- 06 Sep, 2018 1 commit
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Guang authored
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- 05 Sep, 2018 3 commits
- 30 Aug, 2018 1 commit
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Guang authored
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- 29 Aug, 2018 1 commit
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Guang authored
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- 28 Aug, 2018 1 commit
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Guang authored
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- 27 Aug, 2018 4 commits
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Guang authored
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Guang authored
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YANG Guang authored
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YANG Guang authored
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- 27 Feb, 2018 2 commits
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Médéric Boquien authored
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Médéric Boquien authored
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- 26 Feb, 2018 4 commits
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Médéric Boquien authored
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Médéric Boquien authored
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Médéric Boquien authored
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Médéric Boquien authored
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- 19 Feb, 2018 7 commits
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Médéric Boquien authored
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Médéric Boquien authored
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Médéric Boquien authored
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Médéric Boquien authored
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Médéric Boquien authored
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Médéric Boquien authored
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Médéric Boquien authored
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- 16 Feb, 2018 6 commits
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Médéric Boquien authored
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Médéric Boquien authored
When using different line widths during a single run, ensure that the fluxes and other quantities are always computed correctly
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Médéric Boquien authored
Ensure that the computation of the continuum level is correct when determining the equivalent width, in particular when the line width is very narrow.
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Médéric Boquien authored
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Médéric Boquien authored
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Médéric Boquien authored
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- 15 Feb, 2018 1 commit
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Médéric Boquien authored
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- 25 Jan, 2018 4 commits
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Médéric Boquien authored
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Médéric Boquien authored
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Médéric Boquien authored
The formula from Sawicki et al. (2012) used to compute the χ² in the presence of upper limits was not correct. This led the χ² to depend directly on the absolute value of the upper limit. The formula has been rederived and corrected.
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Médéric Boquien authored
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- 15 Jan, 2018 1 commit
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Médéric Boquien authored
Fν was computed by calculating Fλ and then converting to Fν, which led to typical differences in fluxes of typically 1-2% and a bit more for a handful of pathological filters. Now Fν is computed directly and a bit faster. At the same time rather than computing an effective wavelength (which was more a mean wavelength), we compute the pivot wavelength, which is more appropriate when converting between Fν and Fλ.
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- 05 Jan, 2018 1 commit
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Médéric Boquien authored
When computing the attenuation curve, the bump is now added so that its relative strength does not depend on δ.
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- 22 Dec, 2017 1 commit
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Médéric Boquien authored
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- 11 Dec, 2017 1 commit
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Médéric Boquien authored
For more reliability we now save the chi² by blocks. Otherwise it could lead to some crashes when there was more than 1 redshift.
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- 27 Nov, 2017 1 commit
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Médéric Boquien authored
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