17 research outputs found
Global Study of Nuclear Structure Functions
We present the results of a phenomenological study of unpolarized nuclear
structure functions for a wide kinematical region of x and Q^2. As a basis of
our phenomenology we develop a model which takes into account a number of
different nuclear effects including nuclear shadowing, Fermi motion and
binding, nuclear pion excess and off-shell correction to bound nucleon
structure functions. Within this approach we perform a statistical analysis of
available data on the ratio of the nuclear structure functions F_2 for
different nuclei in the range from the deuteron to the lead. We express the
off-shell effect and the effective scattering amplitude describing nuclear
shadowing in terms of few parameters which are common to all nuclei and have a
clear physical interpretation. The parameters are then extracted from
statistical analysis of data. As a result, we obtain an excellent overall
agreement between our calculations and data in the entire kinematical region of
x and Q^2. We discuss a number of applications of our model which include the
calculation of the deuteron structure functions, nuclear valence and sea quark
distributions and nuclear structure functions for neutrino charged-current
scattering.Comment: 67 pages, 18 figures (v3: updated text and references, a new section
with discussion about relation between off-shell effect and modification of
the nucleon size in nuclei, accepted for publication in Nucl. Phys. A
Relativistic Three-Nucleon Calculations within the Bethe-Salpeter Approach
The relativistic properties of the three-nucleon system are investigated using the Faddeev equations within the Bethe-Salpeter approach. The nucleon-nucleon interaction is chosen in a separable form. The Gauss quadrature method is used to calculate the integrals. The system of the integral equations is solved by an iterative method. The binding energy and the partial-wave amplitudes (1S0 and 3S1) of the triton are found
ΠΠΠ’ΠΠ ΠΠΠΠΠΠ¬ΠΠΠΠ Π€ΠΠΠ ΠΠΠΠΠΠΠ Π Π₯ΠΠ Π£Π ΠΠΠ ΠΠΠ’Π ΠΠΠΠΠ’ΠΠ§ΠΠ‘ΠΠΠ₯ ΠΠΠ£Π’Π ΠΠ§ΠΠ ΠΠΠΠ«Π₯ ΠΠ ΠΠΠΠΠΠΠΠ―ΠΠΠ
More than 70% of hypertensive hemorrhages are located in deep brain structures. The removal of such hematomas using encephalotomy is accompanied by additional cerebral trauma and often results in unsatisfactory outcomes. The puncture aspiration with local fibrinolysis is one of the minimal invasive methods for treatment of intracerebral hematomas (ICH). The puncture and aspiration of liquid part of ICH (not more than 20% of ICH volume) is performed via small burr hole. Afterward the catheter is placed into ICH cavity and fibrinolytic is injected via this catheter in postoperative period for lysis of ICH solid part. The lysed blood is aspirated