TW201818624A - Laser pump chamber device - Google Patents
Laser pump chamber device Download PDFInfo
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- TW201818624A TW201818624A TW106128388A TW106128388A TW201818624A TW 201818624 A TW201818624 A TW 201818624A TW 106128388 A TW106128388 A TW 106128388A TW 106128388 A TW106128388 A TW 106128388A TW 201818624 A TW201818624 A TW 201818624A
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES 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
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/02—Constructional details
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES 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
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/09—Processes or apparatus for excitation, e.g. pumping
- H01S3/091—Processes or apparatus for excitation, e.g. pumping using optical pumping
- H01S3/094—Processes or apparatus for excitation, e.g. pumping using optical pumping by coherent light
- H01S3/0941—Processes or apparatus for excitation, e.g. pumping using optical pumping by coherent light of a laser diode
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES 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
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/02—Constructional details
- H01S3/04—Arrangements for thermal management
- H01S3/042—Arrangements for thermal management for solid state lasers
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES 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
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/14—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range characterised by the material used as the active medium
- H01S3/16—Solid materials
- H01S3/163—Solid materials characterised by a crystal matrix
- H01S3/164—Solid materials characterised by a crystal matrix garnet
- H01S3/1643—YAG
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Abstract
Description
本發明係有關一種雷射泵腔室裝置者。The invention relates to a laser pump chamber device.
為了確保振盪穩定性,高輸出的固體雷射振盪裝置(例如,YAG雷射振盪裝置)中雷射介質的冷卻係不可缺少的。先前,高輸出的固體雷射振盪裝置使用作為雷射介質之YAG桿和作為激發光源之閃光燈密閉之水冷套式雷射泵腔室,藉由使冷卻水循環而進行冷卻來保持雷射泵腔室的熱穩定性。 相對於此,在水的使用或水的產生被嚴禁之(禁水)場所,需要使用高輸出的固體雷射振盪裝置,正在開發出代替前述水冷式而以氣冷式應對高輸出之雷射泵腔室。該種雷射泵腔室的先前例已知有如下等,其具備:YAG桿;閃光燈;楕圓形反射光學系統,用於將從閃光燈射出之光聚光在YAG桿並進行照射;及水套,包圍該等,並且具備:溫度調整機構,將配置有雷射泵腔室之雷射振盪裝置的框體內的空氣的溫度調整為恆定;及送風機構,將該框體內的空氣送入雷射泵腔室內(參照下述專利文獻1)。 [先行技術文獻] [專利文獻] 專利文獻1:日本專利公開2012-156435號公報In order to ensure the oscillation stability, the cooling of the laser medium in a high-output solid-state laser oscillation device (for example, a YAG laser oscillation device) is indispensable. Previously, high-output solid-state laser oscillators used a YAG rod as a laser medium and a water-cooled jacketed laser pump chamber sealed by a flash lamp as an excitation light source. The laser pump chamber was maintained by circulating cooling water for cooling Thermal stability. In contrast, in places where water use or water generation is prohibited (water forbidden), high-output solid-state laser oscillation devices are required. Instead of the aforementioned water-cooled type, air-cooled lasers are being developed to deal with high-output lasers. Pump chamber. The previous examples of this type of laser pump chamber are known as follows, including: a YAG rod; a flash lamp; a circular reflection optical system for condensing and emitting light emitted from the flash lamp on the YAG rod; and water It is provided to surround these, and includes: a temperature adjustment mechanism that adjusts the temperature of the air in the frame in which the laser oscillation device of the laser pump chamber is arranged to be constant; and a blower mechanism that sends the air in the frame into the lightning Inside the pump pump chamber (see Patent Document 1 below). [Advanced Technical Documents] [Patent Documents] Patent Document 1: Japanese Patent Publication No. 2012-156435
