Conjugate Fabry-Perot cavity pair for improved astro-comb accuracy

We propose a new astro-comb mode-filtering scheme composed of two Fabry-Perot cavities (coined "conjugate Fabry-Perot cavity pair"). Simulations indicate that this new filtering scheme makes the accuracy of astro-comb spectral lines more robust against systematic errors induced by nonlinear processes associated with power-amplifying and spectral-broadening optical fibers.     

从自散焦到自聚焦的动态转换和相位共轭亮空间孤子

对文献[1]中所报道的LiNbO3:Fe晶体从自散焦到自聚焦动态转换的过程,在实验和理论上作了进一步研究.以实验结果为依据,提出了相位共轭共振腔的理论模型,分析了该共振腔在从自散焦到自聚焦的动态转换过程中所起的作用,并提出了一种新型的亮空间孤子,即相位共轭亮空间孤子,指出相位共轭亮空间孤子是相位共轭共振腔中的一个模 关键词： 相位共轭共振腔 亮空间孤子 自散焦 自聚焦     

STF数字微波低电平系统研究

STF是KEK为国际直线对撞机(ILC)建立的试验装置. 在STF中, 数字微波低电平系统用于控制超导腔的RF相位和幅度. 在没有实际腔运行的情况下, 设计了一个基于FPGA技术的实时超导腔模拟器, 用于测试微波低电平系统的硬件和算法. 超导腔的数字控制器用FPGA实现, 其中采用了PI反馈控制和前馈控制算法. 测试表明, 超导腔模拟器和控制器都工作良好, 可用于STF微波低电平系统的进一步开发.     

波长扫描法布里-珀罗干涉仪的优化设计

分析了可用于绝对距离测量的波长扫描法布里－珀罗干涉仪腔内多光束干涉对输出信号的影响, 及由此产生的相位测量误差。研究表明, 通过选择合适的腔端面反射率和参考腔长度可以减小相位测量误差。优化选择的腔面反射率为０．１０～０．１５, 参考腔长为０．９５ ｍ ｍ , 在１ ｍ ｍ 范围内系统可达到０．０５ μｍ 的测距精度。     

Entanglement and Bell violation with phase decoherence or dissipation

The system of an atom couples to two distinct optical cavities with decoherence is studied by making use of a dynamical algebraic method. We adopt the concurrence to characterize the entanglement between atom and cavities or between two optical cavities in the presence of the phase decoherence or dissipation. It is found that the entanglement between atom and cavities can be controlled by adjusting the detuning parameter. We show that even if the atom is initially prepared in a maximally mixed state, it can also entangle the two mode cavity fields. Finally, the Bell violation of the cavity fields is discussed, and it is shown that both the detuning and decoherence can deteriorate the maximal amount of violation of Bell inequality for two mode cavity fields during the evolution.     

Mott-insulating and glassy phases of polaritons in 1D arrays of coupled cavities

By means of analytical and numerical methods we analyze the phase diagram of polaritons in one-dimensional coupled cavities. We locate the phase boundary, discuss the behavior of the polariton compressibility and visibility fringes across the critical point, and find a nontrivial scaling of the phase boundary as a function of the number of atoms inside each cavity. We also predict the emergence of a polaritonic glassy phase when the number of atoms fluctuates from cavity to cavity.     

三个耦合腔系统中的纠缠特性

本文研究将三个二能级原子分别囚禁在耦合腔A, B和C中, 腔中原子与腔场发生共振相互作用的情况. 采用Negativity熵度量两子系统间的纠缠, 通过数值计算给出了两个原子之间和两个腔场之间的纠缠演化. 讨论了腔场间的耦合强度对纠缠特性的影响. 研究结果表明: 原子间的纠缠与腔场间的耦合系数间存在非线性关系. 另一方面, 相邻腔场腔A和腔B间, 以及腔B和腔C间的纠缠随腔场间的耦合系数增大而减弱, 但非相邻腔场腔A和腔C间的纠缠却随腔场间的耦合系数增大而增强.     

