JPH022190A - Laser device - Google Patents

Laser device

Info

Publication number
JPH022190A
JPH022190A JP14603088A JP14603088A JPH022190A JP H022190 A JPH022190 A JP H022190A JP 14603088 A JP14603088 A JP 14603088A JP 14603088 A JP14603088 A JP 14603088A JP H022190 A JPH022190 A JP H022190A
Authority
JP
Japan
Prior art keywords
laser
dye
excitation light
oscillation element
focal line
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
JP14603088A
Other languages
Japanese (ja)
Inventor
Tatsu Hirano
達 平野
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.)
Hamamatsu Photonics KK
Original Assignee
Hamamatsu Photonics KK
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 Hamamatsu Photonics KK filed Critical Hamamatsu Photonics KK
Priority to JP14603088A priority Critical patent/JPH022190A/en
Publication of JPH022190A publication Critical patent/JPH022190A/en
Pending 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
    • H01S3/09Processes or apparatus for excitation, e.g. pumping
    • H01S3/091Processes or apparatus for excitation, e.g. pumping using optical pumping
    • H01S3/0915Processes or apparatus for excitation, e.g. pumping using optical pumping by incoherent light
    • H01S3/092Processes or apparatus for excitation, e.g. pumping using optical pumping by incoherent light of flash lamp
    • H01S3/093Processes or apparatus for excitation, e.g. pumping using optical pumping by incoherent light of flash lamp focusing or directing the excitation energy into the active medium
    • H01S3/0931Imaging pump cavity, e.g. elliptical
    • 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
    • H01S3/23Arrangements of two or more lasers not provided for in groups H01S3/02 - H01S3/22, e.g. tandem arrangements of separate active media
    • H01S3/2383Parallel arrangements

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Optics & Photonics (AREA)
  • Lasers (AREA)

Abstract

PURPOSE:To emit a plurality of laser lights by one unit of laser device by laminating a plurality of elliptic tube whose inner surface is an excitation light reflecting surface so that one focal line of each tube is common to form a laminated elliptic tube, by arranging an excitation light source on the common focal line of the laser head and by arranging a laser oscillation element on each of the other plurality of focal lines respectively. CONSTITUTION:A laser head 1 is formed in a laminated elliptic tube which is made by joining a curbed plate body divided into four whose inner surface is an excitation light reflecting mirror and by laminating two elliptic tubes 1a, 1b. One focal line 2b of focal lines 2a, 2b, 2b, 2c is made common. A flash lamp 3 of an excitation light source is located on the common focal line 2b and dye cells 4a, 4b of a laser oscillation element to generate a laser light of object wavelength are located on the other two focal lines 2a, 2c. The dye cells 4a, 4b are made by bonding a quartz window plate 9 at the both sides of a transparent quartz tube 8 and an inflow port 10 and an outflow port 11 of dye solution are provided therebetween to circulate the dye solution stored in a dye solution reservoir inside the transparent quartz tube 8 though a circulation pump.

Description

【発明の詳細な説明】 「産業上の利用分野」 本発明は1個の励起光源で複数個のレーザ発振素子を光
励起することのできるレーザ装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION "Field of Industrial Application" The present invention relates to a laser device that can optically excite a plurality of laser oscillation elements with one excitation light source.

「従来の技術」 まず色素レーザ装置の原理を簡単に説明する。"Conventional technology" First, the principle of the dye laser device will be briefly explained.

色素レーザ装置は、色素を溶媒によって所定の濃度に溶
解し、これによってできた溶液を容器に収容して得られ
た色素セルを用いる。この色素セルの両端延長線上に、
互いに反射面が対向するようにしてそれぞれ反射鏡を配
置する。そしてこの色素セルの側面から励起光源で発生
した励起光を照射して色素を発光させる。前記1対の反
射鏡間で多重反射によりレーザ発振を起こさせ、前記色
素の種類に対応した輝線スペクトルを反射鏡の一方より
レーザ光として取り出すものである。
A dye laser device uses a dye cell obtained by dissolving a dye to a predetermined concentration using a solvent and storing the resulting solution in a container. On the extension line of both ends of this dye cell,
The reflecting mirrors are arranged so that their reflecting surfaces face each other. Then, excitation light generated by an excitation light source is irradiated from the side of the dye cell to cause the dye to emit light. Laser oscillation is caused by multiple reflection between the pair of reflecting mirrors, and a bright line spectrum corresponding to the type of dye is extracted as laser light from one of the reflecting mirrors.

