250 research outputs found

    Distribution of xylem hydraulic resistance in fruiting truss of tomato influenced by water stress

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    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‘ΠΎΠ²Ρ€Π΅ΠΌΠ΅Π½Π½Ρ‹Π΅ ΠΌΠ΅Ρ‚ΠΎΠ΄Ρ‹ ΠΈΠ΄Π΅Π½Ρ‚ΠΈΡ„ΠΈΠΊΠ°Ρ†ΠΈΠΈ возбудитСля Π³ΠΎΠ½ΠΎΠΊΠΎΠΊΠΊΠΎΠ²ΠΎΠΉΠΈΠ½Ρ„Π΅ΠΊΡ†ΠΈΠΈ

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    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.ΠŸΡ€ΠΈΠ²Π΅Π΄Π΅Π½Ρ‹ Π΄Π°Π½Π½Ρ‹Π΅ ΠΎ соврСмСнных Π»Π°Π±ΠΎΡ€Π°Ρ‚ΠΎΡ€Π½Ρ‹Ρ… ΠΌΠ΅Ρ‚ΠΎΠ΄Π°Ρ… ΠΈ рСкомСндациях ΠΏΠΎ ΠΈΠ΄Π΅Π½Ρ‚ΠΈΡ„ΠΈΠΊΠ°Ρ†ΠΈΠΈ возбудитСля Π³ΠΎΠ½ΠΎΡ€Π΅ΠΈ, примСняСмых Π² России ΠΈ Π·Π° Ρ€ΡƒΠ±Π΅ΠΆΠΎΠΌ: ΠΌΠ΅Ρ‚ΠΎΠ΄Π΅ микроскопии, ΠΊΡƒΠ»ΡŒΡ‚ΡƒΡ€Π°Π»ΡŒΠ½ΠΎΠΌ (бактСриологичСском) ΠΌΠ΅Ρ‚ΠΎΠ΄Π΅ исслСдования, ΠΌΠ΅Ρ‚ΠΎΠ΄Π°Ρ… Π°ΠΌΠΏΠ»ΠΈΡ„ΠΈΠΊΠ°Ρ†ΠΈΠΈ Π½ΡƒΠΊΠ»Π΅ΠΈΠ½ΠΎΠ²Ρ‹Ρ… кислот, Ρ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ Π”ΠΠš-Ρ‡ΠΈΠΏΠΎΠ²; Π² ΡΡ€Π°Π²Π½ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠΌ аспСктС ΠΎΡ‚Ρ€Π°ΠΆΠ΅Π½Ρ‹ достоинства ΠΈ нСдостатки ΠΊΠ°ΠΆΠ΄ΠΎΠ³ΠΎ ΠΌΠ΅Ρ‚ΠΎΠ΄Π°. ΠŸΠΎΠ΄Ρ‡Π΅Ρ€ΠΊΠ½ΡƒΡ‚ΠΎ, Ρ‡Ρ‚ΠΎ основой диагностики Π³ΠΎΠ½ΠΎΡ€Π΅ΠΈ Π² настоящСС врСмя являСтся ΠΊΡƒΠ»ΡŒΡ‚ΡƒΡ€Π°Π»ΡŒΠ½Ρ‹ΠΉ ΠΌΠ΅Ρ‚ΠΎΠ΄, ΠΎΠ±Π»Π°Π΄Π°ΡŽΡ‰ΠΈΠΉ высокой ΡΠΏΠ΅Ρ†ΠΈΡ„ΠΈΡ‡Π½ΠΎΡΡ‚ΡŒΡŽ ΠΈ Ρ‡ΡƒΠ²ΡΡ‚Π²ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΡΡ‚ΡŒΡŽ, ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡŽΡ‰ΠΈΠΉ ΠΎΠΏΡ€Π΅Π΄Π΅Π»ΡΡ‚ΡŒ Ρ‡ΡƒΠ²ΡΡ‚Π²ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΡΡ‚ΡŒ N. gonorrhoeae ΠΊ Π°Π½Ρ‚ΠΈΠΌΠΈΠΊΡ€ΠΎΠ±Π½Ρ‹ΠΌ ΠΏΡ€Π΅ΠΏΠ°Ρ€Π°Ρ‚Π°ΠΌ, Ρ‡Ρ‚ΠΎ особСнно Π°ΠΊΡ‚ΡƒΠ°Π»ΡŒΠ½ΠΎ Π²Π²ΠΈΠ΄Ρƒ возрастания Π² послСдниС Π³ΠΎΠ΄Ρ‹ рСзистСнтности N. gonorrhoeae ΠΊ Π°Π½Ρ‚ΠΈΠ±ΠΈΠΎΡ‚ΠΈΠΊΠ°ΠΌ. ΠœΠ΅Ρ‚ΠΎΠ΄Ρ‹ Π°ΠΌΠΏΠ»ΠΈΡ„ΠΈΠΊΠ°Ρ†ΠΈΠΈ Π½ΡƒΠΊΠ»Π΅ΠΈΠ½ΠΎΠ²Ρ‹Ρ… кислот ΠΈ ΠΏΡ€Π΅ΠΆΠ΄Π΅ всСго полимСразная цСпная рСакция Π² России ΠΌΠΎΠ³ΡƒΡ‚ ΠΏΡ€ΠΈΠΌΠ΅Π½ΡΡ‚ΡŒΡΡ Π² качСствС скрининговых ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠ²; Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹, ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Π΅ ΠΏΡ€ΠΈ использовании этих ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠ², Ρ‚Ρ€Π΅Π±ΡƒΡŽΡ‚ подтвСрТдСния ΠΊΡƒΠ»ΡŒΡ‚ΡƒΡ€Π°Π»ΡŒΠ½Ρ‹ΠΌ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ

    Nonequilibrium Josephson current in ballistic multiterminal SNS-junctions

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    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 Ο•\phi oscillates as a function of voltage applied between the normal reservoir and the SNS-junction. The period of the oscillations is πℏvF/L\pi \hbar v_F/L, with LL the length of the junction, and the amplitude of the oscillations decays as Vβˆ’3/2V^{-3/2} for eV≫ℏvF/LeV \gg \hbar v_{F}/L and zero temperature. The critical current IcI_c 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

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    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

    Temperature of impurity ions in a RF heated plasma of the U-3M torsatron as measured by means of the Doppler spectrometry

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    Ion generation by tungsten filament for pyroelectric pulsed accelerator

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    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 filament’s application in pyroelectric and piezoelectric pulsed accelerators are discussed.Бтаття присвячСна Π΄ΠΎΡΠ»Ρ–Π΄ΠΆΠ΅Π½Π½ΡŽ Π³Π΅Π½Π΅Ρ€Π°Ρ†Ρ–Ρ— Ρ–ΠΎΠ½Ρ–Π² Π²ΠΎΠ»ΡŒΡ„Ρ€Π°ΠΌΠΎΠ²ΠΎΡŽ Π½ΠΈΡ‚ΠΊΠΎΡŽ розТарСння Ρƒ Π²Π°ΠΊΡƒΡƒΠΌΡ–. Виміряні Ρ‚Π° порівняні струми Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Ρ–Π² Ρ‚Π° Ρ–ΠΎΠ½Ρ–Π² Π²Ρ–Π΄ Π²ΠΎΠ»ΡŒΡ„Ρ€Π°ΠΌΠΎΠ²ΠΎΡ— Π½ΠΈΡ‚ΠΊΠΈ розТарСння ΠΏΡ€ΠΈ Ρ€Ρ–Π·Π½ΠΈΡ… тисках залишкового повітряного Π³Π°Π·Ρƒ. Виміряні залСТності Ρ–ΠΎΠ½Π½ΠΎΠ³ΠΎ Ρ– Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Π½ΠΎΠ³ΠΎ струмів Π²Ρ–Π΄ Π½ΠΈΡ‚ΠΊΠΈ Ρ€ΠΎΠ·ΠΆΠ°Ρ€ΡŽΠ²Π°Π½Π½Ρ Ρ‚Π° Ρ—Ρ— Π½Π°ΠΏΡ€ΡƒΠ³ΠΈ ТивлСння. ΠžΠ±Π³ΠΎΠ²ΠΎΡ€ΡŽΡŽΡ‚ΡŒΡΡ утворСння Ρ–ΠΎΠ½Ρ–Π² Ρƒ бСзпосСрСдній Π±Π»ΠΈΠ·ΡŒΠΊΠΎΡΡ‚Ρ– Π½ΠΈΡ‚ΠΊΠΈ Ρ€ΠΎΠ·ΠΆΠ°Ρ€ΡŽΠ²Π°Π½Π½Ρ. ΠžΠ±Π³ΠΎΠ²ΠΎΡ€ΡŽΡŽΡ‚ΡŒΡΡ пСрспСктиви застосування Π²ΠΎΠ»ΡŒΡ„Ρ€Π°ΠΌΠΎΠ²ΠΎΡ— Π½ΠΈΡ‚ΠΊΠΈ розТарСння Π² ΠΏΡ–Ρ€ΠΎΠ΅Π»Π΅ΠΊΡ‚Ρ€ΠΈΡ‡Π½ΠΎΠΌΡƒ Ρ– ΠΏ'Ρ”Π·ΠΎΠ΅Π»Π΅ΠΊΡ‚Ρ€ΠΈΡ‡Π½ΠΎΠΌΡƒ Ρ–ΠΌΠΏΡƒΠ»ΡŒΡΠ½ΠΈΡ… ΠΏΡ€ΠΈΡΠΊΠΎΡ€ΡŽΠ²Π°Ρ‡Π°Ρ….