JP2591003B2 - Pulse multiplex optical system - Google Patents
Pulse multiplex optical systemInfo
- Publication number
- JP2591003B2 JP2591003B2 JP414288A JP414288A JP2591003B2 JP 2591003 B2 JP2591003 B2 JP 2591003B2 JP 414288 A JP414288 A JP 414288A JP 414288 A JP414288 A JP 414288A JP 2591003 B2 JP2591003 B2 JP 2591003B2
- Authority
- JP
- Japan
- Prior art keywords
- polarizing plate
- pulse
- optical
- light
- output
- 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 - Lifetime
Links
- 230000003287 optical effect Effects 0.000 title claims description 51
- 230000010287 polarization Effects 0.000 claims description 10
- 239000011159 matrix material Substances 0.000 claims 1
- 230000001360 synchronised effect Effects 0.000 claims 1
- 238000010586 diagram Methods 0.000 description 6
- 230000000694 effects Effects 0.000 description 4
- 238000006243 chemical reaction Methods 0.000 description 3
- 229910001385 heavy metal Inorganic materials 0.000 description 2
- 238000005372 isotope separation Methods 0.000 description 2
- 125000004122 cyclic group Chemical group 0.000 description 1
- 230000001934 delay Effects 0.000 description 1
- 230000003111 delayed effect Effects 0.000 description 1
- 238000000034 method Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/26—Optical coupling means
- G02B6/28—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals
- G02B6/2804—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals forming multipart couplers without wavelength selective elements, e.g. "T" couplers, star couplers
- G02B6/2861—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals forming multipart couplers without wavelength selective elements, e.g. "T" couplers, star couplers using fibre optic delay lines and optical elements associated with them, e.g. for use in signal processing, e.g. filtering
-
- 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
- H01S3/005—Optical devices external to the laser cavity, specially adapted for lasers, e.g. for homogenisation of the beam or for manipulating laser pulses, e.g. pulse shaping
- H01S3/0057—Temporal shaping, e.g. pulse compression, frequency chirping
Landscapes
- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Optics & Photonics (AREA)
- Electromagnetism (AREA)
- Signal Processing (AREA)
- Theoretical Computer Science (AREA)
- General Physics & Mathematics (AREA)
- Plasma & Fusion (AREA)
Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明はパルス多重光学系に関し、特にレーザ装置等
が周期的に出力した光パルスをより高い繰返し周波数の
光パルスに変換するパルス多重光学系に関する。Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a pulse multiplexing optical system, and more particularly to a pulse multiplexing optical system that converts a light pulse periodically output by a laser device or the like into a light pulse having a higher repetition frequency. About.
レーザ法重金属同位体分離を行う際、高出力レーザ装
置で発生した光パルスで重金属蒸気を照射する必要があ
る。同位体分離を効率よく行うためには光パルスの繰返
し周波数を数MHz程度にする必要があるが,かかる用途
の高出力レーザ装置の光パルスの繰返し周波数は数kHz
程度である。そのため、高出力レーザ装置で発生した光
パルスを3桁程度高い繰返し周波数の光パルスに変換す
る必要がある。When performing heavy metal isotope separation by the laser method, it is necessary to irradiate heavy metal vapor with light pulses generated by a high-power laser device. In order to perform isotope separation efficiently, the repetition frequency of light pulses must be about several MHz, but the repetition frequency of light pulses in high-power laser equipment for such applications is several kHz.
It is about. Therefore, it is necessary to convert an optical pulse generated by the high-power laser device into an optical pulse having a repetition frequency higher by about three digits.
第3図はかかる光パルスの変換に用いられている従来
のパルス多重光学系の一例の動作原理を説明するための
光路図、第4図は同じくタイミング図である。第3図に
おいて、左右方向の光路は上下方向の光路に比較し拡大
して図示してある。FIG. 3 is an optical path diagram for explaining an operation principle of an example of a conventional pulse multiplexing optical system used for the conversion of the optical pulse, and FIG. 4 is a timing diagram of the same. In FIG. 3, the light path in the left-right direction is shown in an enlarged manner as compared with the light path in the up-down direction.
