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JPS6037636B2 - Carbon dioxide laser emission device - Google Patents
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JPS6037636B2 - Carbon dioxide laser emission device - Google Patents

Carbon dioxide laser emission device

Info

Publication number
JPS6037636B2
JPS6037636B2 JP58036050A JP3605083A JPS6037636B2 JP S6037636 B2 JPS6037636 B2 JP S6037636B2 JP 58036050 A JP58036050 A JP 58036050A JP 3605083 A JP3605083 A JP 3605083A JP S6037636 B2 JPS6037636 B2 JP S6037636B2
Authority
JP
Japan
Prior art keywords
light
optical
carbon dioxide
laser
optical attenuator
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.)
Expired
Application number
JP58036050A
Other languages
Japanese (ja)
Other versions
JPS59161889A (en
Inventor
勝文 熊野
正幸 平間
要右 太田
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.)
Tohoku Ricoh Co Ltd
Original Assignee
Tohoku Ricoh 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 Tohoku Ricoh Co Ltd filed Critical Tohoku Ricoh Co Ltd
Priority to JP58036050A priority Critical patent/JPS6037636B2/en
Publication of JPS59161889A publication Critical patent/JPS59161889A/en
Publication of JPS6037636B2 publication Critical patent/JPS6037636B2/en
Expired legal-status Critical Current

Links

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
    • H01S3/10Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
    • H01S3/13Stabilisation of laser output parameters, e.g. frequency or amplitude
    • H01S3/131Stabilisation of laser output parameters, e.g. frequency or amplitude by controlling the active medium, e.g. by controlling the processes or apparatus for excitation
    • H01S3/134Stabilisation of laser output parameters, e.g. frequency or amplitude by controlling the active medium, e.g. by controlling the processes or apparatus for excitation in gas lasers

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Lasers (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Optics & Photonics (AREA)
  • Surgical Instruments (AREA)
  • Laser Beam Processing (AREA)
  • Laser Surgery Devices (AREA)

Description

【発明の詳細な説明】 (技術分野) 本発明は、レーザメス、レーザ血管吻合装置等の医用機
器に好適な炭酸ガスレーザ出射装置に関するものである
DETAILED DESCRIPTION OF THE INVENTION (Technical Field) The present invention relates to a carbon dioxide laser emitting device suitable for medical equipment such as a laser scalpel and a laser blood vessel anastomosis device.

(従来技術) 従来、医用機器としてのレーザメスや血管吻合装置に炭
酸ガスレーザが使用されているが、この場合、レーザメ
スは通常1〜1肌程度の光出力を必要をし、一方、血管
吻合装置としては5〜100のw程度の微弱出力でよい
(Prior art) Conventionally, carbon dioxide lasers have been used in medical equipment such as laser scalpels and blood vessel anastomosis devices. A weak output of about 5 to 100 watts is sufficient.

このように、両者の所要出力の程度が大きく異なるため
、一般にはそれぞれ専用機として構成されている。とこ
ろで、一連の手術において、切開と吻合の両方が交互に
行なわれるような場合には、一合の装置で兼用できるよ
うにすることが極めて望ましいことは言うまでもない。
As described above, since the required output levels of the two types are significantly different, they are generally configured as dedicated machines for each type. By the way, when both incision and anastomosis are performed alternately in a series of surgeries, it goes without saying that it is extremely desirable to be able to use a single device for both operations.

しかし、光出力を肌wオーダーから1肌オーダーまで3
桁以上も可変にしようとすると、次のような問題がある
。一般にこの種の装置は、レーザ発振部から出射された
レーザ光をビームスプリッタで作業光とモニタ光とに分
割し、モニ夕光を検知してその検知信号により光出力を
制御するようにしている。
However, the light output can be adjusted from skin order to 1 skin order.
If you try to change the number of digits or more, the following problems will occur. Generally, this type of device uses a beam splitter to split the laser light emitted from the laser oscillation unit into working light and monitor light, detects the monitor evening light, and controls the light output based on the detection signal. .

