76 research outputs found
Quite a Character: The Spectrum of Yang-Mills on S^3
We introduce a simple method to extract the representation content of the
spectrum of a system with SU(2) symmetry from its partition function. The
method is easily generalized to systems with SO(2,4) symmetry, such as
conformal field theories in four dimensions. As a specific application we
obtain an explicit generating function for the representation content of free
planar Yang-Mills theory on S^3. The extension to N = 4 super Yang-Mills is
also discussed.Comment: Based on a Brown University undergraduate thesis, 12 page
The monitoring of dirty electricity in A secondary school in kazan, republic of tatarstan, Russia
Electromagnetic fields from electronic equipment are detrimental environmental factors. Recently, a new type of electromagnetic pollution referred to as "dirty electricity" was discovered to affect human health. The current research measures levels of dirty electricity in one secondary school in Kazan, Republic of Tatarstan, Russia. A Microsurge II meter that measures high frequency transients and harmonics between 4 to 100 kHz (expressed as Graham-Stetzer units) was used in this study. Levels of dirty electricity were elevated in all areas of the school and the installation of Graham-Stetzer filters significantly reduced these levels. Taking into account the detrimental effects of the dirty electricity on human health, plugging one Graham-Stetzer filter into each classroom is highly recommended. Β© PSP Volume 18 - No 6. 2009
The Spectrum of Yang Mills on a Sphere
In this note, we determine the representation content of the free, large N,
SU(N) Yang Mills theory on a sphere by decomposing its thermal partition
function into characters of the irreducible representations of the conformal
group SO(4,2). We also discuss the generalization of this procedure to finding
the representation content of N=4 Super Yang Mills.Comment: 18 pages v2. references added. typos fixe
Gauge invariant Lagrangian formulation of massive higher spin fields in (A)dS_3 space
We develop the frame-like formulation of massive bosonic higher spins fields
in the case of 3-dimensional space with the arbitrary cosmological
constant. The formulation is based on gauge-invariant description by involving
the Stueckelberg auxiliary fields. The explicit form of the Lagrangians and the
gauge transformation laws are found. The theory can be written in terms of
gauge-invariant objects similar to the massless theories, thus allowing us to
hope to use the same methods for investigation of interactions. In the massive
spin 3 field example we are able to rewrite the Lagrangian using the new the
so-called separated variables, so that the study of Lagrangian formulation
reduces to finding the Lagrangian containing only half of the fields. The same
construction takes places for arbitrary integer spin field as well. Further
working in terms of separated variables, we build Lagrangian for arbitrary
integer spin and write it in terms of gauge-invariant objects. Also, we
demonstrate how to restore the full set of variables, thus receiving Lagrangian
for the massive fields of arbitrary spin in the terms of initial fields.Comment: 12 page
ΠΡΠ΅Π½ΠΊΠ° ΠΈΠ½Π΄ΠΈΠ²ΠΈΠ΄ΡΠ°Π»ΡΠ½ΠΎ-ΠΏΡΠΈΡ ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ ΡΠ²ΠΎΠΉΡΡΠ² ΡΠ΅Π»ΠΎΠ²Π΅ΠΊΠ° Π² Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡ ΠΊΠΎΠ½ΡΠΈΠ³ΡΡΠ°ΡΠΈΠΎΠ½Π½ΡΡ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠΉ Π΅Π³ΠΎ Π»ΠΈΡΠ°
Introduction. The study examines the relationship between facial configuration and assessing personality traits. Objective determinants of interpersonal perception, such as facial types, a modelβs age and gender, the mode and duration of exposure of facial photographs, etc., are well elaborated in domestic and foreign studies. However, questions remain about how facial structure and also the observer's personality characteristics determine the perception of individual psychological characteristics through facial photographs.
Methods. The study employed the comparative analysis of evaluations of individual psychological characteristics by facial photographs by the scales of the Personal Differential Questionnaire in combination with multidirectional transformations of photographs of neutral faces.