两重外腔的自混合干涉及其信号分析

提出了具有两重外腔的自混合干涉。根据半导体激光器的自混合干涉理论，研究了两重外腔自混合干涉模型，及其信号的调制和解调方法。该方法用一个附加的参考反射镜在半导体激光器(LD)和目标间形成两重外腔，参考外腔用于补偿光学频率涨落引入的相位误差。用快速傅立叶变换相位探测技术(FFT)分析自混合干涉信号。运用这些方法，可提高相位测量精度，在微光机电系统、光学工程和其他工程应用上有潜在的实用价值。     

反射系数相位法计算谐振腔外观品质因数的局限性

 分析了反射系数相位法原理中所采用的完全耦合电路和实际等效电路之间的差异，指出采用反射系数相位法计算谐振腔外观品质因数失效的原因是：传输线与谐振腔只通过部分电感耦合；π模双间隙腔中存在耦合槽。定量计算表明：当谐振腔中耦合电感与非耦合电感之比小于0.1，或者缝模频率小于2π模频率时，反射系数相位法就会失效。结合实际谐振腔的参数值进行分析得出：导致反射系数相位法失效的最主要原因是传输线与谐振腔只通过部分电感耦合，并且耦合电感太小。     

Evaluation of Doppler shifts to improve the accuracy of primary atomic fountain clocks

We demonstrate agreement between measurements and ab initio calculations of the frequency shifts caused by distributed cavity phase variations in the microwave cavity of a primary atomic fountain clock. Experimental verification of the finite element models of the cavities gives the first quantitative evaluation of this leading uncertainty and allows it to be reduced to δν/ν=±8.4×10(-17). Applying these experimental techniques to clocks with improved microwave cavities will yield negligible distributed cavity phase uncertainties, less than ±1×10(-17).     

Controlled Phase Flip Gate and Its Application in Low-Q Cavities by Single-Photon Input-Output Process

By employing an auxiliary cavity, we investigate the possibility to implement the conditional phase flip (CPF) gate on two atoms confined in separate low-Q cavities by single-photon input-output process, based on the Faraday rotation. This indicates a universal quantum computing available with sophisticated cavity QED techniques. As examples, we carry out generation of cluster states of distant atomic qubits and accomplish a teleportation based on Bell-state measurement in low-Q cavities.     

Controlled Phase Flip Gate and Its Application in Low-Q Cavities by Single-Photon Input-Output Process

By employing an auxiliary cavity, we investigate the possibility to implement the conditional phase flip (CPF) gate on two atoms confined in separate low-Q cavities by single-photon input-output process, based on the Faraday rotation. This indicates a universal quantum computing available with sophisticated cavity QED techniques. As examples, we carry out generation of cluster states of distant atomic qubits and accomplish a teleportation based on Bell-state measurement in low-Q cavities.     

The Influences of the Selective Atomic Measurement on Entanglement Properties in the System of Three Atoms Trapped in Two Distant Cavities Connected by an Optical Fiber

Three two-level atoms are trapped in two initially empty cavities connected by an optical fiber. The entanglement evolution between two atoms in the same cavity and the entanglement evolution between two cavities are investigated. The influence of the state-selective measurement of the atom trapped in the other cavity on the entanglement and that of fiber-cavity coupling coefficient on the entanglement are discussed. The results obtained show that atom-atom entanglement property is strengthened, and cavity-cavity entanglement property is weakened with increasing of the cavity-fiber coupling coefficient. On the other hand, the results also show that the entanglement between two cavities and that between two atoms in the same cavity can be strengthened through the state-selective measurement on the atom trapped in the other cavity.     

Input-output relations for a three-port grating coupled Fabry-Perot cavity

We analyze an optical three-port reflection grating by means of a scattering matrix formalism. Amplitude and phase relations among the three ports, i.e., the three orders of diffraction, are derived. Such a grating can be used as an all-reflective, low-loss coupler to Fabry-Perot cavities. We derive the input-output relations of a three-port grating coupled cavity and find distinct properties that are not present in two-port coupled cavities. The cavity relations further reveal that the three-port coupler can be designed such that the additional cavity port interferes destructively. In this case the all-reflective, low-loss, single-end Fabry-Perot cavity becomes equivalent to a standard transmissive, two-port coupled cavity.     