[發明所欲解決之問題] 前述先前例雖然能夠得到可在禁水場所使用之氣冷式的雷射泵腔室,但難以進行與水冷式同等水平的冷卻,無法得到水冷式程度的高輸出。並且,另一方面,要求一種能夠取出高輸出且呈現軸對稱的輸出分佈之高品質的雷射光之雷射泵腔室,但在前述先前技術中存在無法應對該種要求之問題。 本發明係為了應付該種問題而提出者。亦即,本發明的課題為提供一種能夠取出高輸出且高品質的雷射光之雷射泵腔室等。 [解決問題之技術手段] 為了解決該種課題,本發明之雷射泵腔室係具備以下構成者。 一種雷射泵腔室裝置,其特徵在於具備:雷射介質;激發光源元件,圍繞前述雷射介質的中心軸以等間隔被配置,且具有與前述中心軸交叉之光軸;照射光學系統,被配置於前述光軸上,將從前述激發光源元件射出之激發光進行聚光而照射於雷射介質;及框體,支撐前述雷射介質的端部,並且支撐前述照射光學系統和前述激發光源元件,前述框體由熱傳導性構件構成,且於該框體的外表面配置有溫度調整構件。[Problems to be Solved by the Invention] Although the foregoing previous example can obtain an air-cooled laser pump chamber that can be used in a water-restricted place, it is difficult to perform cooling at the same level as the water-cooled type, and it cannot obtain a high output of the water-cooled type. . In addition, on the other hand, a laser pump chamber capable of extracting high-quality laser light having a high output and exhibiting an axis-symmetrical output distribution is required, but there is a problem that the aforementioned prior art cannot meet such a requirement. The present invention has been made in order to cope with such problems. That is, the subject of this invention is providing the laser pump chamber etc. which can extract high-quality and high-quality laser light. [Technical Solution to Problem] In order to solve such a problem, the laser pump chamber of the present invention includes the following components. A laser pump chamber device, comprising: a laser medium; an excitation light source element arranged at equal intervals around a central axis of the laser medium and having an optical axis crossing the central axis; an irradiation optical system, It is arranged on the optical axis, collects the excitation light emitted from the excitation light source element, and irradiates the laser medium; and a frame body supports the end portion of the laser medium, and supports the irradiation optical system and the excitation. In the light source element, the frame is made of a thermally conductive member, and a temperature adjustment member is disposed on an outer surface of the frame.
以下,參照圖式說明本發明的實施形態。以下說明中,不同圖式中之相同符號表示相同功能的部位,適當省略各圖式中之重複說明。 如圖1及圖2所示,雷射泵腔室裝置1具備雷射介質10、激發光源元件2、照射光學系統3及框體4。雷射介質10例如係YAG桿,係具有中心軸10P之圓柱狀的雷射桿,以與中心軸10P正交之端面10A、10B開放之狀態被支撐於框體4上。 激發光源元件2例如係雷射二極體,具有與雷射介質10的中心軸10P交叉之光軸。圍繞中心軸10P以等間隔配置有複數個激發光源元件2。在圖示的例子中,以120°間隔,圍繞中心軸10P配置有3個激發光源元件2,並以各激發光源元件2的光軸與中心軸10P正交之方式被配置。 照射光學系統3被配置於激發光源元件2的光軸上,將從激發光源元件2射出之光進行聚光並照射到雷射介質10。在圖示的例子中,照射光學系統3使用柱面透鏡,其將從激發光源元件2射出之具有發散角之光(雷射光)設為平行光並照射到雷射介質10。為了以高效率將激發光照射到雷射介質10,使用包括柱面透鏡之照射光學系統3,其將從激發光源元件2射出之光聚光成與雷射介質10的桿徑相同直徑的平行光並照射到雷射介質10。 框體4係支撐雷射介質10的端部,並且支撐照射光學系統3和激發光源元件2者,在圖示的例子中,由複數個塊構成。具體而言,框體4具備端部支撐塊40、41、內部塊42、43、44及外周塊45,並且具備端部塊51、52。 端部支撐塊40、41係個別地支撐雷射介質10的長度方向端部者,具有能夠使雷射介質10的端部插入之開口40A、41A。在圖示的例子中,在開口40A、41A內配置有O型圈53,插入到開口40A、41A內之雷射介質10的端部經由O型圈53被支撐於端部支撐塊40、41。 在圖示的例子中,端部支撐塊40、41上連接有端部塊51、52,端部塊51、52的開口51A、52A與端部支撐塊40、41的開口40A、41A被配置於同軸上。藉此,雷射介質10的端面10A經由開口51A被開放,端面10B經由開口52A被開放。在圖示的例子中,將端部支撐塊40、41和端部塊51、52設為不同之塊,但該等亦可以設為一體的塊。 內部塊42、43、44藉由該等而形成雷射介質10的周圍空間4A和照射光學系統3及激發光源元件2的支撐空間4B。周圍空間4A為與雷射介質10的中心軸10P同軸的圓筒狀,其內表面成為與中心軸10P同軸狀的圓筒反射面4C。具體而言,藉由在內部塊42、43、44的內表面實施鍍金等反射塗層來形成圓筒反射面4C。 外周塊45以包圍內部塊42、43、44的周圍之方式被配置,其中一部分支撐激發光源元件2。外周塊45可以係被分割成複數個之塊,亦可以係一體的塊。 