250 research outputs found
Distribution of xylem hydraulic resistance in fruiting truss of tomato influenced by water stress
In this study xylem hydraulic resistances of peduncles (truss stalk), pedicels (fruit stalk) and the future abscission zone (AZ) halfway along the pedicel of tomato (Lycopersicon esculentum L.) plants were directly measured at different stages of fruit development, in plants grown under two levels of water availability in the root environment. The xylem hydraulic connection between shoot and fruits has previously been investigated, but contradictory conclusions were drawn about the presence of a flow resistance barrier in the pedicel. These conclusions were all based on indirect functional measurements and anatomical observations of water-conducting tissue in the pedicel. In the present study, by far the largest resistances were measured in the AZ where most individual vessels ended. Plants grown at low water availability in the root environment had xylem with higher hydraulic resistances in the peduncle and pedicel segments on both sides of the AZ, while the largest increase in hydraulic resistance was measured in the AZ. During fruit development hydraulic resistances in peduncle and pedicel segments decreased on both sides of the AZ, but tended to increase in the AZ. The overall xylem hydraulic resistance between the shoot and fruit tended to increase with fruit development because of the dominating role of the hydraulic resistance in the AZ. It is discussed whether the xylem hydraulic resistance in the AZ of tomato pedicels in response to water stress and during fruit development contributes to the hydraulic isolation of fruits from diurnal cycles of water stress in the shoot
Π‘ΠΎΠ²ΡΠ΅ΠΌΠ΅Π½Π½ΡΠ΅ ΠΌΠ΅ΡΠΎΠ΄Ρ ΠΈΠ΄Π΅Π½ΡΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ Π²ΠΎΠ·Π±ΡΠ΄ΠΈΡΠ΅Π»Ρ Π³ΠΎΠ½ΠΎΠΊΠΎΠΊΠΊΠΎΠ²ΠΎΠΉΠΈΠ½ΡΠ΅ΠΊΡΠΈΠΈ
The authors present the data on the current laboratory methods and recommendations for identifying the gonorrhea
pathogen applied in Russia and abroad: microscopy method, cultural (bacteriological) study method, nucleic acid
