71 research outputs found
Color Effects Associated with the 1999 Microlensing Brightness Peaks in Gravitationally Lensed Quasar Q2237+0305
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
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
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
ΠΡΠΎΠ±Π»Π΅ΠΌΠ° Ρ ΠΈΡΡΡΠ³ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΈΠ½ΡΠ΅ΠΊΡΠΈΠΈ Ρ Π±ΠΎΠ»ΡΠ½ΡΡ Π‘Π°Ρ Π°ΡΠ½ΡΠΌ Π΄ΠΈΠ°Π±Π΅ΡΠΎΠΌ, ΠΎΠΏΠ΅ΡΠΈΡΠΎΠ²Π°Π½Π½ΡΡ Π½Π° Π°ΠΎΡΡΠΎ-ΠΏΠΎΠ΄Π²Π·Π΄ΠΎΡΠ½ΠΎΠΌ ΡΠ΅Π³ΠΌΠ΅Π½ΡΠ΅
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 β 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.Π¦Π΅Π»Ρ ΡΠ°Π±ΠΎΡΡ: ΠΏΡΠΎΠ°Π½Π°Π»ΠΈΠ·ΠΈΡΠΎΠ²Π°ΡΡ ΡΠ°ΡΡΠΎΡΡ ΠΈ ΠΏΡΠΈΡΠΈΠ½Ρ Π³Π½ΠΎΠΉΠ½ΠΎ-ΡΠ΅ΠΏΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΎΡΠ»ΠΎΠΆΠ½Π΅Π½ΠΈΠΉ Ρ Π±ΠΎΠ»ΡΠ½ΡΡ
, ΠΊΠΎΡΠΎΡΡΠΌ Π²ΡΠΏΠΎΠ»Π½Π΅Π½ΠΎ ΡΠ½Π΄ΠΎΠΏΡΠΎΡΠ΅Π·ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ Π°ΠΎΡΡΠΎ-ΠΏΠΎΠ΄Π²Π·Π΄ΠΎΡΠ½ΠΎΠ³ΠΎ ΡΠ΅Π³ΠΌΠ΅Π½ΡΠ°. ΠΡΠΎΠ²Π΅Π΄Π΅Π½ Π°Π½Π°Π»ΠΈΠ· Π³Π½ΠΎΠΉΠ½ΠΎ-ΡΠ΅ΠΏΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΎΡΠ»ΠΎΠΆΠ½Π΅Π½ΠΈΠΉ Ρ 54 Π±ΠΎΠ»ΡΠ½ΡΡ
, ΠΊΠΎΡΠΎΡΡΠ΅ Π±ΡΠ»ΠΈ ΠΎΠΏΠ΅ΡΠΈΡΠΎΠ²Π°Π½Ρ ΠΏΠΎ ΠΏΠΎΠ²ΠΎΠ΄Ρ ΠΈΡΠ΅ΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠΎΡΠ°ΠΆΠ΅Π½ΠΈΠΉ ΡΠΎΡΡΠ΄ΠΎΠ² Π½ΠΈΠΆΠ½ΠΈΡ
ΠΊΠΎΠ½Π΅ΡΠ½ΠΎΡΡΠ΅ΠΉ Π½Π° ΡΠΎΠ½Π΅ ΡΠ°Ρ
Π°ΡΠ½ΠΎΠ³ΠΎ Π΄ΠΈΠ°Π±Π΅ΡΠ°. Π£ Π²ΡΠ΅Ρ
Π±ΠΎΠ»ΡΠ½ΡΡ
