483 research outputs found
Accuracy of one-dimensional collision integral in the rigid spheres approximation
The accuracy of calculation of spectral line shapes in one-dimensional
approximation is studied analytically in several limiting cases for arbitrary
collision kernel and numerically in the rigid spheres model. It is shown that
the deviation of the line profile is maximal in the center of the line in case
of large perturber mass and intermediate values of collision frequency. For
moderate masses of buffer molecules the error of one-dimensional approximation
is found not to exceed 5%.Comment: LaTeX, 24 pages, 8 figure
Determining The Efficiency Of Online Learning Models
The study proposes a method for objectively determining the efficiency of online learning based on quantitative data generated by users while studying at online courses. Classifications of online learning models are researched and the efficiency of 4 common models in Ukraine is evaluated
Search for long lived heaviest nuclei beyond the valley of stability
The existence of long lived superheavy nuclei (SHN) is controlled mainly by
spontaneous fission and -decay processes. According to microscopic
nuclear theory, spherical shell effects at Z=114, 120, 126 and N=184 provide
the extra stability to such SHN to have long enough lifetime to be observed. To
investigate whether the so-called "stability island" could really exist around
the above Z, N values, the -decay half lives along with the spontaneous
fission and -decay half lives of such nuclei are studied. The
-decay half lives of SHN with Z=102-120 are calculated in a quantum
tunneling model with DDM3Y effective nuclear interaction using
values from three different mass formulae prescribed by Koura, Uno, Tachibana,
Yamada (KUTY), Myers, Swiatecki (MS) and Muntian, Hofmann, Patyk, Sobiczewski
(MMM). Calculation of spontaneous fission (SF) half lives for the same SHN are
carried out using a phenomenological formula and compared with SF half lives
predicted by Smolanczuk {\it et al}. Possible source of discrepancy between the
calculated -decay half lives of some nuclei and the experimental data
of GSI, JINR-FLNR, RIKEN are discussed. In the region of Z=106-108 with N
160-164, the -stable SHN is predicted to have
highest -decay half life () using
value from MMM. Interestingly, it is much greater than the recently measured
() of deformed doubly magic
nucleus. A few fission-survived long-lived SHN which are either -stable
or having large -decay half lives are predicted to exist near
, , and .
These nuclei might decay predominantly through -particle emission.Comment: 14 pages, 6 figures, 1 tabl
Alpha-decay lifetimes semiempirical relationship including shell effects
A new version of the semiempirical formula based on fission approach of alpha
decay is derived, by using the optimum values of the fitting parameters
determined for even-even nuclei, combined with hindrance factors for even-odd,
odd-even, and odd-odd nuclides. The deviations from experimental data for two
regions of nuclear chart (493 alpha emitters with Z=52-118 and 142 transuranium
nuclei including superheavies (Z=92-118), respectively) are compared with those
obtained by using the universal curve and the Viola-Seaborg semiempirical
relationship.Comment: 11 pages, 3 figures, revtex
A Note on the Cosmic Evolution of the Axion in a Strong Magnetic Field
It has been pointed out in the literature that in the presence of an external
magnetic field the axion mass receives an electromagnetic contribution. We show
that if a magnetic field with energy density larger than ~10^{-8} times the
energy density of the Universe existed at temperatures of a few GeV, that