構成框體4之塊(端部支撐塊40、41、內部塊42、43、44、外周塊45)全部由熱傳導性構件(銅等熱傳導性高的構件)構成,並且彼此密合而被連結。各塊的密合面之間的接合中使用熱傳導性高的黏接材料(金屬糊劑)為較佳。並且,在框體4的外表面,具體而言在外周塊45的一部分外表面配置有帕耳帖(Peltier)元件等溫度調整構件5。 該種雷射泵腔室裝置1能夠藉由基於溫度調整構件5之溫度調整而使支撐激發光源元件2之框體4成為均勻的溫度,從而將所有激發光源元件2的發光波長維持為恆定。由於構成框體4之塊(端部支撐塊40、41、內部塊42、43、44、外周塊45)全部由熱傳導性構件構成,因此藉由在框體4的外表面的一部分配置溫度調整構件5,能夠使框體4整體成為均勻的溫度。 當使用雷射二極體作為激發光源元件2時,發光波長根據雷射二極體的溫度而發生變化,但為了進行高效的激發,要求被照射到雷射介質10之激發光的波長維持為容易由雷射介質10吸收之一定的波長。例如,當採用釹YAG桿作為雷射介質10時,能夠藉由將激發光的波長維持在798nm至808nm來進行高效的激發。雷射泵腔室裝置1能夠藉由溫度調整構件5將作為激發光源元件2之雷射二極體的溫度維持在於798nm至808nm處發光之溫度(例如,25℃),因此當採用釹YAG桿作為雷射介質10時,能夠進行高效的激發。 由框體4的塊構成之照射光學系統3及激發光源元件2的支撐空間4B,圍繞雷射介質10的中心軸10P以等間隔被配置。在圖示的例子中,圍繞中心軸10P以120°間隔在3處配置有支撐空間4B。在支撐空間4B的一部分,在外周塊45上固定有激發光源元件2的基板2A,激發光源元件2以其光軸與雷射介質10的中心軸10P正交之方式被支撐。並且,在支撐空間4B的一部分配置有作為照射光學系統3之柱面透鏡和透鏡支撐構件3A,照射光學系統3被配置於激發光源元件2的光軸上。由框體4的塊構成之雷射介質10的周圍空間4A係與支撐空間4B連通而其中心與中心軸10P成為同軸狀。 被支撐於支撐空間4B之複數個激發光源元件2從軸對稱的3個方向(其他方向)向雷射介質(YAG桿)10的側方照射激發光。並且,在照射光學系統3中被聚光成與雷射介質10的桿徑大略相同的直徑之激發光高效地被照射到雷射介質10,在雷射介質10的表面上被反射之光被形成於周圍空間4A的內表面之圓筒反射面4C反射並再次被照射到雷射介質10的側面,因此激發光更高效地被照射到雷射介質10。藉此,能夠從雷射介質10得到具有軸對稱的輸出分佈之高品質的發光,並且藉由高效的激發光的照射而得到高輸出的發光。 框體4上設置有冷媒流入路4D和冷媒流出路4F,藉此雷射泵腔室裝置1能夠有效地對雷射介質10進行冷卻。在圖示的例子中,冷媒流入路4D係沿與雷射介質10的中心軸10P交叉之方向被延長設置之直線流路,圍繞中心軸10P均等地配置有3條(複數條),其被形成於端部支撐塊40。並且,冷媒流出路4F係沿中心軸10P之直線流路,其被形成於端部支撐塊41和端部塊52。 氣冷式的雷射泵腔室裝置1中,在框體4中之一方的端部塊51設置有與冷媒流入路4D連通之連接部4E,在連接部4E連接有搬送壓縮空氣之送氣管50。並且,經由被形成於端部塊52和端部支撐塊41之冷媒流出路4F,已與雷射介質10接觸之壓縮空氣被排氣。 如此,雷射泵腔室裝置1在雷射介質10的側面具備使壓縮空氣從多個方向接觸之冷媒流入路4D,且沿著中心軸10P具備將已與雷射介質10接觸之壓縮空氣進行排氣之冷媒流出路4F,因此能夠有效地對雷射介質10進行冷卻。藉此,即使是氣冷式,亦能夠得到高輸出的發光。並且,該種構造的雷射泵腔室裝置1中,形成將前述冷媒流入路4D和冷媒流出路4F進行連接之循環水流路來確保周圍空間4A內的密封性,藉此能夠轉用為水冷式。 圖3表示具備雷射泵腔室裝置1之雷射振盪裝置20。雷射振盪裝置20能夠藉由在框體20A內以與雷射泵腔室裝置1的中心軸10P對面之方式配置包括輸出鏡21和反射鏡22之諧振鏡,且視需要將包括1/4波長板23A、勃克爾斯盒23B、偏光鏡23C等之Q開關23配置於諧振鏡內而得到。 該種雷射振盪裝置20能夠藉由氣冷式的雷射泵腔室裝置1使軸對稱的輸出分佈的光從雷射介質10射出,能夠有效地對雷射介質10進行冷卻,因此係氣冷式,並且能夠取出高輸出且高品質的雷射光。並且,藉由確保雷射泵腔室裝置1的框體4中之周圍空間4A的密封性,還能夠轉用為水冷式的雷射泵腔室裝置1,因此在禁水以外的使用條件下,能夠藉由設為水冷式來得到更高的輸出。 以上,參照圖式詳述了本發明的實施形態,但具體的構成並不限於該等實施形態,即使進行不脫離本發明的要旨之範圍的設計變更等,亦包含於本發明中。並且,上述各實施形態只要其目的及構成等沒有特別的矛盾或問題,則能夠將彼此的技術沿用並組合。Hereinafter, embodiments of the present invention will be described with reference to the drawings. In the following description, the same symbols in different drawings represent the parts with the same function, and repeated descriptions in the drawings are appropriately omitted. As shown in FIGS. 1 and 2, the laser pump chamber device 1 includes a laser medium 10, an excitation light source element 2, an irradiation optical system 3, and a housing 4. The laser medium 10 is, for example, a YAG rod or a cylindrical laser rod having a central axis 10P, and is supported on the frame 4 in a state where the end surfaces 10A and 10B orthogonal to the central axis 10P are open. The excitation light source element 2 is, for example, a laser diode, and has an optical axis crossing the central axis 10P of the laser medium 10. A plurality of excitation light source elements 2 are arranged at equal intervals around the central axis 10P. In the example shown in the figure, three excitation light source elements 2 are arranged around the central axis 10P at 120 ° intervals, and are arranged so that the optical axis of each excitation light source element 2 is orthogonal to the central axis 10P. The irradiation optical system 3 is arranged on the optical axis of the excitation light source element 2, collects light emitted from the excitation light source element 2, and irradiates the laser medium 10. In the example shown in the figure, a cylindrical lens is used as the irradiation optical system 3, and light having a divergence