75 research outputs found
Π Π΅ΡΠΈΠ΄ΠΈΠ² Π³Π΅ΡΠ΅ΡΠΎΡΠΎΠΏΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΎΡΡΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ Π² ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ΅ Π²ΡΠ²ΠΈΡ Π° ΡΠ½Π΄ΠΎΠΏΡΠΎΡΠ΅Π·Π° ΡΠ°Π·ΠΎΠ±Π΅Π΄ΡΠ΅Π½Π½ΠΎΠ³ΠΎ ΡΡΡΡΠ°Π²Π°: ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΠΉ ΡΠ»ΡΡΠ°ΠΉ
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.ΠΠΊΡΡΠ°Π»ΡΠ½ΠΎΡΡΡ. ΠΠ΅ΡΠ΅ΡΠΎΡΠΎΠΏΠΈΡΠ΅ΡΠΊΠ°Ρ ΠΎΡΡΠΈΡΠΈΠΊΠ°ΡΠΈΡ (ΠΠ) ΡΡΠΎ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ Π·ΡΠ΅Π»ΠΎΠΉ ΠΊΠΎΡΡΠΈ Π² ΠΌΡΠ³ΠΊΠΈΡ
ΡΠΊΠ°Π½ΡΡ
. ΠΠ Π² ΠΎΠ±Π»Π°ΡΡΠΈ ΡΠ°Π·ΠΎΠ±Π΅Π΄ΡΠ΅Π½Π½ΠΎΠ³ΠΎ ΡΡΡΡΠ°Π²Π° ΠΌΠΎΠΆΠ΅Ρ Π±ΡΡΡ ΡΠ»Π΅Π΄ΡΡΠ²ΠΈΠ΅ΠΌ ΠΊΠ°ΠΊ ΠΏΠΎΠ²ΡΠ΅ΠΆΠ΄Π΅Π½ΠΈΡ Π½Π΅ΡΠ²Π½ΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΡ, ΡΠ°ΠΊ ΠΈ Π»ΠΎΠΊΠ°Π»ΡΠ½ΠΎΠΉ ΡΡΠ°Π²ΠΌΡ. ΠΠΎΡΠ»Π΅ ΡΠΎΡΠ°Π»ΡΠ½ΠΎΠ³ΠΎ ΡΠ½Π΄ΠΎΠΏΡΠΎΡΠ΅Π·ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΡΠ°Π·ΠΎΠ±Π΅Π΄ΡΠ΅Π½Π½ΠΎΠ³ΠΎ ΡΡΡΡΠ°Π²Π° ΠΠ ΡΠ°Π·Π²ΠΈΠ²Π°Π΅ΡΡΡ Π² 30% Π½Π°Π±Π»ΡΠ΄Π΅Π½ΠΈΠΉ.
Π¦Π΅Π»ΡΡ ΠΏΡΠ±Π»ΠΈΠΊΠ°ΡΠΈΠΈ ΡΠ²Π»ΡΠ΅ΡΡΡ Π΄Π΅ΠΌΠΎΠ½ΡΡΡΠ°ΡΠΈΡ ΡΠ΅Π΄ΠΊΠΎΠ³ΠΎ ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π½Π°Π±Π»ΡΠ΄Π΅Π½ΠΈΡ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠ° Ρ ΡΠ΅ΡΠΈΠ΄ΠΈΠ²ΠΎΠΌ ΠΠ ΠΏΠΎΡΠ»Π΅ ΡΠ»ΠΎΠΆΠ½ΠΎΠ³ΠΎ ΠΏΠ΅ΡΠ²ΠΈΡΠ½ΠΎΠ³ΠΎ ΡΠ½Π΄ΠΎΠΏΡΠΎΡΠ΅Π·ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΡΠ°Π·ΠΎΠ±Π΅Π΄ΡΠ΅Π½Π½ΠΎΠ³ΠΎ ΡΡΡΡΠ°Π²Π°, ΡΠΎΠΏΡΠΎΠ²ΠΎΠΆΠ΄Π°ΡΡΠΈΠΌΡΡ Π°Π½ΠΊΠΈΠ»ΠΎΠ·ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ.