従来、クセノンランプ系のフラッシュランプで励起され
て発振する色素レーザ装置として第6図および第7図に
示すような構造のものが知られている。ここで(1)は
内面が反射鏡の楕円筒からなるレーザヘッドで、このレ
ーザヘッド(1)の2つの焦線(2a)(2b)上にそ
れぞれフラッシュランプ(3)と色素セル(4)が配置
されている。前記レーザヘッド(1)が楕円筒反射鏡か
らなるのは一方の焦線(2a)上の点から出た光は、他
方の焦線(2b)上の点に集まる性質があるからである
。具体的には第7図に示すように、一方の焦線(2a)
上に配置されたフラッシュランプ(3)の1点から出た
励起光が他方の焦線(2b)上に配置した色素セル(4
)に低損失で集光する。したがってレーザの発振効率向
上に役立つ。色素セル(4)はレーザヘッド(1)の外
部に用意された色素溶液溜め(リザーバ)と色素溶液循
環ポンプ(ともに図示せず)に接続されて、色素セル(
4)内部を色素溶液が流れるようになっている。
2. Description of the Related Art Conventionally, a dye laser device having a structure as shown in FIGS. 6 and 7 is known as a dye laser device that oscillates when excited by a flash lamp of a xenon lamp type. Here, (1) is a laser head consisting of an elliptical cylinder whose inner surface is a reflecting mirror, and a flash lamp (3) and a dye cell (4) are placed on the two focal lines (2a) and (2b) of this laser head (1), respectively. is located. The reason why the laser head (1) is composed of an elliptical cylindrical reflecting mirror is that light emitted from a point on one focal line (2a) has a property of converging at a point on the other focal line (2b). Specifically, as shown in Figure 7, one focal line (2a)
The excitation light emitted from one point of the flash lamp (3) placed above excites the dye cell (4) placed on the focal line (2b) of the other side.
) with low loss. Therefore, it is useful for improving laser oscillation efficiency. The dye cell (4) is connected to a dye solution reservoir and a dye solution circulation pump (both not shown) prepared outside the laser head (1).
4) A dye solution is allowed to flow inside.

レーザ光はフラッシュランプ(3)で励起されて色素セ
ル(4)の色素が発する蛍光が色素セル(4)の両端外
部に配置した2つの反射鏡(5) (6)間を多重反射
する間に増幅されて、その一部が反射鏡(6)を透過し
て外部にレーザ光(7)として放出される。
The laser beam is excited by a flash lamp (3), and the fluorescence emitted by the dye in the dye cell (4) undergoes multiple reflections between two reflecting mirrors (5) and (6) placed outside both ends of the dye cell (4). A part of the amplified light passes through a reflecting mirror (6) and is emitted to the outside as a laser beam (7).

また、第8図に示すように、レーザヘッド(1)が2つ
の楕円筒(la) (lb)の一方の焦線(2b)を重
ねて2重楕円筒としたものがあり、この例では共通焦線
上(2b)に色素セル(4)を設置し、他方の2つの焦
線(2a) (2c)上にそれぞれフラッシュランプ(
3a) (3b)を設置したものであるにのようにする
ことによりランプ1本当りの注入エネルギーを半分にし
てランプ寿命を大巾に延ばすことができる。
In addition, as shown in Fig. 8, there is a laser head (1) that has two elliptical cylinders (la) and (lb) with one focal line (2b) overlapping to form a double elliptical cylinder. A dye cell (4) is installed on the common focal line (2b), and a flash lamp (2) is placed on the other two focal lines (2a) (2c).
3a) By installing (3b) as shown below, the energy injected into each lamp can be halved and the lamp life can be greatly extended.

「発明が解決しようとする課題」 しかるに、以上のようなレーザ装置ではいずれの場合も
1色素セル(4)がら放出されるのは1つのレーザ光だ
けである。
``Problems to be Solved by the Invention'' However, in any of the above laser devices, only one laser beam is emitted from one dye cell (4).

ところで、1つの装置で波長の異なる2つのレーザ光を
必要とする場合がある。例えば、水出原人等が既に提案
したレーザパルスを用いた癌の診断装置(特公昭63−
9464号公報参照)では、癌病巣の発見に利用される
405nmと、癌病巣の治療に利用される630nmの
レーザ光パルスが用いられる。
By the way, one device may require two laser beams with different wavelengths. For example, a cancer diagnostic device using laser pulses already proposed by Mizuide et al.
9464) uses 405 nm laser light pulses, which are used to discover cancer foci, and 630 nm laser light pulses, which are used to treat cancer foci.

