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    <title>DSpace Collection:</title>
    <link>http://hdl.handle.net/2117/1132</link>
    <description />
    <items>
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        <rdf:li rdf:resource="http://hdl.handle.net/2117/6777" />
        <rdf:li rdf:resource="http://hdl.handle.net/2117/6775" />
        <rdf:li rdf:resource="http://hdl.handle.net/2117/6773" />
        <rdf:li rdf:resource="http://hdl.handle.net/2117/6700" />
        <rdf:li rdf:resource="http://hdl.handle.net/2117/3046" />
        <rdf:li rdf:resource="http://hdl.handle.net/2117/1244" />
        <rdf:li rdf:resource="http://hdl.handle.net/2117/1242" />
        <rdf:li rdf:resource="http://hdl.handle.net/2117/969" />
      </rdf:Seq>
    </items>
    <dc:date>2013-05-24T04:19:03Z</dc:date>
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  <item rdf:about="http://hdl.handle.net/2117/6777">
    <title>Classification of local stellar populations: the improved MEMPHIS algorithm - Part II</title>
    <link>http://hdl.handle.net/2117/6777</link>
    <description>Title: Classification of local stellar populations: the improved MEMPHIS algorithm - Part II
Authors: Cubarsí Morera, Rafael; Alcobé López, Santiago
Abstract: Discontinuities of the local velocity distribution which are associated with stellar populations&#xD;
are studied from the improved statistical method MEMPHIS (Maximum Entropy of&#xD;
the Mixture Probability from HIerarchical Segregation), by combining a sampling parameter,&#xD;
optimisation of the mixture approach, and maximum partition entropy of populations&#xD;
composing the stellar sample. The sampling parameter is associated with isolating integrals&#xD;
of the star motion and it is used to build a hierarchical family of subsamples. An accurate&#xD;
characterisation of the entropy graph is given where a local maximum of entropy takes place&#xD;
simultaneously with a local minimum  2 error. By working from different sampling parameters&#xD;
the method is applied to samples from HIPPARCOS and Geneva-Copenhagen survey&#xD;
(GCS) to obtain kinematic parameters and mixture proportions of thin disk, thick disk and&#xD;
halo. The sampling parameter P = |(U, V,W)|, absolute heliocentric velocity, allows to build&#xD;
an optimal subsample containing thin and thick disk stars, by leaving aside most of the halo&#xD;
population. The sampling parameter P = |W|, absolute perpendicular velocity, is able to&#xD;
build an optimal subsample containing a mixture of total disk and halo stars, although it&#xD;
does not allow an optimal segregation of thin and thick disks. Other sampling parameters&#xD;
like P = |(U,W)| or P = |V | are found to be less population informative. By comparing&#xD;
both samples, HIPPARCOS provides more accurate estimates for thick disk and halo, while&#xD;
GCS does for the total disk. In particular, the radial velocity dispersion of the halo fits&#xD;
perfectly into the empirical Titius-Bode like law  U = 6.6 ( 4&#xD;
3 )3n+2, which was previously proposed&#xD;
for discrete kinematic components, where the values n = 0, 1, 2, 3 stands for early-type&#xD;
stars, thin disk, thick disk, and halo populations. Population statistics are used to segregate&#xD;
thin disk, thick disk, and halo, and to obtain a more accurate bayesian estimation of the&#xD;
population fractions.</description>
    <dc:date>2010-03-23T11:10:08Z</dc:date>
  </item>
  <item rdf:about="http://hdl.handle.net/2117/6775">
    <title>Partition entropy and chi-squared error: the improved MEMPHIS algorithm - Part I</title>
    <link>http://hdl.handle.net/2117/6775</link>
    <description>Title: Partition entropy and chi-squared error: the improved MEMPHIS algorithm - Part I
Authors: Cubarsí Morera, Rafael; Alcobé López, Santiago
Abstract: The entropy of the population partition is studied as a function of &#xD;
the sampling parameter, so that within a particular interval of its graph,&#xD;
the  plateau region, it is possible to get&#xD;
a stable estimation of the mixture parameters.  The optimal estimation is associated with a local maximum of entropy. Alter&#xD;
natively,&#xD;
the $\chi^2$ error of the mixture approach may also be used to obtain an optimal segregation. The &#xD;
relationship between the fitting error and the population entropy has been&#xD;
analysed in detail. We have proved that, by using an appropriate sampling parameter, within a plateau region of the entropy&#xD;
 graph, &#xD;
a local entropy maximum takes place simultaneously with a local minimum of the $\chi^2$ error. &#xD;
Therefore, the combined statistical method provides the best approximation mixture, as well as the less informative partiti&#xD;
