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121.
Based on the technique of integral within an ordered product of nonlinear bosonic operators we construct a kind of tripartite nonlinear entangled states, which can make up a complete set. As its application, we also derive nonlinear 3-mode charge-related entangled state. The essential point for constructing these states lies in choosing the appropriate charge operator.  相似文献   
122.
推导并用实验验证了光强与入射波前在单位像元面积里成近似线性关系,从而得到入射波前经CCD采样后的功率谱密度(PSD)公式.根据该公式,模拟分析了影响CCD采集系统的系统传递函数的各个因素:入射波前、CCD的填充因子及CCD的曝光时间,得出了他们与系统传递函数的定性关系,并且通过实验明确CCD曝光时间对高空间分辨率波前检测不确定度的影响,为高空间分辨率干涉设计提供了理论依据.  相似文献   
123.
基于TRNSYS的太阳能集热系统能量转化分析与优化   总被引:1,自引:0,他引:1  
建立了太阳能集热器非稳态数学模型。以工程实例为研究对象,借助于TRNSYS软件,分析不同集热器类型,集热面积,水箱容积,水箱流量对太阳能集热系统性能的影响。优化集热器和水箱设计参数,采用变流量水箱系统,对提高太阳能集热系统综合性能有指导意义。  相似文献   
124.
A quasi-cyclic low-density parity check (QC-LDPC) code is constructed by an improved stability of the shortest cycle algorithm for 160-Gb/s non-return zero differential quadrature phase shift keying (NRZ- DQPSK) optical transmission system with the fiber-based optical parametric amplifier (FOPA). The QC- --14 d LDPC code with stability of the shortest cycle reduces the bit error ratio (BER) to 10 an restrains the error floor effectively.  相似文献   
125.
We report a 3.75-Gb/s visible light communication(VLC) system thatusessingle-carrier frequency-domain equalization(SC-FDE) based on a single red–green–blue(RGB) light-emitting diode(LED),with the measured bit error rates(BERs) under a pre-forward-error-correction threshold of 3.8×10-3.The fundamental characteristics of an RGB-LED-based VLC system are measured.We also compare SC-FDE with OFDM in terms of peak-to-average power ratio and BER performance,which shows that SC-FDE outperforms the OFDM modulation scheme.  相似文献   
126.
127.
This paper presents a compact and low-power-based discrete-time chaotic oscillator based on a carbon nanotube field-effect transistor implemented using Wong and Deng's well-known model. The chaotic circuit is composed of a nonlinear circuit that creates an adjustable chaos map, two sample and hold cells for capture and delay functions, and a voltage shifter that works as a buffer and adjusts the output voltage for feedback. The operation of the chaotic circuit is verified with the SPICE software package, which uses a supply voltage of 0.9 V at a frequency of 20 kHz. The time series, frequency spectra, transitions in phase space, sensitivity with the initial condition diagrams, and bifurcation phenomena are presented. The main advantage of this circuit is that its chaotic signal can be generated while dissipating approximately 7.8 μW of power, making it suitable for embedded systems where many chaos-signal generators are required on a single chip.  相似文献   
128.
The Co Mg O and Co Mn Mg O catalysts are prepared by a co-precipitation method and used as the catalysts for the synthesis of carbon nanotubes(CNTs) through the catalytic chemical vapor deposition(CCVD). The effects of Mn addition on the carbon yield and structure are investigated. The catalysts are characterized by temperature programmed reduction(TPR) and X-ray diffraction(XRD) techniques, and the synthesized carbon materials are characterized by transmission electron microscopy(TEM) and thermo gravimetric analysis(TG). TEM measurement indicates that the catalyst Co Mg O enclosed completely in the produced graphite layer results in the deactivation of the catalyst. TG results suggest that the Co Mn Mg O catalyst has a higher selectivity for CNTs than Co Mg O. Meanwhile, different diameters of CNTs are synthesized by Co Mn Mg O catalysts with various amounts of Co content, and the results show that the addition of Mn avoids forming the enclosed catalyst, prevents the formation of amorphous carbon, subsequently promotes the growth of CNTs, and the catalyst with decreased Co content is favorable for the synthesis of CNTs with a narrow diameter distribution.The Co Mn Mg O catalyst with 40% Co content has superior catalytic activity for the growth of carbon nanotubes.  相似文献   
129.
130.
Based on the solvable spin-1/2 Heisenberg chain we demonstrate how two many-body systems are entangled due to their partial entanglement. The entanglement wave in the two spin chains displays a damped oscillation if the spin number is N 〉 3, and only propagates with a certain velocity depending on the coupling constant J. Moreover, the entanglement wave will be reflected on the other ends of the two spin chains. A simple scheme for transferring some special two-qubit states to other two distant qubits is also proposed.  相似文献   
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