ES2148411T3 - Metodo para el control de un laser semiconductor con selectividad de modalidad, con banda ancha de modulacion, y sistema de comunicacion optica. - Google Patents

Metodo para el control de un laser semiconductor con selectividad de modalidad, con banda ancha de modulacion, y sistema de comunicacion optica.

Info

Publication number
ES2148411T3
ES2148411T3 ES95119079T ES95119079T ES2148411T3 ES 2148411 T3 ES2148411 T3 ES 2148411T3 ES 95119079 T ES95119079 T ES 95119079T ES 95119079 T ES95119079 T ES 95119079T ES 2148411 T3 ES2148411 T3 ES 2148411T3
Authority
ES
Spain
Prior art keywords
modulation
semiconductor laser
modality
selectivity
communication system
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
Application number
ES95119079T
Other languages
English (en)
Inventor
Toshihiko Ouchi
Masao Majima
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.)
Canon Inc
Original Assignee
Canon Inc
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 Canon Inc filed Critical Canon Inc
Application granted granted Critical
Publication of ES2148411T3 publication Critical patent/ES2148411T3/es
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Classifications

    • H—ELECTRICITY
    • H04—ELECTRIC COMMUNICATION TECHNIQUE
    • H04B—TRANSMISSION
    • H04B10/00—Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
    • H04B10/50—Transmitters
    • H04B10/516—Details of coding or modulation
    • H04B10/532—Polarisation modulation
    • B—PERFORMING OPERATIONS; TRANSPORTING
    • B82—NANOTECHNOLOGY
    • B82Y—SPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
    • B82Y20/00—Nanooptics, e.g. quantum optics or photonic crystals
    • 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
    • H01S5/00—Semiconductor lasers
    • H01S5/06—Arrangements for controlling the laser output parameters, e.g. by operating on the active medium
    • H01S5/062—Arrangements for controlling the laser output parameters, e.g. by operating on the active medium by varying the potential of the electrodes
    • H01S5/0625—Arrangements for controlling the laser output parameters, e.g. by operating on the active medium by varying the potential of the electrodes in multi-section lasers
    • 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
    • H01S5/00—Semiconductor lasers
    • H01S5/06—Arrangements for controlling the laser output parameters, e.g. by operating on the active medium
    • H01S5/062—Arrangements for controlling the laser output parameters, e.g. by operating on the active medium by varying the potential of the electrodes
    • H01S5/06233—Controlling other output parameters than intensity or frequency
    • H01S5/06236—Controlling other output parameters than intensity or frequency controlling the polarisation, e.g. TM/TE polarisation switching
    • 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
    • H01S5/00—Semiconductor lasers
    • H01S5/06—Arrangements for controlling the laser output parameters, e.g. by operating on the active medium
    • H01S5/062—Arrangements for controlling the laser output parameters, e.g. by operating on the active medium by varying the potential of the electrodes
    • H01S5/0625—Arrangements for controlling the laser output parameters, e.g. by operating on the active medium by varying the potential of the electrodes in multi-section lasers
    • H01S5/06255—Controlling the frequency of the radiation
    • H01S5/06258—Controlling the frequency of the radiation with DFB-structure
    • 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
    • H01S5/00—Semiconductor lasers
    • H01S5/30—Structure or shape of the active region; Materials used for the active region
    • H01S5/34—Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers
    • H01S5/3403—Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers having a strained layer structure in which the strain performs a special function, e.g. general strain effects, strain versus polarisation
    • H01S5/3404—Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers having a strained layer structure in which the strain performs a special function, e.g. general strain effects, strain versus polarisation influencing the polarisation
    • 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
    • H01S5/00—Semiconductor lasers
    • H01S5/30—Structure or shape of the active region; Materials used for the active region
    • H01S5/34—Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers
    • H01S5/343—Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers in AIIIBV compounds, e.g. AlGaAs-laser, InP-based laser
    • H01S5/34306—Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers in AIIIBV compounds, e.g. AlGaAs-laser, InP-based laser emitting light at a wavelength longer than 1000nm, e.g. InP based 1300 and 1500nm lasers
    • 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
    • H01S5/00—Semiconductor lasers
    • H01S5/30—Structure or shape of the active region; Materials used for the active region
    • H01S5/34—Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers
    • H01S5/343—Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers in AIIIBV compounds, e.g. AlGaAs-laser, InP-based laser
    • H01S5/34313—Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers in AIIIBV compounds, e.g. AlGaAs-laser, InP-based laser with a well layer having only As as V-compound, e.g. AlGaAs, InGaAs
    • 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
    • H01S5/00—Semiconductor lasers
    • H01S5/30—Structure or shape of the active region; Materials used for the active region
    • H01S5/34—Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers
    • H01S5/343—Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers in AIIIBV compounds, e.g. AlGaAs-laser, InP-based laser
    • H01S5/3434—Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers in AIIIBV compounds, e.g. AlGaAs-laser, InP-based laser with a well layer comprising at least both As and P as V-compounds

Landscapes

  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Electromagnetism (AREA)
  • Nanotechnology (AREA)
  • Chemical & Material Sciences (AREA)
  • Optics & Photonics (AREA)
  • Biophysics (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Signal Processing (AREA)
  • Crystallography & Structural Chemistry (AREA)
  • Computer Networks & Wireless Communication (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Semiconductor Lasers (AREA)
  • Optical Communication System (AREA)

