CN116260028A - Laser refractive index tuning method, system, device and laser - Google Patents

Laser refractive index tuning method, system, device and laser Download PDF

Info

Publication number
CN116260028A
CN116260028A CN202310542982.6A CN202310542982A CN116260028A CN 116260028 A CN116260028 A CN 116260028A CN 202310542982 A CN202310542982 A CN 202310542982A CN 116260028 A CN116260028 A CN 116260028A
Authority
CN
China
Prior art keywords
tuning
laser
refractive index
laser beam
liquid medium
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.)
Pending
Application number
CN202310542982.6A
Other languages
Chinese (zh)
Inventor
崔晓敏
肖旭辉
王瑶
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Shenzhen Yinggu Laser Co ltd
Original Assignee
Shenzhen Yinggu Laser Co ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Shenzhen Yinggu Laser Co ltd filed Critical Shenzhen Yinggu Laser Co ltd
Priority to CN202310542982.6A priority Critical patent/CN116260028A/en
Publication of CN116260028A publication Critical patent/CN116260028A/en
Pending legal-status Critical Current

Links

Images

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/005Optical devices external to the laser cavity, specially adapted for lasers, e.g. for homogenisation of the beam or for manipulating laser pulses, e.g. pulse shaping
    • H01S3/0085Modulating the output, i.e. the laser beam is modulated outside the laser cavity
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/0014Monitoring arrangements not otherwise provided for
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/005Optical devices external to the laser cavity, specially adapted for lasers, e.g. for homogenisation of the beam or for manipulating laser pulses, e.g. pulse shaping
    • H01S3/0078Frequency filtering
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S5/00Semiconductor lasers
    • H01S5/0014Measuring characteristics or properties thereof
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S5/00Semiconductor lasers
    • H01S5/005Optical components external to the laser cavity, specially adapted therefor, e.g. for homogenisation or merging of the beams or for manipulating laser pulses, e.g. pulse shaping
    • H01S5/0078Optical components external to the laser cavity, specially adapted therefor, e.g. for homogenisation or merging of the beams or for manipulating laser pulses, e.g. pulse shaping for frequency filtering
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S5/00Semiconductor lasers
    • H01S5/005Optical components external to the laser cavity, specially adapted therefor, e.g. for homogenisation or merging of the beams or for manipulating laser pulses, e.g. pulse shaping
    • H01S5/0085Optical components external to the laser cavity, specially adapted therefor, e.g. for homogenisation or merging of the beams or for manipulating laser pulses, e.g. pulse shaping for modulating the output, i.e. the laser beam is modulated outside the laser cavity

Abstract

The invention discloses a laser refractive index tuning method, a system, a device and a laser, which comprise the steps of preprocessing an original laser source to obtain a laser beam to be tuned; setting an optical tuning cavity along the optical path of the laser beam to be tuned, inserting a tuning unit into the optical tuning cavity, enabling the laser beam to be tuned to pass through the tuning unit, and tuning the laser beam to be tuned by the tuning unit by utilizing current to output the tuning laser beam; a re-filtering unit and a detecting unit are arranged at the output end of the laser beam to be tuned passing through the tuning unit. According to the invention, after the original laser source is preprocessed, a regular laser beam is obtained, the regular laser beam is introduced into the optical tuning cavity and is subjected to current tuning through the tuning unit, so that the refractive index in the tuning unit is changed by the current, the tuning of the laser beam is realized, and the refractive index of the laser is changed according to the current. Namely, the defects of slow refractive index change and limited frequency tuning range in the prior art are effectively overcome.

