133 research outputs found
The Origin of the Boson Peak and the Thermal Conductivity Plateau in Low Temperature Glasses
We argue that the intrinsic glassy degrees of freedom in amorphous solids
giving rise to the thermal conductivity plateau and the ``boson peak'' in the
heat capacity at moderately low temperatures are directly connected to those
motions giving rise to the two-level like excitations seen at still lower
temperatures. These degrees of freedom can be thought of as strongly anharmonic
transitions between the local minima of the glassy energy landscape that are
accompanied by ripplon-like domain wall motions of the glassy mosaic structure
predicted to occur at by the random first order transition theory. The
energy spectrum of the vibrations of the mosaic depends on the glass transition
temperature, the Debye frequency and the molecular length scale. The resulting
spectrum reproduces the experimental low temperature Boson peak. The
``non-universality'' of the thermal conductivity plateau depends on and arises from calculable interactions with the phonons.Comment: 4 pages, submitted to PR
Stress distribution and the fragility of supercooled melts
We formulate a minimal ansatz for local stress distribution in a solid that
includes the possibility of strongly anharmonic short-length motions. We
discover a broken-symmetry metastable phase that exhibits an aperiodic,
frozen-in stress distribution. This aperiodic metastable phase is characterized
by many distinct, nearly degenerate configurations. The activated transitions
between the configurations are mapped onto the dynamics of a long range
classical Heisenberg model with 6-component spins and anisotropic couplings. We
argue the metastable phase corresponds to a deeply supercooled non-polymeric,
non-metallic liquid, and further establish an order parameter for the
glass-to-crystal transition. The spin model itself exhibits a continuous range
of behaviors between two limits corresponding to frozen-in shear and uniform
compression/dilation respectively. The two regimes are separated by a
continuous transition controlled by the anisotropy in the spin-spin
interaction, which is directly related to the Poisson ratio of the
material. The latter ratio and the ultra-violet cutoff of the theory determine
the liquid configurational entropy. Our results suggest that liquid's fragility
depends on the Poisson ratio in a non-monotonic way. The present ansatz
provides a microscopic framework for computing the configurational entropy and
relaxational spectrum of specific substances.Comment: 11 pages, 5 figures, Final version published in J Phys Chem
Universality in Glassy Low-Temperature Physics
We propose a microscopic translationally invariant glass model which exhibits
two level tunneling systems with a broad range of asymmetries and barrier
heights in its glassy phase. Their distribution is qualitatively different from
what is commonly assumed in phenomenological models, in that symmetric
tunneling systems are systematically suppressed. Still, the model exhibits the
usual glassy low-temperature anomalies. Universality is due to the collective
origin of the glassy potential energy landscape. We obtain a simple explanation
also for the mysterious {\em quantitative} universality expressed in the
unusually narrow universal glassy range of values for the internal friction
plateau.Comment: 4 pages, 5 figures, uses RevTeX
What are the interactions in quantum glasses?
The form of the low-temperature interactions between defects in neutral
glasses is reconsidered. We analyse the case where the defects can be modelled
either as simple 2-level tunneling systems, or tunneling rotational impurities.
