49 research outputs found
Measuring the gap in ARPES experiments
Angle-resolved photoemission spectroscopy (ARPES) is considered as the only
experimental tool from which the momentum distribution of both the
superconducting and pseudo-gap can be quantitatively derived. The binding
energy of the leading edge of the photoemission spectrum, usually called the
leading edge gap (LEG), is the model-independent quantity which can be measured
in the modern ARPES experiments with the very high accuracy--better than 1 meV.
This, however, may be useless as long as the relation between the LEG and the
real gap is unknown. We present a systematic study of the LEG as a function of
a number of physical and experimental parameters. The absolute gap values which
have been derived from the numerical simulation prove, for example that the
nodal direction in the underdoped Bi-2212 in superconducting state is really
the node--the gap is zero. The other consequences of the simulations are
discussed.Comment: revtex4, 9 pages, 6 figure
Π‘ΡΠ°Π²Π½ΠΈΡΠ΅Π»ΡΠ½ΠΎΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ ΡΠ΅Π³Π΅Π½Π΅ΡΠ°ΡΠΈΠΈ Ρ Π³ΡΠ±ΠΎΠΊ (Porifera)
International audiencet is well known that sponges have unusually high regenerative abilities, which are often associated with their low tissue organization and high dynamics of cell differentiation. In order to identify the diversity of morphogenesis and cellular mechanisms involved in the restoration processes in Porifera, we carried out a detailed comparative study of the regeneration of a number of sponge species from phylogenetically deleted taxa that differ in their anatomical and histological organization. The objects of this project were sponges from the classes Demospongiae, Homoscleromorpha, and Calcarea, which have the leukonoid, siconoid, and asconoid types of the aquiferous system e-mines, as well as different degrees of epithelial development. The main mechanism for the regeneration of leukonoid Demospongiae is the epithelio-mesenchymal transformation involving polypotent archaeocyte cells. Epithelial morphogenesis and cell transdifferentiation are the basis for the regeneration of leukoid Homoscleromorpha and siconoid and asconoid Calcarea. Asconoid Calcarea regeneration is a rare example of βpureβ morphallaxis. We have shown that the morphogenetic processes detected in sponges are as complex and diverse as in other higher animals. Thus, sponges can be a source of important information that will allow us to better understand the early evolution of molecular and cellular mechanisms of morphogenesis in animals.2 Π‘ΠΠ±ΠΠ£, Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠΉ ΡΠ°ΠΊΡΠ»ΡΡΠ΅Ρ 3 ΠΠΠ£ ΠΈΠΌ. ΠΠΎΠΌΠΎΠ½ΠΎΡΠΎΠ²Π°, Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠΉ ΡΠ°ΠΊΡΠ»ΡΡΠ΅Ρ, ΠΠ΅Π»ΠΎΠΌΠΎΡΡΠΊΠ°Ρ Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠ°Ρ ΡΡΠ°Π½ΡΠΈΡ ΠΈΠΌ. Π.