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    • 1. 发明授权
    • Phase locked laser array
    • 锁相激光阵列
    • US4879721A
    • 1989-11-07
    • US274117
    • 1988-11-21
    • Michael T. BraskiCharles H. WissmanRichard A. TiltonPaul F. Robusto
    • Michael T. BraskiCharles H. WissmanRichard A. TiltonPaul F. Robusto
    • H01S3/03H01S3/07H01S3/0975H01S3/23
    • H01S3/073H01S3/0315H01S3/0975H01S3/2383
    • A laser array having effectively separate oscillation regions 70,72,74 that are locked in phase is formed with a ceramic body 60,64 having a single, unpartitioned and relatively wide cavity area 62. Effectively isolated separate side by side laser oscillation regions 70,72,74 within the cavity are provided by use of common reflector optics 66,68 on the respective ends of the common cavity, 62 with one of the end optic arrangements comprising a common substrate 100 provided with several separate areas 102,104,106 of high reflectivity, mutually spaced from one another by areas of relatively low reflectivity. Individual control of the several separate regions of laser energy oscillations is provided by employing a separate pair of exciting electrodes 76,78,82,84,88,90 for each such region and applying separate RF exciting signals to the separate pairs respectively. In a large array, whether using plural isolated regions of laser oscillations in a common cavity or plural bores 121,122,123,124,125 separated by intra-cavity partiitons 126,127,128,129, adjustment of exciting power 150,154 to the outer electrode pairs 134,135,142,143 provides frequency correction for distortion and phase de-locking due to transverse thermal gradients.
    • 具有锁定相位的具有有效分离的振荡区域70,72,74的激光器阵列由陶瓷体60,64形成,陶瓷体60,64具有单个未分开且相对较宽的腔区域62.有效隔离的并排激光振荡区域70, 通过使用公共空腔62的相应端部上的公共反射器光学器件66,68来提供空腔内的72,74,其中端部光学装置中的一个包括具有高反射率的多个单独区域102,104,106的公共基板100 由相对较低反射率的区域彼此间隔开。 通过为每个这样的区域采用单独的一对激励电极76,78,82,84,88,90并且分别向分离的对施加单独的RF激励信号来提供激光能量振荡的几个单独区域的单独控制。 在大阵列中,无论是在公共腔中使用激光振荡的多个隔离区域还是由腔室内部分126,127,128,129分隔的多个孔121,122,123,124,125,对外部电极对134,135,142,143的激发功率150,154的调节提供了用于失真和相位去锁定的频率校正 由于横向热梯度。
    • 4. 发明授权
    • FM laser transmitter
    • FM激光发射机
    • US4932775A
    • 1990-06-12
    • US274240
    • 1988-11-21
    • Charles H. WissmanMichael T. BraskiRichard A. Tilton
    • Charles H. WissmanMichael T. BraskiRichard A. Tilton
    • G01S7/491G01S17/32G01S17/87H01S3/03H01S3/139
    • H01S3/0315G01S17/32G01S17/87G01S7/4911G01S7/4917H01S3/139
    • A laser transmitter utilizes optical far field combination of two independent lasers (80,90) and variation of RF exciting power (86) to one (80) to produce sufficient frequency modulation. Two bores (122,124) within the same dielectric body (120) are provided with two independent sets of electrodes (134,135, 138,139) and two independent RF power sources (150,152). The lasers are operated at different frequencies and the beams transmitted in parallel adjacent paths to provide a combined far field optical beam component at the beat frequency of the two lasers. Variation of the frequency of one of the lasers provides frequency modulation of the far field beat frequency, enabling reception and demodulation of the modulated beam without use of a local oscillator laser at the receiver. The transmitter may also be used in a laser radar.
    • 激光发射器利用两个独立激光器(80,90)的光学远场组合和RF激励功率(86)到一(80)的变化以产生足够的频率调制。 在相同电介质体(120)内的两个孔(122,124)设置有两组独立的电极组(134,135,138,139)和两个独立的RF电源(150,152)。 激光器以不同的频率操作,并且光束以平行的相邻路径传输,以在两个激光器的拍频处提供组合的远场光束分量。 激光器之一的频率的变化提供了远场拍频的频率调制,使得能够在接收机处不使用本地振荡器激光器来调制波束的接收和解调。 发射机也可用于激光雷达。
    • 5. 发明授权
    • Collision laser
    • 碰撞激光
    • US4414671A
    • 1983-11-08
    • US308714
    • 1981-10-05
    • William E. Wells, Jr.S. Douglas MarcumLawrence W. DownesRichard A. Tilton
    • William E. Wells, Jr.S. Douglas MarcumLawrence W. DownesRichard A. Tilton
    • H01S3/09H01S3/097H01S3/22H01S3/223
    • H01S3/223H01S3/09H01S3/09707
    • Electromagnetic radiation (10) is provided in a gas mixture (12) including helium in the X(1) state and nitrogen in the Y(1) state. The helium is pumped to excite a high population density of its atoms from the X(1) state to the X(2) state; and photons (15) of suitable frequency are injected into the mixture (12) to excite, via a three-body radiative collision of an atom of X(2) with a molecule of Y(1) and a photon (15): a high population density of molecules of the nitrogen from the Y(1) state to the Y(3) state, followed by a substantially simultaneous return of a substantial portion of the excited helium atoms to the X(1) state and a substantial depopulation of the Y(3) state of the nitrogen, causing the molecules thereof to drop to the lower energy Y(2) state, thereby stimulating the emission from the nitrogen of two photons (10) at the same wavelength for each absorbed photon (15), and thus providing a total quantity of photon emission (10) with sufficient gain for amplification of electromagnetic radiation (10), and finally resulting in the depopulation of the molecules in the Y(2) state by autoionization.
    • 在包括X(1)中的氦和Y(1)状态的氮气的气体混合物(12)中提供电磁辐射(10)。 泵送氦气以将其原子的高人口密度从X(1)状态激发到X(2)状态; 并且将适当频率的光子(15)注入到混合物(12)中,以通过X(2)的原子与Y(1)的分子和光子(15)的三体辐射碰撞来激发: 从Y(1)状态到Y(3)状态的氮的分子的高人口密度,随后大部分激发的氦原子的大部分同时返回到X(1)状态,并且实质上减少 氮的Y(3)状态,使其分子下降到较低的能量Y(2)状态,由此针对每个吸收的光子(15)刺激相同波长的两个光子(10)的氮的发射, ,从而提供具有足够增益用于放大电磁辐射(10)的光子发射总量(10),并且最终导致通过自动离子化分解为Y(2)状态的分子。