102 research outputs found

    Quantum criticality, particle-hole symmetry, and duality of the plateau-insulator transition in the quantum Hall regime

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    We report new experimental data on the plateau-insulator transition in the quantum Hall regime, taken from a low mobility InGaAs/InP heterostructure. By employing the fundamental symmetries of the quantum transport problem we are able to disentangle the universal quantum critical aspects of the magnetoresistance data (critical indices and scaling functions) and the sample dependent aspects due to macroscopic inhomogeneities. Our new results and methodology indicate that the previously established experimental value for the critical index (kappa = 0.42) resulted from an admixture of both universal and sample dependent behavior. A novel, non-Fermi liquid value is found (kappa = 0.57) along with the leading corrections to scaling. The statement of self-duality under the Chern Simons flux attachment transformation is verified.Comment: 4 pages, 2 figure

    New Insights into the Plateau-Insulator Transition in the Quantum Hall Regime

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    We have measured the quantum critical behavior of the plateau-insulator (PI) transition in a low-mobility InGaAs/GaAs quantum well. The longitudinal resistivity measured for two different values of the electron density follows an exponential law, from which we extract critical exponents kappa = 0.54 and 0.58, in good agreement with the value (kappa = 0.57) previously obtained for an InGaAs/InP heterostructure. This provides evidence for a non-Fermi liquid critical exponent. By reversing the direction of the magnetic field we find that the averaged Hall resistance remains quantized at the plateau value h/e^2 through the PI transition. From the deviations of the Hall resistance from the quantized value, we obtain the corrections to scaling.Comment: accepted proceedings of EP2DS-15 (to be published in Physica E

    The effect of carrier density gradients on magnetotransport data measured in Hall bar geometry

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    We have measured magnetotransport of the two-dimensional electron gas in a Hall bar geometry in the presence of small carrier density gradients. We find that the longitudinal resistances measured at both sides of the Hall bar interchange by reversing the polarity of the magnetic field. We offer a simple explanation for this effect and discuss implications for extracting conductivity flow diagrams of the integer quantum Hall effect.Comment: 7 pages, 8 figure

    The effects of macroscopic inhomogeneities on the magneto transport properties of the electron gas in two dimensions

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    In experiments on electron transport the macroscopic inhomogeneities in the sample play a fundamental role. In this paper and a subsequent one we introduce and develop a general formalism that captures the principal features of sample inhomogeneities (density gradients, contact misalignments) in the magneto resistance data taken from low mobility heterostructures. We present detailed assessments and experimental investigations of the different regimes of physical interest, notably the regime of semiclassical transport at weak magnetic fields, the plateau-plateau transitions as well as the plateau-insulator transition that generally occurs at much stronger values of the external field only. It is shown that the semiclassical regime at weak fields plays an integral role in the general understanding of the experiments on the quantum Hall regime. The results of this paper clearly indicate that the plateau-plateau transitions, unlike the the plateau-insulator transition, are fundamentally affected by the presence of sample inhomogeneities. We propose a universal scaling result for the magneto resistance parameters. This result facilitates, amongst many other things, a detailed understanding of the difficulties associated with the experimental methodology of H.P. Wei et.al in extracting the quantum critical behavior of the electron gas from the transport measurements conducted on the plateau-plateau transitions.Comment: 20 pages, 9 figure

    Modeling electrolytically top gated graphene

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    We investigate doping of a single-layer graphene in the presence of electrolytic top gating. The interfacial phenomena is modeled using a modified Poisson-Boltzmann equation for an aqueous solution of simple salt. We demonstrate both the sensitivity of graphene's doping levels to the salt concentration and the importance of quantum capacitance that arises due to the smallness of the Debye screening length in the electrolyte.Comment: 7 pages, including 4 figures, submitted to Nanoscale Research Letters for a special issue related to the NGC 2009 conference (http://asdn.net/ngc2009/index.shtml

    High-temperature quantum oscillations caused by recurring Bloch states in graphene superlattices

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    Cyclotron motion of charge carriers in metals and semiconductors leads to Landau quantization and magneto-oscillatory behavior in their properties. Cryogenic temperatures are usually required to observe these oscillations. We show that graphene superlattices support a different type of quantum oscillations that do not rely on Landau quantization. The oscillations are extremely robust and persist well above room temperature in magnetic fields of only a few T. We attribute this phenomenon to repetitive changes in the electronic structure of superlattices such that charge carriers experience effectively no magnetic field at simple fractions of the flux quantum per superlattice unit cell. Our work points at unexplored physics in Hofstadter butterfly systems at high temperatures

