126 research outputs found
Quantum criticality, particle-hole symmetry, and duality of the plateau-insulator transition in the quantum Hall regime
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
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
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
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
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
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
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, 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, = 5. For low disorder strength, = 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 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
Π€ΠΈΠ·ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΌΠ΅ΡΠΎΠ΄Ρ ΡΠ΅Π°Π±ΠΈΠ»ΠΈΡΠ°ΡΠΈΠΈ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Ρ ΠΎΡΡΠ΅ΠΎΠ°ΡΡΡΠΎΠ·ΠΎΠΌ: Π½Π°ΡΠΊΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΈΠΉ Π°Π½Π°Π»ΠΈΠ· Π΄ΠΎΠΊΠ°Π·Π°ΡΠ΅Π»ΡΠ½ΡΡ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ
Relevance. A rise in the life expectancy of the planetβs 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.ΠΠΊΡΡΠ°Π»ΡΠ½ΠΎΡΡΡ. Π£Π²Π΅Π»ΠΈΡΠ΅Π½ΠΈΠ΅ ΠΏΡΠΎΠ΄ΠΎΠ»ΠΆΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΠΈ ΠΆΠΈΠ·Π½ΠΈ Π½Π°ΡΠ΅Π»Π΅Π½ΠΈΡ ΠΏΠ»Π°Π½Π΅ΡΡ, Π³ΠΈΠΏΠΎΠ΄ΠΈΠ½Π°ΠΌΠΈΡ ΠΈ ΡΠΎΡΡ ΡΠΈΡΠ»Π° Π»ΡΠ΄Π΅ΠΉ Ρ ΠΈΠ·Π±ΡΡΠΎΡΠ½ΠΎΠΉ ΠΌΠ°ΡΡΠΎΠΉ ΡΠ΅Π»Π° ΠΏΡΠΈΠ²ΠΎΠ΄ΡΡ ΠΊ ΡΠ²Π΅Π»ΠΈΡΠ΅Π½ΠΈΡ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²Π° ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ², ΡΡΡΠ°Π΄Π°ΡΡΠΈΡ
Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΡΠΌΠΈ ΠΎΠΏΠΎΡΠ½ΠΎ-Π΄Π²ΠΈΠ³Π°ΡΠ΅Π»ΡΠ½ΠΎΠ³ΠΎ Π°ΠΏΠΏΠ°ΡΠ°ΡΠ°, Π² ΡΠΎΠΌ ΡΠΈΡΠ»Π΅ ΠΎΡΡΠ΅ΠΎΠ°ΡΡΡΠΎΠ·ΠΎΠΌ. Π£ΡΠΈΡΡΠ²Π°Ρ ΠΎΡΡΡΡΡΡΠ²ΠΈΠ΅ ΡΠΏΠ΅ΡΠΈΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠ°ΡΠΌΠ°ΠΊΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π»Π΅ΡΠ΅Π½ΠΈΡ ΠΎΡΡΠ΅ΠΎΠ°ΡΡΡΠΎΠ·Π°, Π° ΡΠ°ΠΊΠΆΠ΅ ΡΠΎΡΡ ΡΠΈΡΠ»Π° ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Ρ ΠΊΠΎΠΌΠΎΡΠ±ΠΈΠ΄Π½ΠΎΠΉ ΠΏΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΠ΅ΠΉ, Π²ΠΎΠ·Π½ΠΈΠΊΠ»Π° Π½Π΅ΠΎΠ±Ρ
ΠΎΠ΄ΠΈΠΌΠΎΡΡΡ ΠΏΠΎΠΈΡΠΊΠ° Π΄ΠΎΠΊΠ°Π·Π°Π½Π½ΡΡ
ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ ΡΠΈΠ·ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΈ ΡΠ΅Π°Π±ΠΈΠ»ΠΈΡΠ°ΡΠΈΠΎΠ½Π½ΠΎΠΉ ΠΌΠ΅Π΄ΠΈΡΠΈΠ½Ρ (Π€Π Π). Π¦Π΅Π»Ρ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ β Π²ΡΡΠ²ΠΈΡΡ Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΡΠ΅ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ Π€Π Π Π² Π»Π΅ΡΠ΅Π½ΠΈΠΈ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Ρ ΠΎΡΡΠ΅ΠΎΠ°ΡΡΡΠΎΠ·ΠΎΠΌ ΠΈ ΡΡΠΎΡΠΌΡΠ»ΠΈΡΠΎΠ²Π°ΡΡ ΡΠ΅ΠΊΠΎΠΌΠ΅Π½Π΄Π°ΡΠΈΠΈ ΠΏΠΎ ΠΈΡ
ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡ Π΄Π»Ρ ΠΏΡΠ°ΠΊΡΠΈΡΠ΅ΡΠΊΠΈΡ
Π²ΡΠ°ΡΠ΅ΠΉ, ΠΎΡΠ½ΠΎΠ²Π°Π½Π½ΡΠ΅ Π½Π° Π΄ΠΎΠΊΠ°Π·Π°ΡΠ΅Π»ΡΡΡΠ²Π°Ρ
, ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
Π² Ρ
ΠΎΠ΄Π΅ Π°Π½Π°Π»ΠΈΠ·Π° Π±Π°Π· Π΄ΠΎΠΊΠ°Π·Π°ΡΠ΅Π»ΡΠ½ΡΡ
Π΄ΠΎΠ±ΡΠΎΠΊΠ°ΡΠ΅ΡΡΠ²Π΅Π½Π½ΡΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ ΠΏΠΎ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ Π€Π Π. ΠΠ°ΡΠ΅ΡΠΈΠ°Π» ΠΈ ΠΌΠ΅ΡΠΎΠ΄Ρ. Π‘ΡΠ°ΡΡΡ ΠΎΡΠ½ΠΎΠ²Π°Π½Π° Π½Π° ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ°Ρ
Π½Π°ΡΠΊΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π° 1183 ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ, ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½Π½ΡΡ
Ρ 2000 ΠΏΠΎ 2019 Π³., ΠΏΠΎΡΠ²ΡΡΠ΅Π½Π½ΡΡ
ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ Π€Π Π Π² Π»Π΅ΡΠ΅Π½ΠΈΠΈ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Ρ ΠΎΡΡΠ΅ΠΎΠ°ΡΡΡΠΎΠ·ΠΎΠΌ. Π ΠΈΡΠΎΠ³ΠΎΠ²ΡΠΉ Π°Π½Π°Π»ΠΈΠ· ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ Π€Π Π ΠΏΡΠ΅ΠΈΠΌΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎ Π²ΠΊΠ»ΡΡΠ΅Π½Ρ Π·Π°ΡΡΠ±Π΅ΠΆΠ½ΡΠ΅ ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΡΠ΅ΠΊΠΎΠΌΠ΅Π½Π΄Π°ΡΠΈΠΈ/ΡΡΠΊΠΎΠ²ΠΎΠ΄ΡΡΠ²Π° (practice guidelines), ΡΠΈΡΡΠ΅ΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΎΠ±Π·ΠΎΡΡ (Π‘Π), ΠΌΠ΅ΡΠ°Π°Π½Π°Π»ΠΈΠ·Ρ Π ΠΠ, Π΄Π°Π½Π½ΡΠ΅ ΠΎΡΠ΄Π΅Π»ΡΠ½ΡΡ
Π ΠΠ Π½Π° Π°Π½Π³Π»ΠΈΠΉΡΠΊΠΎΠΌ ΠΈΠ»ΠΈ ΡΡΡΡΠΊΠΎΠΌ ΡΠ·ΡΠΊΠ°Ρ
, ΠΎΡΠ΅Π½Π΅Π½Π½ΡΠ΅ Π½Π° 6 Π±Π°Π»Π»ΠΎΠ² ΠΈ Π²ΡΡΠ΅ ΠΏΠΎ ΡΠΊΠ°Π»Π΅ PEDro. Π ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ΅ Π½Π°ΡΠΊΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π° Π±ΡΠ»ΠΈ ΡΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½Ρ ΡΠ°Π±Π»ΠΈΡΡ Π΄ΠΎΠΊΠ°Π·Π°ΡΠ΅Π»ΡΡΡΠ² Ρ ΠΏΡΠΈΡΠ²ΠΎΠ΅Π½ΠΈΠ΅ΠΌ ΠΊΠ°ΠΆΠ΄ΠΎΠΉ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ Π€Π Π ΡΡΠΎΠ²Π½Ρ ΡΠ±Π΅Π΄ΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΠΈ Π΄ΠΎΠΊΠ°Π·Π°ΡΠ΅Π»ΡΡΡΠ² ΠΈ ΠΊΠ»Π°ΡΡΠ° ΡΠ΅ΠΊΠΎΠΌΠ΅Π½Π΄Π°ΡΠΈΠΉ ΠΏΠΎ GRADE Π² ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΠΈΠΈ Ρ ΠΠΠ‘Π’ Π 56034-2014. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ. ΠΠ° ΠΏΠΎΡΠ»Π΅Π΄Π½Π΅Π΅ Π΄Π΅ΡΡΡΠΈΠ»Π΅ΡΠΈΠ΅ ΠΏΡΠΎΠΈΠ·ΠΎΡΠ΅Π» ΠΎΡΡΡΠΈΠΌΡΠΉ ΡΠΎΡΡ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²Π° ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ, ΠΏΠΎΡΠ²ΡΡΠ΅Π½Π½ΡΡ