そこで、ビームスプリッ夕の分割比を、例えば、モニ夕
光/作業光=1/10にすると、作業光が10のw〜1
帆のときモニタ光は1のw〜lwとなる。mwオーダー
の光エネルギーは高感度サーモパィルあるいは魚電素子
を用いれば容易に検出可能であり、従って、作業光のl
owwオーダーの出力を安定に制御することができる。
しかし、作業光を1冊程度にしたときを考えると、光セ
ンサには】wの光エネルギーが入ることになり、これで
は高感度光センサは焼損してしまうという事態に直面す
る。このことから、肌w〜1帆にわたる広に光出力範囲
を単一の光センサを用いて連続制御することは、通常で
きない。これを解決する一つの手段は、モニタ光/作業
光の分割比が、例えば1/10と10/1の2種類のビ
ームスプリッタを用意し、高出力の場合は前者を、低出
力の場合は後者をというように切換えて使用することで
ある。
Therefore, if the division ratio of the beam splitter is set to, for example, monitor evening light/work light = 1/10, the work light will be
When the sail is on, the monitor light is 1 w~lw. Light energies on the order of mw can be easily detected using highly sensitive thermopiles or fish-electronic elements, and therefore the working light
It is possible to stably control output on the order of OWW.
However, if we consider the case where the working light is reduced to about one book, the light energy of ]w will enter the optical sensor, and the high-sensitivity optical sensor will be faced with a situation where it will be burnt out. For this reason, it is usually not possible to continuously control a wide light output range over the skin w~1 sail using a single optical sensor. One way to solve this problem is to prepare two types of beam splitters with split ratios of monitor light/work light, for example 1/10 and 10/1, and use the former for high output and the former for low output. The method is to switch and use the latter.

このようにすれば、モニタ光のエネルギー範囲が狭くな
り、一つの光センサで制御が可能となる。しかしながら
、所要の分割比を有するビームスプリッタを得るには、
複雑なコーティング処理等を必要とするので高価であり
、しかも2種類用意しなければならないのでコストが非
常に上昇するという問題があった。(発明の目的)本発
明は、上記問題点を解消するために、光センサの光入射
口に光減衰器又は光エネルギー制限器を挿脱自在に設け
、光出力の大小に応じてこれを挿脱して光検出エネルギ
ー範囲を狭くするとともに、光エネルギー制限器の挿脱
を検出してその検出信号により制御系の基準設定値の切
換えるようにした、低出力から高出力までの広い範囲の
レーザ光が安定して得られる低コストの炭酸ガスレーザ
出射装置を提供するものである。
In this way, the energy range of the monitor light is narrowed and control can be performed with one optical sensor. However, to obtain a beam splitter with the required splitting ratio,
It is expensive because it requires a complicated coating process, and it also has the problem that the cost increases significantly because two types have to be prepared. (Object of the Invention) In order to solve the above-mentioned problems, the present invention provides a light attenuator or a light energy limiter that can be inserted and removed at the light entrance of an optical sensor, and can be inserted or removed according to the magnitude of the light output. Laser light in a wide range from low output to high output.In addition to narrowing the optical detection energy range, the insertion and removal of the optical energy limiter is detected and the reference setting value of the control system is changed based on the detection signal. The object of the present invention is to provide a low-cost carbon dioxide laser emission device that can stably obtain the following.

以下、図面に基づいて実施例を詳細に説明する。Hereinafter, embodiments will be described in detail based on the drawings.

(実施例) 第1図は、本発明の一実施例を示したもので、1は炭酸
ガスレーザ放電管、2は高電圧発生器、3は放電電流制
御器であり、これらによりレーザ発振部が構成されてい
る。
(Embodiment) Fig. 1 shows an embodiment of the present invention, in which 1 is a carbon dioxide laser discharge tube, 2 is a high voltage generator, and 3 is a discharge current controller, which allows the laser oscillation unit to operate. It is configured.