    Exact eigenstate analysis of finite-frequency conductivity in graphene

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    We employ the exact eigenstate basis formalism to study electrical conductivity in graphene, in the presence of short-range diagonal disorder and inter-valley scattering. We find that for disorder strength, W≄W \ge 5, the density of states is flat. We, then, make connection, using the MRG approach, with the work of Abrahams \textit{et al.} and find a very good agreement for disorder strength, WW = 5. For low disorder strength, WW = 2, we plot the energy-resolved current matrix elements squared for different locations of the Fermi energy from the band centre. We find that the states close to the band centre are more extended and falls of nearly as 1/El21/E_l^{2} as we move away from the band centre. Further studies of current matrix elements versus disorder strength suggests a cross-over from weakly localized to a very weakly localized system. We calculate conductivity using Kubo Greenwood formula and show that, for low disorder strength, conductivity is in a good qualitative agreement with the experiments, even for the on-site disorder. The intensity plots of the eigenstates also reveal clear signatures of puddle formation for very small carrier concentration. We also make comparison with square lattice and find that graphene is more easily localized when subject to disorder.Comment: 11 pages,15 figure

    ЀОзОчДсĐșОД ĐŒĐ”Ń‚ĐŸĐŽŃ‹ рДабОлОтацОО ĐżĐ°Ń†ĐžĐ”ĐœŃ‚ĐŸĐČ Ń ĐŸŃŃ‚Đ”ĐŸĐ°Ń€Ń‚Ń€ĐŸĐ·ĐŸĐŒ: ĐœĐ°ŃƒĐșĐŸĐŒĐ”Ń‚Ń€ĐžŃ‡Đ”ŃĐșĐžĐč Đ°ĐœĐ°Đ»ĐžĐ· ĐŽĐŸĐșĐ°Đ·Đ°Ń‚Đ”Đ»ŃŒĐœŃ‹Ń… ĐžŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœĐžĐč

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    Relevance. A rise in the life expectancy of the planet’s population, lack of exercise and growth in the number of people suffering from overweight lead to an increase in the number of patients suffering from diseases of the musculoskeletal system, including osteoarthritis. Given the absence of specific pharmacological treatment of osteoarthritis, as well as the increase in the number of patients with co-morbid pathology, it became necessary to search for the proven technologies of physical and rehabilitation medicine (PRM). The purpose of the study was to identify the most effective PRM technologies in the treatment of patients with osteoarthritis and to formulate recommendations on their use for practitioners, based on the proof obtained through the analysis of evidence-based high quality studies on the application of PRM technology. Materials and Methods. Over the past decade, there has been a significant increase in the number of studies on non-pharmacological methods of osteoarthritis treatment. The most studied of the PRM technologies with the proven effect were the following: physical exercises combined with traditional healthy gymnastics, acupuncture, peloid therapy, balneo therapy, as well as low-frequency electrotherapy, ultrasound therapy and infrared laser therapy. Conclusion. The use of PRM technologies in the treatment of patients with osteoarthritis should be based on the results of high-quality randomized controlled clinical trials which serve as the basis for the development of clinical recommendations. The process of the obtained data analysis should be conducted on the regular basis.АĐșŃ‚ŃƒĐ°Đ»ŃŒĐœĐŸŃŃ‚ŃŒ. ĐŁĐČĐ”Đ»ĐžŃ‡Đ”ĐœĐžĐ” ĐżŃ€ĐŸĐŽĐŸĐ»Đ¶ĐžŃ‚Đ”Đ»ŃŒĐœĐŸŃŃ‚Đž Đ¶ĐžĐ·ĐœĐž ĐœĐ°ŃĐ”Đ»Đ”ĐœĐžŃ ĐżĐ»Đ°ĐœĐ”Ń‚Ń‹, ĐłĐžĐżĐŸĐŽĐžĐœĐ°ĐŒĐžŃ Đž Ń€ĐŸŃŃ‚ чОсла люЎДĐč с ĐžĐ·Đ±Ń‹Ń‚ĐŸŃ‡ĐœĐŸĐč ĐŒĐ°ŃŃĐŸĐč тДла проĐČĐŸĐŽŃŃ‚ Đș уĐČĐ”Đ»ĐžŃ‡Đ”ĐœĐžŃŽ ĐșĐŸĐ»ĐžŃ‡Đ”ŃŃ‚ĐČĐ° ĐżĐ°Ń†ĐžĐ”ĐœŃ‚ĐŸĐČ, страЮающох Đ·Đ°Đ±ĐŸĐ»Đ”ĐČĐ°ĐœĐžŃĐŒĐž ĐŸĐżĐŸŃ€ĐœĐŸ-ĐŽĐČĐžĐłĐ°Ń‚Đ”Đ»ŃŒĐœĐŸĐłĐŸ аппарата, ĐČ Ń‚ĐŸĐŒ чОслД ĐŸŃŃ‚Đ”ĐŸĐ°Ń€Ń‚Ń€ĐŸĐ·ĐŸĐŒ. УчотыĐČая ĐŸŃ‚ŃŃƒŃ‚ŃŃ‚ĐČОД спДцОфОчДсĐșĐŸĐłĐŸ Ń„Đ°Ń€ĐŒĐ°ĐșĐŸĐ»ĐŸĐłĐžŃ‡Đ”ŃĐșĐŸĐłĐŸ Đ»Đ”Ń‡Đ”ĐœĐžŃ ĐŸŃŃ‚Đ”ĐŸĐ°Ń€Ń‚Ń€ĐŸĐ·Đ°, Đ° таĐșжД Ń€ĐŸŃŃ‚ чОсла ĐżĐ°Ń†ĐžĐ”ĐœŃ‚ĐŸĐČ Ń ĐșĐŸĐŒĐŸŃ€Đ±ĐžĐŽĐœĐŸĐč ĐżĐ°Ń‚ĐŸĐ»ĐŸĐłĐžĐ”Đč, ĐČĐŸĐ·ĐœĐžĐșла ĐœĐ”ĐŸĐ±Ń…ĐŸĐŽĐžĐŒĐŸŃŃ‚ŃŒ ĐżĐŸĐžŃĐșĐ° ĐŽĐŸĐșĐ°Đ·Đ°ĐœĐœŃ‹Ń… Ń‚Đ”Ń…ĐœĐŸĐ»ĐŸĐłĐžĐč фОзОчДсĐșĐŸĐč Đž Ń€Đ”Đ°Đ±ĐžĐ»ĐžŃ‚Đ°Ń†ĐžĐŸĐœĐœĐŸĐč ĐŒĐ”ĐŽĐžŃ†ĐžĐœŃ‹ (Đ€Đ Đœ). ĐŠĐ”Đ»ŃŒ ĐžŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœĐžŃ — ĐČыяĐČоть ĐœĐ°ĐžĐ±ĐŸĐ»Đ”Đ” ŃŃ„Ń„Đ”ĐșтоĐČĐœŃ‹Đ” Ń‚Đ”Ń…ĐœĐŸĐ»ĐŸĐłĐžĐž Đ€Đ Đœ ĐČ Đ»Đ”Ń‡Đ”ĐœĐžĐž ĐżĐ°Ń†ĐžĐ”ĐœŃ‚ĐŸĐČ Ń ĐŸŃŃ‚Đ”ĐŸĐ°Ń€Ń‚Ń€ĐŸĐ·ĐŸĐŒ Đž ŃŃ„ĐŸŃ€ĐŒŃƒĐ»ĐžŃ€ĐŸĐČать рДĐșĐŸĐŒĐ”ĐœĐŽĐ°Ń†ĐžĐž ĐżĐŸ ох ĐżŃ€ĐžĐŒĐ”ĐœĐ”ĐœĐžŃŽ ĐŽĐ»Ń праĐșтОчДсĐșох ĐČрачДĐč, ĐŸŃĐœĐŸĐČĐ°ĐœĐœŃ‹Đ” ĐœĐ° ĐŽĐŸĐșĐ°Đ·Đ°Ń‚Đ”Đ»ŃŒŃŃ‚ĐČах, ĐżĐŸĐ»ŃƒŃ‡Đ”ĐœĐœŃ‹Ń… ĐČ Ń…ĐŸĐŽĐ” Đ°ĐœĐ°Đ»ĐžĐ·Đ° баз ĐŽĐŸĐșĐ°Đ·Đ°Ń‚Đ”Đ»ŃŒĐœŃ‹Ń… ĐŽĐŸĐ±Ń€ĐŸĐșачДстĐČĐ”ĐœĐœŃ‹Ń… ĐžŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœĐžĐč ĐżĐŸ ĐżŃ€ĐžĐŒĐ”ĐœĐ”ĐœĐžŃŽ Ń‚Đ”Ń…ĐœĐŸĐ»ĐŸĐłĐžĐž Đ€Đ Đœ. ĐœĐ°Ń‚Đ”Ń€ĐžĐ°Đ» Đž ĐŒĐ”Ń‚ĐŸĐŽŃ‹. Статья ĐŸŃĐœĐŸĐČĐ°ĐœĐ° ĐœĐ° Ń€Đ”Đ·ŃƒĐ»ŃŒŃ‚Đ°Ń‚Đ°Ń… ĐœĐ°ŃƒĐșĐŸĐŒĐ”Ń‚Ń€ĐžŃ‡Đ”ŃĐșĐŸĐłĐŸ Đ°ĐœĐ°Đ»ĐžĐ·Đ° 1183 ĐžŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœĐžĐč, ĐżŃ€ĐŸĐČĐ”ĐŽĐ”ĐœĐœŃ‹Ń… с 2000 ĐżĐŸ 2019 Đł., ĐżĐŸŃĐČŃŃ‰Đ”ĐœĐœŃ‹Ń… ĐžŃĐżĐŸĐ»ŃŒĐ·ĐŸĐČĐ°ĐœĐžŃŽ Ń‚Đ”Ń…ĐœĐŸĐ»ĐŸĐłĐžĐč Đ€Đ Đœ ĐČ Đ»Đ”Ń‡Đ”ĐœĐžĐž ĐżĐ°Ń†ĐžĐ”ĐœŃ‚ĐŸĐČ Ń ĐŸŃŃ‚Đ”ĐŸĐ°Ń€Ń‚Ń€ĐŸĐ·ĐŸĐŒ. В ĐžŃ‚ĐŸĐłĐŸĐČыĐč Đ°ĐœĐ°Đ»ĐžĐ· Ń‚Đ”Ń…ĐœĐŸĐ»ĐŸĐłĐžĐč Đ€Đ Đœ ĐżŃ€Đ”ĐžĐŒŃƒŃ‰Đ”ŃŃ‚ĐČĐ”ĐœĐœĐŸ ĐČĐșĐ»ŃŽŃ‡Đ”ĐœŃ‹ Đ·Đ°Ń€ŃƒĐ±Đ”Đ¶ĐœŃ‹Đ” ĐșĐ»ĐžĐœĐžŃ‡Đ”ŃĐșОД рДĐșĐŸĐŒĐ”ĐœĐŽĐ°Ń†ĐžĐž/руĐșĐŸĐČĐŸĐŽŃŃ‚ĐČĐ° (practice guidelines), ŃĐžŃŃ‚Đ”ĐŒĐ°Ń‚ĐžŃ‡Đ”ŃĐșОД ĐŸĐ±Đ·ĐŸŃ€Ń‹ (СО), ĐŒĐ”Ń‚Đ°Đ°ĐœĐ°Đ»ĐžĐ·Ń‹ РКИ, ĐŽĐ°ĐœĐœŃ‹Đ” ĐŸŃ‚ĐŽĐ”Đ»ŃŒĐœŃ‹Ń… РКИ ĐœĐ° Đ°ĐœĐłĐ»ĐžĐčсĐșĐŸĐŒ ОлО руссĐșĐŸĐŒ ŃĐ·Ń‹Đșах, ĐŸŃ†Đ”ĐœĐ”ĐœĐœŃ‹Đ” ĐœĐ° 6 Đ±Đ°Đ»Đ»ĐŸĐČ Đž ĐČŃ‹ŃˆĐ” ĐżĐŸ шĐșалД PEDro. В Ń€Đ”Đ·ŃƒĐ»ŃŒŃ‚Đ°Ń‚Đ” ĐœĐ°ŃƒĐșĐŸĐŒĐ”Ń‚Ń€ĐžŃ‡Đ”ŃĐșĐŸĐłĐŸ Đ°ĐœĐ°Đ»ĐžĐ·Đ° былО ŃŃ„ĐŸŃ€ĐŒĐžŃ€ĐŸĐČĐ°ĐœŃ‹ таблОцы ĐŽĐŸĐșĐ°Đ·Đ°Ń‚Đ”Đ»ŃŒŃŃ‚ĐČ Ń просĐČĐŸĐ”ĐœĐžĐ”ĐŒ ĐșĐ°Đ¶ĐŽĐŸĐč Ń‚Đ”Ń…ĐœĐŸĐ»ĐŸĐłĐžĐž Đ€Đ Đœ ŃƒŃ€ĐŸĐČĐœŃ ŃƒĐ±Đ”ĐŽĐžŃ‚Đ”Đ»ŃŒĐœĐŸŃŃ‚Đž ĐŽĐŸĐșĐ°Đ·Đ°Ń‚Đ”Đ»ŃŒŃŃ‚ĐČ Đž Đșласса рДĐșĐŸĐŒĐ”ĐœĐŽĐ°Ń†ĐžĐč ĐżĐŸ GRADE ĐČ ŃĐŸĐŸŃ‚ĐČДтстĐČОО с ГОСб Đ  56034-2014. Đ Đ”Đ·ŃƒĐ»ŃŒŃ‚Đ°Ń‚Ń‹. За ĐżĐŸŃĐ»Đ”ĐŽĐœĐ”Đ” ĐŽĐ”ŃŃŃ‚ĐžĐ»Đ”Ń‚ĐžĐ” ĐżŃ€ĐŸĐžĐ·ĐŸŃˆĐ”Đ» ĐŸŃ‰ŃƒŃ‚ĐžĐŒŃ‹Đč Ń€ĐŸŃŃ‚ ĐșĐŸĐ»ĐžŃ‡Đ”ŃŃ‚ĐČĐ° ĐžŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœĐžĐč, ĐżĐŸŃĐČŃŃ‰Đ”ĐœĐœŃ‹Ń… ĐœĐ”Ń„Đ°Ń€ĐŒĐ°ĐșĐŸĐ»ĐŸĐłĐžŃ‡Đ”ŃĐșĐžĐŒ ĐŒĐ”Ń‚ĐŸĐŽĐ°ĐŒ Đ»Đ”Ń‡Đ”ĐœĐžŃ ĐŸŃŃ‚Đ”ĐŸĐ°Ń€Ń‚Ń€ĐŸĐ·Đ°. ĐĐ°ĐžĐ±ĐŸĐ»Đ”Đ” ĐžĐ·ŃƒŃ‡Đ”ĐœĐœŃ‹ĐŒĐž Оз Ń‚Đ”Ń…ĐœĐŸĐ»ĐŸĐłĐžĐč Đ€Đ Đœ, ĐșĐŸŃ‚ĐŸŃ€Ń‹Đ” ĐžĐŒĐ”ŃŽŃ‚ ĐŽĐŸĐșĐ°Đ·Đ°ĐœĐœŃ‹Đč ŃŃ„Ń„Đ”Đșт, яĐČĐ»ŃŃŽŃ‚ŃŃ фОзОчДсĐșОД ŃƒĐżŃ€Đ°Đ¶ĐœĐ”ĐœĐžŃ ĐČ ŃĐŸŃ‡Đ”Ń‚Đ°ĐœĐžĐž с Ń‚Ń€Đ°ĐŽĐžŃ†ĐžĐŸĐœĐœĐŸĐč ĐŸĐ·ĐŽĐŸŃ€ĐŸĐČĐžŃ‚Đ”Đ»ŃŒĐœĐŸĐč ĐłĐžĐŒĐœĐ°ŃŃ‚ĐžĐșĐŸĐč Đž Đ°ĐșŃƒĐżŃƒĐœĐșŃ‚ŃƒŃ€ĐŸĐč, ĐżĐ”Đ»ĐŸĐžĐŽĐŸŃ‚Đ”Ń€Đ°ĐżĐžŃ, Đ±Đ°Đ»ŃŒĐœĐ”ĐŸŃ‚Đ”Ń€Đ°ĐżĐžŃ, Đ° таĐșжД ĐœĐžĐ·ĐșĐŸŃ‡Đ°ŃŃ‚ĐŸŃ‚ĐœĐ°Ń ŃĐ»Đ”ĐșŃ‚Ń€ĐŸŃ‚Đ”Ń€Đ°ĐżĐžŃ, ŃƒĐ»ŃŒŃ‚Ń€Đ°Đ·ĐČуĐșĐŸĐČая Ń‚Đ”Ń€Đ°ĐżĐžŃ Đž ĐžĐœŃ„Ń€Đ°ĐșŃ€Đ°ŃĐœĐ°Ń Đ»Đ°Đ·Đ”Ń€ĐŸŃ‚Đ”Ń€Đ°ĐżĐžŃ. ЗаĐșĐ»ŃŽŃ‡Đ”ĐœĐžĐ”. Đ˜ŃĐżĐŸĐ»ŃŒĐ·ĐŸĐČĐ°ĐœĐžĐ” Ń‚Đ”Ń…ĐœĐŸĐ»ĐŸĐłĐžĐč Đ€Đ Đœ ĐČ Đ»Đ”Ń‡Đ”ĐœĐžĐž ĐżĐ°Ń†ĐžĐ”ĐœŃ‚ĐŸĐČ Ń ĐŸŃŃ‚Đ”ĐŸĐ°Ń€Ń‚Ń€ĐŸĐ·ĐŸĐŒ ĐŽĐŸĐ»Đ¶ĐœĐŸ Đ±Ń‹Ń‚ŃŒ ĐŸŃĐœĐŸĐČĐ°ĐœĐŸ ĐœĐ° Ń€Đ”Đ·ŃƒĐ»ŃŒŃ‚Đ°Ń‚Đ°Ń… ĐșачДстĐČĐ”ĐœĐœŃ‹Ń… Ń€Đ°ĐœĐŽĐŸĐŒĐžĐ·ĐžŃ€ĐŸĐČĐ°ĐœĐœŃ‹Ń… ĐșĐŸĐœŃ‚Ń€ĐŸĐ»ĐžŃ€ŃƒĐ”ĐŒŃ‹Ń… ĐșĐ»ĐžĐœĐžŃ‡Đ”ŃĐșох ĐžŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœĐžĐč, ĐșĐŸŃ‚ĐŸŃ€Ń‹Đ” ŃĐ»ŃƒĐ¶Đ°Ń‚ ĐŸŃĐœĐŸĐČĐŸĐč ĐŽĐ»Ń Ń€Đ°Đ·Ń€Đ°Đ±ĐŸŃ‚ĐșĐž ĐșĐ»ĐžĐœĐžŃ‡Đ”ŃĐșох рДĐșĐŸĐŒĐ”ĐœĐŽĐ°Ń†ĐžĐč. ĐĐœĐ°Đ»ĐžĐ· ĐŽĐ°ĐœĐœŃ‹Ń… ĐžŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœĐžĐč ĐŽĐŸĐ»Đ¶Đ”Đœ ĐœĐŸŃĐžŃ‚ŃŒ Ń€Đ”ĐłŃƒĐ»ŃŃ€ĐœŃ‹Đč хараĐșтДр

