Natural polarization state single wavelength light source and method

A single-wavelength, polarization technology, applied to the field of optics, can solve the problems of low efficiency of superluminescent light-emitting diodes, low coupling efficiency of single-mode fiber, unfavorable applications, etc., and achieve the effect of simple structure, high gain and power, and convenient realization.

Inactive Publication Date: 2012-12-26
常州奥镭光电科技有限公司
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Problems solved by technology

[0019] Superluminescent light-emitting diodes (SLD/SLED) have low efficiency, poor stability, low coupling efficiency with single-mode fiber, and, like f

Method used

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  • Natural polarization state single wavelength light source and method
  • Natural polarization state single wavelength light source and method
  • Natural polarization state single wavelength light source and method

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[0050] Such as Figure 4 As shown, a single-wavelength natural polarization light source of the present invention is composed of a current-pumped semiconductor optical amplifier (SOA) [1], a fiber grating [2] and a polarization-independent isolator [3].

[0051] The semiconductor amplifier is used to amplify the random distribution of the polarization direction of the spontaneous radiation (ASE) to produce natural polarized light, and the fiber grating [2] reflects the back-output light of the spontaneous radiation back to the SOA [1] to narrow the output spectral width and use its The feedback increases the power of this wavelength, and the polarization-independent isolator [3] prevents the end face of the fiber output end from reflecting to form laser oscillation, ensuring the output of a natural polarization light source independent of polarization.

[0052] A piece of fiber grating [2] is connected to one end of a semiconductor optical amplifier (SOA) [1], the reflection wavelen...

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Abstract

The invention discloses a natural polarization state single wavelength light source and a method. The light source consists of a first semi-conductor light amplifier with a current pump, a fiber grating and a polarization independent isolator, wherein the fiber grating is connected to one end of the first semi-conductor light amplifier; the reflection wavelength of the fiber grating is in the gain spectrum of the first semi-conductor light amplifier; and the other end of the first semi-conductor light amplifier is connected to the input end of the polarization independent isolator. The method has the following steps that: generating spontaneous radiation by the first semi-conductor light amplifier driven by the current; directly outputting forward spontaneous radiation light through the polarization independent isolator; filtering the backward spontaneous radiation light through the fiber grating and reflecting spontaneous radiation light with narrow-band wavelength; outputting and consuming the spontaneous radiation light of other wavebands from the other end of the fiber grating after the spontaneous radiation light of other wavebands being transmitted; and outputting the spontaneous radiation light reflected by the fiber grating from the polarization independent isolator after being amplified by the first semi-conductor light amplifier again. According to the natural polarization state single wavelength light source and the method, the single wavelength natural polarization light can be directly output, so that the energy conversion efficiency is high; and the natural polarization state single wavelength light source and the method disclosed by the invention are convenient to realize and simple in structure.

Description

technical field [0001] The invention relates to the field of optics, in particular to a single-wavelength light source and method with a natural polarization state. Background technique [0002] Common light sources such as semiconductor lasers and fiber lasers have a high degree of linear polarization. During the transmission of optical signals in the optical fiber, due to the inevitable small asymmetry of the fiber core structure, the inhomogeneity of the refractive index distribution, the asymmetry of the external or internal transverse stress, and the twisting, bending or external application of the optical fiber The electromagnetic field will cause the fiber to have a birefringence effect, which will cause the polarization direction and polarization degree of linearly polarized light to change randomly after a certain distance in the fiber. [1] In applications such as high-speed optical fiber communication, optical fiber sensing, and optical fiber gyroscope, random cha...

Claims

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Application Information

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IPC IPC(8): H01S3/10
Inventor 陈国梁张先明宋强蒋祺梅里
Owner 常州奥镭光电科技有限公司
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