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1.
N.V. Vitanov B.W. Shore K. Bergmann 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》1998,4(1):15-29
The well-known process of stimulated Raman adiabatic passage (STIRAP) provides a robust technique for achieving complete population
transfer between the first and last state of a three-state chain, with little population, even transiently, in the intermediate
state. The extension of STIRAP to general N-state chainwise-linked systems continues to generate interest. Recently Malinovsky and Tannor (Phys. Rev. A 56, 4929 (1997)) have shown with numerical simulation that a resonant pulse sequence, which they term “straddle STIRAP”, can
produce (under appropriate conditions, including specific pulse areas) complete population transfer with very little population
in intermediate states. Their proposal supplements a pair of counterintuitively ordered delayed laser pulses, driving the
first and last transition of the chain and corresponding to the pump and Stokes pulses in STIRAP, with one or more additional
strong pulses of longer duration which couple the intermediate transition(s) and overlap both the pump and the Stokes pulses.
In this paper, we modify the “straddling” Malinovsky-Tannor pulse sequence so that the intermediate couplings are constant (and strong), at least during the times when the pump and Stokes pulses are present, and the intermediate states therefore
act as a strongly coupled subsystem with constant eigenvalues. Under this condition, we show that the original N-state chain is mathematically equivalent to a system comprising N-2 parallel -transitions, in which the initial state is coupled simultaneously to N-2 dressed intermediate states, which in turn are coupled to the final state. The population transfer is optimized by suitably
tuning the pump and Stokes frequencies to resonance with one of these dressed intermediate states, which effectively acts
as the single intermediate state in a three-state STIRAP-like process. We show that tuning to a dressed intermediate state
turns the system (for both odd N and even N) into a three-state system - with all of the properties of conventional STIRAP (complete population transfer, little transient
population in the intermediate states, insensitivity to variations in the laser parameters, such as pulse area). The success
of the tuning-to-dressed-state idea is explained by using simple analytic approaches and illustrated with numerical simulations
for four-, five-, six- and seven-state systems.
Received: 17 April 1998 / Accepted: 15 June 1998 相似文献
2.
讨论了在串行Λ系统中制备初态和末态的连续叠加态的方法,这种方法是部分受激拉曼绝热通道的扩充.但是它又不同于部分受激拉曼绝热通道,每个斯托克斯脉冲先行相应的泵浦脉冲,但是所有的中间脉冲提前并且同时消失,而第一束斯托克斯脉冲和最后一束泵浦脉冲稍后同时消失.应用数值方法讨论了脉冲驰豫时间和失谐量对该方法的影响.数值结果表明要制备任意的叠加态,不仅要满足双光子共振,而且要满足单光子共振. 相似文献
3.
我们给出了在A型五能级系统中制备| 3态和| 5态的连续叠加态的方法,这种方法是部分受激拉曼绝热通道的扩充。但是它又不同于部分受激拉曼绝热通道,我们设计了新的斯托克斯脉冲和相应的泵浦脉冲。进而应用数值方法讨论了脉冲驰豫时间和失谐量对该方法的影响.数值结果表明要制备任意的叠加态要满足双光子共振.这种方法可以推广到多能级A系统中制备任意两个下面能级的叠加态. 相似文献
4.
5.
We propose a flexible way to significantly enhance population transfer efficiency with a train of time-separated pump-Stokes pulse pairs when the non-adiabatic coupling between two degenerate adiabatic states exists in a double Λ-type four-level system, where the pump and Stokes pulses in each pair can be applied in either counterintuitive or intuitive order. It is shown that the needed Rabi frequency for achieving complete population transfer can be reduced dramatically with the increase of number of pump-Stokes pulse pairs, which results from temporal constructive quantum interference between the sequential transitions and subsequent coherent accumulation; moreover, an arbitrary coherent superposition between the two lower states can be realized by suitably tuning the Rabi frequency and the time delay between each pump-Stokes pair. The method may find applications in control of chemical reactions, quantum optics, and quantum information processing. 相似文献
6.
