6,381 research outputs found
Performance of the ATLAS Detector on First Single Beam and Cosmic Ray Data
We report on performance studies of the ATLAS detector obtained with first
single LHC (Large Hadron Collider) beam data in September 2008, and large
samples of cosmic ray events collected in the fall of 2008. In particular, the
performance of the calorimeter, crucial for jet and missing transverse energy
measurements, is studied. It is shown that the ATLAS experiment is ready to
record the first LHC collisions.Comment: 4 pages, 6 figures, proceedings contribution of the SUSY 2009
conference in Bosto
Global Cardinality Constraints Make Approximating Some Max-2-CSPs Harder
Assuming the Unique Games Conjecture, we show that existing approximation algorithms for some Boolean Max-2-CSPs with cardinality constraints are optimal. In particular, we prove that Max-Cut with cardinality constraints is UG-hard to approximate within ~~0.858, and that Max-2-Sat with cardinality constraints is UG-hard to approximate within ~~0.929. In both cases, the previous best hardness results were the same as the hardness of the corresponding unconstrained Max-2-CSP (~~0.878 for Max-Cut, and ~~0.940 for Max-2-Sat).
The hardness for Max-2-Sat applies to monotone Max-2-Sat instances, meaning that we also obtain tight inapproximability for the Max-k-Vertex-Cover problem
Competing SDW Phases and Quantum Oscillations in (TMTSF)2ClO4 in Magnetic Field
We propose a new approach for studying spin density waves (SDW) in the
Bechgaard salt (TMTSF)2ClO4 where lattice is dimerized in transverse direction
due to anion ordering. The SDW response is calculated in the matrix formulation
that rigorously treats the hybridization of inter-band and intra-band SDW
correlations. Since the dimerization gap is large, of the order of transverse
bandwidth, we also develop an exact treatment of magnetic breakdown in the
external magnetic field. The obtained results agree with the experimental data
on the fast magneto-resistance oscillations. Experimentally found 260T rapid
oscillations and the characteristic Tc dependance on magnetic field of relaxed
material are fitted with our results for anion potential of the order of
interchain hopping
Peierls-type structural phase transition in a crystal induced by magnetic breakdown
We predict a new type of phase transition in a quasi-two dimensional system
