38 research outputs found
Energy, Hamiltonian, Noether Charge, and Black Holes
It is shown that in general the energy and the Hamiltonian of matter fields on the black hole exterior play different roles. is a generator of the time evolution along the Killing time while enters the first law of black hole thermodynamics. For non-minimally
coupled fields the difference is not zero and is a Noether
charge analogous to that introduced by Wald to define the black hole
entropy. If fields vanish at the spatial boundary, is reduced to an
integral over the horizon. The analysis is carried out and an explicit
expression for is found for general diffeomorphism invariant theories. As
an extension of the results by Wald et al, the first law of black hole
thermodynamics is derived for arbitrary weak matter fields.Comment: 20 pages, latex, no figure
Application of the Large-N_c limit to a Chiral Lagrangian with Resonances
It is shown that the implementation of the Large-- approximation helps
to get insight into the structure of, in principle, any QCD-like theory. As an
example, we will compute the NLO corrections to in the chiral limit
with a Lagrangian with Resonances.Comment: 9 pages, 1 figure. Talk given at the International School of
Subnuclear Physics (Erice 2002). To be published in the Proceeding
Impact of Electrical Current on Single GaAs Nanowire Structure
The impact of electrical current on the structure of single free-standing Be-doped GaAs nanowires grown on a Si 111 substrate is investigated. Single nanowires have been structurally analyzed by X-ray nanodiffraction using synchrotron radiation before and after the application of an electrical current. The conductivity measurements on single nanowires in their as-grown geometry have been realized via W-probes installed inside a dual-beam focused ion beam/scanning electron microscopy chamber. Comparing reciprocal space maps of the 111 Bragg reflection, extracted perpendicular to the nanowire growth axis before and after the conductivity measurement, the structural impact of the electrical current is evidenced, including deformation of the hexagonal nanowire cross section, tilting, and bending with respect to the substrate normal. For electrical current densities below 30βAβmmβ2, the induced changes in the reciprocal space maps are negligible. However, for a current density of 347βAβmmβ2, the diffraction pattern is completely distorted. The mean cross section of the illuminated nanowire volume is reconstructed from the reciprocal space maps before and after the application of electrical current. Interestingly, the elongation of two pairs of opposing side facets accompanied by shrinkage of the third pair of facets is found. The variations in the nanowire diameter, as well as their tilt and bending, are confirmed by scanning electron microscopy. To explain these findings, material melting due to Joule heating during voltage/current application accompanied by anisotropic deformations induced by the W-probe is suggested