Description

Laser refractive index tuning method, system, device and laser
Technical Field
The present invention relates to the field of laser refractive index tuning technologies, and in particular, to a laser refractive index tuning method, system, device, and laser.
Background
In many applications, it is desirable to use a frequency tunable laser in order to accommodate different operating conditions and requirements. Common tuning methods include mechanical tuning and electro-optical tuning. Mechanical tuning typically requires the use of mechanical devices that adjust the cavity length or the position of the cavity mirror, which tend to be relatively complex and expensive. The electro-optic tuning requires voltage or current to control the refractive index in the electro-optic crystal and further adjust the refractive index in the resonant cavity, and the method is simpler than mechanical tuning, but has the problems of slow refractive index change, limited frequency tuning range and the like.
Disclosure of Invention
The invention aims to solve the defects of slow refractive index change and limited frequency tuning range in the prior art, and provides a laser refractive index tuning method, a laser refractive index tuning system, a laser refractive index tuning device and a laser.
In order to achieve the above purpose, the present invention adopts the following technical scheme:
the first aspect of the present invention provides a laser refractive index tuning method, comprising:
preprocessing an original laser source to obtain a laser beam to be tuned;
setting an optical tuning cavity along the optical path of the laser beam to be tuned, inserting a tuning unit into the optical tuning cavity, enabling the laser beam to be tuned to pass through the tuning unit, and tuning the laser beam to be tuned by the tuning unit by utilizing current to output the tuning laser beam;
setting a re-filtering unit and a detection unit at the output end of the laser beam to be tuned passing through the tuning unit, and filtering the output of the tuned laser beam by using the re-filtering unit to obtain the laser beam to be detected;
detecting the output power of the laser beam to be detected by using a detection unit, and directly outputting if the output power of the laser beam to be detected meets the rated requirement;
and if the output power of the laser beam to be detected does not meet the rated requirement, repeating the tuning operation of the tuning unit for the laser beam to be detected by using the current until the rated requirement is met.
In some possible embodiments, the tuning unit comprises:
the liquid medium is electrically controlled and is used for matching with the laser wavelength;
the electronic control subunit is electrically connected with the liquid medium and is used for tuning the refractive index in the liquid medium.
In some possible embodiments, the tuning unit uses a voltage method including:
adding a liquid medium into the optical tuning cavity, and enabling the liquid medium to be matched with the laser wavelength;
according to the addition amount of the liquid medium and the electric control tuning amount, an electric control subunit is utilized for inputting tuning current, and the refractive index of the liquid medium is adjusted by adjusting the temperature or the pressure of the liquid medium;
tuning the frequency of the laser beam to be tuned is achieved by changing the refractive index of the liquid medium versus the refractive index in the optical tuning cavity.
In some possible embodiments, the liquid medium comprises: a single liquid or a mixed liquid.
A second aspect of the present invention provides a laser refractive index tuning system, employing a laser refractive index tuning method as described in any one of the first aspects, the tuning system further comprising:
the microprocessor is used for controlling the electric control subunit to output current;
a power detector for detecting laser output power;
and the tunable output mirror is arranged in the optical tuning cavity and is used for carrying out re-filtering on laser output.
In some possible embodiments, the tuning system further comprises: a liquid medium;
wherein the liquid medium is a liquid crystal.
A third aspect of the present invention provides a laser refractive index tuning device employing a laser refractive index tuning method according to any one of the first aspects or a laser refractive index tuning system according to any one of the second aspects.
A fourth aspect of the invention provides a laser employing a laser refractive index tuning method according to any one of the first aspects or a laser refractive index tuning system according to any one of the second aspects.
The beneficial effects of the invention are as follows:
according to the method, after the original laser source is preprocessed, the regular laser beam is obtained, the regular laser beam is introduced into the optical tuning cavity and is subjected to current tuning through the tuning unit, the current changes the refractive index in the tuning unit, tuning of the laser beam is achieved, and the refractive index of the laser is changed according to the current. Namely, the defects of slow refractive index change and limited frequency tuning range in the prior art are effectively overcome.
Drawings
Fig. 1 is a schematic diagram of an overall flow structure of a laser refractive index tuning method according to an embodiment of the present invention;
FIG. 2 is a schematic flow chart of a laser refractive index tuning method according to an embodiment of the present invention;
fig. 3 is a schematic flow chart of a laser refractive index tuning method according to an embodiment of the present invention.
Detailed Description
The following description of the embodiments of the present invention will be made clearly and fully with reference to the accompanying drawings, in which it is evident that the embodiments described are only some, but not all embodiments of the invention. All other embodiments, which can be made by those skilled in the art based on the embodiments of the invention without making any inventive effort, are intended to be within the scope of the invention.
