333 research outputs found
Role of electronic correlations in the Fermi surface formation of NaCoO
Band structure of metallic sodium cobaltate NaCoO (=0.33, 0.48,
0.61 0.72) has been investigated by local density approximation+Hubbard
(LDA+) method and within Gutzwiller approximation for the Co-
manifold. Correlation effects being taken into account results in suppression
of the hole pockets at the Fermi surface in agreement with recent
angle-resolved photo-emission spectroscopy (ARPES) experiments. In the
Gutzwiller approximation the bilayer splitting is significantly reduced due to
the correlation effects. The formation of high spin (HS) state in Co -shell
was shown to be very improbable.Comment: 6 pages, 2 figure
Two-instanton approximation to the Coulomb blockade problem
We develop the two-instanton approximation to the current-voltage
characteristic of a single electron transistor within the
Ambegaokar-Eckern-Sch\"on model. We determine the temperature and gate voltage
dependence of the Coulomb blockade oscillations of the conductance and the
effective charge. We find that a small (in comparison with the charging energy)
bias voltage leads to significant suppression of the Coulomb blockade
oscillations and to appearance of the bias-dependent phase shift
Charge relaxation resistance in the Coulomb blockade problem
We study the dissipation in a system consisting of a small metallic island
coupled to a gate electrode and to a massive reservoir via single tunneling
junction. The dissipation of energy is caused by a slowly oscillating gate
voltage. We compute it in the regimes of weak and strong Coulomb blockade. We
focus on the regime of not very low temperatures when electron coherence can be
neglected but quantum fluctuations of charge are strong due to Coulomb
interaction. The answers assume a particularly transparent form while expressed
in terms of specially chosen physical observables. We discovered that the
dissipation rate is given by a universal expression in both limiting cases.Comment: 21 pages, 12 figure
Basing factors for young innovative companies resulting from localization of foreign corporations