Results. A systematic variation of four configuration variables β location of the mouth and eyes, nose length, and pupillary distance β not only causes weak persistent impressions of joy or sadness, but also changes ideas about individual psychological traits. The induced joy was associated with the positive poles of the scales of the Personal Differential Questionnaire; the induced sadness was associated with the negative poles of its scales. Directional transformations had different impacts on ideas about the components of the implicit structure of personality β evaluation, potency, and activity. Extraversion was more often associated with female faces, while the perceived dominance/subordination β with male faces. The observed patterns modified under the influence of facial morphotypes and the observerβs self-assessment.
Discussion. The research findings confirm an overgeneralization of weak emotional states when perceiving neutral faces and indicate a close association between overgeneralization and the observerβs self-concept.
In conclusion: a multidirectional variation of the configuration variables of emotionally neutral faces selectively affects the perception of personality traits. The observerβs sympathy/antipathy and also his/her individual psychological features play a special role in assessing the personality characteristics through facial expressions.ΠΠ²Π΅Π΄Π΅Π½ΠΈΠ΅. ΠΡΡΠ»Π΅Π΄ΡΠ΅ΡΡΡ ΡΠ²ΡΠ·Ρ ΠΌΠ΅ΠΆΠ΄Ρ ΠΊΠΎΠ½ΡΠΈΠ³ΡΡΠ°ΡΠΈΠ΅ΠΉ Π»ΠΈΡΠ° Π½Π°ΡΡΡΡΠΈΠΊΠ° ΠΈ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½ΠΈΡΠΌΠΈ ΡΡΠΎΡΠΎΠ½Π½Π΅Π³ΠΎ Π½Π°Π±Π»ΡΠ΄Π°ΡΠ΅Π»Ρ ΠΎ ΡΠ΅ΡΡΠ°Ρ