contribution would be dominant and consequently the cosmic evolution of the
axion field would change substantially. In particular, the expected axion relic
abundance would be lowered, allowing a small relaxation of the present
cosmological bound on the Peccei-Quinn constant.Comment: 2 pages, no figures. Minor changes. References added. Accepted for
publication in JCA
N=2 Superconformal boundary states for free bosons and fermions
The most general N=2 superconformal boundary states for the c=3 theory
consisting of two (uncompactified) free bosons and fermions are constructed. It
is shown that the only N=2 boundary states are the familiar Dirichlet boundary
states, as well as the Neumann boundary states with an arbitrary electric
field.Comment: 20 pages, latex, references added, discussion of GSO projection
clarifie
A novel structure-aware sparse learning algorithm for brain imaging genetics
Brain imaging genetics is an emergent research field where the association between genetic variations such as single nucleotide polymorphisms (SNPs) and neuroimaging quantitative traits (QTs) is evaluated. Sparse canonical correlation analysis (SCCA) is a bi-multivariate analysis method that has the potential to reveal complex multi-SNP-multi-QT associations. Most existing SCCA algorithms are designed using the soft threshold strategy, which assumes that the features in the data are independent from each other. This independence assumption usually does not hold in imaging genetic data, and thus inevitably limits the capability of yielding optimal solutions. We propose a novel structure-aware SCCA (denoted as S2CCA) algorithm to not only eliminate the independence assumption for the input data, but also incorporate group-like structure in the model. Empirical comparison with a widely used SCCA implementation, on both simulated and real imaging genetic data, demonstrated that S2CCA could yield improved prediction performance and biologically meaningful findings
B-blockers, calcium antagonists, and mortality in stable coronary artery disease: An international cohort study
Aims:
The effect of first-line antianginal agents, Ξ²-blockers, and calcium antagonists on clinical outcomes in stable coronary artery disease (CAD) remains uncertain.
Methods and results
We analysed the use of Ξ²-blockers or calcium antagonists (baseline and annually) and outcomes in 22 006 stable CAD patients (enrolled 2009β2010) followed annually to 5βyears, in the CLARIFY registry (45 countries). Primary outcome was all-cause death. Secondary outcomes were cardiovascular death and the composite of cardiovascular death/non-fatal myocardial infarction (MI). After multivariable adjustment, baseline Ξ²-blocker use was not associated with lower all-cause death [1345 (7.8%) in users vs. 407 (8.4%) in non-users; hazard ratio (HR) 0.94, 95% confidence interval (CI) 0.84β1.06; Pβ=β0.30]; cardiovascular death [861 (5.0%) vs. 262 (5.4%); HR 0.91, 95% CI 0.79β1.05; Pβ=β0.20]; or cardiovascular death/non-fatal MI [1272 (7.4%) vs. 340 (7.0%); HR 1.03, 95% CI 0.91β1.16; Pβ=β0.66]. Sensitivity analyses according to Ξ²-blocker use over time and to prescribed dose produced similar results. Among prior MI patients, for those enrolled in the year following MI, baseline Ξ²-blocker use was associated with lower all-cause death [205 (7.0%) vs. 59 (10.3%); HR 0.68, 95% CI 0.50β0.91; Pβ=β0.01]; cardiovascular death [132 (4.5%) vs. 49 (8.5%); HR 0.52, 95% CI 0.37β0.73; Pβ=β0.0001]; and cardiovascular death/non-fatal MI [212 (7.2%) vs. 59 (10.3%); HR 0.69, 95% CI 0.52β0.93; Pβ=β0.01]. Calcium antagonists were not associated with any difference in mortality.