第3図において、各ハーフミラー間の直接の光路にお
ける伝搬時間は無視できるほど小さいものとする。繰返
し周期T0でハーフミラー11に入射した光パルスは2等分
され、一方は直接ハーフミラー14に入射し、他方は反射
鏡12,13で反射してからハーフミラー14に入射する。ハ
ーフミラー11から反射鏡12,13を介してハーフミラー14
までの光路の伝搬時間がT0/2になるように反射鏡12,13
を配置すると,ハーフミラー14には、左から右に入射す
る光パルスに時間T0/2遅れて上から下に光パルス2が入
射する。これら二つの光パルスはそれぞれハーフミラー
14で2等分される。したがって、第4図に図示するよう
に、ハーフミラー14から出力する光パルスはハーフミラ
ー11から出力する光パルスに対し、繰返し周波数が2倍
になり、ピークパワーが1/2になる。In FIG. 3, it is assumed that the propagation time in the direct optical path between the half mirrors is negligibly small. The light pulse incident on the half mirror 11 at the repetition period T 0 is divided into two equal parts, one of which is directly incident on the half mirror 14, and the other is reflected on the reflecting mirrors 12 and 13 before being incident on the half mirror 14. Half mirror 14 from half mirror 11 via reflecting mirrors 12 and 13
Reflectors 12 and 13 as the propagation time of the optical path becomes T 0/2 to
Is arranged, the light pulse 2 is incident on the half mirror 14 from the top to the bottom with a time T 0/2 delayed from the light pulse incident from the left to the right. Each of these two light pulses is a half mirror
Divide by 14 into two. Therefore, as shown in FIG. 4, the repetition frequency of the light pulse output from the half mirror 14 is twice that of the light pulse output from the half mirror 11, and the peak power is halved.
ハーフミラー14から反射鏡15,16を介してハーフミラ
ー17までの光路の伝搬時間をハーフミラー14から出力す
る光パルスの繰返し周期T0/2の1/2、すなわちT0/4にす
れば、上記と同様にして、ハーフミラー17から出力する
光パルスの繰返し周波数およびピークパワーは、ハーフ
ミラー14から出力する光パルスに対し2倍および1/2、
ハーフミラー11から出力する光パルスに対し4倍および
1/4になる。1/2 of the repetition period T 0/2 of the light pulse to output the propagation time of the optical path from the half mirror 14 from the half mirror 14 to the half mirror 17 via the reflecting mirror 15 and 16, i.e. when the T 0/4 In the same manner as described above, the repetition frequency and the peak power of the optical pulse output from the half mirror 17 are twice and 1/2 that of the optical pulse output from the half mirror 14,
4 times the light pulse output from the half mirror 11 and
It becomes 1/4.
ハーフミラー11からハーフミラー14まで、ハーフミラ
ー14からのハーフミラー17まで、ハーフミラー17からハ
ーフミラー20まで……をそれぞれ1段とし、これら各段
における2枚の反射鏡を介する光路の伝搬時間を順次T0
/2,T0/22,T0/23……とすれば、m段目の最後のハー
フミラーから出力する光パルスの繰返し周波数はハーフ
ミラー11に入射した光パルスの繰返し周波数の2m倍にな
る。Each of the half mirror 11 to the half mirror 14, the half mirror 14 to the half mirror 17, the half mirror 17 to the half mirror 20,... Has one stage, and the propagation time of the optical path through two reflecting mirrors at each stage. To T 0
/ 2, T 0/2 2 , T 0/2 3 if ..., 2 of the repetition frequency of the optical pulse repetition frequency of the optical pulses incident on the half mirror 11 to be output from the last half mirror m-th stage m times.
上記のようにして、例えば、繰返し周波数5kHzの光パ
ルスを繰返し周波数約5MHzの光パルスに変換するには、
上記の段数が10段(210=1024)になり、ハーフミラー1
1から反射鏡12,13を介しハーフミラー14までの光路長が
15kmになり、必要なハーフミラーおよび反射鏡の枚数は
それぞれ11枚,20枚になる。As described above, for example, to convert an optical pulse having a repetition frequency of 5 kHz to an optical pulse having a repetition frequency of about 5 MHz,
The above number of stages becomes 10 stages (2 10 = 1024), half mirror 1
The optical path length from 1 to the half mirror 14 via the reflecting mirrors 12 and 13 is
15 km, the number of required half mirrors and reflectors will be 11 and 20, respectively.
