75 research outputs found

    Π Π΅Ρ†ΠΈΠ΄ΠΈΠ² гСтСротопичСской оссификации Π² Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π΅ Π²Ρ‹Π²ΠΈΡ…Π° эндопротСза Ρ‚Π°Π·ΠΎΠ±Π΅Π΄Ρ€Π΅Π½Π½ΠΎΠ³ΠΎ сустава: клиничСский случай

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    Background. Heterotopic ossification (HO) is the formation of mature bone in soft tissues. HO in the hip area can be a consequence of both injury to the nervous system and local trauma. After total hip arthroplasty HO develops in 30% of cases. The aim of the study is to demonstrate a rare clinical case of a recurrence of HO in patient after a primary total hip arthroplasty, accompanied by ankylosing. Case presentation. A 32-year-old patient was admitted to the clinic for revision hip arthroplasty with a diagnosis long-standing dislocation of the right hip joint endoprosthesis head, heterotopic ossification 3 years after dislocation. During the surgery, there were difficulties with the sciatic nerve dissection, as well as the structures of the endoprosthesis. We removed all the ossifications that obstructed the dislocation of the endoprosthesis. The patient had sciatic nerve neuropathy on the right lower limb with lesions of the fibular and tibial nerves on the background of edema. The patient was discharged on the 21st day. The presented clinical case is interesting because the patients relapse could be caused by a combination of various risk factors. Taking into account the fact that the injury was received as a result of an accident and the patient had a fracture of the bones of the contralateral shin, it could be the effect of a local hip injury that aggravated the process. Conclusions. This clinical observation highlights the importance of preventing possible complications after surgery and maintaining feedback with patients, especially those belonging to the high-risk group. It is likely that with adequate prevention of the HO formation and timely reduction of dislocation, the problems described in the article after primary total hip arthroplasty could have been avoided.ΠΠΊΡ‚ΡƒΠ°Π»ΡŒΠ½ΠΎΡΡ‚ΡŒ. ГСтСротопичСская оссификация (Π“Πž) это Ρ„ΠΎΡ€ΠΌΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ Π·Ρ€Π΅Π»ΠΎΠΉ кости Π² мягких тканях. Π“Πž Π² области Ρ‚Π°Π·ΠΎΠ±Π΅Π΄Ρ€Π΅Π½Π½ΠΎΠ³ΠΎ сустава ΠΌΠΎΠΆΠ΅Ρ‚ Π±Ρ‹Ρ‚ΡŒ слСдствиСм ΠΊΠ°ΠΊ поврСТдСния Π½Π΅Ρ€Π²Π½ΠΎΠΉ систСмы, Ρ‚Π°ΠΊ ΠΈ локальной Ρ‚Ρ€Π°Π²ΠΌΡ‹. ПослС Ρ‚ΠΎΡ‚Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ эндопротСзирования Ρ‚Π°Π·ΠΎΠ±Π΅Π΄Ρ€Π΅Π½Π½ΠΎΠ³ΠΎ сустава Π“Πž развиваСтся Π² 30% наблюдСний. ЦСлью ΠΏΡƒΠ±Π»ΠΈΠΊΠ°Ρ†ΠΈΠΈ являСтся дСмонстрация