ΠΠΏΠΈΡΠ°Π½ΠΈΠ΅ ΡΠ»ΡΡΠ°Ρ. ΠΠ°ΡΠΈΠ΅Π½Ρ 32 Π»Π΅Ρ ΠΏΠΎΡΡΡΠΏΠΈΠ» Π² ΠΊΠ»ΠΈΠ½ΠΈΠΊΡ Π΄Π»Ρ ΡΠ΅Π²ΠΈΠ·ΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΡΠ½Π΄ΠΎΠΏΡΠΎΡΠ΅Π·ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΡΠ°Π·ΠΎΠ±Π΅Π΄ΡΠ΅Π½Π½ΠΎΠ³ΠΎ ΡΡΡΡΠ°Π²Π° Ρ Π΄ΠΈΠ°Π³Π½ΠΎΠ·ΠΎΠΌ Π·Π°ΡΡΠ°ΡΠ΅Π»ΡΠΉ Π²ΡΠ²ΠΈΡ
Π³ΠΎΠ»ΠΎΠ²ΠΊΠΈ ΡΠ½Π΄ΠΎΠΏΡΠΎΡΠ΅Π·Π° ΠΏΡΠ°Π²ΠΎΠ³ΠΎ ΡΠ°Π·ΠΎΠ±Π΅Π΄ΡΠ΅Π½Π½ΠΎΠ³ΠΎ ΡΡΡΡΠ°Π²Π°, Π³Π΅ΡΠ΅ΡΠΎΡΠΎΠΏΠΈΡΠ΅ΡΠΊΠ°Ρ ΠΎΡΡΠΈΡΠΈΠΊΠ°ΡΠΈΡ ΡΠΏΡΡΡΡ 3 Π³ΠΎΠ΄Π° ΠΏΠΎΡΠ»Π΅ Π²ΡΠ²ΠΈΡ
Π°. ΠΠΎ Π²ΡΠ΅ΠΌΡ ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΈ Π±ΡΠ»ΠΈ ΡΠ»ΠΎΠΆΠ½ΠΎΡΡΠΈ Ρ Π²ΡΠ΄Π΅Π»Π΅Π½ΠΈΠ΅ΠΌ ΡΠ΅Π΄Π°Π»ΠΈΡΠ½ΠΎΠ³ΠΎ Π½Π΅ΡΠ²Π°, Π° ΡΠ°ΠΊΠΆΠ΅ ΡΡΡΡΠΊΡΡΡ ΡΠ½Π΄ΠΎΠΏΡΠΎΡΠ΅Π·Π°. ΠΠ°ΠΌΠΈ Π±ΡΠ»ΠΈ ΡΠ΄Π°Π»Π΅Π½Ρ Π²ΡΠ΅ ΠΎΡΡΠΈΡΠΈΠΊΠ°ΡΡ, ΠΊΠΎΡΠΎΡΡΠ΅ ΠΏΡΠ΅ΠΏΡΡΡΡΠ²ΠΎΠ²Π°Π»ΠΈ Π²ΡΠ²ΠΈΡ
Ρ ΡΠ½Π΄ΠΎΠΏΡΠΎΡΠ΅Π·Π°. Π£ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠ° Π½Π°Π±Π»ΡΠ΄Π°Π»Π°ΡΡ Π½Π΅Π²ΡΠΎΠΏΠ°ΡΠΈΡ ΡΠ΅Π΄Π°Π»ΠΈΡΠ½ΠΎΠ³ΠΎ Π½Π΅ΡΠ²Π° ΡΠΏΡΠ°Π²Π° Ρ ΠΏΠΎΡΠ°ΠΆΠ΅Π½ΠΈΠ΅ΠΌ ΠΌΠ°Π»ΠΎΠ±Π΅ΡΡΠΎΠ²ΠΎΠ³ΠΎ ΠΈ Π±ΠΎΠ»ΡΡΠ΅Π±Π΅ΡΡΠΎΠ²ΠΎΠ³ΠΎ Π½Π΅ΡΠ²ΠΎΠ² Π½Π° ΡΠΎΠ½Π΅ ΠΎΡΠ΅ΠΊΠ°. ΠΠ°ΡΠΈΠ΅Π½Ρ Π±ΡΠ» Π²ΡΠΏΠΈΡΠ°Π½ Π½Π° 21-ΠΉ Π΄Π΅Π½Ρ. ΠΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Π½ΡΠΉ ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΠΉ ΡΠ»ΡΡΠ°ΠΉ ΠΈΠ½ΡΠ΅ΡΠ΅ΡΠ΅Π½ ΡΠ΅ΠΌ, ΡΡΠΎ Ρ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠ° ΡΠ΅ΡΠΈΠ΄ΠΈΠ² ΠΠ ΠΌΠΎΠ³ Π±ΡΡΡ ΠΎΠ±ΡΡΠ»ΠΎΠ²Π»Π΅Π½ ΠΊΠΎΠΌΠ±ΠΈΠ½Π°ΡΠΈΠ΅ΠΉ ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
