766 research outputs found
Search for Oscillation of the Electron-Capture Decay Probability of Pm
We have searched for time modulation of the electron capture decay
probability of Pm in an attempt to confirm a recent claim from a group
at the Gesellschaft f\"{u}r Schwerionenforschung (GSI). We produced Pm
via the Sn(Na, 5n)Pm reaction at the Berkeley 88-Inch
Cyclotron with a bombardment time short compared to the reported modulation
period. Isotope selection by the Berkeley Gas-filled Separator is followed by
implantation and a long period of monitoring the Nd K x-rays
from the daughter. The decay time spectrum of the x-rays is well-described by a
simple exponential and the measured half-life of 40.68(53) seconds is
consistent with the accepted value. We observed no oscillatory modulation at
the proposed frequency at a level 31 times smaller than that reported by
Litvinov {\it et al.} (Phys. Lett. B 664 (2008) 162; arXiv:0801.2079
[nucl-ex]). A literature search for previous experiments that might have been
sensitive to the reported modulation uncovered another example in Eu
electron-capture decay. A reanalysis of the published data shows no oscillatory
behavior.Comment: 12 pages (double-spaced), 6 figure
A Tobamovirus Genome That Contains an Internal Ribosome Entry Site Functionalin Vitro
AbstractMost eukaryotic mRNAs are translated by a βscanning ribosomeβ mechanism. We have found that unlike the type member of the genusTobamovirus,translation of the 3β²-proximal coat protein (CP) gene of a crucifer infecting tobamovirus (crTMV) (Dorokhovet al.,1993; 1994) occurredin vitroby an internal ribosome entry mechanism. Three types of synthetic dicistronic RNA transcripts were constructed and translatedin vitro:(i) βMP-CP-3β²NTRβ transcripts contained movement protein (MP) gene, CP gene and the 3β²-nontranslated region of crTMV RNA. These constructs were structurally equivalent to dicistronic subgenomic RNAs produced by tobamovirusesin vivo.(ii) βΞNPT-CPβ transcripts contained partially truncated neomycin phosphotransferase I gene and CP gene. (iii) βCP-GUSβ transcripts contained the first CP gene and the gene ofEscherichia coliΞ²-glucuronidase (GUS) at the 3β²-proximal position. The results indicated that the 148-nt region upstream of the CP gene of crTMV RNA contained an internal ribosome entry site (IRESCP) promoting internal initiation of translationin vitro.Dicistronic IRESCP, containing chimeric mRNAs with the 5β²-terminal stemβloop structure preventing translation of the first gene (MP, ΞNPT, or CP), expressed the CP or GUS genes despite their 3β²-proximal