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1.
On the effect of a magnetic field on the yield point and kinetics of macroplasticity in LiF crystals
A strong effect of a static magnetic field B on active deformation kinetics (
=const) in LiF crystals is observed. This is a threshold effect with respect to B and
; it is observed only for B> B
c
(B≃0.4 T) and
. Magnetic sensitivity is exhibited by the yield stress τ
y
, which decreases by approximately a factor of 1.5 for B=0.48 T, and by the stage-II and stage-III hardening coefficients θII and θ III, the former decreasing and the latter increasing in a magnetic field. A physical interpretation is proposed for the observed
behavior.
Pis’ma Zh. éksp. Teor. Fiz. 65, No. 6, 470–474 (25 March 1997) 相似文献
2.
The difference between the quantity
induced by box diagram and the experimentally measured value of ɛ is determined and used to obtain the value of ∈ with high precision. Present-day knowledge of CKM matrix elements (including
B-factory data) allows us to obtain from the SM expression for
the value of parameter B
K
: B
K
=0.89±0.16. It turns out to be very close to the result of vacuum insertion, B
K
=1.
The text was submitted by the authors in English. 相似文献
3.
H. Q. Lu L. M. Shen P. Ji G. F. Ji N. J. Sun 《International Journal of Theoretical Physics》2003,42(4):837-844
In this paper we consider the classical Euclidean wormhole solution of the Born—Infeld scalar field. The corresponding classical Euclidean wormhole solution can be obtained analytically for both very small and large
. At the extreme limit of small
the wormhole solution has the same format as one obtained by Giddings and Strominger (Nuclear Physics B
306, 890, 1988). At the extreme limit of large
the wormhole solution is a new one. The wormhole wave functions can also be obtained for both very small and large
. These wormhole wave functions are regarded as solutions of quantum-mechanical Wheeler—Dewitt equation with certain boundary conditions. 相似文献
4.
5.
6.
7.
Using the self-consistent pseudopotential method, we have calculated the binding energy of the image states for the (0001)
, and
surfaces of beryllium. It is shown for the (0001) face that there exists a pronounced resonance image state with n=1 and energy −0.95 eV at the point
of the surface Brillouin zone. In the
surface, which has a wide band gap in the vicinity of the vacuum level, the calculated image state with n=1 at the point
has energy −1.2 eV and is a surface state of gap type. For the
face in the vicinity of the point
band gaps are absent. However, the symmetry of the bulk states near the vacuum level enables the existence of a resonance
image state with n=1 and energy −0.6 eV.
Fiz. Tverd. Tela (St. Petersburg) 41, 935–940 (June 1999) 相似文献
8.
Given a simple, simply laced, complex Lie algebra
corresponding to the Lie group G, let
be thesubalgebra generated by the positive roots. In this Letter we construct aBV algebra
whose underlying graded commutative algebra is given by the cohomology, with respect to
, of the algebra of regular functions on G with values in
. We conjecture that
describes the algebra of allphysical (i.e., BRST invariant) operators of the noncritical
string. The conjecture is verified in the two explicitly known cases,
2 (the Virasoro string) and
3 (the
string). 相似文献
9.
We examine the absorption and amplification bands of a weak probe signal in the presence of Bose-Einstein condensation of
excitons that emerges in nonequilibrium conditions in the field of coherent laser radiation with a wave vector k
0. We assume that the detuning
from resonance between the energy ħω
ex
(k
0)+L
0 of the exciton level, which is shifted because of exciton-exciton interaction, and the laser photon energy ħω
L
, is generally nonzero. The elementary excitation spectrum consisting of the quasiexcitonic and quasienergy branches determines
the optical properties of the system. When there is real induced Bose-Einstein condensation, at
the two branches touch, as they do in spontaneous Bose-Einstein condensation. In virtual induced Bose-Einstein condensation,
when
, instabilities emerge in the spectrum in certain regions of the k-space. These instabilities are caused by a real transformation of two laser photons into two extracondensate particles. Nonequilibrium
extracondensate excitons strongly affect the absorption and amplification of the probe light signal. We show that light absorption
is due to the quantum transition from the ground state of the crystal to the quasiexcitonic branch of the spectrum. On the
other hand, amplification of the signal is caused by the transition from the quasienergy branch to the ground state of the
crystal. The same transition can be explained by a real transformation of two laser photons into a vacuum photon of frequency
ħcq and a crystal exciton with a wave vector 2k
0−q. Finally, we show that the excitonic absorption and light-amplification bands are essentially anisotropic at
and depend on the orientation of the vectors q and k
0.
Zh. éksp. Teor. Fiz. 112, 167–179 (July 1997) 相似文献
10.
