15 research outputs found
On a subtle point of sum rules calculations: toy model
We consider a two-point correlator in massless model within the
ladder approximation . The spectral density of the correlator is known
explicitly and does not contain any resonances. Meanwhile making use of the
standard sum rules technique with a simple "resonance + continuum" model of the
spectrum allows to predict parameters of the "resonance" very accurately in the
sense that all necessary criteria of stability are perfectly satisfied.Comment: LaTeX fil
A lower limit on the dark particle mass from dSphs
We use dwarf spheroidal galaxies as a tool to attempt to put precise lower
limits on the mass of the dark matter particle, assuming it is a sterile
neutrino. We begin by making cored dark halo fits to the line of sight velocity
dispersions as a function of projected radius (taken from Walker et al. 2007)
for six of the Milky Way's dwarf spheroidal galaxies. We test Osipkov-Merritt
velocity anisotropy profiles, but find that no benefit is gained over constant
velocity anisotropy. In contrast to previous attempts, we do not assume any
relation between the stellar velocity dispersions and the dark matter ones, but
instead we solve directly for the sterile neutrino velocity dispersion at all
radii by using the equation of state for a partially degenerate neutrino gas
(which ensures hydrostatic equilibrium of the sterile neutrino halo). This
yields a 1:1 relation between the sterile neutrino density and velocity
dispersion, and therefore gives us an accurate estimate of the Tremaine-Gunn
limit at all radii. By varying the sterile neutrino particle mass, we locate
the minimum mass for all six dwarf spheroidals such that the Tremaine-Gunn
limit is not exceeded at any radius (in particular at the centre). We find
sizeable differences between the ranges of feasible sterile neutrino particle
