AU609541B2 - A laser pulse shaper - Google Patents
A laser pulse shaper Download PDFInfo
- Publication number
- AU609541B2 AU609541B2 AU25972/88A AU2597288A AU609541B2 AU 609541 B2 AU609541 B2 AU 609541B2 AU 25972/88 A AU25972/88 A AU 25972/88A AU 2597288 A AU2597288 A AU 2597288A AU 609541 B2 AU609541 B2 AU 609541B2
- Authority
- AU
- Australia
- Prior art keywords
- pulse
- laser
- electric
- predistorter
- waveguide
- 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.)
- Ceased
Links
- 230000005669 field effect Effects 0.000 claims description 7
- 238000002347 injection Methods 0.000 claims description 7
- 239000007924 injection Substances 0.000 claims description 7
- 238000000034 method Methods 0.000 claims description 6
- 238000007493 shaping process Methods 0.000 claims 3
- 230000003287 optical effect Effects 0.000 description 6
- 230000000694 effects Effects 0.000 description 3
- 230000010355 oscillation Effects 0.000 description 2
- 241000534944 Thia Species 0.000 description 1
- 238000013459 approach Methods 0.000 description 1
- 238000001208 nuclear magnetic resonance pulse sequence Methods 0.000 description 1
- 230000001151 other effect Effects 0.000 description 1
- 230000005855 radiation Effects 0.000 description 1
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
- H04B10/58—Compensation for non-linear transmitter output
-
- 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
- H01S5/06209—Arrangements for controlling the laser output parameters, e.g. by operating on the active medium by varying the potential of the electrodes in single-section lasers
- H01S5/06216—Pulse modulation or generation
-
- 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
- H04B10/25—Arrangements specific to fibre transmission
- H04B10/2507—Arrangements specific to fibre transmission for the reduction or elimination of distortion or dispersion
- H04B10/2513—Arrangements specific to fibre transmission for the reduction or elimination of distortion or dispersion due to chromatic dispersion
- H04B10/25137—Arrangements specific to fibre transmission for the reduction or elimination of distortion or dispersion due to chromatic dispersion using pulse shaping at the transmitter, e.g. pre-chirping or dispersion supported transmission [DST]
-
- 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
- H04B10/501—Structural aspects
- H04B10/503—Laser transmitters
- H04B10/504—Laser transmitters using direct modulation
-
- 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
- H01S5/04—Processes or apparatus for excitation, e.g. pumping, e.g. by electron beams
- H01S5/042—Electrical excitation ; Circuits therefor
- H01S5/0428—Electrical excitation ; Circuits therefor for applying pulses to the laser
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Engineering & Computer Science (AREA)
- Computer Networks & Wireless Communication (AREA)
- Signal Processing (AREA)
- Optics & Photonics (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Nonlinear Science (AREA)
- Optical Communication System (AREA)
- Semiconductor Lasers (AREA)
Description
609541 UMQRiGa ocl )0 00 COMMONWEALTH OF AUSTRALIA PATENTS ACT 1952-1969 COMPLETE SPECIFICATION FOR THE INVENTION ENTITLED "A LASER PULSE SHAPER" The following statement is a full description of this invention, including the best method of performing it known to us:j a
F
j ,r The present invention relates to a circuit arrangement for modulating an injection laser, comprising a predistorter which predistorts an electric signal containing rectangular pulses for generating an optical signal containing rectangular pulses.
A circuit arrangement of this kind is disclosed in German Patent 25 43 570. A "pulse-wave-modulating facility" is mentioned there which "varies the width and/or amplitude of the modulating pulse" (column 2, line 66, to column 3, °rLQ line 9).
During digital modulation, the following effects, which are undesirable for optical communication, may occur at high o 00 00°° 0 bit rates: 1. The optical output pulses of the laser have different amplitudes depending on the pulse sequence of the input signal (pattern effect). A 1-state output following a 0 0",000 state (no voltage pulse at the laser input) is smaller 0 othan if a 1 was modulated immediately beforehand.
