778 research outputs found
Analysis of network by generalized mutual entropies
Generalized mutual entropy is defined for networks and applied for analysis
of complex network structures. The method is tested for the case of computer
simulated scale free networks, random networks, and their mixtures. The
possible applications for real network analysis are discussed
IMIGE TYPOLOGIES IN COGNITION PROCESS
ΠΠ° ΠΏΡΠΈΠΌΠ΅ΡΠ΅ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠ°ΡΠ½ΡΡ
ΡΡΠ΅Π΅ΠΊ ΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ΅ΡΠ΅ΡΠΎΠΊ, ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠ΅ΠΉ Π€Π΅ΡΠΌΠΈ ΠΌΠ΅ΡΠ°Π»Π»ΠΎΠ² ΠΈ Π°Π΄ΠΈΠ°Π±Π°ΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠΎΡΠ΅Π½ΡΠΈΠ°Π»ΠΎΠ² ΠΏΡΠΈΠΌΠ΅ΡΠ΅ΠΉ Π·Π°ΠΌΠ΅ΡΠ΅Π½ΠΈΡ Π² ΠΊΡΠΈΡΡΠ°Π»Π»Π°Ρ
ΡΠ°ΡΡΠΌΠ°ΡΡΠΈΠ²Π°Π΅ΡΡΡ ΠΏΠΎΡΡΡΠΎΠ΅Π½ΠΈΠ΅ ΡΠΈΠΏΠΎΠ»ΠΎΠ³ΠΈΠΉ, ΠΎΡΠ½ΠΎΠ²Π°Π½Π½ΡΡ
Π½Π° Π²ΠΈΠ·ΡΠ°Π»ΡΠ½ΡΡ
ΠΎΠ±ΡΠ°Π·Π°Ρ
Construction of typologies based on visual images is discussed using elementary cells of crystals, Fermi surfaces of metals and adiabatic potential energies of substitution impurities as the example
On possibility of application of the Jahn-Teller complexes in quantum computers
At present time quantum dots in semiconductors which are characterized by electric charge or spin orientation, Cooper pairs in superconductors and electron states in ions are considered as the element basis for construction of quantum register (logical q-bits). In the present report, the Jahn-Teller complexes formed by impurities in crystals are suggested to use as elements of information storageΠ Π½Π°ΡΡΠΎΡΡΠ΅Π΅ Π²ΡΠ΅ΠΌΡ Π² ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠ½ΠΎΠΉ Π±Π°Π·Ρ Π΄Π»Ρ ΠΏΠΎΡΡΡΠΎΠ΅Π½ΠΈΡ ΠΊΠ²Π°Π½ΡΠΎΠ²ΠΎΠ³ΠΎ ΡΠ΅Π³ΠΈΡΡΡΠ° (Π»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΊΡΠ±ΠΈΡΠΎΠ²) ΡΠ°ΡΡΠΌΠ°ΡΡΠΈΠ²Π°ΡΡΡΡ ΠΊΠ²Π°Π½ΡΠΎΠ²ΡΠ΅ ΡΠΎΡΠΊΠΈ Π² ΠΏΠΎΠ»ΡΠΏΡΠΎΠ²ΠΎΠ΄Π½ΠΈΠΊΠ°Ρ
, Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΠ·ΡΠ΅ΠΌΡΠ΅ Π·Π°ΡΡΠ΄ΠΎΠ²ΡΠΌ ΠΈΠ»ΠΈ ΡΠΏΠΈΠ½ΠΎΠ²ΡΠΌ ΡΠΎΡΡΠΎΡΠ½ΠΈΡΠΌΠΈ, ΠΊΡΠΏΠ΅ΡΠΎΠ²ΡΠΊΠΈΠ΅ ΠΏΠ°ΡΡ Π² ΡΠ²Π΅ΡΡ
ΠΏΡΠΎΠ²ΠΎΠ΄Π½ΠΈΠΊΠ°Ρ
, ΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΡΠ΅ ΡΠΎΡΡΠΎΡΠ½ΠΈΡ Π² ΠΈΠΎΠ½Π°Ρ
. Π Π΄Π°Π½Π½ΠΎΠΌ ΡΠΎΠΎΠ±ΡΠ΅Π½ΠΈΠΈ ΠΏΡΠ΅Π΄Π»Π°Π³Π°Π΅ΡΡΡ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°ΡΡ Π² ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ² Π½ΠΎΡΠΈΡΠ΅Π»Π΅ΠΉ ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΠΈ ΡΠ½-ΡΠ΅Π»Π»Π΅ΡΠΎΠ²ΡΠΊΠΈΠ΅ ΡΠ΅Π½ΡΡΡ, ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½Π½ΡΠ΅ ΠΏΡΠΈΠΌΠ΅ΡΡΠΌΠΈ Π² ΠΊΡΠΈΡΡΠ°Π»Π»Π°
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