CN107806981A - A Measuring Device for Beat Length of Polarization Maintaining Optical Fiber - Google Patents
A Measuring Device for Beat Length of Polarization Maintaining Optical Fiber Download PDFInfo
- Publication number
- CN107806981A CN107806981A CN201711130297.3A CN201711130297A CN107806981A CN 107806981 A CN107806981 A CN 107806981A CN 201711130297 A CN201711130297 A CN 201711130297A CN 107806981 A CN107806981 A CN 107806981A
- Authority
- CN
- China
- Prior art keywords
- polarization
- optical fiber
- fiber
- maintaining
- light source
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01M—TESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
- G01M11/00—Testing of optical apparatus; Testing structures by optical methods not otherwise provided for
- G01M11/30—Testing of optical devices, constituted by fibre optics or optical waveguides
- G01M11/33—Testing of optical devices, constituted by fibre optics or optical waveguides with a light emitter being disposed at one fibre or waveguide end-face, and a light receiver at the other end-face
- G01M11/331—Testing of optical devices, constituted by fibre optics or optical waveguides with a light emitter being disposed at one fibre or waveguide end-face, and a light receiver at the other end-face by using interferometer
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01M—TESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
- G01M11/00—Testing of optical apparatus; Testing structures by optical methods not otherwise provided for
- G01M11/30—Testing of optical devices, constituted by fibre optics or optical waveguides
- G01M11/33—Testing of optical devices, constituted by fibre optics or optical waveguides with a light emitter being disposed at one fibre or waveguide end-face, and a light receiver at the other end-face
- G01M11/336—Testing of optical devices, constituted by fibre optics or optical waveguides with a light emitter being disposed at one fibre or waveguide end-face, and a light receiver at the other end-face by measuring polarization mode dispersion [PMD]
Landscapes
- Physics & Mathematics (AREA)
- Chemical & Material Sciences (AREA)
- Optics & Photonics (AREA)
- Analytical Chemistry (AREA)
- General Physics & Mathematics (AREA)
- Dispersion Chemistry (AREA)
- Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)
Abstract
Description
技术领域technical field
本发明涉及保偏光纤拍长的测量领域,具体为一种保偏光纤拍长的测量装置。The invention relates to the field of measuring the beat length of polarization-maintaining optical fibers, in particular to a measuring device for the beat length of polarization-maintaining optical fibers.
背景技术Background technique
保偏光纤传输线偏振光,广泛用于航天、航空、航海、工业制造技术及通信等过民经济的各个领域。在以光学相干检测为基础的干涉型光纤传感器中,使用保偏光纤能够保证线偏振方向不变,提高相干信噪比,以实现对物理量的高精度测量。保偏光纤作为一种特种光纤,主要应用于光纤陀螺,光纤水听器等传感器和DWDM、EDFA等光纤通信系统。Polarization-maintaining optical fiber transmits linearly polarized light, and is widely used in various fields of national economy such as aerospace, aviation, navigation, industrial manufacturing technology and communication. In the interferometric optical fiber sensor based on optical coherent detection, the use of polarization-maintaining optical fiber can ensure that the linear polarization direction remains unchanged, improve the coherent signal-to-noise ratio, and achieve high-precision measurement of physical quantities. As a special optical fiber, polarization maintaining optical fiber is mainly used in optical fiber gyroscopes, optical fiber hydrophones and other sensors and optical fiber communication systems such as DWDM and EDFA.
高双折射保偏光纤在光纤陀螺,光纤电流互感器和保偏光器件等领域有广泛的应用。在这些应用中,保偏光纤的保偏性能是决定其应用的关键,一般用拍长来衡量保偏光纤的保偏性能。它反映的就是保偏光纤两偏振本征轴折射率差的大小,即保偏光纤双折射。High birefringence polarization-maintaining fibers are widely used in fields such as fiber optic gyroscopes, fiber optic current transformers, and polarization-maintaining optical devices. In these applications, the polarization-maintaining performance of the polarization-maintaining fiber is the key to determine its application. Generally, the beat length is used to measure the polarization-maintaining performance of the polarization-maintaining fiber. It reflects the difference in refractive index between the two polarization eigen axes of the polarization maintaining fiber, that is, the birefringence of the polarization maintaining fiber.
偏光纤拍长的测量主要有扭转法、压力法、电光或磁光调制法、光偏振法、剪断法、偏振模色散法、棱镜耦合法、瑞利散射法、波长扫描法、光频域反射计等方法。保偏光纤在拉制过程中,由于光纤内部产生的结构缺陷会造成保偏性能的下降,本发明提供一种保偏光纤拍长的测量装置。The measurement of polarized fiber beat length mainly includes torsion method, pressure method, electro-optical or magneto-optical modulation method, optical polarization method, shearing method, polarization mode dispersion method, prism coupling method, Rayleigh scattering method, wavelength scanning method, optical frequency domain reflection counting and other methods. During the drawing process of the polarization-maintaining optical fiber, the structural defects generated inside the optical fiber will cause the degradation of the polarization-maintaining performance. The invention provides a measuring device for the beat length of the polarization-maintaining optical fiber.