さらに詳しくは、癌組織と親和性の大きい光感受性物質
であるHematoporphyrin Deriva
tive(HpD)を体内に投与し、その後に405n
mレーザ光を癌病巣に照射すると、癌組織部から発生す
る)IpD特有の赤色蛍光を発生する。これを検出する
ことにより癌病巣のある場所をみつける。つぎに、みつ
け出した癌病巣部に630nmレーザ光を照射して)l
pDを励起する。すると、)IPDは励起され、そのと
き得られたエネルギーを癌病巣部内の酸素に伝達して酸
素を活性化し、その結果この活性酸素により癌組織を壊
死させるものである。
More specifically, Hematoporphyrin Deriva, a photosensitizer with high affinity for cancer tissues.
tive (HpD) into the body, and then 405n
When a cancer focus is irradiated with m-laser light, red fluorescence, which is unique to IpD (generated from cancer tissue), is generated. By detecting this, the location of the cancer focus can be found. Next, 630nm laser light is irradiated to the cancerous lesion that has been found)
Excite pD. Then, the IPD is excited and transmits the energy obtained at that time to the oxygen in the cancer lesion to activate the oxygen, and as a result, the active oxygen causes necrosis of the cancer tissue.

このような405nmと630nmの異なる2つの波長
のレーザ光を必要とする場合、従来は、それぞれ405
nmと630nmの2台のレーザ装置が使用されるか、
405r++++と630nmを発振できる色素レーザ
装置とこれを励起するに必要な紫外線レーザの装置の2
式のレーザ装置が使用されていたため、高価格で、かつ
設置スペースも広く必要であるという問題があった。
Conventionally, when two different wavelengths of laser light, 405 nm and 630 nm, are required, 405 nm and 630 nm, respectively, are required.
Two laser devices are used: nm and 630 nm;
A dye laser device that can oscillate 405r++++ and 630nm, and an ultraviolet laser device necessary to excite it.
Since the type laser device was used, there were problems in that it was expensive and required a large installation space.

本発明は1台のレーザ装置で複数のレーザ光を放出でき
る装置を得ることを目的とするものである。
An object of the present invention is to obtain a device that can emit a plurality of laser beams using one laser device.

「課題を解決するための手段」 本発明は内面を励起光反射面とした複数個の楕円筒を、
それぞれの1つの焦線が共通となるように重合して多重
楕円筒を形成し、この多重楕円筒からなるレーザヘッド
の前記共通焦線上に励起光源を配置し、他の複数個の焦
線上にそれぞれレーザ発振素子を配置してなるものであ
る。
"Means for Solving the Problems" The present invention provides a plurality of elliptical cylinders whose inner surfaces are excitation light reflecting surfaces.
A laser head composed of multiple elliptical cylinders is superimposed so that one focal line of each is common, and an excitation light source is placed on the common focal line, and the excitation light source is placed on the other plural focal lines. Each laser oscillation element is arranged.

「作用」 フラッシュランプなどの励起光源で発生した励起光は色
素セルからなる複数個のレーザ発振素子のそれぞれの目
的の波長のレーザ光を発生する色素を励起して、これら
から必要なレーザ光を発生させる。レーザヘッドは内面
が励起光反射鏡とした多重楕円筒であるから、励起光源
からの励起光を効率よくレーザ発振素子に照射する。
"Operation" The excitation light generated by an excitation light source such as a flash lamp excites the pigments that generate laser light of the desired wavelength in each of the multiple laser oscillation elements consisting of dye cells, and the necessary laser light is extracted from these. generate. Since the laser head is a multiple elliptical cylinder whose inner surface serves as an excitation light reflecting mirror, excitation light from the excitation light source is efficiently irradiated onto the laser oscillation element.

「実施例」 以下1本発明の実施例を図面に基づき説明する。"Example" An embodiment of the present invention will be described below based on the drawings.

第1図において、(1)はレーザヘッドである。In FIG. 1, (1) is a laser head.

このレーザヘッド(1)は、内面を励起光反射鏡とした
4分割の湾曲板体を接合して2つの楕円筒(la) (
lb)を重合したような形状の多重楕円筒に形成され、
それぞれの焦線(2a) (2b)、(2b) (2c
)のうち、1つの焦線(2b)を共通としている。これ
ら2つの楕円筒(la) (lb)の離心率は同一でも
よいし、また異なるものでもよく、要するに1つの焦線
(2b)を共通とするものであればよい、このような多
重楕円筒のレーザヘッド(1)の共通焦線(2b)上に
は励起光源としてのフラッシュランプ(3)が配置され
、また他の2つの焦線(2a) (2c)上にはそれぞ
れ目的波長のレーザ光を発生するレーザ発振素子とじて
の色素セル(4a) (4b)が配置される。この色素
セル(4a)(4b)は、例えば第2図に示すように内
径4mm。
This laser head (1) is made up of two elliptical cylinders (la) (
It is formed into a multi-elliptic cylinder shaped like a polymerized lb),
Each focal line (2a) (2b), (2b) (2c
), one focal line (2b) is shared. The eccentricities of these two elliptical cylinders (la) (lb) may be the same or different, as long as they have one focal line (2b) in common. A flash lamp (3) as an excitation light source is placed on the common focal line (2b) of the laser head (1), and lasers of the target wavelength are placed on the other two focal lines (2a) and (2c), respectively. Dye cells (4a) (4b) as laser oscillation elements that generate light are arranged. The dye cells (4a) (4b) have an inner diameter of 4 mm, for example, as shown in FIG.

