1998
DOI: 10.1046/j.1365-8711.1998.01839.x
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Oscillatory instability of radiative shocks with multiple cooling processes

Abstract: A B S T R A C TThe stand-off shock formed in the accretion flow on to a stationary wall, such as the surface of a white dwarf, may be thermally unstable, depending on the cooling processes which dominate the post-shock flow. Some processes lead to instability, while others tend to stabilize the shock. We consider competition between the destabilizing influence of thermal bremsstrahlung cooling, and a stabilizing process which is a power law in density and temperature. Cyclotron cooling and processes which are … Show more

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Cited by 32 publications
(59 citation statements)
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“…Considering the perturbative analysis, the system is expected to stabilize as cyclotron becomes a strong contribution in the radiative losses (Saxton et al 1998;Saxton 1999;Saxton & Wu 1999). In the results presented in this work, for a white dwarf Fig.…”
Section: Psac Efficiently Cooled By the Cyclotron Processmentioning
confidence: 70%
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“…Considering the perturbative analysis, the system is expected to stabilize as cyclotron becomes a strong contribution in the radiative losses (Saxton et al 1998;Saxton 1999;Saxton & Wu 1999). In the results presented in this work, for a white dwarf Fig.…”
Section: Psac Efficiently Cooled By the Cyclotron Processmentioning
confidence: 70%
“…At such high temperatures, matter radiates strongly through optically thin bremsstrahlung, which dominates the hard X-ray emission (Frank et al 2002). Moreover, for the highest magnetized polars, the energy can also be transported efficiently by the cyclotron process (Saxton et al 1998), which emits mainly in the optical domain for the range of polar magnetic fields. As infalling material cools and slows down, it also gets denser with a sharp gradient near the surface.…”
Section: Brief Review Of the Accretion Column Standard Modelmentioning
confidence: 99%
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“…The cooling time is given by t cool ∼ P/Λ, with P the thermal pressure and Λ the cooling function. The parameter s can then be expressed as a function of the polar parameters (Saxton et al 1998) where m is the specific accretion rate. Bremsstrahlung emission is dominant when s < 1, whereas cyclotron emission dominates for s > 1.…”
Section: The Model Equationsmentioning
confidence: 99%
“…Chevalier & Imamura 1982;Imamura et al 1996;Saxton et al 1997Saxton et al , 1998Saxton & Wu 1999, 2001. When bremsstrahlung emission is the only cooling process the fundamental mode is stable, and the overtones are unstable, with instability δ R tending to increase with harmonic number.…”
Section: Perfect Stationary Wallmentioning
confidence: 99%