mass for each dwarf, but interestingly there exists a small range 270-280eV
which is consistent with all dSphs at the 1- level.Comment: 13 pages, 2 figures, 1 tabl
IMPROVING THE ACCURACY DIGITAL ACQUISITION AND DEMODULATION OF OFDM SIGNALS WITH KNOWN PARAMETERS
ΠΠ°Π½ΠΎ ΠΊΡΠ°ΡΠΊΠΎΠ΅ ΠΎΠΏΠΈΡΠ°Π½ΠΈΠ΅ ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΠ΅ΠΉ OFDM ΡΠΈΠ³Π½Π°Π»ΠΎΠ², ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΡΡΠΈΡ
ΠΏΠ΅ΡΠ΅ΡΠ΅Π½Ρ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΡΡ
ΠΈΠ΄Π΅Π½ΡΠΈΡΠΈΠΊΠ°ΡΠΈΠΎΠ½Π½ΡΡ
ΠΏΡΠΈΠ·Π½Π°ΠΊΠΎΠ². Π£ΡΠΎΠ²Π΅ΡΡΠ΅Π½ΡΡΠ²ΠΎΠ²Π°Π½ ΠΊΠΎΡΡΠ΅Π»ΡΡΠΈΠΎΠ½Π½ΡΠΉ ΠΌΠ΅ΡΠΎΠ΄ ΠΎΡΠ΅Π½ΠΊΠΈ ΠΎΡΠ½ΠΎΠ²Π½ΡΡ
ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² ΡΠΈΠ³Π½Π°Π»ΠΎΠ², ΠΎΡΠ½ΠΎΠ²Π°Π½Π½ΡΠΉ Π½Π° ΡΠΈΠΊΠ»ΠΈΡΠ½ΠΎΠΉ ΠΏΡΠ΅ΡΠΈΠΊΡΠ½ΠΎΠΉ ΡΡΡΡΠΊΡΡΡΠ΅ ΡΠΈΠ³Π½Π°Π»Π°, Π·Π° ΡΡΠ΅Ρ ΠΏΡΠΈΠ²ΡΠ·ΠΊΠΈ Π½Π°ΡΠ°Π» ΠΈΠ½ΡΠ΅ΡΠ²Π°Π»ΠΎΠ² ΠΎΡΡΠΎΠ³ΠΎΠ½Π°Π»ΡΠ½ΠΎΡΡΠΈ ΠΊ ΡΡΠ°Π»ΠΎΠ½Π½ΠΎΠΉ ΡΠ΅ΡΠΊΠ΅ ΡΠ°ΡΡΠΎΡ. ΠΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΏΠΎΠΊΠ°Π·Π°Π½Π° Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΡ ΠΏΠΎΠΌΠ΅Ρ
ΠΎΡΡΡΠΎΠΉΡΠΈΠ²ΠΎΠΉ Π΄Π΅ΠΌΠΎΠ΄ΡΠ»ΡΡΠΈΠΈ ΡΠΈΠ³Π½Π°Π»ΠΎΠ² Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΡΠ΅ΡΠ΅Π½ΠΈΡ ΡΠΈΡΡΠ΅ΠΌ Π»ΠΈΠ½Π΅ΠΉΠ½ΡΡ
Π°Π»Π³Π΅Π±ΡΠ°ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΉ (Π‘ΠΠΠ£).ΠΠ°Π½ΠΎ ΠΊΠΎΡΠΎΡΠΊΠ΅ ΠΎΠΏΠΈΡΠ°Π½Π½Ρ ΠΎΡΠΎΠ±Π»ΠΈΠ²ΠΎΡΡΠ΅ΠΉ OFDM ΡΠΈΠ³Π½Π°Π»ΡΠ², ΡΠΊΡ Π²ΠΈΠ·Π½Π°ΡΠ°ΡΡΡ ΠΏΠ΅ΡΠ΅Π»ΡΠΊ ΠΌΠΎΠΆΠ»ΠΈΠ²ΠΈΡ
ΡΠ΄Π΅Π½ΡΠΈΡΡΠΊΠ°ΡΡΠΉΠ½ΠΈΡ
ΠΎΠ·Π½Π°ΠΊ. Π£Π΄ΠΎΡΠΊΠΎΠ½Π°Π»Π΅Π½ΠΎ ΠΊΠΎΡΠ΅Π»ΡΡΡΠΉΠ½ΠΈΠΉ ΠΌΠ΅ΡΠΎΠ΄ ΠΎΡΡΠ½ΠΊΠΈ ΠΎΡΠ½ΠΎΠ²Π½ΠΈΡ
ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΡΠ² ΡΠΈΠ³Π½Π°Π»ΡΠ², Π·Π°ΡΠ½ΠΎΠ²Π°Π½ΠΈΠΉ Π½Π° ΡΠΈΠΊΠ»ΡΡΠ½ΡΠΉ ΠΏΡΠ΅ΡΡΠΊΡΠ½ΡΠΉ ΡΡΡΡΠΊΡΡΡΡ ΡΠΈΠ³Π½Π°Π»Ρ, Π·Π° ΡΠ°Ρ
ΡΠ½ΠΎΠΊ ΠΏΡΠΈΠ²βΡΠ·ΠΊΠΈ Π½Π°ΡΠ°Π» ΡΠ½ΡΠ΅ΡΠ²Π°Π»ΡΠ² ΠΎΡΡΠΎΠ³ΠΎΠ½Π°Π»ΡΠ½ΠΎΡΡΡ Π΄ΠΎ Π΅ΡΠ°Π»ΠΎΠ½Π½ΠΎΡ ΡΡΡΠΊΠΈ ΡΠ°ΡΡΠΎΡ. ΠΠΎΠ΄Π΅Π»ΡΠ²Π°Π½Π½ΡΠΌ ΠΏΠΎΠΊΠ°Π·Π°Π½Π° ΠΌΠΎΠΆΠ»ΠΈΠ²ΡΡΡΡ Π·Π°Π²Π°Π΄ΠΎΡΡΡΠΉΠΊΠΎΡ Π΄Π΅ΠΌΠΎΠ΄ΡΠ»ΡΡΡΡ ΡΠΈΠ³Π½Π°Π»ΡΠ² ΡΠ»ΡΡ