localization. The capacity of crTMV IRESCPfor mediating internal translation distinguishes this CP tobamovirus from the well-known-type member of the genus, TMV UI. The equivalent 148-nt sequence from TMV RNA was incapable of mediating internal translation. Two mutants were used to study structural elements of IRESCP. It was concluded that integrity of IRESCPwas essential for internal initiation. The crTMV provides a new example of internal initiation of translation, which is markedly distinct from IRESs shown for picornaviruses and other viral and eukaryotic mRNAs
Possible Z2 phase and spin-charge separation in electron doped cuprate superconductors
The SU(2) slave-boson mean-field theory for the tt'J model is analyzed. The
role of next-nearest-neighbor hopping t' on the phase-diagram is studied. We
find a pseudogap phase in hole-doped materials (where t'<0). The pseudo-gap
phase is a U(1) spin liquid (the staggered-flux phase) with a U(1) gauge
interaction and no fractionalization. This agrees with experiments on hole
doped samples. The same calculation also indicates that a positive t' favors a
Z2 state with true spin-charge separation. The Z2 state that exists when t' >
0.5J can be a candidate for the pseudo-gap phase of electron-doped cuprates (if
such a phase exists). The experimental situation in electron-doped materials is
also addressed.Comment: 6 pages, 2 figures, RevTeX4. Homepage http://dao.mit.edu/~wen
ΠΠΎΠ²ΡΠΉ ΡΠΏΠΎΡΠΎΠ± ΠΎΡΠΊΡΡΡΠΎΠΉ ΡΠ΅ΠΏΠΎΠ·ΠΈΡΠΈΠΈ ΠΈ ΡΠ΄Π΅ΡΠΆΠ°Π½ΠΈΡ ΠΊΠΎΡΡΠ½ΡΡ ΠΎΡΠ»ΠΎΠΌΠΊΠΎΠ² Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΏΠ»Π°ΡΡΠΈΠΊΠΎΠ²ΡΡ Ρ ΠΎΠΌΡΡΠΎΠ²-ΡΡΡΠΆΠ΅ΠΊ
Background. The quality of fractures reposition in open osteosynthesis is one of the important factors determining the outcome of treatment. Often, the reposition and fixation of bone fragments is not an easy task. The authors propose a method of reposition and temporary fixation of fragments using plastic ty-raps used in electrical work. The aim of the study is to demonstrate the possibilities of new method of intraoperative reposition and fixation of bone fragments using plastic ty-raps. Materials and Methods. Ty-raps were sterilized before the surgery in the modes intended for the preparation of polymer products. After the fragments were dissected, their reposition and fixation are carried out with the help of clamps and bone clamps. At this stage, there is a need for the use of ty-raps, since the bone clamps prevent the plate from laying on the bone. To do this, 3-4 plastic ty-raps were applied to the areas of bone free from bone clamps in the area of the fragments