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1.
G. T. Kazakov A. V. Kozhevnikov Yu. A. Filimonov 《Journal of Experimental and Theoretical Physics》1999,88(1):174-181
This paper describes an experimental study of variations of the dispersion and damping of magnetostatic surface waves in ferrite
films, caused by three-and four-magnon interactions with parametric spin waves excited by an auxiliary surface magnetostatic
pump wave with frequency f
p. The variations in the dispersion and damping were identified, respectively, with variations Δk″ in the real part and Δk′ in the imaginary part of the wave number of the surface magnetostatic wave. The Δk″ and Δk′ values were determined from the ratio of the changes of the phase increment Δφ and the amplitude increment ΔA of the surface magnetostatic wave to the length L of the nonequilibrium section of the film, where the parametric spin waves exist. It is found that, when three-magnon decay
processes are allowed for the pump wave and the surface magnetostatic probe wave, the probe wave can substantially alter the
distribution of the parametric spin waves in the film.
Zh. éksp. Teor. Fiz. 115, 318–332 (January 1999) 相似文献
2.
The four-magnon instability of magnetostatic surface waves (MSSWs) in yttrium iron garnet epitaxial films is investigated
experimentally. It is shown that four-magnon instability for MSSWs with wave numbers 30–600 cm−1 is a decay instability and develops for values of the wave magnetization close to the threshold level for second-order parametric
instability of a homogeneous transverse pump wave. When the supercriticality of the MSSW power is 15–20 dB, the generated
parametric spin waves themselves become unstable with respect to the four-magnon interaction, so that kinetic instability
develops in the film. It is shown that the pump signal transmitted through the signal and the length of the “nonlinear” part
of the film, where a MSSW is capable of exciting parametric spin waves, increase as the pump power is increased.
Fiz. Tverd. Tela (St. Petersburg) 38, 330–338 (February 1997) 相似文献
3.
Effects of the resonant Bragg scattering of magnetostatic backward volume waves on the periodic structure of a conductive
meander pattern with an alternating current are analyzed theoretically and compared with experiment. It is shown that unlike
a static grating, a dynamic grating causes a frequency shift of the scattered wave. It is proposed that this phenomenon be
utilized for effective control of the intermodal conversion of magnetostatic waves.
Zh. Tekh. Fiz. 68, 105–112 (May 1998) 相似文献
4.
A theoretical study is made of the trajectories and of the changes in magnitude and direction of the wave vectors of magnetostatic
backward surface waves with different frequencies propagating in ferrite-insulator-metal structures with different insulating
layer thicknesses and magnetized by a linearly nonuniform static field. It is shown that both forward and backward magnetostatic
surface waves (MSSWs) propagate in a waveguide channel, on one side of which MSSWs undergo mirror reflection and on the other
side of which their propagation direction is rotated, independently of the thickness of the insulator in the structure. It
is shown that when MSSWs propagate in a nonuniform field, the forward wave is converted into a backward wave and, under certain
conditions, the backward wave is converted into a forward wave. Some features of the propagation characteristics of magnetostatic
backward surface waves are determined.
Zh. Tekh. Fiz. 69, 70–77 (February 1999) 相似文献
5.
G.A. Melkov V.I. Vasyuchka A.V. Chumak A.N. Slavin 《Journal of magnetism and magnetic materials》2006
The wave front reversal (WFR) of non-reciprocal waves has been investigated. The experiment was performed using surface magnetostatic waves (SMSW) excited by a pulsed microwave signal of the carrier frequency ∼4.7 GHz in an epitaxial yttrium–iron garnet (YIG) film. The WFR was realized by pulsed parametric pumping of a double frequency. It was shown that WFR with high efficiency can be achieved for SMSW having relatively small wavenumbers k∼102 rad/cm. 相似文献
6.
