用于凝视焦平面的多视场红外光学系统

红外光学系统决定着红外系统的工作模式与工作精度,影响系统的作用距离,是红外系统的重要组成部分。多视场光学系统可以用不同的视场对同一目标进行搜索、识别、跟踪与瞄准,在军事应用领域获得了广泛的应用。光学系统的结构形式影响红外系统的成像质量、性能指标、外形尺寸、价格成本、机电复杂程度等,因此研究和选取合适的多视场光学系统结构形式显得非常重要。对目前国内外应用于凝视焦平面探测器的多视场红外光学系统结构形式,如切换变焦、光学补偿变焦、机械补偿变焦、混合变焦、双光路变焦等进行了特点分析,比较了其优点与局限性,对光学设计人员合理选用多视场光学系统结构形式具有一定的理论指导作用和意义。     

粘弹性胶层中Ⅰ型裂纹的动态扩展

研究粘弹性胶层中Griffith裂纹在Ⅰ型载荷作用下,裂纹尖端动态应力强度因子和能量释放率的时间响应.首先,利用积分变换方法,推导出粘弹性层的控制方程组;其次,引入位错密度函数,并结合边界条件和界面连接条件,导出反映裂纹尖端奇异性的Cauchy型奇异积分方程组,然后,应用Chebyshev正交多项式化奇异积分方程组为代数方程组,并采用Schmidt方法对其数值求解,最后,经过Laplace逆变换,求得动态应力强度因子和能量释放率的时间响应.通过对材料参数的讨论,得到动应力强度因子和能量释放率随剪切松驰参量的减小而增大,随膨胀松弛参量的减小而减小,弹性参数对其影响较小.     

复杂系统能量传递-转换模型(Ⅰ)

(火用)效率是以(火用)的概念进行系统分析和综合的目标函数。它的定义是否正确和合理,将直接关系到这些工作的结果。 本文将复杂的生产系统看成一个复杂的能量传递-转换系统。如何正确和合理定义复杂的能量传递-转换系统(火用)效率,是一个尚未解决的问题。本文用文献[1]提出的“能量单元”概念,运用系统工程的方法,从考察能量单元间连接的关系上,提出了几种典型的复杂系统能量传递-转换模型及其(火用)效率定义式,由此明确节     

Observation of multiple charge density wave phases in epitaxial monolayer 1T-VSe2 film

As a special order of electronic correlation induced by spatial modulation, the charge density wave (CDW) phenomena in condensed matters attract enormous research interests. Here, using scanning—tunneling microscopy in various temperatures, we discover a hidden incommensurate stripe-like CDW order besides the ($sqrt{7}$ × $sqrt{3}$) CDW phase at low-temperature of 4 K in the epitaxial monolayer 1T-VSe₂} film. Combining the variable-temperature angle-resolved photoemission spectroscopic (ARPES) measurements, we discover a two-step transition of an anisotropic CDW gap structure that consists of two parts Δ₁ and Δ₂. The gap part Δ₁ that closes around ～ 150 K is accompanied with the vanish of the ($sqrt{7}$ × $sqrt{3}$) CDW phase. While another momentum-dependent gap part Δ₂ can survive up to ～ 340 K, and is suggested to the result of the incommensurate CDW phase. This two-step transition with anisotropic gap opening and the resulted evolution in ARPES spectra are corroborated by our theoretical calculation based on a phenomenological form for the self-energy containing a two-gap structure Δ₁ + Δ₂, which suggests different forming mechanisms between the ($sqrt{7}$ × $sqrt{3}$) and the incommensurate CDW phases. Our findings provide significant information and deep understandings on the CDW phases in monolayer 1T-VSe₂} film as a two-dimensional (2D) material.