上述した従来のパルス多重光学系は、光パルスの繰返
し周波数の変化比を大きくするには多数のハーフミラー
と反射鏡とを必要とするので機械的構造が複雑になる欠
点があり、また、最初のハーフミラーから2枚の反射鏡
を介し次のハーフミラーまでの光路長が入力する光パル
スの低い繰返し周波数できまり長いのできわめて大型に
なる欠点がある。The conventional pulse multiplexing optical system described above has a disadvantage that the mechanical structure is complicated because a large number of half mirrors and reflecting mirrors are required to increase the change ratio of the repetition frequency of the light pulse. The optical path length from one half mirror to the next half mirror via two reflecting mirrors is extremely large because the input light pulse has a low repetition frequency and a long repetition frequency.
本発明の目的は、構造が簡単かつ小型であり、しかも
繰返し周波数の変換比を大きくできるパルス多重光学系
を提供することにある。SUMMARY OF THE INVENTION An object of the present invention is to provide a pulse multiplexing optical system having a simple structure and a small size and capable of increasing a repetition frequency conversion ratio.
本発明のパルス多重光学系は、所定の繰り返し周期を
持つ入力パルス光を受ける第1の偏光板と、第1の偏光
板を透過したパルス光を受け入力される光の偏光方向を
制御電圧に応じて変えるシリーズに配列された第1及び
第2の電気光学素子と、第2の電気光学素子の出力のう
ち第1の偏光成分を反射し第2の偏光成分を透過しこの
第1及び第2の偏光成分のうち一方の偏光成分を外部出
力として出力する第2の偏光板と、第2の偏光板の出力
のうち外部出力として出力されない他方の偏光成分を受
け入力パルス光の繰り返し周期の整数分の1の時間だけ
遅延させ第1の偏光板へ帰還させる光遅延素子とを具備
し、入力パルス光を第2の偏光板を経て光遅延素子へ導
くように入力パルス光のタイミングに同期した制御電圧
で第1の電気光学素子を制御するとともに、第2の偏光
板を経て外部出力として出力される偏光成分を発生させ
るために入力パルス光の周期間で漸次変化してゆく制御
電圧で第2の電気光学素子を制御することを特徴とす
る。The pulse multiplexing optical system according to the present invention includes a first polarizing plate that receives input pulse light having a predetermined repetition period, and a polarization direction of light that is input after receiving pulse light transmitted through the first polarizing plate. The first and second electro-optical elements are arranged in a series that changes accordingly, and the first and second electro-optical elements output the first polarized light component while reflecting the first polarized light component and transmitting the second polarized light component. A second polarizing plate that outputs one of the two polarized components as an external output, and a second polarizing plate that outputs the other polarized component of the output of the second polarizing plate that is not output as an external output, and receives a second one of the repetition periods of the input pulse light. An optical delay element that delays by an integral time and feeds back to the first polarizing plate, and synchronizes with the timing of the input pulse light so as to guide the input pulse light to the optical delay element through the second polarizing plate. The first electro-optical element with the applied control voltage And controlling the second electro-optical element with a control voltage that changes gradually during the period of the input pulsed light in order to generate a polarization component output as an external output through the second polarizing plate. It is characterized by.
次に、本発明について図面を参照して説明する。 Next, the present invention will be described with reference to the drawings.
第1図は本発明の一実施例を示すブロック図である。 FIG. 1 is a block diagram showing one embodiment of the present invention.
第1図に示す実施例は、ポッケルスセル(Pockels ce
ll)1,2と、偏光板3と、光遅延セル4と、偏光板5
と、平面鏡61,62と、制御信号CS1,CS2をポッケルスセル
1,2へ出力する制御信号発生器7とを備えて構成されて
いる。これら各構成要素の相互配置については後述す
る。The embodiment shown in FIG. 1 is a Pockels cell.
ll) 1, 2, polarizing plate 3, optical delay cell 4, polarizing plate 5
And the plane mirrors 61 and 62 and the control signals CS1 and CS2 in the Pockels cell
And a control signal generator 7 for outputting to the control signals 1 and 2. The mutual arrangement of these components will be described later.