on, &#xD;
to estimate the kinematic parameters of populations.</description>
    <dc:date>2010-03-23T10:56:41Z</dc:date>
  </item>
  <item rdf:about="http://hdl.handle.net/2117/6773">
    <title>Structure of the velocity distribution of the Galactic disc: a maximum entropy statistical approach - Part I</title>
    <link>http://hdl.handle.net/2117/6773</link>
    <description>Title: Structure of the velocity distribution of the Galactic disc: a maximum entropy statistical approach - Part I
Authors: Cubarsí Morera, Rafael
Abstract: The maximum entropy approach is proposed to describe the local structures of the veloc-&#xD;
ity distribution, which are collected through its sample moments. The method is used with&#xD;
several samples from the HIPPARCOS and Geneva-Copenhagen survey catalogues. For the&#xD;
large-scale distribution, the phase density function may be obtained by fitting moments up&#xD;
to sixth order as a product of two exponential functions, one giving a background ellipsoidal&#xD;
shape of the distribution and the other accounting for the skewness and for the slight shift in&#xD;
the ellipsoidal isocontours in terms of the rotation velocity. The small-scale distribution can&#xD;
be deduced from truncated distributions, such as velocity-bounded samples with |V| ≤ 51&#xD;
km s−1, which contain a complex mixture of early-type and young disc stars. By fitting up&#xD;
to ten-order moments, the maximum entropy approach gives a realistic portrait of actual&#xD;
asymmetries, showing a clear bimodal pattern: (i) around the Hyades-Pleiades stream, with&#xD;
negative radial mean velocity and (ii) around the Sirius-UMa stream, with slightly positive&#xD;
radial mean velocity. The “U-anomaly” along the radial direction is estimated straightfor-&#xD;
wardly 30 − 35 km s−1 from the contour plots.</description>
    <dc:date>2010-03-23T10:45:48Z</dc:date>
  </item>
  <item rdf:about="http://hdl.handle.net/2117/6700">
    <title>Small-scale structure of the disc velocity distribution. A maximum entropy statistical approach - Part II</title>
    <link>http://hdl.handle.net/2117/6700</link>
    <description>Title: Small-scale structure of the disc velocity distribution. A maximum entropy statistical approach - Part II
Authors: Cubarsí Morera, Rafael
Abstract: Among metallicity, colour, and other star properties, the eccentricity of the star’s orbit&#xD;
behaves as a very good sampling parameter to find a more detailed structure for the disc&#xD;
velocity distribution, allowing distinctions between different eccentricity layers. For subsam-&#xD;
ples with eccentricities e &lt; 0.15, star velocities are approximately symmetrically distributed&#xD;
around the LSR in the radial direction, with a dearth of stars at the LSR. For e = 0.15,&#xD;
the core distribution of the thin disc is supported by two major stellar groups with opposite&#xD;
radial velocities. Several simulations confirm that such a double-peaked distribution comes&#xD;
from the lognormal distribution of the velocity amplitudes. For maximum eccentricity 0.3&#xD;
and maximum distance to the Galactic plane 0.5 kpc a representative thin disc sample is&#xD;
obtained. An explanation of the apparent vertex deviation of the disc from the swinging&#xD;
of those major kinematic groups around the LSR is possible, which predicts a continuously&#xD;
changing orientation of the disc’s pseudo ellipsoid.</description>
    <dc:date>2010-03-18T12:49:37Z</dc:date>
  </item>
  <item rdf:about="http://hdl.handle.net/2117/3046">
    <title>On the maximum entropy and the problem of moments: an application to stellar kinematics</title>
    <link>http://hdl.handle.net/2117/3046</link>
    <description>Title: On the maximum entropy and the problem of moments: an application to stellar kinematics
Authors: Cubarsí Morera, Rafael
Abstract: The maximum entropy approach is used to solve the classical moment problem of stellar kinematics. &#xD;
If an extended set of moments is available, the current  method  provides a&#xD;
linear estimation algorithm, which is given by a Gramian system of &#xD;
equations, that leads to a fast and suitable estimation of the velocity&#xD;
distribution. In particular, it can be used as an alternative approach for modelling&#xD;
multimodal distributions that can not be described through gaussian mixtures.</description>
    <dc:date>2009-08-24T09:04:26Z</dc:date>
  </item>
  <item rdf:about="http://hdl.handle.net/2117/1244">
    <title>Closure of the stellar hydrodynamic equations for Gaussian and ellipsoidal velocity distributions</title>
    <link>http://hdl.handle.net/2117/1244</link>