.o o 2. The optical signal approaches the rectangular waveform 08 0 0 much less than the electric signal does. The trailing edge, in particular, is much less steep than that of the 3lectric signal.
3. Due to the phase relationship between photon density and electron density, the optical signal exhibits damped oscillations after the trailing edge.
4. This phenomenon entails an increase in the linewidth of the emitted radiation.
The circuit arrangement disclosed in the above German patent specification predistorts the modulating current.
However, the patent specification does not describe how each individual pulse must be predistorted in order for the laser to produce an optical pulse equivalent to the respective electric pulse.
It is desirable to provide a circuit arrangement which predistorts each electric pulse so as to compensate for distortions caused by the laser.
This specification discloses a method of predistorting a pulse signal comprising the steps of causing the pulse to "o o rise to its full amplitude via an intermediate amplitude, o 00 and causing a backswing in the amplitude of the trailing edge of the pulse.
There is also disclosed a circuit for performing the predistortion.
One of the advantages of the invention is that no discriminator for recognizing the bit sequence is needed, o 0 since each pulse is predistorted independently of the preceding pulse and since even very high pulse frequencies can 000 be processed.
o o A further advantage is that the other effects referred to above are also largely suppressed. The backswing added to the trailing edge of each pulse eliminates the pattern effect and provides sufficient edge steepness. By the preliminary step of the pulse, the damped oscillations and, thus, the increases in linewidth are suppressed.
An embodiment of the invention will now be explained with reference to the accompanying drawings, in which: Fig 1 shows the shape of' a predis tortoed po Iso l~n oomt parison with an input pulse, and Fig. 2 shows a predistorter circuiit emibodyinig Uthi-,r~ vention.
Fig. 1 shows the rectangular input pulse VE (above) and the predistorted pulse (below), consisting of a pre"Liminary step, a constant portion, and a backswing at the trailing edge.
Fig. 2 shows a field-effect transistor, In a ooinmon- ~lQ~source configuration, as is described, Cor examplo, 'in U.
Tietze, Ch. Schenk,, "H albleiter-Schltng3t;echnrlk" llerln, 8th edition, 1986, p. 89. The drain of the Vlold-e~f'ent transistor Fl. :Is connected via a resistor TID to tho poiltive Germninal of a voltage source, and the source of the Moeldeffect transistor is grounded. At t, e inpt end, a ignal Osource providing a voltage VE is connected In tir'ies wit~h the internal resistance ci. to the gate of' the Cede~c 0:00:transistor Fl.; at the output, a voltage VA Is takeon between 0:00 the drain terminal and ground.
A series combination of,' a waveguide TI., haiving a predetermined characteristic Impedance ZI and a prodetomined delay TI, and a reoistor RI in connected between the gate of the field-effect tranW3iitor F)1 and ground, wIth the waveguide having one end connected to the gate,, and the, other grounded through the res~istor Thia aeries combination is shunted by a resistor RG.
Connected to the oarain of the Pield-cff'eot tranoistor is a second waveguide Z2, T2 having a predetermlned characteristic impedance Z2 and a predetermIned delay T2. Thi1s waveguide has an open end at which the waveo are reClected.
The waveguides are preferably implemented with microstrip lines; coaxial lines are also suitable. The network formed by the waveguide Z1, Ti and the resistors Rl and RG deforms the input voltage VE. The gate of the field-effect transistor Fl is thus subjected to a voltage consisting of a component proportional to VE and a superposed component approximately proportional to the time derivative of VE. At that point, the pulse consists of an overshoot, a constant portion, and a backswing. The overshoot of the output volt- Sl"'d age VA is suppressed by suitable choice of the operating point of the field-effect transistor Fl and the stepping of the leading edge. The second waveguide Z2, T2 produces the preliminary step of the pulse. The output of the S predistorter thus provides a voltage VA as shown in the lower part of Fig. 1.