amplification techniques and DNA chip technology. The benefits and shortcomings of each of the techniques have been
compared. The authors emphasize the cultural method is currently considered to be the key one for diagnosing gonorrhea
due to its high specificity and sensitivity making it possible to define the N.gonorrhoeae sensitivity to antimicrobial
drugs, which is very important taking into consideration the N. gonorrhoeae resistance to antibiotics. The nucleic acid
amplification techniques and, first of all, polymerase chain reaction, can be used in Russia as screening methods. The
results obtained by using the techniques need confirmation by the cultural method.ΠΡΠΈΠ²Π΅Π΄Π΅Π½Ρ Π΄Π°Π½Π½ΡΠ΅ ΠΎ ΡΠΎΠ²ΡΠ΅ΠΌΠ΅Π½Π½ΡΡ
Π»Π°Π±ΠΎΡΠ°ΡΠΎΡΠ½ΡΡ
ΠΌΠ΅ΡΠΎΠ΄Π°Ρ
ΠΈ ΡΠ΅ΠΊΠΎΠΌΠ΅Π½Π΄Π°ΡΠΈΡΡ
ΠΏΠΎ ΠΈΠ΄Π΅Π½ΡΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ Π²ΠΎΠ·Π±ΡΠ΄ΠΈΡΠ΅Π»Ρ
Π³ΠΎΠ½ΠΎΡΠ΅ΠΈ, ΠΏΡΠΈΠΌΠ΅Π½ΡΠ΅ΠΌΡΡ
Π² Π ΠΎΡΡΠΈΠΈ ΠΈ Π·Π° ΡΡΠ±Π΅ΠΆΠΎΠΌ: ΠΌΠ΅ΡΠΎΠ΄Π΅ ΠΌΠΈΠΊΡΠΎΡΠΊΠΎΠΏΠΈΠΈ, ΠΊΡΠ»ΡΡΡΡΠ°Π»ΡΠ½ΠΎΠΌ (Π±Π°ΠΊΡΠ΅ΡΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠΌ)
ΠΌΠ΅ΡΠΎΠ΄Π΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ, ΠΌΠ΅ΡΠΎΠ΄Π°Ρ
Π°ΠΌΠΏΠ»ΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ Π½ΡΠΊΠ»Π΅ΠΈΠ½ΠΎΠ²ΡΡ
ΠΊΠΈΡΠ»ΠΎΡ, ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ ΠΠΠ-ΡΠΈΠΏΠΎΠ²; Π² ΡΡΠ°Π²Π½ΠΈΡΠ΅Π»ΡΠ½ΠΎΠΌ
Π°ΡΠΏΠ΅ΠΊΡΠ΅ ΠΎΡΡΠ°ΠΆΠ΅Π½Ρ Π΄ΠΎΡΡΠΎΠΈΠ½ΡΡΠ²Π° ΠΈ Π½Π΅Π΄ΠΎΡΡΠ°ΡΠΊΠΈ ΠΊΠ°ΠΆΠ΄ΠΎΠ³ΠΎ ΠΌΠ΅ΡΠΎΠ΄Π°. ΠΠΎΠ΄ΡΠ΅ΡΠΊΠ½ΡΡΠΎ, ΡΡΠΎ ΠΎΡΠ½ΠΎΠ²ΠΎΠΉ Π΄ΠΈΠ°Π³Π½ΠΎΡΡΠΈΠΊΠΈ Π³ΠΎΠ½ΠΎΡΠ΅ΠΈ
Π² Π½Π°ΡΡΠΎΡΡΠ΅Π΅ Π²ΡΠ΅ΠΌΡ ΡΠ²Π»ΡΠ΅ΡΡΡ ΠΊΡΠ»ΡΡΡΡΠ°Π»ΡΠ½ΡΠΉ ΠΌΠ΅ΡΠΎΠ΄, ΠΎΠ±Π»Π°Π΄Π°ΡΡΠΈΠΉ Π²ΡΡΠΎΠΊΠΎΠΉ ΡΠΏΠ΅ΡΠΈΡΠΈΡΠ½ΠΎΡΡΡΡ ΠΈ ΡΡΠ²ΡΡΠ²ΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΡΡ,
ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡΡΠΈΠΉ ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΡΡ ΡΡΠ²ΡΡΠ²ΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΡ N. gonorrhoeae ΠΊ Π°Π½ΡΠΈΠΌΠΈΠΊΡΠΎΠ±Π½ΡΠΌ ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΠ°ΠΌ, ΡΡΠΎ ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎ Π°ΠΊΡΡΠ°Π»ΡΠ½ΠΎ