Contrary to a standard definition of diabatic states (i.e., those without momentum-dependent coupling), based on the construction from adiabatic ones, we defined diabatic states as bright and dark states of a given experiment. Namely, they are defined as states providing maximum, respectively, zero value of electronic transition dipole moments projected to a given polarization vector. Second, the state from (or to) which the optical transition is performed is not from the space of investigated electronic excited state manifold, but it is chosen by the observer. It is shown, for this case, that the inter-state coupling is a general function of vibrational coordinates. The explicit dependence of the inter-state coupling on vibrational coordinates is particularly important for system with strong Stokes shift. The role of exact definitions of bright and dark states as well as the inter-state coupling is discussed with respect to the coherent structure of electronic population observed in optical spectroscopy. 相似文献
7.
We present the experimental demonstration of a novel, efficient, and selective technique to prepare population inversion. The technique is an extension of Stark-chirped rapid adiabatic passage (SCRAP), i.e., SCRAP among three states. In this process a Lambda-type quantum system is driven by two laser pulses, the pump and Stokes pulses, which are appropriately detuned from transition frequencies. A third laser pulse induces a dynamic Stark shift in the upper energy level, and the timing of all three pulses is controlled in order to prepare population inversion between the two lower states in the Lambda-type level scheme. Our data on population transfer in nitric oxide (NO) molecules clearly show that SCRAP among three states provides an advantageous alternative to such techniques as stimulated Raman adiabatic passage. 相似文献
8.
本文讨论了在双Λ型原子系统中制备相干叠加态的方法:一个Λ型系统通过控制激光而另一个Λ型系统采用部分受激拉曼绝热通道的方法.在理论上分析了产生任意相干叠加态的可能性并且讨论了透热系统在产生相干叠加态过程中的重要性.研究表明,没有透热过程是不可能制备出任意的叠加态.应用数值方法验证理论分析是正确,并且指出任意叠加态的产生只与控制脉冲的时间延迟有关. 相似文献
9.
Y. Xiang S. J. Xiong F. Y. Hong 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2008,47(2):257-260
A bipartite quantum state (for two systems in any dimensions) can be
decomposed as a superposition of many components. For a
superposition of more than two components we prove that there is a
bound of the entanglement of the superposition state which can be
expressed according to entanglements of its component states.
Especially, if the component states are mutually bi-orthogonal, the
entanglement of the superposition state can be exactly given in
terms of the entanglements of the states being superposed. 相似文献
10.
Generation of entangled coherent states for two cavity modes via resonant interaction with a V-type three-level atom
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This paper proposes a scheme for the generation of entangled coherent states for two cavity modes. In the scheme a V-type three-level atom is sent through a two-mode cavity filled with a coherent field. After the atom cavity interaction and detection of the atomic state the cavity modes may evolve to a superposition of two-mode coherent states. As the scheme is based on resonant atom-cavity interaction, the required interaction time is short, which is important in view of the decoherence. Moreover, additional classical pulses are unnecessary before and after the atom-cavlty interaction. 相似文献
11.
MA Aiqun 《Chinese Journal of Lasers》1994,3(2):105-115
High-ordersqueezingofpuresuperpositionstatesMAAiqun(HarbinCollege,Harbin,150020,China)ZHANGYanxun(DepartmentofPhysics,HarbinN... 相似文献
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13.
同科电子L-S耦合原子态的确定 总被引:2,自引:1,他引:1
给出一种确定同科电子L-S耦合原子态的简便方法,同时指出如果两个同科电子组态的电子数之和等于该支壳层上的电子数,那么这两个同科电子组态具有相同的原子态. 相似文献
14.
We propose a method for the creation of arbitrary superposition of N atomic states using generalized stimulated Raman adiabatic passage (STIRAP) techniques with laser fields coupling each one of N lower states to a single upper state in a (N+1)-level atomic system. (N-1) dark states that are composed of N lower states span a dark subspace. In the adiabatic limit, the dark and bright subspaces are decoupled, thus the nonadiabatic interaction within this dark subspace dominates the evolution of the system. Different from general methods to create our required coherent superposition state, in a reverse way, here we consider the required state as the starting point of evolution dynamics, and utilize laser fields to drive it into a single lower state step by step. Time reverse pulses of laser fields return the single lower state back to our required coherent superposition state based on time reversal symmetry. In principle, the computationally simple method allows the case with a large value of N. Based on the STIRAP techniques, it is robust against small variations of parameters of laser pulses and is immune to spontaneous radiation. 相似文献
15.