Π΅Π³ΠΎ Π»ΠΈΡΠ½ΠΎΡΡΠΈ. ΠΠ΅ΡΠΌΠΎΡΡΡ Π½Π° ΡΠΎ, ΡΡΠΎ Π² ΡΠ°Π±ΠΎΡΠ°Ρ
ΠΎΡΠ΅ΡΠ΅ΡΡΠ²Π΅Π½Π½ΡΡ
ΠΈ Π·Π°ΡΡΠ±Π΅ΠΆΠ½ΡΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°ΡΠ΅Π»Π΅ΠΉ Π²Π΅ΡΡΠΌΠ° ΠΏΡΠΎΡΠ°Π±ΠΎΡΠ°Π½ Π²ΠΎΠΏΡΠΎΡ ΠΎΠ± ΠΎΠ±ΡΠ΅ΠΊΡΠΈΠ²Π½ΡΡ
Π΄Π΅ΡΠ΅ΡΠΌΠΈΠ½Π°Π½ΡΠ°Ρ
ΠΌΠ΅ΠΆΠ»ΠΈΡΠ½ΠΎΡΡΠ½ΠΎΠΉ ΠΏΠ΅ΡΡΠ΅ΠΏΡΠΈΠΈ, Π½Π°ΠΏΡΠΈΠΌΠ΅Ρ, ΡΠΈΠΏΠ΅ Π»ΠΈΡΠ°, Π²ΠΎΠ·ΡΠ°ΡΡΠ΅ ΠΈ ΠΏΠΎΠ»Π΅ Π½Π°ΡΡΡΡΠΈΠΊΠ°, ΡΠΎΡΠΌΠ΅ ΠΈ Π΄Π»ΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΠΈ ΡΠΊΡΠΏΠΎΠ·ΠΈΡΠΈΠΈ ΡΠΎΡΠΎΠΈΠ·ΠΎΠ±ΡΠ°ΠΆΠ΅Π½ΠΈΡ ΡΠ΅Π»ΠΎΠ²Π΅ΠΊΠ° ΠΈ Ρ. ΠΏ., ΠΎΡΠΊΡΡΡΡΠΌΠΈ ΠΎΡΡΠ°ΡΡΡΡ Π²ΠΎΠΏΡΠΎΡΡ ΠΎ ΡΠΎΠΌ, Π² ΠΊΠ°ΠΊΠΎΠΉ ΡΡΠ΅ΠΏΠ΅Π½ΠΈ Π²ΠΎΡΠΏΡΠΈΡΡΠΈΠ΅ ΠΈΠ½Π΄ΠΈΠ²ΠΈΠ΄ΡΠ°Π»ΡΠ½ΠΎ-ΠΏΡΠΈΡ
ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊ ΠΏΠΎ ΡΠΎΡΠΎΠΈΠ·ΠΎΠ±ΡΠ°ΠΆΠ΅Π½ΠΈΡ Π»ΠΈΡΠ° ΡΠ΅Π»ΠΎΠ²Π΅ΠΊΠ° Π΄Π΅ΡΠ΅ΡΠΌΠΈΠ½ΠΈΡΠΎΠ²Π°Π½ΠΎ Π΅Π³ΠΎ ΡΡΡΡΠΊΡΡΡΠΎΠΉ, Π° ΡΠ°ΠΊΠΆΠ΅ Π»ΠΈΡΠ½ΠΎΡΡΠ½ΡΠΌΠΈ ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΡΠΌΠΈ ΡΠ°ΠΌΠΎΠ³ΠΎ Π²ΠΎΡΠΏΡΠΈΠ½ΠΈΠΌΠ°ΡΡΠ΅Π³ΠΎ.
ΠΠ΅ΡΠΎΠ΄Ρ. Π ΠΎΡΠ½ΠΎΠ²Π΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ Π»Π΅ΠΆΠΈΡ ΠΌΠ΅ΡΠΎΠ΄ ΡΠΎΠΏΠΎΡΡΠ°Π²ΠΈΡΠ΅Π»ΡΠ½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π° ΠΎΡΠ΅Π½ΠΎΠΊ ΠΈΠ½Π΄ΠΈΠ²ΠΈΠ΄ΡΠ°Π»ΡΠ½ΠΎ-ΠΏΡΠΈΡ
ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ²ΠΎΠΉΡΡΠ² Π½Π°ΡΡΡΡΠΈΠΊΠΎΠ², Π²ΡΠΏΠΎΠ»Π½Π΅Π½Π½ΡΡ
ΠΏΠΎ ΡΠΊΠ°Π»Π°ΠΌ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠΈ Β«ΠΠΈΡΠ½ΠΎΡΡΠ½ΡΠΉ Π΄ΠΈΡΡΠ΅ΡΠ΅Π½ΡΠΈΠ°Π»Β», ΠΏΡΠΈ ΡΠ°Π·Π½ΠΎΠ½Π°ΠΏΡΠ°Π²Π»Π΅Π½Π½ΡΡ
ΡΡΠ°Π½ΡΡΠΎΡΠΌΠ°ΡΠΈΡΡ
ΡΠΎΡΠΎΠΈΠ·ΠΎΠ±ΡΠ°ΠΆΠ΅Π½ΠΈΠΉ ΡΠΏΠΎΠΊΠΎΠΉΠ½ΠΎΠ³ΠΎ Π»ΠΈΡΠ°.
Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ ΡΠΈΡΡΠ΅ΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠ΅ Π²Π°ΡΡΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΡΠ΅ΡΡΡΠ΅Ρ
ΠΊΠΎΠ½ΡΠΈΠ³ΡΡΠ°ΡΠΈΠΎΠ½Π½ΡΡ
ΠΏΡΠΈΠ·Π½Π°ΠΊΠΎΠ² β ΡΠ°ΡΠΏΠΎΠ»ΠΎΠΆΠ΅Π½ΠΈΡ Π»ΠΈΠ½ΠΈΠΈ ΡΡΠ° ΠΈ Π³Π»Π°Π·, Π΄Π»ΠΈΠ½Ρ Π½ΠΎΡΠ° ΠΈ ΡΠ°ΡΡΡΠΎΡΠ½ΠΈΡ ΠΌΠ΅ΠΆΠ΄Ρ Π·ΡΠ°ΡΠΊΠ°ΠΌΠΈ Π½Π΅ ΡΠΎΠ»ΡΠΊΠΎ Π²ΡΠ·ΡΠ²Π°Π΅Ρ ΡΠ»Π°Π±ΡΠ΅ ΡΡΡΠΎΠΉΡΠΈΠ²ΡΠ΅ Π²ΠΏΠ΅ΡΠ°ΡΠ»Π΅Π½ΠΈΡ ΡΠ°Π΄ΠΎΡΡΠΈ Π»ΠΈΠ±ΠΎ Π³ΡΡΡΡΠΈ, Π½ΠΎ ΠΈ ΠΌΠ΅Π½ΡΠ΅Ρ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½ΠΈΠ΅ ΠΎΠ± ΠΈΠ½Π΄ΠΈΠ²ΠΈΠ΄ΡΠ°Π»ΡΠ½ΠΎ-ΠΏΡΠΈΡ
ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΡΡ
Π½Π°ΡΡΡΡΠΈΠΊΠΎΠ². ΠΠ½Π΄ΡΡΠΈΡΠΎΠ²Π°Π½Π½Π°Ρ ΡΠ°Π΄ΠΎΡΡΡ Π°ΡΡΠΎΡΠΈΠΈΡΡΠ΅ΡΡΡ Ρ ΠΏΠΎΠ»ΠΎΠΆΠΈΡΠ΅Π»ΡΠ½ΡΠΌΠΈ ΠΏΠΎΠ»ΡΡΠ°ΠΌΠΈ ΡΠΊΠ°Π» ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠΈ Β«ΠΠΈΡΠ½ΠΎΡΡΠ½ΡΠΉ Π΄ΠΈΡΡΠ΅ΡΠ΅Π½ΡΠΈΠ°Π»Β», ΠΈΠ½Π΄ΡΡΠΈΡΠΎΠ²Π°Π½Π½Π°Ρ Π³ΡΡΡΡΡ β Ρ ΠΎΡΡΠΈΡΠ°ΡΠ΅Π»ΡΠ½ΡΠΌΠΈ. ΠΠ°ΠΏΡΠ°Π²Π»Π΅Π½Π½ΡΠ΅ ΡΡΠ°Π½ΡΡΠΎΡΠΌΠ°ΡΠΈΠΈ ΠΏΠΎ-ΡΠ°Π·Π½ΠΎΠΌΡ Π²Π»ΠΈΡΡΡ Π½Π° ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½ΠΈΡ ΠΎ ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½ΡΠ°Ρ
ΠΈΠΌΠΏΠ»ΠΈΡΠΈΡΠ½ΠΎΠΉ ΡΡΡΡΠΊΡΡΡΡ Π»ΠΈΡΠ½ΠΎΡΡΠΈ β Β«ΠΎΡΠ΅Π½ΠΊΠ΅Β», Β«ΡΠΈΠ»Π΅Β», Β«Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈΒ». Π Π²ΠΎΡΠΏΡΠΈΡΡΠΈΠΈ ΠΆΠ΅Π½ΡΠΊΠΈΡ
Π»ΠΈΡ ΡΠ°ΡΠ΅ Π·Π°ΠΌΠ΅ΡΠ½Π° ΡΠΊΡΡΡΠ°Π²Π΅ΡΡΠΈΡΠΎΠ²Π°Π½Π½ΠΎΡΡΡ, ΠΌΡΠΆΡΠΊΠΈΡ
Π»ΠΈΡ β Π΄ΠΎΠΌΠΈΠ½ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅/ΠΏΠΎΠ΄ΡΠΈΠ½Π΅Π½ΠΈΠ΅. ΠΠ±Π½Π°ΡΡΠΆΠ΅Π½Π½ΡΠ΅ Π·Π°ΠΊΠΎΠ½ΠΎΠΌΠ΅ΡΠ½ΠΎΡΡΠΈ ΠΌΠΎΠ΄ΠΈΡΠΈΡΠΈΡΡΡΡΡΡ ΠΏΠΎΠ΄ Π²Π»ΠΈΡΠ½ΠΈΠ΅ΠΌ ΠΌΠΎΡΡΠΎΡΠΈΠΏΠ° Π»ΠΈΡΠ° ΠΈ ΡΠ°ΠΌΠΎΠΎΡΠ΅Π½ΠΊΠΈ Π½Π°Π±Π»ΡΠ΄Π°ΡΠ΅Π»Ρ.
ΠΠ±ΡΡΠΆΠ΄Π΅Π½ΠΈΠ΅ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΎΠ². Π‘ΠΎΠ²ΠΎΠΊΡΠΏΠ½ΠΎΡΡΡ ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
Π΄Π°Π½Π½ΡΡ
ΠΏΠΎΠ΄ΡΠ²Π΅ΡΠΆΠ΄Π°Π΅Ρ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΡ ΡΠ²Π΅ΡΡ
ΠΎΠ±ΠΎΠ±ΡΠ΅Π½ΠΈΠΉ ΠΏΡΠΎΡΠ²Π»Π΅Π½ΠΈΡ ΡΠ»Π°Π±ΡΡ
ΡΠΌΠΎΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΡ
ΡΠΎΡΡΠΎΡΠ½ΠΈΠΉ Π½Π° ΡΡΠΎΠ²Π½Π΅ Π²ΠΎΡΠΏΡΠΈΡΡΠΈΡ ΠΌΠΈΠΌΠΈΡΠ΅ΡΠΊΠΈ Π½Π΅ΠΉΡΡΠ°Π»ΡΠ½ΠΎΠ³ΠΎ Π»ΠΈΡΠ° ΠΈ ΡΠΊΠ°Π·ΡΠ²Π°Π΅Ρ Π½Π° ΡΠ΅ΡΠ½ΡΡ ΡΠ²ΡΠ·Ρ ΡΠ²Π΅ΡΡ
ΠΎΠ±ΠΎΠ±ΡΠ΅Π½ΠΈΠΉ Ρ Π―-ΠΊΠΎΠ½ΡΠ΅ΠΏΡΠΈΠ΅ΠΉ Π²ΠΎΡΠΏΡΠΈΠ½ΠΈΠΌΠ°ΡΡΠ΅ΠΉ Π»ΠΈΡΠ½ΠΎΡΡΠΈ.
Π Π·Π°ΠΊΠ»ΡΡΠ΅Π½ΠΈΠΈ Π΄Π΅Π»Π°Π΅ΡΡΡ Π²ΡΠ²ΠΎΠ΄ ΠΎ ΡΠΎΠΌ, ΡΡΠΎ ΡΠ°Π·Π½ΠΎΠ½Π°ΠΏΡΠ°Π²Π»Π΅Π½Π½ΠΎΠ΅ Π²Π°ΡΡΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΠΊΠΎΠ½ΡΠΈΠ³ΡΡΠ°ΡΠΈΠΎΠ½Π½ΡΡ
ΠΏΡΠΈΠ·Π½Π°ΠΊΠΎΠ² ΡΠΌΠΎΡΠΈΠΎΠ½Π°Π»ΡΠ½ΠΎ Π½Π΅ΠΉΡΡΠ°Π»ΡΠ½ΠΎΠ³ΠΎ Π»ΠΈΡΠ° ΠΈΠ·Π±ΠΈΡΠ°ΡΠ΅Π»ΡΠ½ΠΎ Π²Π»ΠΈΡΠ΅Ρ Π½Π° ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½ΠΈΠ΅ ΠΎ Π»ΠΈΡΠ½ΠΎΡΡΠΈ Π½Π°ΡΡΡΡΠΈΠΊΠΎΠ². ΠΡΠΎΠ±ΡΡ ΡΠΎΠ»Ρ Π² ΠΎΡΠ΅Π½ΠΊΠ΅ Π»ΠΈΡΠ½ΠΎΡΡΠ½ΡΡ
ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΠ΅ΠΉ ΡΠ΅Π»ΠΎΠ²Π΅ΠΊΠ° ΠΏΠΎ Π²ΡΡΠ°ΠΆΠ΅Π½ΠΈΡ Π΅Π³ΠΎ Π»ΠΈΡΠ° ΠΈΠ³ΡΠ°Π΅Ρ ΡΠΈΠΌΠΏΠ°ΡΠΈΡ/Π°Π½ΡΠΈΠΏΠ°ΡΠΈΡ Π½Π°Π±Π»ΡΠ΄Π°ΡΠ΅Π»Ρ ΠΊ Π½Π°ΡΡΡΡΠΈΠΊΡ, Π° ΡΠ°ΠΊΠΆΠ΅ ΠΈΠ½Π΄ΠΈΠ²ΠΈΠ΄ΡΠ°Π»ΡΠ½ΠΎ-ΠΏΡΠΈΡ
ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΠΈ Π½Π°Π±Π»ΡΠ΄Π°ΡΠ΅Π»Ρ
Indices for Superconformal Field Theories in 3,5 and 6 Dimensions
We present a trace formula for a Witten type Index for superconformal field
theories in d=3,5 and 6 dimensions, generalizing a similar recent construction
in d=4. We perform a detailed study of the decomposition of long
representations into sums of short representations at the unitarity bound to
demonstrate that our trace formula yields the most general index (i.e. quantity
that is guaranteed to be protected by superconformal symmetry alone) for the
corresponding superalgebras. Using the dual gravitational description, we
compute our index for the theory on the world volume of N M2 and M5 branes in
the large N limit. We also compute our index for recently constructed Chern
Simons theories in three dimensions in the large N limit, and find that, in
certain cases, this index undergoes a large N phase transition as a function of