within 1-4 days. The last generations of fibrinolytics are very effective concerning intensity of blood clot lysis and practically have no systematic effect on blood coagulation system during their local usage. Morphological examinations showed that usage of fibrinolysis leads to formation of smaller cysts in the region of former hematoma as well as reparative processes in perihemorrhagical zone are expressed better comparing with treatment methods without usage of fibrinolytics. The morphological pattern is also confirmed by clinical signs of neurological deficit regress corresponding to damage focus. We operated 124 patients with parenchymal hemorrhages and 28 patients with intraventricular hemorrhages using described minimally invasive method at the base of Scientific Research Institute of Emergency Care n.a. N.V. Sklifosovsky. The applied method allowed decreasing lethality from 35% to 21% among patients with parenchymal ICH and from 98% to 48% - among patients with ventricular hemotamponade underwent usage of ventricular drainage combined with local fibrinolysis.Β Β ΠΠΎΠ»Π΅Π΅ 70% Π³ΠΈΠΏΠ΅ΡΡΠ΅Π½Π·ΠΈΠ²Π½ΡΡ
ΠΊΡΠΎΠ²ΠΎΠΈΠ·Π»ΠΈΡΠ½ΠΈΠΉ ΡΠ°ΡΠΏΠΎΠ»Π°Π³Π°ΡΡΡΡ Π² Π³Π»ΡΠ±ΠΈΠ½Π½ΡΡ
ΠΎΡΠ΄Π΅Π»Π°Ρ
Π³ΠΎΠ»ΠΎΠ²Π½ΠΎΠ³ΠΎ ΠΌΠΎΠ·Π³Π°. Π£Π΄Π°Π»Π΅Π½ΠΈΠ΅ ΡΡΠΈΡ
Π³Π΅ΠΌΠ°ΡΠΎΠΌ ΠΏΡΡΠ΅ΠΌ ΡΠ½ΡΠ΅ΡΠ°Π»ΠΎΡΠΎΠΌΠΈΠΈ ΡΠΎΠΏΡΠΎΠ²ΠΎΠΆΠ΄Π°Π΅ΡΡΡ Π΄ΠΎΠΏΠΎΠ»Π½ΠΈΡΠ΅Π»ΡΠ½ΠΎΠΉ ΡΡΠ°Π²ΠΌΠ°ΡΠΈΠ·Π°ΡΠΈΠ΅ΠΉ ΠΌΠΎΠ·Π³Π°, ΠΈ ΡΠ°ΡΡΠΎ Π½Π΅ΡΠ΄ΠΎΠ²Π»Π΅ΡΠ²ΠΎΡΠΈΡΠ΅Π»ΡΠ½ΡΠΌΠΈ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ°ΠΌΠΈ. ΠΠ΄Π½ΠΈΠΌ ΠΈΠ· ΠΌΠ°Π»ΠΎΡΡΠ°Π²ΠΌΠ°ΡΠΈΡΠ½ΡΡ
ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ² ΡΠ²Π°ΠΊΡΠ°ΡΠΈΠΈ Π²Π½ΡΡΡΠΈΠΌΠΎΠ·Π³ΠΎΠ²ΡΡ
Π³Π΅ΠΌΠ°ΡΠΎΠΌ (ΠΠΠ) ΡΠ²Π»ΡΠ΅ΡΡΡ ΠΏΡΠ½ΠΊΡΠΈΠΎΠ½Π½Π°Ρ Π°ΡΠΏΠΈΡΠ°ΡΠΈΡ ΠΈ Π»ΠΎΠΊΠ°Π»ΡΠ½ΡΠΉ ΡΠΈΠ±ΡΠΈΠ½ΠΎΠ»ΠΈΠ·. Π§Π΅ΡΠ΅Π· Π½Π΅Π±ΠΎΠ»ΡΡΠΎΠ΅ ΡΡΠ΅ΠΏΠ°Π½Π°ΡΠΈΠΎΠ½Π½ΠΎΠ΅ ΠΎΡΠ²Π΅ΡΡΡΠΈΠ΅ ΠΠΠ ΠΏΡΠ½ΠΊΡΠΈΡΡΡΡ ΠΈ Π°ΡΠΏΠΈΡΠΈΡΡΡΡ ΠΆΠΈΠ΄ΠΊΡΡ ΡΠ°ΡΡΡ, ΠΊΠΎΡΠΎΡΠ°Ρ ΡΠΎΡΡΠ°Π²Π»ΡΠ΅Ρ Π½Π΅ Π±ΠΎΠ»Π΅Π΅ 20%. Π ΠΏΠΎΠ»ΠΎΡΡΠΈ Π³Π΅ΠΌΠ°ΡΠΎΠΌΡ ΠΎΡΡΠ°Π²Π»ΡΡΡ ΠΊΠ°ΡΠ΅ΡΠ΅Ρ, ΡΠ΅ΡΠ΅Π· ΠΊΠΎΡΠΎΡΡΠΉ Π² ΠΏΠΎΡΠ»Π΅ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΎΠ½Π½ΠΎΠΌ ΠΏΠ΅ΡΠΈΠΎΠ΄Π΅ Π²Π²ΠΎΠ΄ΡΡ ΡΠΈΠ±ΡΠΈΠ½ΠΎΠ»ΠΈΡΠΈΠΊ, ΡΠ°ΡΡΠ²ΠΎΡΡΡΡΠΈΠΉ ΠΏΠ»ΠΎΡΠ½ΡΡ ΡΠ°ΡΡΡ Π³Π΅ΠΌΠ°ΡΠΎΠΌΡ. ΠΠΈΠ·ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ ΠΊΡΠΎΠ²Ρ Π°ΡΠΏΠΈΡΠΈΡΡΡΡ Π² ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ 1-4 ΡΡΡΠΎΠΊ. ΠΠΎΡΠ»Π΅Π΄Π½ΠΈΠ΅ ΠΏΠΎΠΊΠΎΠ»Π΅Π½ΠΈΡ ΡΠΈΠ±ΡΠΈΠ½ΠΎΠ»ΠΈΡΠΈΠΊΠΎΠ² ΠΎΡΠ΅Π½Ρ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½Ρ Π² ΠΏΠ»Π°Π½Π΅ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΠΈ ΡΠ°ΡΡΠ²ΠΎΡΠ΅Π½ΠΈΡ ΡΠ³ΡΡΡΠΊΠ° ΠΊΡΠΎΠ²ΠΈ ΠΈ ΠΏΡΠ°ΠΊΡΠΈΡΠ΅ΡΠΊΠΈ Π½Π΅ ΠΎΠ±Π»Π°Π΄Π°ΡΡ ΡΠΈΡΡΠ΅ΠΌΠ½ΡΠΌ Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ΠΌ Π½Π° ΡΠ²Π΅ΡΡΡΠ²Π°ΡΡΡΡ ΡΠΈΡΡΠ΅ΠΌΡ ΠΊΡΠΎΠ²ΠΈ ΠΏΡΠΈ Π»ΠΎΠΊΠ°Π»ΡΠ½ΠΎΠΌ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠΈ. ΠΠΎΡΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΈ, ΡΡΠΎ ΠΏΡΠΈ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠΈ ΡΠΈΠ±ΡΠΈΠ½ΠΎΠ»ΠΈΠ·Π° Π² ΠΎΠ±Π»Π°ΡΡΠΈ Π±ΡΠ²ΡΠ΅ΠΉ Π³Π΅ΠΌΠ°ΡΠΎΠΌΡ ΡΠΎΡΠΌΠΈΡΡΠ΅ΡΡΡ ΠΊΠΈΡΡΠ° ΠΌΠ΅Π½ΡΡΠ΅Π³ΠΎ ΡΠ°Π·ΠΌΠ΅ΡΠ°, Π° ΡΠ΅ΠΏΠ°ΡΠ°ΡΠΈΠ²Π½ΡΠ΅ ΠΏΡΠΎΡΠ΅ΡΡΡ Π² Π·ΠΎΠ½Π΅, ΠΎΠΊΡΡΠΆΠ°ΡΡΠ΅ΠΉ Π³Π΅ΠΌΠ°ΡΠΎΠΌΡ, Π²ΡΡΠ°ΠΆΠ΅Π½Ρ Π»ΡΡΡΠ΅, ΡΠ΅ΠΌ Π² ΡΠ»ΡΡΠ°ΡΡ