We have investigated the photoionization properties of an atom with a ladder coupling scheme involving two autoionizing states coupled to each other.The effects of the coherent coupling between two autoionizing states and between the low-lying autoionizing state and the continuum on the ionization yield are discussed.The conditions leading to atomic coherent population trapping and the coherent population trapping states are given explicitly. 相似文献
16.
Superpositions of squeezed states were introduced by Sanders [Phys. Rev. A 39 (1998) 4284], Schleich et al. [Phys. Rev. A 38 (1988) 1177], Xin et al. [Phys. Rev. A 50 (1994) 2865], to investigate the occurrence of nonclassical properties of the quantized radiation field. In this report we present a generalized superposition state which interpolates between two arbitrary squeezed states. Nonclassical properties of this intermediate state as function of the interpolating parameters are studied, the previous results in the literature becoming a particularization of ours. An experimental proposal to generate this state is also presented. 相似文献
17.
Subhash Kak 《Pramana》2001,57(4):683-687
Quantum computing algorithms require that the quantum register be initially present in a superposition state. To achieve this,
we consider the practical problem of creating a coherent superposition state of several qubits. We show that the constraints
of quantum statistics require that the entropy of the system be brought down when several independent qubits are assembled
together. In particular, we have: (i) not all initial states are realizable as pure states; (ii) the temperature of the system
must be reduced. These factors, in addition to decoherence and sensitivity to errors, must be considered in the implementation
of quantum computers. 相似文献
18.
A. Wetzels A. Gürtler H.G. Muller L.D. Noordam 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2001,14(2):157-165
An optically excited Rydberg wavepacket can be generated by exciting the electron from a low-lying state to a coherent superposition
of high-lying states with a short broadband optical pulse. A special kind of Rydberg wavepacket is generated in the case of
a interaction of a weak THz half cycle pulse with a stationary Rydberg state, called the THz wavepacket. This THz wavepacket
is a coherent superposition of the initial Rydberg state and its neighbouring states. We have investigated the time evolution
of THz wavepackets by measuring the impact of two in time delayed half cycle pulses ( ≈ 200 V cm-1) on the population of a stationary (n = 40) Rydberg state in rubidium. The first half cycle pulse creates the THz wavepacket and the second half cycle pulse probes
the dynamics of the THz wavepacket. We support our experimental data by numerically solving the Schr?dinger equation and with
a semi-classical picture. Whereas an optically excited wavepacket is initially localized, a THz wavepacket is initially delocalized
and becomes localized after half a revival time.
Received 23 August 2000 and Received in final form 27 March 2001 相似文献
19.
Using the recently developed theory of resonant Raman scattering in the presence of strong double frequency fields, the statistical properties of the spontaneously emitted Stokes and Rayleigh radiation are calculated. In particular, the temporal intensity correlations of arbitrary order are evaluated. It is found that they possess the property of factorization in terms of the probabilities for finding the system in the resonant intermediate excited state when the starting state is the given initial state and when the starting state is a particular superposition of the ground and final excited states. The weight-factors in the particular superposition depend on the direction of observation and on the transition dipole-moments. The second-order intensity correlation is shown to have the complete anti-bunching property. The factorization property of the intensity correlations is useful in the calculation of photo-electron counting distributions. 相似文献
20.
CHEN Mei-Feng 《理论物理通讯》2006,45(1):154-156
A scheme is presented for generating a four-photon coherent state via the degenerate Raman interaction. The scheme does not need classical fields to manipulate the atoms. Its another advantage is that the atomic spontaneous emission can be neglected. Therefore, the coherence of the system may be better maintained. The scheme can be generalized to generate superposition of 2n coherent states and superposition of 2n two-mode coherent states. The coherent states in each mode are on a circle symmetrically. 相似文献