500 research outputs found
On the microscopic theory of the exciton ring fragmentation
The description is presented for the dependence of the indirect exciton
condensate density at the ring as a function of the polar angle at zero
temperature with the involvement of the processes of formation and
recombination of the excitons. In particular, starting from the quasi
one-dimensional Gross-Pitaevskii equation with a spatially uniform generating
term, we derive an exact analytical solution yielding the fragmentation of an
exciton ring which is probably observed in the experiments.Comment: 4 pages, 1 figure. The preprint has been brought into accord with the
journal's varian
ΠΠΏΡΡ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡ Π°Π·Π΅Π»Π°ΠΈΠ½ΠΎΠ²ΠΎΠΉ ΠΊΠΈΡΠ»ΠΎΡΡ Π² ΡΠ΅ΡΠ°ΠΏΠΈΠΈ Π±ΠΎΠ»ΡΠ½ΡΡ Π°ΠΊΠ½Π΅
Treatment of acne is one of the important problems of modern dermatology. The goal of the research. The study of clinical efficacy and safety of the 15% azelaic acid in the form of Azelik-gel in the treatment of patients with papulo-pustular acne, mild to moderate in severity. Material and methods. Open comparative study of 8 weeks, which was attended by 75 patients. To assess the safety and efficacy of the therapy was performed clinical and biochemical blood and urine tests, evaluation of dermatological status, measurement of pH, moisture and oiliness of skin and analysis of DLQI. Results. 82% of patients receiving the Azelik-gel, marked clinical improvement or significant improvement. Conclusions. The results of the study indicate a high level of safety and tolerability of the Azelik-gel and obtained clinical results have shown its therapeutic efficacy in the treatment of papulo-pustular acne mild to moderate in severity.ΠΠ΅ΡΠ΅Π½ΠΈΠ΅ Π°ΠΊΠ½Π΅ ΡΠ²Π»ΡΠ΅ΡΡΡ ΠΎΠ΄Π½ΠΎΠΉ ΠΈΠ· Π°ΠΊΡΡΠ°Π»ΡΠ½ΡΡ
ΠΏΡΠΎΠ±Π»Π΅ΠΌ ΡΠΎΠ²ΡΠ΅ΠΌΠ΅Π½Π½ΠΎΠΉ Π΄Π΅ΡΠΌΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΠΈ. Π¦Π΅Π»Ρ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ. ΠΠ·ΡΡΠ΅Π½ΠΈΠ΅ ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ ΠΈ Π±Π΅Π·ΠΎΠΏΠ°ΡΠ½ΠΎΡΡΠΈ Π»Π΅ΠΊΠ°ΡΡΡΠ²Π΅Π½Π½ΠΎΠ³ΠΎ ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΠ° ΠΠ·Π΅Π»ΠΈΠΊ (15% Π³Π΅Π»Ρ Π°Π·Π΅Π»Π°ΠΈΠ½ΠΎΠ²ΠΎΠΉ ΠΊΠΈΡΠ»ΠΎΡΡ) Π² ΡΠ΅ΡΠ°ΠΏΠΈΠΈ Π±ΠΎΠ»ΡΠ½ΡΡ
ΠΏΠ°ΠΏΡΠ»ΠΎ-ΠΏΡΡΡΡΠ»Π΅Π·Π½ΡΠΌΠΈ Π°ΠΊΠ½Π΅ Π»Π΅Π³ΠΊΠΎΠΉ ΠΈ ΡΡΠ΅Π΄Π½Π΅ΠΉ ΡΡΠ΅ΠΏΠ΅Π½ΠΈ ΡΡΠΆΠ΅ΡΡΠΈ. ΠΠ°ΡΠ΅ΡΠΈΠ°Π» ΠΈ ΠΌΠ΅ΡΠΎΠ΄Ρ. ΠΡΠΊΡΡΡΠΎΠ΅ ΡΡΠ°Π²Π½ΠΈΡΠ΅Π»ΡΠ½ΠΎΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΏΡΠΎΠ΄ΠΎΠ»ΠΆΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΡΡ 8 Π½Π΅Π΄Π΅Π»Ρ, Π² ΠΊΠΎΡΠΎΡΠΎΠΌ ΠΏΡΠΈΠ½ΡΠ»ΠΈ ΡΡΠ°ΡΡΠΈΠ΅ 75 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ². ΠΠ»Ρ ΠΎΡΠ΅Π½ΠΊΠΈ Π±Π΅Π·ΠΎΠΏΠ°ΡΠ½ΠΎΡΡΠΈ ΠΈ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠΌΠΎΠΉ ΡΠ΅ΡΠ°ΠΏΠΈΠΈ Π²ΡΠΏΠΎΠ»Π½ΡΠ»ΠΈ ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΈ Π±ΠΈΠΎΡ
ΠΈΠΌΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΠΊΡΠΎΠ²ΠΈ ΠΈ ΠΌΠΎΡΠΈ, ΠΎΡΠ΅Π½ΠΊΡ Π΄Π΅ΡΠΌΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΡΠ°ΡΡΡΠ°, ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΠ΅ ΡΠ, ΡΠ°Π»ΡΠ½ΠΎΡΡΠΈ ΠΈ Π²Π»Π°ΠΆΠ½ΠΎΡΡΠΈ ΠΊΠΎΠΆΠΈ Π»ΠΈΡΠ° ΠΈ Π°Π½Π°Π»ΠΈΠ· ΠΠΠΠ. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ. Ρ 82% Π±ΠΎΠ»ΡΠ½ΡΡ
, ΠΏΠΎΠ»ΡΡΠ°ΡΡΠΈΡ
Π³Π΅Π»Ρ ΠΠ·Π΅Π»ΠΈΠΊ, ΠΎΡΠΌΠ΅ΡΠ΅Π½ΠΎ ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΎΠ΅ Π²ΡΠ·Π΄ΠΎΡΠΎΠ²Π»Π΅Π½ΠΈΠ΅ ΠΈΠ»ΠΈ Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΠΎΠ΅ ΡΠ»ΡΡΡΠ΅Π½ΠΈΠ΅. ΠΡΠ²ΠΎΠ΄Ρ. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½Π½ΠΎΠ³ΠΎ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΡΠΊΠ°Π·ΡΠ²Π°ΡΡ Π½Π° Π²ΡΡΠΎΠΊΠΈΠΉ ΡΡΠΎΠ²Π΅Π½Ρ Π±Π΅Π·ΠΎΠΏΠ°ΡΠ½ΠΎΡΡΠΈ ΠΈ Ρ
ΠΎΡΠΎΡΡΡ ΠΏΠ΅ΡΠ΅Π½ΠΎΡΠΈΠΌΠΎΡΡΡ Π³Π΅Π»Ρ ΠΠ·Π΅Π»ΠΈΠΊ, Π° ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΈ Π΅Π³ΠΎ ΡΠ΅ΡΠ°ΠΏΠ΅Π²ΡΠΈΡΠ΅ΡΠΊΡΡ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ Π² Π»Π΅ΡΠ΅Π½ΠΈΠΈ ΠΏΠ°ΠΏΡΠ»ΠΎ-ΠΏΡΡΡΡΠ»Π΅Π·Π½ΠΎΠΉ ΡΠΎΡΠΌΡ Π°ΠΊΠ½Π΅ Π»Π΅Π³ΠΊΠΎΠΉ ΠΈ ΡΡΠ΅Π΄Π½Π΅ΡΡΠΆΠ΅Π»ΠΎΠΉ ΡΡΠ΅ΠΏΠ΅Π½ΠΈ
Long-lived magnetoexcitons in 2D-fermion system
