JP2001317995A - Power damper for high power laser, laser power meter and laser power measuring method - Google Patents

Power damper for high power laser, laser power meter and laser power measuring method

Info

Publication number
JP2001317995A
JP2001317995A JP2000134989A JP2000134989A JP2001317995A JP 2001317995 A JP2001317995 A JP 2001317995A JP 2000134989 A JP2000134989 A JP 2000134989A JP 2000134989 A JP2000134989 A JP 2000134989A JP 2001317995 A JP2001317995 A JP 2001317995A
Authority
JP
Japan
Prior art keywords
laser
power
conical
laser beam
light receiving
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.)
Withdrawn
Application number
JP2000134989A
Other languages
Japanese (ja)
Inventor
Motoi Kido
基 城戸
Atsushi Sugibashi
敦史 杉橋
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.)
Nippon Steel Corp
Original Assignee
Nippon Steel Corp
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 Nippon Steel Corp filed Critical Nippon Steel Corp
Priority to JP2000134989A priority Critical patent/JP2001317995A/en
Publication of JP2001317995A publication Critical patent/JP2001317995A/en
Withdrawn legal-status Critical Current

Links

Landscapes

  • Photometry And Measurement Of Optical Pulse Characteristics (AREA)
  • Lasers (AREA)

Abstract

PROBLEM TO BE SOLVED: To prevent laser energy from concentrating locally in a conical laser beam receiving part. SOLUTION: In the power damper for absorbing laser energy at a laser beam receiving part 11 as thermal energy, by having a conical beam receiving surface irradiated with a laser beam and the laser power meter for measuring the laser power, a laser beam LB is inclined with respect to the cone center axis 1 and incident off the cone center axis 1 toward a direction perpendicular thereto, after passing the cone vertex 3 and two laser beams on a plane involving the cone center axis 1 and the laser beam center axis 5 reflect and advance at reflecting regions in the conical beam-receiving surface, where among the reflecting regions the second and third reflecting regions do not mutually overlap.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、高出力レーザ用の
パワーダンパー、レーザ出力計およびレーザ出力測定方
法に関する。
The present invention relates to a power damper for a high-power laser, a laser power meter, and a laser power measuring method.

【0002】[0002]

【従来の技術】近年、レーザ発振器の進歩により、kW
クラスの高出力レーザが金属の切断・溶接等を主体とし
た幅広い工業分野で使用されている。レーザ加工は1mm
径程度の小さなエリアにレーザビームを集光し、極めて
高いエネルギー密度により瞬時に加工を完了することで
精度・品質に優れることが特徴である。加工品質は、レ
ーザ出力、光学系により決定されるレーザ集光径、加工
アシストガスなど加工パラメータの影響を大きく受け、
特にレーザ出力を適切に設定することが良好なレーザ加
工を行なう上で不可欠な要素となる。
2. Description of the Related Art In recent years, with the advance of laser oscillators, kW
High-power lasers of a class are used in a wide range of industrial fields mainly for cutting and welding of metals. Laser processing is 1mm
The laser beam is focused on an area as small as the diameter, and the processing is completed instantaneously with an extremely high energy density. Processing quality is greatly affected by processing parameters such as laser output, laser focus diameter determined by the optical system, and processing assist gas.
In particular, setting the laser output appropriately is an essential element in performing good laser processing.

【0003】図8に、従来用いられている水冷パワーダ
ンプ方式のレーザ出力計の一例を示す。このレーザ出力
計10は、主として、円錐型レーザ受光部11(内側円
錐)と、ケーシング(外側円錐)12と、両者の間に設
けられた案内板14により螺旋状の冷却水路15が形成
されている。給水装置20から冷却水が配管21を介し
て冷却水路15に供給される。レーザ出力計用として、
入口16側に冷却水流量計23、熱電対等の水温計24
が、出口17側に水温計26がそれぞれ設けられてい
る。これら計器で測定された冷却水の流量Q、入側温度
1および出側温度T0の測定値はコントローラー28に
出力される。
FIG. 8 shows an example of a conventional water-cooled power dump type laser power meter. In the laser power meter 10, a helical cooling water passage 15 is mainly formed by a conical laser receiving section 11 (inner cone), a casing (outer cone) 12, and a guide plate 14 provided therebetween. I have. Cooling water is supplied from the water supply device 20 to the cooling water passage 15 via the pipe 21. For laser power meter
A cooling water flow meter 23 and a water temperature meter 24 such as a thermocouple are provided on the inlet 16 side.
However, a water temperature gauge 26 is provided on the outlet 17 side. The measured values of the flow rate Q of the cooling water, the inlet temperature T 1, and the outlet temperature T 0 measured by these instruments are output to the controller 28.