The coupling to strain fields is determined up to 2nd order in the displacement
field. It is shown that the linear coupling generates not only the usual
Ising-like interaction between the rotational tunneling defect modes,
which cause them to freeze around a temperature , but also a random field
term. At lower temperatures the inversion symmetric tunneling modes are still
active - however the coupling of these to the frozen rotational modes, now via
the 2nd-order coupling to phonons, generates another random field term acting
on the inversion symmetric modes (as well as shorter-range interactions
between them). Detailed expressions for all these couplings are given.Comment: 12 pages, 2 figures. Minor modifications, published versio
ΠΠ°Π·Π΅ΡΠ½ΡΠ΅ ΡΠ°Π·ΠΎΠ²ΡΠ΅ Π΄Π°Π»ΡΠ½ΠΎΠΌΠ΅ΡΡ: ΠΏΡΡΠΈ ΠΏΠΎΠ²ΡΡΠ΅Π½ΠΈΡ ΡΠΎΡΠ½ΠΎΡΡΠΈ
Β Β Scientific and technological progress in the field of geodetic and industrial measurements in terms of the use of laser rangefinders operating in ranges up to 5000 meters has led to a reduction in the error of such measuring instruments over the past ten years by two or more times. Such rapid development of high-precision rangefinder technologies has led to a significant revision of the requirements for their metrological support, as well as to the need to develop a new generation of length standards, the stock of metrological accuracy of which would provide an assessment of the metrological characteristics of all types of existing and promising length measuring instruments with a laser rangefinder. To solve this problem, the Instituteβs staff conducted research within the framework of a number of thematic research and development works in terms of developing the appearance of a new generation of length standards operating in the range up to 5000 meters in an open atmosphere. Within the framework of this article, one of the developed models of a high-precision complex of measuring instruments for length and coordinate increments is considered, which is a serial high-precision laser phase light meter, modified by the instituteβs staff in terms of the system for receiving and processing measuring signals. At the same time, in order to increase the accuracy of length measurements using the developed range finder layout, it is proposed to investigate ways to reduce the errors of the model components of the boundaries of its error. To ensure the smallest error in determining the hardware correction of the rangefinder layout, it is proposed to use funds from the state primary special standard of the unit of length. As promising ways to