QCD Instantons and the Soft Pomeron
We study the role of semi-classical QCD vacuum solutions in high energy
scattering by considering the instanton contribution to hadronic cross
sections. We propose a new type of instanton-induced interactions (``instanton
ladder'') that leads to the rising with energy hadronic cross section of Regge
type (the Pomeron). We argue that this interaction may be responsible for the
structure of the soft Pomeron. The intercept is calculated. It has a
non-analytic dependence on the strong coupling constant, allowing a
non-singular continuation into the non-perturbative region. We derive the
Pomeron trajectory, which appears to be approximately linear in some range of
(negative) momentum transfer t, but exhibits a curvature at small t. Possible
role of instantons in multiparticle production is also discussed.Comment: 20 pages, 8 figures, ReVTe
Instantons in the Saturation Environment
We show that instanton calculations in QCD become theoretically well defined
in the gluon saturation environment which suppresses large size instantons. The
effective cutoff scale is determined by the inverse of the saturation scale. We
concentrate on two most important cases: the small-x tail of a gluon
distribution of a high energy hadron or a large nucleus and the central
rapidity region in a high energy hadronic or heavy ion collision. In the
saturation regime the gluon density in a single large ultrarelativistic nucleus
is high and gluonic fields are given by the classical solutions of the
equations of motion. We show that these strong classical fields do not affect
the density of instantons in the nuclear wave function compared to the
instanton density in the vacuum. A classical solution with non-trivial
topological charge is found for the gluon field of a single nucleus at the
lowest order in the instanton perturbation theory. In the case of
ultrarelativistic heavy ion collisions a strong classical gluonic field is
produced in the central rapidity region. We demonstrate that this field
introduces a suppression factor of exp{-c \rho^4 Q_s^4 / [8 \alpha^2 N_c (Q_s
\tau)^2]} in the instanton size distribution, where Q_s is the saturation scale
of both (identical) nuclei, \tau is the proper time and c = 1 is the gluon