angle (laser light) emitted from the excitation light source element 2 is set as parallel light and irradiates the laser medium 10. In order to irradiate the excitation light to the laser medium 10 with high efficiency, an irradiation optical system 3 including a cylindrical lens is used, which condenses the light emitted from the excitation light source element 2 into parallel with the same diameter as the rod diameter of the laser medium 10 Light is irradiated onto the laser medium 10. The frame 4 supports the end portion of the laser medium 10 and supports the irradiation optical system 3 and the excitation light source element 2. In the example shown in the figure, the frame 4 is composed of a plurality of blocks. Specifically, the frame 4 includes end support blocks 40 and 41, inner blocks 42, 43, 44 and an outer peripheral block 45, and includes end blocks 51 and 52. The end support blocks 40 and 41 individually support the longitudinal ends of the laser medium 10 and have openings 40A and 41A through which the ends of the laser medium 10 can be inserted. In the example shown, O-rings 53 are arranged in the openings 40A and 41A, and the ends of the laser medium 10 inserted into the openings 40A and 41A are supported by the end support blocks 40 and 41 via the O-rings 53. . In the example shown, the end support blocks 40 and 41 are connected to the end blocks 51 and 52, and the openings 51A and 52A of the end blocks 51 and 52 and the openings 40A and 41A of the end support blocks 40 and 41 are arranged. On the coaxial. Thereby, the end surface 10A of the laser medium 10 is opened through the opening 51A, and the end surface 10B is opened through the opening 52A. In the illustrated example, the end support blocks 40 and 41 and the end blocks 51 and 52 are different blocks, but these may be integrated blocks. The inner blocks 42, 43, and 44 form a surrounding space 4A of the laser medium 10 and a supporting space 4B of the irradiation optical system 3 and the excitation light source element 2 by these. The surrounding space 4A has a cylindrical shape coaxial with the central axis 10P of the laser medium 10, and its inner surface becomes a cylindrical reflecting surface 4C coaxial with the central axis 10P. Specifically, a cylindrical reflecting surface 4C is formed by applying a reflective coating such as gold plating to the inner surfaces of the inner blocks 42, 43, and 44. The outer peripheral block 45 is arranged so as to surround the periphery of the inner blocks 42, 43, and 44, and a part of the outer peripheral block 45 supports the excitation light source element 2. The peripheral block 45 may be divided into a plurality of blocks, or may be integrated blocks. The blocks (end support blocks 40, 41, inner blocks 42, 43, 44, and outer blocks 45) constituting the frame 4 are all composed of thermally conductive members (highly thermally conductive members such as copper), and are closely connected to each other and connected. . It is preferable to use an adhesive material (metal paste) having high thermal conductivity for bonding between the adhesion surfaces of the blocks. A temperature adjustment member 5 such as a Peltier element is disposed on the outer surface of the housing 4, specifically, a part of the outer surface of the outer peripheral block 45. The laser pump chamber device 1 of this kind can adjust the temperature of the temperature adjusting member 5 to make the frame 4 supporting the excitation light source element 2 a uniform temperature, thereby keeping