【0004】このようなレーザ出力計10の円錐型レー
ザ受光部11に向けてレーザLBを照射すると、レーザ
LBはレーザ受光部11の円錐状受光面で多重反射を繰
り返しながら吸収され、レーザのエネルギーは円錐型レ
ーザ受光部11に熱エネルギーとして伝達される。前記
冷却水路15に冷却水を流すことによって円錐型レーザ
受光部11の熱は冷却水に伝達される。コントローラー
28は、このようにして冷却水に伝達された熱量を冷却
水の流量と温度上昇量から算出してエネルギー換算を行
い、この値に必要に応じて補正を加えた制御信号をレー
ザ発振器(図示しない)に出力する。
When the laser LB is irradiated toward the conical laser receiving section 11 of the laser power meter 10, the laser LB is absorbed while repeating multiple reflections on the conical light receiving surface of the laser receiving section 11, and the energy of the laser LB is absorbed. Is transmitted to the conical laser receiving unit 11 as thermal energy. By flowing the cooling water through the cooling water passage 15, the heat of the conical laser light receiving unit 11 is transmitted to the cooling water. The controller 28 calculates the amount of heat transmitted to the cooling water from the flow rate of the cooling water and the amount of temperature rise in this manner, converts the amount of energy, converts the control signal as necessary to a laser oscillator ( (Not shown).

【0005】水冷パワーダンプ方式のレーザ出力計は、
全レーザ出力を測定する際には、精度が良好で、数10
kWまでの大出力レーザについても出力測定が可能であ
るとされ、炭酸ガスレーザの出力計として広く用いられ
ている。
A water-cooled power dump type laser power meter is
When measuring the total laser output, the accuracy is good,
It is said that the output can be measured even with a high output laser of up to kW, and is widely used as an output meter of a carbon dioxide laser.

【0006】[0006]

【発明が解決しようとする課題】しかしながら、従来、
水冷パワーダンプ方式によりレーザ出力を測定する際に
は、レーザビームBLをレーザ出力計10の円錐中心軸
1と平行に、円錐頂点3に向けて照射していた。このた
め、円錐頂点3付近のエネルギー密度が極めて高くな
り、測定するレーザの出力によっては円錐頂点3付近に
溶損が発生するおそれがあった。
However, conventionally,
When measuring the laser output by the water-cooled power dump method, the laser beam BL was irradiated toward the conical vertex 3 in parallel with the conical center axis 1 of the laser power meter 10. For this reason, the energy density near the conical apex 3 becomes extremely high, and there is a possibility that erosion may occur near the conical apex 3 depending on the output of the laser to be measured.

【0007】[0007]