Π. ΠΠ΅ΡΡΠΎΠ²Π° Π₯ΠΎΡΠΎΡΠΎ ΠΈΠ·Π²Π΅ΡΡΠ½ΠΎ, ΡΡΠΎ Π³ΡΠ±ΠΊΠΈ ΠΎΠ±Π»Π°Π΄Π°ΡΡ Π½Π΅ΠΎΠ±ΡΡΠ°ΠΉΠ½ΠΎ Π²ΡΡΠΎΠΊΠΈΠΌΠΈ ΡΠ΅Π³Π΅Π½Π΅ΡΠ°ΡΠΈΠΎΠ½Π½ΡΠΌΠΈ ΡΠΏ ΠΎ-ΡΠΎΠ±Π½ΠΎΡΡΡΠΌΠΈ ΡΡΠΎ ΡΠ°ΡΡΠΎ ΡΠ²ΡΠ·ΡΠ²Π°ΡΡ Ρ ΠΈΡ
Π½ΠΈΠ·ΠΊΠΎΠΉ ΡΠΊΠ°Π½Π΅Π²ΠΎΠΉ ΠΎΡΠ³Π°Π½ΠΈΠ·Π°ΡΠΈΠ΅ΠΉ ΠΈ Π²ΡΡΠΎΠΊΠΎΠΉ Π΄ΠΈΠ½Π°ΠΌΠΈΠΊΠΎΠΉ ΠΊΠ»Π΅ΡΠΎΡΠ½ΠΎΠΉ Π΄ΠΈΡΡΠ΅ΡΠ΅Π½ΡΠΈΡΠΎΠ²ΠΊΠΈ. ΠΠ»Ρ ΡΠΎΠ³ΠΎ, ΡΡΠΎΠ±Ρ Π²ΡΡΠ²ΠΈΡΡ ΡΠ°Π·Π½ΠΎΠΎΠ±ΡΠ°Π·ΠΈΠ΅ ΠΌΠΎΡΡΠΎΠ³Π΅Π½Π΅Π·ΠΎΠ² ΠΈ ΠΊΠ»Π΅ΡΠΎΡ-Π½ΡΡ
ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΠΎΠ² Π²ΠΎΠ²Π»Π΅ΡΠ΅Π½Π½ΡΡ
Π² Π²ΠΎΡΡΡΠ°Π½ΠΎΠ²ΠΈΡΠ΅Π»ΡΠ½ΡΠ΅ ΠΏΡΠΎΡΠ΅ΡΡΡ Ρ Porifera, Π½Π°ΠΌΠΈ Π±ΡΠ»ΠΎ ΠΏΡΠ΅Π΄ΠΏΡ ΠΈ-Π½ΡΡΠΎ Π΄Π΅ΡΠ°Π»ΡΠ½ΠΎΠ΅ ΡΡΠ°Π²Π½ΠΈΡΠ΅Π»ΡΠ½ΠΎΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ ΡΠ΅Π³Π΅Π½Π΅ΡΠ°ΡΠΈΠΈ ΡΡΠ΄Π° Π²ΠΈΠ΄ΠΎΠ² Π³ΡΠ±ΠΎΠΊ ΠΈΠ· ΡΠΈΠ»ΠΎΠ³Π΅Π½Π΅ΡΠΈΡ Π΅-ΡΠΊΠΈ ΡΠ΄Π°Π»Π΅Π½Π½ΡΡ
ΡΠ°ΠΊΡΠΎΠ½ΠΎΠ², ΠΎΡΠ»ΠΈΡΠ°ΡΡΠΈΠ΅ΡΡ Π°Π½Π°ΡΠΎΠΌΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΈ Π³ΠΈΡΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΎΡΠ³Π°Π½ΠΈΠ·Π°ΡΠΈΠ΅ΠΉ. ΠΠ±ΡΠ΅ΠΊΡΠ°ΠΌΠΈ Π΄Π°Π½Π½ΠΎΠ³ΠΎ ΠΏΡΠΎΠ΅ΠΊΡΠ° ΠΏΠΎΡΠ»ΡΠΆΠΈΠ»ΠΈ Π³ΡΠ±ΠΊΠΈ ΠΈΠ· ΠΊΠ»Π°ΡΡΠΎΠ² Demospongiae, Homoscleromorpha ΠΈ Calcarea, ΠΎΠ±Π»Π°Π΄Π°ΡΡΠΈΠ΅ Π»Π΅ΠΉΠΊΠΎΠ½ΠΎΠΈΠ΄Π½ΠΎΠΉ, ΡΠΈΠΊΠΎΠ½ΠΎΠΈΠ΄Π½ΠΎΠΉ ΠΈ Π°ΡΠΊΠΎΠ½ΠΎΠΈΠ΄Π½ΠΎΠΉ ΡΠΈΠΏΠ°ΠΌΠΈ Π²ΠΎΠ΄ΠΎΠ½ΠΎΡΠ½ΠΎΠΉ ΡΠΈΡΡ Π΅-ΠΌΡ, Π° ΡΠ°ΠΊΠΆΠ΅ ΡΠ°Π·Π½ΠΎΠΉ ΡΡΠ΅ΠΏΠ΅Π½ΡΡ ΡΠ°Π·Π²ΠΈΡΠΈΡ ΡΠΏΠΈΡΠ΅Π»ΠΈΡ. ΠΡΠ½ΠΎΠ²Π½ΡΠΌ ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΠΎΠΌ ΡΠ΅Π³Π΅Π½Π΅ΡΠ°ΡΠΈΠΈ Π»Π΅ΠΉΠΊΠΎ-Π½ΠΎΠΈΠ΄Π½ΡΡ
Demospongiae ΡΠ²Π»ΡΠ΅ΡΡΡ ΡΠΏΠΈΡΠ΅Π»ΠΈΠΎ-ΠΌΠ΅Π·Π΅Π½Ρ
ΠΈΠΌΠ½Π°Ρ ΡΡΠ°Π½ΡΡΠΎΡΠΌΠ°ΡΠΈΡ Ρ Π²ΠΎΠ²Π»Π΅ΡΠ΅Π½ΠΈΠ΅ΠΌ ΠΏΠΎΠ»ΠΈ-ΠΏΠΎΡΠ΅Π½ΡΠ½ΡΡ
ΠΊΠ»Π΅ΡΠΎΠΊ-Π°ΡΡ
Π΅ΠΎΡΠΈΡΠΎΠ². ΠΡΠ½ΠΎΠ²ΠΎΠΉ ΡΠ΅Π³Π΅Π½Π΅ΡΠ°ΡΠΈΠΈ Π»Π΅ΠΉΠΊΠΎΠ½ΠΎΠΈΠ΄Π½ΡΡ
Homoscleromorpha ΠΈ ΡΠΈΠΊΠΎΠ½ΠΎΠΈΠ΄Π½ΡΡ
ΠΈ Π°ΡΠΊΠΎΠ½ΠΎΠΈΠ΄Π½ΡΡ
Calcarea ΡΠ»ΡΠΆΠ°Ρ ΡΠΏΠΈΡΠ΅Π»ΠΈΠ°Π»ΡΠ½ΡΠ΅ ΠΌΠΎΡΡΠΎΠ³Π΅Π½Π΅Π·Ρ ΠΈ ΡΡΠ°Π½ΡΠ΄ΠΈΡΡΠ΅ΡΠ΅Π½-ΡΠΈΡΠΎΠ²ΠΊΠ° ΠΊΠ»Π΅ΡΠΎΠΊ. Π Π΅Π³Π΅Π½Π΅ΡΠ°ΡΠΈΡ Π°ΡΠΊΠΎΠ½ΠΎΠΈΠ΄Π½ΡΡ
Calcarea ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»ΡΠ΅Ρ ΡΠΎΠ±ΠΎΠΉ ΡΠ΅Π΄ΠΊΠΈΠΉ ΠΏΡΠΈΠΌΠ΅Ρ Β«ΡΠΈ-ΡΡΠΎΠ³ΠΎΒ» ΠΌΠΎΡΡΠ°Π»Π»Π°ΠΊΡΠΈΡΠ°. ΠΡ ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΈ, ΡΡΠΎ ΠΌΠΎΡΡΠΎΠ³Π΅Π½Π΅ΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΏΡΠΎΡΠ΅ΡΡΡ, Π²ΡΡΠ²Π»Π΅Π½Π½ΡΠ΅ Ρ Π³ΡΠ±ΠΎΠΊ, ΡΠ²Π»ΡΡΡΡΡ ΡΡΠΎΠ»Ρ ΠΆΠ΅ ΡΠ»ΠΎΠΆΠ½ΡΠΌΠΈ ΠΈ ΡΠ°Π·Π½ΠΎΠΎΠ±ΡΠ°Π·Π½ΡΠΌΠΈ, ΠΊΠ°ΠΊ ΠΈ Ρ Π΄ΡΡΠ³ΠΈΡ
