1,347 research outputs found
Quantum integrability of the Alday-Arutyunov-Frolov model
We investigate the quantum integrability of the Alday-Arutyunov-Frolov (AAF)
model by calculating the three-particle scattering amplitude at the first
non-trivial order and showing that the S-matrix is factorizable at this order.
We consider a more general fermionic model and find a necessary constraint to
ensure its integrability at quantum level. We then show that the quantum
integrability of the AAF model follows from this constraint. In the process, we
also correct some missed points in earlier works.Comment: 40 pages; Replaced with published version. Appendix and comments
adde
Ictal and interictal MEG in pediatric patients with tuberous sclerosis and drug resistant epilepsy
Purpose: Drug resistant epilepsy (DRE) is common in patients with tuberous sclerosis (TS). Interictal MEG has been shown as a valuable instrument in the presurgical workup. The goal of our study was to evaluate the role of ictal MEG in epileptogenic tuber selection, especially in patients with multiple irritative zones. Methods: The clinical and MEG data of 23 patients with TS and DRE from two medical/research centers were reviewed. Seven pediatric patients, who had seizures during MEG recording and underwent resection or disconnection surgery, were included into the study. Cortical sources of ictal and interictal epileptiform MEG discharges were compared with epileptogenic zone location in six patients with favorable surgery outcome. Results: In patients who improved substantially after surgery all resected and several other tubers demonstrated epileptiform activity on interictal MEG. Ictal MEG provided crucial information about lobar location of the seizure onset zone (SOZ) in two cases, and in the other four it confirmed the SOZ location derived from the interictal data. In one case, ictal MEG findings were unreliable. In one patient, who did not benefit from surgical treatment, the resected tubers did not overlap with interictal and ictal MEG sources. Conclusion: The combination of interictal and ictal MEG is a valuable tool for identification of the epileptogenic tuber/tubers in presurgical work-up in patients with TS.Peer reviewe
Quantum oscillations from Fermi arcs
When a metal is subjected to strong magnetic field B nearly all measurable
quantities exhibit oscillations periodic in 1/B. Such quantum oscillations
represent a canonical probe of the defining aspect of a metal, its Fermi
surface (FS). In this study we establish a new mechanism for quantum
oscillations which requires only finite segments of a FS to exist. Oscillations
periodic in 1/B occur if the FS segments are terminated by a pairing gap. Our
results reconcile the recent breakthrough experiments showing quantum
oscillations in a cuprate superconductor YBCO, with a well-established result
of many angle resolved photoemission (ARPES) studies which consistently
indicate "Fermi arcs" -- truncated segments of a Fermi surface -- in the normal
state of the cuprates.Comment: 8 pages, 5 figure
The S-matrix of the Faddeev-Reshetikhin Model, Diagonalizability and PT Symmetry
We study the question of diagonalizability of the Hamiltonian for the
Faddeev-Reshetikhin (FR) model in the two particle sector. Although the two
particle S-matrix element for the FR model, which may be relevant for the
quantization of strings on , has been calculated recently
using field theoretic methods, we find that the Hamiltonian for the system in
this sector is not diagonalizable. We trace the difficulty to the fact that the
interaction term in the Hamiltonian violating Lorentz invariance leads to
discontinuity conditions (matching conditions) that cannot be satisfied. We
determine the most general quartic interaction Hamiltonian that can be
diagonalized. This includes the bosonic Thirring model as well as the bosonic
chiral Gross-Neveu model which we find share the same S-matrix. We explain this
by showing, through a Fierz transformation, that these two models are in fact
equivalent. In addition, we find a general quartic interaction Hamiltonian,
violating Lorentz invariance, that can be diagonalized with the same two
particle S-matrix element as calculated by Klose and Zarembo for the FR model.
