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    • 1. 发明授权
    • Generating terahertz frequency combs from quantum cascade lasers using nonlinear frequency mixing
    • 使用非线性频率混合从量子级联激光器生成太赫兹频率梳
    • US09509123B2
    • 2016-11-29
    • US14919383
    • 2015-10-21
    • Board of Regents, The University of Texas System
    • Mikhail A. BelkinKarun VijayraghavanSeungyong Jung
    • H01S5/00H01S5/34H01S5/10H01S5/125H01S5/50
    • H01S5/3401H01S5/0604H01S5/06258H01S5/1092H01S5/1096H01S5/12H01S5/1215H01S5/125H01S5/34H01S5/3402H01S5/5054H01S2302/02
    • Methods and systems include generating one or more mid-infrared frequencies based at least upon electron transitions in one or more quantum cascade heterostructures. The quantum cascade heterostructures are concurrently configured with a significant second-order nonlinear susceptibility, a significant third-order nonlinear susceptibility, and an insignificant group velocity dispersion. A set of mid-infrared frequencies (that may include a frequency comb) is generated in the quantum cascade heterostructures based at least upon a four-wave mixing of the one or more mid-infrared frequencies. The four-wave mixing arises at least from the significant third-order nonlinear susceptibility and the insignificant group velocity dispersion. A set of terahertz frequencies (that may include a frequency comb) is generated in the quantum cascade heterostructures based at least upon a difference frequency generation from mid-infrared frequency pairs selected from the set of mid-infrared frequencies. The difference frequency generation arises at least from the significant second-order nonlinear susceptibility.
    • 方法和系统包括至少在一个或多个量子级联异质结构中的电子跃迁产生一个或多个中红外频率。 量子级联异质结构同时配置有明显的二阶非线性磁化率,显着的三阶非线性磁化率和不显着的组速度色散。 至少基于一个或多个中红外频率的四波混频,在量子级联异质结构中产生一组中红外频率(可包括频率梳)。 四波混频至少从三阶非线性敏感性和不明显的群速度色散出现。 至少基于从所述一组中红外频率中选择的中红外频率对的差频产生,在量子级联异质结构中产生一组太赫兹频率(可包括频率梳)。 差异频率的产生至少来自于二阶非线性敏感度。
    • 4. 发明授权
    • Wavelength converter and wavelength conversion method
    • 波长转换器和波长转换方法
    • US06323992B1
    • 2001-11-27
    • US09342445
    • 1999-06-29
    • Yoshiyasu Ueno
    • Yoshiyasu Ueno
    • G02F1365
    • G02F2/004G02F1/365H01S5/5054
    • To a first nonlinear waveguide and a second nonlinear waveguide each having a refractive index which varies in response to the input of an optical signal, input optical signal pulses are inputted together with continuous light of a predetermined wave length said input optical signal pulses being caused to have a time delay corresponding to 0.6˜1.2 times the pulse width of said input optical signal pulses. Then, the phase of an optical signal outputted from the second nonlinear waveguide is adjusted to a predetermined amount with respect to the phase of an optical signal outputted from the first nonlinear waveguide, and the optical signal outputted from the first nonlinear waveguide and an output signal outputted from the second nonlinear waveguide are coupled, whereafter a wavelength component of the input optical signal pulse is removed from the coupled optical signal. Consequently, an output optical signal pulse of a wavelength different from that of the input optical signal pulse can be obtained while little wavelength chirping is generated.
    • 对于具有响应于光信号的输入而变化的折射率的第一非线性波导和第二非线性波导,输入光信号脉冲与预定波长的连续光一起输入,所述输入光信号脉冲被引导到 具有对应于所述输入光信号脉冲的脉冲宽度的0.6〜1.2倍的时间延迟。 然后,从第二非线性波导输出的光信号的相位相对于从第一非线性波导输出的光信号的相位被调整为规定量,从第一非线性波导输出的光信号和输出信号 耦合从第二非线性波导输出的输入光信号脉冲的波长分量从耦合光信号中去除。 因此,可以获得与输入光信号脉冲不同的波长的输出光信号脉冲,同时产生少量波长啁啾。
    • 6. 发明授权
    • Optical parametric diffuser
    • 光学参数扩散器
    • US5940206A
    • 1999-08-17
    • US813907
    • 1997-03-07
    • Kenji KurodaHideki Takakura
    • Kenji KurodaHideki Takakura
    • G02F1/35H01S5/50G02F1/39
    • H01S5/50G02F1/3536H01S5/5054
    • An optical parametric diffuser is provided with an optical mixer which receives inputs of a probe light of a wavelength .lambda..sub.1 and a pumping light of a wavelength .lambda..sub.2, multiplexes them, and generates an output signal light including a wavelength .lambda..sub.5 which is apart from the pumping light wavelength on the opposite side of the probe light wavelength by n.DELTA..lambda. (.DELTA..lambda.=.vertline..lambda..sub.1 -.lambda..sub.2 .vertline., n.gtoreq.2). The signal of a wavelength .lambda..sub.5 is then extracted by a band-pass filter. The optical mixer is made to have a peak in output signal generation efficiency at the wavelength .lambda..sub.5 so that an output light beam of the wavelength .lambda..sub.5 can be obtained from the probe light and the pumping light.