the emission wavelengths of all the excitation light source elements 2 constant. Since the blocks (end support blocks 40, 41, inner blocks 42, 43, 44 and outer peripheral blocks 45) constituting the frame 4 are all made of thermally conductive members, the temperature adjustment is arranged by placing a part of the outer surface of the frame 4 The member 5 can make the whole frame 4 uniform temperature. When a laser diode is used as the excitation light source element 2, the emission wavelength changes according to the temperature of the laser diode, but in order to perform efficient excitation, it is required that the wavelength of the excitation light irradiated to the laser medium 10 be maintained at A certain wavelength that is easily absorbed by the laser medium 10. For example, when a neodymium YAG rod is used as the laser medium 10, efficient excitation can be performed by maintaining the wavelength of the excitation light at 798 nm to 808 nm. The laser pump chamber device 1 can maintain the temperature of the laser diode as the excitation light source element 2 by the temperature adjustment member 5 at a temperature (for example, 25 ° C.) that emits light at 798 nm to 808 nm. Therefore, when using a neodymium YAG rod, In the case of the laser medium 10, efficient excitation can be performed. The support space 4B of the irradiation optical system 3 and the excitation light source element 2 composed of the blocks of the housing 4 is arranged at equal intervals around the central axis 10P of the laser medium 10. In the example shown in the figure, the support spaces 4B are arranged at three positions around the central axis 10P at 120 ° intervals. A substrate 2A of the excitation light source element 2 is fixed to a part of the support space 4B on the outer peripheral block 45, and the excitation light source element 2 is supported so that its optical axis is orthogonal to the central axis 10P of the laser medium 10. A cylindrical lens and a lens support member 3A as the irradiation optical system 3 are arranged in a part of the support space 4B, and the irradiation optical system 3 is arranged on the optical axis of the excitation light source element 2. The peripheral space 4A of the laser medium 10 composed of the blocks of the frame 4 is in communication with the support space 4B, and the center thereof is coaxial with the central axis 10P. The plurality of excitation light source elements 2 supported by the support space 4B radiate excitation light from the three directions (other directions) of axisymmetricity to the sides of the laser medium (YAG rod) 10. In addition, in the irradiation optical system 3, the excitation light that is condensed to have a diameter almost the same as the rod diameter of the laser medium 10 is efficiently irradiated to the laser medium 10, and the light reflected on the surface of the laser medium 10 is The cylindrical reflecting surface 4C formed on the inner surface of the surrounding space 4A reflects and is irradiated to the side surface of the laser medium 10 again, so the excitation light is more efficiently radiated to the laser medium 10. Thereby, high-quality light emission having an axis-symmetric output distribution can be obtained from the laser medium 10, and high-output light emission can be obtained by irradiation of efficient excitation light. The housing 4 is provided with a refrigerant inflow path 4D and a refrigerant outflow path 4F, whereby the laser pump chamber device 1 can effectively cool the laser medium 10. In the