ΠΎΠΌ ΡΡΡΠ΅Π½Π½Ρ ΡΠΈΡΡΠ΅ΠΌ Π»ΡΠ½ΡΠΉΠ½ΠΈΡ
Π°Π»Π³Π΅Π±ΡΠ°ΡΡΠ½ΠΈΡ
ΡΡΠ²Π½ΡΠ½Ρ (Π‘ΠΠΠ ).A brief description of the features of OFDM signals, determine a list of possible signs of identity. Improved correlation method for estimating key parameters pas signals, based on the cyclic prefix signal structure by binding began intervals orthogonal to the reference frequency grid. The simulation showed possibility of interference-signal demodulation based on solving systems of linear algebra equations (SLAE)
A DIGITAL CROSS-CORRELATION METHOD OF ANALYSIS OF PARAMETERS OF OFDM SIGNALS IS IN THE SYSTEMS OF THE AUTOMATIC RADIO MONITORING
ΠΠ°Π½ΠΎ ΠΊΡΠ°ΡΠΊΠΎΠ΅ ΠΎΠΏΠΈΡΠ°Π½ΠΈΠ΅ ΡΠ°ΡΡΠΎΡΠ½ΠΎ-Π²ΡΠ΅ΠΌΠ΅Π½Π½ΡΡ
ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΠ΅ΠΉ OFDM ΡΠΈΠ³Π½Π°Π»ΠΎΠ², ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΡΡΠΈΡ
ΠΏΠ΅ΡΠ΅ΡΠ΅Π½Ρ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΡΡ
ΠΈΠ΄Π΅Π½ΡΠΈΡΠΈΠΊΠ°ΡΠΈΠΎΠ½Π½ΡΡ
ΠΏΡΠΈΠ·Π½Π°ΠΊΠΎΠ². ΠΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½ ΠΊΠΎΡΡΠ΅Π»ΡΡΠΈΠΎΠ½Π½ΡΠΉ ΠΌΠ΅ΡΠΎΠ΄ ΠΎΡΠ΅Π½ΠΊΠΈ ΠΎΡΠ½ΠΎΠ²Π½ΡΡ
ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² ΡΠ»ΠΎΠΆΠ½ΡΡ
ΡΠΈΠ³Π½Π°Π»ΠΎΠ² Π² ΡΡΠ»ΠΎΠ²ΠΈΡΡ
Π°ΠΏΡΠΈΠΎΡΠ½ΠΎΠΉ Π½Π΅ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½Π½ΠΎΡΡΠΈ, ΠΎΡΠ½ΠΎΠ²Π°Π½Π½ΡΠΉ Π½Π° ΡΠΈΠΊΠ»ΠΈΡΠ½ΠΎΠΉ ΠΏΡΠ΅ΡΠΈΠΊΡΠ½ΠΎΠΉ ΡΡΡΡΠΊΡΡΡΠ΅ ΠΊΠΎΠΌΠ±ΠΈΠ½ΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΡΠΈΠ³Π½Π°Π»Π° Π² ΠΏΡΠ΅Π΄Π΅Π»Π°Ρ
ΠΈΠ½ΡΠ΅ΡΠ²Π°Π»Π° ΠΌΠΎΠ΄ΡΠ»ΡΡΠΈΠΈ ΠΈ ΠΎΡΡΡΠ΅ΡΡΠ²Π»ΡΠ΅ΠΌΡΠΉ ΠΏΠΎ Π΄Π°Π½Π½ΡΠΌ ΡΠΈΡΡΠΎΠ²ΡΡ
Π²ΡΠ±ΠΎΡΠΎΠΊ ΠΌΠΈΠ½ΠΈΠΌΠ°Π»ΡΠ½ΠΎΠ³ΠΎ ΠΊΠ°ΡΠ΅ΡΡΠ²Π°. ΠΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½Ρ ΡΡΠ°ΠΏΡ ΠΎΠ±ΡΠ°Π±ΠΎΡΠΊΠΈ ΠΈ ΠΏΡΡΠΈ ΠΈΡ
ΡΠ΅Π°Π»ΠΈΠ·Π°ΡΠΈΠΈ. ΠΠΎΠΊΠ°Π·Π°Π½Ρ ΠΏΡΠ΅ΠΈΠΌΡΡΠ΅ΡΡΠ²Π° ΠΏΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½Π½ΠΎΠ³ΠΎ ΠΌΠ΅ΡΠΎΠ΄Π° ΠΏΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Ρ ΡΡΠ°Π΄ΠΈΡΠΈΠΎΠ½Π½ΡΠΌΠΈ ΠΌΠ΅ΡΠΎΠ΄Π°ΠΌΠΈ ΡΠΏΠ΅ΠΊΡΡΠ°Π»ΡΠ½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π° ΡΡΡΡΠΊΡΡΡΡ ΡΠΈΠ³Π½Π°Π»ΠΎΠ².ΠΠ°Π΄Π°Π½ΠΈΠΉ ΠΊΠΎΡΠΎΡΠΊΠΈΠΉ ΠΎΠΏΠΈΡ ΡΠ°ΡΡΠΎΡΠ½ΠΎ-ΡΠ°ΡΠΎΠ²ΠΈΡ