Π±ΡΠ»ΠΈ Π²ΡΠΏΠΎΠ»Π½Π΅Π½Ρ Π²ΠΌΠ΅ΡΠ°ΡΠ΅Π»ΡΡΡΠ²Π° Π½Π° Π°ΠΎΡΡΠΎ-ΠΏΠΎΠ΄Π²Π·Π΄ΠΎΡΠ½ΠΎΠΌ ΡΠ΅Π³ΠΌΠ΅Π½ΡΠ΅ Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΡΠΈΠ½ΡΠ΅ΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠΎΡΡΠ΄ΠΈΡΡΡΡ
ΠΏΡΠΎΡΠ΅Π·ΠΎΠ². Π ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΠΈΠΈ Ρ ΠΊΠ»Π°ΡΡΠΈΡΠΈΠΊΠ°ΡΠΈΠ΅ΠΉ Π³Π½ΠΎΠΉΠ½ΠΎ-ΡΠ΅ΠΏΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΎΡΠ»ΠΎΠΆΠ½Π΅Π½ΠΈΠΉ ΡΠ΅ΠΊΠΎΠ½ΡΡΡΡΠΊΡΠΈΠ²Π½ΡΡ
ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΉ 5 ΡΠ»ΡΡΠ°Π΅Π² ΠΎΡΠ»ΠΎΠΆΠ½Π΅Π½ΠΈΠΉ, ΠΈΠΌΠ΅ΡΡΠΈΡ
ΡΡ Π² Π½Π°ΡΠ΅ΠΉ ΠΏΡΠ°ΠΊΡΠΈΠΊΠ΅, ΠΌΡ ΡΡΠ»ΠΎΠ²Π½ΠΎ ΡΠ°Π·Π΄Π΅Π»ΠΈΠ»ΠΈ Π½Π° 2 Π³ΡΡΠΏΠΏΡ: ΠΏΡΠΎΡΠ΅Π·Π½ΡΠΉ ΡΠ΅ΠΏΡΠΈΡ; ΠΈΠ½ΡΠΈΡΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΡΡΠ°Π½ΡΠΏΠ»Π°Π½ΡΠ°ΡΠ° Π±Π΅Π· ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈ Π»Π°Π±ΠΎΡΠ°ΡΠΎΡΠ½ΡΡ
ΠΏΡΠΎΡΠ²Π»Π΅Π½ΠΈΠΉ ΡΠ΅ΠΏΡΠΈΡΠ°. Π§Π°ΡΡΠΎΡΠ° Π³Π½ΠΎΠΉΠ½ΠΎ-ΡΠ΅ΠΏΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΎΡΠ»ΠΎΠΆΠ½Π΅Π½ΠΈΠΉ ΡΠΎΡΡΠ°Π²ΠΈΠ»Π° 9,2 %, ΠΏΠΎΡΡΠΈ Π²ΡΠ΅ Π±ΠΎΠ»ΡΠ½ΡΠ΅ ΠΈΠΌΠ΅Π»ΠΈ IIIβIV ΡΡΠ΅ΠΏΠ΅Π½Ρ ΠΈΡΠ΅ΠΌΠΈΠΈ ΠΈ Π±ΡΠ»ΠΈ ΠΎΠΏΠ΅ΡΠΈΡΠΎΠ²Π°Π½Ρ ΠΏΠΎ Π½Π΅ΠΎΡΠ»ΠΎΠΆΠ½ΡΠΌ ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΈΡΠΌ. Π 3 ΡΠ»ΡΡΠ°ΡΡ
