GB2110498A - Laser telecommunications system - Google Patents
Laser telecommunications system Download PDFInfo
- Publication number
- GB2110498A GB2110498A GB8220204A GB8220204A GB2110498A GB 2110498 A GB2110498 A GB 2110498A GB 8220204 A GB8220204 A GB 8220204A GB 8220204 A GB8220204 A GB 8220204A GB 2110498 A GB2110498 A GB 2110498A
- Authority
- GB
- United Kingdom
- Prior art keywords
- laser
- signal
- angle modulated
- shift keying
- frequency
- 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.)
- Granted
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
- H04B10/60—Receivers
- H04B10/66—Non-coherent receivers, e.g. using direct detection
- H04B10/69—Electrical arrangements in the receiver
-
- 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
- H01S5/40—Arrangement of two or more semiconductor lasers, not provided for in groups H01S5/02 - H01S5/30
- H01S5/4006—Injection locking
-
- 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
- H04B10/29—Repeaters
- H04B10/291—Repeaters in which processing or amplification is carried out without conversion of the main signal from optical form
- H04B10/2912—Repeaters in which processing or amplification is carried out without conversion of the main signal from optical form characterised by the medium used for amplification or processing
- H04B10/2914—Repeaters in which processing or amplification is carried out without conversion of the main signal from optical form characterised by the medium used for amplification or processing using lumped semiconductor optical amplifiers [SOA]
-
- 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
- H04B10/29—Repeaters
- H04B10/291—Repeaters in which processing or amplification is carried out without conversion of the main signal from optical form
- H04B10/299—Signal waveform processing, e.g. reshaping or retiming
-
- 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
- H04B10/40—Transceivers
- H04B10/43—Transceivers using a single component as both light source and receiver, e.g. using a photoemitter as a photoreceiver
-
- 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
- H04B10/60—Receivers
- H04B10/66—Non-coherent receivers, e.g. using direct detection
- H04B10/67—Optical arrangements in the receiver
- H04B10/671—Optical arrangements in the receiver for controlling the input optical signal
- H04B10/675—Optical arrangements in the receiver for controlling the input optical signal for controlling the optical bandwidth of the input signal, e.g. spectral filtering
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Engineering & Computer Science (AREA)
- Computer Networks & Wireless Communication (AREA)
- Signal Processing (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Optical Communication System (AREA)
Abstract
The output of a spectrum stabilised transmitting laser (5, 15) is angle modulated by a signal to be transmitted and is coupled to a monomode optical fibre link (8). A second spectrum stabilised laser (10, 15) is located at the other end of the link. Each laser is arranged so that it can be injection locked by a signal received from the other so that it can oscillate in synchronism with the other laser. This arrangement provides a bi- directional link. Also disclosed is a demodulator for demodulating angle modulated optical signals. <IMAGE>
Description
SPECIFICATION
Laser telecommunications system
The present invention relates to laser telecommunications systems. The system to be described is particularly, but not exclusively, suitable for use in submarine applications and also for bi-directional data iinks. The invention also relates to a demodulator which can be used in
such systems.
The invention includes a laser telecommunications system comprising a spectrum stabilised first laser having an output which may be angle modulated by a signal to be transmitted and which is coupled to one end of a monomode optical fibre section, and a second laser coupled to the other end of said fibre section and adapted to be injection locked by a received signal and thereby oscillate in synchronism with said transmitting laser.
The second laser can act as a repeater and its output can be coupled to a further monomode optical fibre section. Such a repeater is of extremely simple design and may be produced in a relatively compact package. As the repeater laser is operated as a synchronised oscillator not as a laser amplifier the repeater does not amplify intensity varying noise thus reducing the error rate in digital transmissions and the distortion of analogue signals. By utilising a wavelength, preferably substantially 1 .55,um, at which the loss of the monomode fibre is at a minimum repeater spacing may be further increased.
In one aspect of the invention the second laser is spectrum stabilised and has an output which may be angle modulated by a signal to be transmitted, the system further comprising means for selecting which laser is to transmit and which to receive. In this way a simple bi-directional link may be set up which can transmit data in one direction at a time between two stations.
The signal at the receiver requires demodulation. This can be carried out electrically after heterodyne detection but such detection requires the use of a precisely tuned local oscillator. In the present invention we provide a more simple demodulation technique.
According to another aspect of the present invention there is provided a method of demodulating an angle modulated optical signal comprising dividing the signal into two, passing the two signals along paths of different length, combining the signals and applying the combined signal to a non-linear photo-detector.
According to a further aspect of the present invention there is provided apparatus for demodulating an angle modulated optical signal comprising means for dividing the signal into two so that the two signals can be transmitted along paths of different length, means for combining the signals after transmission along said paths, and non-linear photo-detection means arranged to receive the combined signal.