contact. In those places where an intact periosteum and muscles are attached to the fragment, narrow transverse channels in soft tissues are formed with the instrument to wrap the bone with a ty-rap. Then the free end of the ty-rap is passed through its lock and tightened as much as possible. After tightening all the ty-raps, the bone clamps are removed. The applied ty-raps reliably keep the bone fragments from any displacement, even when the segment rotates. A bone plate is placed on the bone surface with tightened ty-raps. Then the plate fixed to the bone with screws. The plate should be placed on the bone without strong pressing, which allows you to remove the ty-raps from under the plate at any stage of osteosynthesis. The ty-raps are removed by cutting them with a scalpel or snacking with wire cutter, then the plate is fixed to the bone with the remaining screws. Conclusion. Ty-raps have many positive properties: they are affordable, cheap, do not lose their mechanical properties after sterilization, allow you to securely hold bone fragments during reposition, X-ray negative. The method has demonstrated convenience and reliability.ΠΠΊΡΡΠ°Π»ΡΠ½ΠΎΡΡΡ. ΠΠ°ΡΠ΅ΡΡΠ²ΠΎ ΡΠ΅ΠΏΠΎΠ·ΠΈΡΠΈΠΈ ΠΎΡΠ»ΠΎΠΌΠΊΠΎΠ² ΠΏΡΠΈ ΠΎΡΠΊΡΡΡΠΎΠΌ ΠΎΡΡΠ΅ΠΎΡΠΈΠ½ΡΠ΅Π·Π΅ ΡΠ²Π»ΡΠ΅ΡΡΡ ΠΎΠ΄Π½ΠΈΠΌ ΠΈΠ· Π²Π°ΠΆΠ½ΡΡ
ΡΠ°ΠΊΡΠΎΡΠΎΠ², ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΡΡΠΈΡ
ΠΈΡΡ
ΠΎΠ΄ Π»Π΅ΡΠ΅Π½ΠΈΡ. ΠΠ΅ΡΠ΅Π΄ΠΊΠΎ ΡΠ΅ΠΏΠΎΠ·ΠΈΡΠΈΡ ΠΈ ΡΠ΄Π΅ΡΠΆΠ°Π½ΠΈΠ΅ ΠΊΠΎΡΡΠ½ΡΡ
ΠΎΡΠ»ΠΎΠΌΠΊΠΎΠ² ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»ΡΡΡ ΡΠΎΠ±ΠΎΠΉ Π½Π΅ΠΏΡΠΎΡΡΡΡ Π·Π°Π΄Π°ΡΡ. ΠΠ²ΡΠΎΡΠ°ΠΌΠΈ ΠΏΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½ ΡΠΏΠΎΡΠΎΠ± ΡΠ΅ΠΏΠΎΠ·ΠΈΡΠΈΠΈ ΠΈ Π²ΡΠ΅ΠΌΠ΅Π½Π½ΠΎΠ³ΠΎ ΡΠ΄Π΅ΡΠΆΠ°Π½ΠΈΡ ΠΎΡΠ»ΠΎΠΌΠΊΠΎΠ² Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΏΠ»Π°ΡΡΠΈΠΊΠΎΠ²ΡΡ
Ρ
ΠΎΠΌΡΡΠΎΠ²-ΡΡΡΠΆΠ΅ΠΊ, ΠΈΡΠΏΠΎΠ»ΡΠ·ΡΠ΅ΠΌΡΡ
ΠΏΡΠΈ ΡΠ»Π΅ΠΊΡΡΠΎΠΌΠΎΠ½ΡΠ°ΠΆΠ½ΡΡ
ΡΠ°Π±ΠΎΡΠ°Ρ
. Π¦Π΅Π»Ρ ΠΏΡΠΎΠ΄Π΅ΠΌΠΎΠ½ΡΡΡΠΈΡΠΎΠ²Π°ΡΡ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΠΈ Π½ΠΎΠ²ΠΎΠ³ΠΎ ΡΠΏΠΎΡΠΎΠ±Π° ΠΈΠ½ΡΡΠ°ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΎΠ½Π½ΠΎΠΉ ΡΠ΅ΠΏΠΎΠ·ΠΈΡΠΈΠΈ ΠΈ ΡΠ΄Π΅ΡΠΆΠ°Π½ΠΈΡ ΠΊΠΎΡΡΠ½ΡΡ
ΠΎΡΠ»ΠΎΠΌΠΊΠΎΠ² ΠΏΡΠΈ ΠΏΠΎΠΌΠΎΡΠΈ ΠΏΠ»Π°ΡΡΠΈΠΊΠΎΠ²ΡΡ
Ρ
ΠΎΠΌΡΡΠΎΠ²-ΡΡΡΠΆΠ΅ΠΊ. ΠΠ°ΡΠ΅ΡΠΈΠ°Π» ΠΈ ΠΌΠ΅ΡΠΎΠ΄Ρ. Π₯ΠΎΠΌΡΡΡ-ΡΡΡΠΆΠΊΠΈ ΠΏΠ΅ΡΠ΅Π΄ ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠ΅ΠΉ ΠΏΠΎΠ΄Π²Π΅ΡΠ³Π°ΡΡ ΡΡΠ΅ΡΠΈΠ»ΠΈΠ·Π°ΡΠΈΠΈ Π² ΡΠ΅ΠΆΠΈΠΌΠ°Ρ
, ΠΏΡΠ΅Π΄Π½Π°Π·Π½Π°ΡΠ΅Π½Π½ΡΡ
Π΄Π»Ρ ΠΏΠΎΠ΄Π³ΠΎΡΠΎΠ²ΠΊΠΈ ΠΏΠΎΠ»ΠΈΠΌΠ΅ΡΠ½ΡΡ
ΠΈΠ·Π΄Π΅Π»ΠΈΠΉ. ΠΠΎΡΠ»Π΅ Π²ΡΠ΄Π΅Π»Π΅Π½ΠΈΡ ΠΎΡΠ»ΠΎΠΌΠΊΠΎΠ² ΠΎΡΡΡΠ΅ΡΡΠ²Π»ΡΡΡ ΠΈΡ