Ρ€Π΅Π΄ΠΊΠΎΠ³ΠΎ клиничСского наблюдСния ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Π° с Ρ€Π΅Ρ†ΠΈΠ΄ΠΈΠ²ΠΎΠΌ Π“Πž послС слоТного ΠΏΠ΅Ρ€Π²ΠΈΡ‡Π½ΠΎΠ³ΠΎ эндопротСзирования Ρ‚Π°Π·ΠΎΠ±Π΅Π΄Ρ€Π΅Π½Π½ΠΎΠ³ΠΎ сустава, ΡΠΎΠΏΡ€ΠΎΠ²ΠΎΠΆΠ΄Π°ΡŽΡ‰ΠΈΠΌΡΡ Π°Π½ΠΊΠΈΠ»ΠΎΠ·ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ. ОписаниС случая. ΠŸΠ°Ρ†ΠΈΠ΅Π½Ρ‚ 32 Π»Π΅Ρ‚ поступил Π² ΠΊΠ»ΠΈΠ½ΠΈΠΊΡƒ для Ρ€Π΅Π²ΠΈΠ·ΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ эндопротСзирования Ρ‚Π°Π·ΠΎΠ±Π΅Π΄Ρ€Π΅Π½Π½ΠΎΠ³ΠΎ сустава с Π΄ΠΈΠ°Π³Π½ΠΎΠ·ΠΎΠΌ застарСлый Π²Ρ‹Π²ΠΈΡ… Π³ΠΎΠ»ΠΎΠ²ΠΊΠΈ эндопротСза ΠΏΡ€Π°Π²ΠΎΠ³ΠΎ Ρ‚Π°Π·ΠΎΠ±Π΅Π΄Ρ€Π΅Π½Π½ΠΎΠ³ΠΎ сустава, гСтСротопичСская оссификация спустя 3 Π³ΠΎΠ΄Π° послС Π²Ρ‹Π²ΠΈΡ…Π°. Π’ΠΎ врСмя ΠΎΠΏΠ΅Ρ€Π°Ρ†ΠΈΠΈ Π±Ρ‹Π»ΠΈ слоТности с Π²Ρ‹Π΄Π΅Π»Π΅Π½ΠΈΠ΅ΠΌ сСдалищного Π½Π΅Ρ€Π²Π°, Π° Ρ‚Π°ΠΊΠΆΠ΅ структур эндопротСза. Нами Π±Ρ‹Π»ΠΈ ΡƒΠ΄Π°Π»Π΅Π½Ρ‹ всС оссификаты, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ прСпятствовали Π²Ρ‹Π²ΠΈΡ…Ρƒ эндопротСза. Π£ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Π° наблюдалась нСвропатия сСдалищного Π½Π΅Ρ€Π²Π° справа с ΠΏΠΎΡ€Π°ΠΆΠ΅Π½ΠΈΠ΅ΠΌ ΠΌΠ°Π»ΠΎΠ±Π΅Ρ€Ρ†ΠΎΠ²ΠΎΠ³ΠΎ ΠΈ Π±ΠΎΠ»ΡŒΡˆΠ΅Π±Π΅Ρ€Ρ†ΠΎΠ²ΠΎΠ³ΠΎ Π½Π΅Ρ€Π²ΠΎΠ² Π½Π° Ρ„ΠΎΠ½Π΅ ΠΎΡ‚Π΅ΠΊΠ°. ΠŸΠ°Ρ†ΠΈΠ΅Π½Ρ‚ Π±Ρ‹Π» выписан Π½Π° 21-ΠΉ дСнь. ΠŸΡ€Π΅Π΄ΡΡ‚Π°Π²Π»Π΅Π½Π½Ρ‹ΠΉ клиничСский случай интСрСсСн Ρ‚Π΅ΠΌ, Ρ‡Ρ‚ΠΎ Ρƒ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Π° Ρ€Π΅Ρ†ΠΈΠ΄ΠΈΠ² Π“Πž ΠΌΠΎΠ³ Π±Ρ‹Ρ‚ΡŒ обусловлСн ΠΊΠΎΠΌΠ±ΠΈΠ½Π°Ρ†ΠΈΠ΅ΠΉ Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Ρ… Ρ„Π°ΠΊΡ‚ΠΎΡ€ΠΎΠ² риска. Π‘ ΡƒΡ‡Π΅Ρ‚ΠΎΠΌ Ρ‚ΠΎΠ³ΠΎ, Ρ‡Ρ‚ΠΎ Ρ‚Ρ€Π°Π²ΠΌΠ° Π±Ρ‹Π»Π° ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π° Π² Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π΅ Π”Π’ΠŸ ΠΈ Ρƒ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Π° имСлся ΠΏΠ΅Ρ€Π΅Π»ΠΎΠΌ костСй ΠΊΠΎΠ½Ρ‚Ρ€Π°Π»Π°Ρ‚Π΅Ρ€Π°Π»ΡŒΠ½ΠΎΠΉ Π³ΠΎΠ»Π΅Π½ΠΈ, нСльзя ΠΈΡΠΊΠ»ΡŽΡ‡ΠΈΡ‚ΡŒ эффСкт мСстной Ρ‚Ρ€Π°Π²ΠΌΡ‹ Ρ‚Π°Π·ΠΎΠ±Π΅Π΄Ρ€Π΅Π½Π½ΠΎΠ³ΠΎ сустава, ΡƒΡΡƒΠ³ΡƒΠ±ΠΈΠ²ΡˆΠ΅ΠΉ процСсс. Π—Π°ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΠ΅. Π”Π°Π½Π½ΠΎΠ΅ клиничСскоС наблюдСниС ΠΏΠΎΠ΄Ρ‡Π΅Ρ€ΠΊΠΈΠ²Π°Π΅Ρ‚ Π²Π°ΠΆΠ½ΠΎΡΡ‚ΡŒ ΠΏΡ€ΠΎΡ„ΠΈΠ»Π°ΠΊΡ‚ΠΈΠΊΠΈ вСроятных ослоТнСний послС ΠΎΠΏΠ΅Ρ€Π°Ρ†ΠΈΠΈ ΠΈ поддСрТания ΠΎΠ±Ρ€Π°Ρ‚Π½ΠΎΠΉ связи с ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Π°ΠΌΠΈ, особСнно относящимися ΠΊ Π³Ρ€ΡƒΠΏΠΏΠ΅ высокого риска. Π’ΠΏΠΎΠ»Π½Π΅ вСроятно, Ρ‡Ρ‚ΠΎ ΠΏΡ€ΠΈ Π°Π΄Π΅ΠΊΠ²Π°Ρ‚Π½ΠΎΠΉ ΠΏΡ€ΠΎΡ„ΠΈΠ»Π°ΠΊΡ‚ΠΈΠΊΠ΅ формирования Π“Πž ΠΈ своСврСмСнном Π²ΠΏΡ€Π°Π²Π»Π΅Π½ΠΈΠΈ Π²Ρ‹Π²ΠΈΡ…Π° описанных Π² ΡΡ‚Π°Ρ‚ΡŒΠ΅ ΠΏΡ€ΠΎΠ±Π»Π΅ΠΌ послС ΠΏΠ΅Ρ€Π²ΠΈΡ‡Π½ΠΎΠ³ΠΎ эндопротСзирования ΡƒΠ΄Π°Π»ΠΎΡΡŒ Π±Ρ‹ ΠΈΠ·Π±Π΅ΠΆΠ°Ρ‚ΡŒ