    Scattering theory and ground-state energy of Dirac fermions in graphene with two Coulomb impurities

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    We study the physics of Dirac fermions in a gapped graphene monolayer containing two Coulomb impurities. For the case of equal impurity charges, we discuss the ground-state energy using the linear combination of atomic orbitals (LCAO) approach. For opposite charges of the Coulomb centers, an electric dipole potential results at large distances. We provide a nonperturbative analysis of the corresponding low-energy scattering problem

    Measurement of the cross section for isolated-photon plus jet production in pp collisions at √s=13 TeV using the ATLAS detector

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    The dynamics of isolated-photon production in association with a jet in proton–proton collisions at a centre-of-mass energy of 13 TeV are studied with the ATLAS detector at the LHC using a dataset with an integrated luminosity of 3.2 fb−1. Photons are required to have transverse energies above 125 GeV. Jets are identified using the anti- algorithm with radius parameter and required to have transverse momenta above 100 GeV. Measurements of isolated-photon plus jet cross sections are presented as functions of the leading-photon transverse energy, the leading-jet transverse momentum, the azimuthal angular separation between the photon and the jet, the photon–jet invariant mass and the scattering angle in the photon–jet centre-of-mass system. Tree-level plus parton-shower predictions from Sherpa and Pythia as well as next-to-leading-order QCD predictions from Jetphox and Sherpa are compared to the measurements
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