Abstract

UN LASER DE RETROALIMENTACION DISTRIBUIDA REALIZA DE FORMA SELECTIVA UNA O DOS OSCILACIONES EN DIFERENTES MODOS DE POLARIZACION, TE O TM. DOS CORRIENTES DE MODULACION SON INYECTADAS EN DIFERENTES ELECTRODOS DEL LASER SEMICONDUCTOR QUE TIENE UNA PLURALIDAD DE ELECTRODOS. LA RELACION ENTRE LAS FASES DE LAS DOS CORRIENTES DE MODULACION ES AJUSTADA DE MODO QUE UNA FORMA DE ONDA DE SALIDA NO SE DISTORSIONE ESPECIALMENTE CUANDO UNA FRECUENCIA DE MODULACION SEA BAJA. LA MODULACION DE POLARIZACION SE APLICA COMO LA FORMA DE MODULACION.
ES95119079T 1994-12-05 1995-12-04 Metodo para el control de un laser semiconductor con selectividad de modalidad, con banda ancha de modulacion, y sistema de comunicacion optica. Expired - Lifetime ES2148411T3 (es)

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP30095694A JP3244976B2 (ja) 1994-12-05 1994-12-05 半導体レーザの駆動方法及び半導体レーザ装置及び光通信方法及びノード及び光通信システム

Publications (1)

Publication Number Publication Date
ES2148411T3 true ES2148411T3 (es) 2000-10-16

Family

ID=17891111

Family Applications (1)

Application Number Title Priority Date Filing Date
ES95119079T Expired - Lifetime ES2148411T3 (es) 1994-12-05 1995-12-04 Metodo para el control de un laser semiconductor con selectividad de modalidad, con banda ancha de modulacion, y sistema de comunicacion optica.

Country Status (6)

Country Link
US (1) US5850408A (es)
EP (1) EP0718937B1 (es)
JP (1) JP3244976B2 (es)
CA (1) CA2164492C (es)
DE (1) DE69516493T2 (es)
ES (1) ES2148411T3 (es)

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JPH118442A (ja) * 1996-10-07 1999-01-12 Canon Inc 光半導体デバイス、それを用いた光通信システム及び方法
DE19822616A1 (de) * 1998-05-20 1999-11-25 Sel Alcatel Ag Lichtquelle sowie Verfahren für die Übertragung von spektralkodierten Daten
JP3728147B2 (ja) 1999-07-16 2005-12-21 キヤノン株式会社 光電気混載配線基板
JP3990846B2 (ja) * 1999-08-27 2007-10-17 キヤノン株式会社 面型光素子、その製造方法、およびこれを用いた装置
JP4902044B2 (ja) * 1999-09-24 2012-03-21 シャープ株式会社 半導体レーザ装置、光伝送装置、光伝送システム、電子機器、制御装置、接続コネクタ、通信装置、ならびに光伝送方法、データ送受信方法
US6628686B1 (en) * 2001-11-16 2003-09-30 Fox-Tek, Inc Integrated multi-wavelength and wideband lasers
GB0206226D0 (en) * 2002-03-16 2002-05-01 Intense Photonics Ltd Electro-absorption modulator with broad optical bandwidth
JP3927913B2 (ja) * 2003-03-05 2007-06-13 キヤノン株式会社 光電気混載装置、及びその駆動方法
US7615787B2 (en) 2004-03-26 2009-11-10 Canon Kabushiki Kaisha Photo-semiconductor device and method of manufacturing the same
JP4785392B2 (ja) * 2004-03-26 2011-10-05 キヤノン株式会社 テラヘルツ電磁波の発生素子の製造方法
JP3913253B2 (ja) * 2004-07-30 2007-05-09 キヤノン株式会社 光半導体装置およびその製造方法
JP5196779B2 (ja) * 2006-03-17 2013-05-15 キヤノン株式会社 光伝導素子及びセンサ装置
JP4857027B2 (ja) * 2006-05-31 2012-01-18 キヤノン株式会社 レーザ素子
JP4958278B2 (ja) * 2007-03-13 2012-06-20 キヤノン株式会社 検査装置
US8385749B2 (en) * 2009-07-02 2013-02-26 International Business Machines Corporation High speed optical transmitter with directly modulated laser source
CN103762256B (zh) * 2014-01-15 2016-03-02 华南理工大学 生长在Si衬底上的InGaAs薄膜及其制备方法
JP2018060975A (ja) * 2016-10-07 2018-04-12 日本電信電話株式会社 直接変調レーザ
US11079432B2 (en) * 2019-02-19 2021-08-03 Nxp B.V. Integrated laser voltage probe pad for measuring DC or low frequency AC electrical parameters with laser based optical probing techniques
CN110544873B (zh) * 2019-08-29 2020-11-24 厦门市三安集成电路有限公司 分段式调制结构、激光器及其制作方法
US12132296B2 (en) * 2021-05-14 2024-10-29 Microsoft Technology Licensing, Llc Laser having reduced coherence via a phaser shifter
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Also Published As

Publication number Publication date
US5850408A (en) 1998-12-15
EP0718937A2 (en) 1996-06-26
JP3244976B2 (ja) 2002-01-07
DE69516493T2 (de) 2000-12-07
CA2164492C (en) 2000-02-01
JPH08162716A (ja) 1996-06-21
DE69516493D1 (de) 2000-05-31
EP0718937B1 (en) 2000-04-26
CA2164492A1 (en) 1996-06-06
EP0718937A3 (en) 1996-08-21

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