ΠΈΠ½ΡΠΈΡΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΡΡΠ°Π½ΡΠΏΠ»Π°Π½ΡΠ°ΡΠ° Π±Π΅Π· Π±Π°ΠΊΡΠ΅ΡΠΈΠ΅ΠΌΠΈΠΈ ΠΏΠ°ΡΠΈΠ΅Π½ΡΡ ΠΎΠΏΠ΅ΡΠΈΡΠΎΠ²Π°Π½Ρ Π΄ΠΎ ΡΠ°Π·Π²ΠΈΡΠΈΡ Π°ΡΡΠΎΠ·ΠΈΠ²Π½ΠΎΠ³ΠΎ ΠΊΡΠΎΠ²ΠΎΡΠ΅ΡΠ΅Π½ΠΈΡ, ΡΡΠΎ ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΠ»ΠΎ Ρ 2 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² ΡΠΎΡ
ΡΠ°Π½ΠΈΡΡ ΠΊΠΎΠ½Π΅ΡΠ½ΠΎΡΡΠΈ, ΠΈ ΠΎΠ΄ΠΈΠ½ ΠΏΠ°ΡΠΈΠ΅Π½Ρ Π²ΡΠΏΠΈΡΠ°Π½ ΠΏΠΎΡΠ»Π΅ Π²ΡΠΏΠΎΠ»Π½Π΅Π½ΠΈΡ Π²ΡΡΠΎΠΊΠΎΠΉ Π°ΠΌΠΏΡΡΠ°ΡΠΈΠΈ ΠΊΠΎΠ½Π΅ΡΠ½ΠΎΡΡΠΈ.Π Π΄Π²ΡΡ
ΡΠ»ΡΡΠ°ΡΡ
Π²ΡΠΏΠΎΠ»Π½Π΅Π½Π° ΡΠ°ΡΡΠΈΡΠ½Π°Ρ ΡΠ΅Π·Π΅ΠΊΡΠΈΡ ΠΈΠ½ΡΠΈΡΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΉ ΡΠ°ΡΡΠΈ Π±ΠΈΡΡΡΠΊΠ°ΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΏΡΠΎΡΠ΅Π·Π° ΠΈΠ· ΠΎΡΠ΄Π΅Π»ΡΠ½ΠΎΠ³ΠΎ Π΄ΠΎΡΡΡΠΏΠ° Ρ ΠΏΠΎΡΠ»Π΅Π΄ΡΡΡΠ΅ΠΉ ΠΏΠΎΠ²ΡΠΎΡΠ½ΠΎΠΉ ΡΠ΅ΠΊΠΎΠ½ΡΡΡΡΠΊΡΠΈΠ΅ΠΉ. Π ΠΎΠ΄Π½ΠΎΠΌ ΡΠ»ΡΡΠ°Π΅ Ρ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠ° Ρ Π½Π°ΡΠ°ΡΡΠ°ΡΡΠ΅ΠΉ ΠΈΡΠ΅ΠΌΠΈΠ΅ΠΉ ΠΊΠΎΠ½Π΅ΡΠ½ΠΎΡΡΠΈ ΡΠ½ΡΡ ΠΈΠ½ΡΠΈΡΠΈΡΠΎΠ²Π°Π½Π½ΡΠΉ Π±ΠΈΡΡΡΠΊΠ°ΡΠΈΠΎΠ½Π½ΡΠΉ ΠΏΡΠΎΡΠ΅Π· ΠΈ Π²ΡΠΏΠΎΠ»Π½Π΅Π½Π° ΠΎΠΏΠ΅ΡΠ°ΡΠΈΡ ΠΏΠΎΠ΄ΠΊΠ»ΡΡΠΈΡΠ½ΠΎ-Π±Π΅Π΄ΡΠ΅Π½Π½ΠΎΠ³ΠΎ ΡΠΊΡΡΡΠ°Π°Π½Π°ΡΠΎΠΌΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΡΠ½ΡΠΈΡΠΎΠ²Π°Π½ΠΈΡ Ρ ΠΎΠ΄Π½ΠΎΠΉ ΡΡΠΎΡΠΎΠ½Ρ ΠΈ Π²ΡΡΠΎΠΊΠ°Ρ Π°ΠΌΠΏΡΡΠ°ΡΠΈΡ ΠΊΠΎΠ½ΡΡΠ»Π°ΡΠ΅ΡΠ°Π»ΡΠ½ΠΎΠΉ ΠΊΠΎΠ½Π΅ΡΠ½ΠΎΡΡΠΈ. ΠΡΠΎΡΠ΅Π·Π½ΡΠΉ ΡΠ΅ΠΏΡΠΈΡ ΠΈΠΌΠ΅Π» ΠΌΠ΅ΡΡΠΎ Ρ 2 Π±ΠΎΠ»ΡΠ½ΡΡ
, ΡΠΌΠ΅Ρ ΠΎΠ΄ΠΈΠ½ Π±ΠΎΠ»ΡΠ½ΠΎΠΉ.ΠΠ΅ΡΠ° ΡΠΎΠ±ΠΎΡΠΈ: ΠΏΡΠΎΠ°Π½Π°Π»ΡΠ·ΡΠ²Π°ΡΠΈ ΡΠ°ΡΡΠΎΡΡ Ρ ΠΏΡΠΈΡΠΈΠ½ΠΈ Π³Π½ΡΠΉΠ½ΠΎ-ΡΠ΅ΠΏΡΠΈΡΠ½ΠΈΡ
ΡΡΠΊΠ»Π°Π΄Π½Π΅Π½Ρ Ρ Ρ
Π²ΠΎΡΠΈΡ
