lines - Emission/absorption line adjustment¶
GaussianNormed1D(flux, mean, stddev, **kwargs) |
Flux-normalized 1D-Gaussian. |
ComplexHa(wHa, iHa, iNII, sigma, **kwargs) |
[NII] + Hα complex fittable model. |
DoubletOIII(wOIII, iOIII, sigma, **kwargs) |
[OIII] doublet fittable model. |
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class
inspec.lines.GaussianNormed1D(flux, mean, stddev, **kwargs)[source]¶ Flux-normalized 1D-Gaussian.
\[G_N(\lambda; f, \mu, \sigma) = \frac{f}{\sigma\sqrt{2\pi}} \exp\left(-\frac{(\lambda - \mu)^2}{2\sigma^2}\right)\]-
flux= Parameter('flux', value=nan)¶ Gaussian integrated flux
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mean= Parameter('mean', value=nan)¶ Gaussian mean
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stddev= Parameter('stddev', value=nan)¶ Gaussian stddev
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param_names= ('flux', 'mean', 'stddev')¶
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class
inspec.lines.ComplexHa(wHa, iHa, iNII, sigma, **kwargs)[source]¶ [NII] + Hα complex fittable model.
The [NII] + Hα complex is modeled as a tied sum of three
astropy.modeling.models.Gaussian1D:\[\begin{split}P(\lambda) &= I_{H\alpha} \times G(\lambda; \lambda_{H\alpha}, \sigma) \\ & \quad + 3/4\, I_{NII} \times G(\lambda; \lambda_{NIIa}, \sigma) \\ & \quad + 1/4\, I_{NII} \times G(\lambda; \lambda_{NIIb}, \sigma) \\ G(\lambda; \mu, \sigma) &= \exp\left(-\frac{(\lambda - \mu)^2}{2\sigma^2}\right)\end{split}\]where the 4 adjustable parameters are:
- \(\lambda_{H\alpha}\) =
wHa: Hα wavelength [Å] - \(I_{H\alpha}\) =
iHa: Hα amplitude - \(I_{NII}\) =
iNII: [NII] amplitude - \(\sigma\) =
sigma: line width [Å]
and where [NII] doublet wavelengths \(\lambda_{NIIa}\) and \(\lambda_{NIIa}\) are tied to the Hα wavelength \(\lambda_{H\alpha}\).
Warning
the amplitudes
iHaandiNIIare not the line fluxes, since the standardastropy.modeling.models.Gaussian1Dis not flux-normalized. Still, the amplitude ratio holds since the stddev is common to all lines.-
Halpha= 6564.614¶ Hα reference wavelength [Å]
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NIIa= 6585.27¶ NIIa reference wavelength [Å]
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NIIb= 6549.86¶ NIIb reference wavelength [Å]
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rNIIa= 1.0031465673381559¶
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rNIIb= 0.997752495424712¶
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fNIIa= 0.75¶ Intensity ratio wrt NII amplitude
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fNIIb= 0.25¶ Intensity ratio wrt NII amplitude
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wHa= Parameter('wHa', value=nan)¶ Hα wavelength [Å]
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iHa= Parameter('iHa', value=nan)¶ Hα amplitude
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iNII= Parameter('iNII', value=nan)¶ [NII] amplitude
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sigma= Parameter('sigma', value=nan)¶ Line width [Å]
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static
Ha_line(x, wHa, iHa, iNII, sigma)[source]¶ Hα line modeled as a single
astropy.modeling.models.Gaussian1D.
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static
NII_lines(x, wHa, iHa, iNII, sigma)[source]¶ [NII] doublet modeled as a tied sum of two
astropy.modeling.models.Gaussian1D.
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param_names= ('wHa', 'iHa', 'iNII', 'sigma')¶
- \(\lambda_{H\alpha}\) =
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class
inspec.lines.DoubletOIII(wOIII, iOIII, sigma, **kwargs)[source]¶ [OIII] doublet fittable model.
The [OIII] doublet is modeled as a tied sum of two
astropy.modeling.models.Gaussian1D:\[\begin{split}P(\lambda) &= 3/4\, I_{OIII} \times G(\lambda; \lambda_{OIII}, \sigma) \\ & \quad + 1/4\, I_{OIII} \times G(\lambda; \lambda_{OIIIb}, \sigma) \\ G(\lambda; \mu, \sigma) &= \exp\left(-\frac{(\lambda - \mu)^2}{2\sigma^2}\right)\end{split}\]where the 3 adjustable parameters are:
- \(\lambda_{OIII}\) =
wOIII: OIIIa wavelength [Å] - \(I_{OIII}\) =
iOIII: [OIII] doublet amplitude - \(\sigma\) =
sigma: line width [Å]
and where \(\lambda_{OIIIb}\) wavelength is tied to the OIIIa wavelength \(\lambda_{OIII}\).
Warning
the amplitude
iOIIIis not the integrated line flux, since the standardastropy.modeling.models.Gaussian1Dis not flux-normalized. Still, the amplitude ratio holds since the stddev is common to all lines.-
OIII= 5008.24¶ [OIIIa] reference wavelength [Å]
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OIIIb= 4960.295¶ [OIIIb] reference wavelength [Å]
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rOIIIb= 0.9904267766720445¶
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fOIII= 0.75¶ Intensity ratio wrt OIII amplitude
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fOIIIb= 0.25¶ Intensity ratio wrt OIII amplitude
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wOIII= Parameter('wOIII', value=nan)¶ OIIIa wavelength [Å]
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iOIII= Parameter('iOIII', value=nan)¶ [OIII] amplitude
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sigma= Parameter('sigma', value=nan)¶ Line width [Å]
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param_names= ('wOIII', 'iOIII', 'sigma')¶
- \(\lambda_{OIII}\) =