71 research outputs found

    Color Effects Associated with the 1999 Microlensing Brightness Peaks in Gravitationally Lensed Quasar Q2237+0305

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    Photometry of the Q2237+0305gravitational lens in VRI spectral bands with the 1.5-m telescope of the high-altitude Maidanak observatory in 1995-2000 is presented. Monitoring of Q2237+0305 in July-October 2000, made at nearly daily basis, did not reveal rapid (night-to-night and intranight) variations of brightness of the components during this time period. Rather slow changes of magnitudes of the components were observed, such as 0.08 mag fading of B and C components and 0.05 mag brightening of D in R band during July 23 - October 7, 2000. By good luck three nights in 1999 were almost at the time of the strong brightness peak of image C, and approximately in the middle of the ascending slope of the image A brightness peak. The C component was the most blue one in the system in 1998 and 1999, having changed its (V-I) color from 0.56 mag to 0.12 mag since August 1997, while its brightness increased almost 1.2 mag during this time period. The A component behaved similarly between August 1998 and August 2000, having become 0.47 mag brighter in R, and at the same time, 0.15 mag bluer. A correlation between the color variations and variations of magnitudes of the components is demonstrated to be significant and reaches 0.75, with a regression line slope of 0.33. A color (V-I) vrs color (V-R) plot shows the components settled in a cluster, stretched along a line with a slope of 1.31. Both slopes are noticeably smaller than those expected if a standard galactic interstellar reddening law were responsible for the differences between the colors of images and their variations over time. We attribute the brightness and color changes to microlensing of the quasar's structure, which we conclude is more compact at shorter wavelengths, as predicted by most quasar models featuring an energizing central source.Comment: 14 pages, 7 figures, LaTeX, submitted to A&

    Superconductivity in the Pseudogap State due to Fluctuations of Short-Range Order

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    We analyze the anomalies of superconducting state (s and d-wave pairing) in a simple model of pseudogap state, induced by fluctuations of short - range order (e.g. antiferromagnetic), based on the model Fermi surface with "hot patches". We derive a system of recursion relations for Gorkov's equations which take into account all diagrams of perturbation theory for electron interaction with fluctuations of short-range order. Then we find superconducting transition temperature and gap behavior for different values of the pseudogap width and correlation lengths of short-range order fluctuations. In a similar approximation we derive the Ginzburg-Landau expansion and study the main physical characteristics of a superconductor close to the transition temperature, both as functions of the pseudogap width and correlation length of fluctuations. Results obtained are in qualitative agreement with a number of experiments on underdoped HTSC-cuprates.Comment: 18 pages, 12 figures, RevTeX 3.0, minor misprints corrected, to appear in JET

    Nesting Induced Precursor Effects: a Renormalization Group Approach

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    We develop a controlled weak coupling renormalization group (RG) approach to itinerant electrons. Within this formalism we rederive the phase diagram for two-dimensional (2D) non-nested systems. Then we study how nesting modifies this phase diagram. We show that competition between p-p and p-h channels, leads to the manifestation of unstable precursor fixed points in the RG flow. This effect should be experimentally measurable, and may be relevant for an explanation of pseudogaps in the high temperature superconductors (HTC), as a crossover phenomenon.Comment: 4 pages, 4 figures, 1 tabl

    ΠŸΡ€ΠΎΠ±Π»Π΅ΠΌΠ° хирургичСской ΠΈΠ½Ρ„Π΅ΠΊΡ†ΠΈΠΈ Ρƒ Π±ΠΎΠ»ΡŒΠ½Ρ‹Ρ… Π‘Π°Ρ…Π°Ρ€Π½Ρ‹ΠΌ Π΄ΠΈΠ°Π±Π΅Ρ‚ΠΎΠΌ, ΠΎΠΏΠ΅Ρ€ΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Ρ… Π½Π° Π°ΠΎΡ€Ρ‚ΠΎ-подвздошном сСгмСнтС