发明内容Contents of the invention
本发明要解决的技术问题是克服现有保偏光纤在工作过程中,保偏性能难以检测的缺陷,提供一种保偏光纤拍长的测量装置,从而解决上述问题。The technical problem to be solved by the present invention is to overcome the defect that the polarization maintaining performance of the existing polarization maintaining optical fiber is difficult to detect during the working process, and provide a measurement device for the beat length of the polarization maintaining optical fiber, so as to solve the above problems.
为了解决上述技术问题,本发明提供了如下的技术方案:In order to solve the problems of the technologies described above, the present invention provides the following technical solutions:
本发明一种保偏光纤拍长的测量装置,包括包括宽谱光源、光纤起偏器、频谱仪和计算机,宽谱光源经过光纤起偏器进入待测高双折射保偏光纤,待测高双折射保偏光纤末端连接有检偏器,检偏器信号输出端有电光调制器电光调制器上的光载微波信号经过色散光纤后入射到高速光电探测器上,高速光电探测器上的微波信号通过低噪放放大后经过一个微波功分器后,一部分微波信号注入到电光调制器中,一部分微波信号经过频谱仪到达计算机。The present invention is a kind of measurement device of polarization-maintaining optical fiber beat length, which comprises wide-spectrum light source, optical fiber polarizer, spectrum analyzer and computer. The end of the birefringent polarization-maintaining fiber is connected with a polarizer, and the signal output of the polarizer has an electro-optic modulator. The optical-carrying microwave signal on the electro-optic modulator is incident on the high-speed photodetector after passing through the dispersion fiber, and the microwave on the high-speed photodetector After the signal is amplified by a low-noise amplifier and passes through a microwave power divider, a part of the microwave signal is injected into the electro-optical modulator, and a part of the microwave signal reaches the computer through the spectrum analyzer.
作为本发明的一种优选技术方案,待测高双折射保偏光纤与光纤起偏器采用熔接的方式连接,熔接角度为45°,使其连接处非常紧密结实,不会出现空隙。As a preferred technical solution of the present invention, the high birefringence polarization-maintaining optical fiber to be tested is connected to the optical fiber polarizer by welding, and the welding angle is 45°, so that the connection is very tight and firm without gaps.
作为本发明的一种优选技术方案,电光调制器、色散光纤、高速光电探测器、低噪放和微波功分器组成光电振荡器,将光信号变微波信号,使其得以数据化,有利于分析计算和循环使用。As a preferred technical solution of the present invention, the electro-optic modulator, dispersion fiber, high-speed photodetector, low-noise amplifier and microwave power divider form a photoelectric oscillator, which converts optical signals into microwave signals, making it digital, which is beneficial to Analytical calculations and recycling.
作为本发明的一种优选技术方案,宽谱光源可采用高斯型或矩形光源作为发射光源,使得发射光源的选择性更高。As a preferred technical solution of the present invention, the wide-spectrum light source can use a Gaussian or rectangular light source as the emitting light source, so that the selectivity of the emitting light source is higher.
本发明所达到的有益效果是:本发明为一种保偏光纤拍长的测量装置,通过待测高双折射保偏光纤和检偏器共同组成了一个马赫曾德干涉仪,使得宽谱光源经该干涉仪后,当干涉仪两臂光程差在光源相干范围内时,在干涉仪的输出端将产生干涉条纹,该干涉条纹在频域上为一正弦梳状谱;利用熔接,将待测高双折射保偏光纤与光纤起偏器紧紧连接,使其不会出现空隙,同时也是非常稳固;不会出现组装繁琐、容易脱落、连接不稳、美观度差的问题。通过电光调制器,色散光纤,高速光电探测器,低噪放和微波功分器构成光电振荡器环路,将光信号装换成微波信号并测量输出微波信号的中心频率,使其得以大数据化,大大节约了人力物力和时间,提高了准确度。The beneficial effects achieved by the present invention are: the present invention is a measurement device for the beat length of a polarization-maintaining optical fiber. A Mach-Zehnder interferometer is jointly formed by a highly birefringent polarization-maintaining optical fiber to be measured and a polarization analyzer, so that the wide-spectrum light source After passing through the interferometer, when the optical path difference between the two arms of the interferometer is within the coherent range of the light source, interference fringes will be generated at the output end of the interferometer, and the interference fringes are a sinusoidal comb spectrum in the frequency domain; The high birefringence polarization-maintaining fiber to be tested is tightly connected to the fiber polarizer, so that there will be no gaps, and it is also very stable; there will be no problems of cumbersome assembly, easy falling off, unstable connection, and poor aesthetics. The electro-optical modulator, dispersive fiber, high-speed photodetector, low-noise amplifier and microwave power divider constitute the photoelectric oscillator loop, convert the optical signal into a microwave signal and measure the center frequency of the output microwave signal, so that it can be big data It greatly saves manpower, material resources and time, and improves the accuracy.