ΡΠ΅ΠΏΠΎΠ·ΠΈΡΠΈΡ ΠΈ ΡΠ΄Π΅ΡΠΆΠ°Π½ΠΈΠ΅ Ρ ΠΏΠΎΠΌΠΎΡΡΡ Π·Π°ΠΆΠΈΠΌΠΎΠ² ΠΈ ΠΊΠΎΡΡΠΎΠ΄Π΅ΡΠΆΠ°ΡΠ΅Π»Π΅ΠΉ. ΠΠ° ΡΡΠΎΠΌ ΡΡΠ°ΠΏΠ΅ ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΈ Π²ΠΎΠ·Π½ΠΈΠΊΠ°Π΅Ρ ΠΏΠΎΡΡΠ΅Π±Π½ΠΎΡΡΡ Π² ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠΈ Ρ
ΠΎΠΌΡΡΠΎΠ²-ΡΡΡΠΆΠ΅ΠΊ, ΡΠ°ΠΊ ΠΊΠ°ΠΊ ΠΊΠΎΡΡΠΎΠ΄Π΅ΡΠΆΠ°ΡΠ΅Π»ΠΈ ΠΏΡΠ΅ΠΏΡΡΡΡΠ²ΡΡΡ ΡΠΊΠ»Π°Π΄ΠΊΠ΅ ΠΏΠ»Π°ΡΡΠΈΠ½Ρ Π½Π° ΠΊΠΎΡΡΡ. ΠΠ»Ρ ΡΡΠΎΠ³ΠΎ Π½Π° ΡΠ²ΠΎΠ±ΠΎΠ΄Π½ΡΠ΅ ΠΎΡ ΠΊΠΎΡΡΠΎΠ΄Π΅ΡΠΆΠ°ΡΠ΅Π»Π΅ΠΉ ΡΡΠ°ΡΡΠΊΠΈ ΠΊΠΎΡΡΠΈ Π² ΠΎΠ±Π»Π°ΡΡΠΈ ΡΡΡΠΊΠΎΠ²ΠΊΠΈ ΠΎΡΠ»ΠΎΠΌΠΊΠΎΠ² Π½Π°ΠΊΠ»Π°Π΄ΡΠ²Π°ΡΡ 34 ΠΏΠ»Π°ΡΡΠΈΠΊΠΎΠ²ΡΡ
Ρ
ΠΎΠΌΡΡΠ°-ΡΡΡΠΆΠΊΠΈ. Π ΡΠ΅Ρ
ΠΌΠ΅ΡΡΠ°Ρ
, Π³Π΄Π΅ ΠΊ ΠΎΡΠ»ΠΎΠΌΠΊΡ ΠΏΡΠΈΠΊΡΠ΅ΠΏΠ»ΡΡΡΡΡ Π½Π΅ΠΏΠΎΠ²ΡΠ΅ΠΆΠ΄Π΅Π½Π½Π°Ρ Π½Π°Π΄ΠΊΠΎΡΡΠ½ΠΈΡΠ° ΠΈ ΠΌΡΡΡΡ, ΠΈΠ½ΡΡΡΡΠΌΠ΅Π½ΡΠΎΠΌ ΡΠΎΡΠΌΠΈΡΡΡΡ ΡΠ·ΠΊΠΈΠ΅ ΠΏΠΎΠΏΠ΅ΡΠ΅ΡΠ½ΡΠ΅ ΠΊΠ°Π½Π°Π»Ρ Π² ΠΌΡΠ³ΠΊΠΈΡ
ΡΠΊΠ°Π½ΡΡ
Π΄Π»Ρ ΠΎΠ±Ρ
Π²Π°ΡΡΠ²Π°Π½ΠΈΡ ΠΊΠΎΡΡΠΈ Ρ
ΠΎΠΌΡΡΠΎΠΌ. ΠΠ°ΡΠ΅ΠΌ ΡΠ²ΠΎΠ±ΠΎΠ΄Π½ΡΠΉ ΠΊΠΎΠ½Π΅Ρ Ρ
ΠΎΠΌΡΡΠ° ΠΏΡΠΎΠ²ΠΎΠ΄ΡΡ ΡΠ΅ΡΠ΅Π· Π΅Π³ΠΎ Π·Π°ΠΌΠΎΠΊ ΠΈ ΠΌΠ°ΠΊΡΠΈΠΌΠ°Π»ΡΠ½ΠΎ Π·Π°ΡΡΠ³ΠΈΠ²Π°ΡΡ. ΠΠΎΡΠ»Π΅ Π·Π°ΡΡΠ³ΠΈΠ²Π°Π½ΠΈΡ Π²ΡΠ΅Ρ
Ρ
ΠΎΠΌΡΡΠΎΠ² ΠΊΠΎΡΡΠΎΠ΄Π΅ΡΠΆΠ°ΡΠ΅Π»ΠΈ ΡΠ½ΠΈΠΌΠ°ΡΡ. ΠΠ°Π»ΠΎΠΆΠ΅Π½Π½ΡΠ΅ Ρ
ΠΎΠΌΡΡΡ Π½Π°Π΄Π΅ΠΆΠ½ΠΎ ΡΠ΄Π΅ΡΠΆΠΈΠ²Π°ΡΡ ΠΊΠΎΡΡΠ½ΡΠ΅ ΡΡΠ°Π³ΠΌΠ΅Π½ΡΡ ΠΎΡ ΠΊΠ°ΠΊΠΈΡ
-Π»ΠΈΠ±ΠΎ ΡΠΌΠ΅ΡΠ΅Π½ΠΈΠΉ Π΄Π°ΠΆΠ΅ ΠΏΡΠΈ ΡΠΎΡΠ°ΡΠΈΠΈ ΡΠ΅Π³ΠΌΠ΅Π½ΡΠ°. ΠΠΎΠ²Π΅ΡΡ
ΠΊΠΎΡΡΠΈ Ρ Π·Π°ΡΡΠ½ΡΡΡΠΌΠΈ Ρ
ΠΎΠΌΡΡΠ°ΠΌΠΈ-ΡΡΡΠΆΠΊΠ°ΠΌΠΈ ΡΠΊΠ»Π°Π΄ΡΠ²Π°ΡΡ Π½Π°ΠΊΠΎΡΡΠ½ΡΠΉ ΡΠΈΠΊΡΠ°ΡΠΎΡ. ΠΠ°ΡΠ΅ΠΌ ΡΠΈΠΊΡΠΈΡΡΡΡ ΠΏΠ»Π°ΡΡΠΈΠ½Ρ ΠΊ ΠΊΠΎΡΡΠΈ Π²ΠΈΠ½ΡΠ°ΠΌΠΈ. Π‘Π»Π΅Π΄ΡΠ΅Ρ ΡΠΊΠ»Π°Π΄ΡΠ²Π°ΡΡ ΠΏΠ»Π°ΡΡΠΈΠ½Ρ Π½Π° ΠΊΠΎΡΡΡ Π±Π΅Π· ΡΠΈΠ»ΡΠ½ΠΎΠ³ΠΎ ΠΏΡΠΈΠΆΠ°ΡΠΈΡ, ΡΡΠΎ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΠ΅Ρ ΡΠ΄Π°Π»ΡΡΡ Ρ
ΠΎΠΌΡΡΡ-ΡΡΡΠΆΠΊΠΈ ΠΈΠ·-ΠΏΠΎΠ΄ ΠΏΠ»Π°ΡΡΠΈΠ½Ρ Π½Π° Π»ΡΠ±ΠΎΠΌ ΡΡΠ°ΠΏΠ΅ ΠΎΡΡΠ΅ΠΎΡΠΈΠ½ΡΠ΅Π·Π°. Π‘ΡΡΠΆΠΊΠΈ ΡΠ΄Π°Π»ΡΡΡ, ΡΠ°Π·ΡΠ΅Π·Π°Ρ ΠΈΡ
ΡΠΊΠ°Π»ΡΠΏΠ΅Π»Π΅ΠΌ ΠΈΠ»ΠΈ ΠΏΠ΅ΡΠ΅ΠΊΡΡΡΠ²Π°Ρ ΠΊΡΡΠ°ΡΠΊΠ°ΠΌΠΈ, Π·Π°ΡΠ΅ΠΌ ΠΏΠ»Π°ΡΡΠΈΠ½Ρ Π·Π°ΠΊΡΠ΅ΠΏΠ»ΡΡΡ ΠΊ ΠΊΠΎΡΡΠΈ ΠΎΡΡΠ°Π²ΡΠΈΠΌΠΈΡΡ Π²ΠΈΠ½ΡΠ°ΠΌΠΈ. ΠΠ°ΠΊΠ»ΡΡΠ΅Π½ΠΈΠ΅. Π₯ΠΎΠΌΡΡΡ-ΡΡΡΠΆΠΊΠΈ ΠΎΠ±Π»Π°Π΄Π°ΡΡ ΠΌΠ½ΠΎΠ³ΠΈΠΌΠΈ ΠΏΡΠ΅ΠΈΠΌΡΡΠ΅ΡΡΠ²Π°ΠΌΠΈ: ΠΎΠ½ΠΈ Π΄ΠΎΡΡΡΠΏΠ½Ρ, Π΄Π΅ΡΠ΅Π²Ρ, Π½Π΅ ΡΠ΅ΡΡΡΡ ΡΠ²ΠΎΠΈΡ
ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ²ΠΎΠΉΡΡΠ² ΠΏΠΎΡΠ»Π΅ ΡΡΠ΅ΡΠΈΠ»ΠΈΠ·Π°ΡΠΈΠΈ, ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡΡ Π½Π°Π΄Π΅ΠΆΠ½ΠΎ ΡΠ΄Π΅ΡΠΆΠΈΠ²Π°ΡΡ ΠΎΡΠ»ΠΎΠΌΠΊΠΈ ΠΊΠΎΡΡΠ΅ΠΉ Π²ΠΎ Π²ΡΠ΅ΠΌΡ ΡΠ΅ΠΏΠΎΠ·ΠΈΡΠΈΠΈ, ΡΠ΅Π½ΡΠ³Π΅Π½ΠΎΠ½Π΅Π³Π°ΡΠΈΠ²Π½Ρ. ΠΠ΅ΡΠΎΠ΄ ΠΏΡΠΎΠ΄Π΅ΠΌΠΎΠ½ΡΡΡΠΈΡΠΎΠ²Π°Π» ΡΠ΄ΠΎΠ±ΡΡΠ²ΠΎ ΠΈ Π½Π°Π΄Π΅ΠΆΠ½ΠΎΡΡΡ
Π‘Π ΠΠΠΠΠΠΠ Π’Π ΠΠ₯ Π‘ΠΠΠ‘ΠΠΠΠ ΠΠΠ§ΠΠΠΠ― ΠΠΠ ΠΠΠΠΠΠ ΠΠ―Π’ΠΠ§ΠΠΠ ΠΠΠ‘Π’Π