This family of generalized interaction Hamiltonians is not Hermitian, but is
symmetric. We show that the wave functions for this system are also
symmetric. Thus, the theory is in a unbroken phase which guarantees the
reality of the energy spectrum as well as the unitarity of the S-matrix.Comment: 32 pages, 1 figure; references added, version published in JHE
Quasiparticle Hall Transport of d-wave Superconductors in Vortex State
We present a theory of quasiparticle Hall transport in strongly type-II
superconductors within their vortex state. We establish the existence of
integer quantum spin Hall effect in clean unconventional
superconductors in the vortex state from a general analysis of the
Bogoliubov-de Gennes equation. The spin Hall conductivity is
shown to be quantized in units of . This result does not
rest on linearization of the BdG equations around Dirac nodes and therefore
includes inter-nodal physics in its entirety. In addition, this result holds
for a generic inversion-symmetric lattice of vortices as long as the magnetic
field satisfies . We then derive the
Wiedemann-Franz law for the spin and thermal Hall conductivity in the vortex
state. In the limit of , the thermal Hall conductivity satisfies
. The
transitions between different quantized values of as well as
relation to conventional superconductors are discussed.Comment: 18 pages REVTex, 3 figures, references adde
Π‘ΡΠ°Π²Π½ΠΈΡΠ΅Π»ΡΠ½ΡΠΉ Π°Π½Π°Π»ΠΈΠ· Π²ΠΎΠ·Π±ΡΠ΄ΠΈΠΌΠΎΡΡΠΈ ΠΊΠΎΡΠ΅ΡΠΊΠΎΠ²ΠΎΠΉ ΠΈ Π²Π½ΡΡΡΠΈΠΌΡΡΠ΅ΡΠ½ΠΎΠΉ Π°ΠΊΡΠΎΠ½Π°Π»ΡΠ½ΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌ Ρ Π·Π΄ΠΎΡΠΎΠ²ΡΡ Π΄ΠΎΠ±ΡΠΎΠ²ΠΎΠ»ΡΡΠ΅Π² ΠΏΡΠΈ ΠΏΠ΅ΡΠΈΡΠ΅ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎΠΉ ΡΡΠΈΠΌΡΠ»ΡΡΠΈΠΈ
Background. Peripheral magnetic stimulation (PMS) is applied over spinal roots, peripheral nerves, terminal motor nerve branches. PMS has been used as a method of diagnosis and treatment for two decades. Despite the considerable amount of PMS studies, there is no consensus on the approach to determine the intensity of the magnetic stimulus in the treatment stimulation, the need for the differentiated activation of the different parts of the