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1.
Summary We have studied the squeezing properties of the atom and the radiation field in arbitrary intensity-dependent-coupling Jaynes-Cummings
model when it is restricted to the following initial condition: the atom in its coherent state and the field in the vacuum
state. The influence of virtual-photon processes on the atomic squeezing predicted by the Jaynes-Cummings model (JCM) has
been examined. The relationship between the field and atomic squeezing in the resonant multi-photon JCM has been discussed.
The symmetry between the field and atomic squeezing (SFAS) has been exposed in the resonant vacuum one-photon JCM, and the
influence of non-resonant interaction and virtual-photon processes on the SFAS has also been discussed. 相似文献
2.
C. F. Lo 《Il Nuovo Cimento D》1991,13(10):1279-1292
Summary In this paper we investigate the time evolution of a general driven time-dependent oscillator using the evolution operator
method developed by Chenget al. We obtain an exact form of the time evolution operator which, in turn, enables us to find the exact wave functions and coherent
states at any timet. Our analyses indicate that the time-dependent coherent state is equivalent to the well-known squeezed state, while the time-dependent
number state is equivalent to the displaced and squeezed number state. Besides, we also calculate the time-dependent transition
probabilities among the coherent states and number states of a simple harmonic oscillator associated with the initial HamiltonianH(0). 相似文献
3.
X.-G. Wang S.-H. Pan G.-Z. Yang 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2000,10(3):415-422
We study the nonclassical properties and algebraic characteristics of the negative binomial states introduced by Barnett recently.
The ladder operator formalism and displacement operator formalism of the negative binomial states are found and the algebra
involved turns out to be the SU(1,1) Lie algebra via the generalized Holstein-Primarkoff realization. These states are essentially Perelomov's SU(1,1) coherent states. We reveal their connection with the geometric states and find that they are excited geometric states.
As intermediate states, they interpolate between the number states and geometric states. We also point out that they can be
recognized as the nonlinear coherent states. Their nonclassical properties, such as sub-Poissonian distribution and squeezing
effect are discussed. The quasiprobability distributions in phase space, namely the Q and Wigner functions, are studied in detail. We also propose two methods of generation of the negative binomial states. d
32.80.Pj Optical cooling of atoms; trapping
Received 8 May 1999 and Received in final form 8 November 1999 相似文献
4.
Gamal M Abd Al-Kader 《Pramana》1999,53(5):877-890
The linear amplifier with the superposition of displaced Fock states (DFS’s) as an input field is discussed. The s-parameterized characteristic function (CF) of linear amplifier for the superposition of two DFS’s is considered. Several
quantum statistical expectation values for the output of linear amplifier are evaluated once the time dependent CF has been
computed. The Glauber secondorder coherence function is calculated. The squeezing properties of the output field are studied.
The s-ordered quasiprobability distribution function (QDF) for the output of linear amplifier driven by DFS’s superposition is
investigated. The phase properties of the superposition of DFS’s are studied. The s-parameterized phase distribution, obtained by integrating the s-parameterized QDF over radial variable is illustrated. 相似文献
5.
Summary The atomic-dipole squeezing condition for arbitrarily prepared atomic and field states in multi-photon Jaynes-Cummings model
was derived. Three special cases were discussed. For the field initially in a vacuum state and a certain eigenstate of the
Susskind-Glogower phase operator, the analytical dipole squeezing conditions were obtained and the maximum squeezing values
were calculated. For a squeezed vacuum input field, the dipole squeezing behaviours under the influence of the field squeezing
parameterr and the phased atom were numerically treated. 相似文献
6.
F. Plastina F. Piperno 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》1999,5(3):411-415
We propose a simple method to obtain a superposition of coherent states on a circle, including Schr?dinger cat states as a
special case, via conditional measurement of the state of three level atoms interacting with a one mode cavity field. In the low amplitude
limit, very good approximation of Fock states can also be generated in this way.
Received: 8 October 1998 / Accepted: 30 October 1998 相似文献
7.