第2図は、第1図に示す実施例の動作を説明するため
の波形図である。FIG. 2 is a waveform chart for explaining the operation of the embodiment shown in FIG.
高出力レーザ装置(図示せず)からの繰返し周期T2の
直接偏波の光パルスL1を、その信号方向に斜めに、P成
分として入力し通過させポッケルス1へ出力するように
偏光板5を配置する。A polarizing plate 5 is disposed so that a directly polarized light pulse L1 having a repetition period T2 from a high-power laser device (not shown) is input as a P component obliquely in the signal direction, passed therethrough, and output to the Pockels 1. I do.
周知のようにポッケルスセルは、制御電圧を印加しな
ければ特定の偏光方向で入力した直線偏光をそのまま出
力し、制御電圧を印加すると入力した直線偏光の偏光方
向の成分(以下平行成分という)のほか直交する偏光方
向の成分(以下直交成分という)も出力する。平行成分
に対する直交成分のパワー比は印加電圧と共に増大し、
ある電圧値で無限大になり直交成分のみを出力するよう
になる。As is well known, the Pockels cell outputs linearly polarized light input in a specific polarization direction as it is unless a control voltage is applied, and applies a polarization direction component (hereinafter referred to as a parallel component) of the input linearly polarized light when a control voltage is applied. In addition, a component in the orthogonal polarization direction (hereinafter referred to as an orthogonal component) is also output. The power ratio of the orthogonal component to the parallel component increases with the applied voltage,
The voltage becomes infinite at a certain voltage value, and only the orthogonal component is output.
ポッケルスセル1,2に制御信号CS1,CS2を入力しないと
き、偏光板5を通過した光パルスL1が、ポッケルスセル
1を通過し、更にポッケルスセル2を通過し、偏光板3
に斜めに、P成分として入射するようにポッケルスセル
1,2ならびに偏光板3を配置する。When the control signals CS1 and CS2 are not input to the Pockels cells 1 and 2, the light pulse L1 that has passed through the polarizing plate 5 passes through the Pockels cell 1 and further passes through the Pockels cell 2 and
Pockels cell obliquely incident as a P component
1, 2 and the polarizing plate 3 are arranged.
偏光板5を通過した光パルスL1がポッケルスセル1に
到達するタイミングで、ポッケルスセル1が直交成分の
み出力する電圧値のパルス状の制御信号CS1を制御信号
発生器7に発生させる。その結果、ポッケルスセル1か
ら出力する光パルスL1は偏光板3にとってS成分のみに
なる。At the timing when the light pulse L1 that has passed through the polarizing plate 5 reaches the Pockels cell 1, the control signal generator 7 generates a pulse-like control signal CS1 having a voltage value such that the Pockels cell 1 outputs only the orthogonal component. As a result, the light pulse L1 output from the Pockels cell 1 becomes only the S component for the polarizing plate 3.
制御信号発生器7から第2図で図示する波形の繰返し
周期T2の制御信号CS2を発生させる。その結果、ポッケ
ルスセル2から出力する光パルスL1は偏光板3にとって
のP成分とS成分とを含むようになり、P成分は偏光板
3を通気し光パルスL2として外部へ取出され、一方、S
成分は偏光板3で反射され、平面鏡61で反射されて光遅
延セル4に入力し、光遅延セル4から出力し反射鏡62で
反射されて偏光板5に入射する。The control signal generator 7 generates a control signal CS2 having a repetition period T2 of the waveform shown in FIG. As a result, the light pulse L1 output from the Pockels cell 2 contains the P component and the S component for the polarizing plate 3, and the P component is passed through the polarizing plate 3 and extracted outside as a light pulse L2. S
The components are reflected by the polarizing plate 3, reflected by the plane mirror 61, input to the optical delay cell 4, output from the optical delay cell 4, reflected by the reflecting mirror 62, and incident on the polarizing plate 5.