外径6mの透明石英管(8)の両端に石英窓板(9) 
(9)を接着し、途中には色素溶液の流入口(1o)と
流出口(11)を設け1図示しない色素溶液溜(リザー
バ)に貯められた色素溶液(色素を溶媒によって所定濃
度に溶解したもの)を図示しない循環ポンプで前記透明
石英管(8)内に循環させるものである。
Quartz window plates (9) at both ends of a transparent quartz tube (8) with an outer diameter of 6 m
(9), and an inlet (1o) and an outlet (11) for the dye solution are provided in the middle.1 Dye solution stored in a dye solution reservoir (not shown) (the dye is dissolved to a predetermined concentration with a solvent) ) is circulated through the transparent quartz tube (8) using a circulation pump (not shown).

以上第1図のような構成において、励起光源であるフラ
ッシュランプ(3)で発生した励起光は2つの色素セル
(4a) (4b)内の目的波長のレーザ光を発生する
色素を励起して、これらから必要なレーザ光を発生させ
る。レーザヘッド(1)を構成する2つの楕円筒(1a
) (lb)は内部が励起光反射鏡であり、色素セル(
4a)(4b)は焦線(2a)(2c)上に配置されて
いるので、フラッシュランプ(3)からの励起光を効率
良く色素セル(4a) (4b)に照射する。
In the configuration shown in Figure 1 above, the excitation light generated by the flash lamp (3), which is the excitation light source, excites the pigment that generates laser light of the target wavelength in the two pigment cells (4a) (4b). , generate the necessary laser light from these. Two elliptical cylinders (1a
) (lb) has an excitation light reflecting mirror inside, and the dye cell (lb) has an excitation light reflecting mirror inside.
4a) and (4b) are arranged on the focal line (2a) and (2c), so that the excitation light from the flash lamp (3) is efficiently irradiated onto the dye cells (4a) and (4b).

つぎに、第2図は本発明の具体的応用例を示すもので、
色素セル(4a) (4b)のそれぞれの両端に互、い
に反射面を対向させて反射鏡(5a) (6a)、(5
b) (6b)を配置する。また、出力光側にはそれぞ
れシャッタ(12a)(12b)、集光レンズ(13a
) (13b)を介して光ファイバ(14a) (14
b)に導びかれるように配置され、前記シャッタ(12
a) (12b)はシャッタ制御回路(15)で開閉が
制御される。
Next, FIG. 2 shows a specific application example of the present invention.
Reflective mirrors (5a) (6a), (5
b) Place (6b). In addition, on the output light side, there are shutters (12a) (12b) and a condensing lens (13a), respectively.
) (13b) via optical fiber (14a) (14
b), and the shutter (12
a) Opening and closing of (12b) is controlled by a shutter control circuit (15).

この第2図における装置を前述の癌の診断装置に用いた
場合の作用を説明する。
The operation when the apparatus shown in FIG. 2 is used in the above-mentioned cancer diagnostic apparatus will be explained.

一方の色素セル(4a)内には色素D P S (Di
phenyl 5tilben)のジオキサン飽和溶液
が流入されているものとすると、フラッシュランプ(3
)によって励起されたとき、DPS色素より得られる蛍
光が反射鏡(5a) (6a)間で多重反射する結果増
強されて波長がほぼ405nmのレーザ光(7a)とし
て外部に取出される。他方の色素セル(4b)内にはロ
ーダミン640のエチルアルコール溶液(濃度0.1m
M)が流入され、ローダミン640からの蛍光が反射鏡
(5b) (6b)間で多重反射して増強され、その結
果波長がほぼ630nmのレーザ光(7b)として外部
に取出される。
One dye cell (4a) contains a dye D P S (Di
Assuming that a dioxane saturated solution of phenyl 5tilben) is flowing in, a flash lamp (3
), the fluorescence obtained from the DPS dye is multi-reflected between the reflecting mirrors (5a) and (6a), thereby being intensified and extracted to the outside as a laser beam (7a) with a wavelength of approximately 405 nm. Inside the other dye cell (4b) was an ethyl alcohol solution of Rhodamine 640 (concentration 0.1 m).
M) flows in, and the fluorescence from Rhodamine 640 is multi-reflected and intensified between the reflecting mirrors (5b) (6b), and as a result, it is extracted to the outside as a laser beam (7b) with a wavelength of approximately 630 nm.