, ΡΠΊΠΈΠΌ Π±ΡΠ»ΠΎ Π²ΠΈΠΊΠΎΠ½Π°Π½ΠΎ Π΅Π½Π΄ΠΎΠΏΡΠΎΡΠ΅Π·ΡΠ²Π°Π½Π½Ρ Π°ΠΎΡΡΠΎ-ΠΊΠ»ΡΠ±ΠΎΠ²ΠΎΠ³ΠΎ ΡΠ΅Π³ΠΌΠ΅Π½ΡΠ°. ΠΡΠΎΠ²Π΅Π΄Π΅Π½ΠΎ Π°Π½Π°Π»ΡΠ· Π³Π½ΡΠΉΠ½ΠΎ-ΡΠ΅ΠΏΡΠΈΡΠ½ΠΈΡ
ΡΡΠΊΠ»Π°Π΄Π½Π΅Π½Ρ Ρ 54 Ρ
Π²ΠΎΡΠΈΡ
, ΡΠΊΡ Π±ΡΠ»ΠΈ ΠΎΠΏΠ΅ΡΠΎΠ²Π°Π½Ρ Π· ΠΏΡΠΈΠ²ΠΎΠ΄Ρ ΡΡΠ΅ΠΌΡΡΠ½ΠΈΡ
ΡΡΠ°ΠΆΠ΅Π½Ρ ΡΡΠ΄ΠΈΠ½ Π½ΠΈΠΆΠ½ΡΡ
ΠΊΡΠ½ΡΡΠ²ΠΎΠΊ Π½Π° ΡΠ»Ρ ΡΡΠΊΡΠΎΠ²ΠΎΠ³ΠΎ Π΄ΡΠ°Π±Π΅ΡΡ. Π£ Π²ΡΡΡ
Ρ
Π²ΠΎΡΠΈΡ
Π±ΡΠ»ΠΈ Π²ΠΈΠΊΠΎΠ½Π°Π½Ρ Π²ΡΡΡΡΠ°Π½Π½Ρ Π½Π° Π°ΠΎΡΡΠΎ-ΠΊΠ»ΡΠ±ΠΎΠ²ΠΎΠΌΡ ΡΠ΅Π³ΠΌΠ΅Π½ΡΡ Π· Π²ΠΈΠΊΠΎΡΠΈΡΡΠ°Π½Π½ΡΠΌ ΡΠΈΠ½ΡΠ΅ΡΠΈΡΠ½ΠΈΡ
ΡΡΠ΄ΠΈΠ½Π½ΠΈΡ
ΠΏΡΠΎΡΠ΅Π·ΡΠ². ΠΡΠ΄ΠΏΠΎΠ²ΡΠ΄Π½ΠΎ Π΄ΠΎ ΠΊΠ»Π°ΡΠΈΡΡΠΊΠ°ΡΡΡ Π³Π½ΡΠΉΠ½ΠΎ-ΡΠ΅ΠΏΡΠΈΡΠ½ΠΈΡ
ΡΡΠΊΠ»Π°Π΄Π½Π΅Π½Ρ ΡΠ΅ΠΊΠΎΠ½ΡΡΡΡΠΊΡΠΈΠ²Π½ΠΈΡ
ΠΎΠΏΠ΅ΡΠ°ΡΡΠΉ 5 Π²ΠΈΠΏΠ°Π΄ΠΊΡΠ² ΡΡΠΊΠ»Π°Π΄Π½Π΅Π½Ρ, Π½Π°ΡΠ²Π½ΠΈΡ
Ρ Π½Π°ΡΡΠΉ ΠΏΡΠ°ΠΊΡΠΈΡΡ, ΠΌΠΈ ΡΠΌΠΎΠ²Π½ΠΎ ΡΠΎΠ·Π΄ΡΠ»ΠΈΠ»ΠΈ Π½Π° 2 Π³ΡΡΠΏΠΈ: ΠΏΡΠΎΡΠ΅Π·Π½ΠΈΠΉ ΡΠ΅ΠΏΡΠΈΡ; ΡΠ½ΡΡΠΊΡΠ²Π°Π½Π½Ρ ΡΡΠ°Π½ΡΠΏΠ»Π°Π½ΡΠ°ΡΠ° Π±Π΅Π· ΠΊΠ»ΡΠ½ΡΡΠ½ΠΈΡ
ΡΠ° Π»Π°Π±ΠΎΡΠ°ΡΠΎΡΠ½ΠΈΡ
ΠΏΡΠΎΡΠ²ΡΠ² ΡΠ΅ΠΏΡΠΈΡΡ.Π§Π°ΡΡΠΎΡΠ° Π³Π½ΡΠΉΠ½ΠΎ-ΡΠ΅ΠΏΡΠΈΡΠ½ΠΈΡ
ΡΡΠΊΠ»Π°Π΄Π½Π΅Π½Ρ ΡΡΠ°Π½ΠΎΠ²ΠΈΠ»Π° 9,2 %, ΠΌΠ°ΠΉΠΆΠ΅ Π²ΡΡ Ρ
Π²ΠΎΡΡ ΠΌΠ°Π»ΠΈ IIIβIV ΡΡΡΠΏΡΠ½Ρ ΡΡΠ΅ΠΌΡΡ Ρ Π±ΡΠ»ΠΈ ΠΎΠΏΠ΅ΡΠΎΠ²Π°Π½Ρ Π·Π° Π½Π΅Π²ΡΠ΄ΠΊΠ»Π°Π΄Π½ΠΈΠΌΠΈ ΠΏΠΎΠΊΠ°Π·Π°Π½Π½ΡΠΌΠΈ. Π£ 3 Π²ΠΈΠΏΠ°Π΄ΠΊΠ°Ρ
ΡΠ½ΡΡΠΊΡΠ²Π°Π½Π½Ρ ΡΡΠ°Π½ΡΠΏΠ»Π°Π½ΡΠ°ΡΠ° Π±Π΅Π· Π±Π°ΠΊΡΠ΅ΡΡΡΠΌΡΡ ΠΏΠ°ΡΡΡΠ½ΡΠΈ ΠΎΠΏΠ΅ΡΠΎΠ²Π°Π½Ρ Π΄ΠΎ ΡΠΎΠ·Π²ΠΈΡΠΊΡ Π°ΡΠΎΠ·ΠΈΠ²Π½ΠΎΡ ΠΊΡΠΎΠ²ΠΎΡΠ΅ΡΡ, ΡΠΎ Π΄ΠΎΠ·Π²ΠΎΠ»ΠΈΠ»ΠΎ Ρ 2 ΠΏΠ°ΡΡΡΠ½ΡΡΠ² Π·Π±Π΅ΡΠ΅Π³ΡΠΈ ΠΊΡΠ½ΡΡΠ²ΠΊΠΈ, Ρ ΠΎΠ΄Π½ΠΎΠ³ΠΎ ΠΏΠ°ΡΡΡΠ½ΡΠ° Π²ΠΈΠΏΠΈΡΠ°Π»ΠΈ ΠΏΡΡΠ»Ρ Π²ΠΈΠΊΠΎΠ½Π°Π½Π½Ρ Π²ΠΈΡΠΎΠΊΠΎΡ Π°ΠΌΠΏΡΡΠ°ΡΡΡ ΠΊΡΠ½ΡΡΠ²ΠΊΠΈ. Π£ Π΄Π²ΠΎΡ