reduce the error in determining the phase difference of signals, it is proposed to use digital recording and signal processing devices that implement a method for calculating the phase difference of signals by mathematically processing the recorded data using a specially developed computational algorithm based on Fourier analysis. For the most accurate determination of the values of the pulse repetition frequency of signals and the values of the speed of light on the measured track, it is proposed to improve the means of determining these indicators. The use of the proposed methods to improve the accuracy of measuring the length of laser phase rangefinders allows you to provide the necessary margin of metrological accuracy.Β Β ΠΠ°ΡΡΠ½ΠΎ-ΡΠ΅Ρ
Π½ΠΈΡΠ΅ΡΠΊΠΈΠΉ ΠΏΡΠΎΠ³ΡΠ΅ΡΡ Π² ΡΡΠ΅ΡΠ΅ Π³Π΅ΠΎΠ΄Π΅Π·ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈ ΠΏΡΠΎΠΌΡΡΠ»Π΅Π½Π½ΡΡ
ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΠΉ Π² ΡΠ°ΡΡΠΈ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ Π»Π°Π·Π΅ΡΠ½ΡΡ
Π΄Π°Π»ΡΠ½ΠΎΠΌΠ΅ΡΠΎΠ², ΡΠ°Π±ΠΎΡΠ°ΡΡΠΈΡ
Π² Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π°Ρ
Π΄ΠΎ 5 000 ΠΌΠ΅ΡΡΠΎΠ², ΠΏΡΠΈΠ²Π΅Π» ΠΊ ΡΠΌΠ΅Π½ΡΡΠ΅Π½ΠΈΡ ΠΏΠΎΠ³ΡΠ΅ΡΠ½ΠΎΡΡΠΈ Π²ΡΡΠ΅ ΠΏΠ΅ΡΠ΅ΡΠΈΡΠ»Π΅Π½Π½ΡΡ
ΡΡΠ΅Π΄ΡΡΠ² ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΠΉ Π·Π° ΠΏΠΎΡΠ»Π΅Π΄Π½ΠΈΠ΅ Π΄Π΅ΡΡΡΡ Π»Π΅Ρ Π² Π΄Π²Π° ΠΈ Π±ΠΎΠ»Π΅Π΅ ΡΠ°Π·Π°. Π‘Π»Π΅Π΄ΡΡΠ²ΠΈΠ΅ΠΌ ΡΠ°ΠΊΠΎΠ³ΠΎ ΡΡΡΠ΅ΠΌΠΈΡΠ΅Π»ΡΠ½ΠΎΠ³ΠΎ ΡΠ°Π·Π²ΠΈΡΠΈΡ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ Π²ΡΡΠΎΠΊΠΎΡΠΎΡΠ½ΠΎΠΉ Π΄Π°Π»ΡΠ½ΠΎΠΌΠ΅ΡΡΠΈΠΈ ΡΡΠ°Π» Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΡΠΉ ΠΏΠ΅ΡΠ΅ΡΠΌΠΎΡΡ ΡΡΠ΅Π±ΠΎΠ²Π°Π½ΠΈΠΉ ΠΏΠΎ ΠΈΡ
ΠΌΠ΅ΡΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠΌΡ ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠ΅Π½ΠΈΡ, Π° ΡΠ°ΠΊΠΆΠ΅ Π½Π΅ΠΎΠ±Ρ
ΠΎΠ΄ΠΈΠΌΠΎΡΡΡ ΡΠ°Π·ΡΠ°Π±ΠΎΡΠΊΠΈ Π½ΠΎΠ²ΠΎΠ³ΠΎ ΠΏΠΎΠΊΠΎΠ»Π΅Π½ΠΈΡ ΡΡΠ°Π»ΠΎΠ½ΠΎΠ² Π΄Π»ΠΈΠ½Ρ, Π·Π°ΠΏΠ°Ρ ΠΌΠ΅ΡΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠΎΡΠ½ΠΎΡΡΠΈ ΠΊΠΎΡΠΎΡΡΡ
ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠΈΠ²Π°Π» Π±Ρ ΠΎΡΠ΅Π½ΠΊΡ ΠΌΠ΅ΡΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊ Π²ΡΠ΅Ρ
ΡΠΈΠΏΠΎΠ² ΡΡΡΠ΅ΡΡΠ²ΡΡΡΠΈΡ
ΠΈ ΠΏΠ΅ΡΡΠΏΠ΅ΠΊΡΠΈΠ²Π½ΡΡ
ΡΡΠ΅Π΄ΡΡΠ² ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΠΉ Π΄Π»ΠΈΠ½Ρ, ΠΈΠΌΠ΅ΡΡΠΈΡ
Π² ΡΠ²ΠΎΠ΅ΠΌ ΡΠΎΡΡΠ°Π²Π΅ Π»Π°Π·Π΅ΡΠ½ΡΠΉ ΡΠ²Π΅ΡΠΎΠ΄Π°Π»ΡΠ½ΠΎΠΌΠ΅Ρ. ΠΠ»Ρ ΡΠ΅ΡΠ΅Π½ΠΈΡ ΡΡΠΎΠΉ Π·Π°Π΄Π°ΡΠΈ Π°Π²ΡΠΎΡΠ°ΠΌΠΈ Π² ΡΠ°ΠΌΠΊΠ°Ρ
ΡΡΠ΄Π° ΡΠ΅ΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΈΡ
Π½Π°ΡΡΠ½ΠΎ-ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°ΡΠ΅Π»ΡΡΠΊΠΈΡ
ΠΎΠΏΡΡΠ½ΠΎ-ΠΊΠΎΠ½ΡΡΡΡΠΊΡΠΎΡΡΠΊΠΈΡ
