10,068 research outputs found
Identity and identification of Trogulus banaticus (Opiliones: Trogulidae) : a neglected species in the Northern Balkans
Trogulus banaticus Avram, 1971 is characterised and recorded as new for Slovenia. This species was previously mistaken for T. coriziformis C. L. Koch, 1839 and T. graecus Dahl, 1903 which were later rejected from the Slovenian fauna. T. banaticus is compared with the similar, and partly sympatric, T. tingiformis C. L. Koch, 1847 with which it has often been confused. A table of distinguishing characters for both species is provided, and the ecology of T. banaticus and its general distribution are discussed
Comparing one and two class classification methods for multiple fault detection on an induction motor
Core-Cusp revisited and Dark Matter Phase Transition Constrained at O(0.1) eV with LSB Rotation Curve
Recently a new particle physics model called Bound Dark Matter (BDM) has been
proposed in which dark matter (DM) particles are massless above a threshold
energy (Ec) and acquire mass below it due to nonperturbative methods.
Therefore, the BDM model describes DM particles which are relativistic, hot
dark matter, in the inner regions of galaxies and describes nonrelativistic,
cold dark matter, where halo density is below rho_c = Ec^4. To realize this
idea in galaxies we use a particular DM cored profile that contains three
parameters: a scale length (rs) and density (rho_0) of the halo, and a core
radius (rc) stemming from the relativistic nature of the BDM model. We test
this model by fitting rotation curves of seventeen Low Surface Brightness
galaxies from The HI Nearby Galaxy Survey (THINGS). Since the energy Ec
parameterizes the phase transition due to the underlying particle physics
model, it is independent on the details of galaxy or structure formation and
therefore the DM profile parameters rs, rc, Ec are constrained, leaving only
two free parameters. The high spatial and velocity resolution of this sample
allows to derive the model parameters through the numerical implementation of
the chi^2-goodness-of-fit test to the mass models. We compare the fittings with
those of Navarro-Frenk-White (NFW), Burkert, and Pseudo-Isothermal (ISO)
profiles. Through the results we conclude that the BDM profile fits better, or
equally well, than NFW, Burkert, and ISO profiles and agree with previous
results implying that cored profiles are preferred over the N-body motivated
cuspy profile. We also compute 2D likelihoods of the BDM parameters rc and Ec
for the different galaxies and matter contents, and find an average galaxy core
radius rc=300 pc and a transition energy Ec = 0.11 eV when the DM halo is the
only component. In Kroupa mass model, we obtain a core rc=1.48 kpc, and energy
Ec=0.06 eV.Comment: 54 pages, 26 Figures. Submitted to Phys. Rev. D. Refer also to
Phys.Rev.D84:121301,201
Sequential Implementation of Monte Carlo Tests with Uniformly Bounded Resampling Risk
This paper introduces an open-ended sequential algorithm for computing the
p-value of a test using Monte Carlo simulation. It guarantees that the
resampling risk, the probability of a different decision than the one based on
the theoretical p-value, is uniformly bounded by an arbitrarily small constant.
Previously suggested sequential or non-sequential algorithms, using a bounded
sample size, do not have this property. Although the algorithm is open-ended,
the expected number of steps is finite, except when the p-value is on the
threshold between rejecting and not rejecting. The algorithm is suitable as
standard for implementing tests that require (re-)sampling. It can also be used
in other situations: to check whether a test is conservative, iteratively to
implement double bootstrap tests, and to determine the sample size required for
a certain power.Comment: Major Revision 15 pages, 4 figure
Hysteresis between distinct modes of turbulent dynamos
Nonlinear mean-field models of the solar dynamo show long-term variability,
which may be relevant to different states of activity inferred from long-term
radiocarbon data. This paper is aimed to probe the dynamo hysteresis predicted
by the recent mean-field models of Kitchatinov \& Olemskoy (2010) with direct
numerical simulations. We perform three-dimensional simulations of large-scale
dynamos in a shearing box with helically forced turbulence. As initial
condition, we either take a weak random magnetic field or we start from a
snapshot of an earlier simulation. Two quasi-stable states are found to coexist
in a certain range of parameters close to the onset of the large-scale dynamo.
The simulations converge to one of these states depending on the initial
conditions. When either the fractional helicity or the magnetic Prandtl number
is increased between successive runs above the critical value for onset of the
dynamo, the field strength jumps to a finite value. However, when the
fractional helicity or the magnetic Prandtl number is then decreased again, the
field strength stays at a similar value (strong field branch) even below the
original onset. We also observe intermittent decaying phases away from the
strong field branch close to the point where large-scale dynamo action is just
possible. The dynamo hysteresis seen previously in mean-field models is thus
reproduced by 3D simulations. Its possible relation to distinct modes of solar
activity such as grand minima is discussed.Comment: Published in Ap
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