37 research outputs found
Density functional theory of freezing for soft interactions in two dimensions
A density functional theory of two-dimensional freezing is presented for a
soft interaction potential that scales as inverse cube of particle distance.
This repulsive potential between parallel, induced dipoles is realized for
paramagnetic colloids on an interface, which are additionally exposed to an
external magnetic field. An extended modified weighted density approximation
which includes correct triplet correlations in the liquid state is used. The
theoretical prediction of the freezing transition is in good agreement with
experimental and simulation data.Comment: 7 pages, 3 figures, submitted 200
Robustness of "cut and splice" genetic algorithms in the structural optimization of atomic clusters
We return to the geometry optimization problem of Lennard-Jones clusters to
analyze the performance dependence of "cut and splice" genetic algorithms (GAs)
on the employed population size. We generally find that admixing twinning
mutation moves leads to an improved robustness of the algorithm efficiency with
respect to this a priori unknown technical parameter. The resulting very stable
performance of the corresponding mutation+mating GA implementation over a wide
range of population sizes is an important feature when addressing unknown
systems with computationally involved first-principles based GA sampling.Comment: 5 pages including 3 figures; related publications can be found at
http://www.fhi-berlin.mpg.de/th/th.htm
Spin Precession and Oscillations in Mesoscopic Systems
We compare and contrast magneto-transport oscillations in the fully quantum
(single-electron coherent) and classical limits for a simple but illustrative
model. In particular, we study the induced magnetization and spin current in a
two-terminal double-barrier structure with an applied Zeeman field between the
barriers and spin disequilibrium in the contacts. Classically, the spin current
shows strong tunneling resonances due to spin precession in the region between
the two barriers. However, these oscillations are distinguishable from those in
the fully coherent case, for which a proper treatment of the electron phase is
required. We explain the differences in terms of the presence or absence of
coherent multiple wave reflections.Comment: 9 pages, 5 figure
Field exposed water in a nanopore: liquid or vapour?
We study the behavior of ambient temperature water under the combined effects
of nanoscale confinement and applied electric field. Using molecular
simulations we analyze the thermodynamic causes of field-induced expansion at
some, and contraction at other conditions. Repulsion among parallel water
dipoles and mild weakening of interactions between partially aligned water
molecules prove sufficient to destabilize the aqueous liquid phase in isobaric
systems in which all water molecules are permanently exposed to a uniform
electric field. At the same time, simulations reveal comparatively weak
field-induced perturbations of water structure upheld by flexible hydrogen
bonding. In open systems with fixed chemical potential, these perturbations do
not suffice to offset attraction of water into the field; additional water is
typically driven from unperturbed bulk phase to the field-exposed region. In
contrast to recent theoretical predictions in the literature, our analysis and
simulations confirm that classical electrostriction characterizes usual
electrowetting behavior in nanoscale channels and nanoporous materials.Comment: 20 pages, 6 figures + T.O.C. figure, in press in PCC
Superparamagnetic colloids in viscous fluids