ΡΠ°Π±ΠΎΡ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈΡΡ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ Ρ ΡΠ΅Π»ΡΡ ΡΠ°Π·ΡΠ°Π±ΠΎΡΠΊΠΈ Π½ΠΎΠ²ΠΎΠ³ΠΎ ΠΏΠΎΠΊΠΎΠ»Π΅Π½ΠΈΡ ΡΡΠ°Π»ΠΎΠ½ΠΎΠ² Π΄Π»ΠΈΠ½Ρ, ΡΠ°Π±ΠΎΡΠ°ΡΡΠΈΡ
Π² Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π΅ Π΄ΠΎ 5 000 ΠΌΠ΅ΡΡΠΎΠ², Π² ΡΡΠ»ΠΎΠ²ΠΈΡΡ
ΠΎΡΠΊΡΡΡΠΎΠΉ Π°ΡΠΌΠΎΡΡΠ΅ΡΡ. Π Π΄Π°Π½Π½ΠΎΠΉ ΡΡΠ°ΡΡΠ΅ ΡΠ°ΡΡΠΌΠΎΡΡΠ΅Π½ ΠΎΠ΄ΠΈΠ½ ΠΈΠ· ΡΠ°Π·ΡΠ°Π±ΠΎΡΠ°Π½Π½ΡΡ
ΠΌΠ°ΠΊΠ΅ΡΠΎΠ² Π²ΡΡΠΎΠΊΠΎΡΠΎΡΠ½ΠΎΠ³ΠΎ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ° ΡΡΠ΅Π΄ΡΡΠ² ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΠΉ Π΄Π»ΠΈΠ½Ρ ΠΈ ΠΏΡΠΈΡΠ°ΡΠ΅Π½ΠΈΠΉ ΠΊΠΎΠΎΡΠ΄ΠΈΠ½Π°Ρ. ΠΠ°ΠΊΠ΅Ρ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»ΡΠ΅Ρ ΡΠΎΠ±ΠΎΠΉ Π²ΡΡΠΎΠΊΠΎΡΠΎΡΠ½ΡΠΉ Π»Π°Π·Π΅ΡΠ½ΡΠΉ ΡΠ°Π·ΠΎΠ²ΡΠΉ Π΄Π°Π»ΡΠ½ΠΎΠΌΠ΅Ρ Ρ Π΄ΠΎΡΠ°Π±ΠΎΡΠ°Π½Π½ΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΠΎΠΉ ΠΏΡΠΈΠ΅ΠΌΠ° ΠΈ ΠΎΠ±ΡΠ°Π±ΠΎΡΠΊΠΈ ΠΈΠ·ΠΌΠ΅ΡΠΈΡΠ΅Π»ΡΠ½ΡΡ
ΡΠΈΠ³Π½Π°Π»ΠΎΠ². Π‘ ΠΏΠΎΠΌΠΎΡΡΡ Π΄Π°Π½Π½ΠΎΠ³ΠΎ ΠΌΠ°ΠΊΠ΅ΡΠ° Π΄Π°Π»ΡΠ½ΠΎΠΌΠ΅ΡΠ° ΠΏΡΠ΅Π΄Π»Π°Π³Π°Π΅ΡΡΡ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°ΡΡ ΠΏΡΡΠΈ ΡΠΌΠ΅Π½ΡΡΠ΅Π½ΠΈΡ ΡΠΎΡΡΠ°Π²Π»ΡΡΡΠΈΡ
Π΅Π³ΠΎ ΠΏΠΎΠ³ΡΠ΅ΡΠ½ΠΎΡΡΠΈ Ρ ΡΠ΅Π»ΡΡ ΠΏΠΎΠ²ΡΡΠ΅Π½ΠΈΡ ΡΠΎΡΠ½ΠΎΡΡΠΈ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΠΉ Π΄Π»ΠΈΠ½Ρ. ΠΠ»Ρ ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠ΅Π½ΠΈΡ Π½Π°ΠΈΠΌΠ΅Π½ΡΡΠ΅ΠΉ ΠΏΠΎΠ³ΡΠ΅ΡΠ½ΠΎΡΡΠΈ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ Π°ΠΏΠΏΠ°ΡΠ°ΡΡΡΠ½ΠΎΠΉ ΠΏΠΎΠΏΡΠ°Π²ΠΊΠΈ ΠΌΠ°ΠΊΠ΅ΡΠ° Π΄Π°Π»ΡΠ½ΠΎΠΌΠ΅ΡΠ° ΠΌΠΎΠ³ΡΡ ΡΠ»ΡΠΆΠΈΡΡ ΡΡΠ΅Π΄ΡΡΠ²Π° ΠΈΠ· ΡΠΎΡΡΠ°Π²Π° ΠΠΎΡΡΠ΄Π°ΡΡΡΠ²Π΅Π½Π½ΠΎΠ³ΠΎ ΠΏΠ΅ΡΠ²ΠΈΡΠ½ΠΎΠ³ΠΎ ΡΠΏΠ΅ΡΠΈΠ°Π»ΡΠ½ΠΎΠ³ΠΎ ΡΡΠ°Π»ΠΎΠ½Π° Π΅Π΄ΠΈΠ½ΠΈΡΡ Π΄Π»ΠΈΠ½Ρ. Π ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅ ΠΏΠ΅ΡΡΠΏΠ΅ΠΊΡΠΈΠ²Π½ΡΡ
ΠΏΡΡΠ΅ΠΉ ΡΠΌΠ΅Π½ΡΡΠ΅Π½ΠΈΡ ΠΏΠΎΠ³ΡΠ΅ΡΠ½ΠΎΡΡΠΈ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ ΡΠ°Π·Π½ΠΎΡΡΠΈ ΡΠ°Π· ΡΠΈΠ³Π½Π°Π»ΠΎΠ² ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»ΡΠ΅ΡΡΡ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΡΠΌ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°ΡΡ ΡΡΡΡΠΎΠΉΡΡΠ²Π° ΡΠΈΡΡΠΎΠ²ΠΎΠΉ ΡΠ΅Π³ΠΈΡΡΡΠ°ΡΠΈΠΈ ΠΈ ΠΎΠ±ΡΠ°Π±ΠΎΡΠΊΠΈ ΡΠΈΠ³Π½Π°Π»ΠΎΠ², Π² ΠΊΠΎΡΠΎΡΡΡ
ΡΠ΅Π°Π»ΠΈΠ·ΠΎΠ²Π°Π½ ΠΌΠ΅ΡΠΎΠ΄ ΡΠ°ΡΡΠ΅ΡΠ° ΡΠ°Π·Π½ΠΎΡΡΠΈ ΡΠ°Π· ΡΠΈΠ³Π½Π°Π»ΠΎΠ² ΠΏΡΡΠ΅ΠΌ ΠΌΠ°ΡΠ΅ΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΎΠ±ΡΠ°Π±ΠΎΡΠΊΠΈ Π·Π°ΡΠ΅Π³ΠΈΡΡΡΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
Π΄Π°Π½Π½ΡΡ
Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΡΠΏΠ΅ΡΠΈΠ°Π»ΡΠ½ΠΎ ΡΠ°Π·ΡΠ°Π±ΠΎΡΠ°Π½Π½ΠΎΠ³ΠΎ Π²ΡΡΠΈΡΠ»ΠΈΡΠ΅Π»ΡΠ½ΠΎΠ³ΠΎ Π°Π»Π³ΠΎΡΠΈΡΠΌΠ° Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ Π€ΡΡΡΠ΅-Π°Π½Π°Π»ΠΈΠ·Π°. ΠΠ°ΠΈΠ±ΠΎΠ»Π΅Π΅ ΡΠΎΡΠ½ΠΎΠ΅ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ Π·Π½Π°ΡΠ΅Π½ΠΈΠΉ ΡΠ°ΡΡΠΎΡΡ ΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΠΈΠΌΠΏΡΠ»ΡΡΠ½ΡΡ