Π²Π²ΠΈΠ΄Ρ Π²ΠΎΠ·ΡΠ°ΡΡΠ°Π½ΠΈΡ Π² ΠΏΠΎΡΠ»Π΅Π΄Π½ΠΈΠ΅ Π³ΠΎΠ΄Ρ ΡΠ΅Π·ΠΈΡΡΠ΅Π½ΡΠ½ΠΎΡΡΠΈ N. gonorrhoeae ΠΊ Π°Π½ΡΠΈΠ±ΠΈΠΎΡΠΈΠΊΠ°ΠΌ. ΠΠ΅ΡΠΎΠ΄Ρ Π°ΠΌΠΏΠ»ΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ
Π½ΡΠΊΠ»Π΅ΠΈΠ½ΠΎΠ²ΡΡ
ΠΊΠΈΡΠ»ΠΎΡ ΠΈ ΠΏΡΠ΅ΠΆΠ΄Π΅ Π²ΡΠ΅Π³ΠΎ ΠΏΠΎΠ»ΠΈΠΌΠ΅ΡΠ°Π·Π½Π°Ρ ΡΠ΅ΠΏΠ½Π°Ρ ΡΠ΅Π°ΠΊΡΠΈΡ Π² Π ΠΎΡΡΠΈΠΈ ΠΌΠΎΠ³ΡΡ ΠΏΡΠΈΠΌΠ΅Π½ΡΡΡΡΡ Π² ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅
ΡΠΊΡΠΈΠ½ΠΈΠ½Π³ΠΎΠ²ΡΡ
ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ²; ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ, ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ ΠΏΡΠΈ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠΈ ΡΡΠΈΡ
ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ², ΡΡΠ΅Π±ΡΡΡ ΠΏΠΎΠ΄ΡΠ²Π΅ΡΠΆΠ΄Π΅Π½ΠΈΡ
ΠΊΡΠ»ΡΡΡΡΠ°Π»ΡΠ½ΡΠΌ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ
Nonequilibrium Josephson current in ballistic multiterminal SNS-junctions
We study the nonequilibrium Josephson current in a long two-dimensional
ballistic SNS-junction with a normal reservoir coupled to the normal part of
the junction. The current for a given superconducting phase difference
oscillates as a function of voltage applied between the normal reservoir and
the SNS-junction. The period of the oscillations is , with
the length of the junction, and the amplitude of the oscillations decays as
for and zero temperature. The critical
current shows a similar oscillating, decaying behavior as a function of
voltage, changing sign every oscillation. Normal specular or diffusive
scattering at the NS-interfaces does not qualitatively change the picture.Comment: Proceeding of MS2000, to appear in Physica
Nanostructured metal-fullerene field emission cathode
One of the important properties of carbon nanostructures is their cold electron
emission ability. Carbon nanotubes and other nanostructures are capable of
emitting high currents at relatively low electrical fields. They are already
used in functional devices such as field emitters. The conventional method of
carbon nanostructured cathodes manufacturing is thin film nanocarbon deposition
using CVD process on electrically conducting substrate like metal or doped
silicon plates. The alternative way of manufacturing of carbon field emission
