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考虑初始处于最大纠缠态的两全同二能级原子,将其中一个注入单模真空态腔场中发生多光子共振相互作用,而将腔外原子及腔场视为腔内原子的环境,研究通过操作腔外原子实现腔内原子最大相干性恢复调控.考察对腔外原子作Hadamard门操作及基态测量前后两种情况下,腔内原子约化密度矩阵非对角元时间演化曲线.结果表明:对腔外原子操作前,腔内原子总是处于混合态或经典态,相干性不能恢复;对腔外原子操作后,腔内原子密度矩阵非对角元呈现周期性演化,最大相干性可周期性恢复,而且最大相干性恢复周期随光子数目k增大而变小.通过利用腔场与原子之间的共振相互作用和原子之间的纠缠,可实现腔内原子相干性恢复远程控制,与单光之过程相比,多光子过程更有利于原子相干性的恢复. 相似文献
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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
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从量子相干性包括l1 norm相干性和量子相对熵相干性的角度建立了判定开放量子系统中非马尔可夫过程的方法, 并给出了相应的判别条件. 作为它们的具体应用, 研究了一个两能级系统分别经历相位衰减通道、 随机幺正通道和振幅耗散通道作用时对应的非马尔可夫过程发生必须满足的条件. 对于三种通道模型, 得到了l1 norm相干性对系统任意态非马尔可夫过程发生的判别条件, 并发现在相位衰减通道和振幅耗散通道中其非马尔可夫过程发生 的条件与用其他方式如信息回流、可分性和量子互熵给出的条件是相同的, 而在随机幺正通道中给出了一个新的且不完全等价于基于信息回流和可分性对应的条件. 至于量子相对熵相干性, 在相位衰减通道中得到了对系统任意态的非马尔可夫过程发生的具体条件, 并发现该条件也等同于基于信息回流、可分性和量子互熵给出的条件. 而在随机幺正通道和振幅耗散通道中得到了系统最大相干态对应的非马尔可夫过程发生的条件. 相似文献
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考虑初始处于最大纠缠态的两全同二能级原子,将其中一个注入单模真空态腔场中发生多光子共振相互作用,将腔外原子及腔场视为腔内原子的环境,研究通过操作腔外原控制腔内原子最大相干性恢复。考察对腔外原子作Haddmard(H)逻辑门操作及基态测量前后,腔内原子约化密度矩阵非对角元时间演化曲线。结果表明:对腔外原子操作前,腔内任意 光子过程原子密度矩阵非对角元任意时刻都为零,总是处于混合态或经典态,相干性不能恢复。对腔外原子操作后,在光子数 过程中,腔内原子密度矩阵非对角元呈现周期为 的时间演化,在 时刻最大相干性恢复及态被制备。对于多光子( )的过程,腔内原子密度矩阵非对角元时间演化呈高频振荡,振幅呈非线性变化,最大相干性恢复周期变小、恢复次数增多。通过利用腔场与原子之间的共振相互作用和原子之间的纠缠,可实现腔内原子相干性恢复远程控制。与单光之过程相比,多光子过程更有利于原子相干性的恢复。 相似文献
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多原子-腔系统中的量子信息传递 总被引:14,自引:7,他引:7
提出了一个多原子-腔组成的物理系统,并讨论了发生在该系统中量子信息的交换和传递过程,结果发现:由最低两个Fock态|0〉和|1〉任意组成的光量子态腔场,当处于基态的原子以特定的速度通过腔时,原子都能带走腔中的量子态并据为己有;反之,由两能级原子的基态|g〉和激发态|e〉任意组成的量子态,当原子以特定的速度通过处于真空态的腔时,原子都能把携带的量子态释放于腔中,实现了腔-原子之间的信息交换.利用原子能够捡起、释放量子信息这一特点,进一步讨论了把原子作为运输工具实现腔-腔之间异地量子信息传递的物理过程. 相似文献
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提出了一个未知原子的隐形传态方案,它是通过原子与腔场大失谐相互作用实现的.方案中,两原子缠结的EPR态作为联系发送者与接收者之间的量子信息通道,将欲传送的未知原子和EPR态中的一个原子依次注入到初始制备于相干态 |α>的腔场,然后分别对两原子和腔场进行联合测量,通过经典信息通道将测量结果传递给接收者.这样,接收者只要对EPR的另一个原子执行相应的幺正操作就能重构未知原子态. 相似文献
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Entropy squeezing of a moving atom and control of noise of the quantum mechanical channel via the two-photon process 下载免费PDF全文
Based on the quantum information theory, we have investigated the
entropy squeezing of a moving two-level atom interacting with the
coherent field via the quantum mechanical channel of the two-photon
process. The results are compared with those of atomic squeezing
based on the Heisenberg uncertainty relation. The influences of the
atomic motion and field-mode structure parameter on the atomic
entropy squeezing and on the control of noise of the quantum
mechanical channel via the two-photon process are examined. Our
results show that the squeezed period, duration of optimal entropy
squeezing of a two-level atom and the noise of the quantum mechanical
channel can be controlled by appropriately choosing the atomic motion
and the field-mode structure parameter, respectively. The quantum
mechanical channel of two-photon process is an ideal channel for
quantum information (atomic quantum state) transmission. Quantum
information entropy is a remarkably accurate measure of the atomic
squeezing. 相似文献
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We consider the irreversible dynamics of two two-level atoms that interact with a bipartite broad-band electromagnetic field
in an entangled state that forms a heat bath with a quantum correlation. Using Ito’s stochastic integration technique, we
have derived a kinetic equation for atoms and found their steady state, which turns out to be inseparable and leads to a violation
of Bell’s inequalities. The application of the atomic state found as a quantum channel for teleportation is considered. We
have calculated the channel quality or fidelity that determines the possibilities for using the channel, in particular, characterizes
its security. The process of teleportation by means of a quantum channel formed by an entangled heat bath is considered. Comparison
of two (atomic and light) channels has shown that they have different properties with regard to separability and identical
properties with regard to nonlocality. This means that nonlocality can be completely transferred from light to atoms. 相似文献