ΡΠΈΠ³Π½Π°Π»ΠΎΠ² ΠΈ Π·Π½Π°ΡΠ΅Π½ΠΈΠΉ ΡΠΊΠΎΡΠΎΡΡΠΈ ΡΠ²Π΅ΡΠ° Π½Π° ΠΈΠ·ΠΌΠ΅ΡΡΠ΅ΠΌΠΎΠΉ ΡΡΠ°ΡΡΠ΅ ΠΌΠΎΠΆΠ΅Ρ Π±ΡΡΡ ΠΏΠΎΠ»ΡΡΠ΅Π½ΠΎ Π±Π»Π°Π³ΠΎΠ΄Π°ΡΡ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ Π²ΡΡΠΎΠΊΠΎΡΠΎΡΠ½ΡΡ
ΡΡΠ΅Π΄ΡΡΠ² ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ Π΄Π°Π½Π½ΡΡ
ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Π΅ΠΉ. Π Π΅Π°Π»ΠΈΠ·Π°ΡΠΈΡ ΠΏΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½Π½ΡΡ
Π°Π²ΡΠΎΡΠ°ΠΌΠΈ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ² ΠΏΠΎΠ²ΡΡΠ΅Π½ΠΈΡ ΡΠΎΡΠ½ΠΎΡΡΠΈ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΠΉ Π΄Π»ΠΈΠ½Ρ Π»Π°Π·Π΅ΡΠ½ΡΡ
ΡΠ°Π·ΠΎΠ²ΡΡ
Π΄Π°Π»ΡΠ½ΠΎΠΌΠ΅ΡΠΎΠ² ΠΏΠΎΠ·Π²ΠΎΠ»ΡΠ΅Ρ ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠΈΠ²Π°ΡΡ Π½Π΅ΠΎΠ±Ρ
ΠΎΠ΄ΠΈΠΌΡΠΉ Π·Π°ΠΏΠ°Ρ ΠΌΠ΅ΡΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠΎΡΠ½ΠΎΡΡΠΈ
The Ultimate Fate of Supercooled Liquids
In recent years it has become widely accepted that a dynamical length scale
{\xi}_{\alpha} plays an important role in supercooled liquids near the glass
transition. We examine the implications of the interplay between the growing
{\xi}_{\alpha} and the size of the crystal nucleus, {\xi}_M, which shrinks on
cooling. We argue that at low temperatures where {\xi}_{\alpha} > {\xi}_M a new
crystallization mechanism emerges enabling rapid development of a large scale
web of sparsely connected crystallinity. Though we predict this web percolates
the system at too low a temperature to be easily seen in the laboratory, there
are noticeable residual effects near the glass transition that can account for
several previously observed unexplained phenomena of deeply supercooled liquids
including Fischer clusters, and anomalous crystal growth near T_g
ΠΠ΅Ρ Π°Π½ΠΈΠ·ΠΌΡ ΠΏΡΠΈΠΎΠ±ΡΠ΅ΡΠ΅Π½Π½ΠΎΠΉ ΡΠ΅Π·ΠΈΡΡΠ΅Π½ΡΠ½ΠΎΡΡΠΈ ΠΊ Π°Π½ΡΠΈ-EGFR-ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΠ°ΠΌ ΠΏΡΠΈ Π½Π΅ΠΌΠ΅Π»ΠΊΠΎΠΊΠ»Π΅ΡΠΎΡΠ½ΠΎΠΌ ΡΠ°ΠΊΠ΅ Π»Π΅Π³ΠΊΠΎΠ³ΠΎ, Π½Π΅ ΡΠ²ΡΠ·Π°Π½Π½ΠΎΠΉ Ρ ΠΌΡΡΠ°ΡΠΈΠ΅ΠΉ Π’790Π, ΠΈ ΠΈΡ Π·Π½Π°ΡΠ΅Π½ΠΈΠ΅ Π² ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΏΡΠ°ΠΊΡΠΈΠΊΠ΅
The prospects of treatment strategies for patients with non-small cell lung cancer (NSCLC) featuring the acquired resistance to tyrosine kinase inhibitors, not associated with the Π’790Π mutation, are quite vast from a scientific point of view, but in routine clinical practice they are not yet available in full. Understanding the mechanisms of acquired resistance to tyrosine kinase inhibitors is important for clinicians from the perspective