【課題を解決するための手段】本発明は、上記課題を解
決するためのものであって、その要旨とするところは、
以下のとおりである。 (1)断面がリング状のレーザビームを円錐型受光面に
照射し、レーザのエネルギーをレーザ受光部に熱エネル
ギーとして吸収させるパワーダンパーにおいて、レーザ
ビームを円錐中心軸に対して傾けかつ円錐頂点を通り円
錐中心軸に直交する方向にずらして入射させるための受
光部位置調整機能を持つことを特徴とする高出力レーザ
用パワーダンパー。 (2)上記(1)に記載のパワーダンパーに吸収した熱
エネルギーを測定するための熱エネルギー測定手段を付
加したことを特徴とする高出力レーザ用出力計。熱エネ
ルギー測定手段として、冷却水流量計、パワーダンパー
の入側水温計、出側水温計などを用いる。 (3)断面がリング状のレーザビームを円錐型受光面に
照射し、レーザエネルギーをレーザ受光部に熱エネルギ
ーとして吸収させてレーザ出力を測定するレーザ出力測
定方法において、レーザビームを円錐中心軸に対して傾
けかつ円錐頂点を通り円錐中心軸に直交する方向にずら
して入射させ、円錐中心軸とレーザビーム中心軸とを含
む平面内上に存在する二つのレーザビームが前記円錐型
受光面内で反射進行する反射領域のうち、第2番目の反
射領域と第3番目の反射領域とが互いに重ならないよう
にすることを特徴とするレーザ出力測定方法。
SUMMARY OF THE INVENTION The present invention has been made to solve the above problems, and the gist of the invention is as follows.
It is as follows. (1) In a power damper that irradiates a laser beam having a ring-shaped cross section onto a conical light receiving surface and absorbs laser energy as heat energy in a laser light receiving unit, the laser beam is inclined with respect to the central axis of the cone and the vertex of the cone is formed. A power damper for a high-power laser, which has a function of adjusting a position of a light receiving portion for making light incident in a direction orthogonal to a central axis of a through cone. (2) A power meter for a high-power laser, wherein a heat energy measuring means for measuring the heat energy absorbed by the power damper according to (1) is added. As the thermal energy measuring means, a cooling water flow meter, an inlet water temperature meter of the power damper, an outlet water temperature meter, or the like is used. (3) In a laser output measuring method for irradiating a laser beam having a ring-shaped cross section to a conical light receiving surface and causing the laser light receiving portion to absorb laser energy as thermal energy and measure laser output, the laser beam is focused on a conical central axis. The two laser beams which are inclined with respect to each other and are shifted in the direction perpendicular to the conical central axis through the conical apex, and two laser beams existing on a plane including the conical central axis and the laser beam central axis are within the conical light receiving surface. A laser output measuring method, wherein a second reflection region and a third reflection region are not overlapped with each other among reflection regions which are reflected.

【0008】[0008]

【発明の実施の形態】従来の水冷パワーダンパーおよび
パワーダンプ方式によるレーザ測定方法が、レーザビー
ムを円錐型レーザ受光部の中心軸と水平に、レーザ受光
部の中心に向けて照射していたのに対して、本発明のパ
ワーダンパー、レーザ出力計および測定方法は、レーザ
ビームを円錐型レーザ受光部の中心軸に対して、傾斜か
つずらした位置に照射させることを最大の特徴としてい
る。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS A conventional laser measurement method using a water-cooled power damper and a power dump method irradiates a laser beam horizontally to a central axis of a conical laser light receiving portion toward the center of the laser light receiving portion. On the other hand, the power damper, the laser power meter, and the measuring method of the present invention are most characterized in that the laser beam is applied to a position inclined and shifted with respect to the center axis of the conical laser receiving unit.

【0009】図1は、本発明の出力計30を示してい
る。前述の図8に示す部材と同様の部材には同一の参照
符号を付け、その説明は省略する。図1にあるとおり、
円錐状の出力計本体31は、2本のアーム34、35を
介して架台32に支持されている。アーム34.35の
下端部はねじ部36となっており、架台32に固定され
たナット38にはめ合っている。アーム34、35を回
転して長さを調整して、出力計本体31に対する入射レ
ーザビームの高さ位置と傾きを調整する。
FIG. 1 shows a power meter 30 of the present invention. The same members as those shown in FIG. 8 described above are denoted by the same reference numerals, and description thereof will be omitted. As shown in FIG.
The conical power meter main body 31 is supported on a gantry 32 via two arms 34 and 35. The lower ends of the arms 34 and 35 are screw portions 36, which are fitted to nuts 38 fixed to the gantry 32. The height and the inclination of the incident laser beam with respect to the power meter main body 31 are adjusted by rotating the arms 34 and 35 to adjust the length.

