1,873 research outputs found
ΠΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΠΏΠΎΠ»Π΅ΠΉ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ ΠΏΠ»ΠΎΡΠΊΠΎΠ³ΠΎ Π°Π½ΠΈΠ·ΠΎΡΡΠΎΠΏΠ½ΠΎ ΡΠ°ΡΡΠ΅ΠΈΠ²Π°ΡΡΠ΅Π³ΠΎ ΠΎΠ΄Π½ΠΎΡΠΎΠ΄Π½ΠΎΠ³ΠΎ ΡΠ»ΠΎΡ ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ»ΡΠ½ΠΎΠΉ ΠΎΠΏΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠΎΠ»ΡΠΈΠ½Ρ
Modeling of radiation fields of an arbitrary optical thickness uniform slab in the case of a weak absorption and strongly elongated phase functions has been carried. The simple modification of classical Ambarzumianβs β Chandrasekharβs invariance principle indispensable for the receiving of new non-linear integral equations connected with azimuthal Fourier harmonics of generalized unified photometric function and photometric invariants has been used. These values join upgoing and downgoing radiation fields intensities making use of simple linear manner at arbitrary optical levels in mirror vision directions including fixed azimuthal angles and solar zenith distance. Parametrizations of obtained non-linear integral equations have demonstrated in the absence of reflecting underlying surfaces, placed at the lowest level of considered uniform slab, the possibility to express angular-spatial properties of unified photometrical function and appropriate photometrical invariants taking into account the phase functions strongly elongation near small scattering angles and small slabβs absorption with the help of primary scattered radiation field intensities and adaptive fitting multipliers. These functional adaptive corrections have been stipulated by uniform slabβs multiple light scattering and possess the clear physical interpretation. The use of mirror reflection (symmetry) principle, elaborated by the author, and conception of unified photometric function allows one to estimate the above-mentioned peculiarities of real environmentβs phase functions in the framework of photometric invariants numerical modeling. An analysis of appropriate radiative modeling results has shown a dominating influence of primary light scattering in the formation of anisotropically scattered radiation fields of an arbitrary optical thickness uniform slab in the case of weak radiation absorption and strongly elongated phase functions.ΠΡΠΎΠ²Π΅Π΄Π΅Π½ΠΎ ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΠΏΠΎΠ»Π΅ΠΉ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ ΠΏΠ»ΠΎΡΠΊΠΎΠ³ΠΎ ΠΎΠ΄Π½ΠΎΡΠΎΠ΄Π½ΠΎΠ³ΠΎ ΡΠ»ΠΎΡ ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ»ΡΠ½ΠΎΠΉ ΠΎΠΏΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠΎΠ»ΡΠΈΠ½Ρ ΠΏΡΠΈ ΡΠΈΠ»ΡΠ½ΠΎ Π²ΡΡΡΠ½ΡΡΡΡ
ΠΈΠ½Π΄ΠΈΠΊΠ°ΡΡΠΈΡΠ°Ρ
