3,042 research outputs found
Low-field diffusion magneto-thermopower of a high mobility two-dimensional electron gas
The low magnetic field diffusion thermopower of a high mobility
GaAs-heterostructure has been measured directly on an electrostatically defined
micron-scale Hall-bar structure at low temperature (T = 1.6 K) in the low
magnetic field regime (B < 1.2 T) where delocalized quantum Hall states do not
influence the measurements. The sample design allowed the determination of the
field dependence of the thermopower both parallel and perpendicular to the
temperature gradient, denoted respectively by Sxx (longitudinal thermopower)
and Syx (Nernst-Ettinghausen coefficient). The experimental data show clear
oscillations in Sxx and Syx due to the formation of Landau levels for 0.3 T < B
< 1.2 T and reveal that Syx is approximately 120 times larger than Sxx at a
magnetic field of 1 T, which agrees well with the theoretical prediction.Comment: 4 pages, 4 figure
Evaluation OF adherence to various treatment methods among osteoarthritis patients
This article describes the results of questioning which was carried out in 2007 β 2008 years in order to estimate adherence to various treatment methods among the patients with knee and hip osteoarthritis (OA). The 54 patients were randomly selected and questioned in 9 general practices in the city of Yekaterinburg and in the Sverdlovsk region. The analysis of demographic data has confirmed relation between OA and gender (88,8% of participants were females) and increased body mass index (average BMI was 32Β±6,8 kg/m2) as risk factors of OA. Statistically significant connection has been found out between age of 55 and older and increased adherence to local thermal procedures (Cl 0,07-0,73), fangotherapy and medical baths (Cl 0,07-0,96). The majority of patients preferred to use medical interventions several times a month or as needed, meanwhile adherence to daily treatment was low. Revealed data demonstrate high level of NSAID usage as in tablets, as in topical forms, and also high adherence to topical treatment in general. Participants have demonstrated relatively low adherence to weight reduction and exercises, but parapharmaceutics and complementary medicines are very popular. Moreover, significant amount (31,1%) of ungrounded X-ray examinations