    Micro Energy Complex Based on Wet-SteamTurbine

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    AbstractThis work is dedicated to the development of the micro energy complex concept based on a wet-steam microturbine and mixed use of conventional and unconventional energy sources for standalone supply of distributed energy consumer, adapted to Russia's climate condition. The development is stipulated by absence of low powered micro energy complexes (MEC) for standalone individual low rise energy consumers at the power supply market. This article describes the working out of the energy complex cycle arrangement, the choice of optimal power for a standalone consumer and the development of wet-steam micro turbin

    Ultraviolet Complete Electroweak Model Without a Higgs Particle

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    An electroweak model with running coupling constants described by an energy dependent entire function is utraviolet complete and avoids unitarity violations for energies above 1 TeV. The action contains no physical scalar fields and no Higgs particle and the physical electroweak model fields are local and satisfy microcausality. The WW and ZZ masses are compatible with a symmetry breaking SU(2)L×U(1)Y→U(1)emSU(2)_L\times U(1)_Y \rightarrow U(1)_{\rm em}, which retains a massless photon. The vertex couplings possess an energy scale ΛW>1\Lambda_W > 1 TeV predicting scattering amplitudes that can be tested at the LHC.Comment: 19 pages, no figures, LaTex file. Equation and text corrected. Reference added. Results remain the same. Final version published in European Physics Journal Plus, 126 (2011

