共查询到20条相似文献,搜索用时 125 毫秒
1.
为了研究三光子过程中原子与相干态耦合量子体系信息熵压缩随时间演化规律及原子最佳信息熵压缩态的制备,我们采用全量子理论,推导出运动原子与单模简并三光子依赖强度耦合量子体系的精确解;理论上给出制备原子最佳信息熵压缩态的充分及必要条件,并进行了数值模拟验证。研究结果表明:控制相干态场与原子作用时间,切断相干态场与原子的纠缠,选择二能级原子处于等权重相干叠加态,适当选取相干态场与原子的初始位相,可以制备出原子最佳量子信息熵压缩态;调节光腔中场模结构参量,能够得到连续的量子信息熵压缩态。该研究结果在多光子过程低噪声量子信息处理中具有一定意义。 相似文献
2.
为了研究三光子过程中原子与相干态耦合量子体系信息熵压缩随时间演化规律及原子最佳信息熵压缩态的制备,我们采用全量子理论,推导出运动原子与单模简并三光子依赖强度耦合量子体系的精确解;理论上给出制备原子最佳信息熵压缩态的充分及必要条件,并进行了数值模拟验证.研究结果表明:控制相干态场与原子作用时间,切断相干态场与原子的纠缠,选择二能级原子处于等权重相干叠加态,适当选取相干态场与原子的初始位相,可以制备出原子最佳量子信息熵压缩态;调节光腔中场模结构参量,能够得到连续的量子信息熵压缩态.该研究结果在多光子过程低噪声量子信息处理中具有一定意义. 相似文献
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研究了利用相干陷落方法在单原子微激射器中产生具有四阶压缩和振幅平方压缩性质的稳态腔场.结果表明,在目前微激射器实验的腔损条件下,如果注入腔中的原子初始处于相干态,只要原子束的通量适当大,当原子在腔中的飞行时间满足陷落条件时,腔场可进入相干陷落态,此时腔场呈现稳定的四阶压缩和振幅平方压缩性质
关键词: 相似文献
5.
本文提出利用简并Λ型三能级原子与单模腔场的Raman相互作用制备压缩相干态的叠加态的一种新方案,并对单模压缩相干态光场中有关压缩角(即压缩方向)的控制问题进行了详细讨论. 相似文献
6.
利用简并Λ型三能级原子与单模腔场的Raman相互作用制备压缩态的叠加态 总被引:4,自引:1,他引:3
本文提出利用简并Λ型三能级原子与单模腔场的Raman相互作用制备压缩相干态的叠加态的一种新方案,并对单模压缩相干态光场中有关压缩角(即压缩方向)的控制问题进行了详细讨论. 相似文献
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利用J-C模型,采用数值计算方法研究了相干态光场与级联型三能级原子相互作用过程中场的压缩效应和反聚束效应。讨论了选择原子测量对相干态光场与级联型三能级原子相互作用过程中场压缩效应和反聚束效应的影响。 相似文献
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考虑初始处于EPR态的两个二能级原子A、B,将B原子注入处于相干态的腔中,演化一段时问后,对B原子进行选择性测量.当相干态腔场的平均光子数足够大时,原子A可呈现偶极矩压缩效应. 相似文献
11.
Two new types of quantum states are constructed by applying the operator s(ξ) = exp(ξ*ab - ξa b ) on the two-mode even and odd coherent states.The mathematical and quantum statistical properties of such states are investigated.Various nonclassical features of these states,such as squeezing properties,the inter-mode photon bunching,and the violation of Cauchy-Schwarz inequality,are discussed.The Wigner function in these states are studied in detail. 相似文献
12.
二能级原子与压缩光场相互作用中的原子压缩效应 总被引:1,自引:1,他引:0
詹佑邦 《原子与分子物理学报》1994,11(4):409-417
文中采用时间学业伦算符,考察到初始原子相干性及失谐量,研究了单个二能级原子与压缩真态辐射场相互作用中原子的偶极压缩。研究表明,对于各种不同的初始原子态,失谐量对双光子Jaynes-Cummings模型中的原子压缩行为都将产生很大的影响。通过数值计算,还讨论了初始压缩光场的压缩参数对原子压缩的影响。 相似文献
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考虑到失谐量和初始原子相干性,研究了双光子Jaynes-Cummings模型中原子的压缩行为。研究表明,失谐量对场-原子相互作用中的原子压缩行为的影响很大,通过数值计算,还讨论了初始平均光子数与原子压缩的关系。 相似文献
14.
