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Figure 1: NEP 1239: ( top) longslit spectrum of RXJ 1715.4+6239, QSO 2 candidate at z=0.85, obtained with the University of Hawai'i 2.2 m telescope; ( bottom) longslit spectrum of the same object at redder wavelengths taken at the TNG 3.6 m telescope. The dashed lines indicate the positions of the emission lines at the object redshift. Wavelengths of atmospheric absorption (or bad sky subtracion) are also indicated. |
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Figure 2: NEP 1640: ( top) longslit spectrum of RXJ 1724.9+6636, QSO 2 candidate at z=0.6758, obtained with the University of Hawai'i 2.2 m telescope; ( center) longslit spectrum of the same object taken at the TNG 3.6 m telescope with the High Resolution grism and ( bottom) the Medium Resolution grism. The dashed lines indicate the positions of the emission lines at the object redshift. Wavelengths of atmospheric absorption (or bad sky subtracion) are also indicated. |
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Figure 3: NEP 2131: longslit spectrum of RX J1737.0+6601, QSO 2 candidate at z=0.358, obtained with the TNG 3.6 m telescope and the Medium Resolution grism in the bluer ( top) and redder ( bottom) wavelength region. The dashed lines indicate the positions of the emission lines at the object redshift. Wavelengths of bad sky subtraction are also indicated. |
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Figure 4: X-ray spectra and model ( upper panel) and ratio between the two ( lower panel) for NEP 1239. |
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Figure 5: X-ray spectra and model ( upper panel) and ratio between the two ( lower panel) for NEP 1640. |
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Figure 6: X-ray spectra and model ( upper panel) and ratio between the two ( lower panel) for NEP 2131. |
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Figure 7:
Contour plot of the two free parameters in absori + power
law, ![]() ![]() ![]() |
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