The relevance of our research is due to the fact that foreign corporationsβ technologies transfer is an efficient tool of achieving a high pace of economic development in Russia and its regions. Its success depends on the ability of economic actors to embrace innovations and their high innovative activity. The purpose of this study was the consideration of start-up factors of young innovative companies resulting from the localization of foreign corporationsβ technologies and the identification of conditions conducive to accelerating the diffusion of innovation in local markets. During the study of the specifics of Russian start-ups, with the use of the methods such as analysis of documents, content analysis, observation, expert interviews, the following hypothesis was identified and justified: the emergence of new markets for an already developed and functioning innovation makes it possible to intensify the process of establishing new enterprises in the domestic environment. The novelty of the scientific problem is to identify and substantiate the main conditions and factors affecting the creation of a non-pioneer young innovative company in the Russian regional economy based on the experience and technologies of foreign corporations, including learning state of the investment climate and areaβs business ecosystem. The article highlights the stages of transformation of business ideas of such enterprise into functioning business in a context of its design tools, such as: monitoring emerging consumer needs and turning them into business opportunities and business ideas; building business models, business planning. At this point the creation of a new organization is considered in conjunction with factors of regional economic environment. As a result of the survey there was developed theoretical and methodological basis of companiesβ localization based on the concept of lean production; there was proposed a stepwise mechanism involving a sequence of steps that must be made by young enterprises in order to effectively perform the diffusion of innovation.ΠΠΊΡΡΠ°Π»ΡΠ½ΠΎΡΡΡ ΡΠ΅ΠΌΡ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΠΎΠ±ΡΡΠ»ΠΎΠ²Π»Π΅Π½Π° ΡΠ΅ΠΌ, ΡΡΠΎ ΡΡΠ°Π½ΡΡΠ΅Ρ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ Π·Π°ΡΡΠ±Π΅ΠΆΠ½ΡΡ
ΠΊΠΎΡΠΏΠΎΡΠ°ΡΠΈΠΉ ΡΠ²Π»ΡΠ΅ΡΡΡ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΡΠΌ ΡΡΠ΅Π΄ΡΡΠ²ΠΎΠΌ, ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡΡΠΈΠΌ Π΄ΠΎΡΡΠΈΡΡ Π²ΡΡΠΎΠΊΠΈΡ