The influence of a magnetic field on the aggregation process of superparamagnetic colloids has been well known on short time for a few decades. However, the influence of important parameters, such as viscosity of the liquid, has received only little attention. Moreover, the equilibrium state reached after a long time is still challenging on some aspects. Indeed, recent experimental measurements show deviations from pure analytical models in extreme conditions. Furthermore, current simulations would require several years of computing time to reach equilibrium state under those conditions. In the present paper, we show how viscosity influences the characteristic time of the aggregation process, with experimental measurements in agreement with previous theories on transient behaviour. Afterwards, we performed numerical simulations on equivalent systems with lower viscosities. Below a critical value of viscosity, a transition to a new aggregation regime is observed and analysed. We noticed this result can be used to reduce the numerical simulation time from several orders of magnitude, without modifying the intrinsic physical behaviour of the particles. However, it also implies that, for high magnetic fields, granular gases could have a very different behaviour from colloidal liquids
ΠΠ΅ΠΆΠ΄ΡΠ½Π°ΡΠΎΠ΄Π½ΠΎΠ΅ ΡΠΎΡΡΡΠ΄Π½ΠΈΡΠ΅ΡΡΠ²ΠΎ Π Π΅ΡΠΏΡΠ±Π»ΠΈΠΊΠΈ ΠΠ΅Π»Π°ΡΡΡΡ Π² ΡΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΠΈ ΡΡΡΠΎΠΉΡΠΈΠ²ΠΎΠΌΡ ΡΠ°Π·Π²ΠΈΡΠΈΡ ΠΈ ΠΏΡΠΎΠ΄Π²ΠΈΠΆΠ΅Π½ΠΈΠΈ ΠΏΡΠ°Π² ΡΠ΅Π»ΠΎΠ²Π΅ΠΊΠ°
Key words: foreign policy of the Republic of Belarus; international cooperation; the UN; sustainable development; human rights; overcoming of poverty and social inequality. = ΠΠ»ΡΡΠ΅Π²ΡΠ΅ ΡΠ»ΠΎΠ²Π°: Π²Π½Π΅ΡΠ½ΡΡ ΠΏΠΎΠ»ΠΈΡΠΈΠΊΠ° Π Π΅ΡΠΏΡΠ±Π»ΠΈΠΊΠΈ ΠΠ΅Π»Π°ΡΡΡΡ; ΠΌΠ΅ΠΆΠ΄ΡΠ½Π°ΡΠΎΠ΄Π½ΠΎΠ΅ ΡΠΎΡΡΡΠ΄Π½ΠΈΡΠ΅ΡΡΠ²ΠΎ; ΠΠΠ; ΡΡΡΠΎΠΉΡΠΈΠ²ΠΎΠ΅ ΡΠ°Π·Π²ΠΈΡΠΈΠ΅; ΠΏΡΠ°Π²Π° ΡΠ΅Π»ΠΎΠ²Π΅ΠΊΠ°; ΠΏΡΠ΅ΠΎΠ΄ΠΎΠ»Π΅Π½ΠΈΠ΅ Π±Π΅Π΄Π½ΠΎΡΡΠΈ ΠΈ ΡΠΎΡΠΈΠ°Π»ΡΠ½ΠΎΠ³ΠΎ Π½Π΅ΡΠ°Π²Π΅Π½ΡΡΠ²Π°.Promotion of human rights, progress in the sustainable development and overcoming of different forms of poverty on the national, regional and global level is one of the most important directions of the multilateral diplomacy of the Re-public of Belarus since its independence in 1991. Based on an international experience of the Belarusian SSR as one of the United Nations founders in its main bodies, primarily the Economic and Social Council (ECOSOC), as well as its special institutions, the Belarusian diplomacy has already established mutually beneficial and effective cooperation with other countries in many important issues. Among them, there are such key and acute topics as a fighting against poverty and unequal access to social benefits and achievements, as well as overcoming regional and structural imparities for different social groups and communities.
This comprehensive dialogue with our leading international partners including a special role of our partnership with China continued and developed successfully in the early 21st century. It allowed the Republic of Belarus to contribute to the modern understanding of human rights in the context of global sustainable development. Achieving its Goals (SDGs) until 2030, agreed by all UN members is one of the most important aspects and challenges for the policy of the Republic of Belarus and for its primary vision of the promotion of human rights issues in the global world.
Our understanding of them is based on their universal, indivisible, interrelated, interdependent and complementary nature. To ensure each of their most important categories: civil, political, economic, social, cultural it should be adhere to the same positions and attitudes with equal attention. International cooperation in this sphere is to be aimed at strengthening mutual trust and developing effective multilateral mechanisms to solve the most important global problems.