平面鏡62で反射された光パルスが偏光板5にS成分と
して入射しポッケルスセル1へ反射されるように平面鏡
61,62ならびに光遅延セル4を配置する。また、光パル
スL2の所要の繰返し周期をT1(T2/T1は整数nである)
とすると、偏光板5から出力しポッケルスセル1,ポッケ
ルスセル2,偏光板3,平面鏡61,光遅延セル4,平面鏡62を
介し再び偏光板5に戻る光路(以下巡回光路という)に
おける伝搬時間がT1になるように光遅延セル4の遅延時
間を設定する。The light pulse reflected by the plane mirror 62 enters the polarizing plate 5 as an S component and is reflected by the Pockels cell 1 by a plane mirror.
61, 62 and the optical delay cell 4 are arranged. Further, a required repetition period of the light pulse L2 is T1 (T2 / T1 is an integer n).
Then, the propagation time in an optical path (hereinafter referred to as a cyclic optical path) output from the polarizing plate 5 and returned to the polarizing plate 5 again via the Pockels cell 1, the Pockels cell 2, the polarizing plate 3, the plane mirror 61, the optical delay cell 4, and the plane mirror 62 is shown. The delay time of the optical delay cell 4 is set so as to be T1.
上記の各配置,各設定の結果、光パルスL1の一つのパ
ルスがポッケルスセル1,2を通り、その一部が偏光板3
で反射され、反射された成分は巡回光路の一部を通って
全てポッケルスセル1に戻る。このときポッケルスセル
1には制御信号CS1が印加されていないのでポッケルス
セル2に入力する光パルスは偏光板3にとってS成分の
みであり、ポッケルスセル2でその一部が直交成分にな
り偏光板3を通過して光パルスL2になり、残りの平行成
分は再び偏光板3で反射される。以下同様のことを繰返
し、制御信号CS2の波形を第2図に図示するように設定
することにより、光パルスL1の一つのパルスを光パルス
L2のn個のパルスに、各パルスのピークパワーを等し
く、しかも、各構成要素の損失分以外に損失なく変換で
きる。As a result of the above arrangements and settings, one pulse of the light pulse L1 passes through the Pockels cells 1 and 2 and a part thereof
And all the reflected components return to the Pockels cell 1 through a part of the traveling optical path. At this time, since the control signal CS1 is not applied to the Pockels cell 1, the light pulse input to the Pockels cell 2 has only the S component for the polarizing plate 3, and a part of the light pulse becomes an orthogonal component in the Pockels cell 2, and the polarizing plate 3 , And becomes a light pulse L2, and the remaining parallel components are reflected by the polarizing plate 3 again. The same is repeated thereafter, and one pulse of the light pulse L1 is changed to the light pulse by setting the waveform of the control signal CS2 as shown in FIG.
The peak power of each pulse can be converted to n pulses of L2 equal to each other, and the pulse can be converted without loss except for the loss of each component.
光パルスL1の各パルスが入力するごとに制御信号CS1
のパルスを発生させるので、制御信号CS1の繰返し周期
もT2になる。Each time the light pulse L1 is input, the control signal CS1
, The repetition period of the control signal CS1 also becomes T2.
以上説明したように本発明は、光パルスの繰返し周波
数の変化比に関係しない小数の構成要素でパルス多重光
学系を構成しており、必要とする光遅延素子の光路長が
出力する光パルスの高い繰返し周波数できまり短いの
で、パルス多重光学系の構造を簡単かつ小型にできる効
果があり、また、ただ一つの光遅延素子の光路長の変更
のみで出力する光パルスの繰返し周期を変更でき、第1
および第2の制御電圧の繰返し周期の変更のみで入力す
る光パルスの繰返し周期の変更に対応できる効果があ
り、更に、光パルスの繰返し周波数の変換比を2mのみで
なく任意の整数に設定できる効果がある。As described above, in the present invention, the pulse multiplexing optical system is configured with a small number of components that are not related to the change ratio of the repetition frequency of the optical pulse, and the optical path length of the required optical delay element is used to output the optical pulse. Since the high repetition frequency is relatively short, there is an effect that the structure of the pulse multiplexing optical system can be made simple and small, and the repetition period of the output optical pulse can be changed only by changing the optical path length of only one optical delay element. First
In addition, there is an effect that it is possible to cope with the change of the repetition period of the input optical pulse only by changing the repetition period of the second control voltage, and further, the conversion ratio of the repetition frequency of the optical pulse is set to not only 2 m but any integer. There is an effect that can be done.