ΡΠ°ΠΊΡΠΎΡΠΎΠ² ΡΠΈΡΠΊΠ°. Π‘ ΡΡΠ΅ΡΠΎΠΌ ΡΠΎΠ³ΠΎ, ΡΡΠΎ ΡΡΠ°Π²ΠΌΠ° Π±ΡΠ»Π° ΠΏΠΎΠ»ΡΡΠ΅Π½Π° Π² ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ΅ ΠΠ’Π ΠΈ Ρ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠ° ΠΈΠΌΠ΅Π»ΡΡ ΠΏΠ΅ΡΠ΅Π»ΠΎΠΌ ΠΊΠΎΡΡΠ΅ΠΉ ΠΊΠΎΠ½ΡΡΠ°Π»Π°ΡΠ΅ΡΠ°Π»ΡΠ½ΠΎΠΉ Π³ΠΎΠ»Π΅Π½ΠΈ, Π½Π΅Π»ΡΠ·Ρ ΠΈΡΠΊΠ»ΡΡΠΈΡΡ ΡΡΡΠ΅ΠΊΡ ΠΌΠ΅ΡΡΠ½ΠΎΠΉ ΡΡΠ°Π²ΠΌΡ ΡΠ°Π·ΠΎΠ±Π΅Π΄ΡΠ΅Π½Π½ΠΎΠ³ΠΎ ΡΡΡΡΠ°Π²Π°, ΡΡΡΠ³ΡΠ±ΠΈΠ²ΡΠ΅ΠΉ ΠΏΡΠΎΡΠ΅ΡΡ.
ΠΠ°ΠΊΠ»ΡΡΠ΅Π½ΠΈΠ΅. ΠΠ°Π½Π½ΠΎΠ΅ ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΎΠ΅ Π½Π°Π±Π»ΡΠ΄Π΅Π½ΠΈΠ΅ ΠΏΠΎΠ΄ΡΠ΅ΡΠΊΠΈΠ²Π°Π΅Ρ Π²Π°ΠΆΠ½ΠΎΡΡΡ ΠΏΡΠΎΡΠΈΠ»Π°ΠΊΡΠΈΠΊΠΈ Π²Π΅ΡΠΎΡΡΠ½ΡΡ
ΠΎΡΠ»ΠΎΠΆΠ½Π΅Π½ΠΈΠΉ ΠΏΠΎΡΠ»Π΅ ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΈ ΠΈ ΠΏΠΎΠ΄Π΄Π΅ΡΠΆΠ°Π½ΠΈΡ ΠΎΠ±ΡΠ°ΡΠ½ΠΎΠΉ ΡΠ²ΡΠ·ΠΈ Ρ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠ°ΠΌΠΈ, ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎ ΠΎΡΠ½ΠΎΡΡΡΠΈΠΌΠΈΡΡ ΠΊ Π³ΡΡΠΏΠΏΠ΅ Π²ΡΡΠΎΠΊΠΎΠ³ΠΎ ΡΠΈΡΠΊΠ°. ΠΠΏΠΎΠ»Π½Π΅ Π²Π΅ΡΠΎΡΡΠ½ΠΎ, ΡΡΠΎ ΠΏΡΠΈ Π°Π΄Π΅ΠΊΠ²Π°ΡΠ½ΠΎΠΉ ΠΏΡΠΎΡΠΈΠ»Π°ΠΊΡΠΈΠΊΠ΅ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΠ ΠΈ ΡΠ²ΠΎΠ΅Π²ΡΠ΅ΠΌΠ΅Π½Π½ΠΎΠΌ Π²ΠΏΡΠ°Π²Π»Π΅Π½ΠΈΠΈ Π²ΡΠ²ΠΈΡ
Π° ΠΎΠΏΠΈΡΠ°Π½Π½ΡΡ
Π² ΡΡΠ°ΡΡΠ΅ ΠΏΡΠΎΠ±Π»Π΅ΠΌ ΠΏΠΎΡΠ»Π΅ ΠΏΠ΅ΡΠ²ΠΈΡΠ½ΠΎΠ³ΠΎ ΡΠ½Π΄ΠΎΠΏΡΠΎΡΠ΅Π·ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΡΠ΄Π°Π»ΠΎΡΡ Π±Ρ ΠΈΠ·Π±Π΅ΠΆΠ°ΡΡ
Micro Energy Complex Based on Wet-SteamTurbine
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
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 and masses are compatible with a
symmetry breaking , which
retains a massless photon. The vertex couplings possess an energy scale
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
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
, where . 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