cathodes is based on a special processing of carbon microfibers or composite materials in metal holders. We used the similar approach to produce composite
metal-nanocarbon material which may be easily processed and shaped to
produce an effective field emission cathode which can be easily fixed an any
environment.
When you are citing the document, use the following link http://essuir.sumdu.edu.ua/handle/123456789/2058
Ion generation by tungsten filament for pyroelectric pulsed accelerator
The article is devoted to investigation of ion generation by tungsten filament in vacuum. Electron and ion currents from tungsten filament at different residual air gas pressures are measured and compared. Dependencies of ion and electron currents from tungsten filament on its supply voltage are measured. Production of ions in the vicinity of the filament is discussed. Prospects of tungsten filamentβs application in pyroelectric and piezoelectric pulsed accelerators are discussed.Π‘ΡΠ°ΡΡΡ ΠΏΡΠΈΡΠ²ΡΡΠ΅Π½Π° Π΄ΠΎΡΠ»ΡΠ΄ΠΆΠ΅Π½Π½Ρ Π³Π΅Π½Π΅ΡΠ°ΡΡΡ ΡΠΎΠ½ΡΠ² Π²ΠΎΠ»ΡΡΡΠ°ΠΌΠΎΠ²ΠΎΡ Π½ΠΈΡΠΊΠΎΡ ΡΠΎΠ·ΠΆΠ°ΡΠ΅Π½Π½Ρ Ρ Π²Π°ΠΊΡΡΠΌΡ. ΠΠΈΠΌΡΡΡΠ½Ρ ΡΠ° ΠΏΠΎΡΡΠ²Π½ΡΠ½Ρ ΡΡΡΡΠΌΠΈ Π΅Π»Π΅ΠΊΡΡΠΎΠ½ΡΠ² ΡΠ° ΡΠΎΠ½ΡΠ² Π²ΡΠ΄ Π²ΠΎΠ»ΡΡΡΠ°ΠΌΠΎΠ²ΠΎΡ Π½ΠΈΡΠΊΠΈ ΡΠΎΠ·ΠΆΠ°ΡΠ΅Π½Π½Ρ ΠΏΡΠΈ ΡΡΠ·Π½ΠΈΡ
ΡΠΈΡΠΊΠ°Ρ
Π·Π°Π»ΠΈΡΠΊΠΎΠ²ΠΎΠ³ΠΎ ΠΏΠΎΠ²ΡΡΡΡΠ½ΠΎΠ³ΠΎ Π³Π°Π·Ρ. ΠΠΈΠΌΡΡΡΠ½Ρ Π·Π°Π»Π΅ΠΆΠ½ΠΎΡΡΡ ΡΠΎΠ½Π½ΠΎΠ³ΠΎ Ρ Π΅Π»Π΅ΠΊΡΡΠΎΠ½Π½ΠΎΠ³ΠΎ ΡΡΡΡΠΌΡΠ² Π²ΡΠ΄ Π½ΠΈΡΠΊΠΈ ΡΠΎΠ·ΠΆΠ°ΡΡΠ²Π°Π½Π½Ρ ΡΠ° ΡΡ Π½Π°ΠΏΡΡΠ³ΠΈ ΠΆΠΈΠ²Π»Π΅Π½Π½Ρ. ΠΠ±Π³ΠΎΠ²ΠΎΡΡΡΡΡΡΡ ΡΡΠ²ΠΎΡΠ΅Π½Π½Ρ ΡΠΎΠ½ΡΠ² Ρ Π±Π΅Π·ΠΏΠΎΡΠ΅ΡΠ΅Π΄Π½ΡΠΉ Π±Π»ΠΈΠ·ΡΠΊΠΎΡΡΡ Π½ΠΈΡΠΊΠΈ ΡΠΎΠ·ΠΆΠ°ΡΡΠ²Π°Π½Π½Ρ. ΠΠ±Π³ΠΎΠ²ΠΎΡΡΡΡΡΡΡ ΠΏΠ΅ΡΡΠΏΠ΅ΠΊΡΠΈΠ²ΠΈ Π·Π°ΡΡΠΎΡΡΠ²Π°Π½Π½Ρ Π²ΠΎΠ»ΡΡΡΠ°ΠΌΠΎΠ²ΠΎΡ Π½ΠΈΡΠΊΠΈ ΡΠΎΠ·ΠΆΠ°ΡΠ΅Π½Π½Ρ Π² ΠΏΡΡΠΎΠ΅Π»Π΅ΠΊΡΡΠΈΡΠ½ΠΎΠΌΡ Ρ ΠΏ'ΡΠ·ΠΎΠ΅Π»Π΅ΠΊΡΡΠΈΡΠ½ΠΎΠΌΡ ΡΠΌΠΏΡΠ»ΡΡΠ½ΠΈΡ
ΠΏΡΠΈΡΠΊΠΎΡΡΠ²Π°ΡΠ°Ρ
.Π‘ΡΠ°ΡΡΡ ΠΏΠΎΡΠ²ΡΡΠ΅Π½Π° ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ Π³Π΅Π½Π΅ΡΠ°ΡΠΈΠΈ ΠΈΠΎΠ½ΠΎΠ² Π²ΠΎΠ»ΡΡΡΠ°ΠΌΠΎΠ²ΠΎΠΉ Π½ΠΈΡΡΡ Π½Π°ΠΊΠ°Π»Π° Π² Π²Π°ΠΊΡΡΠΌΠ΅. ΠΠ·ΠΌΠ΅ΡΠ΅Π½Ρ ΠΈ ΡΡΠ°Π²Π½Π΅Π½Ρ ΡΠΎΠΊΠΈ ΡΠ»Π΅ΠΊΡΡΠΎΠ½ΠΎΠ² ΠΈ ΠΈΠΎΠ½ΠΎΠ² ΠΎΡ Π²ΠΎΠ»ΡΡΡΠ°ΠΌΠΎΠ²ΠΎΠΉ Π½ΠΈΡΠΈ Π½Π°ΠΊΠ°Π»Π° ΠΏΡΠΈ ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