第1図は本発明の一実施例を示すブロック図、 第2図は第1図に示す実施例の動作を説明するための波
形図、 第3図は従来のパルス多重光学系の一例の動作原理を説
明するための光路図、 第4図は同じくタイミング図である。 1,2……ポッケルスセル、3,5……偏光板、4……光遅延
セル、7……制御信号発生器、61,62……平面鏡。FIG. 1 is a block diagram showing an embodiment of the present invention, FIG. 2 is a waveform diagram for explaining the operation of the embodiment shown in FIG. 1, and FIG. 3 is an operation of an example of a conventional pulse multiplexing optical system. FIG. 4 is an optical path diagram for explaining the principle, and FIG. 1,2 ... Pockels cell, 3,5 ... polarizer, 4 ... optical delay cell, 7 ... control signal generator, 61,62 ... plane mirror.
Claims (1)
受ける第1の偏光板と、第1の偏光板を透過したパルス
光を受け入力される光の偏光方向を制御電圧に応じて変
えるシリーズに配列された第1及び第2の電気光学素子
と、第2の電気光学素子の出力のうち第1の偏光成分を
反射し第2の偏光成分を透過しこの第1及び第2の偏光
成分のうち一方の偏光成分を外部出力として出力する第
2の偏光板と、第2の偏光板の出力のうち外部出力とし
て出力されない他方の偏光成分を受け入力パルス光の繰
り返し周期の整数分の1の時間だけ遅延させ第1の偏光
板へ帰還させる光遅延素子とを具備し、入力パルス光を
第2の偏光板を経て光遅延素子へ導くように入力パルス
光のタイミングに同期した制御電圧で第1の電気光学素
子を制御するとともに、第2の偏光板を経て外部出力と
して出力される偏光成分を発生させるために入力パルス
光の周期間で漸次変化してゆく制御電圧で第2の電気光
学素子を制御することを特徴とするパルス多重光学系。1. A series comprising: a first polarizing plate for receiving an input pulse light having a predetermined repetition period; and a series for changing the polarization direction of the input light by receiving the pulse light transmitted through the first polarizing plate according to a control voltage. The first and second electro-optical elements are arranged in a matrix, and the first and second polarization components of the output of the second electro-optical element reflect the first polarization component and transmit the second polarization component. And a second polarizing plate that outputs one of the polarized light components as an external output, and receives the other polarized light component that is not output as an external output among the outputs of the second polarizing plate, and receives an integer fraction of the repetition period of the input pulse light. And an optical delay element for delaying the input pulse light through the second polarizer to the optical delay element with a control voltage synchronized with the timing of the input pulse light. To control the first electro-optical element The second electro-optical element is controlled by a control voltage gradually changing between the periods of the input pulse light in order to generate a polarization component output as an external output through the second polarizing plate. Pulse multiplexing optical system.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP414288A JP2591003B2 (en) | 1988-01-11 | 1988-01-11 | Pulse multiplex optical system |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP414288A JP2591003B2 (en) | 1988-01-11 | 1988-01-11 | Pulse multiplex optical system |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH01179910A JPH01179910A (en) | 1989-07-18 |
| JP2591003B2 true JP2591003B2 (en) | 1997-03-19 |
Family
ID=11576529
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP414288A Expired - Lifetime JP2591003B2 (en) | 1988-01-11 | 1988-01-11 | Pulse multiplex optical system |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2591003B2 (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR2686198B1 (en) * | 1992-01-14 | 1994-03-11 | Thomson Csf | METHOD AND DEVICE FOR GENERATING A PULSE EMISSION USING A LASER SOURCE. |
| WO1995026517A1 (en) * | 1992-11-10 | 1995-10-05 | United States Department Of Energy | Laser beam pulse formatting method |
| JP5060733B2 (en) * | 2005-03-28 | 2012-10-31 | オリンパス株式会社 | Optical pulse multiplexing unit, optical pulse generator using the same, and optical pulse multiplexing method |
| JP4889417B2 (en) * | 2006-09-13 | 2012-03-07 | オリンパス株式会社 | Optical pulse multiplexing unit |
-
1988
- 1988-01-11 JP JP414288A patent/JP2591003B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH01179910A (en) | 1989-07-18 |
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