CODE	NUCLIDE	ORIGINAL DATA TAKEN FROM	MODIFICATION	ADDITIONAL FILE MODIFICATIONS	ORIGINAL DATA TAKEN FROM	MODIFICATION	ADDITIONAL FILE MODIFICATIONS	COMMENTS
1042098	042_Mo_098	JENDL-3.3	(1,451) Updated. (3.1) Revised. (3,2) Re-calculated. (3,4) Re-calculated. (3,51:54) Revised. (3,203-207) Added. (3,251) Deleted. (4,2) Transformation matrix deleted. (4,16-91) Deleted. (5,16-91) Deleted. (6,16-91) Taken from JENDL fusion file. (12,102) Added. (13,3) Added. (14,3),(14,102) Added. (15,3),(15,102) Added.		JENDL-3.2	(2,151) Unresolved resonance parameters (3,1) Calculated from new optical potential (3,4), (3,51-91), (3,16), (3,17), (3,22), (3,28) Taken from JENDL fusion file (3,32) Deleted (4,16-91) Taken from JENDL fusion file (5,16-91) Taken from JENDL fusion file		"File produced by WPEC Subgroup 23 in 2004-2005 CONVERTED FROM JENDL-3.3 BY JAERI AUG 2005 Covariances, BNL, July 2011 Covariances from COMMARA-2.0 were adopted for the Mo isotopes. Here, new sets of covariances were obtained at BNL in 2010 using the kernel approach in the resonance region and EMPIRE/KALMAN analysis of experimental data in the fast neutron region. Dispersion analysis of the evaluated libraries does not bring much insight since all major libraries are virtually identical. Only ROSFOND differs from other major libraries suggesting 15% uncertainty for elastic above 1 MeV and 50% for capture above 10 MeV. The isotopic data are available for total, elastic and capture so there was no need to resort to elemental measurements. The EMPIRE/KALMAN analysis was performed using ""nuisance"" parameters scaling total and reaction cross sections to account for systematic uncertainties and meet dispersion guidelines."