Π²ΡΡΡΠΈΡ
ΠΆΠΈΠ²ΠΎΡΠ½ΡΡ
. Π’Π°ΠΊΠΈΠΌ ΠΎΠ±ΡΠ°Π·ΠΎΠΌ, Π³ΡΠ±ΠΊΠΈ ΠΌΠΎΠ³ΡΡ Π±ΡΡΡ ΠΈΡΡΠΎΡΠ½ΠΈΠΊΠΎΠΌ Π²Π°ΠΆΠ½ΠΎΠΉ ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΠΈ, ΠΊΠΎΡΠΎΡΠ°Ρ ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΡ Π½Π°ΠΌ Π³Π»ΡΠ±ΠΆΠ΅ ΠΏΠΎΠ½ΡΡΡ ΡΠ°Π½Π½ΡΡ ΡΠ²ΠΎΠ»ΡΡΠΈΡ ΠΌΠΎΠ»Π΅ΠΊΡΠ»ΡΡΠ½ΡΡ
ΠΈ ΠΊΠ»Π΅ΡΠΎΡΠ½ΡΡ
ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΠΎΠ² ΠΌΠΎΡΡΠΎΠ³Π΅Π½Π΅Π·Π° Ρ ΠΆΠΈΠ²ΠΎΡΠ½ΡΡ
. ΠΠ»Π°Π³ΠΎΠ΄Π°ΡΠ½ΠΎΡΡΠΈ ΠΠ°Π½Π½Π°Ρ ΡΠ°Π±ΠΎΡΠ° ΠΎΡΡΡΠ΅ΡΡΠ²Π»Π΅Π½Π° ΠΏΡΠΈ ΡΠΈΠ½Π°Π½ΡΠΎΠ²ΠΎΠΉ ΠΏΠΎΠ΄Π΄Π΅ΡΠΆΠΊΠ΅ Π³ΡΠ°Π½ΡΠΎΠ² Π Π€Π€Π β 16-04-00084, ΠΈ Π ΠΠ€ β 17-14-01089.-8
Nanotube-based source of charges for experiments with solid helium at low temperatures
Methods of preparation of the field-emission sources of charges from carbon nanotubes suitable for study of injected
charges in solid helium at low temperatures T < 1 K are presented. The sources have been prepared by arc
discharge deposition of nanotubes onto a flat copper substrate or by mechanical rubbing of nanotubes into porous
metal surface. The test study of the voltage-current characteristics of a diode cell with the nanotube source in superfluid
He II have shown that at voltages above 120 V one can observe a relatively large current I β₯ 10β»ΒΉΒ³ A of negative
charges in liquid helium. The field and temperature dependences of positive and negative currents in solid β΄He
were studied in samples grown by the blocked capillary technique. Usage of the nanotube based source of injected
charges had permitted us for the first time to observe motion of the positive charges in solid helium at temperatures
below 0.1 Π. The current-voltage dependence could be described by a power law I ~ UΞ±, with the value of the exponent Ξ± >> 2, much higher than what one would expect for the regime of space charge limited currents
Single-photon emitters in GaSe
Single-photon sources are important building blocks for quantum information technology. Emitters based on solid-state systems provide a viable route to integration in photonic devices. Here, we report on single-photon emitters in the layered semiconductor GaSe. We identify the exciton and biexciton transition of the quantum emitters with power-dependent photoluminescence and photon statistics measurements. We find evidence that the localization of the excitons is related to deformations of the GaSe crystal, caused by nanoscale selenium inclusions, which are incorporated in the crystal. These deformations give rise to local strain fields, which induce confinement potentials for the excitons. This mechanism lights the way for the controlled positioning of single-photon emitters in GaSe on the nanoscale