【0010】図9に、レーザビームLBをレーザ受光部
中心軸1と平行にレーザ受光部11の中心3に向けて照
射した際に、円錐状受光面11aで、レーザが多重反射
する様子を示す。このときレーザビームLBは多重反射
しながら円錐状受光面11aに対する入射角が小さくな
る。これに伴い吸収率も例が図6にあるとおり大きくな
り第2番目の反射領域、第3番目の反射領域で大きく吸
収される。この際に、図中にある通り上第2番目の反射
領域と下第3番目の反射領域、下第2番目の反射領域と
上第3番目の反射領域が重なり、同時にあたる点では吸
収エネルギーが重畳され非常に大きくなる。円錐状受光
面11aで吸収されるレーザエネルギー密度分布をシミ
ュレーションした結果を図10に示す。シミュレーショ
ン条件としては、レーザ出力33kW、レーザビームは
図7にあるとおり外径100mm、内径60mmのリング
状、円錐型受光面開口部径は170mm、頂角は30度で
ある。円錐状受光面は吸収効率を上げるため酸化銅等の
黒染め処理が施されており、この結果の吸収率は図6に
あるとおり、角度依存のあるものである。図10に示さ
れる様に円錐頂点より25mm〜45mm付近では、吸収パ
ワー密度が極めて高くなるため、長時間運転においては
円錐頂点付近が溶損するおそれがある。
FIG. 9 shows how the laser beam is reflected multiple times on the conical light receiving surface 11a when the laser beam LB is irradiated toward the center 3 of the laser light receiving portion 11 in parallel with the central axis 1 of the laser light receiving portion. . At this time, the angle of incidence of the laser beam LB on the conical light receiving surface 11a is reduced while performing multiple reflections. As a result, the absorptance also increases as shown in FIG. 6, and is greatly absorbed in the second and third reflection areas. At this time, as shown in the figure, the upper second reflection area and the lower third reflection area, the lower second reflection area and the upper third reflection area overlap, and at the same time, the absorption energy is reduced. Superimposed and very large. FIG. 10 shows a simulation result of the laser energy density distribution absorbed by the conical light receiving surface 11a. As the simulation conditions, the laser output is 33 kW, the laser beam is a ring-shaped, conical light-receiving surface having an outer diameter of 100 mm and an inner diameter of 60 mm as shown in FIG. 7, and the apex angle is 30 degrees. The conical light-receiving surface has been subjected to a black dyeing treatment with copper oxide or the like in order to increase the absorption efficiency, and the resulting absorption rate has an angle dependence as shown in FIG. As shown in FIG. 10, the absorption power density becomes extremely high in the vicinity of 25 mm to 45 mm from the apex of the cone.

【0011】図2にレーザビームをレーザ受光部中心軸
1に対し10度、円錐頂点3に対し20mmずらした位置
にレーザビームLBを照射した様子を示す。シミュレー
ション条件としては、レーザ出力33kW、レーザビー
ムは図7にあるとおり外径100mm、内径60mmのリン
グ状、円錐型受光面開口部径は170mm、頂角は30度
である。レーザ受光部11の円錐状受光面11aは吸収効
率を上げるため酸化銅等の黒染め処理が施されており、
この結果の吸収率は図6にあるとおり、角度依存のある
ものである。この時、図2中にあるとおり上第2番目の
反射領域と下第3番目の反射領域、下第2番目の反射領
域と上第3番目の反射領域が重ならずレーザビームLB
は、分散吸収され、L1、L2上で図3および図4のよう
に、最大位置でも上記レーザビームLBが平行であると
きの条件(図10)に比べ約3割吸収パワーが下がって
いることがわかった。
FIG. 2 shows a state in which the laser beam is irradiated at a position shifted by 10 degrees with respect to the central axis 1 of the laser receiving portion and by 20 mm with respect to the vertex 3 of the cone. As the simulation conditions, the laser output is 33 kW, the laser beam is a ring-shaped, conical light-receiving surface having an outer diameter of 100 mm and an inner diameter of 60 mm as shown in FIG. 7, and the apex angle is 30 degrees. The conical light receiving surface 11a of the laser light receiving unit 11 has been subjected to blackening treatment such as copper oxide to increase absorption efficiency,
The resulting absorptance is angle dependent, as shown in FIG. At this time, as shown in FIG. 2, the upper second reflection area and the lower third reflection area, the lower second reflection area and the upper third reflection area do not overlap, and the laser beam LB does not overlap.
Are dispersed and absorbed, and as shown in FIGS. 3 and 4 on L 1 and L 2 , the absorption power is reduced by about 30% compared to the condition (FIG. 10) when the laser beam LB is parallel even at the maximum position. I knew it was there.

【0012】この条件の具体的な決め方としては、図5
に示すレーザビーム外径Do、ビーム内径Din、円錐頂
角2α、ビーム傾き角β、ビームずらし量Dpにおい
て、以下の2つの式が成立することが必要である。式
(1)は上第2番目の反射領域が下第3番目の反射領域
より奥であることの条件であり、式(2)は上第1番目
の反射領域が円錐状受光面の上部内に収まることの条件
である。
FIG. 5 shows a specific method for determining these conditions.
In the laser beam outer diameter Do, the beam inner diameter Din, the cone apex angle 2α, the beam inclination angle β, and the beam shift amount Dp, the following two expressions need to be satisfied. Equation (1) is a condition that the upper second reflection area is deeper than the lower third reflection area, and equation (2) is that the upper first reflection area is in the upper part of the conical light receiving surface. It is a condition to fit in.