附图说明Description of drawings
附图用来提供对本发明的进一步理解,并且构成说明书的一部分,与本发明的实施例一起用于解释本发明,并不构成对本发明的限制。The accompanying drawings are used to provide a further understanding of the present invention, and constitute a part of the description, and are used together with the embodiments of the present invention to explain the present invention, and do not constitute a limitation to the present invention.
在附图中:In the attached picture:
图1是本发明系统框架结构示意图。Fig. 1 is a schematic diagram of the framework structure of the system of the present invention.
图中标号:101、宽谱光源;102、光纤起偏器;103、待测高双折射保偏光纤;104、检偏器;105、电光调制器;106、色散光纤;107、高速光电探测器;108、低噪放;109、微波功分器;201、频谱仪;202、计算机。Reference numerals in the figure: 101, wide-spectrum light source; 102, optical fiber polarizer; 103, high birefringence polarization-maintaining optical fiber to be tested; 104, polarizer; 105, electro-optic modulator; 106, dispersion optical fiber; 107, high-speed photoelectric detection 108. Low noise amplifier; 109. Microwave power splitter; 201. Spectrum analyzer; 202. Computer.
具体实施方式Detailed ways
以下结合附图对本发明的优选实施例进行说明,应当理解,此处所描述的优选实施例仅用于说明和解释本发明,并不用于限定本发明。The preferred embodiments of the present invention will be described below in conjunction with the accompanying drawings. It should be understood that the preferred embodiments described here are only used to illustrate and explain the present invention, and are not intended to limit the present invention.
在本发明的描述中,需要说明的是,术语“竖直”、“上”、“下”、“水平”等指示的方位或位置关系为基于附图所示的方位或位置关系,仅是为了便于描述本发明和简化描述,而不是指示或暗示所指的装置或元件必须具有特定的方位、以特定的方位构造和操作,因此不能理解为对本发明的限制。In the description of the present invention, it should be noted that the orientation or positional relationship indicated by the terms "vertical", "upper", "lower", "horizontal" etc. is based on the orientation or positional relationship shown in the drawings, and is only In order to facilitate the description of the present invention and simplify the description, it does not indicate or imply that the device or element referred to must have a specific orientation, be constructed and operated in a specific orientation, and thus should not be construed as limiting the present invention.
在本发明的描述中,还需要说明的是,除非另有明确的规定和限定,术语“设置”、“安装”、“相连”、“连接”应做广义理解,例如,可以是固定连接,也可以是可拆卸连接,或一体地连接;可以是机械连接,也可以是电连接;可以是直接相连,也可以通过中间媒介间接相连,可以是两个元件内部的连通。对于本领域的普通技术人员而言,可以根据具体情况理解上述术语在本发明中的具体含义。In the description of the present invention, it should also be noted that, unless otherwise clearly specified and limited, the terms "installation", "installation", "connection" and "connection" should be understood in a broad sense, for example, it may be a fixed connection, It can also be a detachable connection or an integral connection; it can be a mechanical connection or an electrical connection; it can be a direct connection or an indirect connection through an intermediary, and it can be the internal communication of two components. Those of ordinary skill in the art can understand the specific meanings of the above terms in the present invention according to specific situations.