Photoluminescence of two-dimensional GaTe and GaSe films
Gallium chalcogenides are promising building blocks for novel van der Waals heterostructures. We report on the low-temperature micro-photoluminescence (PL) of GaTe and GaSe films with thicknesses ranging from 200 nm to a single unit cell. In both materials, PL shows a dramatic decrease by 10e4β10e5 when film thickness is reduced from 200 to 10 nm. Based on evidence from continuous-wave (cw) and time-resolved PL, we propose a model explaining the PL decrease as a result of non-radiative carrier escape via surface states. Our results emphasize the need for special passivation of two-dimensional films for optoelectronic applications
ARPES Spectra of the Hubbard model
We discuss spectra calculated for the 2D Hubbard model in the intermediate
coupling regime with the dynamical cluster approximation, which is a
non-perturbative approach. We find a crossover from a normal Fermi liquid with
a Fermi surface closed around the Brillouin zone center at large doping to a
non-Fermi liquid for small doping. The crossover is signalled by a splitting of
the Fermi surface around the point of the 2D Brillouin zone, which
eventually leads to a hole-like Fermi surface closed around the point M. The
topology of the Fermi surface at low doping indicates a violation of
Luttinger's theorem. We discuss different ways of presenting the spectral data
to extract information about the Fermi surface. A comparison to recent
experiments will be presented.Comment: 8 pages, 7 color figures, uses RevTeX
Effect of electron irradiation on vortex dynamics in YBa_2Cu_3O_{7-x} single crystals
We report on drastic change of vortex dynamics with increase of quenched
disorder: for rather weak disorder we found a single vortex creep regime, which
we attribute to a Bragg-glass phase, while for enhanced disorder we found an
increase of both the depinning current and activation energy with magnetic
field, which we attribute to entangled vortex phase. We also found that
introduction of additional defects always increases the depinning current, but
it increases activation energy only for elastic vortex creep, while it
decreases activation energy for plastic vortex creep.Comment: 4 pages, 3 figures, submited to Phys. Rev.
