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    • 3. 发明申请
    • Ultra-slow down and storage of light pulses, and altering of pulse spectrum
    • 光脉冲的超慢减速和脉冲光谱的改变
    • US20060115212A1
    • 2006-06-01
    • US11001492
    • 2004-11-30
    • Mehmet YanikShanhui Fan
    • Mehmet YanikShanhui Fan
    • G02B6/26
    • B82Y20/00G02B6/1225
    • Light pulses can be stopped and stored coherently, with an all-optical process that involves an adiabatic and reversible pulse bandwidth compression occurring entirely in the optical domain. Such a process overcomes the fundamental bandwidth-delay constraint in optics, and can generate arbitrarily small group velocities for light pulses with a given bandwidth, without the use of any coherent or resonant light-matter interactions. This is accomplished only by small refractive index modulations performed at moderate speeds and has applications ranging from quantum communications and computing to coherent all-optical memory devices. A complete time reversal and/or temporal/spectral compression and expansion operation on any electromagnetic field is accomplished using only small refractive index modulations and linear optical elements. This process does not require any nonlinear multi-photon processes such as four-wave mixing and thus can be implemented using on-chip tunable microcavity complexes in photonic crystals. The tuning process requires only small refractive index modulations, and moderate modulation speeds without requiring any high-speed electronic sampling.
    • 光脉冲可以被停止并相干地存储,其全光学过程涉及完全在光学域中发生的绝热和可逆的脉冲带宽压缩。 这种过程克服了光学中的基本带宽延迟约束,并且可以为具有给定带宽的光脉冲产生任意小的组速度,而不使用任何相干或共振的光物质相互作用。 这仅通过在中等速度下执行的小折射率调制来实现,并且具有从量子通信和计算到相干全光存储器件的应用。 在任何电磁场上的完全时间反转和/或时间/频谱压缩和扩展操作仅使用小的折射率调制和线性光学元件来实现。 该过程不需要诸如四波混频的任何非线性多光子过程,因此可以使用光子晶体中的片上可调谐微腔复合体来实现。 调谐过程只需要较小的折射率调制和适度的调制速度,而不需要任何高速电子采样。
    • 6. 发明授权
    • Omnidirectional multilayer device for enhanced optical waveguiding
    • 用于增强光波导的全向多层器件
    • US06463200B2
    • 2002-10-08
    • US09418344
    • 1999-10-14
    • Yoel FinkShanhui FanEdwin ThomasChiping ChenJohn Joannopoulos
    • Yoel FinkShanhui FanEdwin ThomasChiping ChenJohn Joannopoulos
    • G02B616
    • G02B6/02304G02B6/102
    • A device having at least one dielectric inner core region in which electromagnetic radiation is confined, and at least two dielectric outer regions surrounding the inner core region, each with a distinct refractive index. The outer regions confine electromagnetic radiation within the inner core region. The refractive indices, the number of outer regions, and thickness of the outer regions result in a reflectivity for a planar geometry that is greater than 95% for angles of incidence ranging from 0° to at least 80° for all polarizations for a range of wavelengths of the electromagnetic radiation. In exemplary embodiments, the inner core region is made of a low dielectric material, and the outer regions include alternating layers of low and high dielectric materials. In one aspect of the invention, the device is a waveguide, and in another aspect the device is a microcavity.
    • 具有至少一个电介质内芯区域的装置,其中电磁辐射被限制在其中,并且至少两个围绕内芯区域的电介质外部区域各自具有不同的折射率。 外部区域将电磁辐射限制在内芯区域内。 折射率,外部区域的数量和外部区域的厚度导致平面几何的反射率,对于所有极化的范围为0°至至少80°的入射角,其平均几何形状的反射率大于95% 波长的电磁辐射。 在示例性实施例中,内芯区域由低电介质材料制成,并且外部区域包括低介电材料和高介电材料的交替层。 在本发明的一个方面,该器件是波导,并且在另一方面,该器件是微腔。
    • 9. 发明授权
    • Optical sensor having a non-negligible source coherence length
    • 光学传感器具有不可忽略的源相干长度
    • US08437005B2
    • 2013-05-07
    • US13493844
    • 2012-06-11
    • Michel J.F. DigonnetShanhui FanSeth Lloyd
    • Michel J.F. DigonnetShanhui FanSeth Lloyd
    • G01C19/72
    • G01C19/721
    • An optical sensor, a method of configuring an optical sensor, and a method of using an optical sensor are provided. The optical sensor includes an optical waveguide having a length and a laser source optically coupled to the waveguide. The laser source has a coherence length. Light from the source is transmitted to the waveguide as a first signal propagating along the waveguide in a first direction and a second signal propagating along the waveguide in a second direction opposite to the first direction. The optical paths of the first signal and the second signal are substantially reciprocal with one another and the first signal and the second signal are combined together after propagating through the waveguide to generate a third signal. The coherence length is greater than 1 meter or is in a range between 200 microns and 10 centimeters.
    • 提供光学传感器,配置光学传感器的方法以及使用光学传感器的方法。 光学传感器包括具有光学耦合到波导的长度的光波导和激光源。 激光源具有相干长度。 源自光源的光作为沿着波导沿第一方向传播的第一信号被传输到波导,第二信号沿着与第一方向相反的第二方向沿着波导传播。 第一信号和第二信号的光路基本上彼此相互倒数,并且在通过波导传播之后将第一信号和第二信号组合在一起以产生第三信号。 相干长度大于1米或处于200微米至10厘米之间的范围内。