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.
TDT | Object (ISO) | Position | ![]() |
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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 |
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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![]() |
The ISO SWS instrument covered the wavelength range from 2.38 to 45.2m.
The two grating spectrometers had a spectral resolution of
(AOT SWS01,02,06; see Table1),
corresponding to a velocity resolution of
kms-1. Higher resolution
(
)
was achieved by inserting one of the two
Fabry-Pérot filters (wavelength range
m, and
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
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.
With the ISO LWS instrument, observations were carried out in the wavelength
range from 43m up to 196.9
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
(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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