ΠΠ·ΡΡΠ΅Π½ΠΈΠ΅ Π²ΠΈΠ΄ΠΎΠ²ΠΎΠ³ΠΎ ΡΠ°Π·Π½ΠΎΠΎΠ±ΡΠ°Π·ΠΈΡ Π±Π°ΠΊΡΠ΅ΡΠΈΠΉ ΡΠΎΠ΄Π° Bifidobacterium ΠΊΠΈΡΠ΅ΡΠ½ΠΎΠΉ ΠΌΠΈΠΊΡΠΎΡΠ»ΠΎΡΡ Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΌΠ΅ΡΠΎΠ΄Π° MALDI-TOF ΠΌΠ°ΡΡ-ΡΠΏΠ΅ΠΊΡΡΠΎΠΌΠ΅ΡΡΠΈΠΈ
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.ΠΡΠ΅Π΄ΡΡΠ°Π²ΠΈΡΠ΅Π»ΠΈ ΡΠΎΠ΄Π° Bifidobacterium ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»ΡΡΡ Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΡΡ ΡΠ°ΡΡΡ ΠΌΠΈΠΊΡΠΎΡΠ»ΠΎΡΡ ΠΊΠΈΡΠ΅ΡΠ½ΠΈΠΊΠ° Π²Π·ΡΠΎΡΠ»ΡΡ
Π»ΡΠ΄Π΅ΠΉ ΠΈ ΡΠΈΡΠ»Π΅Π½Π½ΠΎ Π΄ΠΎΠΌΠΈΠ½ΠΈΡΡΡΡ Π² ΠΌΠΈΠΊΡΠΎΡΠ»ΠΎΡΠ΅ ΠΌΠ»Π°Π΄Π΅Π½ΡΠ΅Π². ΠΠ·Π²Π΅ΡΡΠ½ΠΎ, ΡΡΠΎ Π²ΠΈΠ΄ΠΎΠ²ΠΎΠΉ ΡΠΎΡΡΠ°Π² ΠΊΠΈΡΠ΅ΡΠ½ΡΡ
Π±ΠΈΡΠΈΠ΄ΠΎΠ±Π°ΠΊΡΠ΅ΡΠΈΠΉ ΠΏΠΎΠ΄Π²Π΅ΡΠ³Π°Π΅ΡΡΡ ΡΠΈΠ»ΡΠ½ΡΠΌ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡΠΌ Ρ Π²ΠΎΠ·ΡΠ°ΡΡΠΎΠΌ, ΠΎΠ΄Π½Π°ΠΊΠΎ ΠΌΠ½ΠΎΠ³ΠΈΠ΅ Π΄Π΅ΡΠ°Π»ΠΈ ΡΡΠΎΠ³ΠΎ ΠΏΡΠΎΡΠ΅ΡΡΠ° ΠΎΡΡΠ°ΡΡΡΡ Π½Π΅ΡΡΠ½ΡΠΌΠΈ.Π¦Π΅Π»Ρ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ: ΠΈΠ·ΡΡΠΈΡΡ Π²ΠΈΠ΄ΠΎΠ²ΠΎΠ΅ ΡΠ°Π·Π½ΠΎΠΎΠ±ΡΠ°Π·ΠΈΠ΅ Π±ΠΈΡΠΈΠ΄ΠΎΠ±Π°ΠΊΡΠ΅ΡΠΈΠΉ ΠΊΠΈΡΠ΅ΡΠ½ΠΈΠΊΠ° ΠΈ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΈΡ
ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎΠ³ΠΎ ΠΈ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎΠ³ΠΎ ΡΠΎΡΡΠ°Π²Π° Π² ΠΏΡΠΎΡΠ΅ΡΡΠ΅ Π²Π·ΡΠΎΡΠ»Π΅Π½ΠΈΡ ΡΠ΅Π»ΠΎΠ²Π΅ΠΊΠ° ΠΏΡΠΈ ΠΏΠΎΠΌΠΎΡΠΈ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ MALDI-TOF ΠΌΠ°ΡΡ-ΡΠΏΠ΅ΠΊΡΡΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π° Π±Π΅Π»ΠΊΠΎΠ²ΡΡ
ΠΏΡΠΎΡΠΈΠ»Π΅ΠΉ ΡΠΈΡΡΡΡ