实施例:如图1所示,本发明提供一种保偏光纤拍长的测量装置,其特征在于,包括宽谱光源101、光纤起偏器102、频谱仪201和计算机202;宽谱光源101经过光纤起偏器102进入待测高双折射保偏光纤103,待测高双折射保偏光纤103信号输出端连接有检偏器104,待测高双折射保偏光纤103和检偏器104共同组成了一个马赫曾德干涉仪,马赫曾德干涉仪信号输出端有电光调制器105,电光调制器105上的光载微波信号经过色散光纤106后入射到高速光电探测器107上,高速光电探测器107将光信号装换成微波信号并通过低噪放108放大,低噪放108输出端连接微波功分器109,微波功分器109将一部分微波信号注入到电光调制器105 中,同时将另一部分微波信号输入频谱仪201,频谱仪201末端连接计算机202。Embodiment: as shown in Figure 1, the present invention provides a kind of measurement device of polarization maintaining fiber beat length, it is characterized in that, comprises broadband light source 101, optical fiber polarizer 102, spectrometer 201 and computer 202; Broad spectrum light source 101 Enter the high birefringence polarization maintaining fiber 103 to be tested through the optical fiber polarizer 102, the signal output end of the high birefringence polarization maintaining fiber 103 to be tested is connected with a polarization analyzer 104, the high birefringence polarization maintaining fiber 103 to be tested and the polarization analyzer 104 Together constitute a Mach-Zehnder interferometer, the signal output end of the Mach-Zehnder interferometer has an electro-optic modulator 105, and the light-carrying microwave signal on the electro-optic modulator 105 is incident on the high-speed photodetector 107 after passing through the dispersion fiber 106, and the high-speed photoelectric The detector 107 converts the optical signal into a microwave signal and amplifies it through the low-noise amplifier 108. The output of the low-noise amplifier 108 is connected to the microwave power divider 109, and the microwave power divider 109 injects a part of the microwave signal into the electro-optic modulator 105, and at the same time Another part of the microwave signal is input to the spectrum analyzer 201 , and the end of the spectrum analyzer 201 is connected to the computer 202 .
待测高双折射保偏光纤103与光纤起偏器102采用熔接的方式连接,熔接角度为45°,使其连接处非常紧密结实,不会出现空隙;由电光调制器105,色散光纤106,高速光电探测器 107,低噪放108和微波功分器109组成光电振荡器,且光电振荡器环路输入端与马赫曾德干涉仪的输出端相连接,将光信号变微波信号,使其得以数据化,有利于分析计算和循环使用;宽谱光源101可采用高斯型或矩形光源作为发射光源,使得发射光源的选择性更高。The high birefringence polarization-maintaining optical fiber 103 to be tested is connected to the optical fiber polarizer 102 by fusion splicing, and the fusion splicing angle is 45°, so that the connection is very tight and firm without gaps; the electro-optic modulator 105, the dispersion optical fiber 106, A high-speed photodetector 107, a low-noise amplifier 108 and a microwave power divider 109 form a photoelectric oscillator, and the input end of the photoelectric oscillator loop is connected with the output end of the Mach-Zehnder interferometer, and the optical signal is changed into a microwave signal to make it It can be digitized, which is beneficial for analysis, calculation and recycling; the wide-spectrum light source 101 can use a Gaussian or rectangular light source as the emission light source, so that the selectivity of the emission light source is higher.
本测量方法的原理是通过待测高双折射保偏光纤103的模式双折射使得在待测高双折射保偏光纤103中传播的两路光的光程差不一样,而光电振荡器输出的微波信号的中心频率又跟该光程差有关,根据微波信号的中心频率就可以得到待测高双折射保偏光纤103的拍长。宽谱光源经过拍长为Lp的待测高双折射保偏光纤103后,选取合适长度的待测高双折射保偏光纤 103使得在待测高双折射保偏光纤103两偏振本振轴上传输的两路光在待测高双折射保偏光纤 103末端满足干涉条件而发生干涉,则干涉条纹的输出在频域上可表示为:The principle of this measurement method is that the mode birefringence of the high birefringence polarization-maintaining fiber 103 to be tested makes the optical path difference of the two paths of light propagating in the high-birefringence polarization-maintaining fiber 103 to be tested different, and the output of the photoelectric oscillator The center frequency of the microwave signal is related to the optical path difference, and the beat length of the highly birefringent polarization-maintaining fiber 103 to be tested can be obtained according to the center frequency of the microwave signal. After the wide-spectrum light source passes through the high birefringence polarization-maintaining fiber 103 to be tested with a beat length of Lp , select a suitable length of the high-birefringence polarization-maintaining fiber 103 to be tested so that the two polarization local oscillator axes of the high-birefringence polarization-maintaining fiber 103 to be tested are The two paths of light transmitted above meet the interference conditions at the end of the highly birefringent polarization-maintaining fiber 103 to be tested and interfere, then the output of the interference fringes can be expressed in the frequency domain as:
其中A为干涉仪输出干涉条纹的可见度,Δω为不同干涉仪光程差时输出干涉条纹的频率间隔,为干涉仪的相位漂移,ω0为激光器的中心圆频率。Δω可表示为:Where A is the visibility of the interference fringes output by the interferometer, Δω is the frequency interval of the output interference fringes when the optical path difference of the interferometer is different, is the phase shift of the interferometer, and ω 0 is the central circular frequency of the laser. Δω can be expressed as:
Δω=2πcLp/λ0l (2)Δω=2πcL p /λ 0 l (2)
其中c为光速,λ0为宽谱光源101中心波长,l为待测高双折射保偏光纤103的长度。则该干涉仪的自由光谱范围可表示为:Where c is the speed of light, λ 0 is the central wavelength of the broadband light source 101, and l is the length of the highly birefringent polarization-maintaining fiber 103 to be tested. Then the free spectral range of the interferometer can be expressed as:
干涉的输出光是与波长相关,其电场可表征为:The output light of interference is wavelength-dependent, and its electric field can be characterized as:
E(t)=∫E(ω)ejωtdω (4)E(t)=∫E(ω)e jωt dω (4)
则宽谱光源101的光功率谱密度可表示为:Then the optical power spectral density of the broadband light source 101 can be expressed as:
T(ω)=|E(ω)|2 (5)T(ω)=|E(ω)| 2 (5)
干涉仪输出的干涉条纹经过电光调制器105后,光谱的每个频率分量E(ω)都被调制,并且由光电振荡器环路产生一频率为ξ的微波信号,电光调制器105输出的光场可表示为:After the interference fringes output by the interferometer pass through the electro-optic modulator 105, each frequency component E(ω) of the spectrum is modulated, and a microwave signal with a frequency of ξ is generated by the photoelectric oscillator loop, and the light output by the electro-optic modulator 105 field can be expressed as:
E(ω)=ejωt(1+ejξt+e-jξt) (6)E(ω)=e jωt (1+e jξt +e -jξt ) (6)
光电振荡器中使用色散光纤106作为延迟线,该时延线的电场传递函数可表示为:Dispersion fiber 106 is used as a delay line in the optoelectronic oscillator, and the electric field transfer function of the time delay line can be expressed as:
H(ω)=|H(ω)|e-jφ(ω) (7)H(ω)=|H(ω)|e -jφ(ω) (7)
φ(ω)为色散光纤106延迟引入的相位,根据泰勒级数展开,该相位可表示为:φ(ω) is the phase introduced by the delay of the dispersion fiber 106. According to the Taylor series expansion, the phase can be expressed as:
式中,τ(ω0)为中心频率为ω0时的群时延,β为色散光纤106的色散,其单位为ps2/km,β可表示为:In the formula, τ(ω 0 ) is the group delay when the center frequency is ω 0 , β is the dispersion of the dispersion fiber 106, and its unit is ps 2 /km, and β can be expressed as:
式中D(ps/km/nm)为色散光纤106的色散系数,λ0为宽谱光源101波长。In the formula, D (ps/km/nm) is the dispersion coefficient of the dispersion fiber 106, and λ 0 is the wavelength of the broadband light source 101.
根据式(5)——(9)可得光电振荡器响应函数为:According to formulas (5)-(9), the response function of the photoelectric oscillator can be obtained as:
其中 in
由此可知,光电振荡器输出的微波信号的中心频率可表示为:It can be seen that the center frequency of the microwave signal output by the photoelectric oscillator can be expressed as:
由此可得待测高双折射保偏光纤103的拍长为:Thus, the beat length of the highly birefringent polarization-maintaining fiber 103 to be tested can be obtained as:
由上式可知,根据光电振荡器输出微波信号的中心频率,宽谱光源101的中心波长,色散光纤106的色散系数和长度以及待测高双折射保偏光纤103的长度就可以得到待测高双折射保偏光纤103的拍长。从式(12)可知,若待测高双折射保偏光纤103拍长为1m,色散光纤106 的色散系数为-150ps/km/nm,色散光纤106长度为1km,光源中心波长为1550nm,则拍长测量分辨率可达0.4mm。由于色散光纤106的色散系数一般是几个固定的数值,所以可以通过增加色散光纤106的长度来实现拍长测量分辨率的提高。As can be seen from the above formula, according to the center frequency of the photoelectric oscillator output microwave signal, the center wavelength of the broadband light source 101, the dispersion coefficient and the length of the dispersion fiber 106 and the length of the high birefringence polarization-maintaining fiber 103 to be measured, the height to be measured can be obtained. The beat length of the birefringent polarization-maintaining fiber 103. From formula (12), if the beat length of the high birefringence polarization-maintaining fiber 103 to be measured is 1m, the dispersion coefficient of the dispersion fiber 106 is -150ps/km/nm, the length of the dispersion fiber 106 is 1km, and the central wavelength of the light source is 1550nm, then The beat length measurement resolution can reach 0.4mm. Since the dispersion coefficient of the dispersion fiber 106 is generally several fixed values, the resolution of beat length measurement can be improved by increasing the length of the dispersion fiber 106 .