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In the paper, taking the atomic EPR entanglement states as quantum channel, we investigate the fidelity of quantum teleportation of atomic state in thermal environment and vacuum reservoir by means of quantum theory of damping-density operator approach, and the average fidelities are calculated. the resultsshow that the atomic quantum channel state |ø> = (1/21/2)(| 00>+ |11>) is more robust than | Φ> = (1/21/2)(|01> + |10>) in teleportation process when they are subject to the dissipative environments. 相似文献
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The ground state of an atomic Fermi gas near the Feshbach resonance for a negative scattering length is investigated using the variational method. The structure of the superfluid state is formed by two coherently coupled subsystems, viz., the quasimolecular subsystem in a closed channel and the subsystem of atomic pairs in an open channel. The derived system of equations makes it possible to describe the properties of the ground state for arbitrary values of the parameters (in particular, to find the gap in the single-particle Fermi excitation spectrum and the speed of sound characterizing the branch of collective Bose excitations). 相似文献
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Xiao Y Klein M Hohensee M Jiang L Phillips DF Lukin MD Walsworth RL 《Physical review letters》2008,101(4):043601
We demonstrate a slow light beam splitter using rapid coherence transport in a wall-coated atomic vapor cell. We show that particles undergoing random and undirected classical motion can mediate coherent interactions between two or more optical modes. Coherence, written into atoms via electromagnetically induced transparency using an input optical signal at one transverse position, spreads out via ballistic atomic motion, is preserved by an antirelaxation wall coating, and is then retrieved in outgoing slow light signals in both the input channel and a spatially-separated second channel. The splitting ratio between the two output channels can be tuned by adjusting the laser power. The slow light beam splitter may improve quantum repeater performance and be useful as an all-optical dynamically reconfigurable router. 相似文献
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氦原子(e,2e)反应中库仑波描述入射电子的理论研究 总被引:8,自引:7,他引:1
张穗萌 《原子与分子物理学报》2005,22(1):171-174
在前期工作的基础上,当初通道使用具有有效电荷库仑波时,完成了电子入射离化氦原子三重微分截面的理论推导.计算表明:初通道库仑场对较低入射能量情况下,(e,2e)过程的三重微分截面有较大影响. 相似文献
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N. Knake V. Schulz-von der Gathen 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2010,60(3):645-652
The ascent of atomic oxygen densities created inside the micro-scaled atmospheric pressure plasma jet has been investigated
spatially resolved under parameter variations such as applied power, gas mixture and gas velocity using two-photon absorption
laser induced fluorescence spectroscopy.
Along the discharge channel an increase of the atomic oxygen density within the plasma is observed. The density shows an exponentially
asymptotic convergence into an equilibrium close to the effluent. In the post-discharge effluent an exponential spatial decrease
can be found. Typical ascent distances of a few hundreds of
μm decrease with the applied power and increase with gas velocity and oxygen admixture. The maximum atomic oxygen density increases
with applied power and admixed molecular oxygen up to more than
1016 cm-3. An increase of the maximum atomic oxygen density with increasing gas velocity has been found. Optical emission spectroscopy
measurements indicate a strong increase of the nitrogen emission at low gas flow rates along the channel. 相似文献
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真空背压的变化会改变进入霍尔推力器放电通道内的背景气体量,对工质的电离、电子的传导等物理过程产生影响,从而进一步影响到推力器的宏观放电特性.为分析真空背压对推力器放电的影响规律,通过向真空罐输入流量可控的氪气改变真空背压,在不同真空背压下测量通道内原子、离子的发光特性以及出口处离子流的伏安特性.分析结果表明:背景气体返流对通道内工质放电过程具有全局性的影响,提高背压会使通道内的电子温度降低、电离效率降低,并会在通道内形成一个新的电离区,且背压越高,该电离区距推力器阳极越近. 相似文献
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When N driven atoms emit in phase into a high-Q cavity mode, the intracavity field generated by collective scattering interferes destructively with the pump driving the atoms. Hence atomic fluorescence is suppressed and cavity loss becomes the dominant decay channel for the whole ensemble. Microscopically, 3D light-intensity minima are formed in the vicinity of the atoms that prevent atomic excitation and form a regular lattice. The effect gets more pronounced for large atom numbers, when the sum of the atomic decay rates exceeds the rate of cavity losses and one would expect the opposite behavior. These results provide new insight into recent experiments on collective atomic dynamics in cavities. 相似文献