Π»Π΅ΡΠ΅Π½ΠΈΡ Π±Π΅Π· ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ ΡΠΈΠ±ΡΠΈΠ½ΠΎΠ»ΠΈΡΠΈΠΊΠΎΠ². ΠΠΎΡΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠ°Ρ ΠΊΠ°ΡΡΠΈΠ½Π° ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΡΠ΅Ρ ΠΈ ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΠΌ Π΄Π°Π½Π½ΡΠΌ ΠΎ ΡΠ΅Π³ΡΠ΅ΡΡΠ΅ Π½Π΅Π²ΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠΈΠΌΠΏΡΠΎΠΌΠ°ΡΠΈΠΊΠΈ, ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΡΡΡΠ΅ΠΉ ΠΎΡΠ°Π³Ρ ΠΏΠΎΡΠ°ΠΆΠ΅Π½ΠΈΡ. Π ΠΈΠ½ΡΡΠΈΡΡΡΠ΅ ΡΠΊΠΎΡΠΎΠΉ ΠΏΠΎΠΌΠΎΡΠΈ ΠΈΠΌ. Π.Π. Π‘ΠΊΠ»ΠΈΡΠΎΡΠΎΠ²ΡΠΊΠΎΠ³ΠΎ ΠΏΡΠΎΠΎΠΏΠ΅ΡΠΈΡΠΎΠ²Π°Π½Ρ 124 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠ° Ρ ΠΏΠ°ΡΠ΅Π½Ρ
ΠΈΠΌΠ°ΡΠΎΠ·Π½ΡΠΌΠΈ ΠΊΡΠΎΠ²ΠΎΠΈΠ·Π»ΠΈΡΠ½ΠΈΡΠΌΠΈ ΠΈ 28 β Ρ Π²Π΅Π½ΡΡΠΈΠΊΡΠ»ΡΡΠ½ΡΠΌΠΈ. ΠΠ΅ΡΠΎΠ΄ ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΠ» ΡΠ½ΠΈΠ·ΠΈΡΡ Π»Π΅ΡΠ°Π»ΡΠ½ΠΎΡΡΡ Ρ 35 Π΄ΠΎ 21%Β ΠΏΡΠΈ ΠΏΠ°ΡΠ΅Π½Ρ
ΠΈΠΌΠ°ΡΠΎΠ·Π½ΡΡ
ΠΠΠ ΠΈ Ρ 98 Π΄ΠΎ 48%Β ΠΏΡΠΈ ΡΠΎΡΠ΅ΡΠ°Π½ΠΈΠΈ Π΄ΡΠ΅Π½ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΆΠ΅Π»ΡΠ΄ΠΎΡΠΊΠΎΠ² Ρ Π»ΠΎΠΊΠ°Π»ΡΠ½ΡΠΌ ΡΠΈΠ±ΡΠΈΠ½ΠΎΠ»ΠΈΠ·ΠΎΠΌ Ρ Π±ΠΎΠ»ΡΠ½ΡΡ
Ρ Π²Π΅Π½ΡΡΠΈΠΊΡΠ»ΡΡΠ½ΠΎΠΉ Π³Π΅ΠΌΠΎΡΠ°ΠΌΠΏΠΎΠ½Π°Π΄ΠΎΠΉ.Β
Orientation teachers of physical education for improve own health
Purpose . The features targeted pedagogical influence on students of the Faculty of Physical Education to strengthen their own health. Material and methods . The study involved 192 students of different pedagogical university faculties of both sexes aged 18-21 years. Results . Revealed that the level of health is not very different Arts Students from the students of the Faculty of Physical Education and is the most "below average". In the process of training future teachers of physical culture introduced pedagogical conditions : enriching the content of academic disciplines of scientific information and educational support during the implementation of the rehabilitation program students. Found that as a result of research indicators of physical health of students of physical education have improved significantly. Conclusions . These data indicate the feasibility and necessity of using these pedagogical conditions in the orientation of the future teachers of physical training to strengthen their own health and the health of the younger generation
Effect of Crab cavity HOMs on the coupled-bunch stability of HL-LHC
