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Craig L. Sarazin

Publications and source records attributed to Craig L. Sarazin.

116 records · Page 7Linked to original sources

Excitation of the 3.071mm Hyperfine Line in Li-Like 57-Fe in Astrophysical Plasmas

As noted first by Sunyaev & Churazov (1984), the 3.071 mm hyperfine line from $^{57}Fe^{+23}$ might be observable in astrophysical plasmas. We assess the atomic processes which might contribute to the excitation of this line. We determine the intensity of the hyperfine line from an isothermal, coronal plasma in collisional ionization equilibrium and for a coronal plasma cooling isobarically due to its own radiation. Comparisons of the hyperfine line to other lines emitted by the same ion, Fe$^{+23}$, are shown to be useful for deriving the isotopic fraction of $^{57}$Fe. We calculate the ratios of the hyperfine line to the 2s--2p EUV lines at 192 Åand 255 Å, and the 2s--3p X-ray doublet at 10.6 Å.

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Low Mass X-ray Binaries As the Source of the Very Soft X-ray Emission in the X-ray Faintest Early-Type Galaxies

The X-ray emission from the faintest X-ray elliptical and S0 galaxies is characterized by a hard ~5 keV component, and a very soft ~0.2 keV component. The hard component has generally been regarded as the integrated emission from low mass X-ray binaries (LMXBs), but the origin of the soft component is unknown. We present evidence which suggests that LMXBs also exhibit a soft component, which is responsible for the very soft X-ray emission in the faintest early-type galaxies. This soft component is present in two Galactic LMXBs which lie in directions of low Galactic hydrogen column densities, and in LMXBs in the bulge of M31, which comprise a majority of the X-ray emission in the bulge of that galaxy. The X-ray spectral characteristics and X-ray-to-blue luminosity ratios of the bulges of M31 and the Sa galaxy NGC 1291 are very similar to those of the X-ray faintest early-type galaxies, indicating that LMXBs are responsible for both soft and hard components in the latter. In addition, a low temperature interstellar medium might be present in some X-ray faint galaxies.

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X-Ray Spectral Properties of the Cluster Abell 2029

We have analyzed ASCA and ROSAT PSPC spectra and images of the galaxy cluster Abell 2029. The ASCA spectra of the cluster indicate that the gas temperature declines with radius. The PSPC image shows that the cluster is very regular and smooth. Also, there is no significant evidence for any irregularities in the temperature distribution in the cluster, as would be produced by a subcluster merger. These results suggest that A2029 is a relaxed cluster, and that the gas is in hydrostatic equilibrium. We use the assumption of equilibrium to determine the gravitational mass of the cluster as a function of radius. At a radius of 16' (1.92 h_50^-1 Mpc), the gravitational mass is M_tot = (9.42+-4.22) x 10^14 h_50^-1 Msun, while the mass of gas is M_gas = (2.52+-0.77) x 10^14 h_50^-5/2 Msun. The gas fraction is found to increase with radius; within a spherical radius of 16', the fraction is (M_gas/M_tot) = (0.26+-0.14) h_50^-3/2. The iron abundance in the gas is found to be (0.40+-0.04) of solar. There is no significant evidence for any variation in the abundance with position in the cluster. The global X-ray spectra, central X-ray spectra, and ROSAT surface brightness all require a cooling flow at the cluster center. The global X-ray spectrum implies that the total cooling rate is 363^+79_-96 h_50^-2 Msun/yr. The global X-ray spectra are consistent with the Galactic value for the soft X-ray absorption toward the cluster. The PSPC spectra of the central regions of the cluster are inconsistent with the large value of foreground excess absorption found by White et al. (1991) based on the Einstein SSS spectrum. The upper limit on excess foreground absorption is 7.3 x 10^19 cm^-2. However, the spectra do not rule a significant amount of intrinsic absorbing gas located within the cooling flow region.

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Extreme Ultraviolet Emission from Clusters of Galaxies: Inverse Compton Radiation from a Relic Population of Cosmic Ray Electrons?

We suggest that the luminous extreme ultraviolet (EUV) emission which has been detected recently from clusters of galaxies is Inverse Compton (IC) scattering of Cosmic Microwave Background (CMB) radiation by low energy cosmic ray electrons in the intracluster medium. The cosmic ray electrons would have Lorentz factors of gamma ~ 300, and would lose energy primarily by emitting EUV radiation. These particles have lifetimes comparable to the Hubble time; thus, the electrons might represent a relic population of cosmic rays produced by nonthermal activity over the history of the cluster. The IC model naturally explains the observed increase in the ratio of EUV to X-ray emission with radius in clusters. The required energy in cosmic ray electrons is typically 1--10% of the thermal energy content of the intracluster gas. We suggest that the cosmic ray electrons might have been produced by supernovae in galaxies, by radio galaxies, or by particle acceleration in intracluster shocks.