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    The aim of the work: to analyze the frequency and causes of purulent-septic complications in patients who underwent endoprosthetic repair of the aorto-iliac segment. Analysis of purulent-septic complications in 54 patients who were operated for ischemic lesions of the vessels of the lower extremities in diabetes mellitus was conducted. All patients underwent interventions on the aorto-iliac segment using synthetic vascular prostheses. In accordance with the classification of purulent-septic complications of reconstructive operations 5 cases of complications available in our practice, we divided into 2 groups – prosthetic sepsis; infection of the graft without clinical and laboratory manifestations of sepsis. The frequency of purulent-septic complications 9.2 percent, almost all of these patients had grade III-IV ischemia and were operated on urgent indications. In 3 cases, infection of the graft without bacteremia patients were operated before the development of erosive bleeding, which allowed 2 patients to save limbs, and 1 patient was discharged after performing the high amputation of the limb. In two cases a partial resection of the infected portion of the bifurcation prosthesis from separate access and subsequent re-reconstruction. In one case in a patient with progressive limb ischemia removed the infected bifurcation prosthesis, and surgery was performed subclavianfemoral bypass grafting extraanatomical on the one hand, and high amputation of the contralateral limb. Prosthetic sepsis occurred in 2 patients, 1 patient died.ЦСль Ρ€Π°Π±ΠΎΡ‚Ρ‹: ΠΏΡ€ΠΎΠ°Π½Π°Π»ΠΈΠ·ΠΈΡ€ΠΎΠ²Π°Ρ‚ΡŒ частоту ΠΈ ΠΏΡ€ΠΈΡ‡ΠΈΠ½Ρ‹ Π³Π½ΠΎΠΉΠ½ΠΎ-сСптичСских ослоТнСний Ρƒ Π±ΠΎΠ»ΡŒΠ½Ρ‹Ρ…, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹ΠΌ Π²Ρ‹ΠΏΠΎΠ»Π½Π΅Π½ΠΎ эндопротСзированиС Π°ΠΎΡ€Ρ‚ΠΎ-подвздошного сСгмСнта. ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½ Π°Π½Π°Π»ΠΈΠ· Π³Π½ΠΎΠΉΠ½ΠΎ-сСптичСских ослоТнСний Ρƒ 54 Π±ΠΎΠ»ΡŒΠ½Ρ‹Ρ…, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ Π±Ρ‹Π»ΠΈ ΠΎΠΏΠ΅Ρ€ΠΈΡ€ΠΎΠ²Π°Π½Ρ‹ ΠΏΠΎ ΠΏΠΎΠ²ΠΎΠ΄Ρƒ ΠΈΡˆΠ΅ΠΌΠΈΡ‡Π΅ΡΠΊΠΈΡ… ΠΏΠΎΡ€Π°ΠΆΠ΅Π½ΠΈΠΉ сосудов Π½ΠΈΠΆΠ½ΠΈΡ… конСчностСй Π½Π° Ρ„ΠΎΠ½Π΅ сахарного Π΄ΠΈΠ°Π±Π΅Ρ‚Π°. Π£ всСх Π±ΠΎΠ»ΡŒΠ½Ρ‹Ρ… Π±Ρ‹Π»ΠΈ Π²Ρ‹ΠΏΠΎΠ»Π½Π΅Π½Ρ‹ Π²ΠΌΠ΅ΡˆΠ°Ρ‚Π΅Π»ΡŒΡΡ‚Π²Π° Π½Π° Π°ΠΎΡ€Ρ‚ΠΎ-подвздошном сСгмСнтС с использованиСм синтСтичСских сосудистых ΠΏΡ€ΠΎΡ‚Π΅Π·ΠΎΠ². Π’ соотвСтствии с классификациСй Π³Π½ΠΎΠΉΠ½ΠΎ-сСптичСских ослоТнСний рСконструктивных ΠΎΠΏΠ΅Ρ€Π°Ρ†ΠΈΠΉ 5 случаСв ослоТнСний, ΠΈΠΌΠ΅ΡŽΡ‰ΠΈΡ…ΡΡ Π² нашСй ΠΏΡ€Π°ΠΊΡ‚ΠΈΠΊΠ΅, ΠΌΡ‹ условно Ρ€Π°Π·Π΄Π΅Π»ΠΈΠ»ΠΈ Π½Π° 2 Π³Ρ€ΡƒΠΏΠΏΡ‹: ΠΏΡ€ΠΎΡ‚Π΅Π·Π½Ρ‹ΠΉ сСпсис; ΠΈΠ½Ρ„ΠΈΡ†ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ трансплантата Π±Π΅Π· клиничСских ΠΈ Π»Π°Π±ΠΎΡ€Π°Ρ‚ΠΎΡ€Π½Ρ‹Ρ… проявлСний сСпсиса. Частота Π³Π½ΠΎΠΉΠ½ΠΎ-сСптичСских ослоТнСний составила 9,2 %, ΠΏΠΎΡ‡Ρ‚ΠΈ всС Π±ΠΎΠ»ΡŒΠ½Ρ‹Π΅ ΠΈΠΌΠ΅Π»ΠΈ III–IV ΡΡ‚Π΅ΠΏΠ΅Π½ΡŒ ишСмии ΠΈ Π±Ρ‹Π»ΠΈ ΠΎΠΏΠ΅Ρ€ΠΈΡ€ΠΎΠ²Π°Π½Ρ‹ ΠΏΠΎ Π½Π΅ΠΎΡ‚Π»ΠΎΠΆΠ½Ρ‹ΠΌ показаниям. Π’ 3 случаях инфицирования трансплантата Π±Π΅Π· Π±Π°ΠΊΡ‚Π΅Ρ€ΠΈΠ΅ΠΌΠΈΠΈ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Ρ‹ ΠΎΠΏΠ΅Ρ€ΠΈΡ€ΠΎΠ²Π°Π½Ρ‹ Π΄ΠΎ развития Π°Ρ€Ρ€ΠΎΠ·ΠΈΠ²Π½ΠΎΠ³ΠΎ кровотСчСния, Ρ‡Ρ‚ΠΎ ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΠ»ΠΎ Ρƒ 2 ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ² ΡΠΎΡ…Ρ€Π°Π½ΠΈΡ‚ΡŒ конСчности, ΠΈ ΠΎΠ΄ΠΈΠ½ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ выписан послС выполнСния высокой Π°ΠΌΠΏΡƒΡ‚Π°Ρ†ΠΈΠΈ конСчности.