It should be noted that all directional indicators (such as up, down, left, right, front, and rear … …) in the embodiments of the present invention are merely used to explain the relative positional relationship, movement, etc. between the components in a particular posture (as shown in the drawings), and if the particular posture is changed, the directional indicator is changed accordingly.
In the present invention, unless specifically stated and limited otherwise, the terms "connected," "affixed," and the like are to be construed broadly, and for example, "affixed" may be a fixed connection, a removable connection, or an integral body; can be mechanically or electrically connected; either directly or indirectly, through intermediaries, or both, may be in communication with each other or in interaction with each other, unless expressly defined otherwise. The specific meaning of the above terms in the present invention can be understood by those of ordinary skill in the art according to the specific circumstances.
In addition, if there is a description of "first", "second", etc. in the embodiments of the present invention, the description of "first", "second", etc. is for descriptive purposes only and is not to be construed as indicating or implying a relative importance or implicitly indicating the number of technical features indicated. Thus, a feature defining "a first" or "a second" may explicitly or implicitly include at least one such feature. In addition, the meaning of "and/or" as it appears throughout includes three parallel schemes, for example "A and/or B", including the A scheme, or the B scheme, or the scheme where A and B are satisfied simultaneously. In addition, the technical solutions of the embodiments may be combined with each other, but it is necessary to base that the technical solutions can be realized by those skilled in the art, and when the technical solutions are contradictory or cannot be realized, the combination of the technical solutions should be considered to be absent and not within the scope of protection claimed in the present invention.
Examples
With reference to FIGS. 1, 2 and 3, the present invention is directed to solving the above-described background art
The prior art has the defects of slow refractive index change and limited frequency tuning range. According to the method, after the original laser source is preprocessed, the regular laser beam is obtained, the regular laser beam is introduced into the optical tuning cavity and is subjected to current tuning through the tuning unit, the current changes the refractive index in the tuning unit, tuning of the laser beam is achieved, and the refractive index of the laser is changed according to the current. Namely, the defects of slow refractive index change and limited frequency tuning range in the prior art are effectively overcome.
Specifically, the first aspect of the present invention provides a laser refractive index tuning method, which includes:
preprocessing an original laser source to obtain a laser beam to be tuned; wherein, the method for preprocessing the original laser source comprises, but is not limited to: after the filtering and impurity removal are carried out on the original laser source, the influence of stray light is removed after the original laser source is regulated, so that the subsequent tuning effect on laser is ensured.
Setting an optical tuning cavity along the optical path of the laser beam to be tuned, inserting a tuning unit into the optical tuning cavity, enabling the laser beam to be tuned to pass through the tuning unit, and tuning the laser beam to be tuned by the tuning unit by utilizing current to output the tuning laser beam;
setting a re-filtering unit and a detection unit at the output end of the laser beam to be tuned passing through the tuning unit, and filtering the output of the tuned laser beam by using the re-filtering unit to obtain the laser beam to be detected;
detecting the output power of the laser beam to be detected by using a detection unit, and directly outputting if the output power of the laser beam to be detected meets the rated requirement; and if the output power of the laser beam to be detected does not meet the rated requirement, repeating the work until the rated requirement is met. That is, in this embodiment, the tuning unit performs output tuning of the laser beam to be tuned by means of voltage.
In this embodiment, in order to facilitate understanding of how the tuning unit performs laser refractive index tuning using current or voltage, the tuning unit includes: the liquid medium is electrically controlled and is used for matching with the laser wavelength; the electronic control subunit is electrically connected with the liquid medium and is used for tuning the refractive index in the liquid medium. In addition, to facilitate understanding how the tuning unit controls the refractive index by using current, the tuning unit uses a voltage method including:
adding a liquid medium into the optical tuning cavity, and enabling the liquid medium to be matched with the laser wavelength;
according to the addition amount of the liquid medium and the electric control tuning amount, an electric control subunit is utilized for inputting tuning current, and the refractive index of the liquid medium is adjusted by adjusting the temperature or the pressure of the liquid medium;