Conclusion
In this contemporary cohort of stable CAD, Ξ²-blocker use was associated with lower 5-year mortality only in patients enrolled in the year following MI. Use of calcium antagonists was not associated with superior mortality, regardless of history of MI
Classification of real three-dimensional Lie bialgebras and their Poisson-Lie groups
Classical r-matrices of the three-dimensional real Lie bialgebras are
obtained. In this way all three-dimensional real coboundary Lie bialgebras and
their types (triangular, quasitriangular or factorizable) are classified. Then,
by using the Sklyanin bracket, the Poisson structures on the related
Poisson-Lie groups are obtained.Comment: 17 page
Π ΠΏΡΠΎΠ±Π»Π΅ΠΌΠ΅ ΡΠ°Π΄ΠΈΠ°ΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΊΠ°Π½ΡΠ΅ΡΠΎΠ³Π΅Π½Π΅Π·Π° ΠΏΠΎΡΠ»Π΅ Π»Π΅ΡΠ΅Π½ΠΈΡ Π»ΠΈΠΌΡΠΎΠΌΡ Ρ ΠΎΠ΄ΠΆΠΊΠΈΠ½Π° ΠΈ ΠΎΡΡΡΠΎΠ³ΠΎ Π»ΠΈΠΌΡΠΎΠ±Π»Π°ΡΡΠ½ΠΎΠ³ΠΎ Π»Π΅ΠΉΠΊΠΎΠ·Π° Ρ Π΄Π΅ΡΠ΅ΠΉ ΠΈ ΠΏΠΎΠ΄ΡΠΎΡΡΠΊΠΎΠ²
Twenty-six cases with secondary malignant tumors in children and adolescents receiving treatment for Hodgkinβs lymphoma and acute lymphoblastic leukemia were analyzed. In all cases the lesion had developed in an area of previous radiation treatment. The interval between the primary treatment and secondary cancer development was from 3 to 29 years. The radiation therapy dose was from 12 to 45 Gy. Treatment of secondary cancer was successful only in 5 patients, the remaining patients died of disease progression. The risk of developing secondary cancer should be considered when planning treatment for patients with hemoblastosis. In cases with favorable prognosis (complete remission after induction chemotherapy and other signs of favorable prognosis) it is advisable to withhold radiation therapy as the most important risk factor for cancer.ΠΡΠΎΠ²Π΅Π΄Π΅Π½ Π°Π½Π°Π»ΠΈΠ· 26 ΡΠ»ΡΡΠ°Π΅Π² Π²ΡΠΎΡΡΡ