4は部分透過鏡からなるビームスプリッタで、レーザ発
振部から出射されたレーザ光Poを作業光P,とモニタ
光P2とに分割する。
Reference numeral 4 denotes a beam splitter consisting of a partially transmitting mirror, which splits the laser light Po emitted from the laser oscillation section into working light P and monitor light P2.

作業光P,は、図示しない光学系により集光されて患部
等に照射され、生体組織の切開や血管吻合に供せられる
。一方、モニタ光P2は光センサ5により検出されるが
、モニタ光P2のエネルギーが比較的大きいときは、光
センサ5の入射口に部分透過鏡のような光減衰器若しく
はスリットや孔を設けた平板からなる光エネルギー制限
器6を挿入して、光センサ5に達する検出光P3のエネ
ルギーを小さくする。7a,7bは光エネルギー制限器
6の位置検出器で、例えばマイク。
The working light P is focused by an optical system (not shown) and irradiated onto an affected area, etc., and is used for incision of living tissue and blood vessel anastomosis. On the other hand, the monitor light P2 is detected by the optical sensor 5. When the energy of the monitor light P2 is relatively large, an optical attenuator such as a partially transmitting mirror or a slit or hole is provided at the entrance of the optical sensor 5. A light energy limiter 6 made of a flat plate is inserted to reduce the energy of the detection light P3 reaching the optical sensor 5. 7a and 7b are position detectors of the optical energy limiter 6, such as microphones.

スイッチや光力プラ、磁気センサ等からなり、光エネル
ギー制限器6が正規の挿、脱位置(挿脱途中でない)に
ある状態を検出する。8は位置検出器7a又は7bの検
出信号により予め定められた基準信号e,又はe2を出
力する設定値切換器、9は、出力された基準信号e,は
e2と光センサ5の検出信号とを比較し、放電電流制御
器3に制御信号を帰還する偏差増幅器である。
It consists of a switch, an optical power plastic, a magnetic sensor, etc., and detects when the optical energy limiter 6 is in the normal insertion or removal position (not in the middle of insertion or removal). 8 is a setting value switch that outputs a reference signal e or e2 predetermined by the detection signal of the position detector 7a or 7b, and 9 is a set value switch that outputs the reference signal e or e2 that is determined in advance by the detection signal of the position detector 7a or 7b; This is a deviation amplifier that compares the values and feeds back a control signal to the discharge current controller 3.

さらに10は、光エネルギー制限器6の正規の挿、脱位
置にならないとき、即ち、挿脱途中の中間位置にあると
きこれを検出して信号を発し、高電圧発生器2を遮断し
てし−ザ発振を停止させる中間位置検出器である。以上
のように構成された本実施例では、ビームスプリッタ4
を、例えばP2/P,=1/10に固定しても、光世力
が大きい場合は光エネルギー制限器6を挿入して小エネ
ルギーの検出光P3とし、光出力が小さい場合は光エネ
ルギー制限器6を使用せずにモニタ光P2をそのまま検
出光P3とすることができるから、ビームスプリッタが
1種類で済み、しかも光センサとして低コストの小エネ
ルギー用高感度光検出素子を使用することができる。
Further, 10 detects when the optical energy limiter 6 is not at the normal insertion/removal position, that is, when it is at an intermediate position during insertion/removal, and issues a signal to shut off the high voltage generator 2. - An intermediate position detector that stops the oscillation. In this embodiment configured as described above, the beam splitter 4
Even if P2/P is fixed to, for example, 1/10, if the optical power is large, the optical energy limiter 6 is inserted to make the detection light P3 of low energy, and if the optical output is small, the optical energy limiter is inserted. Since the monitor light P2 can be directly used as the detection light P3 without using the sensor 6, only one type of beam splitter is required, and moreover, a low-cost, low-energy, high-sensitivity light detection element can be used as a light sensor. .