tuning the frequency of the laser beam to be tuned is achieved by changing the refractive index of the liquid medium versus the refractive index in the optical tuning cavity. I.e. adding a certain liquid medium in the optical path along the laser beam and matching it with the laser wavelength; regulating the temperature or pressure of the liquid medium by inputting current, and regulating the refractive index of the liquid medium; the refractive index in the liquid medium is further changed, so that the refractive index of the laser tuning cavity is adjusted, and the frequency adjustment of the laser is realized. In the above method, the liquid medium may be a single liquid or a mixed liquid, and the selection thereof should be determined according to a desired wavelength range and refractive index variation range. The liquid medium can be added through a reserved small hole and the small hole is sealed after injection; it may also be directly injected into the laser tuning cavity and discharged after the laser tuning experiment is completed. In the embodiment of the invention, the refractive index of the liquid medium used for laser can be widely adjusted by adjusting the temperature and the pressure, so that a larger frequency tuning range is realized on one hand. On the other hand, the refractive index of the liquid medium can respond quickly to changes in temperature and pressure, and therefore, the tuning speed is very fast. And compared with the traditional mechanical tuning and electro-optical tuning, the method provided by the invention does not need any complicated mechanical device or electrical element, and has the advantages of simple structure, low maintenance cost and the like. In addition, the cost of preparing the liquid medium used in the present invention is relatively low compared to electro-optic tuning, and therefore, the cost of the present invention is also relatively low.
It should be noted that, in the present invention, the specific implementation of tuning the laser by using different liquid media should be determined according to the actual situation and needs. The refractive index of the liquid medium may also be adjusted, if desired, by adding other substances, for example ionic liquids in appropriate concentrations to the liquid medium. During experimentation, the laser frequency may be monitored and recorded using a spectrometer or other related instrument to ensure tuning range and frequency stability.
What is claimed is intended to cover in the claims the selection of the type and amount of liquid medium used in the present invention and the specific details of the operation of adjusting the temperature and pressure of the liquid medium. Those skilled in the art will be able to make variations and modifications in light of the specific embodiments of the present invention without departing from the spirit or scope of the invention.
A second aspect of the present invention provides a laser refractive index tuning system, employing a laser refractive index tuning method as described in any one of the first aspects, the tuning system further comprising:
the microprocessor is used for controlling the electric control subunit to output current;
and the power detector is used for detecting the laser output power.
And the tunable output mirror is arranged in the optical tuning cavity and is used for carrying out re-filtering on laser output.
In some possible embodiments, the liquid medium is a liquid crystal. In this embodiment, in the method, the liquid crystal may be a single kind or a mixture, and is determined according to a desired wavelength range and refractive index variation range. The injection of the liquid crystal can be carried out through a reserved small hole, and the small hole is sealed after the injection; it may also be injected directly into the cavity and expelled after the experiment is completed. Setting the liquid medium as liquid crystal, the refractive index in the liquid crystal can be adjusted rapidly by changing the electric field, and thus the tuning speed is faster. In addition, the refractive index of the liquid crystal can realize a large frequency tuning range by changing the electric field. In addition, compared with the traditional mechanical tuning and electro-optical tuning, the method provided by the invention does not need any complicated mechanical device or electrical element, and has the advantages of simple structure, low maintenance cost and the like. It should also be noted that the liquid crystal electro-optic tuning method can obtain higher tuning accuracy, and the frequency stability and repeatability are better.
The specific embodiments of the present invention should be determined according to actual situations and requirements. The liquid crystal may be a single kind or a mixture, and the selection of the kind and amount of the liquid crystal may be determined according to a desired wavelength range and refractive index variation range. During experimentation, the laser frequency may be monitored and recorded using a spectrometer or other related instrument to ensure tuning range and frequency stability. The injection of the liquid crystal can be carried out through a reserved small hole, and the small hole is sealed after the injection; it may also be injected directly into the cavity and expelled after the experiment is completed. The invention also comprises a circuit and an electric element related to the circuit so as to realize the control of the liquid crystal electric field.
What is claimed is intended to cover in the claims the selection of the type and amount of liquid crystal used in the present invention and the specific details of the operation of the circuits and electrical elements that regulate the electric field of the liquid crystal. Those skilled in the art will be able to make variations and modifications in light of the specific embodiments of the present invention without departing from the spirit or scope of the invention.
A third aspect of the present invention provides a laser refractive index tuning device employing a laser refractive index tuning method according to any one of the first aspects or a laser refractive index tuning system according to any one of the second aspects.
A fourth aspect of the invention provides a laser employing a laser refractive index tuning method according to any one of the first aspects or a laser refractive index tuning system according to any one of the second aspects.
The foregoing description is only of the preferred embodiments of the present disclosure and description of the principles of the technology being employed. It will be appreciated by those skilled in the art that the scope of the invention in the embodiments of the present disclosure is not limited to the specific combination of the above technical features, but encompasses other technical features formed by any combination of the above technical features or their equivalents without departing from the spirit of the invention. Such as the above-described features, are mutually substituted with (but not limited to) the features having similar functions disclosed in the embodiments of the present disclosure.