ΡΠ°ΡΡΠ΅ΡΠ½ΠΈΡ. ΠΠ»Ρ ΡΠ΅Π°Π»ΠΈΠ·Π°ΡΠΈΠΈ ΡΡΠΎΠΉ Π·Π°Π΄Π°ΡΠΈ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π»Π°ΡΡ ΠΌΠΎΠ΄ΠΈΡΠΈΠΊΠ°ΡΠΈΡ ΠΊΠ»Π°ΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΏΡΠΈΠ½ΡΠΈΠΏΠ° ΠΈΠ½Π²Π°ΡΠΈΠ°Π½ΡΠ½ΠΎΡΡΠΈ ΠΠΌΠ±Π°ΡΡΡΠΌΡΠ½Π° β Π§Π°Π½Π΄ΡΠ°ΡΠ΅ΠΊΠ°ΡΠ°, ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΠ²ΡΠ°Ρ ΠΏΠΎΠ»ΡΡΠΈΡΡ Π½ΠΎΠ²ΡΠ΅ Π½Π΅Π»ΠΈΠ½Π΅ΠΉΠ½ΡΠ΅ ΠΈΠ½ΡΠ΅Π³ΡΠ°Π»ΡΠ½ΡΠ΅ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Π΄Π»Ρ Π°Π·ΠΈΠΌΡΡΠ°Π»ΡΠ½ΡΡ
Π€ΡΡΡΠ΅-Π³Π°ΡΠΌΠΎΠ½ΠΈΠΊ ΠΎΠ±ΠΎΠ±ΡΠ΅Π½Π½ΠΎΠΉ Π΅Π΄ΠΈΠ½ΠΎΠΉ ΡΠΎΡΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΡΠ½ΠΊΡΠΈΠΈ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ ΠΈ ΡΠΎΡΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈΠ½Π²Π°ΡΠΈΠ°Π½ΡΠΎΠ², ΠΊΠΎΡΠΎΡΡΠ΅ ΠΎΠ±ΡΠ΅Π΄ΠΈΠ½ΡΡΡ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΠΈ Π²ΠΎΡΡ
ΠΎΠ΄ΡΡΠ΅Π³ΠΎ ΠΈ Π½ΠΈΡΡ
ΠΎΠ΄ΡΡΠ΅Π³ΠΎ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ Π½Π° ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ»ΡΠ½ΡΡ
Π·Π΅ΡΠΊΠ°Π»ΡΠ½ΠΎ-ΡΠΈΠΌΠΌΠ΅ΡΡΠΈΡΠ½ΡΡ
ΠΎΠΏΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΡΠΎΠ²Π½ΡΡ
Π² Π·Π΅ΡΠΊΠ°Π»ΡΠ½ΡΡ
Π½Π°ΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡΡ
Π²ΠΈΠ·ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΏΡΠΈ ΡΠΈΠΊΡΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
Π°Π·ΠΈΠΌΡΡΠ°Ρ
ΠΈ Π·Π΅Π½ΠΈΡΠ½ΡΡ
ΡΠ°ΡΡΡΠΎΡΠ½ΠΈΡΡ
Π‘ΠΎΠ»Π½ΡΠ°. ΠΠ°ΡΠ°ΠΌΠ΅ΡΡΠΈΠ·Π°ΡΠΈΡ ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
Π½Π΅Π»ΠΈΠ½Π΅ΠΉΠ½ΡΡ
ΠΈΠ½ΡΠ΅Π³ΡΠ°Π»ΡΠ½ΡΡ
ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΉ ΠΏΠΎΠΊΠ°Π·Π°Π»Π°, ΡΡΠΎ ΠΏΡΠΈ ΠΎΡΡΡΡΡΡΠ²ΠΈΠΈ ΠΎΡΡΠ°ΠΆΠ°ΡΡΠ΅ΠΉ ΠΏΠΎΠ΄ΡΡΠΈΠ»Π°ΡΡΠ΅ΠΉ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ Π½Π° ΡΡΠΎΠ²Π½Π΅ Π½ΠΈΠΆΠ½Π΅ΠΉ Π³ΡΠ°Π½ΠΈΡΡ ΡΠ»ΠΎΡ ΠΏΡΠΎΡΡΡΠ°Π½ΡΡΠ²Π΅Π½Π½ΠΎ-ΡΠ³Π»ΠΎΠ²ΡΠ΅ ΡΠ²ΠΎΠΉΡΡΠ²Π° ΡΠΎΡΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈΠ½Π²Π°ΡΠΈΠ°Π½ΡΠΎΠ² ΠΈ Π΅Π΄ΠΈΠ½ΠΎΠΉ ΡΠΎΡΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΡΠ½ΠΊΡΠΈΠΈ Π² ΡΠ»ΡΡΠ°Π΅ ΡΠΈΠ»ΡΠ½ΠΎ Π²ΡΡΡΠ½ΡΡΡΡ
ΠΈΠ½Π΄ΠΈΠΊΠ°ΡΡΠΈΡ ΡΠ°ΡΡΠ΅ΡΠ½ΠΈΡ Ρ ΠΌΠ°ΠΊΡΠΈΠΌΠ°Π»ΡΠ½ΡΠΌΠΈ Π·Π½Π°ΡΠ΅Π½ΠΈΡΠΌΠΈ Π²Π±Π»ΠΈΠ·ΠΈ ΠΌΠ°Π»ΡΡ
ΡΠ³Π»ΠΎΠ² ΡΠ°ΡΡΠ΅ΡΠ½ΠΈΡ ΠΏΡΠΈ ΠΌΠ°Π»ΠΎΠΌ ΠΈΡΡΠΈΠ½Π½ΠΎΠΌ ΠΏΠΎΠ³Π»ΠΎΡΠ΅Π½ΠΈΠΈ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ Π² ΡΡΠ΅Π΄Π΅ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡΡ ΠΏΡΠΈΠ±Π»ΠΈΠΆΠ΅Π½Π½ΠΎ ΠΏΡΠ΅Π΄ΡΡΠ°Π²ΠΈΡΡ ΠΎΠ±ΡΠ΅Π΅ ΠΏΠΎΠ»Π΅ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ Π² Π²ΠΈΠ΄Π΅ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΠ΅ΠΉ ΠΎΠ΄Π½ΠΎΠΊΡΠ°ΡΠ½ΠΎ ΡΠ°ΡΡΠ΅ΡΠ½Π½ΠΎΠ³ΠΎ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ Ρ Π°Π΄Π°ΠΏΡΠΈΠ²Π½ΡΠΌΠΈ ΠΏΠΎΠΏΡΠ°Π²ΠΎΡΠ½ΡΠΌΠΈ ΠΌΠ½ΠΎΠΆΠΈΡΠ΅Π»ΡΠΌΠΈ. ΠΡΠΈ ΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΠ΅ ΠΏΠΎΠΏΡΠ°Π²ΠΊΠΈ ΠΎΠ±ΡΡΠ»ΠΎΠ²Π»Π΅Π½Ρ ΠΌΠ½ΠΎΠ³ΠΎΠΊΡΠ°ΡΠ½ΡΠΌ ΡΠ°ΡΡΠ΅ΡΠ½ΠΈΠ΅ΠΌ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ ΠΈ ΠΈΠΌΠ΅ΡΡ ΡΠ΅ΡΠΊΠΎΠ΅ ΡΠΈΠ·ΠΈΡΠ΅ΡΠΊΠΎΠ΅ ΠΎΠ±ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΈΠ΅. ΠΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΏΡΠΈΠ½ΡΠΈΠΏΠ° Π·Π΅ΡΠΊΠ°Π»ΡΠ½ΠΎΠ³ΠΎ ΠΎΡΠΎΠ±ΡΠ°ΠΆΠ΅Π½ΠΈΡ (ΡΠΈΠΌΠΌΠ΅ΡΡΠΈΠΈ) ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΠ»ΠΎ ΡΡΠ΅ΡΡΡ ΡΠΊΠ°Π·Π°Π½Π½ΡΠ΅ ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΠΈ ΡΠ΅Π°Π»ΡΠ½ΡΡ