A noncascading terahertz (THz) wave parametric oscillator synchronously pumped by a mode-locked picosecond Ti:sapphire laser whose average power was less than 1 W was demonstrated with a noncollinear phase-matching MgO:LiNbO3 crystal in an external enhancement cavity doubly resonant for both pump (780 nm) and signal (781-784 nm) waves. In the external cavity, in which the pump wave enhanced so as to reduce the pumping threshold of parametric processes, the signal wave could also resonate and thus be enhanced simultaneously, resulting in a THz wave output at approximately 0.9 THz as the idler wave. The novel dual enhancement of pump and signal waves reduced the threshold pumping intensity to approximately 50 MW/cm2, which was much lower than that of a conventional externally pumped THz wave parametric oscillator with a crystal. 相似文献
7.
Yu. V. Gulyaev P. E. Zil’berman A. V. Lugovskoi 《Journal of Experimental and Theoretical Physics》1997,84(1):109-119
The equations of motion for the slowly varying complex amplitudes of spin waves parametrically excited by a localized pumping
magnetic field have been derived. A solution of these equations satisfying given boundary and initial conditions has been
obtained. The energy dissipated by spin waves decreases with the pumping intensity beyond a certain pumping power, which can
be termed the regeneration threshold. The losses vanish and change sign at the instability threshold. Both thresholds depend
heavily on the linear dimension L of the pumping zone, increasing with decreasing L. Owing to the regeneration process, the dissipation length of spin waves increases without bound as the pumping power approaches
the instability threshold. Consequently, perturbations of a uniform state due to the boundary penetrate throughout the pumping
zone, regardless of the dimension L. As a result, the full pattern of parametric instability is strongly affected by the zone boundary: 1) the spatial distribution
of wave amplitudes becomes nonuniform everywhere inside the zone; 2) the amplitude growth rate in the unstable regime decreases
at all points when perturbations due to the boundary reach these points; 3) the instability threshold is independent of the
spin-wave frequency offset from the parametric resonance frequency. The calculated minimum instability threshold as a function
of the bias magnetic field (the “butterfly” curve) changes shape with L, in agreement with the available experimental data.
Zh. éksp. Teor. Fiz. 111, 199–219 (January 1997) 相似文献
8.
S. L. Vysotskii G. T. Kazakov Yu. A. Filimonov A. V. Maryakhin 《Technical Physics》1998,43(7):834-845
The influence of exchange coupling of layers on the propagation of magnetostatic dipole volume waves in normally and tangentially
magnetized two-layer epitaxial ferrite structures is investigated. It is shown that the indicated influence is manifested
in the form of dynamic spin pinning effects on the interlayer boundary and formation of a common dipole-exchange wave spectrum
for the entire structure. In this case, at the synchronism frequencies of the dipole and exchange waves the losses of the
dipole waves grow and anomalous segments appear in the dispersion. In films magnetized in the “hard” direction relative to
the axis of normal uniaxial surface anisotropy the magnetostatic dipole volume waves can interact resonantly with the surface
spin waves supported by the boundaries with pinned spins.
Zh. Tekh. Fiz. 68, 97–110 (July 1998) 相似文献
9.
A. R. Muratov 《Journal of Experimental and Theoretical Physics》1997,85(5):887-897
A theory of parametric excitation of acoustic waves is constructed. It is shown that nonlinear attenuation is the main restriction
mechanism for a parametrically generated sound wave. The intensity of generated waves is directly proportional to the difference
ε between the value of pumping and bare attenuation. The calculated proportionality coefficient depends on the shape of the
generated sound wave. Why an ordinary pattern does not form for acoustic waves is explained. The structure of the spectrum
of excited waves was studied. It is shown that this structure has exponential asymptotic behavior at the frequency. The width
of the intensity distribution depends on the shape of a wave. For different cases it behaves as ε
α with α=1, 8/7, and 4/3. The results are compared with the experimental data of Ref. 5.
Zh. éksp. Teor. Fiz. 112, 1630–1648 (November 1997)
Published in English in the original Russian journal. Reproduced here with stylistic changes by the Translation Editor. 相似文献
10.