考虑到失谐量和初始原子相干性,研究了双光子Jaynes-Cummings模型中原子的压缩行为。研究表明,失谐量对场-原子相互作用中的原子压缩行为的影响很大。通过数值计算,还讨论了初始平均光子数与原子压缩的关系。 相似文献
15.
H. Prakash R. Kumar 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2007,42(3):475-481
Saito and Ueda [Phys. Rev. A 59, 3959 (1999)] studied atomic and
radiation squeezing in interaction of a single mode coherent state
of radiation with two excited two-level atoms, using
the Jaynes Cummings Hamiltonian. They considered α real and studied
squeezing of the Dicke operator Sx using the Kitagawa-Ueda criterion for
squeezing and coupling times less than or nearly equal to
. We obtain results to all orders in coupling time for
atoms, which are initially in (i) fully excited, (ii) superradiant or in
(iii) ground states and obtain more general results. We use our recently
reported criterion for atomic squeezing, of which the Kitagawa-Ueda
criterion is a special case, and obtain a much stronger (nearly 95%)
atomic squeezing than that (nearly 1.1%) reported by Saito and Ueda. 相似文献
16.
本文研究了任意初态的双光子Jaynes-Cummings模型的一般演化规律,着重于分析初始原子相干性对辐射场压缩行为的影响,作为例子,讨论了一个任意初态的二能级原子与真空态和相干态光场相互作用时辐射场的压缩.数值计算了各种条件下辐射场压缩的时间演化. 相似文献
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双光子Jaynes—Cummings模型中初始原子相干性对辐射场... 总被引:2,自引:0,他引:2
本文研究了任意初态的双光子Jaynes-Cummings模型的一般演化规律,着重于分析初始原子相干性对辐射场压缩行为的影响,作为例子,讨论了一个任意初态的二能级原子与真空态和相干态光场相互作用时辐射场的压缩.数值计算了各种条件下辐射场压缩的时间演化. 相似文献
18.
Horacio Grinberg 《Annals of Physics》2011,(11):2845-2867
An intensity dependent nonlinear coupling model of N two-level atoms (generalized Dicke model) interacting dispersively with a bimodal cavity field via two-photon transitions is investigated in a scenario where the rotating wave approximation is assumed. The model becomes homogeneous in the sense that the spin transition frequency is the same for all atoms and the coupling constants emerging from the collective interactions of the atomic system with the cavity field depend only on the particular radiation field mode. This allows us to represent the Dicke Hamiltonian entirely in terms of the total angular momentum J. It is assumed that, initially, the atomic system and the field are in a disentangled state where the field modes are in Glauber coherent states and the atomic system is a superposition of states |JM〉 (Dicke states). The model is numerically tested against simulations of normal squeezing variance of the field, squeezing factors based on the Heisenberg uncertainty principle, along with the statistical properties of the light leading to the possible production of nonclassical effects, such as degree of second-order coherence in the modes, degree of intermode correlation, as well as violation of the Cauchy–Schwartz inequality. Analytical expression of the total density operator matrix elements at t>0 shows the present nonlinear model to be strongly entangled, which is reflected in the time evolution of the linear entropy, where the superposition states are reduced to statistical mixtures. Thus, the present generalized Dicke model does not preserve the modulus of the Bloch vector. The computations, performed in the weak coupling and strong field limits, were conducted via second-order Dyson perturbative expansion of the time evolution operator matrix elements for the totality of the angular momentum states of the atomic system. 相似文献
19.
Using an annihilation operator, coherent states related to the electron of graphene layer placed in a magnetic field, can be obtained. In this paper, we define even and odd superposed graphene coherent states and then, we consider their entanglement, squeezing and statistical properties. To study the entanglement, we use concurrence. The results show that odd superposed graphene coherent states are maximally entangled states for all values of coherence parameter. However, the entanglement of graphene coherent states and also even superposed depend on the coherence parameter. In addition, examining the Mandel parameter shows sub-Poissonian statistics for graphene coherent states and their odd superposition; while, even superposed states do not show sub-Poissonian statistics at all. Also, we find that graphene coherent states and even superposition may be squeezed while the odd states do not show squeezing. 相似文献
20.
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