The Republic of Belarus opposes consistently and resolutely any attempts to politicize them and calls for a comprehensive approach to the protection of all categories of human rights and liberties in the framework of international cooperation with-out prioritizing or minimizing them.ΠΡΠΎΠ΄Π²ΠΈΠΆΠ΅Π½ΠΈΠ΅ ΠΏΡΠ°Π² ΡΠ΅Π»ΠΎΠ²Π΅ΠΊΠ°, ΠΏΡΠΎΠ³ΡΠ΅ΡΡ Π² ΠΎΠ±Π»Π°ΡΡΠΈ ΡΡΡΠΎΠΉΡΠΈΠ²ΠΎΠ³ΠΎ ΡΠ°Π·Π²ΠΈΡΠΈΡ ΠΈ ΠΏΡΠ΅ΠΎΠ΄ΠΎΠ»Π΅Π½ΠΈΠ΅ ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
ΡΠΎΡΠΌ Π±Π΅Π΄Π½ΠΎΡΡΠΈ Π½Π° Π½Π°ΡΠΈΠΎΠ½Π°Π»ΡΠ½ΠΎΠΌ, ΡΠ΅Π³ΠΈΠΎΠ½Π°Π»ΡΠ½ΠΎΠΌ ΠΈ Π³Π»ΠΎΠ±Π°Π»ΡΠ½ΠΎΠΌ ΡΡΠΎΠ²Π½ΡΡ
ΡΠ²Π»ΡΡΡΡΡ ΠΎΠ΄Π½ΠΈΠΌ ΠΈΠ· Π²Π°ΠΆΠ½Π΅ΠΉΡΠΈΡ
Π½Π°ΠΏΡΠ°Π²Π»Π΅Π½ΠΈΠΉ ΠΌΠ½ΠΎΠ³ΠΎΡΡΠΎΡΠΎΠ½Π½Π΅ΠΉ Π΄ΠΈΠΏΠ»ΠΎΠΌΠ°ΡΠΈΠΈ Π Π΅ΡΠΏΡΠ±Π»ΠΈΠΊΠΈ ΠΠ΅Π»Π°ΡΡΡΡ Ρ ΠΌΠΎΠΌΠ΅Π½ΡΠ° ΠΎΠ±ΡΠ΅ΡΠ΅Π½ΠΈΡ Π½Π΅Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ Π² 1991 Π³. ΠΠΏΠΈΡΠ°ΡΡΡ Π½Π° ΠΌΠ΅ΠΆΠ΄ΡΠ½Π°ΡΠΎΠ΄Π½ΡΠΉ ΠΎΠΏΡΡ ΠΠ΅Π»ΠΎΡΡΡΡΠΊΠΎΠΉ Π‘Π‘Π ΠΊΠ°ΠΊ ΠΎΠ΄Π½ΠΎΠ³ΠΎ ΠΈΠ· ΠΎΡΠ½ΠΎΠ²Π°ΡΠ΅Π»Π΅ΠΉ ΠΠΠ, ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΠΉ Π² ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ΅ ΡΠ°Π±ΠΎΡΡ Π² Π΅Π΅ ΠΎΡΠ½ΠΎΠ²Π½ΡΡ