example shown in the figure, the refrigerant inflow path 4D is a linear flow path extended along the direction intersecting the central axis 10P of the laser medium 10, and three (plurality) are evenly arranged around the central axis 10P. Formed in the end support block 40. The refrigerant outflow path 4F is a linear flow path along the central axis 10P, and is formed in the end support block 41 and the end block 52. In the air-cooled laser pump chamber device 1, a connection portion 4E communicating with the refrigerant inflow path 4D is provided at one of the end blocks 51 in the housing 4, and an air supply pipe for conveying compressed air is connected to the connection portion 4E. 50. Then, the compressed air that has come into contact with the laser medium 10 is exhausted through the refrigerant outflow path 4F formed in the end block 52 and the end support block 41. In this way, the laser pump chamber device 1 is provided with a refrigerant inflow path 4D for allowing compressed air to come in contact with the air from multiple directions on the side of the laser medium 10, and along the central axis 10P is provided with compressed air that has come into contact with the laser medium 10. Since the exhaust gas has a refrigerant outflow path 4F, the laser medium 10 can be efficiently cooled. Thereby, even if it is an air-cooled type, high-output light emission can be obtained. Furthermore, in the laser pump chamber device 1 having such a structure, a circulating water flow path connecting the refrigerant inflow path 4D and the refrigerant outflow path 4F is formed to ensure the tightness in the surrounding space 4A, thereby enabling conversion to water cooling. formula. FIG. 3 shows a laser oscillation device 20 including a laser pump chamber device 1. The laser oscillating device 20 can be arranged within the frame 20A so as to face the central axis 10P of the laser pump chamber device 1, and the resonant mirror including the output mirror 21 and the reflecting mirror 22 is included, and will include 1/4 if necessary The Q switch 23 such as a wavelength plate 23A, a Bockels cell 23B, a polarizer 23C, and the like is arranged in a resonant mirror. This type of laser oscillation device 20 can emit light with an axially symmetrical output distribution from the laser medium 10 by the air-cooled laser pump chamber device 1, and can effectively cool the laser medium 10. It is cold type and can take out high output and high quality laser light. In addition, by ensuring the tightness of the surrounding space 4A in the casing 4 of the laser pump chamber device 1, it can also be converted to a water-cooled laser pump chamber device 1. It is possible to obtain a higher output by setting the water cooling type. The embodiments of the present invention have been described in detail with reference to the drawings, but the specific configuration is not limited to these embodiments, and design changes and the like without departing from the scope of the present invention are also included in the present invention. In addition, as long as there is no particular contradiction or problem in the purpose and configuration of the above-mentioned embodiments, the technologies of each other can be used and combined.
1‧‧‧雷射泵腔室裝置1‧‧‧Laser pump chamber device
2‧‧‧激發光源元件(雷射二極體)2‧‧‧ Excitation light source element (laser diode)
2A‧‧‧基板2A‧‧‧ substrate
3‧‧‧照射光學系統(柱面透鏡)3‧‧‧illumination optical system (cylindrical lens)
3A‧‧‧透鏡支撐構件3A‧‧‧lens support member
4‧‧‧框體4‧‧‧frame
4A‧‧‧周圍空間4A‧‧‧surrounding space