Claims (8)

1. A method of tuning the refractive index of a laser, comprising:
preprocessing an original laser source to obtain a laser beam to be tuned;
setting an optical tuning cavity along the optical path of the laser beam to be tuned, inserting a tuning unit into the optical tuning cavity, enabling the laser beam to be tuned to pass through the tuning unit, and tuning the laser beam to be tuned by the tuning unit by utilizing current to output the tuning laser beam;
setting a re-filtering unit and a detection unit at the output end of the laser beam to be tuned passing through the tuning unit, and filtering the output of the tuned laser beam by using the re-filtering unit to obtain the laser beam to be detected;
detecting the output power of the laser beam to be detected by using a detection unit, and directly outputting if the output power of the laser beam to be detected meets the rated requirement;
and if the output power of the laser beam to be detected does not meet the rated requirement, repeating the tuning operation of the tuning unit for the laser beam to be detected by using the current until the rated requirement is met.
2. The laser refractive index tuning method according to claim 1, wherein the tuning unit comprises:
the liquid medium is electrically controlled and is used for matching with the laser wavelength;
the electronic control subunit is electrically connected with the liquid medium and is used for tuning the refractive index in the liquid medium.
3. A method of tuning the refractive index of a laser beam according to claim 2, wherein said tuning unit is voltage-dependent, comprising:
adding a liquid medium into the optical tuning cavity, and enabling the liquid medium to be matched with the laser wavelength;
according to the addition amount of the liquid medium and the electric control tuning amount, an electric control subunit is utilized for inputting tuning current, and the refractive index of the liquid medium is adjusted by adjusting the temperature or the pressure of the liquid medium;
tuning the frequency of the laser beam to be tuned is achieved by changing the refractive index of the liquid medium versus the refractive index in the optical tuning cavity.
4. A method of tuning the refractive index of a laser light as claimed in claim 2 or 3, wherein the liquid medium comprises: a single liquid or a mixed liquid.
5. A laser refractive index tuning system employing a laser refractive index tuning method according to any one of claims 1-4, said tuning system further comprising:
the microprocessor is used for controlling the electric control subunit to output current;
a power detector for detecting laser output power;
and the tunable output mirror is arranged in the optical tuning cavity and is used for carrying out re-filtering on laser output.
6. The laser refractive index tuning system of claim 5, wherein the tuning system further comprises: a liquid medium;
wherein the liquid medium is a liquid crystal.
7. A laser refractive index tuning device characterized in that a laser refractive index tuning method according to any one of claims 1-4 or a laser refractive index tuning system according to claim 5 or 6 is used.
8. A laser, characterized in that a laser refractive index tuning method according to any one of claims 1-4 or a laser refractive index tuning system according to claim 5 or 6 is used.
CN202310542982.6A 2023-05-15 2023-05-15 Laser refractive index tuning method, system, device and laser Pending CN116260028A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202310542982.6A CN116260028A (en) 2023-05-15 2023-05-15 Laser refractive index tuning method, system, device and laser

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202310542982.6A CN116260028A (en) 2023-05-15 2023-05-15 Laser refractive index tuning method, system, device and laser

Publications (1)

Publication Number Publication Date
CN116260028A true CN116260028A (en) 2023-06-13

Family

ID=86682877

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202310542982.6A Pending CN116260028A (en) 2023-05-15 2023-05-15 Laser refractive index tuning method, system, device and laser

Country Status (1)

Country Link
CN (1) CN116260028A (en)