Π’ Π΄Π²ΡƒΡ… случаях Π²Ρ‹ΠΏΠΎΠ»Π½Π΅Π½Π° частичная рСзСкция ΠΈΠ½Ρ„ΠΈΡ†ΠΈΡ€ΠΎΠ²Π°Π½Π½ΠΎΠΉ части Π±ΠΈΡ„ΡƒΡ€ΠΊΠ°Ρ†ΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΏΡ€ΠΎΡ‚Π΅Π·Π° ΠΈΠ· ΠΎΡ‚Π΄Π΅Π»ΡŒΠ½ΠΎΠ³ΠΎ доступа с ΠΏΠΎΡΠ»Π΅Π΄ΡƒΡŽΡ‰Π΅ΠΉ ΠΏΠΎΠ²Ρ‚ΠΎΡ€Π½ΠΎΠΉ рСконструкциСй. Π’ ΠΎΠ΄Π½ΠΎΠΌ случаС Ρƒ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Π° с Π½Π°Ρ€Π°ΡΡ‚Π°ΡŽΡ‰Π΅ΠΉ ишСмиСй конСчности снят ΠΈΠ½Ρ„ΠΈΡ†ΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹ΠΉ Π±ΠΈΡ„ΡƒΡ€ΠΊΠ°Ρ†ΠΈΠΎΠ½Π½Ρ‹ΠΉ ΠΏΡ€ΠΎΡ‚Π΅Π· ΠΈ Π²Ρ‹ΠΏΠΎΠ»Π½Π΅Π½Π° опСрация ΠΏΠΎΠ΄ΠΊΠ»ΡŽΡ‡ΠΈΡ‡Π½ΠΎ-Π±Π΅Π΄Ρ€Π΅Π½Π½ΠΎΠ³ΠΎ экстраанатомичСского ΡˆΡƒΠ½Ρ‚ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΡ с ΠΎΠ΄Π½ΠΎΠΉ стороны ΠΈ высокая ампутация ΠΊΠΎΠ½Ρ‚Ρ€Π»Π°Ρ‚Π΅Ρ€Π°Π»ΡŒΠ½ΠΎΠΉ конСчности. ΠŸΡ€ΠΎΡ‚Π΅Π·Π½Ρ‹ΠΉ сСпсис ΠΈΠΌΠ΅Π» мСсто Ρƒ 2 Π±ΠΎΠ»ΡŒΠ½Ρ‹Ρ…, ΡƒΠΌΠ΅Ρ€ ΠΎΠ΄ΠΈΠ½ больной.ΠœΠ΅Ρ‚Π° Ρ€ΠΎΠ±ΠΎΡ‚ΠΈ: ΠΏΡ€ΠΎΠ°Π½Π°Π»Ρ–Π·ΡƒΠ²Π°Ρ‚ΠΈ частоту Ρ– ΠΏΡ€ΠΈΡ‡ΠΈΠ½ΠΈ Π³Π½Ρ–ΠΉΠ½ΠΎ-сСптичних ΡƒΡΠΊΠ»Π°Π΄Π½Π΅Π½ΡŒ Ρƒ Ρ…Π²ΠΎΡ€ΠΈΡ…, яким Π±ΡƒΠ»ΠΎ Π²ΠΈΠΊΠΎΠ½Π°Π½ΠΎ СндопротСзування Π°ΠΎΡ€Ρ‚ΠΎ-ΠΊΠ»ΡƒΠ±ΠΎΠ²ΠΎΠ³ΠΎ сСгмСнта. ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½ΠΎ Π°Π½Π°Π»Ρ–Π· Π³Π½Ρ–ΠΉΠ½ΠΎ-сСптичних ΡƒΡΠΊΠ»Π°Π΄Π½Π΅Π½ΡŒ Ρƒ 54 Ρ…Π²ΠΎΡ€ΠΈΡ…, які Π±ΡƒΠ»ΠΈ ΠΎΠΏΠ΅Ρ€ΠΎΠ²Π°Π½Ρ– Π· ΠΏΡ€ΠΈΠ²ΠΎΠ΄Ρƒ Ρ–ΡˆΠ΅ΠΌΡ–Ρ‡Π½ΠΈΡ… ΡƒΡ€Π°ΠΆΠ΅Π½ΡŒ судин Π½ΠΈΠΆΠ½Ρ–Ρ… ΠΊΡ–Π½Ρ†Ρ–Π²ΠΎΠΊ Π½Π° Ρ‚Π»Ρ– Ρ†ΡƒΠΊΡ€ΠΎΠ²ΠΎΠ³ΠΎ Π΄Ρ–Π°Π±Π΅Ρ‚Ρƒ. Π£ всіх Ρ…Π²ΠΎΡ€ΠΈΡ… Π±ΡƒΠ»ΠΈ Π²ΠΈΠΊΠΎΠ½Π°Π½Ρ– втручання Π½Π° Π°ΠΎΡ€Ρ‚ΠΎ-ΠΊΠ»ΡƒΠ±ΠΎΠ²ΠΎΠΌΡƒ сСгмСнті Π· використанням синтСтичних судинних