The invention will be described now by way of example only with reference to the accompanying
drawings in which:
Figure 1 is a diagrammatic representation of a
laser telecommunications system;
Figure 2 is a diagrammatic representation of a
bi-directional data link, and
Figures 3A, B and C illustrate a demodulation
system.
The system of Figure 1 comprises a transmitter
1 and a receiver 2 with a monomode optical fibre
transmission line 3 therebetween. One or more
repeaters 4 may be spaced at intervals along the
line 3.
The transmitter 1 comprises a spectrum
stabilised first laser 5 which is provided with
wavelength control means 6 arranged such that
the laser 5 produces only a single mode output
with a relatively narrow line width. This spectrum
stabilisation may be achieved by a wavelength
sensing system as described in the Post Office's
UK Patent Specification No. 2,007,01 5A entitled
"Control Apparatus", or by means of an injection
locking system as described in UK Patent
Application No. 8104828 entitled "Spectrum
Stabilised Laser Transmitter" and a paper of the
same title by D. J. Malyon, D. W. Smith and R. W.
Berry published in the proceedings of the Third
International Conference on Integrated Optics and
Optical Fibre Cbmmunication 1 981. The laser 5
may be a semiconductor laser for example a double heterojunction laser based on an InP substrate and having an InP Ga As active region.
In submarine applications it may be desirable to
provide a more complex laser at the transmitter terminal, which laser is capable of producing an
extremely narrow line width and higher power into
the transmission line, thus enabling a higher data
rate and longer repeater spacing to be achieved.
For this purpose a Neodymium/YAG laser may be used.
The laser 5 is angle modulated to produce an output signal which has analogue frequency modulation, or digital frequency shift keying or digital differential phase shift keying.
In order to angle modulate the transmitter laser 5 it is possible either to provide a separate modulator unit or, in the case of a semiconductor laser, to apply the signal to be transmitted as a perturbation to the bias current of the laser. This
latter method is illustrated in Figure 1 where the data input is along line 7 and directly frequency modulates the laser 5. If phase modulation is required a differentiator may be placed in line 7.
Recent work by Koyayashi et al published in
Electronics Letters Vol 1 7 No. 10 has shown that almost frequency independent frequency deviation can be produced in an AlGaAs semiconductor laser having a centre wavelength of 834 nm for modulation frequencies in the range 1 OMHz1 GHz. It will be appreciated that the necessary laser bias current may be experimentally determined for the operation of an appropriate semiconductor laser in this manner about a wavelength of 1 .55um. The modulation frequencies should be sufficiently high so that any wavelength sensing mode control of the laser is not influenced by the small and relatively rapid modulation induced wavelength changes.It is envisaaed that for maximum deviation of the bias current by a few milliamps a frequency variation of about 1GHz can be achieved.
Where other types of laser are utilised external modulator units are required, for example a phase modulator having a Lithium Niobate electrooptic device may be used to phase modulate a 1 523from helium-neon laser.
The single mode angle modulated output from the transmitter laser 5 is coupled into a monomode optical fibre section 8 of the transmission line 3. The fibre is preferably manufactured to have minimum loss at an operating wavelength of 1.55Etm thus taking advantage of the minimum possible theoretical loss region. Such a fibre has been described by
Miya et al in Electronics Letters Vol 1 5 No. 4 under the title "Ultimate Low-Loss Single-Mode
Fibre at 1.5/lem".
Preferably the optical fibre used is polarisation holding so that the transmitted single mode remains in the polarisation emitted by laser 5 and does not spread into the opposite polarisation during transmission.
Repeaters 4 are spaced along the transmission line 3 and connected to each other or to the transmitter 1 or receiver 2 as appropriate by sections of monomode optical fibre 8, 9 which it is envisaged may be of 60km or more in length. Each repeater 4 comprises a second laser 10 which is provided with wavelength control means 11 which monitors a part of the output of laser 10 by means not shown and operates to ensure that a cavity mode of the laser 10 is aligned with that of laser 5. In this way the laser light from the optical fibre section 8 which is incident on laser 10 injection locks the second laser 10 into the same single mode as the transmitting laser and causes it to operate in synchronism with the laser 5 thus reproducing the transmitted angle modulated signal.The second laser 10 is provided with a bias current above the threshold for oscillation and therefore operates as a synchronised oscillator and not as a laser amplifier. Operation as a synchronised oscillator reduces the effects of intensity fluctuations.
Alders formula:
where Nf,= full lock in bandwidth fo = centre optical frequency
Q = cold cavity 0
P, = Injected signal power P2- Power within cavity of locked laser which has been shown to apply to laser injection locking illustrates how the repeater spacing may be limited by the locking ability of the repeater lasers. If small AfL are utilised as may be feasible for transmitting digital signals by frequency or phase shift keying the signal may be permitted to attenuate to a lower power level (P1) before repeating. Whereas if a high bandwidth is required as for transmitting an analogue signal the repeater spacing must be reduced in order that the repeater lasers 10 will lock in over the full bandwidth.