o o a 4 9
Claims (4)
1. A method of predistorting an electric pulse signal for modulating an injection laser, the method comprising the steps of applying an input electric pulse to pulse shaping circuit to cause the pulse to rise to its full amplitude via an intermediate amplitude step, the pulse shaping circuit also causing a backswing in the amplitude of the trailing edge of the pulse, whereby, when the electric pulse signal 0 is used to modulate an injection laser, a substantially rec- o" tangular laser pulse is produced. a 0
2. A method of predistorting an electric pulse signal for a modulating an injection laser, the method as herein de- S0 0 scribed with reference to the accompanying drawings. 0 0
3. A circuit arrangement for modulating an injection la- ser, comprising a predistorter which predistorts an electric 0 0 signal containing rectangular pulses for generating subtantially rectangular laser pulses, wherein the predistorter causes each pulse to rise to its full amplitude in two steps and produces a backswing at the trailing pulse S edge, wherein the predistorted electric signals are applied 0~ to the injection laser to produce substantially rectangular 0 00 laser pulses.
4. A circuit arrangement as claimed in claim 3, wherein Sthe predistorter includes a field-effect transistor in a common-source configuration, the gate of the field-effect transistor is grounded through a first waveguide having a first predetermined characteristic impedance and a first 6 *with a first resistor, wherein the gate is grounded through RA41 a second resistor in parallel with the first waveguide and the first resistor and wherein the drain of the field-effect transistor is connected to a second waveguide having a sec- ond predetermined characteristic impedance and a second pre- determined delay and whose distal end is open. A pulse predistorter for generating an electric pulse signal to modulate an injection laser, the distorter com- prising a pulse shaping circuit as herein described with reference to the accompanying drawings. 0 0 0 0 0 o oQ 0 0 00 0 0 0 00 0 0 0 I SDATED THIS TWENTY-FOURTH DAY OF JANUARY, 1991 I o"o I ALCATEL N.V. 0 0 0 00 o 00 0 o 0 o 'O /^di
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| DE19873741305 DE3741305A1 (en) | 1987-12-05 | 1987-12-05 | CIRCUIT ARRANGEMENT FOR MODULATING A SEMICONDUCTOR INJECTION LASER FOR OPTICAL MESSAGE TRANSMISSION |
| DE3741305 | 1987-12-05 |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| AU2597288A AU2597288A (en) | 1989-06-15 |
| AU609541B2 true AU609541B2 (en) | 1991-05-02 |
Family
ID=6341975
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| AU25972/88A Ceased AU609541B2 (en) | 1987-12-05 | 1988-11-29 | A laser pulse shaper |
Country Status (4)
| Country | Link |
|---|---|
| EP (1) | EP0319852B1 (en) |
| AU (1) | AU609541B2 (en) |
| DE (2) | DE3741305A1 (en) |
| ES (1) | ES2052677T3 (en) |
Families Citing this family (9)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| GB2245756B (en) * | 1990-06-23 | 1994-06-08 | Stc Plc | Digital driving of injection lasers |
| DE59108602D1 (en) * | 1990-07-03 | 1997-04-17 | Siemens Ag | Laser diode transmitter |
| DE4025497C2 (en) * | 1990-08-11 | 1996-12-19 | Hell Ag Linotype | Method and circuit arrangement for correcting the radiation power of a laser diode |
| DE4026087C2 (en) * | 1990-08-17 | 1996-12-12 | Hell Ag Linotype | Method and circuit arrangement for controlling a laser diode |
| DE4318857C1 (en) * | 1993-06-07 | 1994-07-28 | Ant Nachrichtentech | Driver stage for optical transmitter delivering constant current |
| RU2118907C1 (en) * | 1997-03-24 | 1998-09-20 | Георгий Анатольевич Басс | Liquid and gas interaction apparatus |
| US6947456B2 (en) * | 2000-12-12 | 2005-09-20 | Agilent Technologies, Inc. | Open-loop laser driver having an integrated digital controller |