ΠΏΡ€ΠΎΡ‚Π΅Π·Ρ–Π². Π’Ρ–Π΄ΠΏΠΎΠ²Ρ–Π΄Π½ΠΎ Π΄ΠΎ класифікації Π³Π½Ρ–ΠΉΠ½ΠΎ-сСптичних ΡƒΡΠΊΠ»Π°Π΄Π½Π΅Π½ΡŒ рСконструктивних ΠΎΠΏΠ΅Ρ€Π°Ρ†Ρ–ΠΉ 5 Π²ΠΈΠΏΠ°Π΄ΠΊΡ–Π² ΡƒΡΠΊΠ»Π°Π΄Π½Π΅Π½ΡŒ, наявних Ρƒ Π½Π°ΡˆΡ–ΠΉ ΠΏΡ€Π°ΠΊΡ‚ΠΈΡ†Ρ–, ΠΌΠΈ ΡƒΠΌΠΎΠ²Π½ΠΎ Ρ€ΠΎΠ·Π΄Ρ–Π»ΠΈΠ»ΠΈ Π½Π° 2 Π³Ρ€ΡƒΠΏΠΈ: ΠΏΡ€ΠΎΡ‚Π΅Π·Π½ΠΈΠΉ сСпсис; інфікування трансплантата Π±Π΅Π· ΠΊΠ»Ρ–Π½Ρ–Ρ‡Π½ΠΈΡ… Ρ‚Π° Π»Π°Π±ΠΎΡ€Π°Ρ‚ΠΎΡ€Π½ΠΈΡ… проявів сСпсису.Частота Π³Π½Ρ–ΠΉΠ½ΠΎ-сСптичних ΡƒΡΠΊΠ»Π°Π΄Π½Π΅Π½ΡŒ становила 9,2 %, ΠΌΠ°ΠΉΠΆΠ΅ всі Ρ…Π²ΠΎΡ€Ρ– ΠΌΠ°Π»ΠΈ III–IV ΡΡ‚ΡƒΠΏΡ–Π½ΡŒ Ρ–ΡˆΠ΅ΠΌΡ–Ρ— Ρ– Π±ΡƒΠ»ΠΈ ΠΎΠΏΠ΅Ρ€ΠΎΠ²Π°Π½Ρ– Π·Π° Π½Π΅Π²Ρ–Π΄ΠΊΠ»Π°Π΄Π½ΠΈΠΌΠΈ показаннями. Π£ 3 Π²ΠΈΠΏΠ°Π΄ΠΊΠ°Ρ… інфікування трансплантата Π±Π΅Π· Π±Π°ΠΊΡ‚Π΅Ρ€Ρ–Ρ”ΠΌΡ–Ρ— ΠΏΠ°Ρ†Ρ–Ρ”Π½Ρ‚ΠΈ ΠΎΠΏΠ΅Ρ€ΠΎΠ²Π°Π½Ρ– Π΄ΠΎ Ρ€ΠΎΠ·Π²ΠΈΡ‚ΠΊΡƒ Π°Ρ€ΠΎΠ·ΠΈΠ²Π½ΠΎΡ— ΠΊΡ€ΠΎΠ²ΠΎΡ‚Π΅Ρ‡Ρ–, Ρ‰ΠΎ Π΄ΠΎΠ·Π²ΠΎΠ»ΠΈΠ»ΠΎ Ρƒ 2 ΠΏΠ°Ρ†Ρ–Ρ”Π½Ρ‚Ρ–Π² Π·Π±Π΅Ρ€Π΅Π³Ρ‚ΠΈ ΠΊΡ–Π½Ρ†Ρ–Π²ΠΊΠΈ, Ρ– ΠΎΠ΄Π½ΠΎΠ³ΠΎ ΠΏΠ°Ρ†Ρ–Ρ”Π½Ρ‚Π° виписали після виконання високої Π°ΠΌΠΏΡƒΡ‚Π°Ρ†Ρ–Ρ— ΠΊΡ–Π½Ρ†Ρ–Π²ΠΊΠΈ. Π£ Π΄Π²ΠΎΡ… Π²ΠΈΠΏΠ°Π΄ΠΊΠ°Ρ… Π²ΠΈΠΊΠΎΠ½Π°Π½Π° часткова рСзСкція Ρ–Π½Ρ„Ρ–ΠΊΠΎΠ²Π°Π½ΠΎΡ— частини Π±Ρ–Ρ„ΡƒΡ€ΠΊΠ°Ρ†Ρ–ΠΉΠ½ΠΈΡ… ΠΏΡ€ΠΎΡ‚Π΅Π·Π° Π· ΠΎΠΊΡ€Π΅ΠΌΠΎΠ³ΠΎ доступу Π· Π½Π°ΡΡ‚ΡƒΠΏΠ½ΠΎΡŽ ΠΏΠΎΠ²Ρ‚ΠΎΡ€Π½ΠΎΡŽ Ρ€Π΅ΠΊΠΎΠ½ΡΡ‚Ρ€ΡƒΠΊΡ†Ρ–Ρ”ΡŽ. Π’ ΠΎΠ΄Π½ΠΎΠΌΡƒ Π²ΠΈΠΏΠ°Π΄ΠΊΡƒ Ρƒ ΠΏΠ°Ρ†Ρ–Ρ”Π½Ρ‚Π° Π· Π½Π°Ρ€ΠΎΡΡ‚Π°ΡŽΡ‡ΠΎΡŽ Ρ–ΡˆΠ΅ΠΌΡ–Ρ”ΡŽ ΠΊΡ–Π½Ρ†Ρ–Π²ΠΊΠΈ знятий Ρ–Π½Ρ„Ρ–ΠΊΠΎΠ²Π°Π½ΠΈΠΉ Π±Ρ–Ρ„ΡƒΡ€ΠΊΠ°Ρ†Ρ–ΠΉΠ½ΠΈΠΉ ΠΏΡ€ΠΎΡ‚Π΅Π·, Ρ– Π²ΠΈΠΊΠΎΠ½Π°Π½Π° опСрація ΠΏΠΎΠ΄ΠΊΠ»ΡŽΡ‡ΠΈΡ‡Π½ΠΎ-стСгнового Скстраанатомічного ΡˆΡƒΠ½Ρ‚ΡƒΠ²Π°Π½Π½Ρ Π· ΠΎΠ΄Π½ΠΎΠ³ΠΎ Π±ΠΎΠΊΡƒ, Ρ– висока ампутація ΠΊΠΎΠ½Ρ‚Ρ€Π»Π°Ρ‚Π΅Ρ€Π°Π»ΡŒΠ½ΠΎΡ— ΠΊΡ–Π½Ρ†Ρ–Π²ΠΊΠΈ. ΠŸΡ€ΠΎΡ‚Π΅Π·Π½ΠΈΠΉ сСпсис ΠΌΠ°Π² місцС Ρƒ 2 Ρ…Π²ΠΎΡ€ΠΈΡ…, ΠΏΠΎΠΌΠ΅Ρ€ ΠΎΠ΄ΠΈΠ½ Ρ…Π²ΠΎΡ€ΠΈΠΉ