【数1】 (Equation 1)

【0013】本発明は、このようにレーザビームを照射
することによって、円錐状受光面における吸収エネルギ
密度の部分的な集中を防ぎ、円錐型レーザ受光部に発生
する溶損を防止することができる。
According to the present invention, by irradiating the laser beam in this manner, it is possible to prevent the absorption energy density from being partially concentrated on the conical light receiving surface and to prevent the erosion generated in the conical laser light receiving portion. .

【0014】[0014]

【実施例】〔本発明例〕円錐状受光面開口部径が170
mm、円錐頂角は30度であるレーザ出力計を製作した。
円錐状受光面は吸収効率を上げるため酸化銅の黒染め処
理が施されており、この結果の吸収率は図4にあるとお
りであった。レーザ出力は33.0kW、レーザビーム
は外径Do=100mm、内径Din=60mmのリング状で
ある高出力炭酸ガスレーザで、レーザビームをレーザ受
光部中心軸に対しβ=10度、円錐頂点に対しDp=2
0mmずらした位置にレーザビームを照射し出力を測定し
た。冷却部には、水温10度の冷却水を毎分40.0L
で供給した。このとき、入側水温は10度、出側水温は
24度で出力計の指示値は33.0kWであった。この
条件で8000時間連続照射したが、円錐型レーザ受光
部に変形や溶損は発生しなかった。
DESCRIPTION OF THE PREFERRED EMBODIMENTS [Example of the present invention] The conical light receiving surface opening diameter is 170.
A laser power meter having a mm and a cone apex angle of 30 degrees was manufactured.
The conical light-receiving surface was subjected to a blackening treatment of copper oxide in order to increase the absorption efficiency, and the resulting absorption was as shown in FIG. The laser output is 33.0 kW, and the laser beam is a ring-shaped high-power carbon dioxide laser having an outer diameter Do = 100 mm and an inner diameter Din = 60 mm. Dp = 2
A laser beam was irradiated to a position shifted by 0 mm, and the output was measured. In the cooling unit, 40.0 L of cooling water at a water temperature of 10 degrees per minute
Supplied with At this time, the inlet water temperature was 10 degrees, the outlet water temperature was 24 degrees, and the indicated value of the output meter was 33.0 kW. Irradiation was continued for 8000 hours under these conditions, but no deformation or erosion occurred in the conical laser receiving portion.

【0015】〔比較例〕比較例として、その他の条件は
変えずにレーザの傾きβ=0、ずらし量Dp:0とし円
錐中心軸に平行にレーザビームを照射したところ、上記
テストで約5000時間にて円錐頂点より約25mmの位
置で溶損が発生した。
COMPARATIVE EXAMPLE As a comparative example, a laser beam was irradiated in parallel with the central axis of the cone with the laser inclination β = 0 and the shift amount Dp = 0 without changing other conditions. At about 25 mm from the apex of the cone, erosion occurred.

【図面の簡単な説明】[Brief description of the drawings]

【図1】本発明による水冷パワーダンプ方式レーザ出力
計の一例を示す装置構成図である。
FIG. 1 is an apparatus configuration diagram showing an example of a water-cooled power dump laser output meter according to the present invention.

【図2】本発明における円錐状受光面でのレーザ反射の
状態を示す模式図である。
FIG. 2 is a schematic diagram showing a state of laser reflection on a conical light receiving surface in the present invention.

【図3】本発明における円錐状受光面のうち、図2のL
1上での吸収パワー密度のシミュレーション結果を示す
線図である。
FIG. 3 is a perspective view of a conical light receiving surface according to the present invention;
FIG. 4 is a diagram showing a simulation result of an absorption power density on 1 .

【図4】本発明における円錐状受光面のうち、図2のL
2上での吸収パワー密度のシミュレーション結果を示す
線図である。
FIG. 4 is a sectional view of the conical light receiving surface according to the present invention;
Is a graph showing the simulation result of the absorption power density on 2.