of the possibility of forming more effective options for the second and subsequent treatment of NSCLC. The most studied and frequent mechanism causing the formation of the acquired resistance is the appearance of the Π’790Π mutation in 20 exons of the EGFR gene. This article describes the current understanding of the mechanisms of acquired resistance to tyrosine kinase inhibitors not associated with the mutation of T790M, the evolution of views concerning the treatment of NSCLC, progressing in the course of the treatment by this group of drugs. Taking into account the diversity of unresolved issues and directions of further scientific research, we should not forget about the available research results and the ability to use the described options in routine clinical practice in a proper way.ΠΠ΅ΡΡΠΏΠ΅ΠΊΡΠΈΠ²Ρ Π»Π΅ΡΠ΅Π±Π½ΡΡ
ΡΡΡΠ°ΡΠ΅Π³ΠΈΠΉ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Ρ Π½Π΅ΠΌΠ΅Π»ΠΊΠΎΠΊΠ»Π΅ΡΠΎΡΠ½ΡΠΌ ΡΠ°ΠΊΠΎΠΌ Π»Π΅Π³ΠΊΠΎΠ³ΠΎ (ΠΠΠ Π) ΠΈ Π½Π°Π»ΠΈΡΠΈΠ΅ΠΌ ΠΏΡΠΈΠΎΠ±ΡΠ΅ΡΠ΅Π½Π½ΠΎΠΉ ΡΠ΅Π·ΠΈΡΡΠ΅Π½ΡΠ½ΠΎΡΡΠΈ ΠΊ ΠΈΠ½Π³ΠΈΠ±ΠΈΡΠΎΡΠ°ΠΌ ΡΠΈΡΠΎΠ·ΠΈΠ½ΠΊΠΈΠ½Π°Π·Ρ, Π½Π΅ ΡΠ²ΡΠ·Π°Π½Π½ΠΎΠΉ Ρ ΠΌΡΡΠ°ΡΠΈΠ΅ΠΉ Π’790Π, Ρ Π½Π°ΡΡΠ½ΡΡ
ΠΏΠΎΠ·ΠΈΡΠΈΠΉ Π΄ΠΎΡΡΠ°ΡΠΎΡΠ½ΠΎ ΡΠΈΡΠΎΠΊΠΈ, Π½ΠΎ Π² ΡΡΡΠΈΠ½Π½ΠΎΠΉ ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΏΡΠ°ΠΊΡΠΈΠΊΠ΅ Π² ΠΏΠΎΠ»Π½ΠΎΠΌ ΠΎΠ±ΡΠ΅ΠΌΠ΅ ΠΏΠΎΠΊΠ° Π½Π΅Π΄ΠΎΡΡΡΠΏΠ½Ρ. ΠΠΎΠ½ΠΈΠΌΠ°Π½ΠΈΠ΅ ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΠΎΠ² ΠΏΡΠΈΠΎΠ±ΡΠ΅ΡΠ΅Π½Π½ΠΎΠΉ ΡΠ΅Π·ΠΈΡΡΠ΅Π½ΡΠ½ΠΎΡΡΠΈ ΠΊ ΠΈΠ½Π³ΠΈΠ±ΠΈΡΠΎΡΠ°ΠΌ ΡΠΈΡΠΎΠ·ΠΈΠ½ΠΊΠΈΠ½Π°Π·Ρ Π²Π°ΠΆΠ½ΠΎ Π΄Π»Ρ ΠΊΠ»ΠΈΠ½ΠΈΡΠΈΡΡΠΎΠ² Ρ ΠΏΠΎΠ·ΠΈΡΠΈΠΈ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΠ΅ΠΉ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ Π±ΠΎΠ»Π΅Π΅ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΡΡ
ΠΎΠΏΡΠΈΠΉ 2-ΠΉ ΠΈ ΠΏΠΎΡΠ»Π΅Π΄ΡΡΡΠΈΡ
Π»ΠΈΠ½ΠΈΠΉ ΡΠ΅ΡΠ°ΠΏΠΈΠΈ ΠΠΠ Π. ΠΠ°ΠΈΠ±ΠΎΠ»Π΅Π΅ ΠΈΠ·ΡΡΠ΅Π½Π½ΡΠΌ ΠΈ ΡΠ°ΡΡΡΠΌ ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΠΎΠΌ, ΠΎΠ±ΡΡΠ»ΠΎΠ²Π»ΠΈΠ²Π°ΡΡΠΈΠΌ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΠΏΡΠΈΠΎΠ±ΡΠ΅ΡΠ΅Π½Π½ΠΎΠΉ ΡΠ΅Π·ΠΈΡΡΠ΅Π½ΡΠ½ΠΎΡΡΠΈ, ΡΠ²Π»ΡΠ΅ΡΡΡ Π²ΠΎΠ·Π½ΠΈΠΊΠ½ΠΎΠ²Π΅Π½ΠΈΠ΅ ΠΌΡΡΠ°ΡΠΈΠΈ Π’790Π Π² ΡΠΊΠ·ΠΎΠ½Π΅ 20 Π³Π΅Π½Π° EGFR. Π Π΄Π°Π½Π½ΠΎΠΉ ΡΡΠ°ΡΡΠ΅ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Ρ ΡΠΎΠ²ΡΠ΅ΠΌΠ΅Π½Π½ΡΠ΅ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½ΠΈΡ ΠΎ ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΠ°Ρ
ΠΏΡΠΈΠΎΠ±ΡΠ΅ΡΠ΅Π½Π½ΠΎΠΉ ΡΠ΅Π·ΠΈΡΡΠ΅Π½ΡΠ½ΠΎΡΡΠΈ ΠΊ ΠΈΠ½Π³ΠΈΠ±ΠΈΡΠΎΡΠ°ΠΌ ΡΠΈΡΠΎΠ·ΠΈΠ½ΠΊΠΈΠ½Π°Π·Ρ, Π½Π΅ ΡΠ²ΡΠ·Π°Π½Π½ΠΎΠΉ Ρ ΠΌΡΡΠ°ΡΠΈΠ΅ΠΉ Π’790Π, ΠΊΡΠ°ΡΠΊΠΎ ΠΈΠ·Π»ΠΎΠΆΠ΅Π½Π° ΡΠ²ΠΎΠ»ΡΡΠΈΡ Π²Π·Π³Π»ΡΠ΄ΠΎΠ² Π½Π° Π»Π΅ΡΠ΅Π½ΠΈΠ΅ ΠΠΠ Π, ΠΏΡΠΎΠ³ΡΠ΅ΡΡΠΈΡΡΡΡΠ΅Π³ΠΎ Π½Π° ΡΠΎΠ½Π΅ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΠΎΠ² ΡΡΠΎΠΉ Π³ΡΡΠΏΠΏΡ. ΠΡΠΈΠ½ΠΈΠΌΠ°Ρ Π²ΠΎ Π²Π½ΠΈΠΌΠ°Π½ΠΈΠ΅ ΠΌΠ½ΠΎΠ³ΠΎΠ³ΡΠ°Π½Π½ΠΎΡΡΡ Π½Π΅ΡΠ΅ΡΠ΅Π½Π½ΡΡ