Until now the problem of selecting a conservative or operative treatment option for calcaneal fractures and moreover the choice of the most optimal surgical procedure for such lesions have not been solved. Thus, comparative studies in this area is one of the most important tasks of the modern traumatology.Β Purpose of the study β to compare treatment outcomes, pattern and complications rate following the use of three treatment options for calcaneal fractures.Β Material and Methods. The authors analyzed treatment outcomes of 95 patients from 2013 till 2016. Mean age of patients was 39.04Β±12.51 years. Patients were divided into three groups: group 1 consisted of 41 patients with 54 fractures who underwent functional conservative treatment; group 2 consisted of 18 patients with 22 fractures treated by open reduction and plate fixation; group 3 consisted of 36 patients with 40 fractures treated by minimally invasive reduction and intramedullary fixation. Groups did not differ in respect of risk factors rate and rate of surgical risks under ABCDEF scale. Outcomes were evaluated basing on roentgenological criteria of reduction, complications rate and the functional scales FFI (Foot Function Index) and LEFS (Lower Extremity Functional Score).Β Results. Mean follow up was 20.8Β±9.0 months. Catamnesis was controlled in 68 out of 95 patients (71.6%). Variances were observed for all criteria of reduction quality between group 1 (no reduction) and groups 2 and 3. Groups 2 and 3 demonstrated similar criteria in respect of reduction quality of posterior articular surface, restoration of height and axis of calcaneus (Ρ0.05). FFI and LEFS scores in group 1 were inferior to results in groups 2 and 3 (Ρ0.05) at 6 and 12 months follow up. At 24 months follow up the variances persisted for mean values but were not statistically significant (Ρ0.05). No differences between groups 2 and 3 were observed during all follow up terms (Ρ0.05). Sum rate of complications in wound healing in group 2 was significantly higher than in groups 1 and 3 (Ρ = 0.033).Β Conclusion. Any of the described options of surgical treatment resulted in an earlier functional restoration after calcaneal fractures as compared to conservative treatment. Reduction quality and late functional outcomes did not vary between the study groups, however, the rate of complications for wound healing in the group with open internal fixation was higher.ΠΠΊΡΡΠ°Π»ΡΠ½ΠΎΡΡΡ. ΠΠΎΠΏΡΠΎΡΡ Π²ΡΠ±ΠΎΡΠ° ΠΊΠΎΠ½ΡΠ΅ΡΠ²Π°ΡΠΈΠ²Π½ΠΎΠ³ΠΎ ΠΈΠ»ΠΈ ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠ²Π½ΠΎΠ³ΠΎ Π»Π΅ΡΠ΅Π½ΠΈΡ ΠΏΡΠΈ ΠΏΠ΅ΡΠ΅Π»ΠΎΠΌΠ°Ρ
ΠΏΡΡΠΎΡΠ½ΠΎΠΉ ΠΊΠΎΡΡΠΈ, Π° ΡΠ΅ΠΌ Π±ΠΎΠ»Π΅Π΅ Π²ΡΠ±ΠΎΡΠ° ΠΎΠΏΡΠΈΠΌΠ°Π»ΡΠ½ΠΎΠ³ΠΎ ΠΌΠ΅ΡΠΎΠ΄Π° Ρ
ΠΈΡΡΡΠ³ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π»Π΅ΡΠ΅Π½ΠΈΡ ΡΡΠΈΡ