Π²ΠΈΠΏΠ°Π΄ΠΊΠ°Ρ
Π²ΠΈΠΊΠΎΠ½Π°Π½Π° ΡΠ°ΡΡΠΊΠΎΠ²Π° ΡΠ΅Π·Π΅ΠΊΡΡΡ ΡΠ½ΡΡΠΊΠΎΠ²Π°Π½ΠΎΡ ΡΠ°ΡΡΠΈΠ½ΠΈ Π±ΡΡΡΡΠΊΠ°ΡΡΠΉΠ½ΠΈΡ
ΠΏΡΠΎΡΠ΅Π·Π° Π· ΠΎΠΊΡΠ΅ΠΌΠΎΠ³ΠΎ Π΄ΠΎΡΡΡΠΏΡ Π· Π½Π°ΡΡΡΠΏΠ½ΠΎΡ ΠΏΠΎΠ²ΡΠΎΡΠ½ΠΎΡ ΡΠ΅ΠΊΠΎΠ½ΡΡΡΡΠΊΡΡΡΡ. Π ΠΎΠ΄Π½ΠΎΠΌΡ Π²ΠΈΠΏΠ°Π΄ΠΊΡ Ρ ΠΏΠ°ΡΡΡΠ½ΡΠ° Π· Π½Π°ΡΠΎΡΡΠ°ΡΡΠΎΡ ΡΡΠ΅ΠΌΡΡΡ ΠΊΡΠ½ΡΡΠ²ΠΊΠΈ Π·Π½ΡΡΠΈΠΉ ΡΠ½ΡΡΠΊΠΎΠ²Π°Π½ΠΈΠΉ Π±ΡΡΡΡΠΊΠ°ΡΡΠΉΠ½ΠΈΠΉ ΠΏΡΠΎΡΠ΅Π·, Ρ Π²ΠΈΠΊΠΎΠ½Π°Π½Π° ΠΎΠΏΠ΅ΡΠ°ΡΡΡ ΠΏΠΎΠ΄ΠΊΠ»ΡΡΠΈΡΠ½ΠΎ-ΡΡΠ΅Π³Π½ΠΎΠ²ΠΎΠ³ΠΎ Π΅ΠΊΡΡΡΠ°Π°Π½Π°ΡΠΎΠΌΡΡΠ½ΠΎΠ³ΠΎ ΡΡΠ½ΡΡΠ²Π°Π½Π½Ρ Π· ΠΎΠ΄Π½ΠΎΠ³ΠΎ Π±ΠΎΠΊΡ, Ρ Π²ΠΈΡΠΎΠΊΠ° Π°ΠΌΠΏΡΡΠ°ΡΡΡ ΠΊΠΎΠ½ΡΡΠ»Π°ΡΠ΅ΡΠ°Π»ΡΠ½ΠΎΡ ΠΊΡΠ½ΡΡΠ²ΠΊΠΈ. ΠΡΠΎΡΠ΅Π·Π½ΠΈΠΉ ΡΠ΅ΠΏΡΠΈΡ ΠΌΠ°Π² ΠΌΡΡΡΠ΅ Ρ 2 Ρ
Π²ΠΎΡΠΈΡ
, ΠΏΠΎΠΌΠ΅Ρ ΠΎΠ΄ΠΈΠ½ Ρ
Π²ΠΎΡΠΈΠΉ
PG 1115+080: variations of the A2/A1 flux ratio and new values of the time delays
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
ΠΠΌΠΈΡΠ°ΡΠΈΠΎΠ½Π½ΠΎΠ΅ ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΠΌΠ΅ΡΠΎΠ΄Π° ΠΎΡΠ΅Π½ΠΊΠΈ Π·Π°ΡΠΈΡΠ΅Π½Π½ΠΎΡΡΠΈ ΠΊΠ°Π½Π°Π»Π° ΡΡΠ΅ΡΠΊΠΈ ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΠΈ ΠΏΠΎ ΠΎΠ³ΠΈΠ±Π°ΡΡΠ΅ΠΉ ΡΠ΅ΡΠ΅Π²ΠΎΠ³ΠΎ ΡΠΈΠ³Π½Π°Π»Π°
