657,027 research outputs found
The Konkoly Blazhko Survey: Is light-curve modulation a common property of RRab stars?
A systematic survey to establish the true incidence rate of the Blazhko
modulation among short-period, fundamental-mode, Galactic field RR Lyrae stars
has been accomplished. The Konkoly Blazhko Survey (KBS) was initiated in 2004.
Since then more than 750 nights of observation have been devoted to this
project. A sample of 30 RRab stars was extensively observed, and light-curve
modulation was detected in 14 cases. The 47% occurrence rate of the modulation
is much larger than any previous estimate. The significant increase of the
detected incidence rate is mostly due to the discovery of small-amplitude
modulation. Half of the Blazhko variables in our sample show modulation with so
small amplitude that definitely have been missed in the previous surveys. We
have found that the modulation can be very unstable in some cases, e.g. RY Com
showed regular modulation only during one part of the observations while during
two seasons it had stable light curve with abrupt, small changes in the
pulsation amplitude. This type of light-curve variability is also hard to
detect in other Survey's data. The larger frequency of the light-curve
modulation of RRab stars makes it even more important to find the still lacking
explanation of the Blazhko phenomenon. The validity of the [Fe/H](P,phi_{31})
relation using the mean light curves of Blazhko variables is checked in our
sample. We have found that the formula gives accurate result for
small-modulation-amplitude Blazhko stars, and this is also the case for
large-modulation-amplitude stars if the light curve has complete phase
coverage. However, if the data of large-modulation-amplitude Blazhko stars are
not extended enough (e.g. < 500 data points from < 15 nights), the formula may
give false result due to the distorted shape of the mean light curve used.Comment: Accepted for publication in MNRAS, 14 pages, 7 Figure
Fitting Blazhko light curves
The correct amplitude and phase modulation formalism of the Blazhko
modulation is given. The harmonic order dependent amplitude and phase
modulation form is equivalent with the Fourier decomposition of multiplets. The
amplitude and phase modulation formalism used in electronic transmission
technique as introduced by Benk\H{o}, Szab\'o and Papar\'o (2011, MNRAS 417,
974) for Blazhko stars oversimplifies the amplitude and phase modulation
functions thus it does not describe the light variation in full detail.
The results of the different formalisms are compared and documented by
fitting the light curve of a real Blazhko star, CM UMa.Comment: 8 pages, 5 figures. Accepted for publication in MNRA
An extensive photometric study of the Blazhko RR Lyrae star RZ Lyr
The analysis of recent, extended multicolour CCD and archive photoelectric,
photographic and visual observations has revealed several important properties
of RZ Lyr, an RRab-type variable exhibiting large-amplitude Blazhko modulation.
On the time-base of \sim110 yr, a strict anticorrelation between the pulsation
and modulation period changes is established. The light curve of RZ Lyr shows a
remarkable bump on the descending branch in the small-amplitude phase of the
modulation, similarly to the light curves of bump Cepheids. We speculate that
the stellar structure temporally suits a 4:1 resonance between the periods of
the fundamental and one of the higher-order radial modes in this modulation
phase. The light-curve variation of RZ Lyr can be correctly fitted with a
two-modulation-component solution; the 121 d period of the main modulation is
nearly but not exactly four times longer than the period of the secondary
modulation component. Using the inverse photometric method, the variations in
the pulsation-averaged values of the physical parameters in different phases of
both modulation components are determined.Comment: 15 pages, 14 figures, 8 tables. Published in MNRAS, 2012. [v3]: Only
change: title correcte
Acousto-electro-optic light modulation
The acousto-electro-optic effect is analyzed and demonstrated experimentally. The application of the acousto-electro-optic effect to light modulation and deflection is discussed
Error propagation in polarimetric demodulation
The polarization analysis of the light is typically carried out using
modulation schemes. The light of unknown polarization state is passed through a
set of known modulation optics and a detector is used to measure the total
intensity passing the system. The modulation optics is modified several times
and, with the aid of such several measurements, the unknown polarization state
of the light can be inferred. How to find the optimal demodulation process has
been investigated in the past. However, since the modulation matrix has to be
measured for a given instrument and the optical elements can present problems
of repeatability, some uncertainty is present in the elements of the modulation
matrix and/or covariances between these elements. We analyze in detail this
issue, presenting analytical formulae for calculating the covariance matrix
produced by the propagation of such uncertainties on the demodulation matrix,
on the inferred Stokes parameters and on the efficiency of the modulation
process. We demonstrate that, even if the covariance matrix of the modulation
matrix is diagonal, the covariance matrix of the demodulation matrix is, in
general, non-diagonal because matrix inversion is a nonlinear operation. This
propagates through the demodulation process and induces correlations on the
inferred Stokes parameters.Comment: 18 pages, 3 figures, accepted for publication in Applied Optic
Postquench prethermalization in a disordered quantum fluid of light
We study the coherence of a disordered and interacting quantum light field
after propagation along a nonlinear optical fiber. Disorder is generated by a
cross-phase modulation with a randomized auxiliary classical light field, while
interactions are induced by self-phase modulation. When penetrating the fiber
from free space, the incoming quantum light undergoes a disorder and
interaction quench. By calculating the coherence function of the transmitted
quantum light, we show that the decoherence induced by the quench spreads in a
light-cone fashion in the nonequilibrium many-body quantum system, leaving the
latter prethermalize with peculiar features originating from disorder.Comment: 18 pages, 5 figure
Light modulation in phoxonic nanocavities
We report on the occurrence of strong nonlinear acousto-optic interactions in phoxonic structures, that
support, simultaneously, acoustic and optical localized resonant modes, under the influence of acoustic
losses. Deploying a detailed theoretical investigation of the acousto-optic coupling in the specific case
of a one-dimensional phoxonic cavity, realized by homogeneous SiO2 and Si layers, we demonstrate
the possibility for an enhanced modulation of light with sound through multi-phonon exchange mechanisms.
A full electrodynamic and elastodynamic multiple scattering approach is employed to describe the
optical and acoustic modes, and to account for their mutual interaction and the underlying effects both in
time and frequency domains. In particular, we discuss the influence of hypersonic attenuation on the
acousto-optic interaction by considering typical acoustic losses in the GHz regime
Dynamical light control in longitudinally modulated segmented waveguide arrays
We address light propagation in segmented waveguide arrays where the
refractive index is longitudinally modulated with an out-of-phase modulation in
adjacent waveguides, so that the coupling strength varies along propagation
direction. Thus in resonant segments coupling may be inhibited hence light
remains localized, while in detuned segments coupling results in complex
switching scenarios that may be controlled by stacking several resonant and
nonresonant segments. By tuning the modulation frequency and lengths of
waveguide segments one may control the distribution of light among the output
guides, including loca-lizing all light in the selected output channel.Comment: 12 pages, 4 figures, to appear in Europhysics Letter
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