ΠΏΠ΅ΡΠ΅Π»ΠΎΠΌΠΎΠ², ΠΎΠΊΠΎΠ½ΡΠ°ΡΠ΅Π»ΡΠ½ΠΎ Π½Π΅ ΡΠ΅ΡΠ΅Π½Ρ. ΠΡΠΎΠ²Π΅Π΄Π΅Π½ΠΈΠ΅ ΡΡΠ°Π²Π½ΠΈΡΠ΅Π»ΡΠ½ΡΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ Π² ΡΡΠΎΠΉ ΠΎΠ±Π»Π°ΡΡΠΈ ΡΠ²Π»ΡΠ΅ΡΡΡ ΠΎΠ΄Π½ΠΎΠΉ ΠΈΠ· Π²Π°ΠΆΠ½ΡΡ
Π·Π°Π΄Π°Ρ ΡΠΎΠ²ΡΠ΅ΠΌΠ΅Π½-Π½ΠΎΠΉ ΡΡΠ°Π²ΠΌΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΠΈ.Β Π¦Π΅Π»Ρ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ β ΡΡΠ°Π²Π½ΠΈΡΡ ΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΠ΅ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ, Ρ
Π°ΡΠ°ΠΊΡΠ΅Ρ ΠΈ ΡΠ°ΡΡΠΎΡΡ ΠΎΡΠ»ΠΎΠΆΠ½Π΅Π½ΠΈΠΉ ΠΏΡΠΈ ΠΏΡΠΈΠΌΠ΅Π½Π΅-Π½ΠΈΠΈ ΡΡΠ΅Ρ
ΡΠΏΠΎΡΠΎΠ±ΠΎΠ² Π»Π΅ΡΠ΅Π½ΠΈΡ ΠΏΠ΅ΡΠ΅Π»ΠΎΠΌΠΎΠ² ΠΏΡΡΠΎΡΠ½ΠΎΠΉ ΠΊΠΎΡΡΠΈ.Β ΠΠ°ΡΠ΅ΡΠΈΠ°Π» ΠΈ ΠΌΠ΅ΡΠΎΠ΄Ρ. ΠΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Ρ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ Π»Π΅ΡΠ΅Π½ΠΈΡ 95 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ², ΠΏΡΠΎΡ
ΠΎΠ΄ΠΈΠ²ΡΠΈΡ
Π»Π΅ΡΠ΅Π½ΠΈΠ΅ Ρ 2013 ΠΏΠΎ 2016 Π³. Π‘ΡΠ΅Π΄Π½ΠΈΠΉ Π²ΠΎΠ·ΡΠ°ΡΡ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² ΡΠΎΡΡΠ°Π²ΠΈΠ» 39,04Β±12,51 Π»Π΅Ρ. ΠΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² ΡΠ°Π·Π΄Π΅Π»ΠΈΠ»ΠΈ Π½Π° ΡΡΠΈ Π³ΡΡΠΏΠΏΡ: Π³ΡΡΠΏΠΏΡ 1 ΡΠΎΡΡΠ°Π²ΠΈΠ»Β 41 ΠΏΠ°ΡΠΈΠ΅Π½Ρ Ρ 54 ΠΏΠ΅ΡΠ΅Π»ΠΎΠΌΠ°ΠΌΠΈ ΠΏΠΎΡΠ»Π΅ ΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΠΎΠ³ΠΎ ΠΊΠΎΠ½ΡΠ΅ΡΠ²Π°ΡΠΈΠ²Π½ΠΎΠ³ΠΎ Π»Π΅ΡΠ΅Π½ΠΈΡ; Π³ΡΡΠΏΠΏΡ 2 β 18 ΠΏΠ°ΡΠΈ-Π΅Π½ΡΠΎΠ² Ρ 22 ΠΏΠ΅ΡΠ΅Π»ΠΎΠΌΠ°ΠΌΠΈ ΠΏΠΎΡΠ»Π΅ ΠΎΡΠΊΡΡΡΠΎΠΉ ΡΠ΅ΠΏΠΎΠ·ΠΈΡΠΈΠΈ ΠΈ Π½Π°ΠΊΠΎΡΡΠ½ΠΎΠ³ΠΎ ΠΎΡΡΠ΅ΠΎΡΠΈΠ½ΡΠ΅Π·Π°; Π³ΡΡΠΏΠΏΡ 3 β 36 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Ρ 40 ΠΏΠ΅ΡΠ΅Π»ΠΎΠΌΠ°ΠΌΠΈ ΠΏΠΎΡΠ»Π΅ ΠΌΠΈΠ½ΠΈΠΈΠ½Π²Π°Π·ΠΈΠ²Π½ΠΎΠΉ ΡΠ΅ΠΏΠΎΠ·ΠΈΡΠΈΠΈ ΠΈ ΠΎΡΡΠ΅ΠΎΡΠΈΠ½ΡΠ΅Π·Π° ΡΡΠΈΡΡΠΎΠΌ. ΠΡΡΠΏΠΏΡ Π½Π΅ ΠΎΡΠ»ΠΈΡΠ°Π»ΠΈΡΡ ΠΏΠΎ ΡΠ°ΡΡΠΎΡΠ΅ Π²ΡΡΡΠ΅ΡΠ°Π΅ΠΌΠΎΡΡΠΈ ΡΠ°ΠΊΡΠΎΡΠΎΠ² ΡΠΈΡΠΊΠ° Π½Π΅Π±Π»Π°Π³ΠΎΠΏΡΠΈΡΡΠ½ΡΡ
ΠΈΡΡ
ΠΎΠ΄ΠΎΠ² ΠΈ ΡΡΠ΅ΠΏΠ΅Π½ΠΈ Ρ
ΠΈΡΡΡΠ³ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠΈΡΠΊΠ° ΠΏΠΎ ΡΠΊΠ°Π»Π΅ ABCDEF. ΠΡΠ΅Π½ΠΊΡ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΎΠ² ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄ΠΈΠ»ΠΈ Π½Π° ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΈΠΈ ΡΠ΅Π½ΡΠ³Π΅Π½ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΊΡΠΈΡΠ΅ΡΠΈΠ΅Π² ΡΠ΅ΠΏΠΎΠ·ΠΈΡΠΈΠΈ, ΡΠ°ΡΡΠΎΡΡ ΠΎΡΠ»ΠΎΠΆΠ½Π΅-Π½ΠΈΠΉ ΠΈ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Π΅ΠΉ ΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΡ
ΡΠΊΠ°Π» FFI (Foot Function Index) ΠΈ LEFS (Lower Extremity Functional Score).