0, where BNL performed a new evaluation of covariances for a set of four Pb isotopes in the full energy range in 2010. The thermal and resolved resonance region made use of the covariance formalism based on kernel approximation along with data in the Atlas of Neutron Resonances. We note that the resonance region for Pb isotopes extends to very high energies. Elastic scattering uncertainty in the resonance region was largely determined by potential scattering contribution via the uncertainty of the scattering radius R'. In the fast neutron region up to 20 MeV covariance estimates were produced using the nuclear reaction code EMPIRE and the Bayesian code KALMAN. The KALMAN code along with selected experimental data was used to determine the correlation matrix of the model parameters. Furthermore, additional parameters scaling total and absorption cross sections were included to prevent the unrealistic drop in the cross-section uncertainties and, in some instances, to cover spread of the experimental data. For all Pb isotopes, the elastic cross-section uncertainties were computed as difference of total and absorption reaction channel.	Covariances - BNL, July, 2011: Covariances were adopted from COMMARA-2.0, where BNL performed a new evaluation of covariances for a set of four Pb isotopes in the full energy range in 2010. The thermal and resolved resonance region made use of the covariance formalism based on kernel approximation along with data in the Atlas of Neutron Resonances. We note that the resonance region for Pb isotopes extends to very high energies. Elastic scattering uncertainty in the resonance region was largely determined by potential scattering contribution via the uncertainty of the scattering radius R'. In the fast neutron region up to 20 MeV covariance estimates were produced using the nuclear reaction code EMPIRE and the Bayesian code KALMAN. The KALMAN code along with selected experimental data was used to determine the correlation matrix of the model parameters. Furthermore, additional parameters scaling total and absorption cross sections were included to prevent the unrealistic drop in the cross-section uncertainties and, in some instances, to cover spread of the experimental data. For all Pb isotopes, the elastic cross-section uncertainties were computed as difference of total and absorption reaction channel.	ENDF/B-VI MOD 5	Evaluation, March 2006, M. Chadwick,P. Young A new GNASH analysis was performed over the incident neutron energy range from 1.0 to 30.0 MeV. Elastic scattering angular distributions were also calculated with the Koning-Delaroche potential and incorporated in the evaluation at neutron energies below 30 MeV. Data for the following reactions were replaced: MF=3, MT=2, 3, 4, 16, 17, 22, 24, 28, 32, 33, 37, 41, 51-91, 102, 103, 104, 105, 107, 600-649, 650-699, 700-749, 800-849; MF=4,MT=2; MF=6, MT=16, 17, 22, 24, 28, 32, 33, 37, 41, 91, 649, 699, 749, and 849. The total cross section, all angular distributions except elastic, resonance parameters, and data for MF=8, 9, 12, 14, and 15 were preserved from ENDF/B-VI.