两个二能级原子与辐射场的量子动力学性质

用完全量子化方法研究两个二能级原子与腔场相互作用过程中，原子能级占居几率与辐射场的量子动力学性质，讨论了原子间耦合及激光发场对上述性质的影响，揭示了原子耦合与原子－场相互作用之间的联系。     

量子微腔中腔场衰变对运动原子自发辐射的影响

通过分析环形微腔中单模量子电磁场与低速运动二能级原子相互作用过程中光子与原子质心的动量交换效应，本文详细研究了原子质心的运动多谱勒效应及光子反冲对原子能级自发辐射寿命的影响，本文理论证明了这效应起因子腔壁引起腔模的衰变，在一定条件下，原子质心运动将增强或低原子的自发辐射。     

腔靶产生的平面辐射场特性的数值模拟

计算了不同腔靶构型参数对靶板能量效率和辐照均匀度的影响, 由此给出有较大能量效率和辐照均匀度的腔靶构型。合适的平面靶与腔壁的面积比既使平面靶的能量利用效率趋近理想又使得平面靶不太大以满足均匀度要求。     

腔靶产生的平面辐射场特性的数值模拟

 计算了不同腔靶构型参数对靶板能量效率和辐照均匀度的影响, 由此给出有较大能量效率和辐照均匀度的腔靶构型。合适的平面靶与腔壁的面积比既使平面靶的能量利用效率趋近理想又使得平面靶不太大以满足均匀度要求。     

钕玻璃微球腔模式移动的观察

报道钕玻璃微球腔在尺寸发生微小变化时腔模也随之移动；腔模移动对泵浦耦合产生了重大影响。     

半导体光学微腔—研究腔量子电动力学效应的绝妙范例

光学微腔中真空场和电子的行为与它们在自由空间中截然不同，导致了腔量子电动力学的一系列复杂性物理问题，半导体光学微腔是新一代凝聚态微型谐振器的典型代表，是探索腔量子电动力学，寻求新型微腔器及其应用的绝妙范例。文章概要介绍了几种典型的半导体光学微腔及其研究进展。     

开放式法布里-珀罗光学微腔中光与单量子系统的相互作用

光与物质相互作用的过程具有丰富的物理内涵,不仅有助于理解光的本质,更可以提供一种有效操控物质的手段.开放式光学微腔具有光场强局域性、频率域和空间域的可调谐性以及光纤可集成性等特点,为研究微腔内的光与物质相互作用提供了一个理想平台.本文首先介绍基于开放式法布里-珀罗微腔的腔量子电动力学系统的基本特性,然后介绍开放式法布里-珀罗微腔结构的制备方法,进而从弱耦合、强耦合和差发射体三方面着重介绍近年来开放式微腔与固态单量子系统相互作用的研究工作,最后进行了总结与展望.     

量子辐射场与经典流的相互作用：hw（4）线性非自治量子系统的代数动力…

利用代数动力学方法，分别在两种不同的规范条件下，得到了描述量子辐射场与经典流相互作用的ｈｗ（４）线性非自治量子系统在谐振子表象和相干态表象中的精确解及其Ｃａｒｔａｎ不变算子，建立和澄清了量子解与经典解之间存在的直接对应的规则。结果表明代数动力学方法对于具有非半单李代数结构的线性动力系统仍然适用。     

腔QED中利用超导量子干涉仪实现Toffoli门

基于腔量子电动力学技术,提出了利用三能级超导量子干涉仪实现Toffoli门的理论方案.利用超导量子干涉仪与腔场发生耦合,以及与外加经典脉冲发生共振跃迁来实现量子态的演化控制.该方案可以拓展到N比特Toffoli门的实现.最后,讨论了逻辑门的实验可行性,四比特Toffoli 门的作用时间约为30 nm,它远小于腔衰减时间...     

