在经典理论框架下,相干探测性能受限于散粒噪声对应的标准量子极限,而量子增强接收技术通过引入位移算子,采用关联的方式将经典的平衡零拍/零差探测转化为光子数态的测量,理论上可以突破标准量子极限并不断逼近Helstrom极限。无歧义量...在经典理论框架下,相干探测性能受限于散粒噪声对应的标准量子极限,而量子增强接收技术通过引入位移算子,采用关联的方式将经典的平衡零拍/零差探测转化为光子数态的测量,理论上可以突破标准量子极限并不断逼近Helstrom极限。无歧义量子态识别(Unambiguous State Discrimination,USD)是量子增强接收常用的识别判决策略之一。然而,由于微弱光信号的能量有限,传统的USD量子增强接收方法的适用微弱信号范围较小,微弱信号识别的错误率较高。提出了一种QPSK调制量子增强接收的混合测量优化方案,该方案首先通过二态零差测量将QPSK相干态的区分转化为BPSK相干态的区分,然后通过BPSK量子增强接收测量实现相干态的无歧义识别。仿真表明,混合测量方案在平均光子数在3.2~11.3之间优于经典的外差测量方案,而且比传统QPSK量子增强接收方案具有更大的适用信号范围。展开更多
A lossy high-impedance surface comprised of two layers of resistive frequency selective surfaces is employed to design a tunable electromagnetic absorber. The tunability is realized through changing the composite unit...A lossy high-impedance surface comprised of two layers of resistive frequency selective surfaces is employed to design a tunable electromagnetic absorber. The tunability is realized through changing the composite unit cell by moving the top layer mechanically. To explain the absorbing mechanism, an equivalent circuit model with an interacting coefficient is proposed. Then, simulations and measurements are carried out and agree well with each other. Results show that the complex structure with a thickness less than λ0/4 is able to achieve a wideband absorption in a frequency range from5.90 GHz to 19.73 GHz. Moreover, it is tunable in the operation frequency band.展开更多
文摘在经典理论框架下,相干探测性能受限于散粒噪声对应的标准量子极限,而量子增强接收技术通过引入位移算子,采用关联的方式将经典的平衡零拍/零差探测转化为光子数态的测量,理论上可以突破标准量子极限并不断逼近Helstrom极限。无歧义量子态识别(Unambiguous State Discrimination,USD)是量子增强接收常用的识别判决策略之一。然而,由于微弱光信号的能量有限,传统的USD量子增强接收方法的适用微弱信号范围较小,微弱信号识别的错误率较高。提出了一种QPSK调制量子增强接收的混合测量优化方案,该方案首先通过二态零差测量将QPSK相干态的区分转化为BPSK相干态的区分,然后通过BPSK量子增强接收测量实现相干态的无歧义识别。仿真表明,混合测量方案在平均光子数在3.2~11.3之间优于经典的外差测量方案,而且比传统QPSK量子增强接收方案具有更大的适用信号范围。
文摘A lossy high-impedance surface comprised of two layers of resistive frequency selective surfaces is employed to design a tunable electromagnetic absorber. The tunability is realized through changing the composite unit cell by moving the top layer mechanically. To explain the absorbing mechanism, an equivalent circuit model with an interacting coefficient is proposed. Then, simulations and measurements are carried out and agree well with each other. Results show that the complex structure with a thickness less than λ0/4 is able to achieve a wideband absorption in a frequency range from5.90 GHz to 19.73 GHz. Moreover, it is tunable in the operation frequency band.