of knee joints has been found out. Thus, research has shown that diagnostics and treatment of OA in primary care are far from optimal; this situation can be caused by the outdated clinico-organizational standards, insufficient interaction between physicians and patients, and also with difficulties in behavioural stereotypes change and preference of more simple, cheap and accessible methods of treatment among OA patients.Π ΡΡΠ°ΡΡΠ΅ ΠΎΠΏΠΈΡΡΠ²Π°ΡΡΡΡ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ Π°Π½ΠΊΠ΅ΡΠΈΡΠΎΠ²Π°Π½ΠΈΡ, ΠΊΠΎΡΠΎΡΠΎΠ΅ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΎΡΡ Π² 2007-2008 Π³Π³. Π΄Π»Ρ ΠΎΡΠ΅Π½ΠΊΠΈ ΠΏΡΠΈΠ²Π΅ΡΠΆΠ΅Π½Π½ΠΎΡΡΠΈ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Ρ ΠΎΡΡΠ΅ΠΎΠ°ΡΡΡΠΈΡΠΎΠΌ (OΠ) ΠΊΠΎΠ»Π΅Π½Π½ΡΡ
ΠΈ ΡΠ°Π·ΠΎΠ±Π΅Π΄ΡΠ΅Π½Π½ΡΡ
ΡΡΡΡΠ°Π²ΠΎΠ² ΠΊ ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
ΠΌΠ΅ΡΠΎΠ΄Π°ΠΌ Π»Π΅ΡΠ΅Π½ΠΈΡ. ΠΡΠ΅Π³ΠΎ ΠΏΡΠΎΠ°Π½ΠΊΠ΅ΡΠΈΡΠΎΠ²Π°Π½ΠΎ 54 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠ°, Π½Π°Π±Π»ΡΠ΄Π°ΡΡΠΈΡ
ΡΡ Ρ 9 Π²ΡΠ°ΡΠ΅ΠΉ ΠΎΠ±ΡΠ΅ΠΉ ΠΏΡΠ°ΠΊΡΠΈΠΊΠΈ Π³. ΠΠΊΠ°ΡΠ΅ΡΠΈΠ½Π±ΡΡΠ³Π° ΠΈ Π‘Π²Π΅ΡΠ΄Π»ΠΎΠ²ΡΠΊΠΎΠΉ ΠΎΠ±Π»Π°ΡΡΠΈ. ΠΠ½Π°Π»ΠΈΠ· Π΄Π΅ΠΌΠΎΠ³ΡΠ°ΡΠΈΡΠ΅ΡΠΊΠΈΡ
Π΄Π°Π½Π½ΡΡ
ΠΈ ΠΈΠ½Π΄Π΅ΠΊΡΠ° ΠΌΠ°ΡΡΡ ΡΠ΅Π»Π° ΡΠ΅ΡΠΏΠΎΠ½Π΄Π΅Π½ΡΠΎΠ² ΠΏΠΎΠ΄ΡΠ²Π΅ΡΠΆΠ΄Π°Π΅Ρ Π·Π½Π°ΡΠ΅Π½ΠΈΠ΅ ΠΎΠΆΠΈΡΠ΅Π½ΠΈΡ ΠΊΠ°ΠΊ ΡΠ°ΠΊΡΠΎΡΠ° ΡΠΈΡΠΊΠ° 0Π (ΡΡΠ΅Π΄Π½ΠΈΠΉ ΠΠΠ’ 32Β±6,8 ΠΊΠ³/ΠΌ2) ΠΈ ΠΏΡΠ΅ΠΈΠΌΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎΠ΅ ΡΠ°Π·Π²ΠΈΡΠΈΠ΅ Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΡ Ρ Π»ΠΈΡ ΠΆΠ΅Π½ΡΠΊΠΎΠ³ΠΎ ΠΏΠΎΠ»Π° (88,8% ΡΠ΅ΡΠΏΠΎΠ½Π΄Π΅Π½ΡΠΎΠ²). ΠΠ±Π½Π°ΡΡΠΆΠ΅Π½Π° ΡΡΠ°ΡΠΈΡΡΠΈΡΠ΅ΡΠΊΠΈ Π΄ΠΎΡΡΠΎΠ²Π΅ΡΠ½Π°Ρ ΡΠ²ΡΠ·Ρ ΠΌΠ΅ΠΆΠ΄Ρ ΡΠ²Π΅Π»ΠΈΡΠ΅Π½ΠΈΠ΅ΠΌ Π²ΠΎΠ·ΡΠ°ΡΡΠ° ΡΠ΅ΡΠΏΠΎΠ½Π΄Π΅Π½ΡΠΎΠ² ΠΈ ΠΏΠΎΠ²ΡΡΠ΅Π½ΠΈΠ΅ΠΌ ΡΠ°ΡΡΠΎΡΡ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ ΡΠ΅ΠΏΠ»ΠΎΠ²ΡΡ
ΠΏΡΠΎΡΠ΅Π΄ΡΡ (ΠΠ 0,07- 0,73), Π³ΡΡΠ·Π΅Π»Π΅ΡΠ΅Π½ΠΈΡ ΠΈ Π»Π΅ΡΠ΅Π±Π½ΡΡ
Π²Π°Π½Π½ (ΠΠ 0,07-0,96). ΠΡΡΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ ΠΏΡΠ΅Π΄ΠΏΠΎΡΠΈΡΠ°Π΅ΠΌΠ°Ρ ΡΠ°ΡΡΠΎΡΠ° ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ Π±ΠΎΠ»ΡΡΠΈΠ½ΡΡΠ²Π° ΠΌΠ΅Π΄ΠΈΡΠΈΠ½ΡΠΊΠΈΡ