【図5】本発明での条件決定のための、必要パラメータ
を説明する図面である。
FIG. 5 is a view for explaining necessary parameters for determining conditions in the present invention.

【図6】一般に用いられている水冷パワーダンプ方式の
内面吸収率測定結果の一例を示す線図である。
FIG. 6 is a diagram showing an example of a measurement result of an inner surface absorptance of a generally used water-cooled power dump system.

【図7】一般的な高出力レーザのビーム形状の一例を示
す模式図である。
FIG. 7 is a schematic diagram illustrating an example of a beam shape of a general high-power laser.

【図8】従来用いられている水冷パワーダンプ方式のレ
ーザ出力計の一例を示す装置構成図である。
FIG. 8 is a device configuration diagram showing an example of a conventionally used water-cooled power dump type laser power meter.

【図9】従来法における円錐状受光面でのレーザ反射の
状態を示す模式図である。
FIG. 9 is a schematic diagram showing a state of laser reflection on a conical light receiving surface in a conventional method.

【図10】従来法における円錐状受光面での吸収パワー
密度のシミュレーション結果を示す線図である。
FIG. 10 is a diagram showing a simulation result of an absorption power density on a conical light receiving surface in a conventional method.

【符号の説明】[Explanation of symbols]

1 円錐中心軸 3 円錐頂点 5 レーザビーム軸 10 レーザ出力計 11 円錐型レーザ受光部 11a 円錐状受光面 12 ケーシング 15 冷却水路 20 給水装置 23 冷却水流量計 24 入側水温計 26 出側水温計 28 コントローラー 30 レーザ出力計 31 出力計本体 32 架台 34、35 アーム(受光部位置調整機能) 38 ナット (受光部位置調整機能) DESCRIPTION OF SYMBOLS 1 Conical center axis 3 Conical vertex 5 Laser beam axis 10 Laser power meter 11 Conical laser light receiving part 11a Conical light receiving surface 12 Casing 15 Cooling water channel 20 Water supply device 23 Cooling water flow meter 24 Inlet water temperature meter 26 Outlet water temperature meter 28 Controller 30 Laser output meter 31 Output meter main body 32 Mount 34, 35 Arm (Light receiving part position adjusting function) 38 Nut (Light receiving part position adjusting function)

フロントページの続き Fターム(参考) 2G065 AA04 AB09 BA11 BB24 BB41 BC13 DA05 5F072 AA05 HH02 JJ05 TT01 TT11 YY11 Continued on the front page F term (reference) 2G065 AA04 AB09 BA11 BB24 BB41 BC13 DA05 5F072 AA05 HH02 JJ05 TT01 TT11 YY11

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 断面がリング状のレーザビームを円錐状
受光面に照射し、レーザのエネルギーをレーザ受光部に
熱エネルギーとして吸収させるパワーダンパーにおい
て、レーザビームを円錐中心軸に対して傾けかつ円錐頂
点を通り円錐中心軸に直交する方向にずらして入射させ
るための受光部位置調整機能を持つことを特徴とする高
出力レーザ用パワーダンパー。
1. A power damper for irradiating a conical light receiving surface with a laser beam having a ring-shaped cross section to absorb laser energy as heat energy in a laser light receiving section, wherein the laser beam is inclined with respect to a central axis of the cone and conical. A power damper for a high-power laser, which has a function of adjusting the position of a light-receiving portion for causing light to enter while being shifted in a direction perpendicular to a central axis of a cone passing through a vertex.
【請求項2】 請求項1に記載のパワーダンパーに吸収
した熱エネルギーを測定するための熱エネルギー測定手
段を付加したことを特徴とする高出力レーザ用出力計。
2. A power meter for a high-power laser, further comprising a thermal energy measuring means for measuring thermal energy absorbed by the power damper according to claim 1.
【請求項3】 断面がリング状のレーザビームを円錐状
受光面に照射し、レーザエネルギーをレーザ受光部に熱
エネルギーとして吸収させてレーザ出力を測定するレー
ザ出力測定方法において、レーザビームを円錐中心軸に
対して傾けかつ円錐頂点を通り円錐中心軸に直交する方
向にずらして入射させ、円錐中心軸とレーザビーム中心
軸とを含む平面内上に存在する二つのレーザビームが前
記円錐状受光面で反射進行する反射領域のうち、第2番
目の反射領域と第3番目の反射領域とが互いに重ならな
いようにすることを特徴とするレーザ出力測定方法。
3. A laser power measuring method for irradiating a conical light receiving surface with a laser beam having a ring-shaped cross section and absorbing laser energy as heat energy in a laser light receiving section to measure a laser output. Two laser beams present on a plane including the conical central axis and the laser beam central axis are tilted with respect to the axis and shifted in a direction perpendicular to the conical central axis through the conical apex. A second reflection area and a third reflection area of the reflection areas which are reflected and propagated in the step (a), do not overlap each other.
JP2000134989A 2000-05-08 2000-05-08 Power damper for high power laser, laser power meter and laser power measuring method Withdrawn JP2001317995A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2000134989A JP2001317995A (en) 2000-05-08 2000-05-08 Power damper for high power laser, laser power meter and laser power measuring method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2000134989A JP2001317995A (en) 2000-05-08 2000-05-08 Power damper for high power laser, laser power meter and laser power measuring method