Π‘ΡΠ°Π²Π½ΠΈΡΠ΅Π»ΡΠ½ΠΎΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ ΡΠ΅Π³Π΅Π½Π΅ΡΠ°ΡΠΈΠΈ Ρ Π³ΡΠ±ΠΎΠΊ (Porifera)
International audiencet is well known that sponges have unusually high regenerative abilities, which are often associated with their low tissue organization and high dynamics of cell differentiation. In order to identify the diversity of morphogenesis and cellular mechanisms involved in the restoration processes in Porifera, we carried out a detailed comparative study of the regeneration of a number of sponge species from phylogenetically deleted taxa that differ in their anatomical and histological organization. The objects of this project were sponges from the classes Demospongiae, Homoscleromorpha, and Calcarea, which have the leukonoid, siconoid, and asconoid types of the aquiferous system e-mines, as well as different degrees of epithelial development. The main mechanism for the regeneration of leukonoid Demospongiae is the epithelio-mesenchymal transformation involving polypotent archaeocyte cells. Epithelial morphogenesis and cell transdifferentiation are the basis for the regeneration of leukoid Homoscleromorpha and siconoid and asconoid Calcarea. Asconoid Calcarea regeneration is a rare example of βpureβ morphallaxis. We have shown that the morphogenetic processes detected in sponges are as complex and diverse as in other higher animals. Thus, sponges can be a source of important information that will allow us to better understand the early evolution of molecular and cellular mechanisms of morphogenesis in animals.2 