157 research outputs found

    Surface composition of the Co-Cr based alloys after different lab denture treatments using auger electron spectroscopy

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    ΠœΠ΅Ρ‚ΠΎΡŽ Π΄Π°Π½ΠΎΡ— Ρ€ΠΎΠ±ΠΎΡ‚ΠΈ Ρ” Π°Π½Π°Π»Ρ–Π· Ρ…Ρ–ΠΌΡ–Ρ‡Π½ΠΎΠ³ΠΎ складу ΠΏΠΎΠ²Π΅Ρ€Ρ…Π½Ρ– сплаву Π½Π° основі Co-Cr після Π΄Π΅ΠΊΡ–Π»ΡŒΠΊΠΎΡ… Ρ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³Ρ–Ρ‡Π½ΠΈΡ… ΠΏΡ€ΠΎΡ†Π΅Π΄ΡƒΡ€, прийнятих Ρƒ стоматологічній ΠΏΡ€Π°ΠΊΡ‚ΠΈΡ†Ρ– Π·Π° допомогою ΠΎΠΆΠ΅-Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Π½ΠΎΡ— спСктроскопії (ΠžΠ•Π‘). Π¦Π΅ΠΉ Π°Π½Π°Π»Ρ–Π· ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ після відливання Π·Ρ€Π°Π·ΠΊΡ–Π² сплавів ΠΏΡ–Π΄Π΄Π°Π²Π°Π»ΠΈ наступним послідовним ΠΎΠ±Ρ€ΠΎΠ±ΠΊΠ°ΠΌ: розрізанням Π½Π° Π°Π»ΠΌΠ°Π·Π½ΠΎΠΌΡƒ колСсі, СлСктроіскровим різанням Ρ– ΡˆΠ»Ρ–Ρ„ΡƒΠ²Π°Π½Π½ΡΠΌ, СлСктрополірування, Π²ΠΈΡ‚Ρ€ΠΈΠΌΠΊΠΈ Π² ΡˆΡ‚ΡƒΡ‡Π½Ρ–ΠΉ слині 2 Π΄Π½Ρ– після СлСктрополірування

    Time correlations in atmospheric quantum channels

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    Efficient transfer of quantum information between remote parties is a crucial challenge for quantum communication over atmospheric channels. Random fluctuations of the channel transmittance are a major disturbing factor for its practical implementation. We study correlations between channel transmittances at different moments of time and focus on two transmission protocols. The first is related to the robustness of both discrete- and continuous-variable entanglement between time-separated light pulses, showing a possibility to enlarge the effective dimension of the Hilbert space. The second addresses a preselection of high-transmittance events by testing them with bright classical pulses followed by quantum light. Our results show a high capacity of the time-coherence resource for encoding and transferring quantum states of light in atmospheric channels.Comment: 11 pages, 6 figures, ancillary files include Python3 code and simulated dat

    Characterization of unwanted noise in realistic cavities

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    The problem of the description of absorption and scattering losses in high-Q cavities is studied. The considerations are based on quantum noise theories, hence the unwanted noise associated with scattering and absorption is taken into account by introduction of additional damping and noise terms in the quantum Langevin equations and input--output relations. Completeness conditions for the description of the cavity models obtained in this way are studied and corresponding replacement schemes are discussed.Comment: Contribution to XI International Conference on Quantum Optics, Minsk, Belarus, 26-31 May, 200

    The Distribution of Bar and Spiral Strengths in Disk Galaxies

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    The distribution of bar strengths in disk galaxies is a fundamental property of the galaxy population that has only begun to be explored. We have applied the bar/spiral separation method of Buta, Block, and Knapen to derive the distribution of maximum relative gravitational bar torques, Q_b, for 147 spiral galaxies in the statistically well-defined Ohio State University Bright Galaxy Survey (OSUBGS) sample. Our goal is to examine the properties of bars as independently as possible of their associated spirals. We find that the distribution of bar strength declines smoothly with increasing Q_b, with more than 40% of the sample having Q_b <= 0.1. In the context of recurrent bar formation, this suggests that strongly-barred states are relatively short-lived compared to weakly-barred or non-barred states. We do not find compelling evidence for a bimodal distribution of bar strengths. Instead, the distribution is fairly smooth in the range 0.0 <= Q_b < 0.8. Our analysis also provides a first look at spiral strengths Q_s in the OSU sample, based on the same torque indicator. We are able to verify a possible weak correlation between Q_s and Q_b, in the sense that galaxies with the strongest bars tend also to have strong spirals.Comment: Accepted for publication in the Astronomical Journal, August 2005 issue (LaTex, 23 pages + 11 figures, uses aastex.cls