Π΄Π°Π²Π»Π΅Π½ΠΈΡΡ
ΠΎΡΡΠ°ΡΠΎΡΠ½ΠΎΠ³ΠΎ Π²ΠΎΠ·Π΄ΡΡΠ½ΠΎΠ³ΠΎ Π³Π°Π·Π°. ΠΠ·ΠΌΠ΅ΡΠ΅Π½Ρ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΈ ΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΠΎΠ³ΠΎ ΡΠΎΠΊΠΎΠ² ΠΎΡ Π½ΠΈΡΠΈ Π½Π°ΠΊΠ°Π»ΠΈΠ²Π°Π½ΠΈΡ ΠΈ Π΅Π΅ Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΡ ΠΏΠΈΡΠ°Π½ΠΈΡ. ΠΠ±ΡΡΠΆΠ΄Π°ΡΡΡΡ ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΈΠΎΠ½ΠΎΠ² Π² Π½Π΅ΠΏΠΎΡΡΠ΅Π΄ΡΡΠ²Π΅Π½Π½ΠΎΠΉ Π±Π»ΠΈΠ·ΠΎΡΡΠΈ Π½ΠΈΡΠΈ Π½Π°ΠΊΠ°Π»ΠΈΠ²Π°Π½ΠΈΡ. ΠΠ±ΡΡΠΆΠ΄Π°ΡΡΡΡ ΠΏΠ΅ΡΡΠΏΠ΅ΠΊΡΠΈΠ²Ρ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡ Π²ΠΎΠ»ΡΡΡΠ°ΠΌΠΎΠ²ΠΎΠΉ Π½ΠΈΡΠΈ Π½Π°ΠΊΠ°Π»Π° Π² ΠΏΠΈΡΠΎΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΎΠΌ ΠΈ ΠΏΡΠ΅Π·ΠΎΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΎΠΌ ΠΈΠΌΠΏΡΠ»ΡΡΠ½ΡΡ
ΡΡΠΊΠΎΡΠΈΡΠ΅Π»ΡΡ
Nonequilibrium Josephson effect in mesoscopic ballistic multiterminal SNS junctions
We present a detailed study of nonequilibrium Josephson currents and
conductance in ballistic multiterminal SNS-devices. Nonequilibrium is created
by means of quasiparticle injection from a normal reservoir connected to the
normal part of the junction. By applying a voltage at the normal reservoir the
Josephson current can be suppressed or the direction of the current can be
reversed. For a junction longer than the thermal length, , the
nonequilibrium current increases linearly with applied voltage, saturating at a
value equal to the equilibrium current of a short junction. The conductance
exhibits a finite bias anomaly around . For symmetric
injection, the conductance oscillates -periodically with the phase
difference between the superconductors, with position of the minimum
( or ) dependent on applied voltage and temperature. For
asymmetric injection, both the nonequilibrium Josephson current and the
conductance becomes -periodic in phase difference. Inclusion of barriers
at the NS-interfaces gives rise to a resonant behavior of the total Josephson
current with respect to junction length with a period . Both
three and four terminal junctions are studied.Comment: 21 pages, 19 figures, submitted to Phys. Rev.