H. Prakash P. Kumar 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2008,46(2):359-363
We study amplitude-squared squeezing of the Hermitian operator Zθ=Z1
cosθ+Z2 sin θ, in the most general superposition state
, of two coherent states
and
. Here operators Z1,2 are defined by
, a is annihilation operator, θ is angle, and
complex numbers C1,2 , α, β are arbitrary and only
restriction on these is the normalization condition of the state
. We define the condition for a state
to be amplitude-squared squeezed for the operator Zθ
if squeezing parameter
, where N=a+a and
. We find
maximum amplitude-squared squeezing of Zθ in the superposed
coherent state
with minimum value 0.3268 of the
parameter S for an infinite combinations with α- β= 2.16
exp [±i(π/4) + iθ/2],
and with
arbitrary values of (α+β) and θ. For this minimum
value of squeezing parameter S, the expectation value of photon number can
vary from the minimum value 1.0481 to infinity. Variations of the parameter
S with different variables at maximum amplitude-squared squeezing are also
discussed. 相似文献
8.
A. Messina 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2002,18(3):379-383
A new conditional scheme for generating Bell states of two spatially separated high-Q cavities is reported. Our method is based on the passage of one atom only through the two cavities. A distinctive feature
of our treatment is that it incorporates from the very beginning the unavoidable presence of fluctuations in the atom-cavity
interaction times. The possibility of successfully implementing our proposal against cavity losses and atomic spontaneous
decay is carefully discussed.
Received 31 July 2001 and Received in final form 9 October 2001 相似文献
9.
Faisal A.A. El-Orany J. Peřina V. Peřinová M. Sebawe Abdalla 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2003,22(1):141-156
The evolution of the Schr?dinger-cat states in a dissipative parametric amplifier is examined. The main tool in the analysis
is the normally ordered characteristic function. Squeezing, photon-number distribution and reduced factorial moments are discussed
for the single- and compound-mode cases. Also the single-mode Wigner function is demonstrated. In addition to the decoherence
resulting from the interaction with the environment (damped case) there are two sources which can cause such decoherence in
the system even if it is completely isolated: these are the decay of the pump and the relative phases of the initial cat states.
Furthermore, for the damped case there are two regimes, which are underdamped and overdamped. In the first (second) regime
the signal mode or the idler mode “collapses" to a statistical mixture (thermal field).
Received 25 September 2001 / Received in final form 30 May 2002 Published online 13 December 2002
RID="a"
ID="a"e-mail: sebaweh@awalnet.net.sa
RID="b"
ID="b"Joint Laboratory of Optics of Palacky University and Institute of Physics, Academy of Sciences of the Czech Republic,
17. listopadu 50, 772 07 Olomouc, Czech Republic. 相似文献
10.
H.-y. Fan A. Wünsche 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2001,15(3):405-412
We examine the existence of right-hand eigenstates (or eigenkets) of the boson creation operator a
and determine their coordinate and their Bargmann representation. The eigenkets of the creation operator are ultrasingular
and cannot be considered as a limiting case of normalizable states. Applications of these eigenstates as auxiliary states
for purposes of representation of states by path integrals over coherent states are discussed. A completeness relation for
coherent states on paths through the complex plane is derived and special examples of its application are considered.
Received 9 March 2001 and Received in final form 13 June 2001 相似文献
11.
Z.-C. Wang Z.-Y. Chen Y. Xu 《The European Physical Journal B - Condensed Matter and Complex Systems》1998,4(2):185-190
A theoretical study is made of the steady-state populations of a three-level atom in a ladder configuration, driven by a superposition
of a monochromatic laser wave with a broad-band squeezed vacuum. The master equation for the system and the atomic Bloch equations
are derived. The steady-state populations are calculated numerically and shown graphically as functions of two-photon detuning
for various cases of the squeezed vacuum. It is shown that, the atomic populations depend strongly on the relative phase of
the driving field and the squeezed vacuum. When the phase matching condition is fulfilled, there will be a strong two-photon
resonant absorption from the squeezed vacuum, a characteristic different from absorption of photons from a classical field.
Received: 28 May 1997 / Revised and Accepted: 10 December 1997 相似文献
12.
Shi-Biao Zheng Guang-Can Guo 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》1998,1(1):105-107
We propose a method for preparing superpositions of coherent states of the motion of an ion in an anisotropic two-dimensional
trap, in which the ion is tightly bound in the y direction. In the scheme the ion is excited by two resonant laser beams with equal amplitude, propagating along the x and y directions, respectively. In the Dicke-Lamb limit, an initial coherent state of the ion motion can be converted into a superposition
of several coherent states on a circle through the laser-ion interactions and state-selective measurements on the ion.
Received: 30 May 1997 / Revised: 29 July 1997 / Accepted: 22 October 1997 相似文献
13.