    PG 1115+080: variations of the A2/A1 flux ratio and new values of the time delays

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    We report the results of our multicolor observations of PG 1115+080 with the 1.5-m telescope of the Maidanak Observatory (Uzbekistan, Central Asia) in 2001-2006. Monitoring data in filter R spanning the 2004, 2005 and 2006 seasons (76 data points) demonstrate distinct brightness variations of the source quasar with the total amplitude of almost 0.4 mag. Our R light curves have shown image C leading B by 16.4d and image (A1+A2) by 12d that is inconsistent with the previous estimates obtained by Schechter et al. in 1997 - 24.7d between B and C and 9.4d between (A1+A2) and C. The new values of time delays in PG 1115+080 must result in larger values for the Hubble constant, thus reducing difference between its estimates taken from the gravitational lenses and with other methods. Also, we analyzed variability of the A2/A1 flux ratio, as well as color changes in the archetypal "fold" lens PG 1115+080. We found the A1/A2 flux ratio to grow during 2001-2006 and to be larger at longer wavelengths. In particular, the A2/A1 flux ratio reached 0.85 in filter I in 2006. We also present evidence that both the A1 and A2 images might have undergone microlensing during 2001-2006, with the descending phase for A1 and initial phase for A2. We find that the A2/A1 flux ratio anomaly in PG 1115 can be well explained both by microlensing and by finite distance of the source quasar from the caustic fold.Comment: 14 pages, 7 figures, 8 tables, Accepted for publication in MNRA