Π²ΠΌΠ΅ΡΠ°ΡΠ΅Π»ΡΡΡΠ² β Π½Π΅ΡΠΊΠΎΠ»ΡΠΊΠΎ ΡΠ°Π· Π² ΠΌΠ΅ΡΡΡ ΠΈΠ»ΠΈ ΠΏΠΎ ΠΏΠΎΡΡΠ΅Π±Π½ΠΎΡΡΠΈ, ΠΏΡΠΈ ΡΡΠΎΠΌ ΠΊ Π΅ΠΆΠ΅Π΄Π½Π΅Π²Π½ΠΎΠΌΡ Π»Π΅ΡΠ΅Π½ΠΈΡ ΠΏΡΠΈΠ²Π΅ΡΠΆΠ΅Π½Π½ΠΎΡΡΡ Π½ΠΈΠ·ΠΊΠ°Ρ. ΠΠΎΠ»ΡΡΠ΅Π½Ρ Π΄Π°Π½Π½ΡΠ΅ ΠΎ Π²ΡΡΠΎΠΊΠΎΠΉ ΡΠ°ΡΡΠΎΡΠ΅ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ ΠΠΠΠ ΠΊΠ°ΠΊ Π²Π½ΡΡΡΡ, ΡΠ°ΠΊ ΠΈ ΠΌΠ΅ΡΡΠ½ΠΎ, Π° ΡΠ°ΠΊΠΆΠ΅ Π²ΡΡΠΎΠΊΠΎΠΉ ΠΏΡΠΈΠ²Π΅ΡΠΆΠ΅Π½Π½ΠΎΡΡΠΈ ΠΊ Π»ΠΎΠΊΠ°Π»ΡΠ½ΡΠΌ ΡΡΠ΅Π΄ΡΡΠ²Π°ΠΌ Π»Π΅ΡΠ΅Π½ΠΈΡ Π² ΡΠ΅Π»ΠΎΠΌ. Π ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΡ Π²Π΅ΡΠ° ΠΈ Π³ΠΈΠΌΠ½Π°ΡΡΠΈΠΊΠ΅ ΠΏΠ°ΡΠΈΠ΅Π½ΡΡ ΠΏΡΠΎΠ΄Π΅ΠΌΠΎΠ½ΡΡΡΠΈΡΠΎΠ²Π°Π»ΠΈ ΠΎΡΠ½ΠΎΡΠΈΡΠ΅Π»ΡΠ½ΠΎ Π½ΠΈΠ·ΠΊΡΡ ΠΏΡΠΈΠ²Π΅ΡΠΆΠ΅Π½Π½ΠΎΡΡΡ, ΠΏΡΠΈ ΡΡΠΎΠΌ ΡΡΠ΅Π΄ΡΡΠ²Π° Π½Π°ΡΠΎΠ΄Π½ΠΎΠΉ ΠΌΠ΅Π΄ΠΈΡΠΈΠ½Ρ ΠΈ ΠΏΠ°ΡΠ°ΡΠ°ΡΠΌΠ°ΡΠ΅Π²ΡΠΈΠΊΠΈ ΠΏΠΎΠ»ΡΠ·ΡΡΡΡΡ Π²ΡΡΠΎΠΊΠΎΠΉ ΠΏΠΎΠΏΡΠ»ΡΡΠ½ΠΎΡΡΡΡ. ΠΡΠΎΠΌΠ΅ ΡΠΎΠ³ΠΎ, Π² ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ΅ Π°Π½ΠΊΠ΅ΡΠΈΡΠΎΠ²Π°Π½ΠΈΡ Π²ΡΡΠ²Π»Π΅Π½ΠΎ Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΠΎΠ΅ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²ΠΎ Π½Π΅ΠΎΠ±ΠΎΡΠ½ΠΎΠ²Π°Π½Π½ΡΡ
ΡΠ΅Π½ΡΠ³Π΅Π½ΠΎΠ³ΡΠ°ΡΠΈΠΉ ΠΊΠΎΠ»Π΅Π½Π½ΡΡ
ΡΡΡΡΠ°Π²ΠΎΠ² (31,1%). Π ΡΠ΅Π»ΠΎΠΌ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΏΡΠΎΠ΄Π΅ΠΌΠΎΠ½ΡΡΡΠΈΡΠΎΠ²Π°Π»ΠΎ, ΡΡΠΎ Π΄ΠΈΠ°Π³Π½ΠΎΡΡΠΈΠΊΠ° ΠΈ Π»Π΅ΡΠ΅Π½ΠΈΠ΅ ΠΠ Π² ΠΏΠ΅ΡΠ²ΠΈΡΠ½ΠΎΠΌ Π·Π²Π΅Π½Π΅ Π΄Π°Π»Π΅ΠΊΠΈ ΠΎΡ ΠΎΠΏΡΠΈΠΌΠ°Π»ΡΠ½ΡΡ
, ΡΡΠΎ ΠΌΠΎΠΆΠ΅Ρ Π±ΡΡΡ ΡΠ²ΡΠ·Π°Π½ΠΎ Ρ ΡΡΡΠ°ΡΠ΅Π²ΡΠΈΠΌΠΈ ΠΊΠ»ΠΈΠ½ΠΈΠΊΠΎ-ΠΎΡΠ³Π°Π½ΠΈΠ·Π°ΡΠΈΠΎΠ½Π½ΡΠΌΠΈ ΡΡΠ°Π½Π΄Π°ΡΡΠ°ΠΌΠΈ, Π½Π΅Π΄ΠΎΡΡΠ°ΡΠΎΡΠ½ΡΠΌ Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ΠΌ ΠΌΠ΅ΠΆΠ΄Ρ Π²ΡΠ°ΡΠ°ΠΌΠΈ ΠΈ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠ°ΠΌΠΈ, Π° ΡΠ°ΠΊΠΆΠ΅ Ρ ΡΡΡΠ΄Π½ΠΎΡΡΡΠΌΠΈ Π² ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠΈ ΠΏΠΎΠ²Π΅Π΄Π΅Π½ΡΠ΅ΡΠΊΠΈΡ
ΡΡΠ΅ΡΠ΅ΠΎΡΠΈΠΏΠΎΠ² ΠΈ ΠΏΡΠ΅Π΄ΠΏΠΎΡΡΠ΅Π½ΠΈΠ΅ΠΌ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠ°ΠΌΠΈ Π±ΠΎΠ»Π΅Π΅ ΠΏΡΠΎΡΡΡΡ
, Π΄Π΅ΡΠ΅Π²ΡΡ
ΠΈ Π΄ΠΎΡΡΡΠΏΠ½ΡΡ
ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ² Π»Π΅ΡΠ΅Π½ΠΈΡ
Harmonic decomposition to describe the nonlinear evolution of stimulated Brillouin scattering
An efficient method to describe the nonlinear evolution of stimulated Brillouin scattering(SBS) in long scale-length plasmas is presented in the limit of a fluid description. The method is based on the decomposition of the various functions characterizing the plasma into their long- and short-wavelength components. It makes it possible to describe self-consistently the interplay between the plasmahydrodynamics,stimulated Brillouin scattering, and the generation of harmonics of the excited ion acoustic wave(IAW). This description is benchmarked numerically in one and two spatial dimensions [one