本高双折射保偏光纤拍长测量装置的工作流程如下所示:The workflow of the high birefringence polarization-maintaining fiber beat length measurement device is as follows:
上电后,电光调制器105驱动板通过程序自动控制强度型光调制器工作在线性工作点。电光调制器105工作点确定后,光电振荡器输出的微波信号的中心频率。根据式(12)就可得到待测高双折射保偏光纤103的拍长。After being powered on, the driving board of the electro-optic modulator 105 automatically controls the intensity-type optical modulator to work at the linear operating point through a program. After the working point of the electro-optic modulator 105 is determined, the center frequency of the microwave signal output by the photoelectric oscillator. According to formula (12), the beat length of the high birefringence polarization-maintaining fiber 103 to be tested can be obtained.
最后应说明的是:以上仅为本发明的优选实施例而已,并不用于限制本发明,尽管参照前述实施例对本发明进行了详细的说明,对于本领域的技术人员来说,其依然可以对前述各实施例所记载的技术方案进行修改,或者对其中部分技术特征进行等同替换。凡在本发明的精神和原则之内,所作的任何修改、等同替换、改进等,均应包含在本发明的保护范围之内。Finally, it should be noted that the above are only preferred embodiments of the present invention, and are not intended to limit the present invention. Although the present invention has been described in detail with reference to the foregoing embodiments, those skilled in the art can still understand The technical solutions recorded in the foregoing embodiments are modified, or some of the technical features are equivalently replaced. Any modifications, equivalent replacements, improvements, etc. made within the spirit and principles of the present invention shall be included within the protection scope of the present invention.
Claims (4)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201711130297.3A CN107806981B (en) | 2017-11-15 | 2017-11-15 | Measuring device for beat length of polarization maintaining optical fiber |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201711130297.3A CN107806981B (en) | 2017-11-15 | 2017-11-15 | Measuring device for beat length of polarization maintaining optical fiber |
Publications (2)
Publication Number | Publication Date |
---|---|
CN107806981A true CN107806981A (en) | 2018-03-16 |
CN107806981B CN107806981B (en) | 2020-11-17 |
Family
ID=61580220
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201711130297.3A Active CN107806981B (en) | 2017-11-15 | 2017-11-15 | Measuring device for beat length of polarization maintaining optical fiber |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN107806981B (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN108709720A (en) * | 2018-08-01 | 2018-10-26 | 天津博科光电科技有限公司 | A kind of measuring device and method of the mode birefringence of high-birefringence polarisation-maintaining optical fiber |
CN111692972A (en) * | 2020-06-16 | 2020-09-22 | 中国科学院国家授时中心 | Single-fiber unidirectional optical fiber length measuring method and system |
CN115371968A (en) * | 2022-08-26 | 2022-11-22 | 中国科学院上海光学精密机械研究所 | Measurement method of beat length of few-mode polarization-maintaining fiber |
CN115371968B (en) * | 2022-08-26 | 2025-04-15 | 中国科学院上海光学精密机械研究所 | Beat length measurement method for few-mode polarization-maintaining optical fiber |
Citations (11)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS58223032A (en) * | 1982-06-22 | 1983-12-24 | Agency Of Ind Science & Technol | Method for measuring beat length of constant polarization fiber |
JPS60147627A (en) * | 1984-01-13 | 1985-08-03 | Nippon Telegr & Teleph Corp <Ntt> | Method and device for measuring characteristics of polarization maintaining optical fiber |
CN1811365A (en) * | 2006-02-21 | 2006-08-02 | 北京航空航天大学 | System for detecting polarization maintaining optical fiber beat length |
CN101592551A (en) * | 2009-06-05 | 2009-12-02 | 北京航空航天大学 | A method and device for measuring beat length of polarization-maintaining optical fiber based on Sagnac interferometer |
CN102914423A (en) * | 2012-11-01 | 2013-02-06 | 电子科技大学 | Measuring device and method for sag frequency of dispersion optical fiber |
CN103090813A (en) * | 2013-01-15 | 2013-05-08 | 电子科技大学 | High resolution sensing system measuring beat-length and strain of polarization maintaining optical fiber based on optical frequency domain reflectometer (OFDR) system |
CN104330104A (en) * | 2014-10-31 | 2015-02-04 | 浙江大学 | Measuring device for interferential sensor arm length difference |
CN105675258A (en) * | 2016-01-04 | 2016-06-15 | 安徽大学 | High birefringence optical fiber beat length measuring method and measuring device based on interference order |
CN106546411A (en) * | 2016-10-19 | 2017-03-29 | 北京航空航天大学 | Polarization maintaining optical fibre Verdet constant measuring apparatus and method based on Mach Zehnder and Michelson interferometers |