High frequency High Order Modes can significantly affect the coupled-bunch stability in a circular accelerator. With a large enough shunt impedance they may drive a coupled-bunch transverse instability. We have developed an analytical model and implemented it in the NHT Vlasov solver. The results show that the instability is characterized by the excitation of many azimuthal intra-bunch modes, which have similar growth rates, that make the traditional remedies such as a flat resistive feedback and chromaticity inefficient in suppressing it. For the High Luminosity Large Hadron Collider this could result in a significant increase of the stabilizing Landau octupole current, up to A ( of the maximum available current). In order to limit the increase below 10 A (), the transverse shunt impedance has to be kept below 1 M/m.High frequency high order modes can significantly affect the coupled-bunch stability in a circular accelerator. With a large enough shunt impedance they may drive a coupled-bunch transverse instability. We have developed an analytical model and implemented it in the nested head-tail Vlasov solver. The results show that the instability is characterized by the excitation of many azimuthal intrabunch modes, which have similar growth rates, that make the traditional remedies such as a flat resistive feedback and chromaticity inefficient in suppressing it. For the High Luminosity Large Hadron Collider this could result in a significant increase of the stabilizing Landau octupole current, up to βΌ100 A (βΌ20% of the maximum available current). In order to limit the increase below 10Β A (βΌ2%), the transverse shunt impedance has to be kept below 1ββMΞ©/m
Dolerites of Svalbard, north-west Barents Sea Shelf: age, tectonic setting and significance for geotectonic interpretation of the High-Arctic Large Igneous Province
The dolerites of Svalbard are mineralogically and geochemically homogeneous with geochemical features typical of continental within-plate tholeiites. Their geochemistry is similar to tholeiites belonging to a bimodal suite defined as the High-Arctic Large Igneous Province (HALIP). KβAr dating of numerous dolerites sampled from many locations across Svalbard define a narrow time span of this magmatism from 125.5Β±3.6 to 78.3Β±2.6 Mya. Discrete peaks of intensive activity occurred at 115.3, 100.8, 91.3 and 78.5 Mya corresponding to (1) breakup of the continental crust and formation of an initial rift as a result of mantle plume activity, located in the southern part of the Alpha Ridge; (2) magmatic activity related to spreading along the Alpha Ridge that led to the development of the initial oceanic crust and (3) continuation of spreading along the Alpha Ridge and termination of magmatic activity related to HALIP (last two peaks at 91.3 and 78.5 Mya)