共查询到20条相似文献,搜索用时 0 毫秒
1.
X. Luo S. Zhu 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2002,19(1):111-117
A two-dimensional decoupling theory is developed when colored noise is included in a nonlinear dynamical system. By a functional
analysis, the colored noise is transformed to an effective noise that includes the noise correlation time, the mean dynamical
variable, and the original noise strength. When the two-dimensional decoupling theory is applied to single-mode and two-mode
dye laser systems, the mean, variance, and effective eigenvalue of laser intensity are calculated. Excellent agreement between
theoretical analysis, numerical simulations, and experimental measurements are obtained. It is seen that the increase of noise
correlation time can reduce the fluctuations in the laser system. It is also shown that there is relatively large fluctuation
in the phase when the laser undergoes from thermal light to coherent light when the theory is applied to a single mode dye
laser.
Received 20 August 2001 and Received in final form 4 December 2001 相似文献
2.
E. Lantz F. Devaux 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2001,17(1):93-98
We study the properties of the spatial fluctuations in the far-field parametric fluorescence output of a type 1 degenerate traveling-wave parametric amplifier. Results of a semi-classical simulation are compared with experiments in a LBO crystal. This simulation is then used to predict amplified images of a continuous background, in a phase-sensitive as well as in a phase-insensitive configuration. Received 12 March 2001 相似文献
3.
P.J. Edwards G.H. Pollard W.N. Cheung 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2002,18(2):147-153
Quantum key exchanges using weak coherent (Poissonian) single-photon sources are open to attack by a variety of eavesdropping
techniques. Quantum-correlated photon sources provide a means of flagging potentially insecure multiple-photon emissions and
thus extending the secure quantum key channel capacity and the secure key distribution range. We present indicative photon-counting
statistics for a fully correlated Poissonian multibeam photon source in which the transmitted beam is conditioned by photon
number measurements on the remaining beams with non-ideal multiphoton counters. We show that significant rejection of insecure
photon pulses from a twin-beam source cannot be obtained with a detector having a realistic quantum efficiency. However quantum-correlated
(quadruplet or octuplet) multiplet photon sources conditioned by high efficiency multiphoton counters could provide large
improvements in the secure channel capacity and the secure distribution range of high loss systems such as those using the
low earth orbit satellite links proposed for global quantum key distribution.
Received 14 July and Received in final form 20 November 2001 相似文献
4.
C.-Q. Cao C.-G. Yu H. Cao 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2003,23(2):279-284
The spontaneous emission of an excited atom is analyzed by quantum stochastic trajectory approach without both rotating-wave
approximation and Markovian approximation. The atom finite size effect is also taken into account. We show by an example that
the correction due to the counter-rotating wave term is rather small, even for the largest atomic number of real nuclei.
Received 10 July 2002 / Received in final form 12 November 2002 Published online 4 February 2003 相似文献
5.
N.P. Proukakis P. Lambropoulos 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2002,19(3):355-370
We present a consistent second order perturbation theory for the lowest-lying condensed modes of very small, weakly-interacting
Bose-Einstein condensates in terms of bare particle eigenstates in a harmonic trap. After presenting our general approach,
we focus on explicit expressions for a simple three-level system, mainly in order to discuss the analogy of a single condensate
occupying two modes of a trap with the semi-classical theory for two-mode photon lasers. A subsequent renormalization of the
single-particle energies to include the dressing imposed by mean fields demonstrates clearly the consistency of our treatment
with other kinetic approaches.
Received 14 December 2001 相似文献
6.
D.A. Trifonov 《The European Physical Journal B - Condensed Matter and Complex Systems》2002,29(2):349-353
A survey on the generalizations of Heisenberg uncertainty relation and a general scheme for their entangled extensions to
several states and observables is presented. The scheme is illustrated on the examples of one and two states and canonical
quantum observables, and spin and quasi-spin components. Several new uncertainty relations are displayed.
Received 10 October 2001 / Received in final form 6 March 2002 Published online 2 October 2002
RID="a"
ID="a"e-mail: dtrif@inrne.bas.bg 相似文献
7.
Hong-yi Fan J. Chen 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2003,23(3):437-442
Based on the newly constructed Einstein, Podolsky and Rosen (EPR) entangled state representation we introduce macroscopic
classical functions associated with atomic coherent state τ with angular momentum value j. These functions are proportional to the ordinary one-variable Hermite polynomials of order 2j. The corresponding Wigner quasiprobability function for τ in phase space is also derived which turns out to be a two-variable Hermite polynomial H
2j, 2j. In so doing, a new classical-quantum correspondence scheme for angular momentum system is established.