liberation coefficient. This factor suggests that gluonic saturation effects at
the early stages of nuclear collisions regulate the instanton size distribution
in the infrared region and make the instanton density finite by suppressing
large size instantons.Comment: 20 pages, 8 figures, REVTeX, some discussion added including a
possible scenario for unitarization of the soft pomero
ΠΠΌΠΌΡΠ½ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΡΡΡΠ΅ΠΊΡΡ Π°Π΄Π°Π»ΠΈΠΌΡΠΌΠ°Π±Π° ΠΏΡΠΈ ΡΠ΅Π²ΠΌΠ°ΡΠΎΠΈΠ΄Π½ΠΎΠΌ Π°ΡΡΡΠΈΡΠ΅: ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ Π ΠΎΡΡΠΈΠΉΡΠΊΠΎΠ³ΠΎ Π½Π°ΡΠΈΠΎΠ½Π°Π»ΡΠ½ΠΎΠ³ΠΎ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ
A reduction in immunological parameters during therapy for rheumatoid arthritis (RA) can yield new data on the mechanisms of anti-inflammatory action and be of great practical importance since this allows judgment of the depth of impact on the immunological process and therefore may be regarded as one of the components of improvement and remission. Objective: to study the effect of the tumor necrosis factor-a (TNF-Π°) inhibitor adalimumab (ADA) on a number of key immunological parameters in RA. Subjects and methods. The study included 100 patients (11 men and 89 women) diagnosed with RA from 5 research centers. The patients were observed to have high RA activity: at baseline, DAS28 6.22+0.84 scores; C-reactive protein (CRP) 37.1+34.7 mg/l. The mean number of disease-modifying antirheumatic drugs (DMARDs) used by a patient in the history was 2.1. During 24-week treatment, the patients took ADA in a subcutaneous dose of 40 mg every 2 weeks both alone and in combination with DMARDs. The time course of changes in the serum levels of CRP, IGM rheumatoid factor (RF) and in the concentration of anti-cyclic citrullinated peptide 2 (anti-CCP2) antibodies was determined by enzyme immunoassay (EIA) using the Axis-Shield Diagnostics commercial kits (United Kingdom). The levels of TNF-a, interleukin (IL) 6, 12, matrix metalloproteinase 3 (MMP3) were measured in pg/ml by EIA using the Bender MedSystems commercial kits (USA) according to the manufacturer's directions. Results. During ADA therapy, there was a rapid reduction in the level of CRP from 34.3 to 11.317.2 mg/l following 2 weeks (p<0.001), which thereafter remained low (11.9 mg/l), with some fluctuations, until week 24 of the study. There was a significant reduction in blood RF levels from 169.24 to 111.97 at 24 weeks (p<0.001). After 12 weeks of ADA treatment, there was virtually a two-fold decrease in IL-6 content from 8.87 to 4.87 pg/ml and later on to 4.03 pg/ml at week 24 (p>0,05). The mean levels of anti-CCP2 antibodies, IL-12, VEGF, and MMP3 remained unchanged. Conclusion. The time course of changes in immunological parameters during ADA treatment demonstrates the rapid and deep effect of TNF-a inhibitors on the different components of the pathogenesis of RA.