3,515 research outputs found
Self-Consistent Tensor Product Variational Approximation for 3D Classical Models
We propose a numerical variational method for three-dimensional (3D)
classical lattice models. We construct the variational state as a product of
local tensors, and improve it by use of the corner transfer matrix
renormalization group (CTMRG), which is a variant of the density matrix
renormalization group (DMRG) applied to 2D classical systems. Numerical
efficiency of this approximation is investigated through trial applications to
the 3D Ising model and the 3D 3-state Potts model.Comment: 12 pages, 6 figure
Microstructure and mechanical properties of hip-consolidated Rene 95 powders
The effects of heat-treatments on the microstructure of P/M Rene 95 (a nickel-based powder metal), consolidated by the hot-isostatic pressing (HIP), were examined. The microstructure of as-HIP'd specimen was characterized by highly serrated grain boundaries. Mechanical tests and microstructural observations reveal that the serrated grain boundaries improved ductility at both room and elevated temperatures by retarding crack propagation along grain boundaries
Numerical Latent Heat Observation of the q=5 Potts Model
Site energy of the five-state ferromagnetic Potts model is numerically
calculated at the first-order transition temperature using corner transfer
matrix renormalization group (CTMRG) method. The calculated energy of the
disordered phase is clearly different from that of the ordered phase
. The obtained latent heat is 0.027, which
quantitatively agrees with the exact solution.Comment: 2 pages, Latex(JPSJ style files are included), 2 ps figures,
submitted to J. Phys. Soc. Jpn.(short note
The Density Matrix Renormalization Group technique with periodic boundary conditions
The Density Matrix Renormalization Group (DMRG) method with periodic boundary
conditions is introduced for two dimensional classical spin models. It is shown
that this method is more suitable for derivation of the properties of infinite
2D systems than the DMRG with open boundary conditions despite the latter
describes much better strips of finite width. For calculation at criticality,
phenomenological renormalization at finite strips is used together with a
criterion for optimum strip width for a given order of approximation. For this
width the critical temperature of 2D Ising model is estimated with seven-digit
accuracy for not too large order of approximation. Similar precision is reached
for critical indices. These results exceed the accuracy of similar calculations
for DMRG with open boundary conditions by several orders of magnitude.Comment: REVTeX format contains 8 pages and 6 figures, submitted to Phys. Rev.