Received 7 August 2002 / Received in final form 14 December 2002 Published online 24 April 2003
RID="a"
ID="a"Work supported by the National Natural Science Foundation of China under grant 10175057.
RID="b"
ID="b"e-mail: fhym@sjtu.edu.en 相似文献
8.
X.-m. Hu J. Xiong J.-s. Peng 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2001,13(3):401-413
A theoretical analysis of the spectral linewidth of V-type inversionless and Raman lasers is presented. First, we examine
the effects of the atomic coherence between dressed states and the Autler-Townes splitting on the linewidth. It is demonstrated
that near above threshold, the V inversionless laser has a narrower linewidth than that of the two-level laser. Instead of
the dressed coherence, it is the Autler-Townes splitting that is responsible for the linewidth reduction though the dressed
coherence determines the laser gain. Next, we explore the effects of the generated laser intensity on the linewidth. It is
shown that the linewidths of the V inversionless and Raman lasers follow the usual 1/I decrease for smaller laser intensity I, but a slower decrease than 1/I for larger laser intensity. For the V Raman laser, even more surprisingly, with the laser intensity increasing, the linewidth
appreciably increases as well. As a result, well above threshold, the V inversionless and Raman lasers may have a larger linewidth
than that of the two-level laser. Finally, a comparison is made between the V lasers and the Λ lasers. It is found that the
linewidth of the Λ inversionless laser shows a fast 1/I
2 decay under optimum conditions.
Received 25 October 1999 and Received in final form 10 March 2000 相似文献
9.
T. Briant P.F. Cohadon M. Pinard A. Heidmann 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2003,22(1):131-140
We describe an experiment in which the quadratures of the position of an harmonically-bound mirror are observed at the attometer
level. We have studied the Brownian motion of the mirror, both in the free regime and in the cold-damped regime when an external
viscous force is applied by radiation pressure. We have also studied the thermal-noise squeezing when the external force is
parametrically modulated. We have observed both the % theoretical limit of squeezing at low gain and the parametric oscillation
of the mirror for a large gain.
Received 9 July 2002 Published online 29 October 2002
RID="a"
ID="a"e-mail: heidmann@spectro.jussieu.fr
RID="b"
ID="b"Unité mixte de recherche du Centre National de la Recherche Scientifique, de l'école Normale Supérieure et de l'Université
Pierre et Marie Curie. Website: www.spectro.jussieu.fr/Mesure 相似文献
10.
J.-M. Courty A. Heidmann M. Pinard 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2001,17(3):399-408
Thermal noise of a mirror can be reduced by cold damping. The displacement is measured with a high-finesse cavity and controlled
with the radiation pressure of a modulated light beam. We establish the general quantum limits of noise in cold damping mechanisms
and we show that the optomechanical system allows to reach these limits. Displacement noise can be arbitrarily reduced in
a narrow frequency band. In a wide-band analysis we show that thermal fluctuations are reduced as with classical damping whereas
quantum zero-point fluctuations are left unchanged. The only limit of cold damping is then due to zero-point energy of the
mirror.
Received 1st August 2001 and Received in final form 12 October 2001 相似文献
11.
Spatial and temporal properties of parametric fluorescence around degeneracy in a type I LBO crystal
F. Devaux E. Lantz 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2000,8(1):117-124
We present a theoretical and experimental study of the spatio-temporal properties of the spontaneous parametric emission generated
in a type I LBO crystal around degeneracy. The number of quasi-phase-matched modes is shown to be equal to the number of spatio-temporal
degrees of freedom of the image that can be parametrically amplified. From this number, we demonstrate the possibility of
predicting the total number of photons generated by parametric fluorescence. Correlation is observed between spatial intensity
fluctuations corresponding to pairs of signal-idler modes.
Received 18 February 1999 and Received in final form 9 June 1999 相似文献
12.
H.P. Breuer B. Kappler F. Petruccione 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》1998,1(1):9-13
A fast simulation algorithm for the calculation of multitime correlation functions of open quantum systems is presented. It
is demonstrated that any stochastic process which “unravels” the quantum Master equation can be used for the calculation of
matrix elements of reduced Heisenberg picture operators, and thus for the calculation of multitime correlation functions,
by extending the stochastic process to a doubled Hilbert space. The numerical performance of the stochastic simulation algorithm
is investigated by means of a standard example.
Received: 30 May 1997 / Revised: 4 November 1997 / Accepted: 7 November 1997 相似文献
13.
C. Wiele F. Haake K. Rzażewski 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》1999,5(3):405-409
We solve the superradiant laser model in two limiting cases. First the stationary low-pumping regime is considered where a
first-order phase transition in the semiclassical solution occurs. This discontinuity is smeared out in the quantum regime.
