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A spatially resolved study of ionized regions in galaxies at different ...

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58 3 • IFS <strong>of</strong> a GEHR <strong>in</strong> NGC 6946<br />

the spectrophotometric standard star frames.<br />

All the corrections performed to the images, mentioned <strong>in</strong> precedent sections, do not<br />

correct for the differences <strong>in</strong> the shape <strong>of</strong> the emission l<strong>in</strong>es along the cross-dispersion axis.<br />

This effect is also present <strong>in</strong> sky-subtracted spectra from long-slit spectroscopy, show<strong>in</strong>g<br />

characteristic residuals <strong>in</strong> the loc<strong>at</strong>ion <strong>of</strong> the sky emission l<strong>in</strong>es. This effect is more severe<br />

<strong>in</strong> fiber-based spectrographs, s<strong>in</strong>ce the effective dispersion and shape <strong>of</strong> the emission l<strong>in</strong>es<br />

varies fiber-to-fiber.<br />

As mentioned <strong>in</strong> Section 3.2, PPak <strong>in</strong>cludes additional fibers th<strong>at</strong> probe the sky far enough<br />

from the science FOV to avoid contam<strong>in</strong><strong>at</strong>ion by the astronomical object. One simple method<br />

to perform the sky subtraction is to extract all the 36 sky fibers, cre<strong>at</strong>e a median sky spectra<br />

and substract it from the science exposures. Nevertheless, this does not take <strong>in</strong>to account<br />

the distortion <strong>in</strong> the wavelength solution along the cross-dispersion. To <strong>in</strong>crease the accuracy<br />

<strong>of</strong> the sky substraction, a second method can be applied. The rout<strong>in</strong>e cre<strong>at</strong>e sky ppak<br />

determ<strong>in</strong>es the sky spectra correspond<strong>in</strong>g to any science fiber by an <strong>in</strong>terpol<strong>at</strong>ion <strong>of</strong> the<br />

spectra obta<strong>in</strong>ed through the sky l<strong>in</strong>es. As the set <strong>of</strong> Hii <strong>regions</strong> <strong>in</strong> our images presents an<br />

<strong>in</strong>homogeneous distribution through the field <strong>of</strong> view <strong>of</strong> the IFU, we followed another method<br />

to derive a represent<strong>at</strong>ion <strong>of</strong> the sky. The rout<strong>in</strong>e cre<strong>at</strong>e sky clip cre<strong>at</strong>es a sky spectra by<br />

obta<strong>in</strong><strong>in</strong>g the median between a certa<strong>in</strong> number <strong>of</strong> adjacent spectra, clipp<strong>in</strong>g those ones<br />

with a flux over a certa<strong>in</strong> threshold <strong>of</strong> the standard devi<strong>at</strong>ion. The results from the last two<br />

methods are very close from each other <strong>in</strong> our case, with differences less than 3%. The use <strong>of</strong><br />

one or other method depends on the n<strong>at</strong>ure <strong>of</strong> the science observ<strong>at</strong>ions, so it is advisable to<br />

check both solutions. Both results cre<strong>at</strong>e a better represent<strong>at</strong>ion <strong>of</strong> the sky than the simple<br />

method, with less deep residuals, but still present. These residuals are specially strong <strong>in</strong> the<br />

red part <strong>of</strong> the spectrum (8000-11000 Å).<br />

As seen <strong>in</strong> Section 3.1, the Hii complex is loc<strong>at</strong>ed <strong>at</strong> the extreme <strong>of</strong> the NE arm <strong>of</strong> the<br />

galaxy. As the sky fibers surround the object, some <strong>of</strong> them might have some diffuse nebular<br />

emission from the end <strong>of</strong> the arm contam<strong>in</strong><strong>at</strong><strong>in</strong>g the sky spectra. We compared the flux <strong>of</strong><br />

the Hα l<strong>in</strong>e <strong>in</strong> represent<strong>at</strong>ive spectra with and without sky subtraction. The difference <strong>in</strong><br />

the flux was negligible 8 . This reliable, free <strong>of</strong> nebular emission, sky spectra was subtracted<br />

from the science frames.<br />

3.3.8 Mosaics<br />

As expla<strong>in</strong>ed before, adjacent spectra <strong>in</strong> a RSS file may not correspond to <strong>sp<strong>at</strong>ially</strong> near<br />

positions, so it is important to reorder the spectra to their orig<strong>in</strong>al position <strong>in</strong> the sky. A<br />

position table is required, rel<strong>at</strong><strong>in</strong>g the spectra to their loc<strong>at</strong>ions <strong>in</strong> the sky. Then, it is possible<br />

to cre<strong>at</strong>e a regular gridded d<strong>at</strong>a cube by <strong>in</strong>terpol<strong>at</strong><strong>in</strong>g the d<strong>at</strong>a <strong>sp<strong>at</strong>ially</strong>, and reconstruct<br />

the orig<strong>in</strong>al image <strong>of</strong> the target <strong>at</strong> any wavelength. This step is needed if DAR correction is<br />

8 The Hα contribution <strong>of</strong> the sky spectra is about 10% for the lowest value <strong>in</strong> the FOV.

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