    Non-Localizability and Asymptotic Commutativity

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    The mathematical formalism commonly used in treating nonlocal highly singular interactions is revised. The notion of support cone is introduced which replaces that of support for nonlocalizable distributions. Such support cones are proven to exist for distributions defined on the Gelfand-Shilov spaces SΞ²S^\beta, where 0<Ξ²<10<\beta <1 . This result leads to a refinement of previous generalizations of the local commutativity condition to nonlocal quantum fields. For string propagators, a new derivation of a representation similar to that of K\"{a}llen-Lehmann is proposed. It is applicable to any initial and final string configurations and manifests exponential growth of spectral densities intrinsic in nonlocalizable theories.Comment: This version is identical to the initial one whose ps and pdf files were unavailable, with few corrections of misprint

    Π˜Π·ΡƒΡ‡Π΅Π½ΠΈΠ΅ Π²ΠΈΠ΄ΠΎΠ²ΠΎΠ³ΠΎ разнообразия Π±Π°ΠΊΡ‚Π΅Ρ€ΠΈΠΉ Ρ€ΠΎΠ΄Π° Bifidobacterium ΠΊΠΈΡˆΠ΅Ρ‡Π½ΠΎΠΉ ΠΌΠΈΠΊΡ€ΠΎΡ„Π»ΠΎΡ€Ρ‹ с использованиСм ΠΌΠ΅Ρ‚ΠΎΠ΄Π° MALDI-TOF масс-спСктромСтрии