Explicit evaluation of the following parameters has been carried out in the extraU (1) superstring inspired model: (i) As Mz2 varies from 555 GeV to 620 GeV and (m
t) CDF = 175.6 ± 5.7 GeV (Table 1): (a) SNew varies from -0.100 ± 0.089 to -0.130 ± 0.090, (b) TNew varies from -0.098 ± 0.097 to -0.129 ± 0.098, (c) UNew varies from -0.229 ± 0.177 to -0.253 ± 0.206, (d) Τz varies from 2.487 ± 0.027 to 2.486 ± 0.027, (e) ALR varies from 0.0125 ± 0.0003 to 0.0126 ± 0.0003, (f) A
FB
b
remains constant at 0.0080 ± 0.0007. Almost identical values are obtained for (m
t)D0 = 169 GeV (see table 2). (ii) Triple gauge boson vertices (TGV) contributions: AsMz
2 varies from 555 GeV to 620 GeV and (m
t) CDF = 175.6 ±5.7 GeV. (a)√s = 500 GeV, asymptotic case:
varies from -0.301 to -0.179;
varies from -0.622 to -0.379;
varies from +0.0061 to 0.0056;
varies from -3.691 to -2.186.
varies from +0.270 to +0.118;
varies from +0.552 to 0.238;
varies from +0.0004 to +0.0002;
remains constant at -0.110. (b)√s = 700 GeV, asymptotic case:
varies from -0.297 to -0.176;
varies from -0.609 to -0.370;
varies from -0.0082 to -0.0078;
varies from -3.680 to -2.171.√s = 700 GeV, nonasymptotic case:
varies from -0.173 to -0.299;
varies from-0.343 to -0.591;
varies from -0.005 to -0.011;
remains constant at -0.110.
The pattern of form factors values for√s = 1000, 1200 GeV is almost identical to that of√s= 700 GeV. Further the values of the form factors for (m
t)D0 (=169 GeV) follow identical pattern as that of (m
t) CDF form factors values (see tables 5, 6, 9, 10).
We conclude that the values of all the form factors with the exception of these of
,
are comparable or larger than theS, T values and therefore the TGV contributions are important while deciding the use of extraU (1) model for doing physics beyond standard model. 相似文献
11.
12.
Dephasing in open quantum chaotic systems has been investigated in the limit of large system sizes to the Fermi wavelength
ratio, L/λF 〉 1. The weak localization correction g
wl to the conductance for a quantum dot coupled to (i) an external closed dot and (ii) a dephasing voltage probe is calculated
in the semiclassical approximation. In addition to the universal algebraic suppression g
wl ∝ (1 + τD/τϕ)−1 with the dwell time τD through the cavity and the dephasing rate τ
ϕ
−1
, we find an exponential suppression of weak localization by a factor of ∝ exp[−
/τϕ], where
is the system-dependent parameter. In the dephasing probe model,
coincides with the Ehrenfest time,
∝ ln[L/λF], for both perfectly and partially transparent dot-lead couplings. In contrast, when dephasing occurs due to the coupling
to an external dot,
∝ ln[L/ξ] depends on the correlation length ξ of the coupling potential instead of λF.
The text was submitted by the authors in English. 相似文献
13.
R N Mohapatra 《Pramana》2006,67(5):783-791
See-saw mechanism has been a dominant paradigm in the discussion of neutrino masses. We discuss how this idea can be tested
via a baryon number violating process such as N-
oscillation. Since the expected see-saw scale is high and the N-
amplitude goes like M
R
−5
, one might think that this process is not observable in realistic see-saw models for neutrino masses. In this talk I show
that in supersymmetric models, the above conclusion is circumvented leading to an enhanced and observable rate for N
oscillation. I also discuss a new mechanism for baryogenesis in generic models for neutron-anti-neutron oscillation. 相似文献
14.
We consider the Dirichlet Laplacian for astrip in
with one straight boundary and a width
, where $f$ is a smooth function of acompact support with a length 2b. We show that in the criticalcase,
, the operator has nobound statesfor small
.On the otherhand, a weakly bound state existsprovided
. In thatcase, there are positive c
1,c
2 suchthat the corresponding eigenvalue satisfies
for all
sufficiently small. 相似文献
15.
N. M. Agababyan V. V. Ammosov M. Atayan N. Grigoryan H. Gulkanyan A. A. Ivanilov Zh. Karamyan V. A. Korotkov 《Physics of Atomic Nuclei》2006,69(1):35-38
The influence of nuclear effects on the production of neutral strange particles (V
0) is investigated using the data obtained with SKAT propane-freon bubble chamber irradiated in the neutrino beam (with E
v
=3−30 GeV) at the Serpukhov accelerator. The mean multiplicity of V
0 particles in nuclear interactions,
, is found to exceed significantly that in “quasideuteron” interactions,
. The ratio of
is larger than that for π− mesons,
. It is shown that the multiplicity gain of V
0 particles can be explained by intranuclear interactions of produced pions.