ΡΠ΅ΠΌΠΏΠΎΠ² ΡΠΊΠΎΠ½ΠΎΠΌΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠ°Π·Π²ΠΈΡΠΈΡ Π ΠΎΡΡΠΈΠΈ ΠΈ ΡΠ΅Π³ΠΈΠΎΠ½ΠΎΠ². ΠΠΎ Π΅Π³ΠΎ ΡΡΠΏΠ΅ΡΠ½ΠΎΡΡΡ ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ΅ΡΡΡ ΡΠΏΠΎΡΠΎΠ±Π½ΠΎΡΡΡΡ ΡΠΊΠΎΠ½ΠΎΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΡΠ±ΡΠ΅ΠΊΡΠΎΠ² Π²ΠΎΡΠΏΡΠΈΠ½ΠΈΠΌΠ°ΡΡ ΠΈΠ½Π½ΠΎΠ²Π°ΡΠΈΠΈ ΠΈ ΠΈΡ
Π²ΡΡΠΎΠΊΠΎΠΉ ΠΈΠ½Π½ΠΎΠ²Π°ΡΠΈΠΎΠ½Π½ΠΎΠΉ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΡΡ. Π¦Π΅Π»ΡΡ Π½Π°ΡΡΠΎΡΡΠ΅Π³ΠΎ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΡΡΠ°Π»ΠΎ ΡΠ°ΡΡΠΌΠΎΡΡΠ΅Π½ΠΈΠ΅ ΡΠ°ΠΊΡΠΎΡΠΎΠ² ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΈΡ ΠΌΠΎΠ»ΠΎΠ΄ΡΡ
ΠΈΠ½Π½ΠΎΠ²Π°ΡΠΈΠΎΠ½Π½ΡΡ
ΠΊΠΎΠΌΠΏΠ°Π½ΠΈΠΉ, Π²ΠΎΠ·Π½ΠΈΠΊΡΠΈΡ
Π² ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ΅ Π»ΠΎΠΊΠ°Π»ΠΈΠ·Π°ΡΠΈΠΈ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ Π·Π°ΡΡΠ±Π΅ΠΆΠ½ΡΡ
ΠΊΠΎΡΠΏΠΎΡΠ°ΡΠΈΠΉ ΠΈ Π²ΡΡΠ²Π»Π΅Π½ΠΈΠ΅ ΡΡΠ»ΠΎΠ²ΠΈΠΉ, ΡΠΏΠΎΡΠΎΠ±ΡΡΠ²ΡΡΡΠΈΡ
ΡΡΠΊΠΎΡΠ΅Π½ΠΈΡ Π΄ΠΈΡΡΡΠ·ΠΈΠΈ ΠΈΠ½Π½ΠΎΠ²Π°ΡΠΈΠΉ Π½Π° ΡΠ΅Π³ΠΈΠΎΠ½Π°Π»ΡΠ½ΡΡ
ΡΡΠ½ΠΊΠ°Ρ
. Π ΠΏΡΠΎΡΠ΅ΡΡΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΡΠΏΠ΅ΡΠΈΡΠΈΠΊΠΈ ΡΠΎΡΡΠΈΠΉΡΠΊΠΈΡ
ΡΡΠ°ΡΡΠ°ΠΏΠΎΠ² Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΡΠ°ΠΊΠΈΡ
ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ², ΠΊΠ°ΠΊ Π°Π½Π°Π»ΠΈΠ· Π΄ΠΎΠΊΡΠΌΠ΅Π½ΡΠΎΠ², ΠΊΠΎΠ½ΡΠ΅Π½Ρ-Π°Π½Π°Π»ΠΈΠ·, ΡΠΊΡΠΏΠ΅ΡΡΠ½ΡΠΉ ΠΎΠΏΡΠΎΡ Π°Π²ΡΠΎΡΠ°ΠΌΠΈ Π±ΡΠ»Π° Π²ΡΡΠ²Π»Π΅Π½Π° ΠΈ ΠΎΠ±ΠΎΡΠ½ΠΎΠ²Π°Π½Π° ΡΠ»Π΅Π΄ΡΡΡΠ°Ρ Π³ΠΈΠΏΠΎΡΠ΅Π·Π°: Π² ΠΎΡΠ΅ΡΠ΅ΡΡΠ²Π΅Π½Π½ΡΡ
ΡΡΠ»ΠΎΠ²ΠΈΡΡ
ΠΈΠΌΠ΅Π½Π½ΠΎ ΠΏΠΎΡΠ²Π»Π΅Π½ΠΈΠ΅ Π½ΠΎΠ²ΡΡ
ΡΡΠ½ΠΊΠΎΠ² ΡΠ±ΡΡΠ° Π΄Π»Ρ ΡΠΆΠ΅ ΠΎΡΠ²ΠΎΠ΅Π½Π½ΡΡ
ΠΈ ΡΡΠ½ΠΊΡΠΈΠΎΠ½ΠΈΡΡΡΡΠΈΡ
ΠΈΠ½Π½ΠΎΠ²Π°ΡΠΈΠΉ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΠ΅Ρ Π°ΠΊΡΠΈΠ²ΠΈΠ·ΠΈΡΠΎΠ²Π°ΡΡ ΠΏΡΠΎΡΠ΅ΡΡ ΡΠΎΠ·Π΄Π°Π½ΠΈΡ ΠΌΠΎΠ»ΠΎΠ΄ΡΡ
ΠΏΡΠ΅Π΄ΠΏΡΠΈΡΡΠΈΠΉ. ΠΠΎΠ²ΠΈΠ·Π½Π° Π½Π°ΡΡΠ½ΠΎΠΉ ΠΏΡΠΎΠ±Π»Π΅ΠΌΡ Π·Π°ΠΊΠ»ΡΡΠ°Π΅ΡΡΡ Π² Π²ΡΡΠ²Π»Π΅Π½ΠΈΠΈ ΠΈ ΠΎΠ±ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΈΠΈ ΠΎΡΠ½ΠΎΠ²Π½ΡΡ
ΡΡΠ»ΠΎΠ²ΠΈΠΉ ΠΈ ΡΠ°ΠΊΡΠΎΡΠΎΠ², ΠΎΠΊΠ°Π·ΡΠ²Π°ΡΡΠΈΡ
Π²Π»ΠΈΡΠ½ΠΈΠ΅ Π½Π° ΡΠΎΠ·Π΄Π°Π½ΠΈΠ΅ ΠΌΠΎΠ»ΠΎΠ΄ΡΡ
Π½Π΅ ΠΏΠΈΠΎΠ½Π΅ΡΡΠΊΠΈΡ
ΠΈΠ½Π½ΠΎΠ²Π°ΡΠΈΠΎΠ½Π½ΡΡ
ΠΊΠΎΠΌΠΏΠ°Π½ΠΈΠΉ Π² ΡΠΊΠΎΠ½ΠΎΠΌΠΈΠΊΠ΅ Π ΠΎΡΡΠΈΠΈ ΠΈ ΡΠ΅Π³ΠΈΠΎΠ½ΠΎΠ² Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ ΠΎΠΏΡΡΠ° ΠΈ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ Π·Π°ΡΡΠ±Π΅ΠΆΠ½ΡΡ
