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    • 3. 发明公开
    • Photonic crystal fibers for dispersion control in optical communication systems
    • Photonenkristall glasfaser zur Dispersionskontrolle in optischen Kommunikationssystemen
    • EP1148360A2
    • 2001-10-24
    • EP01301432.9
    • 2001-02-19
    • LUCENT TECHNOLOGIES INC.
    • Ranka, Jinendra KumarReed, William AlfredWindeler, Robert Scott
    • G02B6/16
    • G02B6/02366B82Y20/00G02B6/02266G02B6/29377
    • A fiber optic system comprises an optical transmitter, an optical receiver, and an optical fiber transmission path that optically couples the transmitter and the receiver to one another. The transmission path includes a first section that has negative dispersion at an operating wavelength λ o greater than about 1300 nm and a second section that includes a MOF. The MOF has relatively large anomalous dispersion at λ o and is sufficiently long to compensate the accumulated negative dispersion in the first section. In one embodiment the MOF comprises a core, a lower index cladding that includes one or more layers of air holes surrounding the core, characterized in that the diameter of the core is less than about 8 µm and the difference in effective refractive index between the core and cladding is greater than about 0.1 (10%). Preferably, the cladding contains no more than 2 layers of air holes and the distance between the nearest edges of adjacent air holes is less than about 1 µm.
    • 光纤系统包括光发射机,光接收机和将发射机和接收机彼此光耦合的光纤传输路径。 传输路径包括在大于约1300nm的工作波长λo处具有负色散的第一部分和包括MOF的第二部分。 MOF在λo处具有相对较大的异常色散,并且足够长以补偿第一部分中的累积负色散。 在一个实施例中,MOF包括芯,低折射率包层,其包括围绕芯的一层或多层空气孔,其特征在于,芯的直径小于约8μm,并且有效折射率之间的差异在 芯和包层大于约0.1(10%)。 优选地,包层包含不超过2层的气孔,并且相邻气孔的最近边缘之间的距离小于约1μm。
    • 4. 发明公开
    • Method of making preforms for optical waveguide devices
    • Verfahren zum Herstellen von Vorformenfüroptische Wellenleiter
    • EP0955273A1
    • 1999-11-10
    • EP99302854.7
    • 1999-04-13
    • LUCENT TECHNOLOGIES INC.
    • Atkins, Robert MichaelWindeler, Robert Scott
    • C03B37/018
    • C03B37/01807C03B37/01838C03B2201/12C03B2201/28C03B2201/34C03B2201/36C03B2201/40
    • Applicants have determined that much of the nonuniformity in solution doped preforms is due to nonuniformity of the soot layer caused by the high temperature necessary for complete reaction, and that MCVD fabrication using reaction temperature lowering gases such as nitrous oxide (N 2 O) can produce more uniform soot layers. The conventional oxygen/reactant gas mixture presents a very small temperature window in which a uniform silica soot layer can be deposited without sintering. If the temperature in oxygen is too low, SiCl 4 will not react completely and silicon oxychlorides will form. This degrades the soot layer and makes it unusable. If the temperature is too high the soot layer begins to sinter, decreasing the surface area and porosity. Adding a reaction temperature lowering gas lowers the reaction temperature and enables deposition of soot on the tube wall at a temperature substantially lower than the sintering temperature. This results in a more uniform, porous soot layer along the length of the preform and from one preform to another; and, in turn, the greater uniformity permits more uniform solution doping.
    • 申请人已经确定了溶液掺杂预制件中的大部分不均匀性是由于完全反应所需的高温引起的烟灰层的不均匀性,并且使用反应温度降低气体如一氧化二氮(N 2 O)的MCVD制造可以产生更均匀的 烟灰层。 常规的氧气/反应物气体混合物呈现非常小的温度窗口,其中可沉积均匀的二氧化硅烟灰层而不烧结。 如果氧气中的温度太低,SiCl4将不会完全反应,而形成硅氯化物。 这会降低烟灰层,使其不可用。 如果温度太高,烟灰层开始烧结,减少表面积和孔隙率。 添加反应降温气体降低了反应温度,并且能够在基本上低于烧结温度的温度下将烟灰沉积在管壁上。 这导致沿着预成型件的长度和从一个预制件到另一个的更均匀的多孔的烟灰层; 反过来,更大的均匀性允许更均匀的溶液掺杂。
    • 5. 发明公开
    • Decoupling of transverse spatial modes in microstructure optical fibers
    • 在微结构光纤在空间上横向模式的去耦
    • EP1130427A3
    • 2005-01-12
    • EP01301452.7
    • 2001-02-19
    • LUCENT TECHNOLOGIES INC.