of electrons at high magnetic fields, namely the stabilization of a density
wave which transforms a two dimensional open Fermi surface into a periodic
chain of large pockets with small distances between them. The quantum tunneling
of electrons between the neighboring closed orbits enveloping these pockets
transforms the electron spectrum into a set of extremely narrow energy bands
and gaps which decreases the total electron energy, thus leading to a magnetic
breakdown induced density wave (MBIDW) ground state. We show that this DW
instability has some qualitatively different properties in comparison to
analogous DW instabilities of Peierls type. E. g. the critical temperature of
the MBIDW phase transition arises and disappears in a peculiar way with a
change of the inverse magnetic field
Effects of transverse electron dispersion on photo-emission spectra of quasi-one-dimensional systems
The random phase approximation (RPA) spectral function of the one-dimensional
electron band with the three-dimensional long range Coulomb interaction shows a
broad feature which is spread on the scale of the plasmon energy and vanishes
at the chemical potential. The fact that there are no quasi-particle
-peaks is the direct consequence of the acoustic nature of the
collective plasmon mode. This behaviour of the spectral function is in the
qualitative agreement with the angle resolved photo-emission spectra of some
Bechgaard salts. In the present work we consider the modifications in the
spectral function due to finite transverse electron dispersion. The transverse
bandwidth is responsible for the appearance of an optical gap in the long
wavelength plasmon mode. The plasmon dispersion of such kind introduces the
quasi-particle -peak into the spectral function at the chemical
potential. The cross-over from the Fermi liquid to the non-Fermi liquid regime
by decreasing the transverse bandwidth takes place through the decrease of the
quasi-particle weight as the optical gap in the long wavelength plasmon mode is
closing.Comment: 2 pages, 2 figures, ISCOM'0
The Role of Hydrophilic Sandblasted Titanium and Laser Microgrooved Zirconia Surfaces in Dental Implant Treatment