ΠΊΡΠ»ΡΡΡΡ.ΠΠ΅ΡΠΎΠ΄Ρ: ΠΊΡΠΎΡΡ-ΡΠ΅ΠΊΡΠΈΠΎΠ½Π½ΠΎΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ ΡΠ°Π·Π½ΠΎΠΎΠ±ΡΠ°Π·ΠΈΡ Π±ΠΈΡΠΈΠ΄ΠΎΠ±Π°ΠΊΡΠ΅ΡΠΈΠΉ Π² ΡΠΎΡΡΠ°Π²Π΅ Π½ΠΎΡΠΌΠ°Π»ΡΠ½ΠΎΠΉ ΠΌΠΈΠΊΡΠΎΡΠ»ΠΎΡΡ ΠΊΠΈΡΠ΅ΡΠ½ΠΈΠΊΠ° ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΎ Ρ 93 ΡΠ΅Π»ΠΎΠ²Π΅ΠΊ Π² Π²ΠΎΠ·ΡΠ°ΡΡΠ΅ ΠΎΡ 1 ΠΌΠ΅Ρ Π΄ΠΎ 57 Π»Π΅Ρ. ΠΡΡΡΠ΅ΡΡΠ²Π»ΡΠ»ΠΈ Π²ΡΠ΄Π΅Π»Π΅- Π½ΠΈΠ΅ ΡΠΈΡΡΡΡ
ΠΊΡΠ»ΡΡΡΡ ΠΈ ΠΈΡ
ΠΈΠ΄Π΅Π½ΡΠΈΡΠΈΠΊΠ°ΡΠΈΡ Π½Π° ΠΏΡΠΈΠ±ΠΎΡΠ΅ Microflex LT MALDI-TOF MS (Bruker Daltonics, ΠΠ΅ΡΠΌΠ°Π½ΠΈΡ), ΠΏΠΎΠ΄ΡΠ²Π΅ΡΠΆΠ΄Π΅Π½ΠΈΠ΅ ΡΠ΅Π°Π»ΠΈΠ·ΠΎΠ²ΡΠ²Π°Π»ΠΈ Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΡΠ΅ΠΊΠ²Π΅Π½ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΡΡΠ°Π³ΠΌΠ΅Π½ΡΠ° Π³Π΅Π½Π° 16S ΡΠ ΠΠ.Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ: Ρ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ MALDI-TOF ΠΌΠ°ΡΡ-ΡΠΏΠ΅ΠΊΡΡΠΎΠΌΠ΅ΡΡΠΈΠΈ Π±ΡΠ»ΠΎ ΡΡΠΏΠ΅ΡΠ½ΠΎ ΠΈΠ΄Π΅Π½ΡΠΈΡΠΈΡΠΈΡΠΎΠ²Π°Π½ΠΎ 93% Π²ΡΠ΄Π΅Π»Π΅Π½Π½ΡΡ
ΡΡΠ°ΠΌΠΌΠΎΠ² Π±ΠΈΡΠΈΠ΄ΠΎΠ±Π°ΠΊΡΠ΅ΡΠΈΠΉ. ΠΠΈΠ½ΠΈΠΌΡΠΌ ΠΏΠΎ 2 ΠΏΡΠ΅Π΄ΡΡΠ°Π²ΠΈΡΠ΅Π»Ρ ΠΎΡ ΠΊΠ°ΠΆΠ΄ΠΎΠ³ΠΎ ΠΈΠ· Π²ΠΈΠ΄ΠΎΠ² Π±ΡΠ»ΠΈ Π΄ΠΎΠΏΠΎΠ»Π½ΠΈΡΠ΅Π»ΡΠ½ΠΎ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½Ρ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ ΡΠ΅ΠΊΠ²Π΅Π½ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΡΡΠ°Π³ΠΌΠ΅Π½ΡΠ° Π³Π΅Π½Π° 16SΡΠ ΠΠ; Π²ΠΎ Π²ΡΠ΅Ρ
ΡΠ»ΡΡΠ°ΡΡ
ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ² ΡΠΎΠ²ΠΏΠ°Π»ΠΈ. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ Ρ Π²ΠΎΠ·ΡΠ°ΡΡΠΎΠΌ ΠΏΡΠΎΠΈΡΡ
ΠΎΠ΄ΠΈΡ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΠ΅ ΠΎΠ±ΡΠ΅ΠΉ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΠΈ Π±ΠΈΡΠΈΠ΄ΠΎΠ±Π°ΠΊΡΠ΅ΡΠΈΠΉ (p 0,001), ΡΠΌΠ΅Π½ΡΡΠ°Π΅ΡΡΡ Π²ΡΡΡΠ΅ΡΠ°Π΅ΠΌΠΎΡΡΡ Π²ΠΈΠ΄ΠΎΠ² Bifidobacterium bifidum (p =0,020) ΠΈ Bifidobacterium breve (p 0,001), Π° Π²ΡΡΡΠ΅ΡΠ°Π΅ΠΌΠΎΡΡΡ Π²ΠΈΠ΄Π° Bifidobacterium adolescentis ΡΠ²Π΅Π»ΠΈΡΠΈΠ²Π°Π΅ΡΡΡ (p 0,001), ΠΎΡΡΠ°ΠΆΠ°Ρ ΠΏΠΎΡΡΠ΅ΠΏΠ΅Π½Π½ΡΠ΅ ΠΏΡΠΎΡΠ΅ΡΡΡ ΠΏΠ΅ΡΠ΅ΡΡΡΠΎΠΉΠΊΠΈ ΠΌΠΈΠΊΡΠΎΡΠ»ΠΎΡΡ.