WO2000007317A1 - Procede et dispositif de reduction d'interference en amcr optique - Google Patents

Procede et dispositif de reduction d'interference en amcr optique Download PDF

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Publication number
WO2000007317A1
WO2000007317A1 PCT/US1999/017258 US9917258W WO0007317A1 WO 2000007317 A1 WO2000007317 A1 WO 2000007317A1 US 9917258 W US9917258 W US 9917258W WO 0007317 A1 WO0007317 A1 WO 0007317A1
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Prior art keywords
light
optical
code
data
spectral
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PCT/US1999/017258
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English (en)
Inventor
Birendra Dutt
Manouher Naraghi
James K. Chan
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Codestream Technologies Corporation
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Application filed by Codestream Technologies Corporation filed Critical Codestream Technologies Corporation
Priority to CA002339113A priority Critical patent/CA2339113A1/fr
Priority to EP99938889A priority patent/EP1101309A1/fr
Priority to AU53278/99A priority patent/AU5327899A/en
Priority to KR1020017001291A priority patent/KR20010072120A/ko
Priority to JP2000563022A priority patent/JP2002521957A/ja
Priority to BR9912598-6A priority patent/BR9912598A/pt
Publication of WO2000007317A1 publication Critical patent/WO2000007317A1/fr

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    • 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
    • H—ELECTRICITY
    • H04—ELECTRIC COMMUNICATION TECHNIQUE
    • H04J—MULTIPLEX COMMUNICATION
    • H04J11/00—Orthogonal multiplex systems, e.g. using WALSH codes
    • H04J11/0023—Interference mitigation or co-ordination
    • 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
    • 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
    • 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
    • H—ELECTRICITY
    • H04—ELECTRIC COMMUNICATION TECHNIQUE
    • H04J—MULTIPLEX COMMUNICATION
    • H04J14/00—Optical multiplex systems
    • H04J14/005—Optical Code Multiplex
    • H04J14/007—Orthogonal Optical Code Multiplex

Definitions

  • This invention relates to optical communication systems and, more particularly, to optical code-division multiple access communications systems that transmit data over optical fibers.
  • optical fibers over long distances is expensive. Additionally, conventional optical fiber or other optical communication networks utilize only a small fraction of the available bandwidth of the communication system. There is consequently considerable interest m obtaining higher utilization of fiber networks or otherwise increasing the bandwidth of optical fiber systems.
  • Techniques have been developed to increase the bandwidth of optical fiber communication systems and to convey information from plural sources over a fiber system. Generally, these techniques seek to use more of the readily available optical bandwidth of optical fibers by supplementing the comparatively simple coding schemes conventionally used by such systems.
  • TDM time-division multiplexing
  • TDMA time -division multiple access
  • Time division techniques transmit frames of data by assigning successive time slots in the frame to particular communication channels
  • Optical TDMA requires short-pulsed diode lasers and provides only moderate improvements in bandwidth utilization
  • improving the transmission rates on a TDM network requires that all of the transceivers attached to the network be upgraded to the higher transmission rates. No partial network upgrades are possible, which makes TDM systems less flexible than is desirable
  • TDM systems provide a predictable and even data flow, which is very desirable in multi-user systems that expe ⁇ ence "bursty" usage.
  • TDM techniques will have continued importance in optical communications systems, but other techniques must be used to obtain the desired communications bandwidth for the overall system. Consequently, it is desirable to provide increased bandwidth m an optical system that is compatible with TDM communication techniques.
  • WDM wavelength-division multiplexing
  • WDMA wavelength-division multiple access
  • WDM systems provide plural optical channels each using one of a set of non-overlapping wavelength bands to provide expanded bandwidth.
  • Information is transmitted independently m each of the optical channels using a light beam within an assigned wavelength band, typically generated by narrow wavelength band optical sources such as lasers or light emitting diodes.
  • Each of the light sources is modulated with data and the resulting modulated optical outputs for all of the different wavelength bands are multiplexed, coupled into the optical fiber and transmitted over the fiber.
  • the modulation of the narrow wavelength band light corresponding to each channel may encode a simple digital data stream or a further plurality of communication channels defined by TDM. Little interference will occur between the channels defined withm different wavelength bands.