ΠΎΡΠΎΠ±Π»ΠΈΠ²ΠΎΡΡΠ΅ΠΉ OFDM ΡΠΈΠ³Π½Π°Π»ΡΠ², ΡΠΊΡΠΉ Π΄ΠΎΠ·Π²ΠΎΠ»ΡΡ Π²ΠΈΠ·Π½Π°ΡΠΈΡΠΈ ΠΏΠ΅ΡΠ΅Π»ΡΠΊ ΠΌΠΎΠΆΠ»ΠΈΠ²ΠΈΡ
ΡΠ΄Π΅Π½ΡΠΈΡΡΠΊΠ°ΡΡΠΉΠ½ΠΈΡ
ΠΎΠ·Π½Π°ΠΊ. ΠΠ°ΠΏΡΠΎΠΏΠΎΠ½ΠΎΠ²Π°Π½ΠΈΠΉ ΠΊΠΎΡΠ΅Π»ΡΡΡΠΉΠ½ΠΈΠΉ ΠΌΠ΅ΡΠΎΠ΄ ΠΎΡΡΠ½ΠΊΠΈ ΠΎΡΠ½ΠΎΠ²Π½ΠΈΡ
ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΡΠ² ΡΠΊΠ»Π°Π΄Π½ΠΈΡ
ΡΠΈΠ³Π½Π°Π»ΡΠ² Π² ΡΠΌΠΎΠ²Π°Ρ
Π°ΠΏΡΡΠΎΡΠ½ΠΎΡ Π½Π΅Π²ΠΈΠ·Π½Π°ΡΠ΅Π½ΠΎΡΡΡ, Π·Π°ΡΠ½ΠΎΠ²Π°Π½ΠΈΠΉ Π½Π° ΡΠΈΠΊΠ»ΡΡΠ½ΡΠΉ ΠΏΡΠ΅ΡΡΠΊΡΠ½ΡΠΉ ΡΡΡΡΠΊΡΡΡΡ ΠΊΠΎΠΌΠ±ΡΠ½ΠΎΠ²Π°Π½ΠΎΠ³ΠΎ ΡΠΈΠ³Π½Π°Π»Ρ Π² ΠΌΠ΅ΠΆΠ°Ρ
ΡΠ½ΡΠ΅ΡΠ²Π°Π»Ρ ΠΌΠΎΠ΄ΡΠ»ΡΡΡΡ, ΡΠΊΡΠΉ Π·Π΄ΡΠΉΡΠ½ΡΡΡΡΡΡ Π·Π° Π΄Π°Π½ΠΈΠΌΠΈ ΡΠΈΡΡΠΎΠ²ΠΈΡ
Π²ΠΈΠ±ΡΡΠΎΠΊ ΠΌΡΠ½ΡΠΌΠ°Π»ΡΠ½ΠΎΡ ΡΠΊΠΎΡΡΡ. ΠΠ»Ρ Π²ΠΈΠ·Π½Π°ΡΠ΅Π½Π½Ρ ΡΠΏΠΈΡΠΊΡ ΡΠΎΠ±ΠΎΡΠΈΡ
ΠΎΡΡΠΎΠ³ΠΎΠ½Π°Π»ΡΠ½ΠΈΡ
ΡΠ°ΡΡΠΎΡ Π·Π°ΠΏΡΠΎΠΏΠΎΠ½ΠΎΠ²Π°Π½ΠΈΠΉ ΠΌΠ΅ΡΠΎΠ΄ Π»ΡΠ½ΡΠΉΠ½ΠΎΡ Π°Π»Π³Π΅Π±ΡΠΈ, ΡΠΎ Π·Π°Π±Π΅Π·ΠΏΠ΅ΡΡΡ ΠΏΡΠ΄Π²ΠΈΡΠ΅Π½Ρ ΡΠΎΡΠ½ΡΡΡΡ ΠΎΡΡΠ½ΠΎΠΊ ΠΏΡΠΈ ΠΌΡΠ½ΡΠΌΡΠΌΡ ΠΎΠ±ΡΠΈΡΠ»ΡΠ²Π°Π»ΡΠ½ΠΈΡ
Π²ΠΈΡΡΠ°Ρ. ΠΠΎΠΊΠ°Π·Π°Π½Ρ ΠΏΠ΅ΡΠ΅Π²Π°Π³ΠΈ Π·Π°ΠΏΡΠΎΠΏΠΎΠ½ΠΎΠ²Π°Π½ΠΎΠ³ΠΎ ΠΌΠ΅ΡΠΎΠ΄Ρ Π² ΠΏΠΎΡΡΠ²Π½ΡΠ½Π½Ρ Π· ΡΡΠ°Π΄ΠΈΡΡΠΉΠ½ΠΈΠΌΠΈ ΠΌΠ΅ΡΠΎΠ΄Π°ΠΌΠΈ ΡΠΏΠ΅ΠΊΡΡΠ°Π»ΡΠ½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΡΠ·Ρ ΡΡΡΡΠΊΡΡΡΠΈ ΡΠΈΠ³Π½Π°Π»ΡΠ².Short description of frequency-temporal features of OFDM of signals, determining the list of possible identification signs is given. The cross-correlation method of estimation of basic parameters of difficult signals is offered in the conditions of a priori vagueness, based on the cyclic prefix structure of the combined signal within the limits of interval of mo dulation and carried out from data of digital selections of minimum quality. For determination of list of workings orthogonal sub bearings frequencies the method of linear algebra, providing enhanceable exactness of estimations at a min imum of calculable expenses, is offered. Advantages of the offered method are rotined as compared to the traditional methods of spectral structure of signals
