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No consensus has been reached as to a single model for the QPO phenomenon. Theoretical models suggest dense blobs in orbit within the inner disk (Bath 1973), pulsations on the surface of the white dwarf (Papaloizou & Pringle 1978), or oscillating a
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The spectroscopy of GK Per obtained by MSR exhibit broad Balmer and HeI lines, as well as high excitation lines of HeII, NIII and CIII. With this model, both phenomena are taken into account, and no new models of QPO formation are required. The asymmetry appears periodic in the blue-shifted material, and seem to be caused by some type of absorption. coustic waves in the inner regions of the accretion disk (Okuda et al. Observations
To support their hypotheses, MSR observed the source between February 26 and 28 in 1996. By subtracting this fit from the spectra, they correlated the absorption spectra with their templates. Fitting their data with that of previous researchers, MSR calculated ƒ× = 30 „b 1 km/s, K = 119 „b 2 km/s, and ƒÖ0 = 0. Kraft (1964), Gallagher & Oinas (1974), Crampton, Cowley & Fisher (1994) and Reinsch (1994) all identify these as characteristics of a K-type secondary star. 5m Isaac Newton Telescope (INT) at La Palma, they were able to get visual spectrophotometry of GK Per. As a result, the signal will be biased toward the blue (MSR 1999). However, these models can only account for QPOs of a few hundred seconds. Since GK Per has a relatively weak magnetic field, the accretion disk will come very close to the star, completely surrounding the magnetic field. Again using the Lomb-Scargle algorithm, power spectra were produced for the three nights of observations.
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