Π·Π»ΠΎΠΊΠ°ΡΠ΅ΡΡΠ²Π΅Π½Π½ΡΡ
ΠΎΠΏΡΡ
ΠΎΠ»Π΅ΠΉ Ρ Π΄Π΅ΡΠ΅ΠΉ ΠΈ ΠΏΠΎΠ΄ΡΠΎΡΡΠΊΠΎΠ², ΠΏΠΎΠ»ΡΡΠ°Π²ΡΠΈΡ
ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ½ΠΎΠ΅ Π»Π΅ΡΠ΅Π½ΠΈΠ΅ ΠΏΠΎ ΠΏΠΎ- Π²ΠΎΠ΄Ρ Π»ΠΈΠΌΡΠΎΠΌΡ Π₯ΠΎΠ΄ΠΆΠΊΠΈΠ½Π° ΠΈ ΠΎΡΡΡΠΎΠ³ΠΎ Π»ΠΈΠΌΡΠΎΠ±Π»Π°ΡΡΠ½ΠΎΠ³ΠΎ Π»Π΅ΠΉΠΊΠΎΠ·Π°. ΠΠΎ Π²ΡΠ΅Ρ
ΡΠ»ΡΡΠ°ΡΡ
ΠΎΠΏΡΡ
ΠΎΠ»ΠΈ ΡΠ°Π·Π²ΠΈΠ»ΠΈΡΡ Π² Π·ΠΎΠ½Π΅ Π±ΡΠ²ΡΠ΅Π³ΠΎ ΡΠ°Π΄ΠΈΠ°ΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΡ ΠΈΠ»ΠΈ ΠΏΠΎ ΠΊΡΠ°Ρ Π΅Π΅. ΠΠ½ΡΠ΅ΡΠ²Π°Π» ΠΌΠ΅ΠΆΠ΄Ρ ΠΏΠ΅ΡΠ²ΠΈΡΠ½ΡΠΌ Π»Π΅ΡΠ΅Π½ΠΈΠ΅ΠΌ ΠΈ ΡΠ°Π·Π²ΠΈΡΠΈΠ΅ΠΌ Π²ΡΠΎΡΠΎΠΉ ΠΎΠΏΡΡ
ΠΎΠ»ΠΈ ΡΠΎΡΡΠ°Π²ΠΈΠ» ΠΎΡ 3 Π΄ΠΎ 29 Π»Π΅Ρ, Π΄ΠΎΠ·Ρ Π»ΡΡΠ΅Π²ΠΎΠΉ ΡΠ΅ΡΠ°ΠΏΠΈΠΈ β ΠΎΡ 12 Π΄ΠΎ 45 ΠΡ. Π’ΠΎΠ»ΡΠΊΠΎ Ρ 5 Π±ΠΎΠ»ΡΠ½ΡΡ
Π»Π΅ΡΠ΅Π½ΠΈΠ΅ Π²ΡΠΎΡΠΎΠΉ ΠΎΠΏΡΡ
ΠΎΠ»ΠΈ Π±ΡΠ»ΠΎ ΡΡΠΏΠ΅ΡΠ½ΡΠΌ, ΠΎΡΡΠ°Π»ΡΠ½ΡΠ΅ ΡΠΌΠ΅ΡΠ»ΠΈ ΠΎΡ Π΅Π΅ ΠΏΡΠΎΠ³ΡΠ΅Ρ- ΡΠΈΡΠΎΠ²Π°Π½ΠΈΡ. Π ΠΈΡΠΊ ΡΠ°Π·Π²ΠΈΡΠΈΡ Π²ΡΠΎΡΠΎΠΉ ΠΎΠΏΡΡ
ΠΎΠ»ΠΈ Π΄ΠΎΠ»ΠΆΠ΅Π½ ΡΡΠΈΡΡΠ²Π°ΡΡΡΡ ΠΏΡΠΈ ΠΏΠ»Π°Π½ΠΈΡΠΎΠ²Π°Π½ΠΈΠΈ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ½ΠΎΠ³ΠΎ Π»Π΅ΡΠ΅Π½ΠΈΡ Π±ΠΎΠ»ΡΠ½ΡΡ
Π³Π΅ΠΌΠΎΠ±Π»Π°ΡΡΠΎΠ·Π°ΠΌΠΈ ΠΈ Π² ΡΠ»ΡΡΠ°ΡΡ
Π±Π»Π°Π³ΠΎΠΏΡΠΈΡΡΠ½ΠΎΠ³ΠΎ ΠΏΡΠΎΠ³Π½ΠΎΠ·Π° (Π΄ΠΎΡΡΠΈΠΆΠ΅Π½ΠΈΠ΅ ΠΏΠΎΠ»Π½ΠΎΠΉ ΡΠ΅ΠΌΠΈΡΡΠΈΠΈ Π² ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ΅ ΠΈΠ½Π΄ΡΠΊΡΠΈΠΎΠ½Π½ΠΎΠΉ Ρ
ΠΈΠΌΠΈΠΎΡΠ΅ΡΠ°ΠΏΠΈΠΈ, Π½Π°Π»ΠΈΡΠΈΠ΅ Π΄ΡΡΠ³ΠΈΡ
ΠΏΡΠΈΠ·Π½Π°ΠΊΠΎΠ² Π±Π»Π°Π³ΠΎΠΏΡΠΈΡΡΠ½ΠΎΠ³ΠΎ ΠΏΡΠΎΠ³Π½ΠΎΠ·Π°) ΡΠ΅Π»Π΅ΡΠΎΠΎΠ±ΡΠ°Π·Π½ΠΎ Π²ΠΎΠ·Π΄Π΅ΡΠΆΠΈΠ²Π°ΡΡΡΡ ΠΎΡ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΈΡ Π»ΡΡΠ΅Π²ΠΎΠΉ ΡΠ΅ΡΠ°ΠΏΠΈΠΈ ΠΊΠ°ΠΊ Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ ΠΊΠ°Π½ΡΠ΅ΡΠΎΠ³Π΅Π½Π½ΠΎΠ³ΠΎ ΡΠ°ΠΊΡΠΎΡΠ° Π² Π»Π΅ΡΠ΅Π±Π½ΠΎΠΌ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ΅
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