    QualitΓ€tsprodukt Erziehungsberatung. Empfehlungen zu Leistungen, QualitΓ€tsmerkmalen und Kennziffern

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    Neben einer Beschreibung der Leistung Erziehungs- und Familienberatung - Beratung und Therapie, prΓ€ventive Angebote und VernetzungsaktivitΓ€ten - werden ihre QualitΓ€tsmerkmale - gegliedert nach Struktur-, Prozess- und ErgebnisqualitΓ€t - ausfΓΌhrlich dargestellt und Kennziffern zu ihrer quantitativen Erfassung vorgeschlagen. Der Anhang enthΓ€lt u.a. eine Kurzfassung der vorliegenden Empfehlungen zu Leistungen, QualitΓ€tsmerkmalen und Kennziffern. (DIPF/Autor

    Leaky cavities with unwanted noise

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    A phenomenological approach is developed that allows one to completely describe the effects of unwanted noise, such as the noise associated with absorption and scattering, in high-Q cavities. This noise is modeled by a block of beam splitters and an additional input-output port. The replacement schemes enable us to formulate appropriate quantum Langevin equations and input-output relations. It is demonstrated that unwanted noise renders it possible to combine a cavity input mode and the intracavity mode in a nonmonochromatic output mode. Possible applications to unbalanced and cascaded homodyning of the intracavity mode are discussed and the advantages of the latter method are shown.Comment: 13 pages, 7 figures; published versio