Citations (19)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01287427A (en) * 1988-05-16 1989-11-20 Matsushita Electric Ind Co Ltd Laser wavelength detector
US5113275A (en) * 1991-07-03 1992-05-12 Bell Communications Research, Inc. Temperature compensation of liquid-crystal etalon filters
JPH0588138A (en) * 1991-09-25 1993-04-09 Nippon Telegr & Teleph Corp <Ntt> Variable wavelength filter device
JP2000298270A (en) * 1999-04-15 2000-10-24 Yazaki Corp Wavelength selective filter and production therefor
US20020171921A1 (en) * 2001-05-15 2002-11-21 Agilent Technologies, Inc. Laser resonator with direction sensitive decoupling
US20030048817A1 (en) * 2001-09-07 2003-03-13 Agilent Technologies, Inc. Optical path length variation using a liquid crystal for tuning a laser
CN1524326A (en) * 2001-07-06 2004-08-25 ض� External cavity laser apparatus with orthogonal tuning of laser wavelength and cavity optical path length
US20100111119A1 (en) * 2007-03-28 2010-05-06 Kenji Sato External resonator type wavelength variable semiconductor laser
US20110174977A1 (en) * 2008-10-02 2011-07-21 Koninklijke Philips Electronics N.V. Spectral detector
US20120268709A1 (en) * 2011-04-20 2012-10-25 Zilkie Aaron J Tunable optical filters with liquid crystal resonators
CN102820611A (en) * 2012-09-05 2012-12-12 天津奇谱光电技术有限公司 Tunable laser for outputting non-polarized light
CN203326350U (en) * 2013-06-05 2013-12-04 黑龙江科技大学 Dye doped cholesteric liquid crystal tunable laser
CN103713411A (en) * 2014-01-09 2014-04-09 浙江师范大学 Method for manufacturing tunable band-pass optical fiber filter
US20150293614A1 (en) * 2012-11-16 2015-10-15 Pen Generations Inc. Liquid crystal display device and electronic pen system using same
CN107436437A (en) * 2017-06-14 2017-12-05 长春理工大学 Active laser detection apparatus based on tunable liquid crystal variable refractivity
CN112152060A (en) * 2020-10-30 2020-12-29 电子科技大学 Photonic crystal micro laser resonant cavity based on Brewster angle
US20220113602A1 (en) * 2019-01-11 2022-04-14 Optomel Limited Optical filter materials and devices
US20220113570A1 (en) * 2020-10-12 2022-04-14 Research & Business Foundation Sungkyunkwan University Wavelength tunable liquid crystal etalon filter including double seal line and manufacturing method of the same
KR102429828B1 (en) * 2022-04-08 2022-08-05 주식회사 알바트레이스 Ultra-small Wavelength-variable Liquid Crystal Etherone Filter Resistant to External Environmental Changes, Light Source and Optical Transceiver Including the Same