4B‧‧‧支撐空間4B‧‧‧Support Space
4C‧‧‧圓筒反射面4C‧‧‧Cylinder reflective surface
4D‧‧‧冷媒流入路4D‧‧‧Refrigerant inflow
4E‧‧‧連接部4E‧‧‧Connecting Department
4F‧‧‧排氣流出路4F‧‧‧Exhaust Outflow
5‧‧‧溫度調整構件(帕耳帖元件)5‧‧‧Temperature adjustment member (Peltier element)
10‧‧‧雷射介質(YAG桿)10‧‧‧laser medium (YAG rod)
10P‧‧‧中心軸10P‧‧‧Center axis
10A、10B‧‧‧端面10A, 10B‧‧‧face
20‧‧‧雷射振盪裝置20‧‧‧laser oscillator
20A‧‧‧框體20A‧‧‧Frame
21‧‧‧輸出鏡21‧‧‧ output mirror
22‧‧‧反射鏡22‧‧‧Mirror
23‧‧‧Q開關23‧‧‧Q switch
23A‧‧‧1/4波長板23A‧‧‧1 / 4 wave plate
23B‧‧‧勃克爾斯盒23B‧‧‧Bockels Box
23C‧‧‧偏光鏡23C‧‧‧Polarizer
40、41‧‧‧端部支撐塊40, 41‧‧‧ end support blocks
40A、41A‧‧‧開口40A, 41A‧‧‧Open
42、43、44‧‧‧內部塊42, 43, 44 ‧ ‧ ‧ Internal blocks
45‧‧‧外周塊45‧‧‧Peripheral block
50‧‧‧送氣管50‧‧‧Air pipe
51、52‧‧‧端部塊51, 52‧‧‧ end blocks
51A、52A‧‧‧開口51A, 52A‧‧‧Open
53‧‧‧O型圈53‧‧‧O-ring
圖1係表示本發明的實施形態之雷射泵腔室裝置之斷面圖(圖2中之B-B斷面圖)。 圖2係表示本發明的實施形態之雷射泵腔室裝置之斷面圖(圖1中之A-A斷面圖)。 圖3係表示具備雷射泵腔室裝置之雷射振盪裝置之說明圖。Fig. 1 is a sectional view (a sectional view taken along the line B-B in Fig. 2) showing a laser pump chamber device according to an embodiment of the present invention. Fig. 2 is a cross-sectional view (a cross-sectional view taken along A-A in Fig. 1) of a laser pump chamber device according to an embodiment of the present invention. FIG. 3 is an explanatory diagram showing a laser oscillation device including a laser pump chamber device.
Claims (9)
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JP2016162697A JP6736127B2 (en) | 2016-08-23 | 2016-08-23 | Laser pump chamber device |
JP??2016-162697 | 2016-08-23 |
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TW201818624A true TW201818624A (en) | 2018-05-16 |
TWI733886B TWI733886B (en) | 2021-07-21 |
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TW106128388A TWI733886B (en) | 2016-08-23 | 2017-08-22 | Laser pump chamber device and laser oscillation device |
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JP (1) | JP6736127B2 (en) |
KR (1) | KR102332955B1 (en) |
CN (1) | CN109314364B (en) |
TW (1) | TWI733886B (en) |
WO (1) | WO2018037944A1 (en) |
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US5790575A (en) * | 1996-07-15 | 1998-08-04 | Trw Inc. | Diode laser pumped solid state laser gain module |
JPH10341051A (en) * | 1997-06-06 | 1998-12-22 | Toshiba Corp | Solid state laser |
US6052396A (en) * | 1998-02-19 | 2000-04-18 | Trw Inc. | Thermal radiation shield for laser gain module |
JP2008117914A (en) * | 2006-11-02 | 2008-05-22 | Hamamatsu Photonics Kk | Solid-state laser device |
JP2008294484A (en) * | 2008-09-08 | 2008-12-04 | Toshiba Corp | Solid state laser device |
FR2936109B1 (en) * | 2008-09-17 | 2010-10-08 | Thales Sa | OPTICAL PUMPING STRUCTURE. |
CN102237630A (en) * | 2010-04-28 | 2011-11-09 | 北京中视中科光电技术有限公司 | Laser resonant cavity, solid laser and manufacturing method of laser resonant cavity |
JP2012156435A (en) * | 2011-01-28 | 2012-08-16 | Toshiba Corp | Yag laser oscillation device |
CN102377095A (en) * | 2011-11-26 | 2012-03-14 | 刘海强 | Method for clamping crystal by adopting heat emission heat sink in laser diode end-pumped solid-state laser |
CN203747226U (en) * | 2014-03-10 | 2014-07-30 | 上海大学 | Novel multi-lamp pump cavity |
CN205282866U (en) * | 2015-12-18 | 2016-06-01 | 深圳市镭康机械设备有限公司 | Improve ceramic laser pumping cavity of structure |
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CN109314364B (en) | 2021-06-18 |
KR20190039881A (en) | 2019-04-16 |
KR102332955B1 (en) | 2021-11-29 |
TWI733886B (en) | 2021-07-21 |
WO2018037944A1 (en) | 2018-03-01 |
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