    The boundaries and their impact on properties of zirconia electrolyte

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    Interfaces and their complexions created in the zirconia 1Ce10ScSZ ceramic electrolyte and altered by three powder types and sintering temperatures were studied via their effect on mechanical behavior and electrical conductivity. Two boundary complexions, which exist and developed between subgrains and grains with sintering temperature were observed. The transition between boundary categories, which was defined as the boundary complexion transition of the second kind, occurs in both very pure 1Ce10ScSZ ceramics and in ceramics of technical purity, powder of which is contaminated with rather large amounts of silica and titania. The ceramics contaminated with rather large amount of silica and alumina does not reveal any complexion transitions. Joint analysis of data obtained with electron microscopy and related techniques, mechanical tests for strength, scanning electron fractography and impedance spectroscopy of structural constituents of electrical resistance has given a lot of information on the effect of boundaries and their complexions on properties of electrolyte where mechanical behavior is as important as their conductivity.ΠœΠ΅ΠΆΡ– Ρ‚Π° Ρ—Ρ…Π½Ρ– комплСкси Π² ΠΊΠ΅Ρ€Π°ΠΌΡ–Ρ‡Π½ΠΎΠΌΡƒ Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ»Ρ–Ρ‚Ρ– 1Ce10ScSZ, які Π±ΡƒΠ»ΠΈ ΡƒΡ‚Π²ΠΎΡ€Π΅Π½Ρ– Ρ– Π·ΠΌΡ–Π½ΡŽΠ²Π°Π½Ρ– застосуванням Ρ‚Ρ€ΡŒΠΎΡ… Ρ‚ΠΈΠΏΡ–Π² Π²ΠΈΡ…Ρ–Π΄Π½ΠΈΡ… ΠΏΠΎΡ€ΠΎΡˆΠΊΡ–Π² Ρ– Ρ€Ρ–Π·Π½ΠΈΡ… Ρ€Π΅ΠΆΠΈΠΌΡ–Π² спікання, Π²ΠΈΠ²Ρ‡Π΅Π½Ρ– Ρ‡Π΅Ρ€Π΅Π· Ρ—Ρ…Π½Ρ–ΠΉ Π²ΠΏΠ»ΠΈΠ² Π½Π° ΠΌΠ΅Ρ…Π°Π½Ρ–Ρ‡Π½Ρƒ ΠΏΠΎΠ²Π΅Π΄Ρ–Π½ΠΊΡƒ Ρ‚Π° Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠΏΡ€ΠΎΠ²Ρ–Π΄Π½Ρ–ΡΡ‚ΡŒ. Π‘ΠΏΡ–Π»ΡŒΠ½ΠΈΠΉ Π°Π½Π°Π»Ρ–Π· Π΄Π°Π½ΠΈΡ…, ΠΎΡ‚Ρ€ΠΈΠΌΠ°Π½ΠΈΡ… ΠΌΠ΅Ρ‚ΠΎΠ΄Π°ΠΌΠΈ Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Π½ΠΎΡ— мікроскопії Ρ‚Π° Ρ–Π½ΡˆΠΈΠΌΠΈ, пов’язаними Ρ–Π· нСю, ΠΌΠ΅Ρ‚ΠΎΠ΄Π°ΠΌΠΈ ΠΌΠ΅Ρ…Π°Π½Ρ–Ρ‡Π½ΠΈΡ… Π²ΠΈΠΏΡ€ΠΎΠ±ΡƒΠ²Π°Π½ΡŒ Π½Π° ΠΌΡ–Ρ†Π½Ρ–ΡΡ‚ΡŒ, ΡΠΊΠ°Π½ΡƒΡŽΡ‡ΠΎΡ— Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Π½ΠΎΡ— Ρ„Ρ€Π°ΠΊΡ‚ΠΎΠ³Ρ€Π°Ρ„Ρ–Ρ— Ρ‚Π° імпСдансної