  • each of the WDM channels terminates m a receiver assigned to the wavelength band used for transmitting data on that WDM channel. This might be accomplished in a system by separating the total received light signal into different wavelengths using a demultiplexer, such as a tunable filter, and directing the separated narrow wavelength band light signals to receivers assigned to the wavelength of that particular channel.
  • a demultiplexer such as a tunable filter
  • Wavelength stability may also affect the operational charactenstics of the WDM system.
  • the expense of WDM systems limits the application of this technology.
  • One embodiment of a WDM fiber optic communication system is desc ⁇ bed in U.S. Patent No. 5,579,143 as a video distribution network with 128 different channels.
  • the 128 different channels are defined using 128 different lasers operating on 128 closely spaced but distinct wavelengths. These lasers have precisely selected wavelengths and also have the well-defined mode structure and gam charactenstics demanded for communications systems.
  • embodiments of the present invention can provide a video dist ⁇ bution network like that desc ⁇ bed m
  • U.S. Patent No. 5,579,143 and embodiments of the invention can provide other types of medium and wide area network applications, making such systems both more flexible and more economical.
  • embodiments of the present invention may be sufficiently flexible and cost effective to be used in at least some types of local area networks.
  • Embodiments of the present invention use spread spectrum communication techniques to obtain improved loading of the bandwidth of an optical fiber communication system in a more cost-effective manner than known WDM systems.
  • Spread spectrum communication techniques are known to have significant advantages and considerable practical utility, most notably in secure military applications and mobile telephony.
  • spread spectrum techniques most notably code-division multiple access (CDMA)
  • CDMA code-division multiple access
  • Spread spectrum techniques are desirable in optical communications systems because the bandwidth of optical communications systems, such as those based on optical fibers, is sufficiently large that multi-dimensional coding techniques can be used without affecting the data rate of any elect ⁇ cally generated signal that can presently be input to the optical communications system.
  • Different channels of data can be defined in the frequency domain and independent data streams can be supplied over the different channels without limiting the data rate within any one of the channels.
  • the WDM system desc ⁇ bed above might be considered a limiting case of a spread spectrum system m that plural data channels are defined for different wavelengths.
  • the different wavelength channels are defined in the optical frequency domain and time domain signals can be transmitted over each of the wavelength channels.
  • the distinct wavelength channels of the WDM communication system desc ⁇ bed above provide a t ⁇ vial, single position code, where individual code vectors are orthogonal because there is no overlap between code vectors.
  • optical CDMA systems that are generally similar to traditional forms of radio frequency CDMA, for example in Kavehrad, et al., "Optical Code- Division-Multiplexed Systems Based on Spectral Enodmg of Noncoherent Sources," Lightwave Tech.. Vol. 13, No. 3, pp. 534-545 (1995).
  • the suggested optical CDMA system uses a broad-spectrum source and combines frequency (equivalently, wavelength) coding in addition to time-domain coding.
  • FIG. 1 A schematic illustration of the theoretical optical CDMA suggested in the Kavehrad article is presented m FIG. 1.
  • the suggested optical CDMA system uses a broad spectrum, incoherent source 12 such as an edge-emitting LED, super luminescent diode or an erbium-doped fiber amplifier.
  • the broadband source is modulated with a time- domain data stream 10.
  • the time domain modulated broad-spectrum light 14 is directed into a spatial light modulator 16 by a mirror 18 or other beam stee ⁇ ng optics.
  • light beam 20 is incident on a grating 22, which spatially spreads the spectrum of the light to produce a beam of light 24 having its va ⁇ ous component wavelengths spread over a region of space.
  • the spatially spread spectrum beam 24 is then incident on a sphe ⁇ cal lens 26 which shapes and directs the beam onto a spatially patterned mask 28, which filters the incident light
  • Light spatially filtered by the mask 28 passes through a second sphencal lens 30 onto a second diffractive grating 34, which recombines the light.
  • Mask 28 is positioned midway between the pair of confocal lenses 26, 30 and the diffraction gratings 22, 34 are positioned at the respective focal planes of the confocal lens pair 26, 30
  • the broad optical spectrum of the incoherent source is spatially expanded at the spatially patterned mask 28 and the mask spatially modulates the spread spectrum light. Because the spectrum of the light is spatially expanded, the spatial modulation effects a modulation in the wavelength of the light or, equivalently, in the frequency of the light.