Magnetostatic surface waves with fixed frequency and wave vector are predicted to exist in a ferromagnet with an inhomogeneity
of the magnetic anisotropy such that the spectral function has a turning point on the surface. This result is most important
for the case when an external magnetic field magnetizes the ferromagnet perpendicular to its surface. The frequency of the
surface wave is determined by the frequency of the magnetostatic volume wave at the surface of the ferromagnet, and the wave
vector is determined by the surface values of the local magnetic anisotropy field and its derivative.
Zh. Tekh. Fiz. 68, 118–123 (June 1998) 相似文献
11.
V. N. Chukov 《Physics of the Solid State》1997,39(2):233-239
The problem of the scattering of a Rayleigh wave by a surface inhomogeneity of the mass density of an isotropic solid is solved
in the Born approximation of perturbation theory. The inhomogeneity is statistical with a Gaussian correlation function in
the plane parallel to the surface and is deterministic with an exponentially decaying dependence on the coordinate perpendicular
to the surface. Expressions are derived for the displacement fields in the scattered longitudinal (P), transverse (SV and
SH), and Rayleigh (R) waves at large distances from the inhomogeneity. The Rayleigh wave energy scattering coefficients are
calculated as functions of the wavelength λ, the correlation length a of the inhomogeneity, the depth d of the defective layer, and the Poisson ratio of the medium, σ. The angular distribution of the scattered Rayleigh wave energy is determined. Asymptotic expressions are obtained for the
scattering coefficient in various limiting cases with respect to the parameters a/λ and λ/d. The relation between the energies in the scattered P, SV, SH, and R waves is established. The resulting equations are used
to calculate the scattering coefficients numerically over a wide range of variation of the parameters a/λ, λ/d, and σ; the results are presented in the form of graphs and a table. A physical pattern of the scattering process is constructed
and used as a basis for interpreting the results of the study.
Fiz. Tverd. Tela (St. Petersburg) 39, 267–274 (February 1997) 相似文献
12.
The field distribution of magnetostatic surface and volume waves as they propagate at an arbitrary angle to a constant field
in a tangentially magnetized ferromagnetic slab (Damon-Eschbach waves) is investigated. Snapshots of the magnetic field lines
of the wave are constructed. The variation of the magnetic field distribution with thickness is qualitatively identified for
a volume wave as it propagates at an angle equal to the cutoff angle of the surface wave, as a result of which the sinusoidal
profile of the wave over thickness almost discontinuously acquires an additional phase difference.
Zh. Tekh. Fiz. 69, 82–86 (January 1999) 相似文献
13.
14.
Guang S. He Yiping Cui Paras N. Prasad 《Journal of Experimental and Theoretical Physics》1997,85(5):850-856
The spectral structure of backward stimulated scattering from a 10 cm-long CS2-liquid cell is investigated by using Q-switched 10-ns and 532-nm laser pulses with different spectral linewidths. Under a narrow spectral line (∼0.1 cm−1) pump condition, very strong sharp lines near the pump wavelength (λ
0) position and the first-order stimulated Raman scattering (λ
s1) position can be observed. However, under a wide line (≈1 cm−1) pump condition, only a strong and superbroadening spectral band can be observed mainly in the red-shift side of the pump
wavelength. The different spectral features under these two conditions can be explained by a competition between stimulated
Brillouin, Raman, and Rayleigh-Kerr scattering. Under both pump conditions, the broadening spectral distributions are not
consistent with the predictions given by stimulated Rayleigh-wing scattering theories, but can be interpreted well utilizing
the theoretical model of stimulated Rayleigh-Kerr scattering.
Zh. éksp. Teor. Fiz. 112, 1563–1573 (November 1997)
Published in English in the original Russian journal. Reproduced here with stylistic changes by the Translation Editor. 相似文献
15.