Π²ΠΎΠΏΡΠΎΡΠΎΠ² ΠΈ Π½Π°ΠΏΡΠ°Π²Π»Π΅Π½ΠΈΠΉ Π΄Π°Π»ΡΠ½Π΅ΠΉΡΠΈΡ
Π½Π°ΡΡΠ½ΡΡ
ΠΏΠΎΠΈΡΠΊΠΎΠ², Π½Π΅Π»ΡΠ·Ρ Π·Π°Π±ΡΠ²Π°ΡΡ ΠΎΠ± ΠΈΠΌΠ΅ΡΡΠΈΡ
ΡΡ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ°Ρ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ ΠΈ ΡΠΌΠ΅Π½ΠΈΠΈ Π³ΡΠ°ΠΌΠΎΡΠ½ΠΎΠ³ΠΎ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ ΠΎΠΏΠΈΡΠ°Π½Π½ΡΡ
ΠΎΠΏΡΠΈΠΉ Π² ΡΡΡΠΈΠ½Π½ΠΎΠΉ ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΏΡΠ°ΠΊΡΠΈΠΊΠ΅
Analysis of Protein Markers in Plasma of Patients with Drug Dependence Syndrome: Observational Clinical Study
Background. In drug addiction treatment, the diagnostic process is based on the chemical toxicological determination of the intoxication substrate or its metabolite. Laboratory monitoring and prediction issues that could form the basis of secondary prevention remain unresolved. Specific nervous tissue proteins are considered to be the most promising laboratory markers of drug pathology.Objective β to determine some potential biomarkers of protein-chemical nature in the plasma of patients with drug dependence syndrome.Methods. The study was conducted according to the design of an observational clinical trial at the Narcological Dispensary of Krasnodar Krai in the period from 07.2021 to 07.2022. The main group (group 2) included 31 patients diagnosed with substance dependence syndrome. The control group (group 1, n = 15) consisted of healthy subjects submitted to occupational medical examinations. During the detoxification-stabilization therapy and rehabilitation, 5 proteins were determined in the plasma: brainand glial-derived neurotrophic factors, neuron-specific enolase, alpha-synuclein and calcium-binding protein S100B. Statistical analysis of the data involved the Mann-Whitney test for comparing the values of the control and experimental groups and the Wilcoxon test for comparing the values of one group obtained at different stages of observation. The calculations were carried out using StatPlus version 7 (AnalystSoft Inc., USA).Results. A total of 31 patients were included in the main group, 18 of them were followed up with a diagnosis of opioid dependence syndrome (n = 11) or psychostimulant dependence syndrome (n = 7). Patients dropped out of the study due to their refusal to participate in the study or undergo rehabilitation, or due to relapse of the disease. When admitted to the hospital, patients indicated a 45% decrease in brain-derived neurotrophic