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High Resolution X-ray Spectra of Cluster Cooling Flows

The cooling cores of clusters of galaxies are among the brightest thermal X-ray line sources in the universe. High resolution X-ray spectra would allow individual line fluxes to be measured. The fluxes of low ionization X-ray lines in cooling flows should be directly proportional to the cooling rate at relatively cool temperatures, and could be used to determine whether large amounts of gas are really cooling out of the X-ray band (below 10e6 K). By comparing the fluxes of many X-ray lines, we could determine the amounts of gas at different temperatures and densities. This would allow one to test the idea that cooling flows are highly inhomogeneous, as required to explain their surface brightness profiles. High resolution X-ray spectra can be used to determine velocities in the hot gas in cooling flows. If the gas is homogeneous, significant inflow velocities are expected. However, if the gas is as inhomogeneous as we currently believe, the inflow velocities are likely to be rather low (v < 30 km/s). Most of the central galaxies in cooling flows host radio sources, and it appears that the radio lobes are expanding against, displacing, and compressing the cooling X-ray gas. Significant motions associated with the expansion of radio sources should be detectable in X-ray lines. If the cooling X-ray gas rotates and viscosity is not important, rotational motions may also be detectable in X-ray line spectra.

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Cluster Cooling Flows: Recent Progress and Outstanding Questions

Recent results on cluster cooling flows are reviewed. Observations of excess soft X-ray provides the only direct evidence for a major repository for the cooled gas. Unfortunately, the frequency of occurrence of large excess columns is uncertain. There is also great uncertainty about the physical state of the material producing the absorption. Radio observations have ruled out most forms of cold gas. Recent radio observations show that the plasma in cooling flows is strong magnetized. Models for cooling flows including the dynamical effects of the magnetic field are needed. We also need to understand what ultimately happens to the advected magnetic flux. At present, it appears most likely that the field is by field line reconnection. The radio sources associated with the central galaxies in cluster cooling flows seem to come in two varieties. There are ``lobe-dominated sources'' with strong radio jets and well-defined radio lobes, and ``amorphous'' sources without strong jets or lobes. In the lobe-dominated sources, the radio pressures agree approximately with the pressures of the X-ray emitting thermal gas, the X-ray and radio images anticorrelate, and the radio sources are highly polarized and have very large Faraday rotations. In the amorphous sources, the radio pressures are much smaller than the X-ray pressures, the X-ray and radio images correlate, and the radio sources are strongly depolarized. These results suggest that the lobes in the lobe-dominated sources have displaced the X-ray emitting gas, while in the amorphous sources, the radio and thermal plasma are mixed.

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X-ray Emission from Elliptical Galaxies

Elliptical galaxies are generally luminous sources of X-ray radiation, and contain large amounts of hot, interstellar gas. In the brighter X-ray galaxies, the inferred masses of hot gas are consistent with those expected given the present rates of stellar mass loss. The required rates of heating of the gas are also roughly consistent with those expected from the motions of gas losing stars. X-ray observations, particularly X-ray spectra, require a low rate of Type Ia supernova heating and chemical enrichment in the gas. In the brightest X-ray galaxies, the cooling times in the gas are short, which suggests that the gas forms steady-state cooling flows. Steady cooling models explain most of the properties of the brighter X-ray galaxies, including their luminosities, the X-ray--optical correlation, their temperatures, and their surface brightness profiles. Although the optical and X-ray luminosities of early-type galaxies are strongly correlated, there is a large dispersion in this correlation. The origin of the emission in the X-ray faint ellipticals is less certain. All ellipticals appear to have a hard X-ray spectral component due to accreting binary systems. X-ray faint ellipticals also have a very soft X-ray component, which may be residual hot interstellar gas. The X-ray spectra of ellipticals indicate that the abundance of iron is well below the solar value, which implies that the rate of Type Ia supernova contamination is small. The abundances and evidence for gradient gradients suggest that stellar abundance gradients and inflow of the gas affect the X-ray spectra.

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ROSAT X-ray Observations of the Cooling Flow Cluster A2597

The cluster A2597 was observed in X-rays with the ROSAT PSPC and HRI detectors. The X-ray isophotes are oriented similarly to the optical isophotes of the central cD galaxy and to the isopleths of the galaxy distribution in the cluster, but are otherwise quite regular, suggesting that this cluster is reasonably relaxed and in hydrostatic equilibrium. The merged HRI and PSPC surface brightness profile is not adequately fit by a beta model because of the central X-ray surface brightness peak, indicating the presence of a cooling flow. If the central 108 arcsec in radius are excluded, an acceptable fit is found which gives beta = 0.64 but only an upper limit to the core radius, rcore < 78 arcsec. Within a radius of 2 Mpc, we found masses of Mgas = 1.2e14 Msun and Mtot = 6.5e14 Msun, and a gas mass fraction of about 19%. Both the overall cluster spectrum and the spatially resolved spectra within 300 kpc require the presence of both hot gas and a cooling flow in the spectrum. The spectrally determined total cooling rate of Mdot = 344 Msun/yr is in good agreement with those derived from analyses of the X-ray surface brightness profile from the Einstein IPC and the ROSAT HRI images. The ROSAT spatially resolved X-ray spectra indicate that the cooling component is distributed over the inner ~300 kpc in radius of the cluster. We do not detect any significant excess X-ray absorption toward the center of A2597, and we set a very conservative upper limit on the excess column in front of the cooling flow region of NH < 1.72e20 cm**-2.

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