ΠΊΠΎΡΠΏΠΎΡΠ°ΡΠΈΠΉ, Ρ ΡΡΠ΅ΡΠΎΠΌ ΠΈΠ½Π²Π΅ΡΡΠΈΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΊΠ»ΠΈΠΌΠ°ΡΠ° ΠΈ ΠΏΡΠ΅Π΄ΠΏΡΠΈΠ½ΠΈΠΌΠ°ΡΠ΅Π»ΡΡΠΊΠΎΠΉ ΡΠΊΠΎΡΠΈΡΡΠ΅ΠΌΡ ΡΠ΅ΡΡΠΈΡΠΎΡΠΈΠΈ. Π ΡΡΠ°ΡΡΠ΅ Π²ΡΠ΄Π΅Π»Π΅Π½Ρ ΡΡΠ°Π΄ΠΈΠΈ ΡΡΠ°Π½ΡΡΠΎΡΠΌΠ°ΡΠΈΠΈ ΠΏΡΠ΅Π΄ΠΏΡΠΈΠ½ΠΈΠΌΠ°ΡΠ΅Π»ΡΡΠΊΠΎΠΉ ΠΈΠ΄Π΅ΠΈ ΡΠ°ΠΊΠΎΠ³ΠΎ ΠΏΡΠ΅Π΄ΠΏΡΠΈΡΡΠΈΡ Π² ΡΡΠ½ΠΊΡΠΈΠΎΠ½ΠΈΡΡΡΡΠΈΠΉ Π±ΠΈΠ·Π½Π΅Ρ Π² ΠΊΠΎΠ½ΡΠ΅ΠΊΡΡΠ΅ ΠΈΠ½ΡΡΡΡΠΌΠ΅Π½ΡΠΎΠ² Π΅Π³ΠΎ ΠΏΡΠΎΠ΅ΠΊΡΠΈΡΠΎΠ²Π°Π½ΠΈΡ, ΡΠ°ΠΊΠΈΡ
ΠΊΠ°ΠΊ ΠΌΠΎΠ½ΠΈΡΠΎΡΠΈΠ½Π³ Π²ΠΎΠ·Π½ΠΈΠΊΠ°ΡΡΠΈΡ
ΠΏΠΎΡΡΠ΅Π±Π½ΠΎΡΡΠ΅ΠΉ ΠΏΠΎΡΡΠ΅Π±ΠΈΡΠ΅Π»Π΅ΠΉ ΠΈ ΠΏΡΠ΅Π²ΡΠ°ΡΠ΅Π½ΠΈΠ΅ ΠΈΡ
Π² ΠΏΡΠ΅Π΄ΠΏΡΠΈΠ½ΠΈΠΌΠ°ΡΠ΅Π»ΡΡΠΊΠΈΠ΅ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΠΈ ΠΈ Π±ΠΈΠ·Π½Π΅Ρ-ΠΈΠ΄Π΅ΠΈ; ΠΏΠΎΡΡΡΠΎΠ΅Π½ΠΈΠ΅ Π±ΠΈΠ·Π½Π΅Ρ-ΠΌΠΎΠ΄Π΅Π»Π΅ΠΉ, Π±ΠΈΠ·Π½Π΅Ρ-ΠΏΠ»Π°Π½ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅. ΠΡΠΈ ΡΡΠΎΠΌ ΡΡΠ°ΠΏΡ ΡΠΎΠ·Π΄Π°Π½ΠΈΡ Π½ΠΎΠ²ΠΎΠΉ ΠΎΡΠ³Π°Π½ΠΈΠ·Π°ΡΠΈΠΈ ΡΠ°ΡΡΠΌΠ°ΡΡΠΈΠ²Π°ΡΡΡΡ Π²ΠΎ Π²Π·Π°ΠΈΠΌΠΎΡΠ²ΡΠ·ΠΈ Ρ ΡΠ°ΠΊΡΠΎΡΠ°ΠΌΠΈ ΡΠ΅Π³ΠΈΠΎΠ½Π°Π»ΡΠ½ΠΎΠΉ ΡΠΊΠΎΠ½ΠΎΠΌΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΡΠ΅Π΄Ρ. ΠΠΎ ΠΈΡΠΎΠ³Π°ΠΌ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ Π±ΡΠ»ΠΈ ΡΠ°Π·ΡΠ°Π±ΠΎΡΠ°Π½Ρ ΡΠ΅ΠΎΡΠ΅ΡΠΈΠΊΠΎ-ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΎΡΠ½ΠΎΠ²Ρ Π»ΠΎΠΊΠ°Π»ΠΈΠ·Π°ΡΠΈΠΈ ΠΊΠΎΠΌΠΏΠ°Π½ΠΈΠΉ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΊΠΎΠ½ΡΠ΅ΠΏΡΠΈΠΈ Π±Π΅ΡΠ΅ΠΆΠ»ΠΈΠ²ΠΎΠ³ΠΎ ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄ΡΡΠ²Π°; ΠΏΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½ Π΅Π΅ ΠΏΠΎΡΠ°Π³ΠΎΠ²ΡΠΉ ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌ, Π²ΠΊΠ»ΡΡΠ°ΡΡΠΈΠΉ ΠΏΠΎΡΠ»Π΅Π΄ΠΎΠ²Π°ΡΠ΅Π»ΡΠ½ΠΎΡΡΡ ΡΡΠ°ΠΏΠΎΠ², ΠΊΠΎΡΠΎΡΡΠ΅ Π½Π΅ΠΎΠ±Ρ
ΠΎΠ΄ΠΈΠΌΠΎ ΠΏΡΠΎΠΉΡΠΈ ΠΌΠΎΠ»ΠΎΠ΄ΠΎΠΌΡ ΠΏΡΠ΅Π΄ΠΏΡΠΈΡΡΠΈΡ Π΄Π»Ρ ΡΠΎΠ³ΠΎ, ΡΡΠΎΠ±Ρ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎ ΡΠΎΠ²Π΅ΡΡΠΈΡΡ Π΄ΠΈΡΡΡΠ·ΠΈΡ ΠΈΠ½Π½ΠΎΠ²Π°ΡΠΈΠΈ; ΡΠ°ΡΠΊΡΡΡΡ ΡΡΠ»ΠΎΠ²ΠΈΡ, ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡΡΠΈΠ΅ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎ ΡΠΎΠ·Π΄Π°Π²Π°ΡΡ Π½ΠΎΠ²ΡΠ΅ ΠΏΡΠ΅Π΄ΠΏΡΠΈΡΡΠΈΡ Π·Π° ΡΡΠ΅Ρ Π΄ΠΈΡΡΡΠ·ΠΈΠΈ ΠΈΠ½Π½ΠΎΠ²Π°ΡΠΈΠΉ
Transformations in the grain boundary ensemble of M1 copper subjected to equal-channel angular pressing during recrystallization annealing
The grain structure of M1 copper subjected to equal-channel angular pressing (ECAP) and subsequent annealing at 593K for 1 h is studied by means of transmission electron microscopy and scanning electron microscopy with the diffraction of backscattered electron
Itinerant in-plane magnetic fluctuations and many-body correlations in NaCoO
