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    • 8. 发明授权
    • Spin-coating compensation for an optical storage medium with a substrate
groove profile gradient
    • 具有衬底凹槽轮廓梯度的光学存储介质的旋涂补偿
    • US5500266A
    • 1996-03-19
    • US209149
    • 1994-03-10
    • James E. Durnin
    • James E. Durnin
    • G11B7/013G11B7/24G11B7/26B32B3/00
    • G11B7/24085G11B7/24G11B7/26Y10S430/146Y10T428/21
    • When a dye material layer is spin-coated on an optical storage medium of the type having grooves fabricated in a substrate thereof, the dye material layer surface has depressions in the vicinity of the grooves. These depressions have a profile which is a function of the distance from the center of the storage medium. To compensate for the radial dependence of the depressions, the geometry of the grooves is changed by varying the base dimension of the groove as a function of the distance from the center of the storage medium. In this manner, the difference in phase for radiation traversing the storage medium by an optical path that includes a groove as compared to an optical path that does not include an associated groove is constant as a function of distance from the center of the storage medium. The phase difference which is a constant as a function of distance from the center of the storage medium is important in the generation of signals used in tracking the groove.
    • 当将染料材料层旋涂在具有在其基材中制造的槽的类型的光学存储介质上时,染料材料层表面在凹槽附近具有凹陷。 这些凹陷具有与存储介质的中心的距离的函数的轮廓。 为了补偿凹陷的径向依赖性,通过根据从存储介质的中心的距离改变凹槽的基部尺寸来改变凹槽的几何形状。 以这种方式,与不包括关联凹槽的光路相比,通过包括凹槽的光路穿过存储介质的辐射的相位差是作为与存储介质的中心的距离的函数的常数。 作为与存储介质的中心的距离的函数的常数的相位差在生成用于跟踪凹槽的信号中是重要的。
    • 9. 发明授权
    • Diffraction free arrangement
    • 无衍射布置
    • US4887885A
    • 1989-12-19
    • US081394
    • 1987-08-04
    • James E. DurninJoseph H. Eberly
    • James E. DurninJoseph H. Eberly
    • G02B27/42G02B27/00G10K11/26G10K11/30
    • G02B27/0025G10K11/26
    • Arrangements are disclosed for generating a well defined traveling wave beam substantially unaffected by diffractive spreading. In different embodiments, the beam can be an electromagnetic wave, particle beam, a transverse beam, a longitudinal beam such as an acoustic beam, or any type of beam to which the Helmholtz generalized wave equation is applicable. Pursuant to the teachings herein, a beam is generated having a transverse dependence of a Bessel function, and a longitudinal dependence which is entirely in phaser form, which results in a beam having a substantial depth of field which is substantially unaffected by diffractive spreading. In first and second disclosed embodiments respectively, optical and acoustical beams are generated by placing a circular annular source of the beam in the focal plane of a focussing means, which results in the generation of a well defined beam thereby because the far field intensity pattern of an object is the Fourier transform thereof, and the Fourier transform of a Bessel function is a circular function. In a third disclosed embodiment, a microwave beam is generated by transmitting a coherent microwave beam sequentially through a phase modulator, having a periodic stop function pattern, and a spatial filter, whose transmittance is the modulus of the Bessel function, to generate a microwave beam having a transverse Bessel function profile.More specifically, several embodiments are disclosed of an integrated optical laser cavity and an integrated microwave maser cavity for increasing the efficiency of production of the laser or maser beam. The integrated laser and maser cavities are designed to generate directly from their own gain medium a Bessel-mode diffraction-free beam.
    • 公开了用于产生基本上不受衍射扩展影响的明确定义的行波束的布置。 在不同的实施例中,光束可以是电磁波,粒子束,横向光束,诸如声束的纵向光束,或者适用亥姆霍兹广义波方程的任何类型的光束。 根据本文的教导,产生具有贝塞尔函数的横向依赖性的波束,以及完全为相位器形式的纵向相关性,其导致具有基本上不受衍射扩展影响的实质景深的波束。 在第一和第二公开的实施例中,通过将光束的圆形环形光源放置在聚焦装置的焦平面中来产生光学和声波束,这导致产生良好限定的光束,由此由于远场强度图 目标是其傅立叶变换,贝塞尔函数的傅立叶变换是循环函数。 在第三个公开的实施例中,通过相干微波束依次传送具有周期性停止功能图案的相位调制器和透射率是贝塞尔函数的模量的空间滤波器来产生微波波束来产生微波波束 具有横向贝塞尔功能特征。 更具体地,公开了集成的光学激光腔和用于提高激光或激光束的生产效率的集成的微波激光器腔的几个实施例。 集成的激光和激光腔被设计成从其自身的增益介质直接生成贝塞尔模式无衍射光束。
    • 10. 发明授权
    • Diffraction free arrangement
    • 无衍射布置
    • US4852973A
    • 1989-08-01
    • US915187
    • 1986-10-03
    • James E. DurninJoseph H. Eberly
    • James E. DurninJoseph H. Eberly
    • G02B27/00G10K11/26
    • G10K11/26G02B27/0025Y10S359/90
    • Arrangements are disclosed for generating a well defined traveling wave beam substantially unaffected by diffractive spreading. In different embodiments, the beam can be an electromagnetic wave, particle beam, a transverse beam, a longitudinal beam such as an acoustic beam, or any type of beam to which the Helmholtz generalized wave equation is applicable. Pursuant to the teachings herein, a beam is generated having a transverse dependence of a Bessel function, and a longitudinal dependence which is entirely in phaser form, which results in a beam having a substantial depth of field which is substantially unaffected by diffractive spreading. In first and second disclosed embodiments respectively, optical and acoustical beams are generated by placing a circular annular source of the beam in the focal plane of a focusing means, which results in the generation of a well defined beam thereby because the far field intensity pattern of an object is the Fourier transform thereof, and the Fourier transform of a Bessel function is a circular function. In a third disclosed embodiment, a microwave beam is generated by transmitting a coherent microwave beam sequentially through a phase modulator, having a periodic step function pattern, and a spatial filter, whose transmittance is the modulus of the Bessel function, to generate a microwave beam having a transverse Bessel function profile.
    • 公开了用于产生基本上不受衍射扩展影响的明确定义的行波束的布置。 在不同的实施例中,光束可以是电磁波,粒子束,横向光束,诸如声束的纵向光束,或者适用亥姆霍兹广义波方程的任何类型的光束。 根据本文的教导,产生具有贝塞尔函数的横向依赖性的波束,以及完全为相位器形式的纵向相关性,其导致具有基本上不受衍射扩展影响的实质景深的波束。 在第一和第二公开的实施例中,通过将光束的圆形环形光源放置在聚焦装置的焦平面中来产生光学和声波束,这导致产生良好限定的光束,由此,由于远场强度图 目标是其傅立叶变换,贝塞尔函数的傅立叶变换是循环函数。 在第三个公开的实施例中,通过相干微波束顺序地通过具有周期性阶跃函数图案的相位调制器和透射率是贝塞尔函数的模量的空间滤波器来产生微波波束来产生微波波束, 具有横向贝塞尔功能特征。