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    • 8. 发明授权
    • Tunable, diode side-pumped Er: YAG laser
    • 可调谐二极管侧泵浦Er:YAG激光器
    • US5623510A
    • 1997-04-22
    • US436690
    • 1995-05-08
    • Charles E. HamiltonLaurence H. Furu
    • Charles E. HamiltonLaurence H. Furu
    • H01S3/081H01S3/0941H01S3/106H01S3/16H01S3/091H01S3/094
    • H01S3/0941H01S3/081H01S3/1062H01S3/1608H01S3/1643
    • A discrete-element Er:YAG laser, side pumped by a 220 Watt peak-power InGaAs diode array, generates >500 mWatts at 2.94 .mu.m, and is tunable over a 6 nm range near about 2.936 .mu.m. The oscillator is a plano-concave resonator consisting of a concave high reflector, a flat output coupler, a Er:YAG crystal and a YAG intracavity etalon, which serves as the tuning element. The cavity length is variable from 3 cm to 4 cm. The oscillator uses total internal reflection in the Er:YAG crystal to allow efficient coupling of the diode emission into the resonating modes of the oscillator. With the tuning element removed, the oscillator produces up to 1.3 Watts of average power at 2.94 .mu.m. The duty factor of the laser is 6.5% and the repetition rate is variable up to 1 kHz. This laser is useful for tuning to an atmospheric transmission window at 2.935 .mu.m (air wavelength). The laser is also useful as a spectroscopic tool because it can access several infrared water vapor transitions, as well as transitions in organic compounds. Other uses include medical applications (e.g., for tissue ablation and uses with fiber optic laser scalpels) and as part of industrial effluent monitoring systems.
    • 由220瓦峰值功率InGaAs二极管阵列泵浦的离散元件Er:YAG激光器,在2.94微米处产生> 500mWat,并且在约2.936μm附近可调谐超过6nm。 该振荡器是由凹高反射器,扁平输出耦合器,Er:YAG晶体和YAG腔内标准具组成的平凹谐振器,用作调谐元件。 腔长度从3厘米到4厘米不等。 振荡器在Er:YAG晶体中使用全内反射,以使二极管发射有效耦合到振荡器的谐振模式。 调谐元件去除后,振荡器产生高达1.3瓦的平均功率为2.94微米。 激光器的占空比为6.5%,重复率可变为1 kHz。 该激光器可用于调谐到2.935微米(空气波长)的大气透射窗口。 激光也可用作光谱工具,因为它可以访问几个红外水蒸气跃迁以及有机化合物的转变。 其他用途包括医疗应用(例如用于组织消融和使用光纤激光解剖刀),并且作为工业污水监测系统的一部分。
    • 9. 发明授权
    • Tunable pulsed titanium:sapphire laser and conditions for its operation
    • 可调脉冲钛:蓝宝石激光器及其操作条件
    • US5081630A
    • 1992-01-14
    • US414886
    • 1989-09-29
    • Dennis D. LowenthalClifford H. MullerCharles E. HamiltonDean R. GuyerKenneth W. Kangas
    • Dennis D. LowenthalClifford H. MullerCharles E. HamiltonDean R. GuyerKenneth W. Kangas
    • H01S3/08H01S3/1055
    • H01S3/1055H01S3/08036
    • A laser system for producing pulsed, longitudinal mode optical energy over a widely tunable range of wavelengths. The system includes an optical cavity and a solid-state gain medium. The optical cavity comprises first, second, and third optical element means. The first optical element means reflects energy received along a first reflective optical axis and directs the energy toward the second optical element means, which diffracts the optical energy into at least two orders of interference. The energy diffracted according to a first order of interference is reflected back toward the second optical element means by a third optical element means, thereby creating a resonant optical cavity. Another portion of the optical energy diffracted by the second optical element means is produced as an output beam. The solid-state gain medium is located on the optical axis between the first and second optical element means and receives pump energy from a plurality of pump beams that are within two degrees of being colinear with the first reflective optical axis. The solid-state gain medium converts the pump beam energy to optical energy having a desired wavelength with a very high efficiency, without required pump beam energy densities above a predetermined level. The laser system is tunable by moving the third optical element means with respect to the second optical element means, thereby causing optical energy at a tunable wavelength to resonate within the optical cavity.
    • 一种用于在广泛可调波长范围内产生脉冲,纵向模式光能的激光系统。 该系统包括光腔和固态增益介质。 光腔包括第一,第二和第三光学元件装置。 第一光学元件意味着反射沿着第一反射光轴接收的能量并且将能量引导到第二光学元件装置,其将光能衍射为至少两个干涉级。 根据第一干涉级衍射的能量通过第三光学元件装置反射回第二光学元件装置,由此产生共振光学腔。 产生由第二光学元件装置衍射的光能的另一部分作为输出光束。 固态增益介质位于第一和第二光学元件装置之间的光轴上,并且从与第一反射光轴共线的两个角度内的多个泵浦光束接收泵浦能量。 固态增益介质以非常高的效率将泵浦能量转换成具有期望波长的光能,而不需要高于预定水平的泵浦光束能量密度。 激光系统可通过相对于第二光学元件装置移动第三光学元件装置来调节,从而使可调波长的光能在光学腔内谐振。
    • 10. 发明授权
    • Osmotic fiber systems
    • 渗透纤维系统
    • US4805343A
    • 1989-02-21
    • US920440
    • 1986-10-20
    • James A. PattersonRobert M. PiecuchCharles E. Hamilton
    • James A. PattersonRobert M. PiecuchCharles E. Hamilton
    • A01G27/04B01D63/02B01D67/00B01D69/08A01G27/00
    • B01D67/0086A01G27/04B01D63/02B01D67/0088B01D69/08B01D2313/23
    • A hollow fiber formed of hydrophilic material and having permeable walls is treated to enhance the permeability. Reactions used to treat the fiber have a gas inside and gas outside, a gas inside and liquid outside, a liquid inside and gas outside, and a liquid inside and a liquid outside. The treatments generally involve the plasticizing of the fiber material while having the inside of the fiber at a higher pressure than the outside. These treatments produce a structural change in the fiber from a flexible tube having strong walls to expanded, rigid and somewhat fragile walls. Where more than a short length of the treated fiber is to be used, an open mesh cage is used to confine the fiber to a desired volume during treatment and to protect it subsequently. A technique for joining flexible tubing to the treated fiber is presented. The treated fiber may be used in apparatus and methods involving osmosis and reverse osmosis. Novel plant irrigation methods and apparatus are disclosed, and structures for changing the solvent quanties of solutes and measuring the osmotic pressures of solutions are also presented.
    • 处理由亲水材料形成且具有可渗透壁的中空纤维以增强渗透性。 用于处理纤维的反应具有内部气体和外部气体,内部气体和液体外部,内部液体和气体外部,以及液体内部和液体外部。 处理通常涉及纤维材料的增塑,同时纤维内部的压力高于外部。 这些处理从具有强壁的柔性管到膨胀的,刚性的和稍微脆弱的壁产生纤维中的结构变化。 在使用多于短长度的经处理的纤维的情况下,使用开式网状笼来在处理期间将纤维限制在所需体积并随后进行保护。 提出了将柔性管连接到经处理的纤维的技术。 经处理的纤维可用于涉及渗透和反渗透的设备和方法中。 还提出了新型植物灌溉方法和装置,并提出了改变溶质溶剂量和测定溶液渗透压的结构。