спСктроскопії структурних складових Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΈΡ‡Π½ΠΎΠ³ΠΎ ΠΎΠΏΠΎΡ€Ρƒ, Π½Π°Π΄Π°Π² Π±Π°Π³Π°Ρ‚ΠΎ Ρ–Π½Ρ„ΠΎΡ€ΠΌΠ°Ρ†Ρ–Ρ— Ρ‰ΠΎΠ΄ΠΎ Π²ΠΏΠ»ΠΈΠ²Ρƒ ΠΌΠ΅ΠΆ Ρ‚Π° Ρ—Ρ…Π½Ρ–Ρ… комплСксів Π½Π° властивості Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ»Ρ–Ρ‚Ρƒ, для якого ΠΌΠ΅Ρ…Π°Π½Ρ–Ρ‡Π½Π° ΠΏΠΎΠ²Π΅Π΄Ρ–Π½ΠΊΠ° Ρ” Π½Π°ΡΡ‚Ρ–Π»ΡŒΠΊΠΈ ваТливою, як Ρ– ΠΉΠΎΠ³ΠΎ ΠΏΡ€ΠΎΠ²Ρ–Π΄Π½Ρ–ΡΡ‚ΡŒ. БпостСрСТСно корСлятивний Π²ΠΏΠ»ΠΈΠ² ΠΌΠ΅ΠΆ, які Π²ΠΈΠ·Π½Π°Ρ‡Π°ΡŽΡ‚ΡŒΡΡ Π²ΠΈΡ…Ρ–Π΄Π½ΠΈΠΌΠΈ Ρ‚ΠΈΠΏΠ°ΠΌΠΈ ΠΏΠΎΡ€ΠΎΡˆΠΊΡ–Π² Ρ‚Π° Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€ΠΎΡŽ Ρ—Ρ…Π½ΡŒΠΎΠ³ΠΎ спікання, Π½Π° ΠΌΠ΅Ρ…Π°Π½Ρ–Ρ‡Π½Ρƒ ΠΏΠΎΠ²Π΅Π΄Ρ–Π½ΠΊΡƒ Ρ– Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΈΡ‡Π½Ρƒ ΠΏΡ€ΠΎΠ²Ρ–Π΄Π½Ρ–ΡΡ‚ΡŒ Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ»Ρ–Ρ‚Ρƒ. Π’ΠΈΠ·Π½Π°Ρ‡Π΅Π½ΠΎ Π΄Π²Π° Ρ‚ΠΈΠΏΠΈ ΠΌΠ΅ΠΆΠ΅Π²ΠΈΡ… комплСксів, які Ρ–ΡΠ½ΡƒΡŽΡ‚ΡŒ Ρ– Ρ€ΠΎΠ·Π²ΠΈΠ²Π°ΡŽΡ‚ΡŒΡΡ ΠΌΡ–ΠΆ субзСрнами Ρ‚Π° Π·Π΅Ρ€Π½Π°ΠΌΠΈ Π· ростом Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€ΠΈ спікання. ΠŸΠ΅Ρ€Π΅Ρ…Ρ–Π΄ ΠΌΡ–ΠΆ Ρ†ΠΈΠΌΠΈ катСгоріями ΠΌΠ΅ΠΆ, Ρ‰ΠΎ Π±ΡƒΠ»ΠΎ Π½Π°Π·Π²Π°Π½ΠΎ ΠΏΠ΅Ρ€Π΅Ρ…ΠΎΠ΄ΠΎΠΌ ΠΌΠ΅ΠΆΠ΅Π²ΠΈΡ… комплСксів Π΄Ρ€ΡƒΠ³ΠΎΠ³ΠΎ Ρ€ΠΎΠ΄Ρƒ, Π²Ρ–Π΄Π±ΡƒΠ²Π°Ρ”Ρ‚ΡŒΡΡ як Π² Ρ…Ρ–ΠΌΡ–Ρ‡Π½ΠΎ чистій ΠΊΠ΅Ρ€Π°ΠΌΡ–Ρ†Ρ– 1Ce10ScSZ, Ρ‚Π°ΠΊ Ρ– Π² ΠΊΠ΅Ρ€Π°ΠΌΡ–Ρ†Ρ– Ρ‚Π΅Ρ…Π½Ρ–Ρ‡Π½ΠΎΡ— чистоти, ΠΏΠΎΡ€ΠΎΡˆΠΊΠΈ якої Π·Π±Π°Π³Π°Ρ‡Π΅Π½Ρ– Π΄ΠΎΡΠΈΡ‚ΡŒ Π·Π½Π°Ρ‡Π½ΠΎΡŽ ΠΊΡ–Π»ΡŒΠΊΡ–ΡΡ‚ΡŽ оксидів ΠΊΡ€Π΅ΠΌΠ½Ρ–ΡŽ Ρ‚Π° Ρ‚ΠΈΡ‚Π°Π½Ρƒ. Π’ ΠΊΠ΅Ρ€Π°ΠΌΡ–Ρ†Ρ– 1Ce10ScSZ Π· Π²Π΅Π»ΠΈΠΊΠΈΠΌ вмістом оксидів ΠΊΡ€Π΅ΠΌΠ½Ρ–ΡŽ Ρ‚Π° Π°Π»ΡŽΠΌΡ–Π½Ρ–ΡŽ ΠΏΠΎΠΌΡ–Ρ‚Π½ΠΈΡ… ΠΏΠ΅Ρ€Π΅Ρ…ΠΎΠ΄Ρ–Π² Π½Π΅ виявлСно.ΠžΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½Π½Ρ‹Π΅ Π² кСрамичСском элСктролитС 1Ce10ScSZ Π³Ρ€Π°Π½ΠΈΡ†Ρ‹ ΠΈ ΠΈΡ… комплСксы, ΠΈΠ·ΠΌΠ΅Π½Π΅Π½Π½Ρ‹Π΅ посрСдством контроля Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹ спСкания с использованиСм исходных ΠΏΠΎΡ€ΠΎΡˆΠΊΠΎΠ² Ρ‚Ρ€Ρ‘Ρ… Ρ‚ΠΈΠΏΠΎΠ², исслСдовали, анализируя ΠΈΡ… влияниС Π½Π° мСханичСскоС ΠΏΠΎΠ²Π΅Π΄Π΅Π½ΠΈΠ΅ ΠΈ ΡΠ»Π΅ΠΊΡ‚Ρ€ΠΎΠΏΡ€ΠΎΠ²ΠΎΠ΄Π½ΠΎΡΡ‚ΡŒ. КомплСксная ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚ΠΊΠ° Π΄Π°Π½Π½Ρ‹Ρ…, ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Ρ… ΠΌΠ΅Ρ‚ΠΎΠ΄Π°ΠΌΠΈ элСктронной микроскопии ΠΈ Π΄Ρ€ΠΈΠ³ΠΈΠΌΠΈ, связаннными с Π½Π΅ΠΉ, ΠΌΠ΅Ρ‚ΠΎΠ΄Π°ΠΌΠΈ мСханичСских испытаний Π½Π° ΠΏΡ€ΠΎΡ‡Π½ΠΎΡΡ‚ΡŒ, ΡΠΊΠ°Π½ΠΈΡ€ΡƒΡŽΡ‰Π΅ΠΉ элСктронной Ρ„Ρ€Π°ΠΊΡ‚ΠΎΠ³Ρ€Π°Ρ„ΠΈΠΈ, Π° Ρ‚Π°ΠΊΠΆΠ΅ импСдансной спСктроскопиСй структурных ΡΠΎΡΡ‚Π°Π²Π»ΡΡŽΡ‰ΠΈΡ… элСктричСского сопротивлСния, прСдоставила ΠΈΠ½Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΡŽ ΠΎ влиянии Π³Ρ€Π°Π½ΠΈΡ† ΠΈ ΠΈΡ… соСдинСний Π½Π° свойства элСктролита, для ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠ³ΠΎ мСханичСскоС ΠΏΠΎΠ²Π΅Π΄Π΅Π½ΠΈΠ΅ Ρ‚Π°ΠΊΠΆΠ΅ Π²Π°ΠΆΠ½ΠΎ, ΠΊΠ°ΠΊ ΠΈ Π΅Π³ΠΎ ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠΌΠΎΡΡ‚ΡŒ. Наблюдалась коррСляция ΠΌΠ΅ΠΆΠ΄Ρƒ влияниСм Π³Ρ€Π°Π½ΠΈΡ†, ΠΎΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½Π½Ρ‹Ρ… исходными ΠΏΠΎΡ€ΠΎΡˆΠΊΠ°ΠΌΠΈ Ρ‚Ρ€Ρ‘Ρ… Ρ‚ΠΈΠΏΠΎΠ² ΠΈ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€ΠΎΠΉ ΠΈΡ… спСкания, Π½Π° мСханичСскоС ΠΏΠΎΠ²Π΅Π΄Π΅Π½ΠΈΠ΅ ΠΈ ΡΠ»Π΅ΠΊΡ‚Ρ€ΠΈΡ‡Π΅ΡΠΊΡƒΡŽ ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠΌΠΎΡΡ‚ΡŒ элСктролита 1Ce10ScSZ. НайдСно Π΄Π²Π΅ ΠΊΠΎΠΌΠ±ΠΈΠ½Π°Ρ†ΠΈΠΈ Π³Ρ€Π°Π½ΠΈΡ‡Π½Ρ‹Ρ… комплСксов, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ ΡΡƒΡ‰Π΅ΡΡ‚Π²ΡƒΡŽΡ‚ ΠΈ ΡƒΠ»ΡƒΡ‡ΡˆΠ°ΡŽΡ‚ΡΡ с ростом Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹ спСкания ΠΌΠ΅ΠΆΠ΄Ρƒ субзСрнами ΠΈ Π·Π΅Ρ€Π½Π°ΠΌΠΈ. ΠŸΠ΅Ρ€Π΅Ρ…ΠΎΠ΄ ΠΌΠ΅ΠΆΠ΄Ρƒ Π²ΠΈΠ΄Π°ΠΌΠΈ Π³Ρ€Π°Π½ΠΈΡ‡Π½Ρ‹Ρ… комплСксов, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹ΠΉ Π±Ρ‹Π» ΠΎΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½ ΠΊΠ°ΠΊ ΠΏΠ΅Ρ€Π΅Ρ…ΠΎΠ΄ Π²Ρ‚ΠΎΡ€ΠΎΠ³ΠΎ Ρ€ΠΎΠ΄Π°, происходит ΠΊΠ°ΠΊ Π² химичСски чистой ΠΊΠ΅Ρ€Π°ΠΌΠΈΠΊΠ΅ 1Ce10ScSZ, Ρ‚Π°ΠΊ ΠΈ Π² ΠΊΠ΅Ρ€Π°ΠΌΠΈΠΊΠ΅ тСхничСской чистоты ΠΈΠ· ΠΏΠΎΡ€ΠΎΡˆΠΊΠΎΠ², ΠΎΠ±ΠΎΠ³Π°Ρ‰Π΅Π½Π½Ρ‹Ρ… оксидами крСмния ΠΈ Ρ‚ΠΈΡ‚Π°Π½Π°. Π’ ΠΊΠ΅Ρ€Π°ΠΌΠΈΠΊΠ΅ 1Ce10ScSZ содСрТащСй Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Π΅ количСства оксидов крСмния ΠΈ алюминия, ΠΏΠ΅Ρ€Π΅Ρ…ΠΎΠ΄Ρ‹ Π½Π΅ ΠΎΠ±Π½Π°Ρ€ΡƒΠΆΠ΅Π½Ρ‹