Π‘Ρ‚Π°Ρ‚ΡŒΡ посвящСна исслСдованию Π³Π΅Π½Π΅Ρ€Π°Ρ†ΠΈΠΈ ΠΈΠΎΠ½ΠΎΠ² Π²ΠΎΠ»ΡŒΡ„Ρ€Π°ΠΌΠΎΠ²ΠΎΠΉ Π½ΠΈΡ‚ΡŒΡŽ Π½Π°ΠΊΠ°Π»Π° Π² Π²Π°ΠΊΡƒΡƒΠΌΠ΅. Π˜Π·ΠΌΠ΅Ρ€Π΅Π½Ρ‹ ΠΈ сравнСны Ρ‚ΠΎΠΊΠΈ элСктронов ΠΈ ΠΈΠΎΠ½ΠΎΠ² ΠΎΡ‚ Π²ΠΎΠ»ΡŒΡ„Ρ€Π°ΠΌΠΎΠ²ΠΎΠΉ Π½ΠΈΡ‚ΠΈ Π½Π°ΠΊΠ°Π»Π° ΠΏΡ€ΠΈ Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Ρ… давлСниях остаточного Π²ΠΎΠ·Π΄ΡƒΡˆΠ½ΠΎΠ³ΠΎ Π³Π°Π·Π°. Π˜Π·ΠΌΠ΅Ρ€Π΅Π½Ρ‹ зависимости ΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΈ элСктронного Ρ‚ΠΎΠΊΠΎΠ² ΠΎΡ‚ Π½ΠΈΡ‚ΠΈ накаливания ΠΈ Π΅Π΅ напряТСния питания. ΠžΠ±ΡΡƒΠΆΠ΄Π°ΡŽΡ‚ΡΡ ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΈΠΎΠ½ΠΎΠ² Π² нСпосрСдствСнной близости Π½ΠΈΡ‚ΠΈ накаливания. ΠžΠ±ΡΡƒΠΆΠ΄Π°ΡŽΡ‚ΡΡ пСрспСктивы примСнСния Π²ΠΎΠ»ΡŒΡ„Ρ€Π°ΠΌΠΎΠ²ΠΎΠΉ Π½ΠΈΡ‚ΠΈ Π½Π°ΠΊΠ°Π»Π° Π² пироэлСктричСском ΠΈ ΠΏΡŒΠ΅Π·ΠΎΡΠ»Π΅ΠΊΡ‚Ρ€ΠΈΡ‡Π΅ΡΠΊΠΎΠΌ ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠ½Ρ‹Ρ… ускоритСлях

    Nonequilibrium Josephson effect in mesoscopic ballistic multiterminal SNS junctions

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    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, L≫ξTL\gg\xi_T, 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 eVβˆΌβ„vF/LeV \sim \hbar v_F/L. For symmetric injection, the conductance oscillates 2Ο€2\pi-periodically with the phase difference Ο•\phi between the superconductors, with position of the minimum (Ο•=0\phi=0 or Ο€\pi) dependent on applied voltage and temperature. For asymmetric injection, both the nonequilibrium Josephson current and the conductance becomes Ο€\pi-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 ∼λF\sim \lambda_F. 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