ΠΠ°ΠΊΠ»ΡΡΠ΅Π½ΠΈΠ΅: ΠΌΠ΅ΡΠΎΠ΄ MALDI-TOF ΠΌΠ°ΡΡ-ΡΠΏΠ΅ΠΊΡΡΠΎΠΌΠ΅ΡΡΠΈΠΈ ΠΏΠΎΠΊΠ°Π·Π°Π» Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΡ Π±ΡΡΡΡΠΎΠΉ ΠΈ Π½Π°Π΄Π΅ΠΆΠ½ΠΎΠΉ ΠΈΠ΄Π΅Π½ΡΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ Π±ΠΈΡΠΈΠ΄ΠΎΠ±Π°ΠΊΡΠ΅ΡΠΈΠΉ, ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΠ²ΡΠ΅ΠΉ ΠΏΡΠΎΠ²Π΅ΡΡΠΈ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠΉ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²Π΅Π½Π½ΡΡ
ΠΈ ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅Π½Π½ΡΡ
ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Π΅ΠΉ ΠΌΠΈΠΊΡΠΎΡΠ»ΠΎΡΡ ΡΠ΅Π»ΠΎΠ²Π΅ΠΊΠ° Π² ΠΏΡΠΎΡΠ΅ΡΡΠ΅ Π²Π·ΡΠΎΡΠ»Π΅Π½ΠΈ
Volume element structure and roton-maxon-phonon excitations in superfluid helium beyond the Gross-Pitaevskii approximation
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
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
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
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
Electromagnetic fields are quantized in manifestly covariant way by means of
a class of reducible representations of CCR. 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 four-dimensional oscillators. Vacuum is a Bose-Einstein
condensate of the -oscillator gas. Both the form of 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 . 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
- β¦