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    Background: The members of genus Bifidobacterium represent a significant part of intestinal microbiota in adults and predominate in infants. Species repertoire of the intestinal bifidobacteria is known to be subjected to major changes with age; however, many details of this process are still to be elucidated.Objective: Our aim was to study the diversity of intestinal bifidobacteria and changes of their qualitative and quantitative composition characteristics during the process of growing up using MALDI-TOF mass-spectrometric analysis of pure bacterial cultures.Methods: A cross-sectional study of bifidobacteria in the intestinal microbiota was performed in 93 healthy people of the ages from 1 month to 57 years. Strains were identified using Microflex LT MALDI-TOF MS, the confirmation was performed by 16S rRNA gene fragment sequencing.Results: 93% of isolated bifidobacterial strains were successfully identified using MALDI-TOF mass-spectrometry. At least two of the strains from each species were additionally identified by 16S rRNA gene fragment sequencing, in all of the cases the results were the same. It was shown that the total concentration of bifidobacteria decreases with age (p 0.001) as well as the frequency of isolation of Bifidobacterium bifidum (p =0.020) and Bifidobacterium breve (p 0.001), and the frequency of isolation of Bifidobacterium adolescentis, increases (p 0.001), representing the continuous process of transformation of microbiota.Conclusion: The method of MALDI-TOF mass spectrometry demonstrated the ability to perform rapid and reliable identification of bifidobacteria that allowed the study of changes in the quantitative and qualitative characteristics of human microbiota in the process of growing up.ΠŸΡ€Π΅Π΄ΡΡ‚Π°Π²ΠΈΡ‚Π΅Π»ΠΈ Ρ€ΠΎΠ΄Π° Bifidobacterium ΠΏΡ€Π΅Π΄ΡΡ‚Π°Π²Π»ΡΡŽΡ‚ Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½ΡƒΡŽ Ρ‡Π°ΡΡ‚ΡŒ ΠΌΠΈΠΊΡ€ΠΎΡ„Π»ΠΎΡ€Ρ‹ ΠΊΠΈΡˆΠ΅Ρ‡Π½ΠΈΠΊΠ° взрослых людСй ΠΈ числСнно Π΄ΠΎΠΌΠΈΠ½ΠΈΡ€ΡƒΡŽΡ‚ Π² ΠΌΠΈΠΊΡ€ΠΎΡ„Π»ΠΎΡ€Π΅ ΠΌΠ»Π°Π΄Π΅Π½Ρ†Π΅Π². Π˜Π·Π²Π΅ΡΡ‚Π½ΠΎ, Ρ‡Ρ‚ΠΎ Π²ΠΈΠ΄ΠΎΠ²ΠΎΠΉ состав ΠΊΠΈΡˆΠ΅Ρ‡Π½Ρ‹Ρ… Π±ΠΈΡ„ΠΈΠ΄ΠΎΠ±Π°ΠΊΡ‚Π΅Ρ€ΠΈΠΉ подвСргаСтся ΡΠΈΠ»ΡŒΠ½Ρ‹ΠΌ измСнСниям с возрастом, ΠΎΠ΄Π½Π°ΠΊΠΎ ΠΌΠ½ΠΎΠ³ΠΈΠ΅ Π΄Π΅Ρ‚Π°Π»ΠΈ этого процСсса ΠΎΡΡ‚Π°ΡŽΡ‚ΡΡ нСясными.