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Felix Ryde

Publications and source records attributed to Felix Ryde.

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On the Shape of Pulse Spectra in Gamma-Ray Bursts

The discovery (Liang & Kargatis 1996), that the peak energy of time-resolved spectra of gamma-ray burst (GRB) pulses decays exponentially with fluence, is analytically shown to imply that the time-integrated photon number spectrum of a pulse should have a unique shape, given by an underlying E^-1 behavior. We also show that the asymptotic low energy normalization of the time-integrated spectrum is equal to the exponential decay constant. We study analytically how this general behavior is modified in more realistic situations and show that diversity is then introduced in the properties of time-integrated GRB pulse spectra. We argue that further diversity will occur in time-integrated multi-pulse (complex) GRB spectra. The total energy received per cm^2 is approximately the decay constant times the maximum peak energy of the pulse. Our analytical results connect the properties of the time-integrated pulse spectrum with those of the time-resolved spectra, and can thus be used when studying observed GRB pulse spectra. We illustrate with the bright burst GRB 910807 and comment on GRB 910525 and GRB 921207.

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The Nature of Spectral Transitions in Accreting Black Holes: The Case of Cyg X-1

Accreting black holes radiate in one of several spectral states, switching from one to another for reasons that are as yet not understood. Using the best studied example, Cyg X-1, we identify the geometry and physical conditions characterizing these states. In particular, we show that in the hard state most of the accretion energy is dissipated in a corona-like structure which fills the inner few tens of gravitational radii around the black hole and has Compton optical depth of order unity. In this state, an optically thick accretion disc extends out to greater distance, but penetrates only a short way into the coronal region. In the soft state, the optically thick disc moves inward and receives the majority of the dissipated energy, while the "corona" becomes optically thin and extends around much of the inner disc. The mass accretion rate in both states is $~10^{-8} M_{\odot}$ yr$^{-1}$.

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The variable X/gamma-ray spectrum of the Seyfert 2 galaxy NGC 7172

A broad band X-, gamma-ray spectral study of the Seyfert 2 galaxy NGC 7172 is presented. We use our ASCA observations from May 1995 and combine these with the CGRO OSSE data from March 1995. The only Seyfert 2 galaxy previously to have been modelled over such a broad spectral range is NGC 4945. We find that the most probable model for the data is an absorbed power law, being affected by a high energy exponential cut-off. The power law is flat with Gamma = 1.54 \pm 0.13, while N_H = (8.1 \pm 0.6) 10^{22} cm$^{-2}$. An Fe K$α$ emission line is not required by the fits. The observed flux in the 2-10 keV range is F_{2-10} = (4.75\pm 0.09) 10^{-11} erg cm$^{-2}$ s$^{-1}$, which corresponds to a small increase since the Ginga measurement in October 1989. The spectral index of the underlying power law of NGC 7172 appears actually to have varied from 1.85 to 1.5 since the Ginga observations in 1989. The e-folding energy is relatively well constrained and lies at 140 ^{+310} _{-70} keV. We note, however, that the CGRO OSSE spectral shape appears to be variable on a time scale of weeks.

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The X/gamma-ray spectral properties of NGC 7172

We present a combined, non-simultaneous, ASCA GIS and CGRO OSSE spectrum of the Seyfert 2 galaxy, NGC 7172, and make broad band spectral fits. The only Seyfert 2 galaxy previously studied over such a broad band is NGC 4945. We find that the most probable model for the data is a power law with an exponential cut-off being affected by a neutral absorber. The best fit parameters are found to be $Γ= 1.47 \pm 0.15$ and $\NH = (7.8 \pm 0.6) 10^{22}$ cm$^{-2}$. The spectral index of the underlying power law of NGC 7172 has therefore varied from 1.8 to 1.5 since the Ginga observations in 1989. For this simple model the e-folding energy at $88^{+65}_{-28}$ keV is relatively well constrained. The observed flux in the 2-10 keV range is $F_{2-10}=4.7 10^{-11}$ erg cm$^{-2}$ s$^{-1}$, which corresponds to a small increase since the Ginga measurement in October 1989.

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