"Non-cold" dark matter at small scales: A general approach
Structure formation at small cosmological scales provides an important frontier for dark matter (DM) research. Scenarios with small DM particle masses, large momenta or hidden interactions tend to suppress the gravitational clustering at small scales. The details of this suppression depend on the DM particle nature, allowing for a direct link between DM models and astrophysical observations. However, most of the astrophysical constraints obtained so far refer to a very specific shape of the power suppression, corresponding to thermal warm dark matter (WDM), i.e., candidates with a Fermi-Dirac or Bose-Einstein momentum distribution. In this work we introduce a new analytical fitting formula for the power spectrum, which is simple yet flexible enough to reproduce the clustering signal of large classes of non-thermal DM models, which are not at all adequately described by the oversimplified notion of WDM . We show that the formula is able to fully cover the parameter space of sterile neutrinos (whether resonantly produced or from particle decay), mixed cold and warm models, fuzzy dark matter, as well as other models suggested by effective theory of structure formation (ETHOS). Based on this fitting formula, we perform a large suite of N-body simulations and we extract important nonlinear statistics, such as the matter power spectrum and the halo mass function. Finally, we present first preliminary astrophysical constraints, based on linear theory, from both the number of Milky Way satellites and the Lyman-\uce\ub1 forest. This paper is a first step towards a general and comprehensive modeling of small-scale departures from the standard cold DM model