两模腔中的参量上转换和下转换

提出了一种通过建立双线性二次哈密顿量在量子腔中实现参量上转换和下转换的方案.通常在非线性过程中,介质本身不参与能量的净交换,但光波频率可以发生转换的作用称为参量转换作用.此方案建立在一个四能级原子同时与两经典场和两量子场相互作用的基础上,理论属于非线性光学四波混频范畴.将原子制备在合适的能级上,经典光场与相应的能级发生...     

QED中相互作用场的量子化

提出在QED中利用自由场的量子化条件和场方程,可以全面解决独立和非独立的相互作用场中￠(x),Aμ(x)的量子化问题.证明了:(1)当外规范场(x)≠0时,￠(x)与Aμ(x)相互独立,它与常规的场量子化方法一致.(2)当(x)=0时,￠(x)与Aμ(x)不再相互独立,常规的量子化方法不再适用,而本文提出的方法继续有效.并以1+1维QED作为实例.     

Asymptotic Entanglement Sudden Death in Two Atoms with Dipole–Dipole and Ising Interactions Coupled to a Radiation Field at Non-Zero Detuning

We investigate the time evolution and asymptotic behavior of a system of two two-level atoms (qubits) interacting off-resonance with a single mode radiation field. The two atoms are coupled to each other through dipole–dipole as well as Ising interactions. An exact analytic solution for the system dynamics that spans the entire phase space is provided. We focus on initial states that cause the system to evolve to entanglement sudden death (ESD) between the two atoms. We find that combining the Ising and dipole–dipole interactions is very powerful in controlling the entanglement dynamics and ESD compared with either one of them separately. Their effects on eliminating ESD may add up constructively or destructively depending on the type of Ising interaction (Ferromagnetic or anti-Ferromagnetic), the detuning parameter value, and the initial state of the system. The asymptotic behavior of the ESD is found to depend substantially on the initial state of the system, where ESD can be entirely eliminated by tuning the system parameters except in the case of an initial correlated Bell state. Interestingly, the entanglement, atomic population and quantum correlation between the two atoms and the field synchronize and reach asymptotically quasi-steady dynamic states. Each one of them ends up as a continuous irregular oscillation, where the collapse periods vanish, with a limited amplitude and an approximately constant mean value that depend on the initial state and the system parameters choice. This indicates an asymptotic continuous exchange of energy (and strong quantum correlation) between the atoms and the field takes place, accompanied by diminished ESD for these chosen setups of the system. This system can be realized in spin states of quantum dots or Rydberg atoms in optical cavities, and superconducting or hybrid qubits in linear resonators.     

Dynamical Properties of Two Coupled Dissipative QED Cavities Driven by Coherent Fields

When two identical QED cavities driven by the coherent fields are located in a uniform environment, in addition to dissipation, there appears an indirect coupling between the two cavities induced by the background fields. We investigate the effects of the coherent fields, the dissipation as well as the incoherent coupling on the following dynamical properties of the system： photon transfer, reversible decoherence, and quantum state transfer, etc. We find that the photons in the cavities do not leak completely into the environment due to the collective coupling between the cavities and the enviroment, and the photons are transferred irreversibly from the cavity with more photons to the cavity with less ones due to the incoherent coupling so that they are equally distributed among the two cavities. The coherent field pumping on the two cavities increases the mean photons, complements the revived magnitude of the reversible decoherence, but hinders the quantum state transfer between the two cavities. The above phenomena may find applications in quantum communication and other basic fields.     

Dynamical Properties of Two Coupled Dissipative QED Cavities Driven by Coherent Fields

When two identical QED cavities driven by the coherent fields are located in a uniform environment, in addition to dissipation, there appears an indirect coupling between the two cavities induced by the background fields. We investigate the effects of the coherent fields, the dissipation as well as the incoherent coupling on the following dynamical properties of the system: photon transfer, reversible decoherence, and quantum state transfer, etc. We find that the photons in the cavities do not leak completely into the environment due to the collective coupling between the cavities and the enviroment, and the photons are transferred irreversibly from the cavity with more photons to the cavity with less ones due to the incoherent coupling so that they are equally distributed among the two cavities. The coherent field pumping on the two cavities increases the mean photons, complements the revived magnitude of the reversible decoherence, but hinders the quantum state transfer between the two cavities. The above phenomena may find applications in quantum communication and other basic fields.     