Π‘Π½ΠΈΠΆΠ΅Π½ΠΈΠ΅ ΠΈΠΌΠΌΡΠ½ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Π΅ΠΉ Π½Π° ΡΠΎΠ½Π΅ ΡΠ΅ΡΠ°ΠΏΠΈΠΈ ΡΠ΅Π²ΠΌΠ°ΡΠΎΠΈΠ΄Π½ΠΎΠ³ΠΎ Π°ΡΡΡΠΈΡΠ° (Π Π) ΠΏΠΎΠ·Π²ΠΎΠ»ΡΠ΅Ρ ΠΏΠΎΠ»ΡΡΠΈΡΡ Π½ΠΎΠ²ΡΠ΅ Π΄Π°Π½Π½ΡΠ΅ ΠΎ ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΠ°Ρ
ΠΏΡΠΎΡΠΈΠ²ΠΎΠ²ΠΎΡΠΏΠ°Π»ΠΈΡΠ΅Π»ΡΠ½ΠΎΠ³ΠΎ Π΄Π΅ΠΉΡΡΠ²ΠΈΡ ΠΈ ΠΈΠΌΠ΅Π΅Ρ Π²Π°ΠΆΠ½ΠΎΠ΅ ΠΏΡΠ°ΠΊΡΠΈΡΠ΅ΡΠΊΠΎΠ΅ Π·Π½Π°ΡΠ΅Π½ΠΈΠ΅, ΠΏΠΎΡΠΊΠΎΠ»ΡΠΊΡ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΠ΅Ρ ΡΡΠ΄ΠΈΡΡ ΠΎ Π³Π»ΡΠ±ΠΈΠ½Π΅ Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΡ Π½Π° ΠΈΠΌΠΌΡΠ½ΠΎΠΏΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠΉ ΠΏΡΠΎΡΠ΅ΡΡ ΠΈ ΠΏΠΎΡΡΠΎΠΌΡ ΠΌΠΎΠΆΠ΅Ρ ΠΎΡΠ΅Π½ΠΈΠ²Π°ΡΡΡΡ ΠΊΠ°ΠΊ ΠΎΠ΄ΠΈΠ½ ΠΈΠ· ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½ΡΠΎΠ² ΡΠ»ΡΡΡΠ΅Π½ΠΈΡ ΠΈ ΡΠ΅ΠΌΠΈΡΡΠΈΠΈ. Π¦Π΅Π»Ρ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ β ΠΈΠ·ΡΡΠ΅Π½ΠΈΠ΅ Π²Π»ΠΈΡΠ½ΠΈΡ ΠΈΠ½Π³ΠΈΠ±ΠΈΡΠΎΡΠ° ΡΠ°ΠΊΡΠΎΡΠ° Π½Π΅ΠΊΡΠΎΠ·Π° ΠΎΠΏΡΡ
ΠΎΠ»ΠΈ Ξ± (Π€ΠΠΞ±) Π°Π΄Π°Π»ΠΈΠΌΡΠΌΠ°Π±Π° (ΠΠΠ) Π½Π° ΡΡΠ΄ ΠΊΠ»ΡΡΠ΅Π²ΡΡ
ΠΈΠΌΠΌΡΠ½ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Π΅ΠΉ ΠΏΡΠΈ Π Π. ΠΠ°ΡΠ΅ΡΠΈΠ°Π» ΠΈ ΠΌΠ΅ΡΠΎΠ΄Ρ. Π ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ Π²ΠΊΠ»ΡΡΠ΅Π½ΠΎ 100 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² ΠΈΠ· 5 ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°ΡΠ΅Π»ΡΡΠΊΠΈΡ
ΡΠ΅Π½ΡΡΠΎΠ² Ρ Π΄ΠΈΠ°Π³Π½ΠΎΠ·ΠΎΠΌ Π Π (11 ΠΌΡΠΆΡΠΈΠ½ ΠΈ 89 ΠΆΠ΅Π½ΡΠΈΠ½). Π£ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Π½Π°Π±Π»ΡΠ΄Π°Π»Π°ΡΡ Π²ΡΡΠΎΠΊΠ°Ρ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ Π Π: ΠΈΡΡ
ΠΎΠ΄Π½ΠΎ ΠΈΠ½Π΄Π΅ΠΊΡ DAS28 β 6,22Β±0,84 Π±Π°Π»Π»Π°, ΡΡΠΎΠ²Π΅Π½Ρ Π‘-ΡΠ΅Π°ΠΊΡΠΈΠ²Π½ΠΎΠ³ΠΎ Π±Π΅Π»ΠΊΠ° (Π‘Π Π) β 37,1+34,7ΠΌΠ³/Π». Π‘ΡΠ΅Π΄Π½Π΅Π΅ ΡΠΈΡΠ»ΠΎ Π±Π°Π·ΠΈΡΠ½ΡΡ
ΠΏΡΠΎΡΠΈΠ²ΠΎΠ²ΠΎΡΠΏΠ°Π»ΠΈΡΠ΅Π»ΡΠ½ΡΡ
ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΠΎΠ² (ΠΠΠΠ) Π² Π°Π½Π°ΠΌΠ½Π΅Π·Π΅, ΠΏΡΠΈΠΌΠ΅Π½ΡΠ²ΡΠΈΡ
ΡΡ ΠΎΠ΄Π½ΠΈΠΌ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠΌ, ΡΠΎΡΡΠ°Π²ΠΈΠ»ΠΎ 2,1. ΠΠ° Π²ΡΠ΅ΠΌΡ Π»Π΅ΡΠ΅Π½ΠΈΡ (24 Π½Π΅Π΄) ΠΏΠ°ΡΠΈΠ΅Π½ΡΡ ΠΏΠΎΠ»ΡΡΠ°Π»ΠΈ ΠΠΠ Π² Π΄ΠΎΠ·Π΅ 40 ΠΌΠ³ ΠΊΠ°ΠΆΠ΄ΡΠ΅ 2 Π½Π΅Π΄ ΠΏΠΎΠ΄ΠΊΠΎΠΆΠ½ΠΎ ΠΊΠ°ΠΊ Π² ΠΊΠΎΠΌΠ±ΠΈΠ½Π°ΡΠΈΠΈ Ρ ΠΠΠΠ, ΡΠ°ΠΊ ΠΈ Π² ΠΌΠΎΠ½ΠΎΡΠ΅ΡΠ°ΠΏΠΈΠΈ. ΠΠΏΡΠ΅Π΄Π΅Π»ΡΠ»ΠΈ Π² Π΄ΠΈΠ½Π°ΠΌΠΈΠΊΠ΅ ΡΡΠ²ΠΎΡΠΎΡΠΎΡΠ½ΡΠ΅ ΡΡΠΎΠ²Π½ΠΈ Π‘Π Π, IgM ΡΠ΅Π²ΠΌΠ°ΡΠΎΠΈΠ΄Π½ΠΎΠ³ΠΎ ΡΠ°ΠΊΡΠΎΡΠ° (Π Π€), ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΡ Π°Π½ΡΠΈΡΠ΅Π» ΠΊ ΡΠΈΠΊΠ»ΠΈΡΠ΅ΡΠΊΠΎΠΌΡ ΡΠΈΡΡΡΠ»Π»ΠΈΠ½ΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΌΡ ΠΏΠ΅ΠΏΡΠΈΠ΄Ρ 2 (ΠΠ¦Π¦Π2) ΠΈΠ·ΡΡΠ°Π»ΠΈ ΠΈΠΌΠΌΡΠ½ΠΎΡΠ΅ΡΠΌΠ΅Π½ΡΠ½ΡΠΌ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ (ΠΠ€Π) Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΠΊΠΎΠΌΠΌΠ΅ΡΡΠ΅ΡΠΊΠΈΡ