また光エネルギー制限器6の挿脱に応じて、それぞれ発
振部制御用の基本設定値が自動的に選択されるので、制
限器挿脱に伴う誤動作を防ぐことができる。さらに、光
エネルギー制限器6の挿脱途中においては発振が停止さ
れるので、レーザ光により生体組織に不用意に損傷を与
えるようなことはない。第2図は、本発明の他の実施例
を示したもので、ビームスプリッタの代りに全反射鏡か
らなるシャツ夕11を使用したものである。
Moreover, since the basic setting values for controlling the oscillator are automatically selected in accordance with the insertion and removal of the optical energy limiter 6, malfunctions caused by insertion and removal of the limiter can be prevented. Furthermore, since the oscillation is stopped during the insertion and removal of the optical energy limiter 6, the laser beam will not inadvertently damage living tissue. FIG. 2 shows another embodiment of the present invention, in which a mirror 11 consisting of a total reflection mirror is used in place of the beam splitter.

この場合、作業時はシャッター1をレーザビームの光路
から外して出射しーザ光Poをそのまま作業光Po′と
し、非作業時はシャツ夕1 1を光路に挿入してPoを
全反射させ、これをモニタ光Po″とする。一般に、レ
ーザ光の連続照射時間は短かし、ので、照射直前の安定
化された放電電流を照射時、つまり非モニタ時に保持す
るようにする。そのためのホールド回路12を偏差増幅
器9と放電電流制御器3の間の設けている。なお、第1
図と同一符号のものは同一のものを示している。以上の
ように構成された本実施例も、光出力の大小に応じて光
エネルギー制御器6を挿脱するので、小エネルギー用光
センサで光世力の制御を行なうことができるとともに、
高価なビームスプリッタを使用せずに済む。
In this case, when working, the shutter 1 is removed from the optical path of the laser beam and the emitted laser beam Po is used as working light Po', and when not working, the shutter 1 is inserted into the optical path to completely reflect Po. This is the monitor light Po''.Generally, the continuous irradiation time of the laser beam is short, so the stabilized discharge current immediately before irradiation is maintained during irradiation, that is, when not monitoring.Hold for this purpose A circuit 12 is provided between the deviation amplifier 9 and the discharge current controller 3.
Items with the same reference numerals as those in the figures indicate the same items. In this embodiment configured as described above, the light energy controller 6 is inserted and removed depending on the magnitude of the light output, so that the light energy can be controlled using a small energy light sensor.
Eliminates the need for expensive beam splitters.

(発明の効果) 以上説明したように、本発明によれば、低出力から高出
力までの広い範囲のレーザ光を安定して出力することが
でき、しかも高価なビームスプリッタの数を減らし、か
つ、光センサも安価な小ェネルギー用光検出素子で済む
ので、コストを大幅に低減することができる。
(Effects of the Invention) As explained above, according to the present invention, it is possible to stably output laser light in a wide range from low output to high output, and also to reduce the number of expensive beam splitters. Since the optical sensor can be an inexpensive low-energy photodetecting element, the cost can be significantly reduced.

さらに、光エネルギー制限器の挿脱に伴なう誤動作を防
ぎ、操作性及び安全性を向上することができる。本発明
になるガスレーザ出射装置は、レーザメス及び血管吻合
兼用機に適用して極めて有効である。
Furthermore, it is possible to prevent malfunctions due to insertion and removal of the optical energy limiter, and improve operability and safety. The gas laser emitting device according to the present invention is extremely effective when applied to a laser scalpel and a device for vascular anastomosis.