Π‘ΠΠ±ΠΠ£, Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠΉ ΡΠ°ΠΊΡΠ»ΡΡΠ΅Ρ 3 ΠΠΠ£ ΠΈΠΌ. ΠΠΎΠΌΠΎΠ½ΠΎΡΠΎΠ²Π°, Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠΉ ΡΠ°ΠΊΡΠ»ΡΡΠ΅Ρ, ΠΠ΅Π»ΠΎΠΌΠΎΡΡΠΊΠ°Ρ Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠ°Ρ ΡΡΠ°Π½ΡΠΈΡ ΠΈΠΌ. Π.Π. ΠΠ΅ΡΡΠΎΠ²Π° Π₯ΠΎΡΠΎΡΠΎ ΠΈΠ·Π²Π΅ΡΡΠ½ΠΎ, ΡΡΠΎ Π³ΡΠ±ΠΊΠΈ ΠΎΠ±Π»Π°Π΄Π°ΡΡ Π½Π΅ΠΎΠ±ΡΡΠ°ΠΉΠ½ΠΎ Π²ΡΡΠΎΠΊΠΈΠΌΠΈ ΡΠ΅Π³Π΅Π½Π΅ΡΠ°ΡΠΈΠΎΠ½Π½ΡΠΌΠΈ ΡΠΏ ΠΎ-ΡΠΎΠ±Π½ΠΎΡΡΡΠΌΠΈ ΡΡΠΎ ΡΠ°ΡΡΠΎ ΡΠ²ΡΠ·ΡΠ²Π°ΡΡ Ρ ΠΈΡ
Π½ΠΈΠ·ΠΊΠΎΠΉ ΡΠΊΠ°Π½Π΅Π²ΠΎΠΉ ΠΎΡΠ³Π°Π½ΠΈΠ·Π°ΡΠΈΠ΅ΠΉ ΠΈ Π²ΡΡΠΎΠΊΠΎΠΉ Π΄ΠΈΠ½Π°ΠΌΠΈΠΊΠΎΠΉ ΠΊΠ»Π΅ΡΠΎΡΠ½ΠΎΠΉ Π΄ΠΈΡΡΠ΅ΡΠ΅Π½ΡΠΈΡΠΎΠ²ΠΊΠΈ. ΠΠ»Ρ ΡΠΎΠ³ΠΎ, ΡΡΠΎΠ±Ρ Π²ΡΡΠ²ΠΈΡΡ ΡΠ°Π·Π½ΠΎΠΎΠ±ΡΠ°Π·ΠΈΠ΅ ΠΌΠΎΡΡΠΎΠ³Π΅Π½Π΅Π·ΠΎΠ² ΠΈ ΠΊΠ»Π΅ΡΠΎΡ-Π½ΡΡ
ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΠΎΠ² Π²ΠΎΠ²Π»Π΅ΡΠ΅Π½Π½ΡΡ
Π² Π²ΠΎΡΡΡΠ°Π½ΠΎΠ²ΠΈΡΠ΅Π»ΡΠ½ΡΠ΅ ΠΏΡΠΎΡΠ΅ΡΡΡ Ρ Porifera, Π½Π°ΠΌΠΈ Π±ΡΠ»ΠΎ ΠΏΡΠ΅Π΄ΠΏΡ ΠΈ-Π½ΡΡΠΎ Π΄Π΅ΡΠ°Π»ΡΠ½ΠΎΠ΅ ΡΡΠ°Π²Π½ΠΈΡΠ΅Π»ΡΠ½ΠΎΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ ΡΠ΅Π³Π΅Π½Π΅ΡΠ°ΡΠΈΠΈ ΡΡΠ΄Π° Π²ΠΈΠ΄ΠΎΠ² Π³ΡΠ±ΠΎΠΊ ΠΈΠ· ΡΠΈΠ»ΠΎΠ³Π΅Π½Π΅ΡΠΈΡ Π΅-ΡΠΊΠΈ ΡΠ΄Π°Π»Π΅Π½Π½ΡΡ
ΡΠ°ΠΊΡΠΎΠ½ΠΎΠ², ΠΎΡΠ»ΠΈΡΠ°ΡΡΠΈΠ΅ΡΡ Π°Π½Π°ΡΠΎΠΌΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΈ Π³ΠΈΡΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΎΡΠ³Π°Π½ΠΈΠ·Π°ΡΠΈΠ΅ΠΉ. ΠΠ±ΡΠ΅ΠΊΡΠ°ΠΌΠΈ Π΄Π°Π½Π½ΠΎΠ³ΠΎ ΠΏΡΠΎΠ΅ΠΊΡΠ° ΠΏΠΎΡΠ»ΡΠΆΠΈΠ»ΠΈ Π³ΡΠ±ΠΊΠΈ ΠΈΠ· ΠΊΠ»Π°ΡΡΠΎΠ² Demospongiae, Homoscleromorpha ΠΈ Calcarea, ΠΎΠ±Π»Π°Π΄Π°ΡΡΠΈΠ΅ Π»Π΅ΠΉΠΊΠΎΠ½ΠΎΠΈΠ΄Π½ΠΎΠΉ, ΡΠΈΠΊΠΎΠ½ΠΎΠΈΠ΄Π½ΠΎΠΉ ΠΈ Π°ΡΠΊΠΎΠ½ΠΎΠΈΠ΄Π½ΠΎΠΉ ΡΠΈΠΏΠ°ΠΌΠΈ Π²ΠΎΠ΄ΠΎΠ½ΠΎΡΠ½ΠΎΠΉ ΡΠΈΡΡ Π΅-ΠΌΡ, Π° ΡΠ°ΠΊΠΆΠ΅ ΡΠ°Π·Π½ΠΎΠΉ ΡΡΠ΅ΠΏΠ΅Π½ΡΡ ΡΠ°Π·Π²ΠΈΡΠΈΡ ΡΠΏΠΈΡΠ΅Π»ΠΈΡ. ΠΡΠ½ΠΎΠ²Π½ΡΠΌ ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΠΎΠΌ ΡΠ΅Π³Π΅Π½Π΅ΡΠ°ΡΠΈΠΈ Π»Π΅ΠΉΠΊΠΎ-Π½ΠΎΠΈΠ΄Π½ΡΡ