ΠΈΠ½Π΄ΠΈΠΊΠ°ΡΡΠΈΡ ΡΠ°ΡΡΠ΅ΡΠ½ΠΈΡ ΠΏΡΠΈ ΡΠΈΡΠ»Π΅Π½Π½ΠΎΠΌ ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΠΈ ΡΠΎΡΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈΠ½Π²Π°ΡΠΈΠ°Π½ΡΠΎΠ² ΠΈ Π΅Π΄ΠΈΠ½ΠΎΠΉ ΡΠΎΡΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΡΠ½ΠΊΡΠΈΠΈ. ΠΡΠΎΠ²Π΅Π΄Π΅Π½Π½ΡΠΉ Π°Π½Π°Π»ΠΈΠ· ΠΏΠΎΠΊΠ°Π·Π°Π» Π΄ΠΎΠΌΠΈΠ½ΠΈΡΡΡΡΡΡ ΡΠΎΠ»Ρ ΠΎΠ΄Π½ΠΎΠΊΡΠ°ΡΠ½ΠΎΠ³ΠΎ ΡΠ°ΡΡΠ΅ΡΠ½ΠΈΡ ΠΏΡΠΈ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΠΈ ΠΏΠΎΠ»Π΅ΠΉ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ Π°Π½ΠΈΠ·ΠΎΡΡΠΎΠΏΠ½ΠΎ ΡΠ°ΡΡΠ΅ΠΈΠ²Π°ΡΡΠ΅Π³ΠΎ ΠΎΠ΄Π½ΠΎΡΠΎΠ΄Π½ΠΎΠ³ΠΎ ΡΠ»ΠΎΡ Π² ΡΠ»ΡΡΠ°Π΅ ΡΠ»Π°Π±ΠΎΠ³ΠΎ ΠΏΠΎΠ³Π»ΠΎΡΠ΅Π½ΠΈΡ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ ΠΏΡΠΈ ΡΠΈΠ»ΡΠ½ΠΎ Π²ΡΡΡΠ½ΡΡΡΡ
ΠΈΠ½Π΄ΠΈΠΊΠ°ΡΡΠΈΡΠ°Ρ
ΡΠ°ΡΡΠ΅ΡΠ½ΠΈΡ
Statistical Description of a Magnetized Corona above a Turbulent Accretion Disk
We present a physics-based statistical theory of a force-free magnetic field
in the corona above a turbulent accretion disk. The field is represented by a
statistical ensemble of loops tied to the disk. Each loop evolves under several
physical processes: Keplerian shear, turbulent random walk of the disk
footpoints, and reconnection with other loops. To build a statistical
description, we introduce the distribution function of loops over their sizes
and construct a kinetic equation that governs its evolution. This loop kinetic
equation is formally analogous to Boltzmann's kinetic equation, with loop-loop
reconnection described by a binary collision integral. A dimensionless
parameter is introduced to scale the (unknown) overall rate of reconnection
relative to Keplerian shear. After solving for the loop distribution function
numerically, we calculate self-consistently the distribution of the mean
magnetic pressure and dissipation rate with height, and the equilibrium shapes
of loops of different sizes. We also compute the energy and torque associated
with a given loop, as well as the total magnetic energy and torque in the
corona. We explore the dependence of these quantities on the reconnection
parameter and find that they can be greatly enhanced if reconnection between
loops is suppressed.Comment: 22 pages, 15 figures. Submitted to the Astrophysical Journa
Gravitating discs around black holes
Fluid discs and tori around black holes are discussed within different
approaches and with the emphasis on the role of disc gravity. First reviewed