dimensional (1D), two dimensional (2D)], by comparing the numerical results obtained along this method with those provided by a numerical code in which the decomposition into separate spatial scales is not made. The decomposition method proves to be very efficient in terms of computing time, especially in 2D, and very reliable, even in the extreme case of undamped ion acoustic waves. A novel picture of the SBS nonlinear behavior arises, in which the IAWharmonics generation gives rise to local defects appearing in the density and velocity hydrodynamics profiles. Consequently, SBS develops in various spatial domains which seem to be decorrelated one from each other, so that the backscattered Brillouin light is the sum of various backscatteredwaves generated in several independent spatial domains. It follows that the SBSreflectivity is chaotic in time and the resulting time-averaged value is significantly reduced as compared to the case when the IAWharmonics generation and flow modification are ignored. From the results of extensive numerical simulations carried out in 1D and 2D, we are able to infer the SBSreflectivity scaling law as a function of the plasma parameters and laser intensity, in the limit where the kinetic effects are negligible. It appears that this scaling law can be derived in the limit where the IAWharmonics generation is modeled simply by a nonlinear frequency shift
Critical Strain Region Evaluation of Self-Assembled Semiconductor Quantum Dots
A novel peak finding method to map the strain from high resolution transmission electron micrographs, known as the Peak Pairs method, has been applied to In(Ga) As/AlGaAs quantum dot (QD) samples, which present stacking faults emerging from the QD edges. Moreover, strain distribution has been simulated by the finite element method applying the elastic theory on a 3D QD model. The agreement existing between determined and simulated strain values reveals that these techniques are consistent enough to qualitatively characterize the strain distribution of nanostructured materials. The correct application of both methods allows the localization of critical strain zones in semiconductor QDs, predicting the nucleation of defects, and being a very useful tool for the design of semiconductor device