| DE10065838C2 (en) | 2000-12-29 | 2003-06-26 | Infineon Technologies Ag | Electronic driver circuit for a directly modulated semiconductor laser |
| DE10218939B4 (en) * | 2002-04-19 | 2005-08-25 | Infineon Technologies Ag | Laser driver and method for controlling the modulation of a laser diode |
Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3711740A (en) * | 1969-12-05 | 1973-01-16 | Hitachi Ltd | Response time controlled light emitting devices |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE3307309A1 (en) * | 1983-03-02 | 1984-09-13 | Bosch Gmbh Robert | Method and arrangement for the optical transmission of an electric signal |
-
1987
- 1987-12-05 DE DE19873741305 patent/DE3741305A1/en not_active Withdrawn
-
1988
- 1988-11-29 AU AU25972/88A patent/AU609541B2/en not_active Ceased
- 1988-12-02 DE DE88120118T patent/DE3888472D1/en not_active Expired - Fee Related
- 1988-12-02 ES ES88120118T patent/ES2052677T3/en not_active Expired - Lifetime
- 1988-12-02 EP EP88120118A patent/EP0319852B1/en not_active Expired - Lifetime
Patent Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3711740A (en) * | 1969-12-05 | 1973-01-16 | Hitachi Ltd | Response time controlled light emitting devices |
Also Published As
| Publication number | Publication date |
|---|---|
| DE3888472D1 (en) | 1994-04-21 |
| AU2597288A (en) | 1989-06-15 |
| ES2052677T3 (en) | 1994-07-16 |
| EP0319852B1 (en) | 1994-03-16 |
| DE3741305A1 (en) | 1989-06-15 |
| EP0319852A2 (en) | 1989-06-14 |
| EP0319852A3 (en) | 1989-09-06 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| AU609541B2 (en) | A laser pulse shaper | |
| US4412337A (en) | Power amplifier and envelope correction circuitry | |
| JPH03195101A (en) | Feed-forward predistortion linearizer | |
| US20030164782A1 (en) | Method and apparatus for electrical non-return to zero to return to zero conversion | |
| US5930022A (en) | Driving circuit for electro-absorption optical modulator | |
| US6985020B2 (en) | Inline predistortion for both CSO and CTB correction | |
| WO2002071663A3 (en) | Method for reducing the out-of-band emission in am transmitters for digital transmission | |
| US4322811A (en) | Clamping circuit for an adaptive filter | |
| US4021685A (en) | Pulse circuit for reshaping long line pulses | |
| US4412336A (en) | Storage comparator, for regenerating digital electric signals and digital transmission system using such a comparator | |
| US4298841A (en) | Signal envelope detecting system | |
| US4933626A (en) | Methods and apparatus for controlling power amplifiers driving highly inductive loads | |
| US5391933A (en) | Driver circuit for generating pulses | |
| US20020070784A1 (en) | Dynamic line termination with self-adjusting impedance | |
| WO1998026501A8 (en) | Class d amplifier | |
| US5373388A (en) | AC coupled fiber optic receiver with DC coupled characteristics | |
| CN101379697A (en) | Power amplifier with digital predistortion | |
| US4432024A (en) | Method and apparatus for minimizing non-linear distortion in the recording of a bi-level signal | |
| EP1039631A1 (en) | Pre/post-distortion circuit and method, particularly for microwave radio-frequency systems | |
| GB975944A (en) | Improvements in or relating to electric pulse transmission systems | |
| CN109889188B (en) | Triangular wave generating device and system | |
| BE905922R (en) | Amplitude limiting circuit for telephone system - derives reference voltages by bridge measuring voltage drop across IGFET strapped as diode | |
| KR100224178B1 (en) | Noise suppression device for car audio | |
| GB2245756A (en) | Digital driving of injection lasers | |
| JPH0817336B2 (en) | Signal receiving circuit and optical pulse receiving circuit using the same |