are the prospects of investigating the gravitational field of a black
hole--disc system by analytical solutions of stationary, axially symmetric
Einstein's equations. Then, more detailed considerations are focused to middle
and outer parts of extended disc-like configurations where relativistic effects
are small and the Newtonian description is adequate.
Within general relativity, only a static case has been analysed in detail.
Results are often very inspiring, however, simplifying assumptions must be
imposed: ad hoc profiles of the disc density are commonly assumed and the
effects of frame-dragging and completely lacking. Astrophysical discs (e.g.
accretion discs in active galactic nuclei) typically extend far beyond the
relativistic domain and are fairly diluted. However, self-gravity is still
essential for their structure and evolution, as well as for their radiation
emission and the impact on the environment around. For example, a nuclear star
cluster in a galactic centre may bear various imprints of mutual star--disc
interactions, which can be recognised in observational properties, such as the
relation between the central mass and stellar velocity dispersion.Comment: Accepted for publication in CQG; high-resolution figures will be
available from http://www.iop.org/EJ/journal/CQ
Π§ΠΈΡΠ»Π΅Π½Π½ΠΎΠ΅ ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠΎΠ² ΡΡΠΊΠΎΡΡΠΈ ΠΏΠ»ΠΎΡΠΊΠΎΠ³ΠΎ ΠΎΠ΄Π½ΠΎΡΠΎΠ΄Π½ΠΎΠ³ΠΎ ΡΠ»ΠΎΡ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΏΡΠΈΠ½ΡΠΈΠΏΠ° Π·Π΅ΡΠΊΠ°Π»ΡΠ½ΠΎΠ³ΠΎ ΠΎΡΠΎΠ±ΡΠ°ΠΆΠ΅Π½ΠΈΡ ΠΈ ΡΠ΅ΡΠ΅Π½ΠΈΠΉ Π»ΠΈΠ½Π΅ΠΉΠ½ΡΡ ΡΠΈΠ½Π³ΡΠ»ΡΡΠ½ΡΡ ΠΈΠ½ΡΠ΅Π³ΡΠ°Π»ΡΠ½ΡΡ ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΉ
Based on the mirror reflection principle and solutions of modified linear singular integral equations, the numerical modeling of the unified exit function of the outside radiation field and photometrical invariants of brightness coefficients for a uniform slab of finite optical thickness has been carried out. The efficacy of applying the angular discretization method for problems of numerical modeling of outer radiation fields in the Β«atmosphere β underlying surfaceΒ» system has been proved. This new approach allows generalizing the basic results in the particular case of a semi-infinite uniform slab. In this connection the main mathematical aspects and computational peculiarity of the numerical realization of the angular discretization method have been considered. Due to linearity of the used basic integral equations, the conducted analysis can be generalized to the case of scalar and polarized inner radiation fields taking into account the multiple anisotropic scattering of photons and their reflection from an arbitrary horizontally uniform underlying surface.ΠΠ° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΏΡΠΈΠ½ΡΠΈΠΏΠ° Π·Π΅ΡΠΊΠ°Π»ΡΠ½ΠΎΠ³ΠΎ ΠΎΡΠΎΠ±ΡΠ°ΠΆΠ΅Π½ΠΈΡ ΠΈ ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΡΡΡΠΈΡ
ΡΠ΅ΡΠ΅Π½ΠΈΠΉ ΠΌΠΎΠ΄ΠΈΡΠΈΡΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
Π»ΠΈΠ½Π΅ΠΉΠ½ΡΡ
ΡΠΈΠ½Π³ΡΠ»ΡΡΠ½ΡΡ
ΠΈΠ½ΡΠ΅Π³ΡΠ°Π»ΡΠ½ΡΡ
ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΉ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΎ ΡΠΈΡΠ»Π΅Π½Π½ΠΎΠ΅ ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ Π΅Π΄ΠΈΠ½ΠΎΠΉ ΡΡΠ½ΠΊΡΠΈΠΈ Π²Π½Π΅ΡΠ½Π΅Π³ΠΎ ΠΏΠΎΠ»Ρ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ ΠΈ ΡΠΎΡΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈΠ½Π²Π°ΡΠΈΠ°Π½ΡΠΎΠ² ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠΎΠ² ΡΡΠΊΠΎΡΡΠΈ ΠΏΠ»ΠΎΡΠΊΠΎΠ³ΠΎ ΠΎΠ΄Π½ΠΎΡΠΎΠ΄Π½ΠΎΠ³ΠΎ ΡΠ»ΠΎΡ ΠΊΠΎΠ½Π΅ΡΠ½ΠΎΠΉ ΠΎΠΏΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠΎΠ»ΡΠΈΠ½Ρ Π½Π° Π΅Π³ΠΎ Π²Π½Π΅ΡΠ½ΠΈΡ
Π³ΡΠ°Π½ΠΈΡΠ°Ρ
. ΠΠΎΠΊΠ°Π·Π°Π½Π° ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ ΡΡΠΈΡ
ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΉ ΠΏΡΠΈ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠΈ ΠΌΠ΅ΡΠΎΠ΄Π° ΡΠ³Π»ΠΎΠ²ΠΎΠΉ Π΄ΠΈΡΠΊΡΠ΅ΡΠΈΠ·Π°ΡΠΈΠΈ Π² Π·Π°Π΄Π°ΡΠ°Ρ
ΡΠΈΡΠ»Π΅Π½Π½ΠΎΠ³ΠΎ ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΏΠΎΠ»Π΅ΠΉ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ ΡΠΈΡΡΠ΅ΠΌΡ Β«Π°ΡΠΌΠΎΡΡΠ΅ΡΠ° β ΠΏΠΎΠ΄ΡΡΠΈΠ»Π°ΡΡΠ°Ρ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΡΒ». Π£ΠΊΠ°Π·Π°Π½Π½ΡΠΉ Π½ΠΎΠ²ΡΠΉ ΠΏΠΎΠ΄Ρ
ΠΎΠ΄ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΠ΅Ρ ΠΎΠ±ΠΎΠ±ΡΠΈΡΡ ΠΎΡΠ½ΠΎΠ²Π½ΡΠ΅ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΡΠΈΡΠ»Π΅Π½Π½ΠΎΠ³ΠΎ ΡΠ°Π΄ΠΈΠ°ΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΡ Π² ΡΠ°ΡΡΠ½ΠΎΠΌ ΡΠ»ΡΡΠ°Π΅ ΠΏΠΎΠ»ΡΠ±Π΅ΡΠΊΠΎΠ½Π΅ΡΠ½ΠΎΠ³ΠΎ ΠΎΠ΄Π½ΠΎΡΠΎΠ΄Π½ΠΎΠ³ΠΎ ΡΠ»ΠΎΡ. Π ΡΡΠΎΠΉ ΡΠ²ΡΠ·ΠΈ ΡΠ°ΡΡΠΌΠΎΡΡΠ΅Π½Ρ ΠΎΡΠ½ΠΎΠ²Π½ΡΠ΅ ΠΌΠ°ΡΠ΅ΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ Π°ΡΠΏΠ΅ΠΊΡΡ ΠΈ Π²ΡΡΠΈΡΠ»ΠΈΡΠ΅Π»ΡΠ½ΡΠ΅ ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΠΈ ΡΠΈΡΠ»Π΅Π½Π½ΠΎΠΉ ΡΠ΅Π°Π»ΠΈΠ·Π°ΡΠΈΠΈ ΠΌΠ΅ΡΠΎΠ΄Π° ΡΠ³Π»ΠΎΠ²ΠΎΠΉ Π΄ΠΈΡΠΊΡΠ΅ΡΠΈΠ·Π°ΡΠΈΠΈ. ΠΡΠ»Π΅Π΄ΡΡΠ²ΠΈΠ΅ Π»ΠΈΠ½Π΅ΠΉΠ½ΠΎΡΡΠΈ ΠΈΡΠΏΠΎΠ»ΡΠ·ΡΠ΅ΠΌΡΡ
Π±Π°Π·ΠΎΠ²ΡΡ
ΠΈΠ½ΡΠ΅Π³ΡΠ°Π»ΡΠ½ΡΡ
ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΉ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½Π½ΡΠΉ Π°Π½Π°Π»ΠΈΠ· ΠΌΠΎΠΆΠ½ΠΎ ΠΎΠ±ΠΎΠ±ΡΠΈΡΡ Π½Π° ΡΠ»ΡΡΠ°ΠΉ ΡΠΊΠ°Π»ΡΡΠ½ΡΡ
ΠΈ ΠΏΠΎΠ»ΡΡΠΈΠ·ΠΎΠ²Π°Π½Π½ΡΡ
ΠΏΠΎΠ»Π΅ΠΉ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ ΠΏΡΠΈ ΡΡΠ΅ΡΠ΅ ΠΌΠ½ΠΎΠ³ΠΎΠΊΡΠ°ΡΠ½ΠΎΠ³ΠΎ Π°Π½ΠΈΠ·ΠΎΡΡΠΎΠΏΠ½ΠΎΠ³ΠΎ ΡΠ°ΡΡΠ΅ΡΠ½ΠΈΡ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ ΠΈ Π΅Π³ΠΎ ΠΎΡΡΠ°ΠΆΠ΅Π½ΠΈΡ ΠΎΡ ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ»ΡΠ½ΠΎΠΉ Π³ΠΎΡΠΈΠ·ΠΎΠ½ΡΠ°Π»ΡΠ½ΠΎ-ΠΎΠ΄Π½ΠΎΡΠΎΠ΄Π½ΠΎΠΉ ΠΏΠΎΠ΄ΡΡΠΈΠ»Π°ΡΡΠ΅ΠΉ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ
Large Deployable Reflector Science and Technology Workshop. Volume 3: Systems and Technology Assessment
The results of five technology panels which convened to discuss the Large Deployable Reflector (LDR) are presented. The proposed LDR is a large, ambient-temperature, far infrared/submillimeter telescope designed for space. Panel topics included optics, materials and structures, sensing and control, science instruments, and systems and missions. The telescope requirements, the estimated technology levels, and the areas in which the generic technology work has to be augmented are enumerated
Polarized thermal emission from X-ray Dim Isolated Neutron Stars: the case of RX J1856.5-3754
The observed polarization properties of thermal radiation from isolated,
cooling neutron stars depend on both the emission processes at the surface and
the effects of the magnetized vacuum which surrounds the star. Here we
investigate the polarized thermal emission from X-ray Dim Isolated Neutron
Stars, taking RX J1856.5-3754 as a representative case. The physical conditions
of the star outermost layers in these sources is still debated, and so we
consider emission from a magnetized atmosphere and a condensed surface,
accounting for the effects of vacuum polarization as the radiation propagates
in the star magnetosphere. We have found that, for a significant range of
viewing geometries, measurement of the phase-averaged polarization fraction and
phase-averaged polarization angle at both optical and X-ray wavelengths allow
us to determine whether this neutron star has an atmosphere or a condensed
surface. Our results may therefore be relevant in view of future developments
of soft X-ray polarimeters.Comment: 12 pages, 12 figures, accepted for publication in MNRA
Imaging light transport at the femtosecond scale
Paper, milk, clouds and white paint share a common property: they are opaque disordered media through which light scatters randomly rather than propagating in a straight path. For very thick and turbid media, indeed, light eventually propagates in a βdiffusiveβ way, i.e. similarly to how tea infuses through hot water. Frequently though, a material is neither perfectly opaque nor transparent and the simple diffusion model does not hold. In this work, we developed a novel optical-gating setup that allowed us to observe light transport in scattering media with sub-ps time resolution. An array of unexplored aspects of light propagation emerged from this spatio-temporal description, unveiling transport regimes that were previously inaccessibile due to the extreme time scales involved and the lack of analytical models
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