【図面の簡単な説明】 第1図は、本発明の一実施例の構成図、第2図は、本発
明の他の実施例の構成図である。 1・・・・・・炭酸ガスレーザ放電管、2・・・・・・
高電圧発生器、3・・・・・・放電電流制御器、4・・
・・・・ビームスプリツタ、5……光センサ、6……光
エネルギー制御器、7a,7b・・・…位置検出器、8
・・・・・・設定値切換器、9・・・・・・偏差増幅器
、10・・・・・・中間位置検出器、11……シャツ夕
、12……ホールド回路。 舞ー図 第2図
BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a block diagram of one embodiment of the present invention, and FIG. 2 is a block diagram of another embodiment of the present invention. 1... Carbon dioxide laser discharge tube, 2...
High voltage generator, 3... Discharge current controller, 4...
... Beam splitter, 5... Optical sensor, 6... Light energy controller, 7a, 7b... Position detector, 8
. . . Set value switch, 9 . . . Deviation amplifier, 10 . . . Intermediate position detector, 11 . . . Maizu figure 2

Claims (1)

【特許請求の範囲】 1 炭酸ガス放電管、高電圧発生器、放電電流制御器か
らなるレーザ発振部と、該レーザ発振部から出射された
レーザ光を作業光とモニタ光とに分割する手段若しくは
作業光とモニタ光に切換える手段と、前記モニタ光を検
出する光検出器と、該光検出器の光入射口に挿脱自在に
設けられた光減衰器若しくは光エネルギー制限器と、該
光減衰器若しくは光エネルギー制限器の位置を検出する
位置検出手段と、前記光減衰器若しくは光エネルギー制
限器が正規の挿、脱位置にあるとき前記位置検出手段か
らそれぞれ出力される信号に応じて予め決められた基準
信号を出力する手段と、出力された基準信号と前記光検
出器の検出信号とを比較して前記放電電流制御器に帰還
する制御信号を出力する手段とからなることを特徴とす
る炭酸ガスレーザ出射装置。 2 前記位置検出手段は、前記光減衰器若しくは光エネ
ルギー制限器が正規の挿、脱位置にないとき、前記高電
圧発生器を遮断する信号を出力し、レーザ発振を停止す
ることを特徴とする特許請求の範囲第1項記載の炭酸ガ
スレーザ出射装置。
[Scope of Claims] 1. A laser oscillation section consisting of a carbon dioxide gas discharge tube, a high voltage generator, and a discharge current controller, and means for dividing the laser light emitted from the laser oscillation section into working light and monitor light. means for switching between working light and monitor light; a photodetector for detecting the monitor light; an optical attenuator or optical energy limiter removably installed in a light entrance of the photodetector; and the optical attenuator. position detection means for detecting the position of the optical attenuator or optical energy limiter; and a position detection means for detecting the position of the optical attenuator or optical energy limiter, and and means for comparing the output reference signal and the detection signal of the photodetector and outputting a control signal to be fed back to the discharge current controller. Carbon dioxide laser emission device. 2. The position detection means is characterized in that when the optical attenuator or the optical energy limiter is not in the normal insertion/removal position, the position detection means outputs a signal that cuts off the high voltage generator and stops laser oscillation. A carbon dioxide laser emission device according to claim 1.
JP58036050A 1983-03-07 1983-03-07 Carbon dioxide laser emission device Expired JPS6037636B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58036050A JPS6037636B2 (en) 1983-03-07 1983-03-07 Carbon dioxide laser emission device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58036050A JPS6037636B2 (en) 1983-03-07 1983-03-07 Carbon dioxide laser emission device

Publications (2)

Publication Number Publication Date
JPS59161889A JPS59161889A (en) 1984-09-12
JPS6037636B2 true JPS6037636B2 (en) 1985-08-27

Family

ID=12458882

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58036050A Expired JPS6037636B2 (en) 1983-03-07 1983-03-07 Carbon dioxide laser emission device

Country Status (1)

Country Link
JP (1) JPS6037636B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH07108302B2 (en) * 1992-08-14 1995-11-22 旭光学工業株式会社 Output attenuator for laser treatment device

Also Published As

Publication number Publication date
JPS59161889A (en) 1984-09-12

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