peripheral nervous system. This was the prerequisite for carrying out this study. Β Objective: to investigate the PMS intensity required to activate spinal roots and terminal nerve branches, the second object was the comparison of the threshold values among volunteers. Materials and methods. Thirty four healthy subjects with no neuromuscular diseases were enrolled in the study (mean age 31.0 Β± 8.6 years). PNS was applied by Magstim 200 magnetic stimulator (Great Britain). During the research the subjective threshold, the threshold of muscle contraction, the threshold of the root activation (according to motor evoked potential) were estimated. Stimulation-induced muscle activity was recorded via surface EMG system (Neurosoft, Russia) synchronized with the magnetic stimulator. Results. The analysis of data identified the significant differences (p <0.05) between the root activation and terminal nerve branches threshold values. There were no reports of gender differences between the threshold values of all investigated parameters within the group (p >0.05). There were no significant differences between right and left limbs (p >0.05) in the comparison of all parameters. Conclusion. The results of the present study can indicate the possibility of the individual approach of the determination the intensity of the magnetic stimulus for each patient. The findings of our study provide an opportunity for a better understanding of the action mechanism of PMS and can be used in order to develop the treatment algorithm for the use in the clinical settings.ΠΠ²Π΅Π΄Π΅Π½ΠΈΠ΅. ΠΠ΅ΡΠΈΡΠ΅ΡΠΈΡΠ΅ΡΠΊΠ°Ρ ΠΌΠ°Π³Π½ΠΈΡΠ½Π°Ρ ΡΡΠΈΠΌΡΠ»ΡΡΠΈΡ (ΠΠΠ‘) ΠΏΡΠ΅Π΄ΠΏΠΎΠ»Π°Π³Π°Π΅Ρ Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ ΠΈΠΌΠΏΡΠ»ΡΡΠ½ΠΎΠ³ΠΎ ΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΠ»Ρ Π½Π° ΡΡΡΡΠΊΡΡΡΡ ΠΏΠ΅ΡΠΈΡΠ΅ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ Π½Π΅ΡΠ²Π½ΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΡ: ΠΊΠΎΡΠ΅ΡΠΊΠΈ, ΡΠΏΠΈΠ½Π½ΠΎΠΌΠΎΠ·Π³ΠΎΠ²ΡΠ΅ ΠΈ ΠΏΠ΅ΡΠΈΡΠ΅ΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ Π½Π΅ΡΠ²Ρ. Π ΠΏΠΎΡΠ»Π΅Π΄Π½ΠΈΠ΅ Π³ΠΎΠ΄Ρ ΠΠΠ‘ ΡΠΈΡΠΎΠΊΠΎ ΠΈΡΠΏΠΎΠ»ΡΠ·ΡΠ΅ΡΡΡ Π² ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅ ΠΌΠ΅ΡΠΎΠ΄Π° Π΄ΠΈΠ°Π³Π½ΠΎΡΡΠΈΠΊΠΈ ΠΈ Π»Π΅ΡΠ΅Π½ΠΈΡ. ΠΠ΅ΡΠΌΠΎΡΡΡ Π½Π° Π±ΠΎΠ»ΡΡΠΎΠ΅ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²ΠΎ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ ΠΠΠ‘, Π½Π΅ ΡΡΡΠ΅ΡΡΠ²ΡΠ΅Ρ Π΅Π΄ΠΈΠ½ΠΎΠ³ΠΎ ΠΌΠ½Π΅Π½ΠΈΡ ΠΎ ΠΏΠΎΠ΄Ρ