Demospongiae ΡΠ²Π»ΡΠ΅ΡΡΡ ΡΠΏΠΈΡΠ΅Π»ΠΈΠΎ-ΠΌΠ΅Π·Π΅Π½Ρ
ΠΈΠΌΠ½Π°Ρ ΡΡΠ°Π½ΡΡΠΎΡΠΌΠ°ΡΠΈΡ Ρ Π²ΠΎΠ²Π»Π΅ΡΠ΅Π½ΠΈΠ΅ΠΌ ΠΏΠΎΠ»ΠΈ-ΠΏΠΎΡΠ΅Π½ΡΠ½ΡΡ
ΠΊΠ»Π΅ΡΠΎΠΊ-Π°ΡΡ
Π΅ΠΎΡΠΈΡΠΎΠ². ΠΡΠ½ΠΎΠ²ΠΎΠΉ ΡΠ΅Π³Π΅Π½Π΅ΡΠ°ΡΠΈΠΈ Π»Π΅ΠΉΠΊΠΎΠ½ΠΎΠΈΠ΄Π½ΡΡ
Homoscleromorpha ΠΈ ΡΠΈΠΊΠΎΠ½ΠΎΠΈΠ΄Π½ΡΡ
ΠΈ Π°ΡΠΊΠΎΠ½ΠΎΠΈΠ΄Π½ΡΡ
Calcarea ΡΠ»ΡΠΆΠ°Ρ ΡΠΏΠΈΡΠ΅Π»ΠΈΠ°Π»ΡΠ½ΡΠ΅ ΠΌΠΎΡΡΠΎΠ³Π΅Π½Π΅Π·Ρ ΠΈ ΡΡΠ°Π½ΡΠ΄ΠΈΡΡΠ΅ΡΠ΅Π½-ΡΠΈΡΠΎΠ²ΠΊΠ° ΠΊΠ»Π΅ΡΠΎΠΊ. Π Π΅Π³Π΅Π½Π΅ΡΠ°ΡΠΈΡ Π°ΡΠΊΠΎΠ½ΠΎΠΈΠ΄Π½ΡΡ
Calcarea ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»ΡΠ΅Ρ ΡΠΎΠ±ΠΎΠΉ ΡΠ΅Π΄ΠΊΠΈΠΉ ΠΏΡΠΈΠΌΠ΅Ρ Β«ΡΠΈ-ΡΡΠΎΠ³ΠΎΒ» ΠΌΠΎΡΡΠ°Π»Π»Π°ΠΊΡΠΈΡΠ°. ΠΡ ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΈ, ΡΡΠΎ ΠΌΠΎΡΡΠΎΠ³Π΅Π½Π΅ΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΏΡΠΎΡΠ΅ΡΡΡ, Π²ΡΡΠ²Π»Π΅Π½Π½ΡΠ΅ Ρ Π³ΡΠ±ΠΎΠΊ, ΡΠ²Π»ΡΡΡΡΡ ΡΡΠΎΠ»Ρ ΠΆΠ΅ ΡΠ»ΠΎΠΆΠ½ΡΠΌΠΈ ΠΈ ΡΠ°Π·Π½ΠΎΠΎΠ±ΡΠ°Π·Π½ΡΠΌΠΈ, ΠΊΠ°ΠΊ ΠΈ Ρ Π΄ΡΡΠ³ΠΈΡ
Π²ΡΡΡΠΈΡ
ΠΆΠΈΠ²ΠΎΡΠ½ΡΡ
. Π’Π°ΠΊΠΈΠΌ ΠΎΠ±ΡΠ°Π·ΠΎΠΌ, Π³ΡΠ±ΠΊΠΈ ΠΌΠΎΠ³ΡΡ Π±ΡΡΡ ΠΈΡΡΠΎΡΠ½ΠΈΠΊΠΎΠΌ Π²Π°ΠΆΠ½ΠΎΠΉ ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΠΈ, ΠΊΠΎΡΠΎΡΠ°Ρ ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΡ Π½Π°ΠΌ Π³Π»ΡΠ±ΠΆΠ΅ ΠΏΠΎΠ½ΡΡΡ ΡΠ°Π½Π½ΡΡ ΡΠ²ΠΎΠ»ΡΡΠΈΡ ΠΌΠΎΠ»Π΅ΠΊΡΠ»ΡΡΠ½ΡΡ
ΠΈ ΠΊΠ»Π΅ΡΠΎΡΠ½ΡΡ
ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΠΎΠ² ΠΌΠΎΡΡΠΎΠ³Π΅Π½Π΅Π·Π° Ρ ΠΆΠΈΠ²ΠΎΡΠ½ΡΡ
. ΠΠ»Π°Π³ΠΎΠ΄Π°ΡΠ½ΠΎΡΡΠΈ ΠΠ°Π½Π½Π°Ρ ΡΠ°Π±ΠΎΡΠ° ΠΎΡΡΡΠ΅ΡΡΠ²Π»Π΅Π½Π° ΠΏΡΠΈ ΡΠΈΠ½Π°Π½ΡΠΎΠ²ΠΎΠΉ ΠΏΠΎΠ΄Π΄Π΅ΡΠΆΠΊΠ΅ Π³ΡΠ°Π½ΡΠΎΠ² Π Π€Π€Π β 16-04-00084, ΠΈ Π ΠΠ€ β 17-14-01089.-8