Π ΠΎΠ»Ρ Π²ΠΈΡΠ°ΠΌΠΈΠ½ΠΎΠ²-Π°Π½ΡΠΈΠΎΠΊΡΠΈΠ΄Π°Π½ΡΠΎΠ² Π² ΡΡΠΈΠΎΠ»ΠΎΠ³ΠΈΠΈ ΡΠ΅Π²ΠΌΠ°ΡΠΎΠΈΠ΄Π½ΠΎΠ³ΠΎ Π°ΡΡΡΠΈΡΠ°
There is evidence that insufficient intake of antioxidants may increase the risk of autoimmune inflammatory diseases, including rheumatoidΒ arthritis (RA). Also, lower plasma concentrations of antioxidant vitamins can be a sign of their heavy expenditure to suppress inflammatoryΒ processes in the preclinical stage of RA.Β This article provides an overview of modern studies that have assessed a relationship between the incidence of RA and serum levels or dietaryΒ intake of vitamins A, E, C and beta-carotene. Case-control studies have revealed that Ξ±-tocopherol and Ξ²-cryptoxanthin have a protectiveΒ effect and their high plasma levels are associated with the decreased incidence of RA. An inverse relationship has been also found between theΒ dietary intake of carotenoids and vitamin C and the risk of RA. At the same time, larger prospective cohort studies have failed to confirm theΒ relationship between the levels of consumption of the major antioxidant vitamins and the risk of RA. The currently available data on the role ofΒ antioxidant vitamins in the development of RA remains controversial. Conceivably, sufficient intake of the vitamins has no self-protective activityΒ against RA, but serves as a marker for a healthier lifestyle that lowers the risk of many diseases, including autoimmune disorders.ΠΠΎ Π½Π΅ΠΊΠΎΡΠΎΡΡΠΌ Π΄Π°Π½Π½ΡΠΌ, Π½Π΅Π΄ΠΎΡΡΠ°ΡΠΎΡΠ½ΠΎΠ΅ ΠΏΠΎΡΡΠ΅Π±Π»Π΅Π½ΠΈΠ΅ Π°Π½ΡΠΈΠΎΠΊΡΠΈΠ΄Π°Π½ΡΠΎΠ² ΠΌΠΎΠΆΠ΅Ρ ΠΏΠΎΠ²ΡΡΠ°ΡΡ ΡΠΈΡΠΊ ΡΠ°Π·Π²ΠΈΡΠΈΡ Π°ΡΡΠΎΠΈΠΌΠΌΡΠ½Π½ΡΡ
Π²ΠΎΡΠΏΠ°Π»ΠΈΡΠ΅Π»ΡΠ½ΡΡ
Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΠΉ, Π² ΡΠΎΠΌ ΡΠΈΡΠ»Π΅ ΡΠ΅Π²ΠΌΠ°ΡΠΎΠΈΠ΄Π½ΠΎΠ³ΠΎ Π°ΡΡΡΠΈΡΠ° (Π Π). ΠΡΠΎΠΌΠ΅ ΡΠΎΠ³ΠΎ, ΠΏΠΎΠ½ΠΈΠΆΠ΅Π½Π½Π°Ρ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΡ Π²ΠΈΡΠ°ΠΌΠΈΠ½ΠΎΠ²-Π°Π½ΡΠΈΠΎΠΊΡΠΈΠ΄Π°Π½ΡΠΎΠ² Π² ΠΏΠ»Π°Π·ΠΌΠ΅ ΠΌΠΎΠΆΠ΅Ρ Π±ΡΡΡ ΡΠ²ΡΠ·Π°Π½Π° Ρ ΠΈΡ
ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΡΠΌ ΡΠ°ΡΡ
ΠΎΠ΄ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ Π½Π° ΠΏΠΎΠ΄Π°Π²Π»Π΅Π½ΠΈΠ΅ Π²ΠΎΡΠΏΠ°Π»ΠΈΡΠ΅Π»ΡΠ½ΡΡ
ΠΏΡΠΎΡΠ΅ΡΡΠΎΠ² Π² Π΄ΠΎΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΡΡΒ ΡΡΠ°Π΄ΠΈΡ Π Π.Β Π Π½Π°ΡΡΠΎΡΡΠ΅ΠΉ ΡΡΠ°ΡΡΠ΅ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½ ΠΎΠ±Π·ΠΎΡ ΡΠΎΠ²ΡΠ΅ΠΌΠ΅Π½Π½ΡΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ, Π² ΠΊΠΎΡΠΎΡΡΡ