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    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 ≀ 30% within the area 0.36 mΒ² (irradiation spot diameter is 0.6 m).ΠŸΡ€ΠΈΠ²Π΅Π΄Π΅Π½Ρ‹ описаниС ΠΈ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ исслСдований ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠ½ΠΎΠ³ΠΎ элСктронного ускоритСля БВРАУБ-Π  (3,5 ΠœΡΠ’, 60 кА, 60 нс) Π² Π΄Π²ΡƒΡ… Ρ€Π΅ΠΆΠΈΠΌΠ°Ρ… Π΅Π³ΠΎ Ρ€Π°Π±ΠΎΡ‚Ρ‹. Π’ Ρ€Π΅ΠΆΠΈΠΌΠ΅ фокусировки элСктронного ΠΏΡƒΡ‡ΠΊΠ° ΡƒΡΠΊΠΎΡ€ΠΈΡ‚Π΅Π»ΡŒ обСспСчиваСт ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½ΠΈΠ΅ Π½Π° мишСни фокусного пятна Π΄ΠΈΠ°ΠΌΠ΅Ρ‚Ρ€ΠΎΠΌ 3…4 ΠΌΠΌ ΠΏΡ€ΠΈ максимальной Π΄ΠΎΠ·Π΅ Ρ‚ΠΎΡ€ΠΌΠΎΠ·Π½ΠΎΠ³ΠΎ излучСния 27 Π  Π½Π° расстоянии 1 ΠΌ ΠΎΡ‚ Π²Ρ‹Ρ…ΠΎΠ΄Π½ΠΎΠ³ΠΎ Ρ„Π»Π°Π½Ρ†Π°. Π’ ΠΎΠ±Π»ΡƒΡ‡Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠΌ Ρ€Π΅ΠΆΠΈΠΌΠ΅ максимальная Π΄ΠΎΠ·Π° Ρ‚ΠΎΡ€ΠΌΠΎΠ·Π½ΠΎΠ³ΠΎ излучСния Π½Π° расстоянии 1 ΠΌ ΠΎΡ‚ мишСни ΠΏΠΎ оси ускоритСля достигаСт 36 Π  с Π½Π΅ΠΎΠ΄Π½ΠΎΡ€ΠΎΠ΄Π½ΠΎΡΡ‚ΡŒΡŽ ≀ 30% Π½Π° ΠΏΠ»ΠΎΡ‰Π°Π΄ΠΈ 0,36 ΠΌΒ² (Π΄ΠΈΠ°ΠΌΠ΅Ρ‚Ρ€ пятна облучСния 0,6 ΠΌ).НавСдСно опис Ρ– Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΈ Π΄ΠΎΡΠ»Ρ–Π΄ΠΆΠ΅Π½ΡŒ Ρ–ΠΌΠΏΡƒΠ»ΡŒΡΠ½ΠΎΠ³ΠΎ Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΏΡ€ΠΈΡΠΊΠΎΡ€ΡŽΠ²Π°Ρ‡Π° БВРАУБ-Π  (3,5 ΠœΠ΅Π’, 60 кА, 60 нс) Ρƒ Π΄Π²ΠΎΡ… Ρ€Π΅ΠΆΠΈΠΌΠ°Ρ… ΠΉΠΎΠ³ΠΎ Ρ€ΠΎΠ±ΠΎΡ‚ΠΈ. Π£ Ρ€Π΅ΠΆΠΈΠΌΡ– фокусування Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΏΡƒΡ‡ΠΊΠ° ΠΏΡ€ΠΈΡΠΊΠΎΡ€ΡŽΠ²Π°Ρ‡ Π·Π°Π±Π΅Π·ΠΏΠ΅Ρ‡ΡƒΡ” одСрТання Π½Π° ΠΌΡ–ΡˆΠ΅Π½Ρ– фокусної плями Π΄Ρ–Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠΌ 3...4 ΠΌΠΌ ΠΏΡ€ΠΈ ΠΌΠ°ΠΊΡΠΈΠΌΠ°Π»ΡŒΠ½Ρ–ΠΉ Π΄ΠΎΠ·Ρ– Π³Π°Π»ΡŒΠΌΡ–Π²Π½ΠΎΠ³ΠΎ Π²ΠΈΠΏΡ€ΠΎΠΌΡ–Π½ΡŽΠ²Π°Π½Π½Ρ 27 Π  Π½Π° відстані 1 ΠΌ Π²Ρ–Π΄ Π²ΠΈΡ…Ρ–Π΄Π½ΠΎΠ³ΠΎ фланця. ΠŸΡ€ΠΈ ΠΎΠΏΡ€ΠΎΠΌΡ–Π½Π΅Π½Π½Ρ– максимальна Π΄ΠΎΠ·Π° гальмового Π²ΠΈΠΏΡ€ΠΎΠΌΡ–Π½ΡŽΠ²Π°Π½Π½Ρ Π½Π° відстані 1 ΠΌ Π²Ρ–Π΄ ΠΌΡ–ΡˆΠ΅Π½Ρ– ΠΏΠΎ осі ΠΏΡ€ΠΈΡΠΊΠΎΡ€ΡŽΠ²Π°Ρ‡Π° досягає 36 Π  с Π½Π΅ΠΎΠ΄Π½ΠΎΡ€Ρ–Π΄Π½Ρ–ΡΡ‚ΡŽ ≀ 30% Π½Π° ΠΏΠ»ΠΎΡ‰Ρ– 0,36 ΠΌΒ² (Π΄Ρ–Π°ΠΌΠ΅Ρ‚Ρ€ плями опромінСння 0,6 ΠΌ)

    Exact conserved quantities on the cylinder I: conformal case

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    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 +1/2+1/2 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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