Π½Π°Π±ΠΎΡΠΎΠ² Axis-Shield Diagnostics (ΠΠ΅Π»ΠΈΠΊΠΎΠ±ΡΠΈΡΠ°Π½ΠΈΡ). Π‘ΠΎΠ΄Π΅ΡΠΆΠ°Π½ΠΈΠ΅ Π€ΠΠΠ°, ΠΈΠ½ΡΠ΅ΡΠ»Π΅ΠΉΠΊΠΈΠ½Π° (ΠΠ) 6, 12, ΠΌΠ°ΡΡΠΈΠΊΡΠ½ΠΎΠΉ ΠΌΠ΅ΡΠ°Π»Π»ΠΎΠΏΡΠΎΡΠ΅ΠΈΠ½Π°Π·Ρ 3 (ΠΠΠ 3) ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ»ΠΈ ΠΠ€Π (Π² ΠΏΠ³/ΠΌΠ») Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΊΠΎΠΌΠΌΠ΅ΡΡΠ΅ΡΠΊΠΈΡ
Π½Π°Π±ΠΎΡΠΎΠ² Bender MedSystems (Π‘Π¨Π) ΡΠΎΠ³Π»Π°ΡΠ½ΠΎ ΠΈΠ½ΡΡΡΡΠΊΡΠΈΡΠΌ ΡΠΈΡΠΌΡ-ΠΈΠ·Π³ΠΎΡΠΎΠ²ΠΈΡΠ΅Π»Ρ. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ. ΠΠ° ΡΠΎΠ½Π΅ ΡΠ΅ΡΠ°ΠΏΠΈΠΈ ΠΠΠ Π½Π°Π±Π»ΡΠ΄Π°Π»ΠΎΡΡ Π±ΡΡΡΡΠΎΠ΅ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΠ΅ ΡΡΠΎΠ²Π½Ρ Π‘Π Π Ρ 34,3 Π΄ΠΎ 11,3+17,2 ΠΌΠ³/Π» ΡΠ΅ΡΠ΅Π· 2 Π½Π΅Π΄ (p<0,001), ΠΊΠΎΡΠΎΡΡΠΉ Π² Π΄Π°Π»ΡΠ½Π΅ΠΉΡΠ΅ΠΌ Ρ Π½Π΅ΠΊΠΎΡΠΎΡΡΠΌΠΈ ΠΊΠΎΠ»Π΅Π±Π°Π½ΠΈΡΠΌΠΈ ΠΎΡΡΠ°Π²Π°Π»ΡΡ Π½ΠΈΠ·ΠΊΠΈΠΌ (11,9 ΠΌΠ³/Π») Π΄ΠΎ 24-ΠΉ Π½Π΅Π΄Π΅Π»ΠΈ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ. ΠΠ°Π±Π»ΡΠ΄Π°Π»ΠΎΡΡ Π΄ΠΎΡΡΠΎΠ²Π΅ΡΠ½ΠΎΠ΅ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΠ΅ ΡΡΠΎΠ²Π½Ρ Π Π€ Π² ΠΊΡΠΎΠ²ΠΈ Ρ 169,24 Π΄ΠΎ 111,97Π½Π° 24-ΠΉ Π½Π΅Π΄Π΅Π»Π΅ (p<0,001). Π§Π΅ΡΠ΅Π· 12 Π½Π΅Π΄ ΠΏΠΎΡΠ»Π΅ Π½Π°ΡΠ°Π»Π° Π»Π΅ΡΠ΅Π½ΠΈΡ ΠΠΠ ΠΎΡΠΌΠ΅ΡΠ°Π»ΠΎΡΡ ΠΏΡΠ°ΠΊΡΠΈΡΠ΅ΡΠΊΠΈ 2-ΠΊΡΠ°ΡΠ½ΠΎΠ΅ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΠ΅ ΡΠΎΠ΄Π΅ΡΠΆΠ°Π½ΠΈΡ ΠΠ6 Ρ 8,87 Π΄ΠΎ 4,87 ΠΏΠ³/ΠΌΠ» ΠΈ Π² Π΄Π°Π»ΡΠ½Π΅ΠΉΡΠ΅ΠΌ, ΠΊ 24-ΠΉ Π½Π΅Π΄Π΅Π»Π΅, β Π΄ΠΎ 4,03 ΠΏΠ³/ΠΌΠ» (p>0,05). Π‘ΡΠ΅Π΄Π½ΠΈΠ΅ ΡΡΠΎΠ²Π½ΠΈ ΠΠ¦Π¦Π, ΠΠ12, ΡΠ°ΠΊΡΠΎΡΠ° ΡΠΎΡΡΠ° ΡΠ½Π΄ΠΎΡΠ΅Π»ΠΈΡ ΡΠΎΡΡΠ΄ΠΎΠ² (VEGF), ΠΠΠ3 Π½Π΅ ΠΈΠ·ΠΌΠ΅Π½ΠΈΠ»ΠΈΡΡ. ΠΡΠ²ΠΎΠ΄Ρ. ΠΠΈΠ½Π°ΠΌΠΈΠΊΠ° ΠΈΠΌΠΌΡΠ½ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² ΠΏΡΠΈ Π»Π΅ΡΠ΅Π½ΠΈΠΈ ΠΠΠ Π΄Π΅ΠΌΠΎΠ½ΡΡΡΠΈΡΡΠ΅Ρ Π±ΡΡΡΡΠΎΠ΅ ΠΈ Π³Π»ΡΠ±ΠΎΠΊΠΎΠ΅ Π΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ ΠΈΠ½Π³ΠΈΠ±ΠΈΡΠΎΡΠΎΠ² Π€ΠΠΠ° Π½Π° ΡΠ°Π·Π»ΠΈΡΠ½ΡΠ΅ Π·Π²Π΅Π½ΡΡ ΠΏΠ°ΡΠΎΠ³Π΅Π½Π΅Π·Π° Π Π
Pressure Treatment of Polytene Chromosomes and Computer Vision Techniques for High Resolution Cytogenetic Studies
48 p.Thesis (Ph.D.)--University of Illinois at Urbana-Champaign, 2008.The exceptional cytology provided by the interphase chromatin organization in polytene chromosomes has made Drosophila the premier model organism for analysis of chromosome structure and behavior. A major impediment to full exploitation of polytene chromosome cytology has been the difficulty in producing high quality chromosome spreads. This is particularly true for applications