Polymorphisms in the 5β²-UTR of PTEN and other gene polymorphisms in normal Japanese individuals
Polymorphisms are distributed differently in populations, including those of regions, ethnic groups, and diseased patients. In order to investigate variation in nucleotide sequences in normal individuals, we isolated genomic DNA from the blood of healthy Japanese individuals and sequenced the 5'-untranslated region (5'- UTR) of the phosphatase and tensin homolog deleted on chromosome 10 (PTEN) gene and the gene promoter, intron, and exon nucleotides of p53, p14ARF, murine double minute 2 (MDM2), and the Ξ²2- and Ξ²3-adrenoceptor (-AR). We found polymorphisms in these regions, including a deletion at positions β465 to β463 and a substitution at position β404 in PTEN and a substitution at position β4924 in p14ARF, in normal individuals. Individuals with or without the PTEN polymorphism harbored a different distribution of polymorphisms, including simultaneous alterations in nucleotides of p53, MDM2, and Ξ²3-AR, and also harbored some polymorphic nucleotides located in the same set of associatively altered nucleotides. Our results show that multiple nucleotides, including the PTEN nucleotides, are altered in normal Japanese individuals and provide useful information for genotyping studies in individuals and populations.ΠΠΎΠ»ΠΈΠΌΠΎΡΡΠΈΠ·ΠΌΡ ΡΠΈΡΠΎΠΊΠΎ ΡΠ°ΡΠΏΡΠΎΡΡΡΠ°Π½Π΅Π½Ρ Π² ΠΏΠΎΠΏΡΠ»ΡΡΠΈΡΡ
, Π²ΠΊΠ»ΡΡΠ°Ρ ΡΠ΅Π³ΠΈΠΎΠ½Ρ, ΡΡΠ½ΠΈΡΠ΅ΡΠΊΠΈΠ΅ Π³ΡΡΠΏΠΏΡ ΠΈ Π±ΠΎΠ»ΡΠ½ΡΡ
ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ². ΠΠ»Ρ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΠΈΠ·ΠΌΠ΅Π½ΡΠΈΠ²ΠΎΡΡΠΈ Π½ΡΠΊΠ»Π΅ΠΎΡΠΈΠ΄Π½ΡΡ
ΠΏΠΎΡΠ»Π΅Π΄ΠΎΠ²Π°ΡΠ΅Π»ΡΠ½ΠΎΡΡΠ΅ΠΉ Ρ Π½ΠΎΡΠΌΠ°Π»ΡΠ½ΡΡ
ΠΈΠ½Π΄ΠΈΠ²ΠΈΠ΄ΠΎΠ² , ΠΌΡ Π²ΡΠ΄Π΅Π»ΠΈΠ»ΠΈ Π³Π΅Π½ΠΎΠΌΠ½ΡΡ ΠΠΠ ΠΈΠ· ΠΊΡΠΎΠ²ΠΈ Π·Π΄ΠΎΡΠΎΠ²ΡΡ
ΡΠΏΠΎΠ½ΡΠ΅Π² ΠΈ ΡΠ΅ΠΊΠ²Π΅Π½ΠΈΡΠΎΠ²Π°Π»ΠΈ 5β²-Π½Π΅ΡΡΠ°Π½ΡΠ»ΠΈΡΡΠ΅ΠΌΡΠΉ ΡΡΠ°ΡΡΠΎΠΊ (5β²-UTR) Π³Π΅Π½Π° ΡΠΎΡΡΠ°ΡΠ°Π·Ρ ΠΈ Π³ΠΎΠΌΠΎΠ»ΠΎΠ³Π° ΡΠ΅Π½Π·ΠΈΠ½Π° (PTEN), ΠΏΡΠΎΠΌΠΎΡΠΎΡΠ½ΡΠ΅ ΠΏΠΎΡΠ»Π΅Π΄ΠΎΠ²Π°ΡΠ΅Π»ΡΠ½ΠΎΡΡΠΈ, ΠΈΠ½ΡΡΠΎΠ½Ρ ΠΈ ΡΠΊΠ·ΠΎΠ½Ρ Π³Π΅Π½ΠΎΠ² p53 ΠΈ p14ARF, ΠΈΠ½Π³ΠΈΠ±ΠΈΡΠΎΡΠ° ΡΡΠΏΡΠ΅ΡΡΠΎΡΠ° ΠΎΠΏΡΡ
ΠΎΠ»Π΅Π²ΠΎΠ³ΠΎ ΡΠΎΡΡΠ° p53 (MDM2) ΠΈ Π³Π΅Π½ΠΎΠ² Ξ²2- and Ξ²3-Π°Π΄ΡΠ΅Π½ΠΎΡΠ΅ΡΠ΅ (-AR). ΠΡ ΠΎΠ±Π½Π°ΡΡΠΆΠΈΠ»ΠΈ ΠΏΠΎΠ»ΠΈΠΌΠΎΡΡΠΈΠ·ΠΌ ΠΏΠΎ ΡΡΠΈΠΌ ΡΡΠ°ΡΡΠΊΠ°ΠΌ, Π²ΠΊΠ»ΡΡΠ°Ρ Π΄Π΅Π»Π΅ΡΠΈΡ Π² ΠΏΠΎΠ»ΠΎΠΆΠ΅Π½ΠΈΠΈ Ρ β465 to β463 ΠΈ Π·Π°ΠΌΠ΅Π½Ρ Π² ΠΏΠΎΠ»ΠΎΠΆΠ΅Π½ΠΈΠΈ β404 Π² PTEN ΠΈ Π·Π°ΠΌΠ΅Π½Ρ Π² ΠΏΠΎΠ»ΠΎΠΆΠ΅Π½ΠΈΠΈ β4924 Π² p14ARF Ρ Π½ΠΎΡΠΌΠ°Π»ΡΠ½ΡΡ
ΠΈΠ½Π΄ΠΈΠ²ΠΈΠ΄ΠΎΠ². ΠΠ½Π΄ΠΈΠ²ΠΈΠ΄Ρ Ρ ΠΈ Π±Π΅Π· ΠΏΠΎΠ»ΠΈΠΌΠΎΡΡΠΈΠ·ΠΌΠ° PTEN ΠΈΠΌΠ΅Π»ΠΈ ΡΠ°Π·Π»ΠΈΡΠ½ΠΎΠ΅ ΡΠ°ΡΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ ΠΏΠΎΠ»ΠΈΠΌΠΎΡΡΠΈΠ·ΠΌΠ°, Π²ΠΊΠ»ΡΡΠ°Ρ ΠΎΠ΄Π½ΠΎΠ²ΡΠ΅ΠΌΠ΅Π½Π½ΡΠ΅ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ Π² Π½ΡΠΊΠ»Π΅ΠΎΡΠΈΠ΄Π°Ρ