  • the modulated light thus has a frequency pattern charactenstic of the particular mask used to modulate the mask. This frequency pattern can then be used to identify a particular user withm an optical network or to identify a particular channel within a multi-channel transmission system.
  • the spatially modulated light After passing through the mask 28, the spatially modulated light passes through the lens 30 and the wavelength modulated light beam 32 is then spectrally condensed by the second grating 34.
  • the wavelength modulated and spectrally condensed light beam 36 passes out of the spatial light modulator 16 and is directed by mirror 38 or other beam steenng optics into a fiber network or transmission system 42.
  • the portion of the CDMA system desc ⁇ bed to this point is the transmitter portion of the system and that portion of the illustrated CDMA system down the optical path from the fiber network 42 constitutes the receiver for the illustrated system.
  • the receiver is adapted to identify a particular transmitter within a network including many users.
  • a particular user with the illustrated transmitter selects a particular receiver or user to receive the transmitted data stream by alternateng the spatial pattern of the mask 28, and hence the frequency coding of the transmitted beam 40, so that the transmitter mask 28 corresponds to a spatial coding charactenstic of the intended receiver.
  • the receiver illustrated in FIG. 1 detects data transmitted from a particular transmitter by detecting the frequency or wavelength modulation charactenstic of the transmitter mask 28 and rejecting signals having different charactenstic frequency modulation patterns.
  • Light received from the optical fiber network 42 is coupled into two different receiving channels by coupler 44.
  • the first receiver channel includes a spatial light modulator 46 identical to the spatial light modulator 16 and the second receiver channel includes a spatial light modulator 48 of similar construction to the transmitter's spatial light modulator 16, but having a mask the "opposite" of the transmitter mask 28
  • Each of the spatial light modulators 46, 48 performs a filtenng function on the received optical signals and each passes the filtered hght out to an associated photodetector 50, 52.
  • Photodetectors 50, 52 detect the filtered hght signals and provide output signals to a differential amplifier 54.
  • the output of the differential amplifier is provided to a low pass filter 56 and the onginally transmitted data 58 are retrieved.
  • FIG. 2 provides an illustration of the receiver circuitry in greater detail.
  • spatial light modulators 46 and 48 are generally similar to the spatial hght modulator 16 shown in FIG. 1 and so individual components of the systems are not separately descnbed Received light 60 is input to the receiver and is split using coupler 62, with a portion of the light directed into spatial light modulator 46 and another portion of the hght directed into the other spatial light modulator 48 using mirror 64.
  • Spatial light modulator 46 filters the received light 60 using the same spatial (frequency, wavelength) modulation function as is used in the transmitter's spatial light modulator 16 and provides the filtered light to photodetector 50.
  • Spatial hght modulator 48 filters the received light using a complementary spatial filtenng function and provides the output to the detector 52.
  • Amplifier 54 provides subtracts the output signals from the two photodetectors.
  • the spatial light modulator 46 includes a mask 66 identical to the transmitter mask 28.
  • Spatial light modulator 48 includes a mask 68 that performs a filtenng function complementary to masks 28 and 66 so that spatial light modulator 48 performs a filtenng function complementary to the filtenng function of spatial light modulators 16, 46.
  • each of these masks 16, 66, 68 is a liquid crystal element so that the masks are fully programmable.
  • RF CDMA techniques are not readily applicable to optical systems m which an incoherent light source and direct detection (i e , square-law detection of the intensity using photodetectors) are employed, because such optical systems cannot detect phase information. Code sequences defining negative symbol values cannot be used in such optical systems. As a result, only unipolar codes, i e , code sequences of 0 and 1 values, can be used for CDMA in a direct-detection optical system.
  • the Kavehrad article suggests the adaption of va ⁇ ous bipolar codes for the masks within the system illustrated m FIGS.
  • the Kavehrad article indicates that the bipolar code of length N must be converted into a unipolar code sequence of length 2N and that a system including such codes could support a total of N-l users.
  • the Kavehrad article addresses only a theoretical application of a CDMA system, with little discussion of the implementation of such a system.
  • the transmitter 80 employs a broad spectrum light source 82 which is split by a beam splitter 84 into two beams 86 and 88 to be processed by two spatial light modulators 90 and 92.
