1,484 research outputs found

    Composite Dark Matter and Puzzles of Dark Matter Searches

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    Positive results of dark matter searches in DAMA/NaI and DAMA/LIBRA experiments, being put together with the results of other groups, can imply nontrivial particle physics solutions for cosmological dark matter. Stable particles with charge -2, bound with primordial helium in O-helium "atoms" (OHe), represent a specific Warmer than Cold nuclear-interacting form of dark matter. Slowed down in the terrestrial matter, OHe is elusive for direct methods of underground Dark matter detection used in cryogenic experiments. However radiative capture of OHe by Na and I nuclei can lead to annual variations of energy release in the interval of energy 2-5 keV in DAMA/NaI and DAMA/LIBRA experiments.Comment: 10 pages, 2 figures, Invited contribution to proceeding of the 4th International Workshop on Astronomy and Relativistic Astrophysics (IWARA09

    Student Recital

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    Internet as a factor in the developnet of extremism in the youth environment

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    Π‘Ρ‚Π°Ρ‚ΡŒΡ посвящСна ΠΈΠ·ΡƒΡ‡Π΅Π½ΠΈΡŽ Π˜Π½Ρ‚Π΅Ρ€Π½Π΅Ρ‚Π° ΠΊΠ°ΠΊ Ρ„Π°ΠΊΡ‚ΠΎΡ€Π°, Π²Π»ΠΈΡΡŽΡ‰Π΅Π³ΠΎ Π½Π° Ρ€Π°Π·Π²ΠΈΡ‚ΠΈΠ΅ экстрСмизма. На основС Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΎΠ² эмпиричСского исслСдования Π°Π²Ρ‚ΠΎΡ€ ΠΏΡ€ΠΈΡ…ΠΎΠ΄ΠΈΡ‚ ΠΊ Π²Ρ‹Π²ΠΎΠ΄Ρƒ, Ρ‡Ρ‚ΠΎ ΡΠΎΡ†ΠΈΠ°Π»ΡŒΠ½Π°Ρ ΡΠ΅Ρ‚ΡŒ Π’ΠšΠΎΠ½Ρ‚Π°ΠΊΡ‚Π΅ являСтся самой часто ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΡƒΠ΅ΠΌΠΎΠΉ ΠΏΠ»ΠΎΡ‰Π°Π΄ΠΊΠΎΠΉ для воздСйствия экстрСмистов Π½Π° молодСТь.The article considers the Internet as the factor which influence on developing of extremism. Based on the results of empirical research the author concludes that a social network as VKontakte is frequently used for exstremist’s influence on the youth

    Conductance of p-n-p graphene structures with 'air-bridge' top gates

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    We have fabricated graphene devices with a top gate separated from the graphene layer by an air gap--a design which does not decrease the mobility of charge carriers under the gate. This gate is used to realise p-n-p structures where the conducting properties of chiral carriers are studied. The band profile of the structures is calculated taking into account the specifics of the graphene density of states and is used to find the resistance of the p-n junctions expected for chiral carriers. We show that ballistic p-n junctions have larger resistance than diffusive ones. This is caused by suppressed transmission of chiral carriers at angles away from the normal to the junction.Comment: to be published in Nano Letter

    Weak localisation in bilayer graphene

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    We have performed the first experimental investigation of quantum interference corrections to the conductivity of a bilayer graphene structure. A negative magnetoresistance - a signature of weak localisation - is observed at different carrier densities, including the electro-neutrality region. It is very different, however, from the weak localisation in conventional two-dimensional systems. We show that it is controlled not only by the dephasing time, but also by different elastic processes that break the effective time-reversal symmetry and provide invervalley scattering.Comment: 4 pages, 4 figures (to be published in PRL

    Density of states and zero Landau level probed through capacitance of graphene

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    We report capacitors in which a finite electronic compressibility of graphene dominates the electrostatics, resulting in pronounced changes in capacitance as a function of magnetic field and carrier concentration. The capacitance measurements have allowed us to accurately map the density of states D, and compare it against theoretical predictions. Landau oscillations in D are robust and zero Landau level (LL) can easily be seen at room temperature in moderate fields. The broadening of LLs is strongly affected by charge inhomogeneity that leads to zero LL being broader than other levels