两个双能级原子与双模腔场的拉曼相互作用

研究了两个双能级原子与双模辐射腔场的拉曼相互作用，计算了两个原子与腔场具有相同耦合常数但同时考虑原子间偶极一偶极相互作用情形下的辐射谱．讨论了双模腔场处于不同数态时辐射谱的新特点．     

"两原子-双模腔场"系统的腔场谱

研究了存在偶极相互作用的两等同原子与双模腔场共振相互作用双光子过程的腔场谱,研究发现,当两模初态都为光子数态或相干态时,两模腔场谱之间有很强的相互影响,在两模场强相同时,两划的光谱结构也相同,且在强场下呈现三峰结构;当两模初态场强不同时,较强的一模出现简单的单峰结构,而较弱模光谱中三峰的距离随另一模光子数的增加而增大。当两模均为压缩真空态时,在强场下得到经典共振荧光谱,且两模腔场谱之间的相互影响很弱。     

两个原子与双模腔场多光子相互作用过程中光场的相位性质

研究了偶极－偶极关联的两个全同二能级原子与双模强相干光场多光子共振相互作用过程中光场相位的演化性质,分别讨论了三种不同原子初态下,初态场强度和原子间偶极相互作用对光场相位概率分布,相位扩散及频率漂移的影响。     

中国区临近空间太阳辐射环境研究

临近空间(20~50km)航空活动是全世界航空大国竞相研究的热点。太阳辐射环境研究是开展该高度层航空活动的必要前提,然而临近空间辐射观测资料空白对其开发利用造成了障碍。臭氧是影响高空辐射环境的关键因子,基于欧洲中尺度预报中心再分析资料对中国区临近空间臭氧的空间分布、季节变化特征进行了分析,发现其时空分布及演变具备区域性特点,同时根据平流层大气数据及地表特征等将中国临近空间划分为5个区域,确定不同区域关键参数值,利用SBDART辐射传输模型对临近空间全波段太阳辐射及紫外辐射分别进行模拟。模拟结果显示受纬度、臭氧总量、垂直分布等影响,辐射值变化规律较为复杂。全波段太阳辐射年均和逐月值随纬度降低而增大,年较差则相反;大气的吸收作用与纬度、海陆差异有关,表现出不同的强度和季节变化特征;在紫外波段,南海上空辐射最强,年较差小,月较差很小且夏强冬弱,其他区域辐射值夏强冬弱,月较差呈双峰特征,春秋强,冬夏弱;大气的吸收作用受多因子影响,除南海外,各区域夏季辐射垂向差异更大;大气吸收引起的月较差垂向变化均表现为6、7月高低空月振幅一致,其它月份辐射值在高层月较差更大。     

级联环境下双原子的纠缠动力学

文献Phys.Rev.A 90,042108(2014)提出了一种级联环境模型,即单量子系统与光学腔作用,而腔又级联着一个有结构的零温玻色热库。本文在此基础上,研究两个二能级原子在该级联环境下的纠缠动力学,考察原子与腔场的耦合强度、原子间的偶极-偶极相互作用、热库的谱宽度、腔场与库间的失谐对原子间纠缠以及两原子与腔组成的三体纠缠动力学的影响。结果表明,在一定条件下两原子间的二体纠缠和原子-腔的三体纠缠在长时极限下都趋于稳定值,且随着偶极-偶极相互作用增加而增大,而无论腔场与热库耦合强弱,失谐量的增加都可以抑制纠缠的衰减。