ここでシャッタ制御回路(15)からの制御信号により
シャッタ(12a)(12b)は開閉制御される。シャ
ッタ(12a) (12b)を通過したレーザ光(7a
) (7b)は集光レンズ(13a) (13b)によ
り集光されて、光ファイバ(14a) (14b)に入
射され、光ファイバ(14a) (14b)中を通過し
てレーザ光を必要とする目的対象物まで伝送する。シャ
ッタ(12a) (12b)を通過する2つのレーザ光
(7a) (7b)はシャッタ制御回路(15)の制御
信号により同時刻の開閉、交互の開閉など目的によって
開閉制御する。例えば、癌診断時にはまず一方のシャッ
タ(12a)を開き、他′方のシャッタ(12b)を閉
じて405nmのレーザ光パルスだけを送って癌病巣の
発見に利用し、つぎに、シャッタ(12a)を閉じ、シ
ャッタ(12b)を開いて630nmのレーザ光パルス
を送って癌病巣の治療に利用する。
Here, the shutters (12a) (12b) are controlled to open and close by control signals from the shutter control circuit (15). Laser light (7a) passed through shutter (12a) (12b)
) (7b) is condensed by condensing lenses (13a) (13b), enters the optical fibers (14a) (14b), and passes through the optical fibers (14a) (14b) to generate laser light. It is transmitted to the target object. The two laser beams (7a) (7b) passing through the shutters (12a) (12b) are controlled to open and close depending on the purpose, such as opening and closing at the same time, alternate opening and closing, etc., by control signals from the shutter control circuit (15). For example, when diagnosing cancer, one shutter (12a) is first opened, the other shutter (12b) is closed, and only a 405 nm laser light pulse is sent to discover cancer lesions, and then the shutter (12a) is opened. is closed, the shutter (12b) is opened, and a 630 nm laser light pulse is sent for use in treating cancer lesions.

つぎに、第3図は本発明によるレーザ装置の他の応用例
を示すものである。この例では色素セル(4a) (4
b)は、異なる波長のレーザ光を発生させるためのもの
ではなくて、同一波長レーザ光の発振用および増幅用に
使用される。例えば色素セル(4a)(4b)には波長
630nmレーザ光を発生させるために、ローダミン6
40色素のエチルアルコール溶液が0.11IIM濃度
で流入されているものとする。フラッシュランプ(3)
からの励起光は色素セル(4a) (4b)中の色素を
照射して励起する。一方の色素セル(4a)で発生した
ローダミン640の蛍光は反射鏡(5a)、凹レンズ(
16)、凸レンズ(17) 、回折格子(18)の組合
せの共振器中を往復する間に増強され、反射鏡(5a)
の外部にレーザ光(7a)として取出される。ここでフ
ラッシュランプ(3)と色素セル(4a)間のフィルタ
(19)はフラッシュランプ(3)からの励起光強度を
調整するためのもので、回折格子(18)が色素レーザ
光のエネルギーにより損傷しない程度にレーザ光強度を
低減するために使われる。また組合せレンズ(16) 
(17)は回折格子(18)への入射レーザビームサイ
ズを大きくして波長分解能を大きくし、かつ単位面積当
りのレーザエネルギー密度を小さくして回折格子(18
)を損傷から保護するためのビームエキスパンダである
Next, FIG. 3 shows another application example of the laser device according to the present invention. In this example, the dye cell (4a) (4
b) is not used to generate laser beams of different wavelengths, but is used for oscillation and amplification of laser beams of the same wavelength. For example, in the dye cells (4a) (4b), rhodamine 6
It is assumed that an ethyl alcohol solution of 40 dyes is flowing in at a concentration of 0.11 IIM. Flash lamp (3)
The excitation light from irradiates and excites the dyes in the dye cells (4a) and (4b). The fluorescence of rhodamine 640 generated in one dye cell (4a) is reflected by a reflecting mirror (5a) and a concave lens (
16), a combination of a convex lens (17) and a diffraction grating (18) is strengthened while reciprocating in the resonator, and a reflecting mirror (5a)
The laser light is extracted to the outside as a laser beam (7a). Here, the filter (19) between the flash lamp (3) and the dye cell (4a) is for adjusting the excitation light intensity from the flash lamp (3), and the diffraction grating (18) is It is used to reduce the intensity of laser light to an extent that does not cause damage. Also combination lens (16)
(17) increases the wavelength resolution by increasing the laser beam size incident on the diffraction grating (18), and decreases the laser energy density per unit area.
) is a beam expander to protect the beam from damage.