ΠΎΡΠ³Π°Π½Π°Ρ
, ΠΏΡΠ΅ΠΆΠ΄Π΅ Π²ΡΠ΅Π³ΠΎ ΠΠΊΠΎΠ½ΠΎΠΌΠΈΡΠ΅ΡΠΊΠΎΠΌ ΠΈ ΡΠΎΡΠΈΠ°Π»ΡΠ½ΠΎΠΌ ΡΠΎΠ²Π΅ΡΠ΅, Π° ΡΠ°ΠΊΠΆΠ΅ ΡΠΏΠ΅ΡΠΈΠ°Π»ΡΠ½ΡΡ
ΡΡΡΠ΅ΠΆΠ΄Π΅Π½ΠΈΡΡ
, Π±Π΅Π»ΠΎΡΡΡΡΠΊΠ°Ρ Π΄ΠΈΠΏΠ»ΠΎΠΌΠ°ΡΠΈΡ Π½Π°Π»Π°Π΄ΠΈΠ»Π° Π²Π·Π°ΠΈΠΌΠΎΠ²ΡΠ³ΠΎΠ΄Π½ΠΎΠ΅ ΠΈ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΠ΅ ΡΠΎΡΡΡΠ΄Π½ΠΈΡΠ΅ΡΡΠ²ΠΎ Ρ Π΄ΡΡΠ³ΠΈΠΌΠΈ ΡΡΡΠ°Π½Π°ΠΌΠΈ Π² ΡΠ΅ΡΠ΅Π½ΠΈΠΈ ΠΌΠ½ΠΎΠ³ΠΈΡ
Π²Π°ΠΆΠ½ΡΡ
ΠΏΡΠΎΠ±Π»Π΅ΠΌ. Π‘ΡΠ΅Π΄ΠΈ Π½ΠΈΡ
ΡΠ°ΠΊΠΈΠ΅ ΠΊΠ»ΡΡΠ΅Π²ΡΠ΅ ΠΈ Π·Π»ΠΎΠ±ΠΎΠ΄Π½Π΅Π²Π½ΡΠ΅ ΡΠ΅ΠΌΡ, ΠΊΠ°ΠΊ Π±ΠΎΡΡΠ±Π° Ρ Π±Π΅Π΄Π½ΠΎΡΡΡΡ ΠΈ Π½Π΅ΡΠ°Π²Π½ΡΠΌ Π΄ΠΎΡΡΡΠΏΠΎΠΌ ΠΊ ΡΠΎΡΠΈΠ°Π»ΡΠ½ΡΠΌ Π±Π»Π°Π³Π°ΠΌ ΠΈ Π΄ΠΎΡΡΠΈΠΆΠ΅Π½ΠΈΡΠΌ, Π° ΡΠ°ΠΊΠΆΠ΅ ΠΏΡΠ΅ΠΎΠ΄ΠΎΠ»Π΅Π½ΠΈΠ΅ ΡΠ΅Π³ΠΈΠΎΠ½Π°Π»ΡΠ½ΠΎΠ³ΠΎ ΠΈ ΡΡΡΡΠΊΡΡΡΠ½ΠΎΠ³ΠΎ Π½Π΅ΡΠ°Π²Π΅Π½ΡΡΠ²Π° ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
ΡΠΎΡΠΈΠ°Π»ΡΠ½ΡΡ
Π³ΡΡΠΏΠΏ ΠΈ ΠΎΠ±ΡΠ½ΠΎΡΡΠ΅ΠΉ.
ΠΡΠ΅ΡΡΠΎΡΠΎΠ½Π½ΠΈΠΉ Π΄ΠΈΠ°Π»ΠΎΠ³ Ρ Π½Π°ΡΠΈΠΌΠΈ Π²Π΅Π΄ΡΡΠΈΠΌΠΈ ΠΌΠ΅ΠΆΠ΄ΡΠ½Π°ΡΠΎΠ΄Π½ΡΠΌΠΈ ΠΏΠ°ΡΡΠ½Π΅ΡΠ°ΠΌΠΈ, Π²ΠΊΠ»ΡΡΠ°Ρ ΠΎΡΠΎΠ±ΡΡ ΡΠΎΠ»Ρ ΡΠΎΡΡΡΠ΄Π½ΠΈΡΠ΅ΡΡΠ²Π° Ρ ΠΠΈΡΠ°Π΅ΠΌ, ΠΏΡΠΎΠ΄ΠΎΠ»ΠΆΠ°Π»ΡΡ ΠΈ ΡΡΠΏΠ΅ΡΠ½ΠΎ ΡΠ°Π·Π²ΠΈΠ²Π°Π»ΡΡ Π² Π½Π°ΡΠ°Π»Π΅ XXI Π². ΠΡΠΎ ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΠ»ΠΎ Π