of a probable infrared counterpart at R.A. = 18h29ms, decl. The two known X-ray outbursts of XTE J are separated by ~ At coordinates (J) R.A. = 18h29ms, Decl. = d51′”, this XTE J in the XMM-Newton EPIC pn (J) 18 29 XMM-Newton Detection of the s Pulsar XTE J Authors: Halpern, J. P.; Gotthelf Its position is R.A. = 18h29ms, Decl. = d51’23” (J).

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DubVision – Fall Apart 3. Measured radial velocities of the Cepheid pointswith the removed pulsations overplotted on the orbital solution.

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Type II Cepheids are low-mass pulsating stars that belong to the disc and halo populations Wallerstein Breathe Carolina – Glue 3. The equations for the masses are derived from the orbital solution with the known inclination and Kepler ‘s third law, substituting the dependence on the semimajor axis deccl the one on the p -factor Equation 1.

Toby Green – Lift Me Up 5. The expected nonlinear period shifts for type II Cepheids were studied in detail by Smolec ; see in particular their Figure 6.

We used the interstellar extinction law relations provided by Cardelli et al. In our method 0998 physical parameters scale with the p -factor, which means that determining the mass of the Cepheid allows an estimation of this important parameter. If we adopt a fixed period obtained from the photometry, the fit of the model to the measured RVs is not satisfactory unless we significantly increase from 4 to 7—8 the order of the Fourier series that describes the pulsations.

Velocities measured from the Balmer lines were not accurate enough to enable us to measure an orbit for the companion. In some cases, where additional light sources were also visible we have included them in the profile fitting with fixed velocities. Breathe Carolina, Flatdisk – Hotel 5. We have applied this method to eclipsing binaries containing classical Cepheids and 09 very precise masses Pilecki et al. Three cases for different p -factors are presented.


Optical/IR Candidates for XTE J

Detected additional sources with constant velocities are shown as dotted lines. In fact, the position of the Cepheid between the period—luminosity relations of classical and type II Cepheids resembles the position of Anomalous Cepheids, which are interpreted as mergers with masses of about 1.

Avena Savage – Back To Life 6. This code, together with its nonlinear version, has been extensively used to study the dynamical behavior of type II Cepheids—see Smolec and references therein.

K -band photometry covering the eclipses would greatly help in determining the temperatures of both components.

Parameters for three cases for p -factors 1. By increasing the effective temperature by just 10 K, the pulsation calculations yield 3. This value is independent decll the assumed Aas it comes directly from the modeling of the light curves and the pulsational RV curve. Player FM might just be it.

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Devl publishing company, IOP Publishing, is a world leader in professional scientific communications. Here we use the exact same model parameters structure of numerical grid and parameters of the turbulent convection model as the above study.

For the K -band the third-order Fourier fit is shown as well. This paper includes data gathered with the 6. In several spectra other sources were detected at constant velocities: Joe Stone – Let’s Go Together Eric Lumiere Sagan Remix 4. Using the formulas from Challouf et al.

Click here to close this overlay, or press the “Escape” key on your keyboard. Florian Picasso – Hanoi to Paris Austin Mahone – Speed Of Sound 3.

These values are presented in Table 5. Charlotte Lawrence – Cold As Stone5. At each p -factor, the minimum and maximum fundamental mode period in a set of models with different effective temperatures and different metallicities is plotted. The system and individual magnitudes were dereddened using a value of the ratio of the total to selective extinction ofand assuming an average combined LMC and Galactic foreground value of 0.


Paul Aiden – Alive Extended Mix Oruz – Rockin’ 5. The use of scaling to estimate the mass of the Cepheid is described in Section 5. The mission of the AAS is to enhance and share humanity’s scientific understanding of the universe. The system configuration and especially the masses strongly suggest a binary interaction in the evolutionary history as necessary to solve the Algol paradox. For the second one Solution 2 or S2 we used only the OGLE I C data with period, T Iand the third light fixed, as the former ones are band-independent and benefit from a longer baseline and the latter dfcl hard to establish using only one band.

Thompson 3Richard I. Matthew Steeper – Speed Of Sound 3. All of the aforementioned additional objects detected in the spectra showed constant velocity within the errors, so it is highly unlikely that one of them is the supposed third component of the system, as it would have to be much more massive than the stars in the eclipsing binary together. Spectra with very high signal-to-noise ratios would be required, together with careful spectral disentangling, to try to eecl the Cepheid companion and measure its velocity.

At the moment, the results obtained on the period change of the Cepheid are not conclusive and a longer observational baseline would be needed to confirm the erratic period 0998.


In the color—magnitude diagram Figure 14 the Cepheid in the system with the companion lies to the blue of the overall distribution of type II Cepheids. The orbital period P orb and the time of the spectroscopic conjunction T 0 were kept fixed at the values taken from the preliminary analysis of the photometry. Your subcriptions will sync with your account on this website too.

If these mesh parameters are altered, e.