Β Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ. Π‘ΡΠ΅Π΄Π½ΠΈΠΉ ΡΡΠΎΠΊ Π½Π°Π±Π»ΡΠ΄Π΅Π½ΠΈΡ ΡΠΎΡΡΠ°Π²ΠΈΠ» 20,8Β±9,0 ΠΌΠ΅Ρ. ΠΠ°ΡΠ°ΠΌΠ½Π΅Π· ΠΎΡΡΠ»Π΅ΠΆΠ΅Π½ Ρ 68 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² ΠΈΠ· 95 (71,6%). Π Π°Π·Π½ΠΈΡΡ ΠΏΠΎ Π²ΡΠ΅ΠΌ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»ΡΠΌ ΠΊΠ°ΡΠ΅ΡΡΠ²Π° ΡΠ΅ΠΏΠΎΠ·ΠΈΡΠΈΠΈ Π½Π°Π±Π»ΡΠ΄Π°Π»ΠΈ ΠΌΠ΅ΠΆΠ΄Ρ Π³ΡΡΠΏΠΏΠΎΠΉ 1, Π³Π΄Π΅ ΡΠ΅ΠΏΠΎΠ·ΠΈΡΠΈΡ Π½Π΅ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»Π°ΡΡ, ΠΈ Π³ΡΡΠΏΠΏΠ°ΠΌΠΈ 2 ΠΈ 3 (Ρ0,05). ΠΡΡΠΏΠΏΡ 2 ΠΈ 3 Π±ΡΠ»ΠΈ ΠΎΠ΄ΠΈΠ½Π°ΠΊΠΎΠ²Ρ ΠΏΠΎ ΠΊΠ°ΡΠ΅ΡΡΠ²Ρ ΡΠ΅ΠΏΠΎΠ·ΠΈΡΠΈΠΈ Π·Π°Π΄Π½Π΅ΠΉ ΡΡΡΒ ΡΠ°Π²Π½ΠΎΠΉ ΠΏΠ»ΠΎΡΠ°Π΄ΠΊΠΈ, Π²ΠΎΡΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΈΡ Π²ΡΡΠΎΡΡ ΠΈ ΠΎΡΠΈ ΠΏΡΡΠΎΡΠ½ΠΎΠΉ ΠΊΠΎΡΡΠΈ (Ρ0,05). ΠΠΎΠΊΠ°Π·Π°ΡΠ΅Π»ΠΈ FFI ΠΈ LEFS Π² Π³ΡΡΠΏΠΏΠ΅ 1 ΡΡΡΡΠΏΠ°Π»ΠΈ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»ΡΠΌ Π² Π³ΡΡΠΏΠΏΠ°Ρ
2 ΠΈ 3 (Ρ0,05) Π½Π° ΡΡΠΎΠΊΠ°Ρ
6 ΠΈ 12 ΠΌΠ΅Ρ. ΠΠ° ΡΡΠΎΠΊΠ΅ Π² 24 ΠΌΠ΅Ρ. ΡΠ°Π·Π»ΠΈΡΠΈΡ ΡΠΎΡ
ΡΠ°Π½ΡΠ»ΠΈΡΡ Π² ΡΡΠ΅Π΄Π½ΠΈΡ
Π·Π½Π°ΡΠ΅Π½ΠΈΡΡ
, Π½ΠΎ Π½Π΅ Π±ΡΠ»ΠΈ ΡΡΠ°ΡΠΈΡΡΠΈΡΠ΅ΡΠΊΠΈ Π·Π½Π°ΡΠΈΠΌΡΠΌΠΈ (Ρ0,05). Π Π°Π·Π»ΠΈΡΠΈΠΉ ΠΌΠ΅ΠΆΠ΄Ρ Π³ΡΡΠΏΠΏΠ°ΠΌΠΈ 2 ΠΈ 3 Π½Π΅ Π²Ρ-ΡΠ²Π»Π΅Π½ΠΎ Π½Π° Π²ΡΠ΅Ρ
ΡΡΠΎΠΊΠ°Ρ
Π½Π°Π±Π»ΡΠ΄Π΅Π½ΠΈΡ (Ρ0,05). Π‘ΡΠΌΠΌΠ°ΡΠ½Π°Ρ ΡΠ°ΡΡΠΎΡΠ° ΠΎΡΠ»ΠΎΠΆΠ½Π΅Π½ΠΈΠΉ Π·Π°ΠΆΠΈΠ²Π»Π΅Π½ΠΈΡ ΡΠ°Π½Ρ Π² Π³ΡΡΠΏΠΏΠ΅ 2 Π±ΡΠ»Π° Π·Π½Π°ΡΠΈΠΌΠΎ Π²ΡΡΠ΅, ΡΠ΅ΠΌ Π² Π³ΡΡΠΏΠΏΠ°Ρ
1 ΠΈ 3 (Ρ = 0,033).Β ΠΡΠ²ΠΎΠ΄Ρ. ΠΠ°ΠΆΠ΄ΡΠΉ ΠΈΠ· ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Π½ΡΡ
Π²ΠΈΠ΄ΠΎΠ² ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠ²Π½ΠΎΠ³ΠΎ Π»Π΅ΡΠ΅Π½ΠΈΡ ΠΏΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Ρ ΠΊΠΎΠ½ΡΠ΅ΡΠ²Π°ΡΠΈΠ²Π½ΡΠΌ ΠΏΠΎ-Π·Π²ΠΎΠ»ΡΠ΅Ρ Π±ΡΡΡΡΠ΅Π΅ Π²ΠΎΡΡΡΠ°Π½ΠΎΠ²ΠΈΡΡ ΡΡΠ½ΠΊΡΠΈΡ ΠΏΠΎΡΠ»Π΅ ΠΏΠ΅ΡΠ΅Π»ΠΎΠΌΠ° ΠΏΡΡΠΎΡΠ½ΠΎΠΉ ΠΊΠΎΡΡΠΈ. ΠΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΠΌΠΈΠ½ΠΈΠΌΠ°Π»ΡΠ½ΠΎ ΠΈΠ½Π²Π°Π·ΠΈΠ²-Π½ΠΎΠΉ ΡΠ΅ΠΏΠΎΠ·ΠΈΡΠΈΠΈ ΠΈ ΠΎΡΡΠ΅ΠΎΡΠΈΠ½ΡΠ΅Π·Π° ΡΡΠΈΡΡΠΎΠΌ Π½Π΅ ΡΡΡΡΠΏΠ°Π΅Ρ ΠΏΠΎ ΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΠΌ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ°ΠΌ ΠΎΡΠΊΡΡΡΠΎΠΉ ΡΠ΅ΠΏΠΎΠ·ΠΈΡΠΈΠΈ ΠΈ Π½Π°ΠΊΠΎΡΡΠ½ΠΎΠΉ ΡΠΈΠΊΡΠ°ΡΠΈΠΈ, Π½ΠΎ Π½Π΅ΡΠ΅Ρ ΠΌΠ΅Π½ΡΡΠΈΠΉ ΡΠΈΡΠΊ ΠΎΡΠ»ΠΎΠΆΠ½Π΅Π½ΠΈΠΉ ΠΏΡΠΈ Π·Π°ΠΆΠΈΠ²Π»Π΅Π½ΠΈΠΈ ΡΠ°Π½Ρ
Vertex Operators for Closed Superstrings
We construct an iterative procedure to compute the vertex operators of the
closed superstring in the covariant formalism given a solution of IIA/IIB
supergravity. The manifest supersymmetry allows us to construct vertex
operators for any generic background in presence of Ramond-Ramond (RR) fields.
We extend the procedure to all massive states of open and closed superstrings
and we identify two new nilpotent charges which are used to impose the gauge
fixing on the physical states. We solve iteratively the equations of the vertex
for linear x-dependent RR field strengths. This vertex plays a role in studying
non-constant C-deformations of superspace. Finally, we construct an action for