CN106643522A (en) * | 2016-12-28 | 2017-05-10 | 西南交通大学 | Optical-fiber low-coherence interference displacement demodulation device and method based on photoelectric oscillator |
CN107271152A (en) * | 2017-07-25 | 2017-10-20 | 苏州润桐专利运营有限公司 | A kind of measuring method of the measuring system based on dispersive optical fiber abbe number |
-
2017
- 2017-11-15 CN CN201711130297.3A patent/CN107806981B/en active Active
Patent Citations (11)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS58223032A (en) * | 1982-06-22 | 1983-12-24 | Agency Of Ind Science & Technol | Method for measuring beat length of constant polarization fiber |
JPS60147627A (en) * | 1984-01-13 | 1985-08-03 | Nippon Telegr & Teleph Corp <Ntt> | Method and device for measuring characteristics of polarization maintaining optical fiber |
CN1811365A (en) * | 2006-02-21 | 2006-08-02 | 北京航空航天大学 | System for detecting polarization maintaining optical fiber beat length |
CN101592551A (en) * | 2009-06-05 | 2009-12-02 | 北京航空航天大学 | A method and device for measuring beat length of polarization-maintaining optical fiber based on Sagnac interferometer |
CN102914423A (en) * | 2012-11-01 | 2013-02-06 | 电子科技大学 | Measuring device and method for sag frequency of dispersion optical fiber |
CN103090813A (en) * | 2013-01-15 | 2013-05-08 | 电子科技大学 | High resolution sensing system measuring beat-length and strain of polarization maintaining optical fiber based on optical frequency domain reflectometer (OFDR) system |
CN104330104A (en) * | 2014-10-31 | 2015-02-04 | 浙江大学 | Measuring device for interferential sensor arm length difference |
CN105675258A (en) * | 2016-01-04 | 2016-06-15 | 安徽大学 | High birefringence optical fiber beat length measuring method and measuring device based on interference order |
CN106546411A (en) * | 2016-10-19 | 2017-03-29 | 北京航空航天大学 | Polarization maintaining optical fibre Verdet constant measuring apparatus and method based on Mach Zehnder and Michelson interferometers |
CN106643522A (en) * | 2016-12-28 | 2017-05-10 | 西南交通大学 | Optical-fiber low-coherence interference displacement demodulation device and method based on photoelectric oscillator |
CN107271152A (en) * | 2017-07-25 | 2017-10-20 | 苏州润桐专利运营有限公司 | A kind of measuring method of the measuring system based on dispersive optical fiber abbe number |
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN108709720A (en) * | 2018-08-01 | 2018-10-26 | 天津博科光电科技有限公司 | A kind of measuring device and method of the mode birefringence of high-birefringence polarisation-maintaining optical fiber |
CN108709720B (en) * | 2018-08-01 | 2023-09-01 | 天津博科光电科技有限公司 | Device and method for measuring mode birefringence of high-birefringence polarization-maintaining optical fiber |
CN111692972A (en) * | 2020-06-16 | 2020-09-22 | 中国科学院国家授时中心 | Single-fiber unidirectional optical fiber length measuring method and system |
CN115371968A (en) * | 2022-08-26 | 2022-11-22 | 中国科学院上海光学精密机械研究所 | Measurement method of beat length of few-mode polarization-maintaining fiber |
CN115371968B (en) * | 2022-08-26 | 2025-04-15 | 中国科学院上海光学精密机械研究所 | Beat length measurement method for few-mode polarization-maintaining optical fiber |
Also Published As
Publication number | Publication date |
---|---|
CN107806981B (en) | 2020-11-17 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN103743553B (en) | The dual channel optical performance testing device of a kind of integrated waveguide manipulator and polarization crosstalk identification thereof and processing method | |
CN106546411B (en) | Polarization maintaining optical fibre Verdet constant measuring apparatus and method based on Mach-Zehnder and Michelson interferometers | |
CN102281107A (en) | Apparatus and method for measuring dispersion of optical fiber optics | |
CN111912400B (en) | A polarization-maintaining fiber loop distributed polarization crosstalk bidirectional simultaneous measurement device and method | |
CN102288388A (en) | Device and method for improving polarization-maintaining optical fiber polarization coupling measurement precision and symmetry | |
Calvani et al. | Polarization measurements on single-mode fibers | |
CN101968508B (en) | All-fiber current sensor and polarization state control method thereof | |
CN104280217B (en) | A kind of Y waveguide dual channel optical device for measuring properties | |
CN104280216B (en) | Dual-channel optical performance simultaneous testing device for Y waveguide device and Y waveguide polarization crosstalk recognizing and processing method thereof | |
WO2020192269A1 (en) | Device employing differential delay of principal axes to measure polarization-maintaining fiber | |
CN107976300B (en) | A method for measuring the beat length of polarization-maintaining fibers | |