Study of operating modes of STRAUS-R accelerator
The description of a pulsed electron accelerator STRAUS-R (3.5 MeV, 60 kA, 60 ns) and results of its experimental
research for two operation modes are given. In the mode of electron beam focusing the accelerator provides the focal spot of 3-4 mm diameter on a target and maximum exposure dose of 27 R at 1-m distance from the output window. In the irradiating mode the maximum dose achieves 36 R at 1-m distance from the target with inhomogeneity β€ 30% within the area 0.36 mΒ² (irradiation spot diameter is 0.6 m).ΠΡΠΈΠ²Π΅Π΄Π΅Π½Ρ ΠΎΠΏΠΈΡΠ°Π½ΠΈΠ΅ ΠΈ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ ΠΈΠΌΠΏΡΠ»ΡΡΠ½ΠΎΠ³ΠΎ ΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΠΎΠ³ΠΎ ΡΡΠΊΠΎΡΠΈΡΠ΅Π»Ρ Π‘Π’Π ΠΠ£Π‘-Π (3,5 ΠΡΠ, 60 ΠΊΠ, 60 Π½Ρ) Π² Π΄Π²ΡΡ
ΡΠ΅ΠΆΠΈΠΌΠ°Ρ
Π΅Π³ΠΎ ΡΠ°Π±ΠΎΡΡ. Π ΡΠ΅ΠΆΠΈΠΌΠ΅ ΡΠΎΠΊΡΡΠΈΡΠΎΠ²ΠΊΠΈ ΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΏΡΡΠΊΠ° ΡΡΠΊΠΎΡΠΈΡΠ΅Π»Ρ ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠΈΠ²Π°Π΅Ρ ΠΏΠΎΠ»ΡΡΠ΅Π½ΠΈΠ΅ Π½Π° ΠΌΠΈΡΠ΅Π½ΠΈ ΡΠΎΠΊΡΡΠ½ΠΎΠ³ΠΎ ΠΏΡΡΠ½Π° Π΄ΠΈΠ°ΠΌΠ΅ΡΡΠΎΠΌ 3β¦4 ΠΌΠΌ ΠΏΡΠΈ ΠΌΠ°ΠΊΡΠΈΠΌΠ°Π»ΡΠ½ΠΎΠΉ Π΄ΠΎΠ·Π΅ ΡΠΎΡΠΌΠΎΠ·Π½ΠΎΠ³ΠΎ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ 27 Π Π½Π° ΡΠ°ΡΡΡΠΎΡΠ½ΠΈΠΈ 1 ΠΌ ΠΎΡ Π²ΡΡ
ΠΎΠ΄Π½ΠΎΠ³ΠΎ ΡΠ»Π°Π½ΡΠ°. Π ΠΎΠ±Π»ΡΡΠ°ΡΠ΅Π»ΡΠ½ΠΎΠΌ ΡΠ΅ΠΆΠΈΠΌΠ΅ ΠΌΠ°ΠΊΡΠΈΠΌΠ°Π»ΡΠ½Π°Ρ Π΄ΠΎΠ·Π° ΡΠΎΡΠΌΠΎΠ·Π½ΠΎΠ³ΠΎ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ Π½Π° ΡΠ°ΡΡΡΠΎΡΠ½ΠΈΠΈ 1 ΠΌ ΠΎΡ ΠΌΠΈΡΠ΅Π½ΠΈ ΠΏΠΎ ΠΎΡΠΈ ΡΡΠΊΠΎΡΠΈΡΠ΅Π»Ρ Π΄ΠΎΡΡΠΈΠ³Π°Π΅Ρ 36 Π Ρ Π½Π΅ΠΎΠ΄Π½ΠΎΡΠΎΠ΄Π½ΠΎΡΡΡΡ β€ 30% Π½Π° ΠΏΠ»ΠΎΡΠ°Π΄ΠΈ 0,36 ΠΌΒ² (Π΄ΠΈΠ°ΠΌΠ΅ΡΡ ΠΏΡΡΠ½Π° ΠΎΠ±Π»ΡΡΠ΅Π½ΠΈΡ 0,6 ΠΌ).ΠΠ°Π²Π΅Π΄Π΅Π½ΠΎ ΠΎΠΏΠΈΡ Ρ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΈ Π΄ΠΎΡΠ»ΡΠ΄ΠΆΠ΅Π½Ρ ΡΠΌΠΏΡΠ»ΡΡΠ½ΠΎΠ³ΠΎ Π΅Π»Π΅ΠΊΡΡΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΏΡΠΈΡΠΊΠΎΡΡΠ²Π°ΡΠ° Π‘Π’Π ΠΠ£Π‘-Π (3,5 ΠΠ΅Π, 60 ΠΊΠ, 60 Π½Ρ) Ρ Π΄Π²ΠΎΡ