  • the first spatial light modulator 90 compnses a dispersion grating 94 to spectrally disperse the light beam 86 and a lens 96 to direct the dispersed light onto a first spatial encoding mask 98 which selectively passes or blocks the spectral components of the light beam.
  • Lens 100 collects the spectral components of the spatially modulated light beam and recombination grating 102 recombines the spread beam into encoded beam 104.
  • the "pass" and “block” state of the encoding masks represent a sequence of 0's and 1 's, ⁇ e , a binary, unipolar code.
  • the code 106 for the first mask 98 has a code U®U*, where U is a unipolar code of length N, U* is its complement and ' V denotes the concatenation of the two codes.
  • the second encoder 92 (details not shown) is similar in structure to the first encoder 90 except that its encoding mask has a code U*®U.
  • Symbol source 108 outputs a sequence of pulses representing 0's and l's into a first ON/OFF modulator 110 and through an inverter 112 into a second ON/OFF modulator 114.
  • the two modulators 110 and 114 modulate the two spatially modulated beams of light and the two beams are combined using a beam splitter 116 to combine the two encoded light beams 118 and 120.
  • the modulated light beams are alternately coupled to the output port depending on whether the bit from the source is 0 or 1.
  • This system can then use a receiver with differential detection of two complementary channels, as illustrated in the receiver of FIG. 2.
  • the receiving channels are equipped with masks beanng the codes U*®U and U®U*, respectively, and sequences of 0's and l's are detected according to which channel receives a signal correlated to that channel's mask.
  • the system proposed in the Young patent allows the use of the bipolar codes developed for RF CDMA technologies to be used in optical CDMA systems.
  • N codes can be defined since the code U and its complement U* must be concatenated on the mask. Therefore, it is an object of the invention to provide a frequency-domain CDMA encoding/decoding scheme and an optical communication system incorporating such a scheme where the number of users is maximized without raising interference unduly.
  • the throughput of an optical fiber based communication system is defined as the product of each user's data rate times the number of user pairs.
  • the throughput of an optical fiber communication system is a function of the optical source power of the users, the optical source bandwidth, user data rate, the number of users and the desired bit error rate (BER).
  • BER bit error rate
  • the limiting factor is the user-to-user interference, which is independent of the optical source power. Such interference imposes a maximum data rate at which the users may transmit information. It is an object of the present invention to increase the system throughput of spread spectrum CDMA communications systems.
  • a spatial encoder with binary or analog encoding and a decoding receiver or decoder.
  • a broad-spectrum light source is modulated with data to be transmitted.
  • the modulated light beam is then spatially dispersed, for example using a diffraction grating, and passed through a spatial spectrum-codmg mask.
  • the spatial coding mask preferably embodies a unipolar code belonging to a set of unipolar codes that are preferably denved from a set of balanced bipolar orthogonal codes.
  • the dispersed frequencies of the encoded modulated light beam are then recombmed to provide a modulated, encoded spread spectrum optical signal for injection into an optical fiber or another optical communication system.
  • a beam separator which is in some particularly preferred embodiments a polanzation insensitive splitter, diverts part of the beam in the fiber through a diffraction grating to spatially separate the spectrum of the light in the fiber.
  • the spatially spread signal potentially comp ⁇ sing of many distinct spread spectrum optical communication channels, is passed to a receiver providing signal recovery.
  • the optical signal is converted to an elect ⁇ cal signal by differential detection, the resulting electrical signal is preferably low pass filtered and then, in particularly advantageous embodiments, the electrical signal is provided to a limiting element that removes the negative components of the elect ⁇ cal signal.
  • the differential detection of the receiver can be implemented m a number of ways.
  • the masks in the encoder and decoder include unipolar binary codes comp ⁇ sing 0's and l's such as Walsh codes.
  • the spatially spread light will pass through two decoding masks.
  • One decoding mask is the same as the encoder mask while the other decoding mask is the bit-wise complement of the encoder mask, or otherwise the complement of the encoder mask if the code is, for example, analog.
  • the spatially spread decoded light signals are combined, and the two channels of optical signals are preferably converted to electncal signals by differential detection.
  • the spatially spread light can be detected by an anay of detectors.
  • Each detector m the array measures the light power of the corresponding optically spread wave length and outputs a corresponding a ⁇ ay of electncal signals.
  • the array of electncal signals will then be processed by a digital signal processor (DSP).
