17 research outputs found
Doppler tomography and photometry of the cataclysmic variable 1RXS J064434.5+334451
We have obtained simultaneous photometric and spectroscopic observations of the cataclysmic variable 1RXS J064434.5+334451. We have calibrated the spectra for slit losses using simultaneous photometry, allowing us to construct reliable Doppler images from H? and He?ii 4686-Å emission lines. We have improved the ephemeris of the object based on new photometric eclipse timings, obtaining HJD = 245?3403.759?533 + 0.269?374?46E. Some eclipses present a clear internal structure, which we attribute to a central He?ii emission region surrounding the white dwarf, a finding supported by Doppler tomography. This indicates that the system has a large inclination angle i = 78 ± 2°. We have also analysed the radial velocity curve from the emission lines to measure its semi-amplitude, K1, from H? and He?ii 4686 and derive the masses of the components M1 = 0.82 ± 0.06 M?, M2 = 0.78 ± 0.04 M? and their separation a = 2.01 ± 0.06 R?. The Doppler tomography and other observed features in this nova-like system strongly suggest that this is a SW Sex type system
Aneurisma de arteria renal como causa de hipertensión arterial en paciente joven
Renal artery aneurysms are a rare cause of arterial hypertension. The diagnosis is made usually with imaging techniques during the evaluation of secondary hypertension. Their resolution, by percutaneous procedures or surgery, drives mostly to remission of hypertension.Los aneurismas de arteria renal son una causa poco frecuente de hipertensión arterial. Se diagnostican mediante pruebas de imagen durante el cribado de hipertensión arterial secundaria. Su reparación, tanto por vÃa percutánea como quirúrgica, conduce en la mayorÃa de los casos a la resolución de la hipertensión arterial
U Geminorum: a test case for orbital parameters determination
High-resolution spectroscopy of U Gem was obtained during quiescence. We did
not find a hot spot or gas stream around the outer boundaries of the accretion
disk. Instead, we detected a strong narrow emission near the location of the
secondary star. We measured the radial velocity curve from the wings of the
double-peaked H emission line, and obtained a semi-amplitude value that
is in excellent agreement with the obtained from observations in the
ultraviolet spectral region by Sion et al. (1998). We present also a new method
to obtain K_2, which enhances the detection of absorption or emission features
arising in the late-type companion. Our results are compared with published
values derived from the near-infrared NaI line doublet. From a comparison of
the TiO band with those of late type M stars, we find that a best fit is
obtained for a M6V star, contributing 5 percent of the total light at that
spectral region. Assuming that the radial velocity semi-amplitudes reflect
accurately the motion of the binary components, then from our results: K_em =
107+/-2 km/s; K_abs = 310+/-5 km/s, and using the inclination angle given by
Zhang & Robinson(1987); i = 69.7+/-0.7, the system parameters become: M_WD =
1.20+/-0.05 M_sun,; M_RD = 0.42+/-0.04 M_sun; and a = 1.55+/- 0.02 R_sun. Based
on the separation of the double emission peaks, we calculate an outer disk
radius of R_out/a ~0.61, close to the distance of the inner Lagrangian point
L_1/a~0.63. Therefore we suggest that, at the time of observations, the
accretion disk was filling the Roche-Lobe of the primary, and that the matter
leaving the L_1 point was colliding with the disc directly, producing the hot
spot at this location.Comment: 36 pages, 14 figures, ccepted for publication in A