回折格子(18)の刻線に対して垂直な面内にレーザ光
を入射し、刻線に平行な回転軸の回りに回折格子(18
)を回転すると、この回転によって定められ回折光波長
がレーザ波長として定められる。すなわち回折格子(1
8)はレーザ波長を変化させるために使用する。なお、
回折格子(18)の代りに波長可変素子としてプリズム
を使用することも可能である。この場合にはプリズムを
通して分散された光が再度色素セル(4a)側に戻るた
めにプリズムの後に反射鏡が必要となる。
Laser light is incident in a plane perpendicular to the score lines of the diffraction grating (18), and the laser beam is rotated around the rotation axis parallel to the score lines of the diffraction grating (18).
), the diffracted light wavelength determined by this rotation is determined as the laser wavelength. That is, the diffraction grating (1
8) is used to change the laser wavelength. In addition,
It is also possible to use a prism as a wavelength variable element instead of the diffraction grating (18). In this case, a reflecting mirror is required after the prism so that the light dispersed through the prism returns to the dye cell (4a) side again.

前記反射fi(5a)から出力したレーザ光(7a)は
反射鏡(20) (21)で反射され、他方の色素セル
(4b)中に入射して増幅される。フラッシュランプ(
3)の照射により色素セル(4b)中の色素ローダミン
640は上準位に励起される。この時一方の色素セル(
4a)で発生したレーザ光(7a)が入射して誘導放出
を起こすので、結局他方の色素セル(4b)から得られ
るレーザ光(7b)は一方のレーザ光(7a)が増幅さ
れたものとなる。
The laser beam (7a) outputted from the reflection fi (5a) is reflected by the reflecting mirrors (20) and (21), enters the other dye cell (4b), and is amplified. Flash lamp (
The dye rhodamine 640 in the dye cell (4b) is excited to the upper level by the irradiation in step 3). At this time, one dye cell (
Since the laser light (7a) generated in cell 4a) enters and causes stimulated emission, the laser light (7b) obtained from the other dye cell (4b) is the amplified version of the laser light (7a) from the other dye cell. Become.

前記実施例においては2波長発振の装置を説明したが、
3波長、4波長、・・・のレーザ光を得ることができる
。例えば3波長を得る場合には第4図に示すように、3
つの楕円筒(la) (lb) (lc)を用意し、そ
れぞれの1つの焦線(2b)が共通となるように合体し
、共通となった焦線(2b)上にフラッシュランプ(3
)を、他の3つの焦線(2a) (2c) (2d)上
に色素セル(4a) (4b) (4c)を配置する。
In the above embodiment, a two-wavelength oscillation device was explained, but
Laser light with 3 wavelengths, 4 wavelengths, etc. can be obtained. For example, when obtaining 3 wavelengths, as shown in Figure 4, 3 wavelengths are obtained.
Prepare two elliptical cylinders (la), (lb), and (lc), combine them so that one focal line (2b) of each is common, and place a flash lamp (3) on the common focal line (2b).
), and the dye cells (4a) (4b) (4c) are placed on the other three focal lines (2a) (2c) (2d).

各色素セル(4a) (4b) (4c)内の色素はフ
ラッシュランプ(3)による照射で励起され、それぞれ
の色素によるレーザ光を発生させることができる。また
、4波長を得る場合には、第5図に示すように4つの楕
円筒(1a) (lb) (lc) (ld)を合体し
て、上記と同様のことを行えばよい。
The dyes in each dye cell (4a), (4b), and (4c) are excited by irradiation with the flash lamp (3), and each dye can generate laser light. Further, in order to obtain four wavelengths, the same thing as above may be performed by combining four elliptical cylinders (1a) (lb) (lc) (ld) as shown in FIG.