ΠΎΡΠ΅Π½ΠΈΠ²Π°Π»Π°ΡΡ ΡΠ²ΡΠ·Ρ ΠΌΠ΅ΠΆΠ΄Ρ Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π΅ΠΌΠΎΡΡΡΡ Π Π ΠΈ ΡΡΠ²ΠΎΡΠΎΡΠΎΡΠ½ΡΠΌ ΡΡΠΎΠ²Π½Π΅ΠΌ, ΠΈΠ»ΠΈ Π΄ΠΈΠ΅ΡΠΈΡΠ΅ΡΠΊΠΈΠΌ ΠΏΠΎΡΡΠ΅Π±Π»Π΅Π½ΠΈΠ΅ΠΌ, Π²ΠΈΡΠ°ΠΌΠΈΠ½ΠΎΠ² Π, Π, Π‘ ΠΈ Π±Π΅ΡΠ°-ΠΊΠ°ΡΠΎΡΠΈΠ½Π°. Π ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡΡ
ΡΠ»ΡΡΠ°ΠΉ-ΠΊΠΎΠ½ΡΡΠΎΠ»Ρ ΡΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ Π°Π»ΡΡΠ°-ΡΠΎΠΊΠΎΡΠ΅ΡΠΎΠ» ΠΈ Π±Π΅ΡΠ°-ΠΊΡΠΈΠΏΡΠΎΠΊΡΠ°Π½ΡΠΈΠ½ ΠΎΠ±Π»Π°Π΄Π°ΡΡ Π·Π°ΡΠΈΡΠ½ΡΠΌ ΡΡΡΠ΅ΠΊΡΠΎΠΌ ΠΈ ΠΈΡ
Π²ΡΡΠΎΠΊΠΈΠ΅ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΠΈ Π² ΠΏΠ»Π°Π·ΠΌΠ΅Β Π°ΡΡΠΎΡΠΈΠΈΡΠΎΠ²Π°Π½Ρ ΡΠΎ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΠ΅ΠΌ Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π΅ΠΌΠΎΡΡΠΈ Π Π. Π’Π°ΠΊΠΆΠ΅ Π±ΡΠ»Π° ΠΏΠΎΠΊΠ°Π·Π°Π½Π° ΠΎΠ±ΡΠ°ΡΠ½ΠΎ ΠΏΡΠΎΠΏΠΎΡΡΠΈΠΎΠ½Π°Π»ΡΠ½Π°Ρ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΡ ΠΌΠ΅ΠΆΠ΄Ρ ΠΏΠΎΡΡΠ΅Π±Π»Π΅Π½ΠΈΠ΅ΠΌ ΠΊΠ°ΡΠΎΡΠΈΠ½ΠΎΠΈΠ΄ΠΎΠ² ΠΈ Π²ΠΈΡΠ°ΠΌΠΈΠ½Π° Π‘ ΠΈ ΡΠΈΡΠΊΠΎΠΌ ΡΠ°Π·Π²ΠΈΡΠΈΡ Π Π. Π ΡΠΎ ΠΆΠ΅ Π²ΡΠ΅ΠΌΡ Π² Π±ΠΎΠ»Π΅Π΅ ΠΊΡΡΠΏΠ½ΡΡ
ΠΏΡΠΎΡΠΏΠ΅ΠΊΡΠΈΠ²Π½ΡΡ
ΠΊΠΎΠ³ΠΎΡΡΠ½ΡΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡΡ
Π²Π·Π°ΠΈΠΌΠΎΡΠ²ΡΠ·Ρ ΡΡΠΎΠ²Π½Ρ ΠΏΠΎΡΡΠ΅Π±Π»Π΅Π½ΠΈΡ ΠΎΡΠ½ΠΎΠ²Π½ΡΡ
Π²ΠΈΡΠ°ΠΌΠΈΠ½ΠΎΠ²-Π°Π½ΡΠΈΠΎΠΊΡΠΈΠ΄Π°Π½ΡΠΎΠ² ΠΈ ΡΠΈΡΠΊΠ° Π²ΠΎΠ·Π½ΠΈΠΊΠ½ΠΎΠ²Π΅Π½ΠΈΡ Π Π Π½Π΅ ΠΏΠΎΠ΄ΡΠ²Π΅ΡΠΆΠ΄Π΅Π½Π°. ΠΠΌΠ΅ΡΡΠΈΠ΅ΡΡ Π΄Π°Π½Π½ΡΠ΅ ΠΎ ΡΠΎΠ»ΠΈ Π²ΠΈΡΠ°ΠΌΠΈΠ½ΠΎΠ²-Π°Π½ΡΠΈΠΎΠΊΡΠΈΠ΄Π°Π½ΡΠΎΠ² Π² ΡΠ°Π·Π²ΠΈΡΠΈΠΈ Π Π ΠΏΡΠΎΡΠΈΠ²ΠΎΡΠ΅ΡΠΈΠ²Ρ. ΠΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎ, Π΄ΠΎΡΡΠ°ΡΠΎΡΠ½ΠΎΠ΅ ΠΏΠΎΡΡΠ΅Π±Π»Π΅Π½ΠΈΠ΅ Π²ΠΈΡΠ°ΠΌΠΈΠ½ΠΎΠ² Π½Π΅Β ΠΎΠΊΠ°Π·ΡΠ²Π°Π΅Ρ ΡΠ°ΠΌΠΎΡΡΠΎΡΡΠ΅Π»ΡΠ½ΠΎΠ³ΠΎ Π·Π°ΡΠΈΡΠ½ΠΎΠ³ΠΎ Π΄Π΅ΠΉΡΡΠ²ΠΈΡ Π² ΠΎΡΠ½ΠΎΡΠ΅Π½ΠΈΠΈ ΡΠ°Π·Π²ΠΈΡΠΈΡ Π Π, Π½ΠΎ ΡΠ²Π»ΡΠ΅ΡΡΡ ΠΌΠ°ΡΠΊΠ΅ΡΠΎΠΌ Π±ΠΎΠ»Π΅Π΅ Π·Π΄ΠΎΡΠΎΠ²ΠΎΠ³ΠΎ ΠΎΠ±ΡΠ°Π·Π° ΠΆΠΈΠ·Π½ΠΈ, ΠΏΡΠΈ ΠΊΠΎΡΠΎΡΠΎΠΌ ΡΠΌΠ΅Π½ΡΡΠ°Π΅ΡΡΡ Π²Π΅ΡΠΎΡΡΠ½ΠΎΡΡΡ ΠΌΠ½ΠΎΠ³ΠΈΡ
Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΠΉ, Π² ΡΠΎΠΌ ΡΠΈΡΠ»Π΅ Π°ΡΡΠΎΠΈΠΌΠΌΡΠ½Π½ΡΡ
The seasonal cycle of the greenhouse gas balance of a continental tundra site in the Indigirka lowlands, NE Siberia
