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The original code did not do that, maybe the veto domes are included in the transmission coefficients of the material above D1 and between D1 & D2.
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… coefficients and not mass attenuation coefficients (#2186)
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Now only the low-energy thresholds are missing in the D1 & D2 module responses. Once I got this going the job is essentially done!
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… and add escape peaks to D2 response (#2186)
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There is a first version that performs an IAQ computation, without however the correction coefficients.
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It seems more logical to start with the calibration database and then specify the response name in that calibration database.
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…ients argument (#1847) The eval_gradients() methods duplicate much of the code of the eval() methods. To increase the maintainability of the code, the eval_gradients() methods have been removed, and the computation of partial derivatives is now done by the eval() methods if the optional gradients argument is set to true.
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The following new names have been introduced for the spatial model components: * "PointSource" (alias: "SkyDirFunction") * "RadialDisk" (alias: "DiskFunction") * "RadialGaussian" (alias: "GaussFunction") * "RadialShell" (alias: "ShellFunction") * "EllipticalDisk" * "EllipticalGaussian" (alias: "EllipticalGauss") * "DiffuseIsotropic" (alias: "ConstantValue") * "DiffuseMap" (alias: "SpatialMap") * "DiffuseMapCube" (alias: "MapCubeFunction")
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… methods from GTools.
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Removed size() method. Renamed filename() method to url(). Renamed fullname() method to operator().
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…ilename object. This allows now replacing all std::string filenames by GFilename arguments.
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… simplify the code for reading and writing of XML files.