Patent Citations (20)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01287427A (en) * 1988-05-16 1989-11-20 Matsushita Electric Ind Co Ltd Laser wavelength detector
US5113275A (en) * 1991-07-03 1992-05-12 Bell Communications Research, Inc. Temperature compensation of liquid-crystal etalon filters
JPH0588138A (en) * 1991-09-25 1993-04-09 Nippon Telegr & Teleph Corp <Ntt> Variable wavelength filter device
JP2000298270A (en) * 1999-04-15 2000-10-24 Yazaki Corp Wavelength selective filter and production therefor
US20020171921A1 (en) * 2001-05-15 2002-11-21 Agilent Technologies, Inc. Laser resonator with direction sensitive decoupling
CN1524326A (en) * 2001-07-06 2004-08-25 ض� External cavity laser apparatus with orthogonal tuning of laser wavelength and cavity optical path length
US20030048817A1 (en) * 2001-09-07 2003-03-13 Agilent Technologies, Inc. Optical path length variation using a liquid crystal for tuning a laser
US20100111119A1 (en) * 2007-03-28 2010-05-06 Kenji Sato External resonator type wavelength variable semiconductor laser
US20110174977A1 (en) * 2008-10-02 2011-07-21 Koninklijke Philips Electronics N.V. Spectral detector
CN102171544A (en) * 2008-10-02 2011-08-31 皇家飞利浦电子股份有限公司 Spectral detector comprising a cholesteric liquid crystal mixture
US20120268709A1 (en) * 2011-04-20 2012-10-25 Zilkie Aaron J Tunable optical filters with liquid crystal resonators
CN102820611A (en) * 2012-09-05 2012-12-12 天津奇谱光电技术有限公司 Tunable laser for outputting non-polarized light
US20150293614A1 (en) * 2012-11-16 2015-10-15 Pen Generations Inc. Liquid crystal display device and electronic pen system using same
CN203326350U (en) * 2013-06-05 2013-12-04 黑龙江科技大学 Dye doped cholesteric liquid crystal tunable laser
CN103713411A (en) * 2014-01-09 2014-04-09 浙江师范大学 Method for manufacturing tunable band-pass optical fiber filter
CN107436437A (en) * 2017-06-14 2017-12-05 长春理工大学 Active laser detection apparatus based on tunable liquid crystal variable refractivity
US20220113602A1 (en) * 2019-01-11 2022-04-14 Optomel Limited Optical filter materials and devices
US20220113570A1 (en) * 2020-10-12 2022-04-14 Research & Business Foundation Sungkyunkwan University Wavelength tunable liquid crystal etalon filter including double seal line and manufacturing method of the same
CN112152060A (en) * 2020-10-30 2020-12-29 电子科技大学 Photonic crystal micro laser resonant cavity based on Brewster angle
KR102429828B1 (en) * 2022-04-08 2022-08-05 주식회사 알바트레이스 Ultra-small Wavelength-variable Liquid Crystal Etherone Filter Resistant to External Environmental Changes, Light Source and Optical Transceiver Including the Same

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
赵近芳 周林: "农产品质量安全光学无损检测技术及应用", 北京邮电大学出版社, pages: 178 - 184 *

Similar Documents

Publication Publication Date Title
CN103762487B (en) A kind of tunable laser with dual output light beam
CN106526751B (en) A kind of temperature control turnable fiber filter and preparation method thereof based on micro-nano fiber
WO2015050591A2 (en) Tunable add-drop filter with an active resonator
CN103701030A (en) Unimodal 87 Rb isotopic atomic filter used for laser frequency stabilization and filter method thereof
JP2018519667A (en) Method and device for stabilization of optical power and emission spectral lines by mode-locked ultrashort pulse fiber laser
CN103682952A (en) Invisible laser with light output path mark and marking method of light output path
CN108039636A (en) A kind of mid-infrared light fibre optical parametric oscillator based on 2 μm of ultra-short pulse laser pumpings
CN108663731A (en) The making of dielectrophoretic force liquid zoom lens and focal-length measurement method
CN104079345A (en) Wavelength monitor and wavelength monitoring method
CN116260028A (en) Laser refractive index tuning method, system, device and laser
CN108899758A (en) A kind of hybrid integrated tunable external cavity laser and wavelength tuning method
WO2019200886A1 (en) Method for realizing synchronous tuning of wavelength and repetition frequency in passive mode-locking laser
CN110165547A (en) A kind of laser frequency stabilisation device and method
CN107425409B (en) Mode-locked laser and optical system
CN101566776B (en) Method for tuning laser output wavelength based on self-mixing effect
CN102687060B (en) Electronically controlled collimating apparatus in laser resonator
CN111106511A (en) Frequency synchronization passive mode-locking fiber laser and method for realizing frequency synchronization
CN207116907U (en) Mode-locked laser and optical system
CN114284845A (en) Single-frequency distributed feedback optical fiber unit laser device and wavelength tuning method thereof
CN103885324B (en) Optical clock based on full-optical frequency stabilization and manufacturing method of optical clock
CN208157848U (en) Realize laser with active-passive lock mould medium wavelength adjustable device synchronous with repetition rate
US3541300A (en) Apparatus for stabilizing the modulation of coherent radiation
CN113964637A (en) Laser wavelength switching device
KR100464599B1 (en) Optical Fiber Grating Device Using Liquid Crystals And Its Manufacturing Method
EP2726922B1 (en) Methods and systems for trimming photonic devices

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