Dental implant surface modifications affect surface roughness, chemistry, topography, and consequently influence biological bone response. Current surface treatments are directed toward increased hydrophilicity and wettability of dental surfaces that allow earlier implant loading due to accelerated osseointegration. This is clinically reflected in increased implant stability and mainteined crestal bone level. Further modification includes microgrooving of zirconia implants by femtosecond laser ablation. Favorable initial results encourage further clinical assessment of this microgrooved zirconia implants
ΠΠΈΠΊΡΠΎΡΡΡΡΠΊΡΡΡΠ½Π° Π°Π΄Π°ΠΏΡΠ°ΡΠΈΡΠ° ΠΊΠΎΡΡΠ°Π½ΠΎΠ³ ΡΠΊΠΈΠ²Π° ΡΠ°ΡΠΈΡΠ°Π»Π½ΠΎΠ³ ΡΠΊΠ΅Π»Π΅ΡΠ° Π½Π° Π΄ΠΈΡΡΡΠΈΠ±ΡΡΠΈΡΡ ΠΎΠΊΠ»ΡΠ·Π°Π»Π½ΠΎΠ³ ΠΎΠΏΡΠ΅ΡΠ΅ΡΠ΅ΡΠ° ΠΊΠΎΠ΄ ΠΎΡΠΎΠ±Π° ΡΠ° ΠΏΡΠ½ΠΈΠΌ Π·ΡΠ±Π½ΠΈΠΌ Π½ΠΈΠ·ΠΎΠΌ ΠΈ ΡΠ΅Π½Π° ΡΠ»ΠΎΠ³Π° Ρ Π½Π°ΡΡΠ°Π½ΠΊΡ ΠΏΡΠ΅Π»ΠΎΠΌΠ° ΡΠ°ΡΠΈΡΠ°Π»Π½ΠΎΠ³ ΡΠΊΠ΅Π»Π΅ΡΠ°
Occlusal forces have traditionally been explained to transfer through the facial
skeleton along specific osseous trajectories known as buttresses. These regions were
assumed as zones of strength due to their thick cortical bone structure, while the areas
between the buttresses containing thin cortical bone were considered weak and fragile.
However, recent studies revealed that both cortical and trabecular bone of the mid-facial
skeleton of dentulous individuals exhibit remarkable regional variations in structure and
elastic properties. These variations have been frequently suggested to result from the
different involvement of cortical and trabecular bone in the transfer of occlusal forces,
although there has been no study to link bone microarchitecture to the occlusal loading.
Moreover, although the classical concept of buttresses has been extensively studied by
mechanical methods, such as finite element (FE) analysis, there is still no direct
evidence for occlusal load distribution through the cortical and trabecular bone
compartments individually. Additionally, relatively less scientific attention has been
paid to the investigation of bone structure along Le Fort fracture lines that have
traditionally been assumed as weak areas at which the mid-facial skeleton commonly
fractures after injury. Papers published so far in this field focused mainly on the
epidemiology and the role of injury mechanism in the fracture development, without
considering the structural basis of increased bone fragility along the Le Fort fracture
lines...ΠΡΠ΅ΠΌΠ° ΡΡΠ°Π΄ΠΈΡΠΈΠΎΠ½Π°Π»Π½ΠΎΠΌ ΠΎΠ±ΡΠ°ΡΡeΡΡ, ΠΏΡΠ΅Π½ΠΎΡ ΠΎΠΊΠ»ΡΠ·Π°Π»Π½ΠΎΠ³ ΠΎΠΏΡΠ΅ΡΠ΅ΡΠ΅ΡΠ° ΠΊΡΠΎΠ·
ΠΊΠΎΡΡΠΈ Π»ΠΈΡΠ° ΡΠΎΠΊΠΎΠΌ ΠΆΠ²Π°ΠΊΠ°ΡΠ° ΠΎΠ±Π°Π²ΡΠ° ΡΠ΅ Π΄ΡΠΆ ΡΠΏΠ΅ΡΠΈΡΠΈΡΠ½ΠΈΡ
ΠΏΡΡΠ°ΡΠ° ΡΠ½ΡΡΠ°Ρ ΠΊΠΎΡΡΠΈ
Π·Π²Π°Π½ΠΈΡ
ΡΡΠ°ΡΠ΅ΠΊΡΠΎΡΠΈΡΠ΅ ΠΈΠ»ΠΈ βΠ±Π°ΡΡΠ΅ΡΠΈβ. ΠΠ²ΠΈ Π΄Π΅Π»ΠΎΠ²ΠΈ ΠΊΠΎΡΡΠΈΡΡ Π»ΠΈΡΠ° ΡΠΌΠ°ΡΡΠ°Π½ΠΈ ΡΡ ΡΠ°ΠΊΠΈΠΌ
Π·ΠΎΠ½Π°ΠΌΠ° ΡΠ΅Ρ ΠΈΡ
ΠΈΠ·Π³ΡΠ°ΡΡΡΠ΅ ΠΊΠΎΡΡΠΈΠΊΠ°Π»Π½Π° ΠΊΠΎΡΡ Π²Π΅Π»ΠΈΠΊΠ΅ Π΄Π΅Π±ΡΠΈΠ½Π΅, Π΄ΠΎΠΊ ΡΡ Π΄Π΅Π»ΠΎΠ²ΠΈ ΠΊΠΎΡΡΠΈ
ΡΠΌΠ΅ΡΡΠ΅Π½ΠΈ ΠΈΠ·ΠΌΠ΅ΡΡ ΡΡΠ°ΡΠ΅ΠΊΡΠΎΡΠΈΡΠ° ΡΠΌΠ°ΡΡΠ°Π½ΠΈ ΡΠ»Π°Π±ΠΈΠΌ ΠΈ ΡΡΠ°Π³ΠΈΠ»Π½ΠΈΠΌ Π·Π±ΠΎΠ³ ΡΠΈΡ
ΠΎΠ²Π΅ ΡΠ°Π½ΠΊΠ΅
ΠΊΠΎΡΡΠΈΠΊΠ°Π»Π½Π΅ Π³ΡΠ°ΡΠ΅. ΠΠ΅ΡΡΡΠΈΠΌ, Π½Π΅Π΄Π°Π²Π½ΠΈΠΌ ΠΈΡΡΡΠ°ΠΆΠΈΠ²Π°ΡΠΈΠΌΠ° ΡΠ΅ ΠΎΡΠΊΡΠΈΠ²Π΅Π½ΠΎ Π΄Π° ΠΈ
ΠΊΠΎΡΡΠΈΠΊΠ°Π»Π½Π° ΠΈ ΡΡΠ°Π±Π΅ΠΊΡΠ»Π°ΡΠ½Π° ΠΊΠΎΡΡ ΡΡΠ΅Π΄ΡΠ΅Π³ ΠΌΠ°ΡΠΈΠ²Π° Π»ΠΈΡΠ° ΠΊΠΎΠ΄ ΠΎΡΠΎΠ±Π° ΡΠ° ΠΏΡΠ½ΠΈΠΌ Π·ΡΠ±Π½ΠΈΠΌ
Π½ΠΈΠ·ΠΎΠΌ ΠΏΠΎΠΊΠ°Π·ΡΡΡ Π·Π½Π°ΡΠ°ΡΠ½Π΅ ΡΠ΅Π³ΠΈΠΎΠ½Π°Π»Π½Π΅ Π²Π°ΡΠΈΡΠ°ΡΠΈΡΠ΅ Ρ Π³ΡΠ°ΡΠΈ ΠΈ Π΅Π»Π°ΡΡΠΈΡΠ½ΠΈΠΌ ΡΠ²ΠΎΡΡΡΠ²ΠΈΠΌΠ°.
ΠΠ²Π΅ ΡΠ΅ Π²Π°ΡΠΈΡΠ°ΡΠΈΡΠ΅ ΡΠ΅ΡΡΠΎ ΡΠΌΠ°ΡΡΠ°ΡΡ Π°Π΄Π°ΠΏΡΠ°ΡΠΈΡΠΎΠΌ ΠΊΠΎΡΡΠΈΠΊΠ°Π»Π½Π΅ ΠΈ ΡΡΠ°Π±Π΅ΠΊΡΠ»Π°ΡΠ½Π΅ ΠΊΠΎΡΡΠΈ Π½Π°
ΡΠ°Π·Π»ΠΈΡΠΈΡΠΎ ΠΎΠΏΡΠ΅ΡΠ΅ΡΠ΅ΡΠ΅ Ρ ΠΏΡΠ΅Π½ΠΎΡΡ ΠΎΠΊΠ»ΡΠ·Π°Π»Π½ΠΈΡ
ΡΠΈΠ»Π° ΡΠΎΠΊΠΎΠΌ ΠΆΠ²Π°ΠΊΠ°ΡΠ°, ΠΈΠ°ΠΊΠΎ
ΠΏΠΎΠ²Π΅Π·Π°Π½ΠΎΡΡ ΠΌΠΈΠΊΡΠΎΠ°ΡΡ
ΠΈΡΠ΅ΠΊΡΡΡΠ΅ ΠΊΠΎΡΡΠΈ ΠΈ ΠΎΠΊΠ»ΡΠ·Π°Π»Π½ΠΎΠ³ ΠΎΠΏΡΠ΅ΡΠ΅ΡΠ΅ΡΠ° Π΄ΠΎ ΡΠ°Π΄Π° Π½ΠΈΡΠ΅
ΠΈΡΠΏΠΈΡΠΈΠ²Π°Π½Π° ΠΊΠΎΠ΄ ΡΡΠ΄ΠΈ. Π¨ΡΠ°Π²ΠΈΡΠ΅, ΠΈΠ°ΠΊΠΎ ΡΠ΅ ΠΊΠ»Π°ΡΠΈΡΠ½ΠΈ ΠΊΠΎΠ½ΡΠ΅ΠΏΡ ΠΏΡΠ΅Π½ΠΎΡΠ° ΠΎΠΊΠ»ΡΠ·Π°Π»Π½ΠΎΠ³
ΠΎΠΏΡΠ΅ΡΠ΅ΡΠ΅ΡΠ° Π΄ΡΠΆ ΡΡΠ°ΡΠ΅ΠΊΡΠΎΡΠΈΡΠ° ΠΈΠ½ΡΠ΅Π½Π·ΠΈΠ²Π½ΠΎ ΠΏΡΠΎΡΡΠ°Π²Π°Π½ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠΊΠΈΠΌ ΠΌΠ΅ΡΠΎΠ΄Π°ΠΌΠ°, ΠΊΠ°ΠΎ
ΡΡΠΎ ΡΠ΅ ΠΌΠ΅ΡΠΎΠ΄ ΠΊΠΎΠ½Π°ΡΠ½ΠΈΡ
Π΅Π»Π΅ΠΌΠ΅Π½Π°ΡΠ°, ΡΠΎΡ ΡΠ²Π΅ΠΊ Π½ΠΈΡΠ΅ ΠΈΡΠΏΠΈΡΠ°Π½ΠΎ Π½Π° ΠΊΠΎΡΠΈ Π½Π°ΡΠΈΠ½ ΡΠ΅
ΠΎΠΊΠ»ΡΠ·Π°Π»Π½Π΅ ΡΠΈΠ»Π΅ ΠΏΡΠ΅Π½ΠΎΡΠ΅ ΠΏΠΎΡΠ΅Π΄ΠΈΠ½Π°ΡΠ½ΠΎ ΠΊΡΠΎΠ· ΠΊΠΎΡΡΠΈΠΊΠ°Π»Π½Ρ ΠΈ ΡΡΠ°Π±Π΅ΠΊΡΠ»Π°ΡΠ½Ρ ΠΊΠΎΡΡ.
ΠΠ½Π°ΡΠ°ΡΠ½ΠΎ ΠΌΠ°ΡΡ Π½Π°ΡΡΠ½Ρ ΠΏΠ°ΠΆΡΡ ΡΠ΅ ΠΏΡΠΈΠ²Π»Π°ΡΠΈΠ»ΠΎ ΠΈΡΠΏΠΈΡΠΈΠ²Π°ΡΠ΅ Π³ΡΠ°ΡΠ΅ ΠΊΠΎΡΡΠΈΡΡ Π»ΠΈΡΠ° Π΄ΡΠΆ
Le Fort Π»ΠΈΠ½ΠΈΡΠ° ΠΊΠΎΡΠ΅ ΡΡ ΡΡΠ°Π΄ΠΈΡΠΈΠΎΠ½Π°Π»Π½ΠΎ ΡΠΌΠ°ΡΡΠ°Π½Π΅ Π½Π°ΡΡΠ΅ΡΡΠΈΠΌ ΠΌΠ΅ΡΡΠΈΠΌΠ° ΠΏΡΠ΅Π»ΠΎΠΌΠ°
ΠΊΠΎΡΡΠΈΡΡ ΡΠ°ΡΠΈΡΠ°Π»Π½ΠΎΠ³ ΡΠΊΠ΅Π»Π΅ΡΠ° ΡΠ·ΡΠΎΠΊΠΎΠ²Π°Π½ΠΈΡ
ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠΊΠΈΠΌ ΡΠΈΠ»Π°ΠΌΠ°. ΠΠΎΡΠ°Π΄Π°ΡΡΠ΅ ΡΡΡΠ΄ΠΈΡΠ΅
Ρ ΠΎΠ²ΠΎΡ ΠΎΠ±Π»Π°ΡΡΠΈ ΡΡ Π±ΠΈΠ»Π΅ ΡΠΎΠΊΡΡΠΈΡΠ°Π½Π΅ ΡΠ³Π»Π°Π²Π½ΠΎΠΌ Π½Π° Π΅ΠΏΠΈΠ΄Π΅ΠΌΠΈΠΎΠ»ΠΎΡΠΊΠ° ΠΈΡΡΡΠ°ΠΆΠΈΠ²Π°ΡΠ° ΠΈ
ΡΠ»ΠΎΠ³Ρ ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΠ° ΠΏΠΎΠ²ΡΠ΅Π΄Π΅ Ρ Π½Π°ΡΡΠ°Π½ΠΊΡ ΠΎΠ²ΠΈΡ
ΠΏΡΠ΅Π»ΠΎΠΌΠ°, Π΄ΠΎΠΊ ΡΡΡΡΠΊΡΡΡΠ½Π° ΠΎΡΠ½ΠΎΠ²Π°
ΠΏΠΎΠ²Π΅ΡΠ°Π½Π΅ ΡΡΠ°Π³ΠΈΠ»Π½ΠΎΡΡΠΈ ΠΊΠΎΡΡΠΈ Π΄ΡΠΆ Le Fort Π»ΠΈΠ½ΠΈΡΠ° Π½ΠΈΡΠ΅ ΠΈΡΠΏΠΈΡΠΈΠ²Π°Π½Π°..
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