Based on the {\it ab-initio} band structure for NaCoO we derive the
single-electron energies and the effective tight-binding description for the
bands using projection procedure. Due to the presence of the
next-nearest-neighbor hoppings a local minimum in the electronic dispersion
close to the point of the first Brillouin zone forms. Correspondingly,
in addition to a large Fermi surface an electron pocket close to the
point emerges at high doping concentrations. The latter yields the new
scattering channel resulting in a peak structure of the itinerant magnetic
susceptibility at small momenta. This indicates dominant itinerant in-plane
ferromagnetic fluctuations above certain critical concentration , in
agreement with neutron scattering data. Below the magnetic susceptibility
shows a tendency towards the antiferromagnetic fluctuations. We further analyze
the many-body effects on the electronic and magnetic excitations using various
approximations applicable for different ratio.Comment: 10 page
Quasiparticle states of the Hubbard model near the Fermi level
The spectra of the t-U and t-t'-U Hubbard models are investigated in the
one-loop approximation for different values of the electron filling. It is
shown that the four-band structure which is inherent in the case of
half-filling and low temperatures persists also for some excess or deficiency
of electrons. Besides, with some departure from half-filling an additional
narrow band of quasiparticle states arises near the Fermi level. The dispersion
of the band, its bandwidth and the variation with filling are close to those of
the spin-polaron band of the t-J model. For moderate doping spectral
intensities in the new band and in one of the inner bands of the four-band
structure decrease as the Fermi level is approached which leads to the
appearance of a pseudogap in the spectrum.Comment: 8 pages, 7 figure
Electronic theory for itinerant in-plane magnetic fluctuations in NaCoO
Starting from {\it ab-initio} band structure for NaCoO, we derive the
single-electron energies and the effective tight-binding description for the
bands using a projection procedure. We find that due to the presence
of the next-nearest-neighbor hoppings a local minimum in the electronic
dispersion close to the point of the first Brillouin zone forms.