ΠΎΠ΄Π΅ ΠΊ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΠΈ ΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎΠ³ΠΎ ΡΡΠΈΠΌΡΠ»Π° ΠΏΡΠΈ Π»Π΅ΡΠ΅Π±Π½ΠΎΠΉ ΡΡΠΈΠΌΡΠ»ΡΡΠΈΠΈ, Π½Π΅ΠΎΠ±Ρ
ΠΎΠ΄ΠΈΠΌΠΎΡΡΠΈ Π΄ΠΈΡΡΠ΅ΡΠ΅Π½ΡΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΉ ΡΡΠΈΠΌΡΠ»ΡΡΠΈΠΈ ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
ΠΎΡΠ΄Π΅Π»ΠΎΠ² ΠΏΠ΅ΡΠΈΡΠ΅ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ Π½Π΅ΡΠ²Π½ΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΡ, ΡΡΠΎ ΡΠ²ΠΈΠ»ΠΎΡΡ ΠΏΡΠ΅Π΄ΠΏΠΎΡΡΠ»ΠΊΠΎΠΉ Π΄Π»Ρ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΈΡ Π΄Π°Π½Π½ΠΎΠΉ ΡΠ°Π±ΠΎΡΡ. Π¦Π΅Π»Ρ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ β ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ ΠΏΠΎΡΠΎΠ³ΠΎΠ² Π²ΠΎΠ·Π±ΡΠΆΠ΄Π΅Π½ΠΈΡ Π΄Π²ΠΈΠ³Π°ΡΠ΅Π»ΡΠ½ΠΎΠΉ ΠΊΠΎΡΠ΅ΡΠΊΠΎΠ²ΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΡ ΠΈ ΡΠ΅ΡΠΌΠΈΠ½Π°Π»ΡΠ½ΡΡ
Π²Π΅ΡΠ²Π΅ΠΉ Π°ΠΊΡΠΎΠ½Π° ΠΏΡΠΈ ΠΠΠ‘. ΠΡΠ»ΠΎ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΠ΅ ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
ΠΏΠΎΡΠΎΠ³ΠΎΠ²ΡΡ
Π·Π½Π°ΡΠ΅Π½ΠΈΠΉ ΡΡΠ΅Π΄ΠΈ Π·Π΄ΠΎΡΠΎΠ²ΡΡ
Π΄ΠΎΠ±ΡΠΎΠ²ΠΎΠ»ΡΡΠ΅Π². ΠΠ°ΡΠ΅ΡΠΈΠ°Π»Ρ ΠΈ ΠΌΠ΅ΡΠΎΠ΄Ρ. Π ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΈ ΠΏΡΠΈΠ½ΡΠ»ΠΈ ΡΡΠ°ΡΡΠΈΠ΅ 34 Π·Π΄ΠΎΡΠΎΠ²ΡΡ
Π΄ΠΎΠ±ΡΠΎΠ²ΠΎΠ»ΡΡΠ° (ΡΡΠ΅Π΄Π½ΠΈΠΉ Π²ΠΎΠ·ΡΠ°ΡΡ 31,0 Β± 8,6 Π³ΠΎΠ΄Π°). ΠΠΠ‘ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ Π½Π° ΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎΠΌ ΡΡΠΈΠΌΡΠ»ΡΡΠΎΡΠ΅ ΡΠΈΡΠΌΡ Magstim 200 (ΠΠ΅Π»ΠΈΠΊΠΎΠ±ΡΠΈΡΠ°Π½ΠΈΡ). Π Ρ
ΠΎΠ΄Π΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΠΎΡΠ΅Π½ΠΈΠ²Π°Π»ΠΈ ΡΡΠ±ΡΠ΅ΠΊΡΠΈΠ²Π½ΡΠΉ ΠΏΠΎΡΠΎΠ³, ΠΏΠΎΡΠΎΠ³ ΡΠΎΠΊΡΠ°ΡΠ΅Π½ΠΈΡ ΠΌΡΡΡΡ ΠΈ ΠΏΠΎΡΠΎΠ³ Π°ΠΊΡΠΈΠ²Π°ΡΠΈΠΈ ΠΊΠΎΡΠ΅ΡΠΊΠ° (ΠΏΠΎ Π΄Π°Π½Π½ΡΠΌ Π²ΡΠ·Π²Π°Π½Π½ΠΎΠ³ΠΎ ΠΌΠΎΡΠΎΡΠ½ΠΎΠ³ΠΎ ΠΎΡΠ²Π΅ΡΠ°). ΠΠ»Π΅ΠΊΡΡΠΎΡΠΈΠ·ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΡΡ ΡΠ΅Π³ΠΈΡΡΡΠ°ΡΠΈΡ Π²ΡΠ·Π²Π°Π½Π½ΠΎΠ³ΠΎ ΠΌΠΎΡΠΎΡΠ½ΠΎΠ³ΠΎ ΠΎΡΠ²Π΅ΡΠ° ΠΎΡΡΡΠ΅ΡΡΠ²Π»ΡΠ»ΠΈ Π½Π° ΠΊΠΎΠΌΠΏΡΡΡΠ΅ΡΠ½ΠΎΠΌ ΡΠ»Π΅ΠΊΡΡΠΎΠΌΠΈΠΎΠ³ΡΠ°ΡΠ΅ (ΠΠ΅ΠΉΡΠΎΡΠΎΡΡ, Π ΠΎΡΡΠΈΡ), ΡΠΈΠ½Ρ