    Π˜ΠΌΠΈΡ‚Π°Ρ†ΠΈΠΎΠ½Π½ΠΎΠ΅ ΠΌΠΎΠ΄Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΌΠ΅Ρ‚ΠΎΠ΄Π° ΠΎΡ†Π΅Π½ΠΊΠΈ защищСнности ΠΊΠ°Π½Π°Π»Π° ΡƒΡ‚Π΅Ρ‡ΠΊΠΈ ΠΈΠ½Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΈ ΠΏΠΎ ΠΎΠ³ΠΈΠ±Π°ΡŽΡ‰Π΅ΠΉ Ρ€Π΅Ρ‡Π΅Π²ΠΎΠ³ΠΎ сигнала

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    A method of information leakage channel security estimating based on the test speech signal envelope cross-correlation analysis is proposed and its includes: test signal generating and extracting its envelope, emitting and measuring in a leakage channel, extracting the resulting signal envelope, calculating the correlation coefficient between the original and received envelopes, and comparing with a threshold value. A metod for extracting a low-frequency signal envelope using the Hilbert transform is shown. A description of the cross-correlation analysis based on the Pearson correlation coefficient is given. The leakage channel simulation modeling, formation and measurement of the test signals was performed in the MatLab. The obtained results confirm the greater efficiency of using the envelope compared to the original signal, and demonstrate the speech signals advantage over harmonic signals as test signals for assessing the information leakage channel security.ΠŸΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½ ΠΌΠ΅Ρ‚ΠΎΠ΄ ΠΎΡ†Π΅Π½ΠΊΠΈ защищСнности ΠΊΠ°Π½Π°Π»Π° ΡƒΡ‚Π΅Ρ‡ΠΊΠΈ ΠΈΠ½Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΈ Π½Π° основС Π²Π·Π°ΠΈΠΌΠ½ΠΎ- коррСляционного Π°Π½Π°Π»ΠΈΠ·Π° ΠΎΠ³ΠΈΠ±Π°ΡŽΡ‰Π΅ΠΉ ΠΈΠ·ΠΌΠ΅Ρ€ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠ³ΠΎ сигнала Π² Ρ€Π΅Ρ‡Π΅Π²ΠΎΠΌ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π΅ частот. Алгоритм Π²ΠΊΠ»ΡŽΡ‡Π°Π΅Ρ‚ Π³Π΅Π½Π΅Ρ€Π°Ρ†ΠΈΡŽ ΠΈΠ·ΠΌΠ΅Ρ€ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠ³ΠΎ сигнала ΠΈ Π²Ρ‹Π΄Π΅Π»Π΅Π½ΠΈΠ΅ Π΅Π³ΠΎ ΠΎΠ³ΠΈΠ±Π°ΡŽΡ‰Π΅ΠΉ, ΠΈΠ·Π»ΡƒΡ‡Π΅Π½ΠΈΠ΅ ΠΈ ΠΈΠ·ΠΌΠ΅Ρ€Π΅Π½ΠΈΠ΅ Π² ΠΊΠ°Π½Π°Π»Π΅ ΡƒΡ‚Π΅Ρ‡ΠΊΠΈ, Π²Ρ‹Π΄Π΅Π»Π΅Π½ΠΈΠ΅ ΠΎΠ³ΠΈΠ±Π°ΡŽΡ‰Π΅ΠΉ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚ΠΈΡ€ΡƒΡŽΡ‰Π΅Π³ΠΎ сигнала, вычислСниС коэффициСнта коррСляции ΠΌΠ΅ΠΆΠ΄Ρƒ исходной ΠΈ ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½ΠΎΠΉ ΠΎΠ³ΠΈΠ±Π°ΡŽΡ‰ΠΈΠΌΠΈ, сравнСниС с ΠΏΠΎΡ€ΠΎΠ³ΠΎΠ²Ρ‹ΠΌ Π·Π½Π°Ρ‡Π΅Π½ΠΈΠ΅ΠΌ. Описан ΠΌΠ΅Ρ‚ΠΎΠ΄ выдСлСния низкочастотной ΠΎΠ³ΠΈΠ±Π°ΡŽΡ‰Π΅ΠΉ сигнала с ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽ прСобразования Π“ΠΈΠ»ΡŒΠ±Π΅Ρ€Ρ‚Π°. ΠŸΡ€ΠΈΠ²Π΅Π΄Π΅Π½ΠΎ описаниС Π²Π·Π°ΠΈΠΌΠ½ΠΎ-коррСляционного Π°Π½Π°Π»ΠΈΠ·Π° Π½Π° основС коэффициСнта коррСляции ΠŸΠΈΡ€ΡΠΎΠ½Π°. Π’Ρ‹ΠΏΠΎΠ»Π½Π΅Π½ΠΎ ΠΈΠΌΠΈΡ‚Π°Ρ†ΠΈΠΎΠ½Π½ΠΎΠ΅ ΠΌΠΎΠ΄Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΊΠ°Π½Π°Π»Π° ΡƒΡ‚Π΅Ρ‡ΠΊΠΈ, формирования ΠΈ измСрСния ΠΈΠ·ΠΌΠ΅Ρ€ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… сигналов, Π° Ρ‚Π°ΠΊΠΆΠ΅ ΠΈΡ… ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚ΠΊΠ° Π² ΠΏΡ€ΠΎΠ³Ρ€Π°ΠΌΠΌΠ½ΠΎΠΉ срСдС MatLab. ΠŸΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Π΅ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ ΠΏΠΎΠ΄Ρ‚Π²Π΅Ρ€ΠΆΠ΄Π°ΡŽΡ‚ Π±ΠΎΠ»ΡŒΡˆΡƒΡŽ ΡΡ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ использования ΠΎΠ³ΠΈΠ±Π°ΡŽΡ‰Π΅ΠΉ ΠΏΠΎ ΡΡ€Π°Π²Π½Π΅Π½ΠΈΡŽ с исходным сигналом, Π° Ρ‚Π°ΠΊΠΆΠ΅ Π΄Π΅ΠΌΠΎΠ½ΡΡ‚Ρ€ΠΈΡ€ΡƒΡŽΡ‚ прСимущСство Ρ€Π΅Ρ‡Π΅Π²Ρ‹Ρ… сигналов ΠΏΠ΅Ρ€Π΅Π΄ гармоничСскими сигналами Π² качСствС ΠΈΠ·ΠΌΠ΅Ρ€ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… для ΠΎΡ†Π΅Π½ΠΊΠΈ защищСнности ΠΊΠ°Π½Π°Π»Π° ΡƒΡ‚Π΅Ρ‡ΠΊΠΈ ΠΈΠ½Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΈ

    Correlation functions for a two-dimensional electron system with bosonic interactions and a square Fermi surface

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    We calculate zero-temperature correlation functions for a model of 2D interacting electrons with short-range interactions and a square Fermi surface. The model was arrived at by mapping electronic states near a square Fermi surface with Hubbard-like interactions onto one-dimensional quantum chains, retaining terms which can be written in terms of bosonic density operators. Interactions between orthogonal chains, corresponding to orthogonal faces of the square Fermi surface, are neglected. The correlation functions become sums of Luttinger-type correlation functions due to the bosonic model. However, the correlation function exponents differ in form from those of the Luttinger model. As a consequence, the simple scaling relations found to exist between the Luttinger model exponents, do not carry over to the leading exponents of our model. We find that for repulsive effective interactions, charge-density wave/spin-density wave instabilities are dominant. We do not consider d-wave instabilities here.Comment: 12 pages, no figures; to be published in Physical Review

    Mid-infrared Hall effect in thin-film metals: Probing the Fermi surface anisotropy in Au and Cu

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    A sensitive mid-infrared (MIR, 900-1100 cm-1, 112-136 meV) photo-elastic polarization modulation technique is used to measure simultaneously Faraday rotation and circular dichroism in thin metal films. These two quantities determine the complex AC Hall conductivity. This novel technique is applied to study Au and Cu thin films at temperatures down to 20 K and magnetic fields up to 8 T. The Hall frequency is consistent with band theory predictions. We report the first measurement of the MIR Hall scattering rate, which is significantly lower than that derived from Drude analysis of zero magnetic field MIR transmission measurements. This difference is qualitatively explained in terms of the anisotropy of the Fermi surface in Au and Cu.Comment: 14 pages of text, 5 figure

    Probing photo-ionization: simulations of positive streamers in varying N2:O2 mixtures

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    Photo-ionization is the accepted mechanism for the propagation of positive streamers in air though the parameters are not very well known; the efficiency of this mechanism largely depends on the presence of both nitrogen and oxygen. But experiments show that streamer propagation is amazingly robust against changes of the gas composition; even for pure nitrogen with impurity levels below 1 ppm streamers propagate essentially with the same velocity as in air, but their minimal diameter is smaller, and they branch more frequently. Additionally, they move more in a zigzag fashion and sometimes exhibit a feathery structure. In our simulations, we test the relative importance of photo-ionization and of the background ionization from pulsed repetitive discharges, in air as well as in nitrogen with 1 ppm O2 . We also test reasonable parameter changes of the photo-ionization model. We find that photo- ionization dominates streamer propagation in air for repetition frequencies of at least 1 kHz, while in nitrogen with 1 ppm O2 the effect of the repetition frequency has to be included above 1 Hz. Finally, we explain the feather-like structures around streamer channels that are observed in experiments in nitrogen with high purity, but not in air.Comment: 12 figure

    Exact solution of a 2D interacting fermion model

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    We study an exactly solvable quantum field theory (QFT) model describing interacting fermions in 2+1 dimensions. This model is motivated by physical arguments suggesting that it provides an effective description of spinless fermions on a square lattice with local hopping and density-density interactions if, close to half filling, the system develops a partial energy gap. The necessary regularization of the QFT model is based on this proposed relation to lattice fermions. We use bosonization methods to diagonalize the Hamiltonian and to compute all correlation functions. We also discuss how, after appropriate multiplicative renormalizations, all short- and long distance cutoffs can be removed. In particular, we prove that the renormalized two-point functions have algebraic decay with non-trivial exponents depending on the interaction strengths, which is a hallmark of Luttinger-liquid behavior.Comment: 59 pages, 3 figures, v2: further references added; additional subsections elaborating mathematical details; additional appendix with details on the relation to lattice fermion
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