Therefore, in addition to a large Fermi surface an electron pocket close to the
point emerges at high doping concentrations. The latter yields the new
scattering channel resulting in a peak structure of the itinerant magnetic
susceptibility at small momenta. This indicates itinerant in-plane
ferromagnetic state above certain critical concentration , in agreement
with neutron scattering data. Below the magnetic susceptibility shows a
tendency towards the antiferromagnetic fluctuations. We estimate the value of
within the rigid band model and within the Hubbard model
with infinite on-site Coulomb repulsion consistent with the experimental phase
diagram.Comment: 4 pages, 4 figures; LDA calculations were done with Na in the
symmetric 2d position contrary to the 6h position in a previous version of
this pape
The problem of "macroscopic charge quantization" in single-electron devices
In a recent Letter by the authors [I.S. Burmistrov and A.M.M. Pruisken, Phys.
Rev. Lett. 101, 056801 (2008)] it was shown that single-electron devices
(single electron transistor or SET) display "macroscopic charge quantization"
which is completely analogous to the quantum Hall effect observed on very
different electron systems. In this investigation we present more detail on
these new findings. Based on the Ambegaokar-Eckern-Schoen (AES) theory of the
Coulomb blockade we introduce a general response theory that probes the
sensitivity of SET to changes in the boundary conditions. This response theory
defines a new set of physical observables and we establish the contact with the
standard results obtained from ordinary linear response theory. The response
parameters generally define the renormalization behavior of the SET in the
entire regime from weak coupling with large values of the tunneling conductance
all the way down to the strong coupling phase where the system displays the
Coulomb blockade. We introduce a general criterion for charge quantization that
is analogous to the Thouless criterion for Anderson localization. We present
the results of detailed computations on the weak coupling side of the theory,
i.e. both perturbative and non-perturbative (instantons). Based on an effective
theory in terms of quantum spins we study the quantum critical behavior of the
AES model on the strong coupling side. Consequently, a unifying scaling diagram
of the SET is obtained. This diagram displays all the super universal
topological features of the theta-angle concept that previously arose in the
theory of the quantum Hall effect.Comment: RevTex, 22 pages, 10 figure
Parameters of the Effective Singlet-Triplet Model for Band Structure of High- Cuprates by Different Approaches
The present paper covers the problem of parameters determination for
High- superconductive copper oxides. Different approaches, {\it ab initio}
LDA and LDA+U calculations and Generalized Tight-Binding (GTB) method for
strongly correlated electron systems, are used to calculate hopping and
exchange parameters of the effective singlet-triplet model for -layer.
The resulting parameters are in remarkably good agreement with each other and
with parameters extracted from experiment. This set of parameters is proposed
for proper quantitative description of physics of hole doped High-
cuprates in the framework of effective models.Comment: PACS 74.72.h; 74.20.z; 74.25.Jb; 31.15.A
- β¦