ΡΠΎΠ½ΠΈΠ·ΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΌ Ρ ΠΌΠ°Π³Π½ΠΈΡΠ½ΡΠΌ ΡΡΠΈΠΌΡΠ»ΡΡΠΎΡΠΎΠΌ. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ. ΠΡΠ»ΠΈ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½Ρ ΡΡΠ°ΡΠΈΡΡΠΈΡΠ΅ΡΠΊΠΈ Π΄ΠΎΡΡΠΎΠ²Π΅ΡΠ½ΡΠ΅ ΡΠ°Π·Π»ΠΈΡΠΈΡ (Ρ <0,05) ΠΌΠ΅ΠΆΠ΄Ρ ΠΏΠΎΡΠΎΠ³ΠΎΠ²ΡΠΌΠΈ Π·Π½Π°ΡΠ΅Π½ΠΈΡΠΌΠΈ Π°ΠΊΡΠΈΠ²Π°ΡΠΈΠΈ ΠΊΠΎ-ΡΠ΅ΡΠΊΠΎΠ²ΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΡ ΠΈ ΡΠ΅ΡΠΌΠΈΠ½Π°Π»ΡΠ½ΡΡ
Π²Π½ΡΡΡΠΈΠΌΡΡΠ΅ΡΠ½ΡΡ
Π²Π΅ΡΠ²Π΅ΠΉ. ΠΠ΅ΠΆΠ΄Ρ ΠΏΠΎΡΠΎΠ³ΠΎΠ²ΡΠΌΠΈ Π·Π½Π°ΡΠ΅Π½ΠΈΡΠΌΠΈ Π²ΡΠ΅Ρ
ΠΈΡΡΠ»Π΅Π΄ΡΠ΅ΠΌΡΡ
ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² Π²Π½ΡΡΡΠΈ Π³ΡΡΠΏΠΏΡ Π΄ΠΎΡΡΠΎΠ²Π΅ΡΠ½ΡΡ
Π³Π΅Π½Π΄Π΅ΡΠ½ΡΡ
ΡΠ°Π·Π»ΠΈΡΠΈΠΉ Π½Π΅ Π·Π°ΡΠ΅Π³ΠΈΡΡΡΠΈΡΠΎΠ²Π°Π½ΠΎ (Ρ >0,05). Π’Π°ΠΊΠΆΠ΅ Π½Π΅ Π²ΡΡΠ²Π»Π΅Π½ΠΎ Π΄ΠΎΡΡΠΎΠ²Π΅ΡΠ½ΡΡ
ΡΠ°Π·Π»ΠΈΡΠΈΠΉ ΠΏΡΠΈ ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΈ Π²ΡΠ΅Ρ
ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² ΠΌΠ΅ΠΆΠ΄Ρ ΠΏΡΠ°Π²ΠΎΠΉ ΠΈ Π»Π΅Π²ΠΎΠΉ ΠΊΠΎΠ½Π΅ΡΠ½ΠΎΡΡΡΠΌΠΈ (p >0,05). ΠΠ°ΠΊΠ»ΡΡΠ΅Π½ΠΈΠ΅. ΠΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡΡ ΠΏΡΠ΅Π΄ΠΏΠΎΠ»ΠΎΠΆΠΈΡΡ, ΡΡΠΎ ΠΏΡΠΈ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΠΈ ΠΏΡΠΎΡΠΎΠΊΠΎΠ»Π° ΠΠΠ‘ ΡΠ»Π΅Π΄ΡΠ΅Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°ΡΡ ΠΈΠ½Π΄ΠΈΠ²ΠΈΠ΄ΡΠ°Π»ΡΠ½ΡΠΉ ΠΏΠΎΠ΄Ρ
ΠΎΠ΄ ΠΊ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΠΈ ΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎΠ³ΠΎ ΡΡΠΈΠΌΡΠ»Π° Π΄Π»Ρ ΠΊΠ°ΠΆΠ΄ΠΎΠ³ΠΎ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠ°. ΠΠ°Π½Π½ΡΠ΅ Π½Π°ΡΠ΅Π³ΠΎ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ Π΄Π°ΡΡ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΡ Π»ΡΡΡΠ΅Π³ΠΎ ΠΏΠΎΠ½ΠΈΠΌΠ°Π½ΠΈΡ ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΠ° Π΄Π΅ΠΉΡΡΠ²ΠΈΡ ΠΠΠ‘ ΠΈ ΠΌΠΎΠ³ΡΡ Π±ΡΡΡ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½Ρ Π΄Π»Ρ ΡΠ°Π·ΡΠ°Π±ΠΎΡΠΊΠΈ Π»Π΅ΡΠ΅Π±Π½ΠΎΠ³ΠΎ Π°Π»Π³ΠΎΡΠΈΡΠΌΠ° ΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎΠΉ ΡΡΠΈΠΌΡΠ»ΡΡΠΈΠΈ Π² ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΏΡΠ°ΠΊΡΠΈΠΊΠ΅.Β
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