The use of incoherent multiwave pump radiation or randomly varying magnetostatic fields (stochastic undulators) for improving
the energy conversion efficiency in free-electron lasers based on stimulated wave scattering and the stimulated undulator
emission of relativistic electron beams is proposed. It is shown within the quasilinear approximation that the electronic
efficiency increases in proportion to the width of the pump spectrum due to enrichment of the spectrum of combination waves
which are synchronous with the electron beam and realization of a mechanism of stochastic particle deceleration when the signal
wave is monochromatic. At the same time, the efficiency scarcely depends on the spread of the beam parameters, making the
use of the method promising for improving the efficiency of free-electron lasers powered by intense relativistic electron
beams.
Zh. Tekh. Fiz. 67, 77–81 (July 1997) 相似文献
16.
The possibility of the existence of a magnetostatic analog of Love surface elastic waves is predicted. They appear in situations
where the conditions for the existence of magnetostatic volume waves hold in the upper layer of a ferromagnetic bilayer, but
not in the lower layer.
Zh. Tekh. Fiz. 68, 85–90 (October 1998) 相似文献
17.
Bound states and critical behavior of the Yukawa potential 总被引:1,自引:0,他引:1
We investigate the bound states of the Yukawa potential V (r)=−λexp(−αr)/r, using different algorithms: solving the Schr?dinger equation numerically and our Monte Carlo Hamiltonian approach. There
is a critical α = αC, above which no bound state exists. We study the relation between αC and λ for various angular momentum quantum number l, and find in atomic units, αC(l) = λ[A
1 exp(−l/B
1) + A
2 exp(−l/B
2)], with A
1 = 1.020(18), B
1 = 0.443(14), A
2 = 0.170(17), and B
2 = 2.490(180). 相似文献
18.
M. Hosseini Farzad 《Pramana》2007,69(3):395-409
The coupled-wave equations describing optical parametric amplification (OPA) are usually solved in the slowly varying amplitude
(SVA) approximation regime, in which the second-order derivatives of the signal and idler amplitudes are ignored and in fact
the electromagnetic effects due to exit face of the medium is not involved. Here, an analytical plane-wave solution of these
coupled-wave equations in a non-absorbing medium is presented. The solutions are derived beyond the SVA approximation up to
order of κ/k (coupling constant over the wave number). The intensity distributions of the signal and the idler waves show a periodic behavior
about their corresponding distributions of SVA-adapted solution. This behavior can be explained by the interference of the
forward propagating signal (idler) wave and the corresponding backward one resulted from the reflection by the end face of
the medium. Furthermore, this interference pattern in the medium can in turn serve as a periodic source for the next generations
of the signal and idler waves. Therefore, the superposition of the waves, generated from different points of this periodic
source, at the exit face of the medium shows an oscillatory behavior of the transmitted signal (idler) wave in terms of normalized
coupling constant, κL. This study also shows that this effect is more considerable for high intensity pump beam, high relative refractive index
and short length of the nonlinear medium.
相似文献
19.
R.K. Varma 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2002,18(2):211-218
It has been shown earlier [3,6] that matter waves which are known to lie typically in the range of a few angstrom, can also
manifest in the macrodomain with a wave length of a few centimeters, for electrons propagating along a magnetic field. This
followed from the predictions of a probability amplitude theory by the author [1,2] in the classical macrodomain of the dynamics
of charged particles in a magnetic field. It is shown in this paper that this case constitutes only a special case of a generic
situation whereby composite systems such as atoms and molecules in their highly excited internal states, can exhibit matter
wave manifestation in macro and mesodomains, in one-dimensional scattering. The wave length of these waves is determined,
not by the mass of the particle as in the case of the de Broglie wave, but by the frequency ω, of the classical orbital motion
of the internal state in the correspondence limit, and is given by a nonquantal expression, λ = 2πv/ω, v being the velocity of the particle. For the electrons in a magnetic field the frequency corresponds to the gyrofrequency,
Ω and the nonquantal wave length is given by λ = 2πv
|| /Ω; v
|| being the velocity of electrons along the magnetic field.
Received 29 September 2001 / Received in final form 23 May 2002 Published online 19 July 2002 相似文献