International audienceCarbon dioxide and methane fluxes were measured at a tundra site near Chokurdakh, in the lowlands of the Indigirka river in north-east Siberia. This site is one of the few stations on Russian tundra and it is different from most other tundra flux stations in its continentality. A suite of methods was applied to determine the fluxes of NEE, GPP, Reco and methane, including eddy covariance, chambers and leaf cuvettes. Net carbon dioxide fluxes were unusually high, compared with other tundra sites, with NEE=?92 g C m?2 yr?1, which is composed of an Reco=+141 g C m?2 yr?1 and GPP=?232 g C m?2 yr?1. This large carbon dioxide sink may be explained by the continental climate, that is reflected in low winter soil temperatures (?14Β°C), reducing the respiration rates, and short, relatively warm summers, stimulating high photosynthesis rates. Interannual variability in GPP was dominated by the frequency of light limitation (Rg ?2), whereas Reco depends most directly on soil temperature and time in the growing season, which serves as a proxy of the combined effects of active layer depth, leaf area index, soil moisture and substrate availability. The methane flux, in units of global warming potential, was +28 g C-CO2e m?2 yr?1, so that the greenhouse gas balance was ?64 g C-CO2e m?2 yr?1. Methane fluxes depended only slightly on soil temperature and were highly sensitive to hydrological conditions and vegetation composition
Presence of nanoplastics in rural and remote surface waters
It is now established that microplastics are a pervasive presence in aquatic and terrestrial ecosystems. The same is assumed to be true for nanoplastics but data are lacking due to technical difficulties associated with sample analysis. Here, we measured nanoplastics in waterbodies at two contrasting sites: remote Siberian Arctic tundra and a forest landscape in southern Sweden. Nanoplastics were detected in all sampled Swedish lakes (n = 7) and streams (n = 4) (mean concentration = 563 Β΅g lβ1) and four polymer types were identified (polyethylene, polyvinyl chloride (PVC), polypropylene, polyethylene terephthalate). In Siberia nanoplastics were detected in 7/12 sampled lakes, ponds and surface flooding, but only two polymer types were detected (PVC and polystyrene) and concentrations were lower (mean 51 Β΅g lβ1). Based on back-calculation of air mass trajectories and particle dispersion, we infer that nanoplastics arrive at both sites by aerial deposition from local and regional sources. Our results suggest that nanoplastics may be a near-ubiquitous presence even in remote ecosystems