Allowing 2 x 4dB coupling losses, 0.3dB/km fibre, 0.2 dB/km splicing lass a repeater section length of 60km or more may be possible for 1 GHz lock-in range:
Preferably the repeater lasers 10 are semiconductor lasers thus allowing the repeater structure to be reduced to the minimum size. The size of the repeater package is particularly important in submarine cables so that the repeaters do not unduly disturb the cable laying and burying operations. The simplicity of the repeater structure also increases overall reliability in a submarine cable as there are fewer components to fail.
An isolator 1 2 is interposed between the end of the fibre section 8 and the input to repeater laser 10 in order to prevent output from the back mirror of laser 10 travelling back along the transmission line 3 and interacting with the transmitted signal.
Preferably the isolator is a magneto-optic Faraday effect isolator. If the lasers are ring lasers an isolator may not be required.
Clearly any number of repeaters 4 may be provided with intermediate monomode optical fibre sections depending on the required length of the overall line 3. The first repeater laser will be locked to the transmitting laser 5 and thereafter each repeater laser will lock to the last preceding repeater laser in the line 3.
The last optical fibre section 9 links the last repeater with the receiver 2. The receiver 2 comprises a demodulator 1 3 which may be a direct optical frequency discriminator, for example, a Fabry-Perot Interferometer which converts the frequency variations into intensity variations.
Alternatively demodulation may be done electrically after heterodyne detection. Heterodyne detection requires the provision of a precisely tuned local oscillator which increases the cost and decreases system reliability. In order to overcome this problem a demodulating arrangement as shown in Figure 3 is proposed.
This demodulator requires the data to be encoded in a return-to-zero format as shown in
Figure 3A wherein each bit has a length T. The incoming signal is divided into two paths 20 and 21 before recombining at 22 and supplying the output to a photodiode 23. The path 21 is longer than path 20 by an amount which produces a delay of T/2 in the signal propagated along that path. The signal applied to the photodiode 23 will either be the 'zero' frequency alone or both the 'one' and 'zero' frequencies simultaneously.
Because of the intrinsic square law characteristic of the photodetection process the difference frequency or d.c. will appear at the output of the photodiode as seen in Figure 3C. This output is passed through a suitable filter 24 to produce the data output.
The bi-directional data link of Figure 2 works on the same principle as the above described system.
In this case at each end of the transmission line 3 an identical transmitter/receiver unit 14 is provided. Each unit 14 comprises a spectrum stabilised laser 1 5 with wavelength control means 16. The data input is fed via line 17 to produce perturbations in the laser bias current to directly frequency modulate the laser. As previously a differentiator (not shown) may be placed in line 1 7 to produce phase modulation. A demodulator 1 8 is also provided coupled to one of the mirrors of its associated laser. The output data is fed along line 19.
At any one time only one of the lasers 1 5 is transmitting along the monomode fibre transmission line 3. The other laser 1 5 is injection locked to the transmitting laser in the same manner as the repeater laser 10 of the Figure 1 system. Therefore both lasers act as synchronised oscillators and the output from the other mirror of the receiving laser 1 5 is fed directly to its associated demodulator 1 8.
As it is necessary to provide the possibility of transmission in both directions along the line 3 it is not possible to place an isolator in the line to prevent backward transmissions by the receiving laser which result in ringing between the lasers.
In order to overcome this problem one or both lasers 15 may be turned off for a short period intermittently. An alternative solution is for the transmitting laser to operate at a higher power than the receiving laser to prevent interaction.
It will be appreciated that the above described systems may be used to transmit digital or analogue signals by frequency or phase modulation. Phase modulation, in particular phase shift keying is a preferred form of modulation as this method avoids slippage of injection locking. In order to maximise repeater spacing the minimum bandwidth should be used; however data transmission rates can be increased by the use of multi-level phase or frequency shift keying.
Claims (19)
1. A method of demodulating an angle modulated optical signal comprising dividing the signal into two, passing the two signals along paths of different length, combining the signals and applying the combined signal to a non-linear photo-detector.
2. A method as claimed in claim 1 wherein the difference in path length is equivalent to T/2 where T is the width of an encoded bit.
3. A method as claimed in claim 1 or claim 2 wherein the detector is a photodiode.
4. A method as claimed in any preceding claim wherein the modulation is one of analogue frequency modulation, digital frequencies shift keying or digital differential phase shift keying.
5. Apparatus for demodulating an angle modulated optical signal comprising means for dividing the signal into two so that the two signals can be transmitted along paths of different length, means for combining the signals after transmission along said paths, and non-linear photo-detection means arranged to receive the combined signal.
