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	docs: CHANGELOG updated.
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							|  | @ -2,6 +2,26 @@ | |||
| 
 | ||||
| All notable changes to this project will be documented in this file. | ||||
| 
 | ||||
| ## [2.1.0] - 2022-05-31 | ||||
| ### Added | ||||
| - `obs.covariance` now has the option to smooth small eigenvalues of the matrix with the method described in hep-lat/9412087. | ||||
| - `Corr.prune` was added which can reduce the size of a correlator matrix before solving the GEVP. | ||||
| - `Corr.show` has two additional optional arguments. `hide_sigma` to hide data points with large errors and `references` to display reference values as horizontal lines. | ||||
| - I/O routines for ALPHA dobs format added. | ||||
| - `input.hadrons` functionality extended. | ||||
| 
 | ||||
| ### Changed | ||||
| - The standard behavior of the `Corr.GEVP` method has changed. It now returns all eigenvectors of the system instead of only the specified ones as default. The standard way of sorting the eigenvectors was changed to `Eigenvalue`. The argument `sorted_list` was deprecated in favor of `sort`. | ||||
| - Before performing a correlated fit the routine first runs an uncorrelated one to obtain a better guess for the initial parameters. | ||||
| 
 | ||||
| ### Fixed | ||||
| - `obs.covariance` now also gives correct estimators if data defined on non-identical configurations is passed to the function. | ||||
| - Rounding errors in estimating derivatives of fit parameters with respect to input data from the inverse hessian reduced. This should only make a difference when the magnitude of the errors of different fit parameters vary vastly. | ||||
| - Bug in json.gz format fixed which did not properly store the replica mean values. Format version bumped to 1.1. | ||||
| - The GEVP matrix is now symmetrized before solving the system for all sorting options not only the one with fixed `ts`. | ||||
| - Automatic range estimation improved in `fits.residual_plot`. | ||||
| - Bugs in `input.bdio` fixed. | ||||
| 
 | ||||
| ## [2.0.0] - 2022-03-31 | ||||
| ### Added | ||||
| - The possibility to work with Monte Carlo histories which are evenly or unevenly spaced was added. | ||||
|  |  | |||
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