Quantum nondemolition measurement of transverse atomic position in Kapitza-Dirac atomic beam scattering

It is demonstrated that one can measure the distribution of the transverse position of an atom crossing one or more optical cavities by monitoring the phase of the standing wave fields in the cavities. For the atom-field interaction the Kapitza-Dirac regime is assumed; it is shown that in this regime the method represents a quantum nondemolition measurement of the atomic position. On the other hand it can be applied to prepare narrow distributions of the transverse atomic position. In order to show this, a numerical simulation is performed, which illustrates the collapse of a broad initial Gaussian wavepacket, which can be coherent or incoherent, to a distribution with narrow peaks. Preparing the cavity fields in a squeezed state, one can greatly enhance the impact of the cavity field measurements on the atomic density matrix.     

Ku波段径向线相对论速调管放大器的仿真与设计

高频段相对论速调管放大器(RKA)是近年来高功率微波领域的研究热点之一,其发展主要受限于模式竞争、相位抖动和效率偏低等问题。设计了一种径向线RKA,主要由输入腔、两组非均匀双间隙群聚腔和三间隙提取腔等四部分构成。通过比较单双间隙群聚腔与电子束互作用的耦合系数,说明了非均匀双间隙群聚腔具备对电子束较强的调制能力。前端加载TEM模式反射器的非均匀双间隙群聚腔的工作在TM01-π模式,Q值较大,有利于谐振腔之间的能量隔离。采用两组非均匀双间隙群聚腔级联的方式,在注入功率仅10 kW情况下,实现短漂移管长度下电子束深度群聚达110%。粒子模拟结果表明,该器件具有效率高的优点,在电子束电压400 kV,电流5 kA,磁场强度0.4 T条件下,得到功率825 MW,频率14.25 GHz,效率41%的微波输出。     

半导体超常媒质矩形谐振腔(英文)

设计并研究了两个有不同各向异性参数的半导体超常媒质矩形谐振腔,其中填充了部分右手半导体超常媒质和部分左手半导体超常媒质。通过作图法研究了充满非色散的右手半导体超常媒质和色散的左手半导体超常媒质的谐振腔中谐振模式的解。结果显示,谐振腔的谐振模式取决于半导体超常媒质的色散关系。讨论了每种谐振腔中包含的六种情况,分别表示两个区域的传播常数为实数和虚数的不同的组合,并且揭示了构建具有无相差特性的谐振腔的几何参数要求。     

弱相干场耦合腔系统中的纠缠特性

研究由三个全同的二能级原子与耦合腔构成的系统, 考虑腔场处于弱相干态的情况. 采用Negativity熵度量两子系统间的纠缠, 利用数值计算方法研究了两个原子之间和两个腔场之间的纠缠性质. 讨论了腔场间的耦合系数和腔场的强度对纠缠特性的影响. 研究结果表明: 随光场强度增大, 原子间纠缠和腔场间纠缠均增强. 另一方面, 随耦合腔的耦合系数增大, 两原子间的纠缠减弱, 腔A和腔B间的纠缠增强; 而腔B和腔C间的纠缠, 以及腔A和腔C间纠缠与腔场间的耦合系数间存在非线性关系.     

The Entanglement Properties in the Coupled-Cavity System with the Detuning between an Atom and Cavity Field

We consider the situation that two atomic ensembles are separately trapped in coupled single-mode cavities, and each atom non-resonantly interacts with cavity field via a one-photon hopping. By employing the negativity measure of entanglement, we investigate the temporal evolution of entanglements between the cavities as well as between the cavity and atomic ensemble. By means of the numerical calculations, we discuss the influences of the number of atoms in an atomic ensemble and the detuning on the entanglement. The results show that as the number of atoms increases, the entanglement between the cavities is strengthened, contrary the entanglement between atomic ensemble and cavity is weakened. On the other hand, as the detuning increases, the entanglement between the cavities is weakened, contrary the entanglement between atomic ensemble and cavity is strengthened.

     

Application of a phase conjugate Brillouin cavity for the generation of a train of short laser pulses

Summary An oscillator and a regenerative amplifier have been realized using a phase conjugate mirror in the amplifier laser cavity. The phase conjugate mirror, via stimulated Brillouin scattering, acts as a modulator owing to its time-depending reflectivity. A pulse-forming network applied to the amplifier increases the discharging time which contributes to get an output beam formed by a train having four short pulses. The shortest pulse was 2 ns FWHM long.