ΡΠ΅ΠΆΠΈΠΌΠ°Ρ
ΠΉΠΎΠ³ΠΎ ΡΠΎΠ±ΠΎΡΠΈ. Π£ ΡΠ΅ΠΆΠΈΠΌΡ ΡΠΎΠΊΡΡΡΠ²Π°Π½Π½Ρ Π΅Π»Π΅ΠΊΡΡΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΏΡΡΠΊΠ° ΠΏΡΠΈΡΠΊΠΎΡΡΠ²Π°Ρ Π·Π°Π±Π΅Π·ΠΏΠ΅ΡΡΡ ΠΎΠ΄Π΅ΡΠΆΠ°Π½Π½Ρ Π½Π° ΠΌΡΡΠ΅Π½Ρ ΡΠΎΠΊΡΡΠ½ΠΎΡ ΠΏΠ»ΡΠΌΠΈ Π΄ΡΠ°ΠΌΠ΅ΡΡΠΎΠΌ 3...4 ΠΌΠΌ ΠΏΡΠΈ ΠΌΠ°ΠΊΡΠΈΠΌΠ°Π»ΡΠ½ΡΠΉ Π΄ΠΎΠ·Ρ Π³Π°Π»ΡΠΌΡΠ²Π½ΠΎΠ³ΠΎ Π²ΠΈΠΏΡΠΎΠΌΡΠ½ΡΠ²Π°Π½Π½Ρ 27 Π Π½Π° Π²ΡΠ΄ΡΡΠ°Π½Ρ 1 ΠΌ Π²ΡΠ΄ Π²ΠΈΡ
ΡΠ΄Π½ΠΎΠ³ΠΎ ΡΠ»Π°Π½ΡΡ. ΠΡΠΈ ΠΎΠΏΡΠΎΠΌΡΠ½Π΅Π½Π½Ρ ΠΌΠ°ΠΊΡΠΈΠΌΠ°Π»ΡΠ½Π° Π΄ΠΎΠ·Π° Π³Π°Π»ΡΠΌΠΎΠ²ΠΎΠ³ΠΎ Π²ΠΈΠΏΡΠΎΠΌΡΠ½ΡΠ²Π°Π½Π½Ρ Π½Π° Π²ΡΠ΄ΡΡΠ°Π½Ρ 1 ΠΌ Π²ΡΠ΄ ΠΌΡΡΠ΅Π½Ρ ΠΏΠΎ ΠΎΡΡ ΠΏΡΠΈΡΠΊΠΎΡΡΠ²Π°ΡΠ° Π΄ΠΎΡΡΠ³Π°Ρ 36 Π Ρ Π½Π΅ΠΎΠ΄Π½ΠΎΡΡΠ΄Π½ΡΡΡΡ β€ 30% Π½Π° ΠΏΠ»ΠΎΡΡ 0,36 ΠΌΒ² (Π΄ΡΠ°ΠΌΠ΅ΡΡ ΠΏΠ»ΡΠΌΠΈ ΠΎΠΏΡΠΎΠΌΡΠ½Π΅Π½Π½Ρ 0,6 ΠΌ)
Exact conserved quantities on the cylinder I: conformal case
The nonlinear integral equations describing the spectra of the left and right
(continuous) quantum KdV equations on the cylinder are derived from integrable
lattice field theories, which turn out to allow the Bethe Ansatz equations of a
twisted ``spin -1/2'' chain. A very useful mapping to the more common nonlinear
integral equation of the twisted continuous spin chain is found. The
diagonalization of the transfer matrix is performed. The vacua sector is
analysed in detail detecting the primary states of the minimal conformal models
and giving integral expressions for the eigenvalues of the transfer matrix.
Contact with the seminal papers \cite{BLZ, BLZ2} by Bazhanov, Lukyanov and
Zamolodchikov is realised. General expressions for the eigenvalues of the
infinite-dimensional abelian algebra of local integrals of motion are given and
explicitly calculated at the free fermion point.Comment: Journal version: references added and minor corrections performe
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