    <description>Title: Closure of the stellar hydrodynamic equations for Gaussian and ellipsoidal velocity distributions
Authors: Cubarsí Morera, Rafael
Abstract: The closure conditions, which make a finite set of moment equations&#xD;
equivalent to the collisionless Boltzmann equation, are investigated for&#xD;
Gaussian and ellipsoidal velocity distributions working from the com-&#xD;
plete mathematical expression for the nth-order stellar hydrodynamic&#xD;
equation, which was explicitly obtained depending on the comoving mo-&#xD;
ments in a previous paper. First, for a Schwarzschild distribution, it&#xD;
is proved that the whole set of hydrodynamic equations is reduced to&#xD;
the equations of orders n = 0,1,2,3, owing to the recurrent form of the&#xD;
central moments. Furthermore, the equations of order n = 2 and n = 3&#xD;
become closure conditions for higher even- and odd-order equations, re-&#xD;
spectively. An arbitrary quadratic function in the peculiar velocities, the&#xD;
generalised Schwarzschild distribution, is also investigated. Analogous&#xD;
closure conditions could be obtained from a similar recurrence law for&#xD;
central moments, but an alternative procedure is preferred, which con-&#xD;
sists in to expand a generalised ellipsoidal function as a power series of&#xD;
Schwarzschild distributions with the same mean. Then, due to the linear&#xD;
nature of the problem, the equivalence between the moment equations&#xD;
and the system of equations that Chandrasekhar had obtained working&#xD;
from the collisionless Boltzmann equation is borne out.</description>
    <dc:date>2007-10-11T18:30:08Z</dc:date>
  </item>
  <item rdf:about="http://hdl.handle.net/2117/1242">
    <title>The complete form of moment equations of stellar dynamics</title>
    <link>http://hdl.handle.net/2117/1242</link>
    <description>Title: The complete form of moment equations of stellar dynamics
Authors: Cubarsí Morera, Rafael
Abstract: The exact mathematical expression for an arbitrary nth-order stellar&#xD;
hydrodynamic equation is explicitly obtained depending on the central&#xD;
moments of the velocity distribution. In such a form the equations are&#xD;
physically meaningful, since they can be compared with the ordinary hy-&#xD;
drodynamic equations of compressible, viscous fluids. The equations are&#xD;
deduced without any particular assumptions about symmetries, steadi-&#xD;
ness, or particular kinematic behaviours, so that they can be used in&#xD;
their complete form, and for any order, in future works with improved&#xD;
observational data. Also, in order to work with a finite number of equa-&#xD;
tions and unknowns, which would provide a dynamic model for the stel-&#xD;
lar system, the nth-order equation is needed to investigate in a more&#xD;
general way the closure conditions, which may be expressed in terms of&#xD;
velocity distribution statistics, as it is shown in a case example.</description>
    <dc:date>2007-10-11T18:04:39Z</dc:date>
  </item>
  <item rdf:about="http://hdl.handle.net/2117/969">
    <title>Study of several interpolation schemes to provide ionospheric corrections for navigation</title>
    <link>http://hdl.handle.net/2117/969</link>
    <description>Title: Study of several interpolation schemes to provide ionospheric corrections for navigation
Authors: Orús Pérez, Raül; García Fernández, Miquel; Prats Menéndez, Xavier; Hernández Pajares, Manuel; Juan, Miguel
Abstract: Since the development of space based geodesic techniques, the increasing of the positioning accuracy has been a&#xD;
major goal. In this context, the effect of the ionosphere has been a key issue to be taken into account to improve&#xD;
the navigation results obtained using several types of receivers: from dual frequency phase receivers at distances&#xD;
greater than tens of kilometres of the nearest fixed site to single frequency code receivers.&#xD;
To overcome this problem, it is necessary either an accurate modelling of the ionosphere at the fixed stations and&#xD;
an optimum interpolation scheme for the rover receiver.&#xD;
This approach is either valid for single frequency users or rovers using dual frequency phase receiver. The current&#xD;
work studies the performance of different interpolation schemes such as linear interpolation and kriging, which can&#xD;
be implemented in a rover receiver in order to interpolate either the Slant Total Electron Content (from now on&#xD;
STEC) or the Double Differenced STEC from the transmitted corrections that are computed at the fixed&#xD;
stations.</description>
    <dc:date>2007-05-10T09:02:21Z</dc:date>
  </item>
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