    Бвойства гармоничСских ΠΈ составных ΠΏΠΎΠ»ΡƒΠ²ΠΎΠ»Π½, ΠΎΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ ΠΈΠ½Ρ‚Π΅Ρ€Π²Π°Π»Π° Ρ€Π°Π²Π½ΠΎΠΌΠ΅Ρ€Π½ΠΎΠΉ дискрСтизации Π²Ρ€Π΅ΠΌΠ΅Π½ΠΈ Ρ†ΠΈΡ„Ρ€ΠΎΠ²Ρ‹Ρ… ΡΠΈΠ³Π½Π°Π»ΡŒΠ½Ρ‹Ρ… процСссоров

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    ΠŸΡ€ΠΈ построСнии Π°Π²Ρ‚ΠΎΠ½ΠΎΠΌΠ½Ρ‹Ρ… систСм Ρ€Π΅Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ Π²Ρ€Π΅ΠΌΠ΅Π½ΠΈ (Π‘Π Π’) Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΠΎ Ρ€Π΅ΡˆΠ°Ρ‚ΡŒ Π·Π°Π΄Π°Ρ‡Ρƒ ΠΎΠΏΡ‚ΠΈΠΌΠ°Π»ΡŒΠ½ΠΎΠΉ ΠΌΠ½ΠΎΠ³ΠΎΠ·Π°Π΄Π°Ρ‡Π½ΠΎΠΉ Π·Π°Π³Ρ€ΡƒΠ·ΠΊΠΈ ряда ΠΏΠ°Ρ€Π°Π»Π»Π΅Π»ΡŒΠ½ΠΎ Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΎΠ½ΠΈΡ€ΡƒΡŽΡ‰ΠΈΡ… Ρ†ΠΈΡ„Ρ€ΠΎΠ²Ρ‹Ρ… ΡΠΈΠ³Π½Π°Π»ΡŒΠ½Ρ‹Ρ… процСссоров. Одним ΠΈΠ· Ρ€Π΅Π·Π΅Ρ€Π²ΠΎΠ² достиТСния Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΠΎΠ³ΠΎ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π° выступаСт рСализация Π²Ρ‹Π±ΠΎΡ€ΠΎΠΊ ΠΈΠ· сигналов Π΄Π°Ρ‚Ρ‡ΠΈΠΊΠΎΠ² ΠΈΠ½Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΈ ΠΎ Π²Π΅Π»ΠΈΡ‡ΠΈΠ½Π΅ сигнала Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ Ρ€Π΅Π΄ΠΊΠΎ Π²ΠΎ Π²Ρ€Π΅ΠΌΠ΅Π½ΠΈ. ΠŸΡ€ΠΈ этом Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΠΎ ΠΎΠ±Π΅ΡΠΏΠ΅Ρ‡ΠΈΠ²Π°Ρ‚ΡŒ Π»ΠΈΠ½Π΅ΠΉΠ½ΡƒΡŽ ΠΈΠ»ΠΈ ΡΡ‚ΡƒΠΏΠ΅Π½Ρ‡Π°Ρ‚ΡƒΡŽ Π°ΠΏΠΏΡ€ΠΎΠΊΡΠΈΠΌΠ°Ρ†ΠΈΡŽ сигнала ΠΏΠΎ Π²Ρ‹Π±ΠΎΡ€ΠΊΠ°ΠΌ с допустимой ΠΏΠΎΠ³Ρ€Π΅ΡˆΠ½ΠΎΡΡ‚ΡŒΡŽ восстановлСния. Одной ΠΈΠ· систСмных Π·Π°Π΄Π°Ρ‡ этих процСссоров являСтся Ρ„ΠΈΠ»ΡŒΡ‚Ρ€Π°Ρ†ΠΈΡ сигналов ΠΈΠ»ΠΈ ΠΎΠ³Ρ€Π°Π½ΠΈΡ‡Π΅Π½ΠΈΠ΅ спСктра Π΄ΠΎ частоты срСза. ΠžΡ‚Π»ΠΈΡ‡ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠΉ ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡ‚ΡŒΡŽ ΠΏΡ€Π΅Π΄Π»Π°Π³Π°Π΅ΠΌΠΎΠ³ΠΎ Π² ΡΡ‚Π°Ρ‚ΡŒΠ΅ ΠΏΠΎΠ΄Ρ…ΠΎΠ΄Π° являСтся Π²Ρ‹ΠΏΠΎΠ»Π½Π΅Π½ΠΈΠ΅ условия: Ссли ΠΈΠ·ΠΌΠ΅Ρ€Π΅Π½ΠΈΠ΅ этой частоты Π·Π°Ρ‚Ρ€ΡƒΠ΄Π½Π΅Π½ΠΎ (Π½Π°ΠΏΡ€ΠΈΠΌΠ΅Ρ€, Π² элСктромСханичСских срСдствах Π‘Π Π’), Ρ‚ΠΎ для Ρ‚Π°ΠΊΠΈΡ… сигналов ΠΏΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½ΠΎ ΡΠΎΠ³Π»Π°ΡΠΎΠ²Ρ‹Π²Π°Ρ‚ΡŒ ΠΌΠ°ΠΊΡΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹Π΅ Π²Π΅Π»ΠΈΡ‡ΠΈΠ½Ρ‹ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ² гармоничСской ΠΏΠΎΠ»ΡƒΠ²ΠΎΠ»Π½Ρ‹: ΠΏΠΎΠ³Ρ€Π΅ΡˆΠ½ΠΎΡΡ‚ΡŒ аппроксимации, ΡΠΊΠΎΡ€ΠΎΡΡ‚ΡŒ ΠΈ ускорСниС. ИсслСдованиС ΠΎΡ‚ΠΊΡ€Ρ‹Π²Π°Π΅Ρ‚ пСрспСктиву примСнСния Π½ΠΎΠ²Ρ‹Ρ… ΠΏΠΎΠ΄Ρ…ΠΎΠ΄ΠΎΠ² ΠΏΠΎ дискрСтизации Π²Ρ€Π΅ΠΌΠ΅Π½ΠΈ сигналов Π² Π°ΠΌΠΏΠ»ΠΈΡ‚ΡƒΠ΄Π½ΠΎ-Π²Ρ€Π΅ΠΌΠ΅Π½Π½ΠΎΠΉ области ΠΈ ΠΎΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ для Ρ‚Π°ΠΊΠΈΡ… сигналов эквивалСнтной частоты срСза спСктра сигнала. Π’ настоящСй ΡΡ‚Π°Ρ‚ΡŒΠ΅ ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Ρ‹ зависимости Π²Π΅Π»ΠΈΡ‡ΠΈΠ½Ρ‹ Π΅Π΄ΠΈΠ½ΠΈΡ†Ρ‹ систСмного Π²Ρ€Π΅ΠΌΠ΅Π½ΠΈ Π²Π²ΠΎΠ΄Π°-Π²Ρ‹Π²ΠΎΠ΄Π° Π΄Π°Π½Π½Ρ‹Ρ… ΠΎΡ‚ стСпСни согласования ΠΌΠ΅ΠΆΠ΄Ρƒ собой ΠΌΠ°ΠΊΡΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹Ρ… Π²Π΅Π»ΠΈΡ‡ΠΈΠ½ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ² сигнала. ΠœΠ°Ρ‚Π΅ΠΌΠ°Ρ‚ΠΈΡ‡Π΅ΡΠΊΠ°Ρ модСль ΡΠΊΡΡ‚Ρ€Π΅ΠΌΠ°Π»ΡŒΠ½ΠΎΠ³ΠΎ повСдСния сигнала ΠΌΠ΅ΠΆΠ΄Ρƒ двумя сосСдними Π²Ρ‹Π±ΠΎΡ€ΠΊΠ°ΠΌΠΈ Π·Π°Π΄Π°Π½Π° Π² Π²ΠΈΠ΄Π΅ гармоничСской ΠΏΠΎΠ»ΡƒΠ²ΠΎΠ»Π½Ρ‹. ИсслСдованиС распространСно Ρ‚Π°ΠΊΠΆΠ΅ Π½Π° Π²Ρ‹ΠΏΡƒΠΊΠ»Ρ‹Π΅ составныС гармоничСскиС Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΈ, ΠΏΠΎ ΠΊΠΎΡ‚ΠΎΡ€Ρ‹ΠΌ сигнал ΠΌΠΎΠΆΠ΅Ρ‚ ΠΎΡ‚ΠΊΠ»ΠΎΠ½ΡΡ‚ΡŒΡΡ ΠΎΡ‚ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΎΠ² Π»ΠΈΠ½Π΅ΠΉΠ½ΠΎΠΉ ΠΈΠ»ΠΈ ступСнчатой аппроксимации сигнала ΠΏΠΎ этим Π²Ρ‹Π±ΠΎΡ€ΠΊΠ°ΠΌ. ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½ΠΎ сравнСниС ΠΌΠΎΠ΄Π΅Π»Π΅ΠΉ ΠΏΠΎ Π²Π΅Π»ΠΈΡ‡ΠΈΠ½Π΅ ΠΎΡ‚Π½ΠΎΡΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… ΠΈΠ½Ρ‚Π΅Ρ€Π²Π°Π»ΠΎΠ² дискрСтизации Π²Ρ€Π΅ΠΌΠ΅Π½ΠΈ, зависящих ΠΎΡ‚ стСпСни согласования ΠΌΠ°ΠΊΡΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹Ρ… ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ² гармоничСской ΠΏΠΎΠ»ΡƒΠ²ΠΎΠ»Π½Ρ‹. ΠŸΡ€ΠΈ сравнСнии, ΠΊΡ€ΠΎΠΌΠ΅ этих ΠΌΠ°ΠΊΡΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹Ρ… ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ², ΡƒΡ‡Ρ‚Π΅Π½Π° связь максимальной скорости сигнала с ΠΏΠΎΠ³Ρ€Π΅ΡˆΠ½ΠΎΡΡ‚ΡŒΡŽ аппроксимации Π²Ρ‹Π±ΠΎΡ€ΠΎΠΊ ΡΡ‚ΡƒΠΏΠ΅Π½ΡŒΠΊΠ°ΠΌΠΈ ΠΈ связь максимального ускорСния сигнала с максимальной ΠΏΠΎΠ³Ρ€Π΅ΡˆΠ½ΠΎΡΡ‚ΡŒΡŽ Π»ΠΈΠ½Π΅ΠΉΠ½ΠΎΠΉ аппроксимации. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡŽΡ‚ ΠΎΠΏΡ€Π΅Π΄Π΅Π»ΡΡ‚ΡŒ Π΄Π»ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΡΡ‚ΠΈ ΠΈΠ½Ρ‚Π΅Ρ€Π²Π°Π»ΠΎΠ² Ρ€Π°Π²Π½ΠΎΠΌΠ΅Ρ€Π½ΠΎΠΉ дискрСтизации Π²Ρ€Π΅ΠΌΠ΅Π½ΠΈ сигнала ΠΏΠΎ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π°ΠΌ обслСдования ΠΎΠ±ΡŠΠ΅ΠΊΡ‚Π° управлСния, ΠΎΠ±ΠΎΡΠ½ΠΎΠ²Ρ‹Π²Π°ΡŽΡ‚ сущСствСнноС ΡƒΠ²Π΅Π»ΠΈΡ‡Π΅Π½ΠΈΠ΅ ΠΈΠ½Ρ‚Π΅Ρ€Π²Π°Π»Π° дискрСтизации Π²Ρ€Π΅ΠΌΠ΅Π½ΠΈ ΠΈΠ»ΠΈ Π°Π½Π°Π»ΠΎΠ³ΠΈΡ‡Π½ΠΎΠ΅ ΡƒΠ²Π΅Π»ΠΈΡ‡Π΅Π½ΠΈΠ΅ числа Ρ€Π΅ΡˆΠ°Π΅ΠΌΡ‹Ρ… Π·Π°Π΄Π°Ρ‡ Π² Π΅Π΄ΠΈΠ½ΠΈΡ†Ρƒ систСмного Π²Ρ€Π΅ΠΌΠ΅Π½ΠΈ
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