factor in the plasma ( p < 0.001), and a 3.9-fold decrease after rehabilitation course ( p < 0.001). Glial-derived neurotrophic factor in the plasma exceeded the controls 1.9 times ( p < 0.001) upon admission to hospital, but rapidly returned to normal values thereafter. Level of neuron-specific enolase in the plasma was also poor, 36% lower than the controls ( p <0.001), but approached the control values by the end of rehabilitation.Conclusion. The study obtained data indicating the changes in neurotrophic factors in the blood plasma of patients with opioid or psychostimulant dependence. The rehabilitation period was marked by a relatively rapid improving level of neurotrophins; however, brain-derived neurotrophic factor remained reduced despite the successful treatment, which may indicate the irreversible changes
Detection of hidden structures for arbitrary scales in complex physical systems
Recent decades have experienced the discovery of numerous complex materials. At the root of the complexity underlying many of these materials lies a large number of contending atomic- and largerscale configurations. In order to obtain a more detailed understanding of such systems, we need tools that enable the detection of pertinent structures on all spatial and temporal scales. Towards this end, we suggest a new method that applies to both static and dynamic systems which invokes ideas from network analysis and information theory. Our approach efficiently identifies basic unit cells, topological defects, and candidate natural structures. The method is particularly useful where a clear definition of order is lacking, and the identified features may constitute a natural point of departure for further analysis
The Shapes of Cooperatively Rearranging Regions in Glass Forming Liquids
The shapes of cooperatively rearranging regions in glassy liquids change from
being compact at low temperatures to fractal or ``stringy'' as the dynamical
crossover temperature from activated to collisional transport is approached
from below. We present a quantitative microscopic treatment of this change of
morphology within the framework of the random first order transition theory of
glasses. We predict a correlation of the ratio of the dynamical crossover
temperature to the laboratory glass transition temperature, and the heat
capacity discontinuity at the glass transition, Delta C_p. The predicted
correlation agrees with experimental results for the 21 materials compiled by
Novikov and Sokolov.Comment: 9 pages, 6 figure
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