Π΅ΡΠΏΡΠ±Π»ΠΈΠΊΠ΅ ΠΠ΅Π»Π°ΡΡΡΡ Π²Π½Π΅ΡΡΠΈ ΡΠ²ΠΎΠΉ Π²ΠΊΠ»Π°Π΄ Π² ΡΠΎΠ²ΡΠ΅ΠΌΠ΅Π½Π½ΠΎΠ΅ ΠΏΠΎΠ½ΠΈΠΌΠ°Π½ΠΈΠ΅ ΠΏΡΠ°Π² ΡΠ΅Π»ΠΎΠ²Π΅ΠΊΠ° Π² ΠΊΠΎΠ½ΡΠ΅ΠΊΡΡΠ΅ Π³Π»ΠΎΠ±Π°Π»ΡΠ½ΠΎΠ³ΠΎ ΡΡΡΠΎΠΉΡΠΈΠ²ΠΎΠ³ΠΎ ΡΠ°Π·Π²ΠΈΡΠΈΡ. ΠΠΎΡΡΠΈΠΆΠ΅Π½ΠΈΠ΅ Π΅Π³ΠΎ ΡΠ΅Π»Π΅ΠΉ (Π¦Π£Π ) Π΄ΠΎ 2030 Π³., ΡΠΎΠ³Π»Π°ΡΠΎΠ²Π°Π½Π½ΠΎΠ΅ Π²ΡΠ΅ΠΌΠΈ ΡΠ»Π΅Π½Π°ΠΌΠΈ ΠΠΠ, ΡΠ²Π»ΡΠ΅ΡΡΡ ΠΎΠ΄Π½ΠΎΠΉ ΠΈΠ· Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ Π²Π°ΠΆΠ½ΡΡ
Π·Π°Π΄Π°Ρ Π΄Π»Ρ ΠΏΠΎΠ»ΠΈΡΠΈΠΊΠΈ Π Π΅ΡΠΏΡΠ±Π»ΠΈΠΊΠΈ ΠΠ΅Π»Π°ΡΡΡΡ ΠΈ Π΅Π΅ ΠΎΡΠ½ΠΎΠ²ΠΎΠΏΠΎΠ»Π°Π³Π°ΡΡΠ΅Π³ΠΎ Π²ΠΈΠ΄Π΅Π½ΠΈΡ ΠΏΡΠΎΠ΄Π²ΠΈΠΆΠ΅Π½ΠΈΡ ΠΏΡΠ°Π² ΡΠ΅Π»ΠΎΠ²Π΅ΠΊΠ° Π² Π³Π»ΠΎΠ±Π°Π»ΡΠ½ΠΎΠΌ ΠΌΠΈΡΠ΅.
ΠΠ°ΡΠ΅ ΠΈΡ
ΠΏΠΎΠ½ΠΈΠΌΠ°Π½ΠΈΠ΅ ΠΎΡΠ½ΠΎΠ²ΡΠ²Π°Π΅ΡΡΡ Π½Π° ΡΠ½ΠΈΠ²Π΅ΡΡΠ°Π»ΡΠ½ΠΎΠΌ, Π½Π΅Π΄Π΅Π»ΠΈΠΌΠΎΠΌ, Π²Π·Π°ΠΈΠΌΠΎΡΠ²ΡΠ·Π°Π½Π½ΠΎΠΌ, Π²Π·Π°ΠΈΠΌΠΎΠ·Π°Π²ΠΈΡΠΈΠΌΠΎΠΌ ΠΈ Π²Π·Π°ΠΈΠΌΠΎΠ΄ΠΎΠΏΠΎΠ»Π½ΡΡΡΠ΅ΠΌ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠ΅. Π Π΄Π΅Π»Π΅ ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠ΅Π½ΠΈΡ ΠΊΠ°ΠΆΠ΄ΠΎΠΉ ΠΈΠ· Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ Π²Π°ΠΆΠ½ΡΡ
ΠΊΠ°ΡΠ΅Π³ΠΎΡΠΈΠΉ ΠΏΡΠ°Π² ΡΠ΅Π»ΠΎΠ²Π΅ΠΊΠ°: Π³ΡΠ°ΠΆΠ΄Π°Π½ΡΠΊΠΈΡ
, ΠΏΠΎΠ»ΠΈΡΠΈΡΠ΅ΡΠΊΠΈΡ
