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Subsections

2 Observations and data reduction

The spectra presented in this study were obtained using the ISO satellite (Kessler et al. 1996) with the SWS (de Graauw et al. 1996) and the LWS (Clegg et al. 1996) instruments. A log of the observations is provided in Table1.

For CepA, the positions of the spectrograph apertures are displayed in Fig.1. Our position CepA "East'' includes data with object names CepA IRS6A and CepA (except for observation 79201033) in the ISO data archive, while CepA "West'' assembles the CepA (W), CepA PK2 and the 79201033 data.

For L1448, the positions of the spectrograph apertures are shown in Fig.2. Here, we have six different positions, which we name N2, N1 in the northern lobe, C in the centre, and S1, S2, S3 in the southern lobe. They include the data with ISO names (see Table1) N and IRS3 for position N2, N2 for N1, L1448ON for C, S1 for S1, S for S2, and S2 and SIO for S3.

  

 
Table 1: Observation log for the CepheusA and L1448 data.

TDT
Object (ISO) Position $\alpha$(J2000) $ \delta$(J2000) AOT

09605051
CepAPK2 West 22 56 05 +61 01 57 SWS02
10101553 CepAPK2 West 22 56 05 +61 01 59 LWS01
22000636 CepAIRS6A East 22 56 19 +61 02 01 SWS02
22001001 CepA(W) West 22 56 05 +61 01 57 SWS02
24800552 CepAPK2 West 22 56 05 +61 01 57 SWS07
28301183 CepA East 22 56 21 +61 02 02 LWS01
41400837 CepA East 22 56 21 +61 02 03 SWS06
46500654 CepAPK2 West 22 56 05 +61 01 59 LWS04
46500669 CepAPK2 West 22 56 05 +61 01 59 LWS01
46500801 CepA(W) West 22 56 05 +61 01 59 LWS04
46500802 CepA(W) West 22 56 05 +61 01 59 LWS01
56300803 CepA East 22 56 18 +61 01 50 SWS07
56300918 CepA East 22 56 18 +61 01 48 LWS04
56301021 CepA East 22 56 18 +61 01 50 SWS02
56600809 CepAIRS6A East 22 56 19 +61 02 01 SWS02
56600810 CepAIRS6A East 22 56 20 +61 01 59 LWS02
65701021 CepA East 22 56 18 +61 01 50 SWS02
79201033 CepA West 22 56 05 +61 01 57 SWS02
84300404 CepAIRS6A East 22 56 20 +61 01 59 SWS01
65300362 L1448N2 N1 03 25 37 +30 44 42 LWS01
65300363 L1448S1 S1 03 25 40 +30 43 24 LWS01
65300364 L1448S2 S3 03 25 41 +30 41 59 LWS01
65300701 L1448 C 03 25 39 +30 44 05 LWS01
65300702 L1448N N2 03 25 36 +30 45 20 LWS01
65300703 L1448S S2 03 25 41 +30 42 44 LWS01
81401066 L1448ON C 03 25 39 +30 44 05 SWS02
81401067 L1448IRS3 N2 03 25 36 +30 45 20 SWS02
81601568 L1448N2 N1 03 25 37 +30 44 42 SWS02
81601569 L1448SIO S3 03 25 41 +30 41 58 SWS02
84701470 L1448S1 S1 03 25 40 +30 43 24 SWS02
84701471 L1448S S2 03 25 41 +30 42 44 SWS02



  \begin{figure}
\par\resizebox{6.5cm}{!}{\includegraphics[angle=-90,clip]{10188f2.eps}}
\end{figure} Figure 2: Positions of apertures of SWS and LWS observations in L1448 superimposed on an image in the 1-0S(1) line of H2 at 2.12$\mu $m.

2.1 SWS data

The ISO SWS instrument covered the wavelength range from 2.38 to 45.2$\mu $m. The two grating spectrometers had a spectral resolution of $R\approx1000{-}2000$ (AOT SWS01,02,06; see Table1), corresponding to a velocity resolution of $\Delta\nu\approx150{-}300$ kms-1. Higher resolution ( $R\approx 30\,000$) was achieved by inserting one of the two Fabry-Pérot filters (wavelength range $15{-}26~\mu$m, and $26{-}35~\mu$m respectively; AOT SWS07). The aperture of the SWS instrument is rectangular, with a size depending on the detector (i.e., wavelength). The typical aperture sizes of $14\hbox{$^{\prime\prime}$ }\times 27\hbox{$^{\prime\prime}$ }$are shown in Figs.1 and 2. For more details on the instrument and AOTs see the ISO Handbook, Volume VI: SWS-The Short Wavelength Spectrometer[*] and de Graauw et al. 1996.

The data were reduced using the standard pipeline version 8.4. We deglitched and flux calibrated the spectra with the ISO Spectral Analyses Package (ISAP 1.6a). Line fluxes (Gaussian fit centred on the line) were measured above the continuum (fit by a second order polynomial). We measured the line fluxes for each observation (TDT number) separately. Then the fluxes of the same line were averaged for each of our positions (see Table1). "Lines'' with a measured FWHM significantly smaller than the instrumental profile are not included, because we do not consider them as real.

2.2 LWS data

With the ISO LWS instrument, observations were carried out in the wavelength range from 43$\mu $m up to 196.9$\mu $m. Like with SWS, grating (AOT LWS01,02) or Fabry-Pérot (AOT LWS04) modes are available. Grating scans have a resolving power between 150-300 and the spectral resolution of the Fabry-Pérot mode varies between 6800 and 9700. The spatial resolution of the instrument is of the order of 80 $^{\prime\prime}$ (Swinyard et al. 1996). See the ISO Handbook, Volume IV: LWS-The Long Wavelength Spectrometer[*] and Clegg et al. (1996) for details.

The data were reduced using the standard pipeline 7. Data reduction was done similar to the SWS data, using the ISAP and LIA (version 7.3) software. Glitches due to cosmic rays were rejected and for every observation (TDT number) the line fluxes were measured. As for the SWS data, line fluxes of the same lines of spectra for each of our positions (see Table1) were averaged, again also excluding lines with FWHM significantly smaller than the instrumental profile. The FP data reduction was done by standard processing and we used associated LWS01 grating scans for optimizing the dark current. Afterwards the continuum was aligned horizontally in an interactive mode.


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