    • Ranka, Jinendra KumarWindeler, Robert Scott
    • G02B6/16
    • G02B6/02366G02B6/02214
    • A properly designed MOF can simultaneously exhibit large anomalous dispersion at visible and near infrared wavelengths and support numerous transverse spatial modes that are essentially decoupled from one another, even in the presence of significant perturbations. In a MOF that includes an inner cladding region comprising at least one thin layer of air holes surrounding a core region, the key is to achieve a relatively large wave vector mismatch between the lowest order modes by appropriate design of the size of the core region and of the effective refractive index difference between the core region and the inner cladding region. In accordance with one aspect of our invention, MOFs are designed to exhibit simultaneously relatively large anomalous dispersion and essentially decoupled transverse spatial modes by making the diameter of the core region less than about 6 µm and the difference in effective refractive index between the core and cladding regions greater than about 0.1 (10%). Preferably, the cladding region contains no more than 2 layers of air holes, and the distance between the nearest edges of adjacent air holes is less than about 1 µm. MOFs with these features enable several embodiments of our invention. One embodiment is a nonlinear optical system comprising an optical pump source, an optical signal source, a utilization device and an optical fiber transmission path that optically couples the sources to the device. The transmission path includes at least a section of MOF in which at least two transverse modes are decoupled from one another over the length of the MOF section, the output of the pump source propagating in one of the transverse modes and the output of the signal source propagating in another of the transverse modes. Another embodiment is an optical transmission system comprising an optical transmitter, a utilization device and an optical fiber transmission path that optically couples the transmitter and the utilization device. The transmission path includes at least a section of MOF in which at least two of the transverse modes are decoupled from one another over the length of the MOF section, and further includes a first modulator for impressing information on a first optical signal to be propagated along the MOF in one of the transverse modes and a second modulator for impressing information on a second optical signal to be propagated along the MOF in another of the transverse modes.
    • 8. 发明公开
    • Article utilizing optical waveguides with anomalous dispersion at visible and near infrared wavelengths
    • 使用具有在可见光和近红外反常色散的波导装置
    • EP1054273A2
    • 2000-11-22
    • EP00303895.7
    • 2000-05-09
    • LUCENT TECHNOLOGIES INC.
    • Ranka, Jinendra KumarWindeler, Robert Scott
    • G02B6/16
    • G02B6/02366G02B6/02004G02B6/02214G02B6/02333G02B6/02361G02B6/02385G02F1/365G02F2001/3528G02F2202/32
    • Properly designed optical waveguides exhibit anomalous (positive) dispersion over a continuum of visible and near infrared wavelengths and, in one embodiment, the fiber has zero-dispersion at a visible wavelength (e.g., about 760 nm). Preferably, the zero-dispersion point occurs at a vis-nir wavelength where the normal (negative) material dispersion is relatively high and the effective refractive index difference between the core and the cladding is sufficiently large that the anomalous (positive) waveguide dispersion compensates the normal material dispersion. Illustratively, the optical waveguide is a microstructured fiber comprising a solid silica core surrounded by an inner cladding that includes a plurality of capillary air holes that allow for index-guiding within the core. The pattern formed by the cross-sections of the air holes, typically circles, may take on a variety geometric configurations, such as a closely packed hexagon or triangle. Alternatively, the cross-section of the air holes may form two mating, essentially semicircular regions on either side of a core that is supported by a pair of radial webs. As a result of the novel dispersion characteristics of the microstructured fibers combined with small effective area cores, we have demonstrated several applications of the invention that, in the prior art of standard single-mode fibers, have been possible only at wavelengths greater than about 1300 nm, including pulse compression, bright soliton propagation, fundamental mode-to-fundamental mode second harmonic generation, and broadband continuum generation in the visible.
    • 适当设计的光波导呈现反常(正的)色散在可见光和近红外波长的连续,并且在一个实施例中,纤维具有在可见波长(例如,约760nm)零色散。 优选地,所述零色散点在VIS-NIR波长,其中正常(负)的材料色散相对较高并且在芯和包层之间的有效折射率差发生足够大做了反常(正的)波导色散补偿 正常材料色散。 说明性地,该光波导是微结构化的光纤,其包括通过在内部包层包围的固体二氧化硅芯包括没有的毛细管空气的多个通孔并允许折射率波导的核心内。 由空气孔,通常圆的横截面所形成的图案可以采用多种几何构造,检查作为紧密堆积六边形或三角形。 可替代地,空气孔的横截面可以形成两个配合,基本上在芯一左一右半圆形区域也被一对径向网状物支撑。 由于结构化纤维与小有效面积核相结合的微的新颖色散特性的结果,我们已实例阐述了本发明的几个应用程序,标准单模光纤的在现有技术中,已经有可能仅在波长大于约1300 纳米,包括脉冲压缩,亮孤子传播,基本模式到模式从根本上二次谐波生成,和宽带连续谱产生在可见。