  • DSP digital signal processor
  • the digital signal processing includes multiplying the signal from each detector m the array by a positive or negative one depending on whether the encoder mask bit is a one (transparent) or a zero (opaque).
  • the resulted bit products are then summed before thresholding for data recovery.
  • This digital processing corresponds to multiplying the signal from individual detectors in the array by the corresponding bit in a Hadamard code, which is the bipolar version of the Walsh encoder code.
  • some embodiments of the present invention provide plural broad band light sources.
  • a particularly desirable and particularly economical implementation of multiple sources having desirable spectral similanties is to provide a single onginatmg light source that is coupled to a fiber, where the output of the source is split, amplified. Each of the split and amplified sources is then split and amplified again, and this process is repeated a sufficient number of times to provide a sufficient number of sources for the many user system.
  • Particularly preferred embodiments decorrelate the different sources, whether generated m this manner or in another that provides at least somewhat correlated sources, by providing delays of different duration along the optical paths between the sources and the corresponding encoders of the system.
  • Another method of reducing interference is the use of a data modulation scheme that limits the amount of time that the source is maintained in an on state.
  • Sources may be directly modulated or may be modulated by passing the source light through an element that can modulate the source.
  • modulation is accomplished so that a light pulse of predetermined intensity is provided to the optical system when one binary value is to be transmitted and no light is provided to the optical system when the other binary value is to be transmitted.
  • FIG. 1 illustrates a conventional optical fiber mediated CDMA communication system.
  • FIG. 2 provides a more detailed view of one receiver configuration that might be used in the system of FIG. 1.
  • FIG. 3 illustrates an encoder for using bipolar codes in an optical CDMA system.
  • FIGS. 4 & 5 present different configurations of an optical fiber network according to the present invention.
  • FIG. 6 is a block diagram of a first embodiment of an encoder according to the present invention.
  • FIG 7 is a block diagram of a first embodiment of a decoder according to the present invention.
  • FIG. 8 is a block diagram of a second embodiment of a decoder according to the present invention.
  • FIG. 9 is a sketch of a liquid crystal mask for use m a third embodiment of an encoder according to the present invention.
  • FIGS. 10A, B and C are continuous representations of discrete transparency functions for the mask of FIG. 9.
  • FIG. 11 is a graphical representation of a Fou ⁇ er transform of light received from the fiber.
  • FIGS. 12A and B schematically illustrate an encoder and a decoder according to a third embodiment of the invention.
  • FIGS. 13 A, B and C present a graphical representation of a mask and mask functions according to a third embodiment of the invention.
  • FIG. 14 schematically illustrates an apparatus for generating an anay of N broad- spectrum optical sources having sufficient intensity to generate light beams for N channels of communication over a fiber using methods in accordance with the present invention.
  • FIG. 15 schematically illustrates a polanzation insensitive beam separator that is preferred in accordance with prefened embodiments of the present invention.
  • FIG. 16 illustrates in greater detail the optical detection circuitry schematically illustrated m FIG. 7.
  • FIG. 17 illustrates a modification to the source generation mechanism of FIG. 14.
  • FIG. 18 illustrates a set of data streams (a)-(c) that might be used to modulate a source in accordance with aspects of the present invention.
  • FIG. 1 illustrates a circuit that may be used to generate a pulse stream such as that illustrated in FIG. 18(b) or 18(c) from a data stream such as that illustrated in FIG. 18(a).
  • Particularly preferred embodiments of the present invention provide an optical fiber communications system using spread spectrum code division multiple access techniques to achieve better bandwidth utilization
  • the particular codes used in the most preferred embodiments of the present invention utilize one or more techniques for decorrelating noise signals or other reducing the interference between different users. Different techniques might be used to accomplish this result, with such techniques being used either individually in or combination with each other.
  • Certain particularly preferred embodiments of the present invention use more than one of the techniques descnbed herein m combination because certain of the techniques are sufficiently independent as to provide additive benefits.
  • a particularly desirable and particularly economical implementation of multiple sources having desirable spectral similanties is to provide a single originating light source that is coupled to a fiber, where the output of the source is split, for example into four components by a star splitter. Each of the split off components are then amplified to an appropnate level and then each of the split off and amplified components is provided to a separate start splitter.
  • a hierarchical structure of an onginal source that is split and amplified, with each successive source channel being split and amplified, can be used to develop a great many sources having essentially identical spectral charactenstics.