The text was submitted by the authors in English. 相似文献
16.
Let
be the Haag--Kastler net generated by the
(2) chiral current algebra at level 1. We classify the SL(2,
)-covariant subsystems
by showing that they are all fixed points nets
H
for some subgroup H of the gauge automorphisms group SO(3) of
. Then, using the fact that the net
1 generated by the
(1) chiral current can be regarded as a subsystem of
, we classify the subsystems of
1. In this case, there are two distinct proper subsystems: the one generated by the energy-momentum tensor and the gauge invariant subsystem
. 相似文献
17.
N. M. Panyunin 《Russian Journal of Mathematical Physics》2007,14(4):501-504
In the note, a Smolyanov-Shavgulidze model of infinite-dimensional superspace H
Λ = Λ0
H
0 ⊕ Λ1
H
1 corresponding to a Hilbert space H = H
0 ⊕ H
1 over a Hilbert superalgebra Λ = Λ0 ⊕ Λ1 is considered. Its relation to the Khrennikov superspace is discussed. Moreover, H
Λ is equipped with the structure of Hilbert superspace with an inner superproduct (·, ·)Λ. The supermeasures are defined as Λℂ
(∧H
1)-valued measures on H
0 (Λℂ stands for the complexification of Λ). The definition of the Fourier supertransform is similar to the ordinary one,
(y) =
μ(dz). It turns out that the values of the Fourier supertransform of a supermeasure on the subspace
= H
0 ⊕ Λ1
H
1 can be obtained by applying a certain operator to the values of the classical Fourier transform. The main result is the theorem
claiming that the Fourier supertransform of supermeasures is isometric on superspaces with zero even part (H
0 = {0}). As a corollary, we note that the operator of Fourier supertransform is injective. We also give necessary and sufficient
conditions for the countable additivity of cylindrical supermeasures in terms of continuity of their Fourier supertransforms
(an analog of the Minlos-Sazonov theorem). 相似文献
18.
Carl M. Bender 《Czechoslovak Journal of Physics》2006,56(9):1047-1062
In this paper, two independent methods are used to show that the non-Hermitian
-symmetric wrong-sign quartic Hamiltonian H = (1/2m)p
2 − gx
4 is exactly equivalent to the conventional Hermitian Hamiltonian
. First, this equivalence is demonstrated by using elementary differential-equation techniques and second, it is demonstrated
by using functional-integration methods. As the linear term in the Hermitian Hamiltonian
is proportional to ℏ, this term is anomalous; that is, the linear term in the potential has no classical analog. The anomaly
is a consequence of the broken parity symmetry of the original non-Hermitian
-symmetric Hamiltonian. The anomaly term in
remains unchanged if an x
2 term is introduced into H. When such a quadratic term is present in H, this Hamiltonian possesses bound states. The corresponding bound states in
are a direct physical measure of the anomaly. If there were no anomaly term, there would be no bound states. 相似文献
19.
Ersan Demiralp 《Czechoslovak Journal of Physics》2005,55(9):1081-1084
We have investigated bound state solutions of the Schrodinger equation for one-dimensional harmonic oscillator potential together
with even number of Dirac delta functions. These point interactions are located at symmetric points x = x
i
and x = −x
i
(i = 1, 2,..., N) and they have complex conjugate strengths
and
, respectively. We present explicit forms of eigenfunctions and an algebraic eigenvalue equation and numerical solutions for
this
-symmetric Hamiltonian.
Presented at the 3rd International Workshop “Pseudo-Hermitian Hamiltonians in Quantum Physics”, Istanbul, Turkey, June 20–22,
2005. 相似文献
20.
Yu. M. Andreev S. I. Bityukov N. V. Krasnikov A. N. Toropin 《Physics of Atomic Nuclei》2007,70(10):1717-1724
The LHC (CMS) discovery potential in the search for supersymmetry and lepton-flavor violation in neutralino decays using the
e
± μ∓ + E
T
miss
signature is studied. A detailed study is done for the CMS test points LM1-LM9. It is shown that, for the point LM1, it is
possible to detect lepton-flavor violation in neutralino decays with lepton-flavor-violating branching Br(
→ μ±
e
∓
) ≥ 0.04 Br(
→ e
+
e
−
, μ+ μ−
) for an integral luminosity of 10 fb−1. The discovery potential in the mSUGRA-SUSY scenario with tan β = 10, sgn(μ) = + in the (m
0, m
1/2) plane using the e
± μ∓ + E
T
miss
signature is determined.
The text was submitted by the authors in English. 相似文献