, ΡΠΊΠΎΠ½ΠΎΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
, ΡΠΎΡΠΈΠ°Π»ΡΠ½ΡΡ
, ΠΊΡΠ»ΡΡΡΡΠ½ΡΡ
ΡΠ»Π΅Π΄ΡΠ΅Ρ ΠΏΡΠΈΠ΄Π΅ΡΠΆΠΈΠ²Π°ΡΡΡΡ ΠΎΠ΄ΠΈΠ½Π°ΠΊΠΎΠ²ΡΡ
ΠΏΠΎΠ·ΠΈΡΠΈΠΉ ΠΈ ΠΎΡΠ½ΠΎΡΠΈΡΡΡΡ ΠΊ Π½ΠΈΠΌ Ρ ΡΠ°Π²Π½ΡΠΌ Π²Π½ΠΈΠΌΠ°Π½ΠΈΠ΅ΠΌ. ΠΠ΅ΠΆΠ΄ΡΠ½Π°ΡΠΎΠ΄Π½ΠΎΠ΅ ΡΠΎΡΡΡΠ΄Π½ΠΈΡΠ΅ΡΡΠ²ΠΎ Π² ΡΡΠΎΠΉ ΡΡΠ΅ΡΠ΅ Π΄ΠΎΠ»ΠΆΠ½ΠΎ Π±ΡΡΡ Π½Π°ΠΏΡΠ°Π²Π»Π΅Π½ΠΎ Π½Π° ΡΠΊΡΠ΅ΠΏΠ»Π΅Π½ΠΈΠ΅ Π²Π·Π°ΠΈΠΌΠ½ΠΎΠ³ΠΎ Π΄ΠΎΠ²Π΅ΡΠΈΡ ΠΈ ΡΠ°Π·ΡΠ°Π±ΠΎΡΠΊΡ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΡΡ
ΠΌΠ½ΠΎΠ³ΠΎΡΡΠΎΡΠΎΠ½Π½ΠΈΡ
ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΠΎΠ² Π΄Π»Ρ ΡΠ΅ΡΠ΅Π½ΠΈΡ Π²Π°ΠΆΠ½Π΅ΠΉΡΠΈΡ
Π³Π»ΠΎΠ±Π°Π»ΡΠ½ΡΡ
ΠΏΡΠΎΠ±Π»Π΅ΠΌ.
Π Π΅ΡΠΏΡΠ±Π»ΠΈΠΊΠ° ΠΠ΅Π»Π°ΡΡΡΡ ΠΏΠΎΡΠ»Π΅Π΄ΠΎΠ²Π°ΡΠ΅Π»ΡΠ½ΠΎ ΠΈ ΡΠ΅ΡΠΈΡΠ΅Π»ΡΠ½ΠΎ Π²ΡΡΡΡΠΏΠ°Π΅Ρ ΠΏΡΠΎΡΠΈΠ² Π»ΡΠ±ΡΡ
ΠΏΠΎΠΏΡΡΠΎΠΊ ΠΈΡ
ΠΏΠΎΠ»ΠΈΡΠΈΠ·Π°ΡΠΈΠΈ ΠΈ ΠΏΡΠΈΠ·ΡΠ²Π°Π΅Ρ ΠΊ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ½ΠΎΠΌΡ ΠΏΠΎΠ΄Ρ
ΠΎΠ΄Ρ ΠΊ ΡΠΎΠ±Π»ΡΠ΄Π΅Π½ΠΈΡ Π²ΡΠ΅Ρ
ΠΊΠ°ΡΠ΅Π³ΠΎΡΠΈΠΉ ΠΏΡΠ°Π² ΠΈ ΡΠ²ΠΎΠ±ΠΎΠ΄ ΡΠ΅Π»ΠΎΠ²Π΅ΠΊΠ° Π² ΡΠ°ΠΌΠΊΠ°Ρ
ΠΌΠ΅ΠΆΠ΄ΡΠ½Π°ΡΠΎΠ΄Π½ΠΎΠ³ΠΎ ΡΠΎΡΡΡΠ΄Π½ΠΈΡΠ΅ΡΡΠ²Π°, Π½Π΅ ΠΏΡΡΠ°ΡΡΡ Π²ΡΠ΄Π΅Π»ΠΈΡΡ ΡΡΠ΅Π΄ΠΈ Π½ΠΈΡ
ΠΏΡΠΈΠΎΡΠΈΡΠ΅ΡΠ½ΡΠ΅ ΠΈΠ»ΠΈ ΡΠ²Π΅ΡΡΠΈ ΠΈΡ
ΠΊ ΠΌΠΈΠ½ΠΈΠΌΡΠΌΡ