    • 光学参数漫射器设置有光学混合器,其接收波长λ1的探测光和波长λ2的泵浦光的输入,将其复用,并产生包括波长λ5的输出信号光 在探针光波长相反侧的泵浦光波长为n DELTAλ(DELTAλ= |λ1-λ2 |,n> / = 2)。 然后通过带通滤波器提取波长λ5的信号。 使得光学混合器在波长λ5处具有输出信号产生效率的峰值,使得可以从探测光和泵浦光获得波长λ5的输出光束。
    • 8. 发明申请
    • Generating Terahertz Frequency Combs from Quantum Cascade Lasers using Nonlinear Frequency Mixing
    • 使用非线性频率混频从量子级联激光器生成太赫兹频率梳
    • US20160156153A1
    • 2016-06-02
    • US14919383
    • 2015-10-21
    • Board of Regents, The University of Texas System
    • Mikhail A. BelkinKarun VijayraghavanSeungyong Jung
    • H01S5/10H01S5/125H01S5/34
    • H01S5/3401H01S5/0604H01S5/06258H01S5/1092H01S5/1096H01S5/12H01S5/1215H01S5/125H01S5/34H01S5/3402H01S5/5054H01S2302/02
    • Methods and systems include generating one or more mid-infrared frequencies based at least upon electron transitions in one or more quantum cascade heterostructures. The quantum cascade heterostructures are concurrently configured with a significant second-order nonlinear susceptibility, a significant third-order nonlinear susceptibility, and an insignificant group velocity dispersion. A set of mid-infrared frequencies (that may include a frequency comb) is generated in the quantum cascade heterostructures based at least upon a four-wave mixing of the one or more mid-infrared frequencies. The four-wave mixing arises at least from the significant third-order nonlinear susceptibility and the insignificant group velocity dispersion. A set of terahertz frequencies (that may include a frequency comb) is generated in the quantum cascade heterostructures based at least upon a difference frequency generation from mid-infrared frequency pairs selected from the set of mid-infrared frequencies. The difference frequency generation arises at least from the significant second-order nonlinear susceptibility.
    • 方法和系统包括至少在一个或多个量子级联异质结构中的电子跃迁产生一个或多个中红外频率。 量子级联异质结构同时配置有明显的二阶非线性磁化率,显着的三阶非线性磁化率和不显着的组速度色散。 至少基于一个或多个中红外频率的四波混频,在量子级联异质结构中产生一组中红外频率(可包括频率梳)。 四波混频至少从三阶非线性敏感性和不明显的群速度色散出现。 至少基于从所述一组中红外频率中选择的中红外频率对的差频产生,在量子级联异质结构中产生一组太赫兹频率(可包括频率梳)。 差异频率的产生至少来自于二阶非线性敏感度。
    • 10. 发明授权
    • Wavelength conversion device and wavelength conversion method
    • 波长转换装置和波长转换方法
    • US08279516B2
    • 2012-10-02
    • US12695435
    • 2010-01-28
    • Hitoshi Murai
    • Hitoshi Murai
    • H01S3/10
    • H04B10/299G02F1/353H01S5/5027H01S5/5054
    • A first wavelength converter of a wavelength-conversion device includes: an optical amplifier amplifying an incident light beam; a first dispersion flat fiber spreading the wavelength spectrum width of the amplified beam; and a first wavelength filter transmitting a predetermined wavelength bandwidth of the first fiber output beam. A center wavelength of the first wavelength converted beam is shifted by Δλ1 from that of the incident light beam. A second wavelength converter of the device does not include an optical amplifier and includes: a second dispersion flat fiber spreading the wavelength spectrum width of the first wavelength converted beam; and a second wavelength filter transmitting a predetermined wavelength bandwidth of the second fiber output beam. A center wavelength of the second wavelength converted beam is shifted by Δλ2 from that of the first wavelength converted beam. The Δλ1 and Δλ2 satisfy Δλ1+Δλ2=Δλ, Δλ1×Δλ2
    • 波长转换装置的第一波长转换器包括:放大入射光束的光放大器; 扩展放大光束的波长光谱宽度的第一色散平面光纤; 以及传输第一光纤输出光束的预定波长带宽的第一波长滤波器。 第一波长转换光束的中心波长与入射光束的中心波长偏移&Dgr;λ1。 该器件的第二波长转换器不包括光放大器,包括:扩展第一波长转换波束的波长光谱宽度的第二色散平面光纤; 以及传输第二光纤输出光束的预定波长带宽的第二波长滤波器。 第二波长转换光束的中心波长与第一波长转换光束的中心波长偏移&Dgr;λ2。 &Dgr;λ1和&Dgr;λ2满足&Dgr;λ1+&Dgr;λ2=&Dgr;λ,&Dgr;λ1×&Dgr;λ2<0和|&Dgr;λ1| <|&Dgr;λ2|。