E. Cormier P. Lambropoulos 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》1998,2(1):15-20
We report on observable new features related to ionization of atoms by laser pulses of only few cycles and some intensity.
We show that for particular photo-electron energies, the angular distribution becomes asymmetric and that this asymmetry is
related to the initial phase of the field.
Received: 4 November 1997/Revised: 21 January 1998/Accepted: 23 February 1998 相似文献
14.
Preparation of Fock states and quantum entanglement via stimulated Raman adiabatic passage using a four-level atom 总被引:3,自引:0,他引:3
S.-Q. Gong R. Unanyan K. Bergmann 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2002,19(2):257-262
We study the behaviour of an atom-cavity system exposed to a stimulated Raman adiabatic passage (STIRAP) process in a four-level
system, with a coupling scheme which generate two degenerate dark states. We find that the non-adiabatic interaction of the
two dark states guarantees that the cavity Fock states can always be generated by both intuitively and counterintuitively
ordered pulses. Furthermore, we propose a method to entangle two atoms. Depending on the ordering of the pulses two orthogonal
entangled states can be prepared. Since these entangled states do not have component of the excited states included, the technique
is robust against the detrimental consequences of spontaneous emission.
Received 20 March 2001 相似文献
15.
Effects of photon addition on the quantum nonlocality of squeezed entangled-coherent states 下载免费PDF全文
Effects of photon addition on the quantum nonlocality of squeezed entangled coherent states for Bell-inequality tests are studied theoretically. By utilizing the method of photon-parity measurement, it is found that photon addition can always increase the degrees of Bell violations within a certain parameter range. A possible scheme for generating photon-added squeezed entangled coherent states is proposed. 相似文献
16.
Paulina Marian Tudor A. Marian 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2000,11(2):257-265
We analyze the transient nonclassical behaviour of a single-mode field whose interaction with an environment is governed by
the quantum optical master equation. Our analytic method makes use of the generalized characteristic function of the field
state. First, we find a time at which all squeezing effects disappear by decoherence regardless of the initial state of the
mode. In the case of an input even coherent state, an unusual modification of higher-order squeezing at low values of thermal
mean occupancy transferred to the field is found and discussed. For the same initial state, we also perform a comprehensive
analysis of the mixing process during the interaction with the reservoir. We prove that a maximum in the evolution of the
2-entropy of the attenuated mode exists on condition that its initial mean photon number exceeds the mean occupancy of the
reservoir. This transient mixing enhancement can be considered as a quantum effect of the initial state on the mode damping.
Received 22 April 1999 and Received in final form 2 November 1999 相似文献
17.
M. Feng 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2002,18(3):371-377
The Raman interaction of a ultracold ion trapped with two travelling wave lasers is studied analytically with series solutions,
in the absence of the rotating wave approximation (RWA) and without restrictions of both the Lamb-Dicke limit and the weak
excitation regime. The comparison is made between our solutions and those obtained under the RWA in order to demonstrate the
validity region of the RWA. As a practical example, the preparation of Schr?dinger-cat states is proposed beyond the weak
excitation regime, using our calculations.
Received 12 March 2001 and Received in final form 16 October 2001 相似文献
18.
G.M. Abd Al-Kader 《The European Physical Journal B - Condensed Matter and Complex Systems》1999,8(3):429-438
The s-parameterized characteristic function for the output field with the superposition of squeezed displaced Fock states (SDFS's)
as input field is given. The s-ordered distribution functions for the output field with superposition of SDFS's as input state are investigated. Various
moments are calculated by using the s-ordered characteristic function for that field. The Glauber second-order coherence function is calculated. The quadrature
squeezing for the output field are discussed. Some Quasiprobability distribution functions of the output fields are plotted
as functions of the interaction time. The quadrature squeezing for the output field are discussed.
Received 30 September 1998 相似文献
19.
Summary The density of states in the mobility gap of halogenated amorphous silicon has been measured by the field effect technique.
The results are discussed to shed light on the reality of a peak found in the DOS. A comparison is made with the DOS curves
obtained by SCLC in the same material.
To speed up publication, the authors of this paper have agreed to not receive the proofs for correction. 相似文献
20.
Effects of photon addition on quantum nonlocality of squeezed entangled coherent states for Bell-inequality tests are studied theoretically. By utilizing the method of photon-parity measurement, it is found that photon addition can always increase the degrees of Bell violations within a certain parameter range. A possible scheme for generating photon-added squeezed entangled coherent states is proposed. 相似文献