Table 1:

SPIRE observations of the Polaris flare.
$\lambda$ Pixel size FWHM G S0 Noise $\gamma$ P0
($\mu $m) (arcsec) (arcsec)   (MJy sr-1) (MJy sr-1)   (Jy2 sr-1)
               
250 6 18.1 $3.3\pm0.5$ (0.01) $20.1\pm3.1$ (0.1) 1.26 $-2.65\pm0.10$ $5\pm 2\times 10^3$
350 10 25.2 $1.7\pm0.3$ (0.008) $10.1\pm1.6$ (0.05) 0.55 $-2.69\pm 0.13$ 4 $\pm 2 \times 10^3$
500 14 36.9 $0.7\pm0.1$ (0.003) $4.3\pm0.7$ (0.02) 0.34 $-2.62\pm 0.17$ $1\pm 1 \times 10^3$

Notes. Columns 4 and 5: gain and offset coefficients of the SPIRE-IRIS 100 $\mu $m correlations. The uncertainty on G represents the rms of the ratio $S(\lambda)/S(100~\mu{\rm m})$ once the offset S0 is removed from the SPIRE data. Similarly the uncertainty on S0 is the rms of $S(\lambda) - G\times S(100~\mu{\rm m})$. These two uncertainties are correlated, but they give more realistic estimates compared to the statistical ones obtained with the linear regression fit (given in brackets). Column 6: noise level estimated directly on the power spectrum for $k>0.75k_{\rm max}$ (3.75<k<5 arcmin-1 at 250 $\mu $m). Column 7: power spectrum exponent of the interstellar component. Column 8: level of the Poissonian component associated with point sources and the CIB fluctuations. The fit of the power spectrum ($\gamma$ and P0) was done between k = 0.025 arcmin-1 and about twice the FWHM (2.0, 1.2 and 0.86 arcmin-1 at 250, 350 and 500 $\mu $m respectively).


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