The paper addresses the experimental technique that, when applied to a 2D-electron system in the integer quantum Hall regime with filling factor Ξ½β=β2 (the Hall insulating state), allows resonant excitation of magnetoexcitons, their detection, control of an ensemble of long-lived triplet excitons and investigation of their radiationless decay related to exciton spin relaxation into the ground state. The technique proposed enables independent control of photoexcited electrons and Fermi-holes using photoinduced resonance reflection spectra as well as estimate with a reasonable degree of accuracy the resulting density of photoinduced electron-hole pairs bound into magnetoexcitons. The mere existence of triplet excitons was directly established by inelastic light scattering spectra which were analyzed to determine the value of singlet-triplet exciton splitting. It was found that the lifetimes of triplet excitons conditioned by electron spin relaxation in highly perfect GaAs/AlGaAs heterostructures with highly mobile 2D electrons are extremely long exceeding 100β ΞΌs at Tβ<β1βK. The paper presents a qualitative explanation of the long-spin relaxation lifetimes which are unprecedented for translation-invariant 2D systems. This enabled us to create sufficiently high concentrations of triplet magnetoexcitons, electrically neutral excitations following BoseβEinstein statistics, in a Fermi electron system and investigate their collective properties. At sufficiently high densities of triplet magnetoexcitons and low temperatures, Tβ<β1βK, the degenerate magnetofermionic system exhibits condensation of the triplet magnetoexcitons into a qualitatively new collective state with unusual properties which occurs in the space of generalized moments (magnetic translation vectors). The occurrence of a condensed phase is accompanied with a significant decrease in the viscosity of the photoexcited system, which is responsible for electron spin transport at macroscopic distances, as well as with the effects of threshold enhancement of the system response to the external action of the electromagnetic field and emergence of a new intensive radiative recombination channel
Anisotropic physical properties of single crystal U2Rh2Sn in high magnetic fields
We report on the crystal and magnetic structures,magnetic, transport, and thermal properties of U2Rh2Sn single crystals studied in part in high magnetic fields up to 58 T. The material adopts a U3Si2 related tetragonal crystal structure and orders antiferromagnetically below TN 25 K. The antiferromagnetic structure is characterized by a propagation vector k 0,0,1 2 . The magnetism in U2Rh2Sn is found to be associated mainly with 5f states. However, both unpolarized and polarized neutron experiments reveal at low temperatures in zero field non negligible magnetic moments also on Rh sites. U moments of 0.50 2 amp; 956;B are directed along the tetragonal axis while Rh moments of 0.06 4 amp; 956;B form a noncollinear arrangement confined to the basal plane. The response to applied magnetic field is highly anisotropic. Above amp; 8764;15 K the easy magnetization direction is along the tetragonal axis. At lower temperatures, however, a stronger response is found perpendicular to the c axis. While for the a axis no magnetic phase transition is observed up to 58 T, for the field applied at 1.8 K along the tetragonal axis we observe above 22.5 T a field polarized state. A magnetic phase diagram for the field applied along the c axis is presented
Acoustic signatures of the phase transitions in the antiferromagnet U2Rh2Sn
We report on ultrasound measurements in a single crystal of the antiferromagnet U2Rh2Sn as a function of temperature and magnetic field. We find pronounced anomalies in the sound velocity at the N el temperature, 25 K, and at the field induced spin flop like transition at 22.5 T, which points to a strong magnetoelastic coupling. Additionally, we find that in the paramagnetic regime the temperature dependence of the magnetic susceptibility and the field dependences of the magnetization and sound velocity of transverse acoustic waves can be well described assuming a localized character of the 5f electrons. Using this premise, the crystal electric field scheme of U2Rh2Sn has been determine
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