3,734 research outputs found
A connection between orthogonal polynomials on the unit circle and matrix orthogonal polynomials on the real line
Szego's procedure to connect orthogonal polynomials on the unit circle and
orthogonal polynomials on [-1,1] is generalized to nonsymmetric measures. It
generates the so-called semi-orthogonal functions on the linear space of
Laurent polynomials L, and leads to a new orthogonality structure in the module
LxL. This structure can be interpreted in terms of a 2x2 matrix measure on
[-1,1], and semi-orthogonal functions provide the corresponding sequence of
orthogonal matrix polynomials. This gives a connection between orthogonal
polynomials on the unit circle and certain classes of matrix orthogonal
polynomials on [-1,1]. As an application, the strong asymptotics of these
matrix orthogonal polynomials is derived, obtaining an explicit expression for
the corresponding Szego's matrix function.Comment: 28 page
A Statistical Study of Photospheric Magnetic Field Changes During 75 Solar Flares
Abrupt and permanent changes of photospheric magnetic fields have been
observed during solar flares. The changes seem to be linked to the
reconfiguration of magnetic fields, but their origin is still unclear. We
carried out a statistical analysis of permanent line-of-sight magnetic field
() changes during 18 X-, 37 M-, 19 C- and 1 B-class flares using
data from Solar Dynamics Observatory/Helioseismic and Magnetic Imager. We
investigated the properties of permanent changes, such as frequency, areas, and
locations. We detected changes of in 59/75 flares. We find that
strong flares are more likely to show changes, with all flares M1.6
exhibiting them. For weaker flares, permanent changes are observed in 6/17
C-flares. 34.3\% of the permanent changes occurred in the penumbra and 18.9\%
in the umbra. Parts of the penumbra appeared or disappeared in 23/75 flares.
The area where permanent changes occur is larger for stronger flares. Strong
flares also show a larger change of flux, but there is no dependence of the
magnetic flux change on the heliocentric angle. The mean rate of change of
flare-related magnetic field changes is 20.7 Mx cm min. The
number of permanent changes decays exponentially with distance from the
polarity inversion line. The frequency of the strength of permanent changes
decreases exponentially, and permanent changes up to 750 Mx cm were
observed. We conclude that permanent magnetic field changes are a common
phenomenon during flares, and future studies will clarify their relation to
accelerated electrons, white light emission, and sunquakes to further
investigate their origin.Comment: Piblished in Ap
Multipliers of Laplace Transform Type for Laguerre and Hermite Expansions
We present a new criterion for the weighted boundedness of
multiplier operators for Laguerre and Hermite expansions that arise from a
Laplace-Stieltjes transform. As a special case, we recover known results on
weighted estimates for Laguerre and Hermite fractional integrals with a unified
and simpler approach.Comment: 22 pages; new section added, corrected typos, new references adde
Quadratic Maps in Two Variables on Arbitrary Fields
Let be a field of characteristic different from and , and
let be a vector space of dimension over . The generic
classification of homogeneous quadratic maps under the action
of the linear group of , is given and efficient computational criteria to
recognize equivalence are provided.Comment: 12 pages, no figure
Interface growth in two dimensions: A Loewner-equation approach
The problem of Laplacian growth in two dimensions is considered within the
Loewner-equation framework. Initially the problem of fingered growth recently
discussed by Gubiec and Szymczak [T. Gubiec and P. Szymczak, Phys. Rev. E 77,
041602 (2008)] is revisited and a new exact solution for a three-finger
configuration is reported. Then a general class of growth models for an
interface growing in the upper-half plane is introduced and the corresponding
Loewner equation for the problem is derived. Several examples are given
including interfaces with one or more tips as well as multiple growing
interfaces. A generalization of our interface growth model in terms of
``Loewner domains,'' where the growth rule is specified by a time evolving
measure, is briefly discussed.Comment: To appear in Physical Review
Kinematic study of planetary nebulae in NGC 6822
By measuring precise radial velocities of planetary nebulae (which belong to
the intermediate age population), H II regions, and A-type supergiant stars
(which are members of the young population) in NGC 6822, we aim to determine if
both types of population share the kinematics of the disk of H I found in this
galaxy.
Spectroscopic data for four planetary nebulae were obtained with the high
spectral resolution spectrograph Magellan Inamori Kyocera Echelle (MIKE) on the
Magellan telescope at Las Campanas Observatory. Data for other three PNe and
one H II region were obtained from the SPM Catalog of Extragalactic Planetary
Nebulae which employed the Manchester Echelle Spectrometer attached to the 2.1m
telescope at the Observatorio Astron\'omico Nacional, M\'exico. In the
wavelength calibrated spectra, the heliocentric radial velocities were measured
with a precision better than 5-6 km s. Data for three additional H II
regions and a couple of A-type supergiant stars were collected from the
literature. The heliocentric radial velocities of the different objects were
compared to the velocities of the H i disk at the same position.
From the analysis of radial velocities it is found that H II regions and
A-type supergiants do share the kinematics of the H I disk at the same
position, as expected for these young objects. On the contrary, planetary
nebula velocities differ significantly from that of the H I at the same
position. The kinematics of planetary nebulae is independent from the young
population kinematics and it is closer to the behavior shown by carbon stars,
which are intermediate-age members of the stellar spheroid existing in this
galaxy. Our results are confirming that there are at least two very different
kinematical systems in NGC 6822
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