CN107917669A (en) | A kind of optical fibre displacement sensor demodulation method | |
CN112082735B (en) | Optical fiber sensing ring bidirectional synchronous measurement device and method based on Sagnac structure | |
CN110595515A (en) | A dual-parameter optical fiber sensor based on polarization-maintaining optical fiber and FP cavity | |
Yu et al. | Optical frequency domain polarimetry for distributed polarization crosstalk measurement beyond a 110 dB dynamic range | |
CN103344925A (en) | Slow light Sagnac nonreciprocal interference optical fiber magnetic field sensor | |
CN107806981B (en) | Measuring device for beat length of polarization maintaining optical fiber | |
CN104280215A (en) | Dual-channel optical performance bi-directional multi-alignment-angle automatic testing device for Y waveguide | |
CN104729750A (en) | Distributed optical fiber temperature sensor based on Brillouin scattering | |
CN107632180B (en) | Optical fiber voltage sensing probe and optical fiber voltage sensing demodulation system | |
Li et al. | Inconsistency measurement between two branches of LiNbO3 integrated optic Y-junction | |
Meng et al. | Birefringence characterization in a dual-hole microstructured optical fiber using an OFDR method | |
CN106197741B (en) | Temperature-detecting device based on micro-nano long-period fiber grating sensor and method | |
CN112082651A (en) | Polarization characteristic measurement method for assembling full polarization-maintaining Sagnac closed light path | |
Yuan et al. | Simultaneous evaluation of two branches of a multifunctional integrated optic chip with an ultra-simple dual-channel configuration |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
PB01 | Publication | ||
PB01 | Publication | ||
SE01 | Entry into force of request for substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
TA01 | Transfer of patent application right | ||
TA01 | Transfer of patent application right |
Effective date of registration: 20201022 Address after: 322000 1st floor, No.3, building 20, Qiyi village, Chengxi street, Yiwu City, Jinhua City, Zhejiang Province Applicant after: Yiwu Lansi sporting goods Co.,Ltd. Address before: 215600 Building A 145, Emerging Industry Development Center, Zhangjiagang Free Trade Zone, Suzhou City, Jiangsu Province Applicant before: Huang Maolian |
|
GR01 | Patent grant | ||
GR01 | Patent grant | ||
TR01 | Transfer of patent right |
Effective date of registration: 20240424 Address after: Room 2A, Science and Technology Building, No. 968 Xuefeng West Road, Beiyuan Street, Yiwu City, Jinhua City, Zhejiang Province, 322000 Patentee after: Zhejiang Jinguo Intellectual Property Co.,Ltd. Country or region after: China Address before: 322000 1st floor, No.3, building 20, Qiyi village, Chengxi street, Yiwu City, Jinhua City, Zhejiang Province Patentee before: Yiwu Lansi sporting goods Co.,Ltd. Country or region before: China |
|
TR01 | Transfer of patent right | ||
CP03 | Change of name, title or address | ||
CP03 | Change of name, title or address |
Address after: 2A, Science and Technology Building, 968 Xuefeng West Road, Beiyuan Street, Yiwu City, Jinhua City, Zhejiang Province 321000 Patentee after: Yiwu Jinguo Intellectual Property Co.,Ltd. Country or region after: China Address before: 1st Floor, No. 1-2, Building 9, Beiyuan Commercial and Trade Zone, Beiyuan Street, Yiwu City, Jinhua City, Zhejiang Province Patentee before: Zhejiang Jinguo Intellectual Property Co.,Ltd. Country or region before: China |
|
TR01 | Transfer of patent right | ||
TR01 | Transfer of patent right |
Effective date of registration: 20250117 Address after: 510000 B852, 3rd Floor, No. 11 Tangdong East Road, Tianhe District, Guangzhou City, Guangdong Province (Office only) Patentee after: Guangzhou Qilan Technology Co.,Ltd. Country or region after: China Address before: 2A, Science and Technology Building, 968 Xuefeng West Road, Beiyuan Street, Yiwu City, Jinhua City, Zhejiang Province 321000 Patentee before: Yiwu Jinguo Intellectual Property Co.,Ltd. Country or region before: China |
|
TR01 | Transfer of patent right |
Effective date of registration: 20250320 Address after: Room 201, 2nd Floor, Building 2, Yincheng INC Center Keya Project, No. 59 Tianyuan West Road, Jiangning District, Nanjing City, Jiangsu Province, 211100 (Jiangning Development Zone) Patentee after: Jiangsu Juli Science and Technology Innovation Development Co.,Ltd. Country or region after: China Address before: 510000 B852, 3rd Floor, No. 11 Tangdong East Road, Tianhe District, Guangzhou City, Guangdong Province (Office only) Patentee before: Guangzhou Qilan Technology Co.,Ltd. Country or region before: China |