    Toward Global Quantum Communication: Beam Wandering Preserves Nonclassicality

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    Tap-proof long-distance quantum communication requires a deep understanding of the strong losses in transmission channels. Here we provide a rigorous treatment of the effects of beam wandering, one of the leading disturbances in atmospheric channels, on the quantum properties of light. From first principles we derive the probability distribution of the beam transmissivity, with the aim to completely characterize the quantum state of light. It turns out that beam wandering may preserve nonclassical effects, such as entanglement, quadrature and photon number squeezing, much better than a standard attenuating channel of the same losses.Comment: published versio

    ЦикличСский Ρ…Π°Ρ€Π°ΠΊΡ‚Π΅Ρ€ измСнСния микротвСрдости алюминиСвого сплава Π”16 ΠΏΠΎΠ΄ дСйствиСм ΡƒΠ»ΡŒΡ‚Ρ€Π°Π·Π²ΡƒΠΊΠΎΠ²ΠΎΠΉ ΡƒΠ΄Π°Ρ€Π½ΠΎΠΉ ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ

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    ДослідТСно моТливості Π±Ρ–Π»ΡŒΡˆ Π΅Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΠ³ΠΎ, порівняно Ρ–Π· Ρ‚Ρ€Π°Π΄ΠΈΡ†Ρ–ΠΉΠ½ΠΎΡŽ Ρ‚Π΅Ρ€ΠΌΠΎΠΌΠ΅Ρ…Π°Π½Ρ–Ρ‡Π½ΠΎΡŽ ΠΎΠ±Ρ€ΠΎΠ±ΠΊΠΎΡŽ, зміцнСння ΠΏΠΎΠ²Π΅Ρ€Ρ…Π½Ρ– Π»Π΅Π³ΠΊΠΈΡ… конструкційних сплавів ΡƒΠ»ΡŒΡ‚Ρ€Π°Π·Π²ΡƒΠΊΠΎΠ²ΠΎΡŽ ΡƒΠ΄Π°Ρ€Π½ΠΎΡŽ ΠΎΠ±Ρ€ΠΎΠ±ΠΊΠΎΡŽ (Π£Π—Π£Πž) Π½Π° ΠΏΠΎΠ²Ρ–Ρ‚Ρ€Ρ– Π·Π° ΡƒΠΌΠΎΠ² ΠΊΠ²Π°Π·Ρ–-гідростатичного стиснСння Π·Ρ€Π°Π·ΠΊΠ°. На ΠΏΡ€ΠΈΠΊΠ»Π°Π΄Ρ– промислового Π°Π»ΡŽΠΌΡ–Π½Ρ–Ρ”Π²ΠΎΠ³ΠΎ сплаву Π”16 ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ ΡƒΠ½Ρ–ΠΊΠ°Π»ΡŒΠ½Ρƒ ΠΌΠΎΠΆΠ»ΠΈΠ²Ρ–ΡΡ‚ΡŒ зміцнСння ΠΏΠΎΠ²Π΅Ρ€Ρ…Π½Ρ– (Π΄ΠΎ ∼600 %), Π·ΡƒΠΌΠΎΠ²Π»Π΅Π½ΠΎΠ³ΠΎ синСргСтичним Π²ΠΏΠ»ΠΈΠ²ΠΎΠΌ процСсі Π½ΠΈΠ·ΡŒΠΊΠΎΡ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π½ΠΎΡ— ΠΌΠ΅Ρ…Π°Π½Ρ–Ρ‡Π½ΠΎΡ— наноструктуризації Ρ‚Π° ΠΌΠ΅Ρ…Π°Π½ΠΎΡ…Ρ–ΠΌΡ–Ρ‡Π½ΠΎΡ— Π²Π·Π°Ρ”ΠΌΠΎΠ΄Ρ–Ρ— Π°Π»ΡŽΠΌΡ–Π½Ρ–ΡŽ Ρ–Π· киснСм ΠΏΡ–Π΄ Π΄Ρ–Ρ”ΡŽ Π£Π—Π£Πž. Π—Π°ΠΏΡ€ΠΎΠΏΠΎΠ½ΠΎΠ²Π°Π½ΠΎ якісну модСль формування оксидного покриття Ρ‚ΠΎΠ²Ρ‰ΠΈΠ½ΠΎΡŽ ΠΊΡ–Π»ΡŒΠΊΠ° дСсятків ΠΌΡ–ΠΊΡ€ΠΎΠΌΠ΅Ρ‚Ρ€Ρ–Π². Π— використанням комплСксу Ρ„Ρ–Π·ΠΈΡ‡Π½ΠΈΡ… ΠΌΠ΅Ρ‚ΠΎΠ΄Ρ–Π² дослідТСння встановлСно основні закономірності формування Ρ„Π°Π·ΠΎΠ²ΠΎΠ³ΠΎ Ρ– Ρ…Ρ–ΠΌΡ–Ρ‡Π½ΠΎΠ³ΠΎ складу, структури Ρ‚Π° ΠΌΠ΅Ρ…Π°Π½Ρ–Ρ‡Π½ΠΈΡ… властивостСй ΠΏΠΎΠ²Π΅Ρ€Ρ…Π½Π΅Π²ΠΈΡ… ΡˆΠ°Ρ€Ρ–Π² сплаву