前記実施例によるレーザ装置は、色素レーザについて記
載したが1本発明の趣旨、本質は色素レーザに限定され
るものではなく1色素セルの代わりに固体レーザ発振素
子を配置すれば、そのまま固体レーザ装置として使用で
きる。例えば第1図および第2図において、2つの色素
セル(4a) (4b)の代わりに、ルビー結晶、Nd
:YAG結晶のレーザ発振素子を配置すればそれぞれか
ら0.694μm、 1.06μへのレーザ光が同時に
得られる。この場合、レーザ共振器を構成する結晶に対
向する反射鏡はそれぞれのレーザ光に対して高反射率を
有することが必要となる。
Although the laser device according to the above embodiment has been described with respect to a dye laser, the purpose and essence of the present invention is not limited to a dye laser.If a solid-state laser oscillation element is placed in place of a dye cell, the laser device can be used as a solid-state laser device. Can be used as For example, in Figures 1 and 2, instead of the two dye cells (4a) (4b), ruby crystals, Nd
:If YAG crystal laser oscillation elements are arranged, laser beams of 0.694 μm and 1.06 μm can be obtained from each at the same time. In this case, the reflecting mirror facing the crystal forming the laser resonator needs to have a high reflectance for each laser beam.

「発明の効果」 本発明は上述のように構成したので、従来例えば405
nmと630nmのレーザ光を必要とする場合、2台の
レーザ装置が使われていたので高価格であり。
"Effects of the Invention" Since the present invention is configured as described above, conventionally, for example, 405
When laser beams of nm and 630 nm were required, two laser devices were used, resulting in high costs.

また広い設置スペースが必要であったのに対し。Also, a large installation space was required.

本発明によりこの問題は解消され、安価で、設置スペー
スも少なくて済み、実用上の効果甚大である。
The present invention solves this problem, is inexpensive, requires less installation space, and has great practical effects.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明によるレーザ装置の説明図、第2図は本
発明のレーザ装置を応用した装置の説明図、第3図は本
発明の他の応用装置の説明図、第4図および第5図は本
発明の他の実施例の説明図、第6図は従来の色素レーザ
装置の断面図、第7図は第6図を側面からみた説明図、
・第8図は従来の他の例の説明図である。 (1)・・・レーザヘッド、(la) (lb) (l
c) (ld)−楕円筒、(2a) (2b) (2c
) (2d) (2e) ”’焦線、 (3)−・・フ
ラッシュランプ(励起光源)、(4) (4a) (4
b) (4c) (4d)−色素セル(レーザ発振素子
)、(5) (5a) (5b) (6) (6a) 
(6b)・・・反射鏡、(7) (7a) (7b)・
・・レーザ光、(8)・・・透明石英管、(9)・・・
石英窓板、(10)・・・流入口、(11)・・・流出
口、 (12a)(12b)−シャッタ、(13a) 
(13b) ・=集光レンズ、(14a) (14b)
・・・光ファイバ、(15)・・・シャッタ制御回路、
(16)・・・凹レンズ、(17)・・・凸レンズ。 (18)・・・回折格子、(19)・・・フィルタ。 出願人  浜松ホトニクス株式会社 第 図 第 図
FIG. 1 is an explanatory diagram of a laser device according to the present invention, FIG. 2 is an explanatory diagram of a device to which the laser device of the present invention is applied, FIG. 3 is an explanatory diagram of another applied device of the present invention, and FIGS. 5 is an explanatory diagram of another embodiment of the present invention, FIG. 6 is a sectional view of a conventional dye laser device, and FIG. 7 is an explanatory diagram of FIG. 6 viewed from the side.
- FIG. 8 is an explanatory diagram of another conventional example. (1)... Laser head, (la) (lb) (l
c) (ld) - Elliptical cylinder, (2a) (2b) (2c
) (2d) (2e) ”'Focal line, (3)--Flash lamp (excitation light source), (4) (4a) (4
b) (4c) (4d) - Dye cell (laser oscillation element), (5) (5a) (5b) (6) (6a)
(6b)...Reflector, (7) (7a) (7b)
...Laser light, (8)...Transparent quartz tube, (9)...
Quartz window plate, (10)...Inlet, (11)...Outlet, (12a) (12b)-Shutter, (13a)
(13b) ・=Condensing lens, (14a) (14b)
...Optical fiber, (15)...Shutter control circuit,
(16)...Concave lens, (17)...Convex lens. (18)...diffraction grating, (19)...filter. Applicant: Hamamatsu Photonics Co., Ltd.