Second, we solve the model in the non-stationary regime where we find a temporally periodic solution. For a certain parameter
range well-separated pulses may occur.
Received: 19 June 1998 / Accepted: 19 October 1998 相似文献
14.
G. Li S. Wu P. Zhou 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2001,15(2):267-277
The dressed-state populations and the resonance fluorescence spectrum of a V-type three-level atom driven by a strong coherent
field and a weak stochastic one simultaneously are investigated. There can be significant population inversion due to the
effect of the stochastic field. The atomic resonance fluorescence spectrum can be controlled by adjusting the frequency difference
between the coherent field and the stochastic one and the coherent Rabi frequency. Peak suppression and line narrowing occur
under appropriate conditions.
Received 23 June 2000 and Received in final form 18 January 2001 相似文献
15.
G. Baym J.-P. Blaizot M. Holzmann F. Laloë D. Vautherin 《The European Physical Journal B - Condensed Matter and Complex Systems》2001,24(1):107-124
We study the effects of repulsive interactions on the critical density for the Bose-Einstein transition in a homogeneous dilute
gas of bosons. First, we point out that the simple mean field approximation produces no change in the critical density, or
critical temperature, and discuss the inadequacies of various contradictory results in the literature. Then, both within the
frameworks of Ursell operators and of Green's functions, we derive self-consistent equations that include correlations in
the system and predict the change of the critical density. We argue that the dominant contribution to this change can be obtained
within classical field theory and show that the lowest order correction introduced by interactions is linear in the scattering
length, a, with a positive coefficient. Finally, we calculate this coefficient within various approximations, and compare with various
recent numerical estimates.
Received 15 July 2001 相似文献
16.
S. Yuan J.-Y. Gao 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2000,11(2):267-272
A new scheme of the influence of quantum interference on the spontaneous emission in a coherently driven three-level medium
is presented in this paper. The results are the same with that discussed by [S.-Y. Zhu, L.M. Narducci, M.O. Scully, Phys.
Rev. A 52, 4791 (1995)] under resonance conditions, but they are different when the driven field is detuned.
Received 8 September 1999 and Received in final form 13 January 2000 相似文献
17.
J. Gemmer G. Mahler 《The European Physical Journal B - Condensed Matter and Complex Systems》2003,31(2):249-257
For a closed bi-partite quantum system partitioned into system proper and environment we interpret the microcanonical and
the canonical condition as constraints for the interaction between those two subsystems. In both cases the possible pure-state
trajectories are confined to certain regions in Hilbert space. We show that in a properly defined thermodynamical limit almost
all states within those accessible regions represent states of some maximum local entropy. For the microcanonical condition
this dominant state still depends on the initial state; for the canonical condition it coincides with that defined by Jaynes'
principle. It is these states which thermodynamical systems should generically evolve into.
Received 13 June 2002 / Received in final form 14 November 2002 Published online 4 February 2003
RID="a"
ID="a"e-mail: jochen@theol.physik.uni-stuttgart.de 相似文献
18.
C.M. Granzow A. Liebman G. Mahler 《The European Physical Journal B - Condensed Matter and Complex Systems》1998,2(1):131-142
Continuous measurement models are conveniently based on master equations specified by the respective Hamiltonian and appropriate
environment operators. As demonstrated by stochastic unraveling, the latter specify the dynamical process rather than static
detection modes. We show that certain environment operators acting on a simple system may, in fact, require extended networks
for implementation: Their Hamilton parameters re-appear in the effective environment operators of the reduced model. The resulting
quantum trajectories typically involve competing paths, which may give rise to different fluctuation and noise properties
even when the corresponding ensemble behavior is practically the same.
Received: 21 July 1997 / Received in final form: 10 November 1997 / Accepted: 27 October 1997 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
20.
Y. Jiang O. Jedrkiewicz S. Minardi P. DiTrapani A. Mosset E. Lantz F. Devaux 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2003,22(3):521-526
The pixel by pixel calibration of a scientific CCD camera allows Poissonian statistics of the spatial fluctuations of an uniform
enlightening to be retrieved in the full range of the camera dynamic. The procedure works efficiently for thermal as well
as for laser sources, provided that the wavelength and the coherence properties of the source are chosen in order to avoid
the formation of equal thickness fringes in the chip (etaloning effect). Calibration allows also the comparison at the shot
noise level of images recorded at different places on the chip.
Received 9 September 2002 / Received in final form 16 October 2002 Published online 21 January 2003 相似文献