Π”16 Π·Π°Π»Π΅ΠΆΠ½ΠΎ Π²Ρ–Π΄ Π°ΠΌΠΏΠ»Ρ–Ρ‚ΡƒΠ΄ΠΈ Ρ‚Π° тривалості ΠΎΠ±Ρ€ΠΎΠ±ΠΊΠΈ. Показано, Ρ‰ΠΎ Ρ†ΠΈΠΊΠ»Ρ–Ρ‡Π½ΠΈΠΉ Ρ…Π°Ρ€Π°ΠΊΡ‚Π΅Ρ€ Π·ΠΌΡ–Π½ мікротвСрдості Π·ΡƒΠΌΠΎΠ²Π»ΡŽΡ”Ρ‚ΡŒΡΡ ΠΏΠ΅Ρ€Π΅Π±Ρ–Π³ΠΎΠΌ дисипативних процСсів Π΄ΠΈΠ½Π°ΠΌΡ–Ρ‡Π½ΠΎΠ³ΠΎ повСрнСння Ρ‚Π° Π΄ΠΈΠ½Π°ΠΌΡ–Ρ‡Π½ΠΎΡ— рСкристалізації. Π—Π° ΠΎΠΏΡ‚ΠΈΠΌΠ°Π»ΡŒΠ½ΠΈΡ… Ρ€Π΅ΠΆΠΈΠΌΡ–Π² Π£Π—Π£Πž Π·Π½ΠΎΡΠΎΡΡ‚Ρ–ΠΉΠΊΡ–ΡΡ‚ΡŒ ΠΏΠΎΠ²Π΅Ρ€Ρ…Π½Π΅Π²ΠΈΡ… ΡˆΠ°Ρ€Ρ–Π² зростає Ρƒ 2,5 Ρ€Π°Π·Ρƒ, Ρ€Ρ–Π²Π΅Π½ΡŒ Π·Π°Π»ΠΈΡˆΠΊΠΎΠ²ΠΈΡ… ΠΌΠ°ΠΊΡ€ΠΎΠ½Π°ΠΏΡ€ΡƒΠΆΠ΅Π½ΡŒ стиснСння Π΄ΠΎΡ€Ρ–Π²Π½ΡŽΡ” 650 МПа.The article studies possibilities of more effective surface hardening as compared with conventional thermomechanical processing. Specifically, we provide the insight into surface hardening of light structural alloys by ultrasonic impact treatment (UIT) in air under quasi-hydrostatic pressure of the sample. By example of the commercial aluminum alloy D16 we demonstrate the unique opportunity to harden the surface (up to ~600 %) using the synergistic effect of low-temperature processes of mechanical nanostructuring as well as mechanical and chemical interaction of aluminum with oxygen under the influence of UIT. We propose the qualitative model for formation of oxide coating several tens of micrometers thick. By employing a set of physical methods we establish basic laws of the phase formation and chemical composition, structure and mechanical properties of the D16 alloy surface layers depending on the amplitude and duration of UIT. We show that the development of dynamic recovery and dynamic recrystallization processes causes the cyclic nature of microhardness changes. Under optimal conditions of UIT the wear resistance of surface layers increased by ~2,5 times, and the compression residual stresses level is 650 MPa.Π˜ΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Ρ‹ возмоТности Π±ΠΎΠ»Π΅Π΅ эффСктивного, ΠΏΠΎ ΡΡ€Π°Π²Π½Π΅Π½ΠΈΡŽ с Ρ‚Ρ€Π°Π΄ΠΈΡ†ΠΈΠΎΠ½Π½ΠΎ тСрмомСханичСской ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚ΠΊΠΎΠΉ, упрочнСния повСрхности Π»Π΅Π³ΠΊΠΈΡ… конструкционных сплавов ΡƒΠ»ΡŒΡ‚Ρ€Π°Π·Π²ΡƒΠΊΠΎΠ²ΠΎΠΉ ΡƒΠ΄Π°Ρ€Π½ΠΎΠΉ ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚ΠΊΠΎΠΉ (Π£Π—Π£Πž) Π½Π° Π²ΠΎΠ·Π΄ΡƒΡ…Π΅ Π² условиях квазигидростатичСского сТатия ΠΎΠ±Ρ€Π°Π·Ρ†Π°. На ΠΏΡ€ΠΈΠΌΠ΅Ρ€Π΅ ΠΏΡ€ΠΎΠΌΡ‹ΡˆΠ»Π΅Π½Π½ΠΎΠ³ΠΎ алюминиСвого