ЦСль исслСдования: ΠΈΠ·ΡƒΡ‡ΠΈΡ‚ΡŒ Π²ΠΈΠ΄ΠΎΠ²ΠΎΠ΅ Ρ€Π°Π·Π½ΠΎΠΎΠ±Ρ€Π°Π·ΠΈΠ΅ Π±ΠΈΡ„ΠΈΠ΄ΠΎΠ±Π°ΠΊΡ‚Π΅Ρ€ΠΈΠΉ ΠΊΠΈΡˆΠ΅Ρ‡Π½ΠΈΠΊΠ° ΠΈ измСнСния ΠΈΡ… качСствСнного ΠΈ количСствСнного состава Π² процСссС взрослСния Ρ‡Π΅Π»ΠΎΠ²Π΅ΠΊΠ° ΠΏΡ€ΠΈ ΠΏΠΎΠΌΠΎΡ‰ΠΈ Ρ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ MALDI-TOF масс-спСктромСтричСского Π°Π½Π°Π»ΠΈΠ·Π° Π±Π΅Π»ΠΊΠΎΠ²Ρ‹Ρ… ΠΏΡ€ΠΎΡ„ΠΈΠ»Π΅ΠΉ чистых ΠΊΡƒΠ»ΡŒΡ‚ΡƒΡ€.ΠœΠ΅Ρ‚ΠΎΠ΄Ρ‹: кросс-сСкционноС исслСдованиС разнообразия Π±ΠΈΡ„ΠΈΠ΄ΠΎΠ±Π°ΠΊΡ‚Π΅Ρ€ΠΈΠΉ Π² составС Π½ΠΎΡ€ΠΌΠ°Π»ΡŒΠ½ΠΎΠΉ ΠΌΠΈΠΊΡ€ΠΎΡ„Π»ΠΎΡ€Ρ‹ ΠΊΠΈΡˆΠ΅Ρ‡Π½ΠΈΠΊΠ° ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½ΠΎ Ρƒ 93 Ρ‡Π΅Π»ΠΎΠ²Π΅ΠΊ Π² возрастС ΠΎΡ‚ 1 мСс Π΄ΠΎ 57 Π»Π΅Ρ‚. ΠžΡΡƒΡ‰Π΅ΡΡ‚Π²Π»ΡΠ»ΠΈ Π²Ρ‹Π΄Π΅Π»Π΅- Π½ΠΈΠ΅ чистых ΠΊΡƒΠ»ΡŒΡ‚ΡƒΡ€ ΠΈ ΠΈΡ… ΠΈΠ΄Π΅Π½Ρ‚ΠΈΡ„ΠΈΠΊΠ°Ρ†ΠΈΡŽ Π½Π° ΠΏΡ€ΠΈΠ±ΠΎΡ€Π΅ Microflex LT MALDI-TOF MS (Bruker Daltonics, ГСрмания), ΠΏΠΎΠ΄Ρ‚Π²Π΅Ρ€ΠΆΠ΄Π΅Π½ΠΈΠ΅ Ρ€Π΅Π°Π»ΠΈΠ·ΠΎΠ²Ρ‹Π²Π°Π»ΠΈ с использованиСм сСквСнирования Ρ„Ρ€Π°Π³ΠΌΠ΅Π½Ρ‚Π° Π³Π΅Π½Π° 16S Ρ€Π ΠΠš.Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹: с ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ MALDI-TOF масс-спСктромСтрии Π±Ρ‹Π»ΠΎ ΡƒΡΠΏΠ΅ΡˆΠ½ΠΎ ΠΈΠ΄Π΅Π½Ρ‚ΠΈΡ„ΠΈΡ†ΠΈΡ€ΠΎΠ²Π°Π½ΠΎ 93% Π²Ρ‹Π΄Π΅Π»Π΅Π½Π½Ρ‹Ρ… ΡˆΡ‚Π°ΠΌΠΌΠΎΠ² Π±ΠΈΡ„ΠΈΠ΄ΠΎΠ±Π°ΠΊΡ‚Π΅Ρ€ΠΈΠΉ. ΠœΠΈΠ½ΠΈΠΌΡƒΠΌ ΠΏΠΎ 2 прСдставитСля ΠΎΡ‚ ΠΊΠ°ΠΆΠ΄ΠΎΠ³ΠΎ ΠΈΠ· Π²ΠΈΠ΄ΠΎΠ² Π±Ρ‹Π»ΠΈ Π΄ΠΎΠΏΠΎΠ»Π½ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ ΠΎΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½Ρ‹ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ сСквСнирования Ρ„Ρ€Π°Π³ΠΌΠ΅Π½Ρ‚Π° Π³Π΅Π½Π° 16SΡ€Π ΠΠš; Π²ΠΎ всСх случаях Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠ² совпали. Показано, Ρ‡Ρ‚ΠΎ с возрастом происходит сниТСниС ΠΎΠ±Ρ‰Π΅ΠΉ ΠΊΠΎΠ½Ρ†Π΅Π½Ρ‚Ρ€Π°Ρ†ΠΈΠΈ Π±ΠΈΡ„ΠΈΠ΄ΠΎΠ±Π°ΠΊΡ‚Π΅Ρ€ΠΈΠΉ (p 0,001), ΡƒΠΌΠ΅Π½ΡŒΡˆΠ°Π΅Ρ‚ΡΡ Π²ΡΡ‚Ρ€Π΅Ρ‡Π°Π΅ΠΌΠΎΡΡ‚ΡŒ Π²ΠΈΠ΄ΠΎΠ² Bifidobacterium bifidum (p =0,020) ΠΈ Bifidobacterium breve (p 0,001), Π° Π²ΡΡ‚Ρ€Π΅Ρ‡Π°Π΅ΠΌΠΎΡΡ‚ΡŒ Π²ΠΈΠ΄Π° Bifidobacterium adolescentis увСличиваСтся (p 0,001), отраТая постСпСнныС процСссы пСрСстройки ΠΌΠΈΠΊΡ€ΠΎΡ„Π»ΠΎΡ€Ρ‹.Π—Π°ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΠ΅: ΠΌΠ΅Ρ‚ΠΎΠ΄ MALDI-TOF масс-спСктромСтрии ΠΏΠΎΠΊΠ°Π·Π°Π» Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡ‚ΡŒ быстрой ΠΈ Π½Π°Π΄Π΅ΠΆΠ½ΠΎΠΉ ΠΈΠ΄Π΅Π½Ρ‚ΠΈΡ„ΠΈΠΊΠ°Ρ†ΠΈΠΈ Π±ΠΈΡ„ΠΈΠ΄ΠΎΠ±Π°ΠΊΡ‚Π΅Ρ€ΠΈΠΉ, позволившСй провСсти исслСдованиС ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠΉ количСствСнных ΠΈ качСствСнных ΠΏΠΎΠΊΠ°Π·Π°Ρ‚Π΅Π»Π΅ΠΉ ΠΌΠΈΠΊΡ€ΠΎΡ„Π»ΠΎΡ€Ρ‹ Ρ‡Π΅Π»ΠΎΠ²Π΅ΠΊΠ° Π² процСссС взрослСни