p53, MDM2 ΠΈ 3-AR, ΠΈ ΡΠ°ΠΊΠΆΠ΅ ΠΈΠΌΠ΅Π»ΠΈ ΠΏΠΎΠ»ΠΈΠΌΠΎΡΡΠ½ΡΠ΅ Π½ΡΠΊΠ»Π΅ΠΎΡΠΈΠ΄Ρ, Π»ΠΎΠΊΠ°Π»ΠΈΠ·ΠΎΠ²Π°Π½Π½ΡΠ΅ Π² ΡΠΎΠΌ ΠΆΠ΅ Π½Π°Π±ΠΎΡΠ΅ ΡΠΎΠ²ΠΌΠ΅ΡΡΠ½ΠΎ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½Π½ΡΡ
Π½ΡΠΊΠ»Π΅ΠΎΡΠΈΠ΄ΠΎΠ². ΠΠ°ΡΠΈ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΏΠΎΠΊΠ°Π·ΡΠ²Π°ΡΡ, ΡΡΠΎ ΠΌΠ½ΠΎΠΆΠ΅ΡΡΠ²Π΅Π½Π½ΡΠ΅ Π½ΡΠΊΠ»Π΅ΠΎΡΠΈΠ΄Ρ, Π²ΠΊΠ»ΡΡΠ°Ρ Π½ΡΠΊΠ»Π΅ΠΎΡΠΈΠ΄Ρ PTEN, ΠΈΠ·ΠΌΠ΅Π½Π΅Π½Ρ Ρ Π½ΠΎΡΠΌΠ°Π»ΡΠ½ΡΡ
ΡΠΏΠΎΠ½ΡΠΊΠΈΡ
ΠΈΠ½Π΄ΠΈΠ²ΠΈΠ΄ΠΎΠ² ΠΈ Π΄Π°ΡΡ ΠΏΠΎΠ»Π΅Π·Π½ΡΡ ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΡ Π΄Π»Ρ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ ΠΏΠΎ Π³Π΅Π½ΠΎΡΠΈΠΏΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΈΠ½Π΄ΠΈΠ²ΠΈΠ΄ΠΎΠ² ΠΈ ΠΏΠΎΠΏΡΠ»ΡΡΠΈΠΉ
Incommensurate structures studied by a modified Density Matrix Renormalization Group Method
A modified density matrix renormalization group (DMRG) method is introduced
and applied to classical two-dimensional models: the anisotropic triangular
nearest- neighbor Ising (ATNNI) model and the anisotropic triangular
next-nearest-neighbor Ising (ANNNI) model. Phase diagrams of both models have
complex structures and exhibit incommensurate phases. It was found that the
incommensurate phase completely separates the disordered phase from one of the
commensurate phases, i. e. the non-existence of the Lifshitz point in phase
diagrams of both models was confirmed.Comment: 14 pages, 14 figures included in text, LaTeX2e, submitted to PRB,
presented at MECO'24 1999 (Wittenberg, Germany
Macroscopic nucleation phenomena in continuum media with long-range interactions
Nucleation, commonly associated with discontinuous transformations between
metastable and stable phases, is crucial in fields as diverse as atmospheric
science and nanoscale electronics. Traditionally, it is considered a
microscopic process (at most nano-meter), implying the formation of a
microscopic nucleus of the stable phase. Here we show for the first time, that
considering long-range interactions mediated by elastic distortions, nucleation
can be a macroscopic process, with the size of the critical nucleus
proportional to the total system size. This provides a new concept of
"macroscopic barrier-crossing nucleation". We demonstrate the effect in
molecular dynamics simulations of a model spin-crossover system with two
molecular states of different sizes, causing elastic distortions.Comment: 12 pages, 4 figures. Supplementary information accompanies this paper
at http://www.nature.com/scientificreport
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