Π½Π΅ΡΠ°ΡΠΌΠ°ΠΊΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠΌ ΠΌΠ΅ΡΠΎΠ΄Π°ΠΌ Π»Π΅ΡΠ΅Π½ΠΈΡ ΠΎΡΡΠ΅ΠΎΠ°ΡΡΡΠΎΠ·Π°. ΠΠ°ΠΈΠ±ΠΎΠ»Π΅Π΅ ΠΈΠ·ΡΡΠ΅Π½Π½ΡΠΌΠΈ ΠΈΠ· ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ Π€Π Π, ΠΊΠΎΡΠΎΡΡΠ΅ ΠΈΠΌΠ΅ΡΡ Π΄ΠΎΠΊΠ°Π·Π°Π½Π½ΡΠΉ ΡΡΡΠ΅ΠΊΡ, ΡΠ²Π»ΡΡΡΡΡ ΡΠΈΠ·ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΡΠΏΡΠ°ΠΆΠ½Π΅Π½ΠΈΡ Π² ΡΠΎΡΠ΅ΡΠ°Π½ΠΈΠΈ Ρ ΡΡΠ°Π΄ΠΈΡΠΈΠΎΠ½Π½ΠΎΠΉ ΠΎΠ·Π΄ΠΎΡΠΎΠ²ΠΈΡΠ΅Π»ΡΠ½ΠΎΠΉ Π³ΠΈΠΌΠ½Π°ΡΡΠΈΠΊΠΎΠΉ ΠΈ Π°ΠΊΡΠΏΡΠ½ΠΊΡΡΡΠΎΠΉ, ΠΏΠ΅Π»ΠΎΠΈΠ΄ΠΎΡΠ΅ΡΠ°ΠΏΠΈΡ, Π±Π°Π»ΡΠ½Π΅ΠΎΡΠ΅ΡΠ°ΠΏΠΈΡ, Π° ΡΠ°ΠΊΠΆΠ΅ Π½ΠΈΠ·ΠΊΠΎΡΠ°ΡΡΠΎΡΠ½Π°Ρ ΡΠ»Π΅ΠΊΡΡΠΎΡΠ΅ΡΠ°ΠΏΠΈΡ, ΡΠ»ΡΡΡΠ°Π·Π²ΡΠΊΠΎΠ²Π°Ρ ΡΠ΅ΡΠ°ΠΏΠΈΡ ΠΈ ΠΈΠ½ΡΡΠ°ΠΊΡΠ°ΡΠ½Π°Ρ Π»Π°Π·Π΅ΡΠΎΡΠ΅ΡΠ°ΠΏΠΈΡ. ΠΠ°ΠΊΠ»ΡΡΠ΅Π½ΠΈΠ΅. ΠΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ Π€Π Π Π² Π»Π΅ΡΠ΅Π½ΠΈΠΈ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Ρ ΠΎΡΡΠ΅ΠΎΠ°ΡΡΡΠΎΠ·ΠΎΠΌ Π΄ΠΎΠ»ΠΆΠ½ΠΎ Π±ΡΡΡ ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΎ Π½Π° ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ°Ρ
ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅Π½Π½ΡΡ
ΡΠ°Π½Π΄ΠΎΠΌΠΈΠ·ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΠΊΠΎΠ½ΡΡΠΎΠ»ΠΈΡΡΠ΅ΠΌΡΡ
ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ, ΠΊΠΎΡΠΎΡΡΠ΅ ΡΠ»ΡΠΆΠ°Ρ ΠΎΡΠ½ΠΎΠ²ΠΎΠΉ Π΄Π»Ρ ΡΠ°Π·ΡΠ°Π±ΠΎΡΠΊΠΈ ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ΅ΠΊΠΎΠΌΠ΅Π½Π΄Π°ΡΠΈΠΉ. ΠΠ½Π°Π»ΠΈΠ· Π΄Π°Π½Π½ΡΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ Π΄ΠΎΠ»ΠΆΠ΅Π½ Π½ΠΎΡΠΈΡΡ ΡΠ΅Π³ΡΠ»ΡΡΠ½ΡΠΉ Ρ
Π°ΡΠ°ΠΊΡΠ΅Ρ
Abelian gauge potentials on cubic lattices
The study of the properties of quantum particles in a periodic potential
subject to a magnetic field is an active area of research both in physics and
mathematics; it has been and it is still deeply investigated. In this review we
discuss how to implement and describe tunable Abelian magnetic fields in a
system of ultracold atoms in optical lattices. After discussing two of the main
experimental schemes for the physical realization of synthetic gauge potentials
in ultracold set-ups, we study cubic lattice tight-binding models with
commensurate flux. We finally examine applications of gauge potentials in
one-dimensional rings.Comment: To appear on: "Advances in Quantum Mechanics: Contemporary Trends and
Open Problems", G. Dell'Antonio and A. Michelangeli eds., Springer-INdAM
series 201
Scattering theory and ground-state energy of Dirac fermions in graphene with two Coulomb impurities
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
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