Vertical-external-cavity surface-emitting lasers and quantum dot lasers
The use of cavity to manipulate photon emission of quantum dots (QDs) has
been opening unprecedented opportunities for realizing quantum functional
nanophotonic devices and also quantum information devices. In particular, in
the field of semiconductor lasers, QDs were introduced as a superior
alternative to quantum wells to suppress the temperature dependence of the
threshold current in vertical-external-cavity surface-emitting lasers
(VECSELs). In this work, a review of properties and development of
semiconductor VECSEL devices and QD laser devices is given. Based on the
features of VECSEL devices, the main emphasis is put on the recent development
of technological approach on semiconductor QD VECSELs. Then, from the viewpoint
of both single QD nanolaser and cavity quantum electrodynamics (QED), a
single-QD-cavity system resulting from the strong coupling of QD cavity is
presented. A difference of this review from the other existing works on
semiconductor VECSEL devices is that we will cover both the fundamental aspects
and technological approaches of QD VECSEL devices. And lastly, the presented
review here has provided a deep insight into useful guideline for the
development of QD VECSEL technology and future quantum functional nanophotonic
devices and monolithic photonic integrated circuits (MPhICs).Comment: 21 pages, 4 figures. arXiv admin note: text overlap with
arXiv:0904.369
Measurement of the Longitudinal Spin Transfer to Lambda and Anti-Lambda Hyperons in Polarised Muon DIS
The longitudinal polarisation transfer from muons to lambda and anti-lambda
hyperons, D_LL, has been studied in deep inelastic scattering off an
unpolarised isoscalar target at the COMPASS experiment at CERN. The spin
transfers to lambda and anti-lambda produced in the current fragmentation
region exhibit different behaviours as a function of x and xF . The measured x
and xF dependences of D^lambda_LL are compatible with zero, while
D^anti-lambda_LL tends to increase with xF, reaching values of 0.4 - 0.5. The
resulting average values are D^lambda_LL = -0.012 +- 0.047 +- 0.024 and
D^anti-lambda_LL = 0.249 +- 0.056 +- 0.049. These results are discussed in the
frame of recent model calculations.Comment: 13 pages, 7 figure
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