    Volume element structure and roton-maxon-phonon excitations in superfluid helium beyond the Gross-Pitaevskii approximation

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    We propose a theory which deals with the structure and interactions of volume elements in liquid helium II. The approach consists of two nested models linked via parametric space. The short-wavelength part describes the interior structure of the fluid element using a non-perturbative approach based on the logarithmic wave equation; it suggests the Gaussian-like behaviour of the element's interior density and interparticle interaction potential. The long-wavelength part is the quantum many-body theory of such elements which deals with their dynamics and interactions. Our approach leads to a unified description of the phonon, maxon and roton excitations, and has noteworthy agreement with experiment: with one essential parameter to fit we reproduce at high accuracy not only the roton minimum but also the neighboring local maximum as well as the sound velocity and structure factor.Comment: 9 pages, 6 figure

    Bosonization in Particle Physics

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    Path integral techniques in collective fields are shown to be a useful analytical tool to reformulate a field theory defined in terms of microscopic quark (gluon) degrees of freedom as an effective theory of collective boson (meson) fields. For illustrations, the path integral bosonization approach is applied to derive a (non)linear sigma model from a Nambu-Jona-Lasinio (NJL) quark model. The method can be extended to include higher order derivative terms in meson fields or heavy-quark symmetries. It is also approximately applicable to QCD.Comment: 12 pages, LaTeX, uses lamuphys.sty, 5 LaTeX figures, talk given at the Workshop "Field Theoretical Tools in Polymer and Particle Physics", University Wuppertal, June 17-19, 199

    On The Universality Class Of Little String Theories

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    We propose that Little String Theories in six dimensions are quasilocal quantum field theories. Such field theories obey a modification of Wightman axioms which allows Wightman functions (i.e. vacuum expectation values of products of fundamental fields) to grow exponentially in momentum space. Wightman functions of quasilocal fields in x-space violate microlocality at short distances. With additional assumptions about the ultraviolet behavior of quasilocal fields, one can define approximately local observables associated to big enough compact regions. The minimum size of such a region can be interpreted as the minimum distance which observables can probe. We argue that for Little String Theories this distance is of order {\sqrt N}/M_s.Comment: 25 pages, late

    f0(980) meson as a K bar K molecule in a phenomenological Lagrangian approach

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    We discuss a possible interpretation of the f0(980) meson as a hadronic molecule - a bound state of K and bar K mesons. Using a phenomenological Lagrangian approach we calculate the strong f0(980) to pi pi and electromagnetic f0(980) to gamma gamma decays. The compositeness condition provides a self-consistent method to determine the coupling constant between f0 and its constituents, K and bar K. Form factors governing the decays of the f0(980) are calculated by evaluating the kaon loop integrals. The predicted f0(980) to pi pi and f0(980) to gamma gamma decay widths are in good agreement with available data and results of other theoretical approaches.Comment: 21 pages, 11 figures, revised version accepted for publication in Eur. Phys. J.

    Automatic regularization by quantization in reducible representations of CCR: Point-form quantum optics with classical sources

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    Electromagnetic fields are quantized in manifestly covariant way by means of a class of reducible representations of CCR. Aa(x)A_a(x) transforms as a Hermitian four-vector field in Minkowski four-position space (no change of gauge), but in momentum space it splits into spin-1 massless photons (optics) and two massless scalars (similar to dark matter). Unitary dynamics is given by point-form interaction picture, with minimal-coupling Hamiltonian constructed from fields that are free on the null-cone boundary of the Milne universe. SL(2,C) transformations and dynamics are represented unitarily in positive-norm Hilbert space describing NN four-dimensional oscillators. Vacuum is a Bose-Einstein condensate of the NN-oscillator gas. Both the form of Aa(x)A_a(x) and its transformation properties are determined by an analogue of the twistor equation. The same equation guarantees that the subspace of vacuum states is, as a whole, Poincar\'e invariant. The formalism is tested on quantum fields produced by pointlike classical sources. Photon statistics is well defined even for pointlike charges, with UV/IR regularizations occurring automatically as a consequence of the formalism. The probabilities are not Poissonian but of a R\'enyi type with Ξ±=1βˆ’1/N\alpha=1-1/N. The average number of photons occurring in Bremsstrahlung splits into two parts: The one due to acceleration, and the one that remains nonzero even if motion is inertial. Classical Maxwell electrodynamics is reconstructed from coherent-state averaged solutions of Heisenberg equations. Static pointlike charges polarize vacuum and produce effective charge densities and fields whose form is sensitive to both the choice of representation of CCR and the corresponding vacuum state.Comment: 2 eps figures; in v2 notation in Eq. (39) and above Eq. (38) is correcte
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