the free massless sector of closed strings, and we propose a form for the
kinetic term for closed string field theory in the pure spinor formalism.Comment: TeX, harvmac, amssym.tex, 41 pp; references adde
Exponential distribution of long heart beat intervals during atrial fibrillation and their relevance for white noise behaviour in power spectrum
The statistical properties of heart beat intervals of 130 long-term surface
electrocardiogram recordings during atrial fibrillation (AF) are investigated.
We find that the distribution of interbeat intervals exhibits a characteristic
exponential tail, which is absent during sinus rhythm, as tested in a
corresponding control study with 72 healthy persons. The rate of the
exponential decay lies in the range 3-12 Hz and shows diurnal variations. It
equals, up to statistical uncertainties, the level of the previously uncovered
white noise part in the power spectrum, which is also characteristic for AF.
The overall statistical features can be described by decomposing the intervals
into two statistically independent times, where the first one is associated
with a correlated process with 1/f noise characteristics, while the second one
belongs to an uncorrelated process and is responsible for the exponential tail.
It is suggested to use the rate of the exponential decay as a further parameter
for a better classification of AF and for the medical diagnosis. The relevance
of the findings with respect to a general understanding of AF is pointed out
Instanton Calculations for N=1/ 2 super Yang-Mills Theory
We study (anti-) instantons in super Yang-Mills theories defined on a non
anticommutative superspace. The instanton solution that we consider is the same
as in ordinary SU(2) N=1 super Yang-Mills, but the anti-instanton receives
corrections to the U(1) part of the connection which depend quadratically on
fermionic coordinates, and linearly on the deformation parameter C. By
substituting the exact solution into the classical Lagrangian the topological
charge density receives a new contribution which is quadratic in C and quartic
in the fermionic zero-modes. The topological charge turns out to be zero. We
perform an expansion around the exact classical solution in presence of a
fermionic background and calculate the full superdeterminant contributing to
the one-loop partition function. We find that the one-loop partition function
is not modified with respect to the usual N=1 super Yang-Mills.Comment: 27 pages, harmvac, Redone the computation of topological charge, a
section has been rewritten and references adde
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