сплава Π”16 ΠΏΠΎΠΊΠ°Π·Π°Π½Π° ΡƒΠ½ΠΈΠΊΠ°Π»ΡŒΠ½Π°Ρ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡ‚ΡŒ упрочнСния повСрхности (Π΄ΠΎ ∼ 600 %), обусловлСнного синСргСтичСским влияниСм процСссов Π½ΠΈΠ·ΠΊΠΎΡ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π½ΠΎΠΉ мСханичСской наноструктуризации ΠΈ мСханохимичСского взаимодСйствия алюминия с кислородом ΠΏΠΎΠ΄ дСйствиСм Π£Π—Π£Πž. ΠŸΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½Π° качСствСнная модСль формирования оксидного покрытия Ρ‚ΠΎΠ»Ρ‰ΠΈΠ½ΠΎΠΉ нСсколько дСсятков ΠΌΠΈΠΊΡ€ΠΎΠΌΠ΅Ρ‚Ρ€ΠΎΠ². Π‘ использованиСм комплСкса физичСских ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠ² исслСдования установлСны основныС закономСрности формирования Ρ„Π°Π·ΠΎΠ²ΠΎΠ³ΠΎ ΠΈ химичСского состава, структуры ΠΈ мСханичСских свойств повСрхностных слоСв сплава Π”16 Π² зависимости ΠΎΡ‚ Π°ΠΌΠΏΠ»ΠΈΡ‚ΡƒΠ΄Ρ‹ ΠΈ Π΄Π»ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΡΡ‚ΠΈ ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ. Показано, Ρ‡Ρ‚ΠΎ цикличСский Ρ…Π°Ρ€Π°ΠΊΡ‚Π΅Ρ€ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠΉ микротвСрдости обусловлСн Ρ€Π°Π·Π²ΠΈΡ‚ΠΈΠ΅ΠΌ диссипативных процСссов динамичСского Π²ΠΎΠ·Π²Ρ€Π°Ρ‚Π° ΠΈ динамичСской рСкристаллизации. ΠŸΡ€ΠΈ ΠΎΠΏΡ‚ΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹Ρ… Ρ€Π΅ΠΆΠΈΠΌΠ°Ρ… Π£Π—Π£Πž ΠΈΠ·Π½ΠΎΡΠΎΡΡ‚ΠΎΠΉΠΊΠΎΡΡ‚ΡŒ повСрхностных слоСв возрастаСт Π² 2,5 Ρ€Π°Π·Π°, ΡƒΡ€ΠΎΠ²Π΅Π½ΡŒ остаточных макронапряТСний сТатия Ρ€Π°Π²Π΅Π½ 650 МПа

    Analytical solutions for semiconductor luminescence including Coulomb correlations with applications to dilute bismides

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    In this paper we introduce analytical solutions of interband polarization, which is the self-energy of the Dyson equation for the photon Green’s functions, and apply them to studying photoluminescence of Coulomb-correlated semiconductor materials. The accuracy of the easily programmable solutions is proven by consistently demonstrating the low-temperature s-shape of the luminescence peak of dilute bismide semiconductors. The different roles of homogeneous versus inhomogeneous broadening at low and high temperatures are described, as well as the importance of many body effects, which are in very good agreement with experiments
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