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.ΠΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½ ΠΌΠ΅ΡΠΎΠ΄ ΠΎΡΠ΅Π½ΠΊΠΈ Π·Π°ΡΠΈΡΠ΅Π½Π½ΠΎΡΡΠΈ ΠΊΠ°Π½Π°Π»Π° ΡΡΠ΅ΡΠΊΠΈ ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΠΈ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ Π²Π·Π°ΠΈΠΌΠ½ΠΎ- ΠΊΠΎΡΡΠ΅Π»ΡΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π° ΠΎΠ³ΠΈΠ±Π°ΡΡΠ΅ΠΉ ΠΈΠ·ΠΌΠ΅ΡΠΈΡΠ΅Π»ΡΠ½ΠΎΠ³ΠΎ ΡΠΈΠ³Π½Π°Π»Π° Π² ΡΠ΅ΡΠ΅Π²ΠΎΠΌ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π΅ ΡΠ°ΡΡΠΎΡ. ΠΠ»Π³ΠΎΡΠΈΡΠΌ Π²ΠΊΠ»ΡΡΠ°Π΅Ρ Π³Π΅Π½Π΅ΡΠ°ΡΠΈΡ ΠΈΠ·ΠΌΠ΅ΡΠΈΡΠ΅Π»ΡΠ½ΠΎΠ³ΠΎ ΡΠΈΠ³Π½Π°Π»Π° ΠΈ Π²ΡΠ΄Π΅Π»Π΅Π½ΠΈΠ΅ Π΅Π³ΠΎ ΠΎΠ³ΠΈΠ±Π°ΡΡΠ΅ΠΉ, ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΠ΅ ΠΈ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΠ΅ Π² ΠΊΠ°Π½Π°Π»Π΅ ΡΡΠ΅ΡΠΊΠΈ, Π²ΡΠ΄Π΅Π»Π΅Π½ΠΈΠ΅ ΠΎΠ³ΠΈΠ±Π°ΡΡΠ΅ΠΉ ΡΠ΅Π·ΡΠ»ΡΡΠΈΡΡΡΡΠ΅Π³ΠΎ ΡΠΈΠ³Π½Π°Π»Π°, Π²ΡΡΠΈΡΠ»Π΅Π½ΠΈΠ΅ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠ° ΠΊΠΎΡΡΠ΅Π»ΡΡΠΈΠΈ ΠΌΠ΅ΠΆΠ΄Ρ ΠΈΡΡ
ΠΎΠ΄Π½ΠΎΠΉ ΠΈ ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΠΎΠΉ ΠΎΠ³ΠΈΠ±Π°ΡΡΠΈΠΌΠΈ, ΡΡΠ°Π²Π½Π΅Π½ΠΈΠ΅ Ρ ΠΏΠΎΡΠΎΠ³ΠΎΠ²ΡΠΌ Π·Π½Π°ΡΠ΅Π½ΠΈΠ΅ΠΌ. ΠΠΏΠΈΡΠ°Π½ ΠΌΠ΅ΡΠΎΠ΄ Π²ΡΠ΄Π΅Π»Π΅Π½ΠΈΡ Π½ΠΈΠ·ΠΊΠΎΡΠ°ΡΡΠΎΡΠ½ΠΎΠΉ ΠΎΠ³ΠΈΠ±Π°ΡΡΠ΅ΠΉ ΡΠΈΠ³Π½Π°Π»Π° Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΡ ΠΠΈΠ»ΡΠ±Π΅ΡΡΠ°. ΠΡΠΈΠ²Π΅Π΄Π΅Π½ΠΎ ΠΎΠΏΠΈΡΠ°Π½ΠΈΠ΅ Π²Π·Π°ΠΈΠΌΠ½ΠΎ-ΠΊΠΎΡΡΠ΅Π»ΡΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π° Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠ° ΠΊΠΎΡΡΠ΅Π»ΡΡΠΈΠΈ ΠΠΈΡΡΠΎΠ½Π°. ΠΡΠΏΠΎΠ»Π½Π΅Π½ΠΎ ΠΈΠΌΠΈΡΠ°ΡΠΈΠΎΠ½Π½ΠΎΠ΅ ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΠΊΠ°Π½Π°Π»Π° ΡΡΠ΅ΡΠΊΠΈ, ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΈ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΡ ΠΈΠ·ΠΌΠ΅ΡΠΈΡΠ΅Π»ΡΠ½ΡΡ
ΡΠΈΠ³Π½Π°Π»ΠΎΠ², Π° ΡΠ°ΠΊΠΆΠ΅ ΠΈΡ
ΠΎΠ±ΡΠ°Π±ΠΎΡΠΊΠ° Π² ΠΏΡΠΎΠ³ΡΠ°ΠΌΠΌΠ½ΠΎΠΉ ΡΡΠ΅Π΄Π΅ MatLab. ΠΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΏΠΎΠ΄ΡΠ²Π΅ΡΠΆΠ΄Π°ΡΡ Π±ΠΎΠ»ΡΡΡΡ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ ΠΎΠ³ΠΈΠ±Π°ΡΡΠ΅ΠΉ ΠΏΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Ρ ΠΈΡΡ
ΠΎΠ΄Π½ΡΠΌ ΡΠΈΠ³Π½Π°Π»ΠΎΠΌ, Π° ΡΠ°ΠΊΠΆΠ΅ Π΄Π΅ΠΌΠΎΠ½ΡΡΡΠΈΡΡΡΡ ΠΏΡΠ΅ΠΈΠΌΡΡΠ΅ΡΡΠ²ΠΎ ΡΠ΅ΡΠ΅Π²ΡΡ
ΡΠΈΠ³Π½Π°Π»ΠΎΠ² ΠΏΠ΅ΡΠ΅Π΄ Π³Π°ΡΠΌΠΎΠ½ΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΡΠΈΠ³Π½Π°Π»Π°ΠΌΠΈ Π² ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅ ΠΈΠ·ΠΌΠ΅ΡΠΈΡΠ΅Π»ΡΠ½ΡΡ
Π΄Π»Ρ ΠΎΡΠ΅Π½ΠΊΠΈ Π·Π°ΡΠΈΡΠ΅Π½Π½ΠΎΡΡΠΈ ΠΊΠ°Π½Π°Π»Π° ΡΡΠ΅ΡΠΊΠΈ ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΠΈ
Correlation functions for a two-dimensional electron system with bosonic interactions and a square Fermi surface
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
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
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
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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