Claims (5)

【特許請求の範囲】[Claims] (1)内面を励起光反射面とした複数個の楕円筒を、そ
れぞれの1つの焦線が共通となるように重合して多重楕
円筒を形成し、この多重楕円筒からなるレーザヘッドの
前記共通焦線上に励起光源を配置し、他の複数個の焦線
上にそれぞれレーザ発振素子を配置してなることを特徴
とするレーザ装置。
(1) A plurality of elliptical cylinders each having an inner surface as an excitation light reflecting surface are superimposed so that each has a common focal line to form a multiple elliptical cylinder, and the laser head made of the multiple elliptical cylinders is A laser device characterized in that an excitation light source is disposed on a common focal line, and laser oscillation elements are disposed on each of a plurality of other focal lines.
(2)レーザ発振素子は内部に適量濃度の色素溶液を流
入する色素セルである請求項(1)記載のレーザ装置。
(2) The laser device according to claim (1), wherein the laser oscillation element is a dye cell into which a dye solution of an appropriate concentration flows.
(3)一方の色素セルは波長405nmのレーザ光を発
生することのできる色素溶液を有し、他方の色素セルは
波長630nmのレーザ光を発生することのできる色素
溶液を有するものからなる請求項(2)記載のレーザ装
置。
(3) A claim in which one dye cell has a dye solution capable of generating a laser beam with a wavelength of 405 nm, and the other dye cell has a dye solution capable of generating a laser beam with a wavelength of 630 nm. (2) Laser device described.
(4)レーザ発振素子はルビー、Nd:YAG等のレー
ザ光を発生させる固体レーザ発振素子である請求項(1
)記載のレーザ装置。
(4) Claim (1) wherein the laser oscillation element is a solid state laser oscillation element that generates laser light such as ruby or Nd:YAG.
) Laser device described.
(5)一方のレーザ発振素子の共振器として、レーザビ
ーム拡大光学系、分散素子、反射鏡の組合せを具備し、
励起光源から発した励起光の光量を調節するためのフィ
ルタを一方のレーザ発振素子と励起光源の間に配置し、
かつ一方のレーザ発振素子から発生したレーザ光を他方
のレーザ発振素子中に導く反射光学系を有する請求項(
1)記載のレーザ装置。
(5) As a resonator of one laser oscillation element, a combination of a laser beam expansion optical system, a dispersion element, and a reflecting mirror is provided,
A filter for adjusting the amount of excitation light emitted from the excitation light source is placed between one laser oscillation element and the excitation light source,
and a reflective optical system that guides the laser beam generated from one laser oscillation element into the other laser oscillation element (
1) The laser device described above.
JP14603088A 1988-06-14 1988-06-14 Laser device Pending JPH022190A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14603088A JPH022190A (en) 1988-06-14 1988-06-14 Laser device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14603088A JPH022190A (en) 1988-06-14 1988-06-14 Laser device

Publications (1)

Publication Number Publication Date
JPH022190A true JPH022190A (en) 1990-01-08

Family

ID=15398517

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14603088A Pending JPH022190A (en) 1988-06-14 1988-06-14 Laser device

Country Status (1)

Country Link
JP (1) JPH022190A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1992015135A1 (en) * 1991-02-23 1992-09-03 Aesculap Ag Laser
US5828690A (en) * 1995-12-18 1998-10-27 General Electric Company Unitary body laser head
WO2007093715A1 (en) * 2006-02-17 2007-08-23 Ecole Polytechnique Device for amplifying light pulses with flash lamp-pumped solid-state matrix

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5989480A (en) * 1982-11-15 1984-05-23 Toshiba Corp Bi-output solid-state laser device
JPS60189277A (en) * 1984-03-09 1985-09-26 Hoya Corp Oscillatation for erbium laser and device thereof
JPS60239078A (en) * 1984-05-11 1985-11-27 Toshiba Corp Solid-state laser oscillator
JPS61168987A (en) * 1985-01-22 1986-07-30 Hamamatsu Photonics Kk Dye laser device

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5989480A (en) * 1982-11-15 1984-05-23 Toshiba Corp Bi-output solid-state laser device
JPS60189277A (en) * 1984-03-09 1985-09-26 Hoya Corp Oscillatation for erbium laser and device thereof
JPS60239078A (en) * 1984-05-11 1985-11-27 Toshiba Corp Solid-state laser oscillator
JPS61168987A (en) * 1985-01-22 1986-07-30 Hamamatsu Photonics Kk Dye laser device

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1992015135A1 (en) * 1991-02-23 1992-09-03 Aesculap Ag Laser
US5828690A (en) * 1995-12-18 1998-10-27 General Electric Company Unitary body laser head
WO2007093715A1 (en) * 2006-02-17 2007-08-23 Ecole Polytechnique Device for amplifying light pulses with flash lamp-pumped solid-state matrix
FR2897725A1 (en) * 2006-02-17 2007-08-24 Ecole Polytechnique Etablissem LUMINOUS PULSE AMPLIFIER DEVICE WITH SOLID MATRIX PUMPED BY FLASHLIGHTS

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