requiring prior formaldehyde fixation. Individual chromosome bands are seldom resolved in typical preparations, with many appearing fused. Here we describe a new procedure for preparing polytene chromosome spreads which exploits high pressure, together with other modifications, to produce high quality chromosome spreads whose light microscopy images reproducibly show comparable detail to electron microscopy images of conventionally prepared spreads. We illustrate results obtained with this procedure from typical cytological applications, including immunofluorescence and fluorescence in situ hybridization (FISH). Description of optimized downstream staining procedures for light and electron microscopy is included. Development of computer vision applications for automated recognition and structural analysis of polytene chromosomes are discussed. Prospective and collaborative studies are described.U of I OnlyRestricted to the U of I community idenfinitely during batch ingest of legacy ETD
Theta and alpha band modulations reflect error-related adjustments in the auditory condensation task
Error commission leads to adaptive adjustments in a number of brain networks that subserve goal-directed behavior, resulting in either enhanced stimulus processing or increased motor threshold depending on the nature of errors committed. Here, we studied these adjustments by analyzing post-error modulations of alpha and theta band activity in the auditory version of the two-choice condensation task, which is highly demanding for sustained attention while involves no inhibition of prepotent responses. Errors were followed by increased frontal midline theta (FMT) activity, as well as by enhanced alpha band suppression in the parietal and the left central regions; parietal alpha suppression correlated with the task performance, left central alpha suppression correlated with the post-error slowing, and FMT increase correlated with both behavioral measures. On post-error correct trials, left-central alpha band suppression started earlier before the response, and the response was followed by weaker FMT activity, as well as by enhanced alpha band suppression distributed over the entire scalp. These findings indicate that several separate neuronal networks are involved in post-error adjustments, including the midfrontal performance monitoring network, the parietal attentional network, and the sensorimotor network. Supposedly, activity within these networks is rapidly modulated after errors, resulting in optimization of their functional state on the subsequent trials, with corresponding changes in behavioral measures