6. Apparatus as claimed in claim 5 wherein the difference in path length is equivalent to T/2 where T is the width of an encoded bit.
7. Apparatus as claimed in claim 5 or claim 6 wherein the detector is a photodiode.
8. Apparatus as claimed in any one of claims 5 to 7 wherein the modulation is one of analogue frequency modulation, digital frequency shift keying or digital differential phase shift keying.
9. A laser telecommunication system comprising a spectrum stabilised first laser arranged to produce an output which may be angle modulated and which is coupled to one end of an optical fibre link, a spectrum stabilised second laser coupled to the other end of the fibre link and arranged to produce an output which may be angle modulated, each said laser being arranged so that it can be injection locked by a signal received from the other laser so that it can oscillate in synchronism with said other laser, and means for selecting which laser is to transmit and which to receive.
10. A system as claimed in claim 9 wherein said selecting means comprises means for supplying a higher power to the transmitting laser.
11. A system as claimed in claim 9 or claim 10 wherein the signal to be transmitted modulates the laser bias current either directly or via a differentiator to frequency or phase modulate the laser respectively.
12. A system as claimed in any one of claims 9 to 11 wherein a digital signal is transmitted by frequency or phase shift keying.
13. A system as claimed in any one of claims 9 to 12 wherein at least one of the lasers is a semiconductor laser.
14. A system as claimed in any one of claims 9 to 1 3 wherein the or each monomode optical fibre section is polarisation holding.
1 5. A system as claimed in any one of claims 9 to 14 which operates at a centre wavelength of substantially 1.55cm.
1 6. A system as claimed in any one of claims 9 to 1 5 including one or more repeaters, the or each repeater comprising a laser which is arranged to be injection locked by a received signal.
17. A method of demodulating an angle modulated optical signal substantially as hereinbefore described.
1 8. Apparatus for demodulating an angle modulated signal substantially as hereinbefore described with reference to and as shown in
Figure 3 of the accompanying drawings.
19. A laser telecommunications system substantially as hereinbefore described with reference to and as shown in Figure 2 of the accompanying drawings.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
GB8220204A GB2110498B (en) | 1981-07-14 | 1982-07-12 | Laser telecommunications system |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
GB8121709 | 1981-07-14 | ||
GB8220204A GB2110498B (en) | 1981-07-14 | 1982-07-12 | Laser telecommunications system |
Publications (2)
Publication Number | Publication Date |
---|---|
GB2110498A true GB2110498A (en) | 1983-06-15 |
GB2110498B GB2110498B (en) | 1985-09-04 |
Family
ID=26280122
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
GB8220204A Expired GB2110498B (en) | 1981-07-14 | 1982-07-12 | Laser telecommunications system |
Country Status (1)
Country | Link |
---|---|
GB (1) | GB2110498B (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO1987001538A1 (en) * | 1985-09-05 | 1987-03-12 | Caterpillar Industrial Inc. | Optical communication apparatus for a vehicle |
FR2652465A1 (en) * | 1989-09-27 | 1991-03-29 | France Etat | PHOTORECEPTOR FOR OPTICAL SIGNALS MODULES IN FREQUENCY. |
US5189544A (en) * | 1990-09-14 | 1993-02-23 | Siemens Aktiengesellschaft | Bidirectional light waveguide telecommunication system |
-
1982
- 1982-07-12 GB GB8220204A patent/GB2110498B/en not_active Expired
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO1987001538A1 (en) * | 1985-09-05 | 1987-03-12 | Caterpillar Industrial Inc. | Optical communication apparatus for a vehicle |
US4691385A (en) * | 1985-09-05 | 1987-09-01 | Caterpillar Industrial Inc. | Optical communication apparatus for a vehicle |
FR2652465A1 (en) * | 1989-09-27 | 1991-03-29 | France Etat | PHOTORECEPTOR FOR OPTICAL SIGNALS MODULES IN FREQUENCY. |
EP0420742A1 (en) * | 1989-09-27 | 1991-04-03 | France Telecom | Photoreceptor for frequency-modulated optical signals |
US5063567A (en) * | 1989-09-27 | 1991-11-05 | L'etat Francais Represente Par Le Ministre Des Postes, Des Telecommunications Et De L'espace (Centre National D'etudes Des Telecommunications) | Photoreceptor for frequency-modulated optical signals |
US5189544A (en) * | 1990-09-14 | 1993-02-23 | Siemens Aktiengesellschaft | Bidirectional light waveguide telecommunication system |
Also Published As
Publication number | Publication date |
---|---|
GB2110498B (en) | 1985-09-04 |
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
732 | Registration of transactions, instruments or events in the register (sect. 32/1977) | ||
PCNP | Patent ceased through non-payment of renewal fee |
Effective date: 19950712 |