chemical potentials.Comment: a small typo corrected, 46 page
Deformed Oscillator Algebras and Higher-Spin Gauge Interactions of Matter Fields in 2+1 Dimensions
We formulate a non-linear system of equations which describe higher-spin
gauge interactions of massive matter fields in 2+1 dimensional space-time and
explain some properties of the deformed oscillator algebra which underlies this
formulation. In particular we show that the parameter of mass of matter
fields is related to the deformation parameter in this algebra.Comment: LaTex, 12 pages, no figures; Invited talk at the International
Seminar Supersymmetry and Quantum Field Theory dedicated to the memory of
Dmitrij V. Volkov; Kharkov, January 1997; to appear in the proceeding
The role of AmtB, GlnK and glutamine synthetase in regulation of transcription factor tnra in bacillus subtilis
The nitrogen is a macroelement for all alive cells, from bacteria to animals. Although NH3/NH4 are highly toxic to animal, they are the preferred source of nitrogen for the most microorganisms and are assimilated by glutamine synthetase in the GOGAT cycle. The nitrogen limitation triggers a number of regulatory processes and activates many genes, providing the utilizing of alternative nitrogen sources. In Bacillus subtilis the genes of nitrogen metabolism are regulated by the transcription factor TnrA. In a cells it is bound to AmtB-GlnK proteins, the interaction with Glutamine synthetase (GS) represses its DNA-binding activity. Here we show the lack of AmtB leads to the nitrogen deficiency in a cell and, consequently, the increased expression of TnrA-de-pendent genes. In the lack of GlnK the transcription factor TnrA is constitutive bound to GS, the TnrA activity is repressed even under nitrogen limit conditions. Apparently, the TnrA activity is subjected to permanent repression by GS. In the absence of GS, the TnrA activity is strongly higher in compare to control, even under nitrogen limitation, when GS is active. These data allow to suggest that TnrA activity is regulated by the competitive binding to GlnK and GS
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