Publications (1)

Publication Number Publication Date
JP2001317995A true JP2001317995A (en) 2001-11-16

Family

ID=18643160

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2000134989A Withdrawn JP2001317995A (en) 2000-05-08 2000-05-08 Power damper for high power laser, laser power meter and laser power measuring method

Country Status (1)

Country Link
JP (1) JP2001317995A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103148948A (en) * 2013-02-06 2013-06-12 西北核技术研究所 Device for measuring high-energy laser energy
CN104685329A (en) * 2012-09-27 2015-06-03 三菱电机株式会社 Power damper, laser output meter, laser output measurement method, and laser output monitoring system
CN104833418A (en) * 2015-05-13 2015-08-12 西安交通大学 Method for measuring laser energy density and total energy by use of mall-measuring-range energy meter
CN113884181A (en) * 2020-07-03 2022-01-04 住友重机械工业株式会社 Laser power measuring device

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104685329A (en) * 2012-09-27 2015-06-03 三菱电机株式会社 Power damper, laser output meter, laser output measurement method, and laser output monitoring system
CN103148948A (en) * 2013-02-06 2013-06-12 西北核技术研究所 Device for measuring high-energy laser energy
CN104833418A (en) * 2015-05-13 2015-08-12 西安交通大学 Method for measuring laser energy density and total energy by use of mall-measuring-range energy meter
CN113884181A (en) * 2020-07-03 2022-01-04 住友重机械工业株式会社 Laser power measuring device

Similar Documents

Publication Publication Date Title
EP1982221B9 (en) Optical fiber connector
US11255723B2 (en) Beam power measurement with widening
US20060186098A1 (en) Method and apparatus for laser processing
CN108563034B (en) Reflective spatial filter debugging device and method
EP1700665B1 (en) Laser apparatus
Miyamoto et al. Analysis of thermally induced optical distortion in lens during focusing high-power CO2 laser beam
JP2011082298A (en) Laser beam absorbing device, and solid-state laser device including the same
JP4537763B2 (en) Method and apparatus for spot welding using a laser beam
JP2001317995A (en) Power damper for high power laser, laser power meter and laser power measuring method
JPH03137538A (en) Method and device for deciding focus of laser beam
JPH06152018A (en) Solid-state laser device and laser machining device
JP2002214037A (en) Power damper for high power laser, laser power meter and laser power measuring method
KR100809924B1 (en) Method and device for the measuring of the optical power loss in a fiber of optical contact means
CN111571019A (en) Device and method for laser shock processing of curved surface part
JPH0819881A (en) Laser beam device for heating of tubular body
JP2602711B2 (en) Optical system thermal deformation control device and operation method thereof
JP2000227576A (en) Emission optical system for laser processing device
JP4225121B2 (en) Laser annealing method and apparatus
JPH0466288A (en) Laser beam machine
CN118699606A (en) Laser power meter, laser processing system and method of using the same
JPH10326931A (en) Laser beam damper
US7071444B2 (en) High performance system and method for capturing and absorbing radiation
JPH07232291A (en) Laser beam machine
JP2817555B2 (en) Laser processing machine
EP1687662A2 (en) High performance system and method for capturing and absorbing radiation

Legal Events

Date Code Title Description
A300 Withdrawal of application because of no request for examination

Free format text: JAPANESE INTERMEDIATE CODE: A300

Effective date: 20070807