  • a difficulty observed by the present inventors when implementing this source strategy is an undesired level of temporal correlation between the different sources.
  • This level of correlation can give nse to undesirable levels of correlation between the different communication channels associated with the different sources. Consequently, preferred embodiments decorrelate the different sources.
  • Such optical delays could consist of optical delay lines.
  • Causing each of the sources to pass through different lengths of fiber delay lines might provide appropnate delays. Delays might alternately be generated using free space propagation through different optical paths. Fiber delays are preferred since they can be implemented using only minimal space, so that the overall optical system can be provided in a sufficiently small space as to allow a wider range of implementations for systems embodying this aspect of the present invention.
  • Time domain modulated data are provided to the optical communication system by modulating the sources.
  • Sources may be directly modulated or may be modulated by passing the source light through an element that can modulate the source.
  • modulation is accomplished so that a light pulse of predetermined intensity is provided to the optical system when one binary value is to be transmitted and no light is provided to the optical system when the other binary value is to be transmitted.
  • each clock cycle defines a data penod and the data can consume some or all of the clock cycle. If all of the clock cycle is consumed by the data, then the duty cycle is said to be 100%. If the data consumes only half of the clock cycle, then the duty cycle is said to be 50%. In particularly preferred embodiments of the present invention, it is prefe ⁇ ed that the duty cycle be reduced to a low but still detectable level, generally using a duty cycle of less than 50%. This has the effect of reducing the total optical signal that is present within the optical fiber system at any point in time. In other words, the use of shortened duty cycles reduces the amount of light within the system, thereby reducing the noise signals and the amount of interference expe ⁇ enced by a desired signal. Circuitry exists for reducing duty cycles considerably. As a practical matter, however, the reduction m duty cycle must be limited in extent so that the optical signal remains detectable.
  • Signals within the two channels of a receiver are preferably detected in a differential fashion, for example by coupling the light from each channel to different ones of a pair of photodiodes in a back-to-back configuration.
  • the electncal output from the photodiodes will then be a difference measurement of the signal received in the two channels.
  • the electncal output signal is low pass filtered and then provided to an electncal square law circuit element such as a diode. This square law element or limiter preferably removes the negative going portions of the received electncal signal and might also be used to amplify the positive going portions of the received electncal signal.
  • FIG. 4 illustrates the architecture of an exemplary optical communications system in which the present invention may be applied.
  • a plurality of pairs of users s ⁇ , s 12 , s 2 may be applied to an optical fiber medium 130.
  • s N1 may be proximately located and coupled to the fiber 130 in a star configuration
  • the second group of users s, 2 , s 22 , . . . s N2 may be proximately located but remote from the first group and coupled to the fiber 130 in a star configuration.
  • the users in the first group or the second group or both may be coupled to the fiber 130 at separate and distributed points, as shown m FIG. 5.
  • the architecture of FIG. 4 may be more appropnate, for example, for a fiber backbone, whereas the architecture of FIG. 5 may be more appropnate for a telephone system.
  • Pairs of users s_,,, s j2 communicate with each other using a channel of the optical fiber, and different pairs of users may simultaneously communicate over the same optical fiber.
  • Each pair of users (S j ,, s j2 ) is assigned a code u, for transmitting and receiving data between the two users, and different pairs of users are preferably assigned different codes.
  • the transmitting user in a user pair e.g. s, shall encodes the optical signal using the code U j assigned to the user pair (s jb s j2 ), and the receiving user s j2 m the pair decodes the optical signal using the same code u r
  • This architecture may be used, for example, for a fiber optic backbone of a communication network.
  • the embodiments of the present invention are descnbed as they may be applied in this network environment; other system architectures in which the invention is also applicable are descnbed later.
  • FIG. 6 shows a first embodiment 140 of a CDMA modulator/encoder.
  • a broadband light source 142 such as a super luminescent diode (SLD) or erbium-doped fiber source (EDFS)
  • SLD super luminescent diode
  • EDFS erbium-doped fiber source
  • the optical modulator modulates the hght from the optical source 142 based upon data or other information from the data source 146, using, for example, keying or pulse code modulation Encoder 150, which is similar to the spatial light modulator 16 shown in FIG. 1 with the exception of the mask and coding scheme, then spatially encodes the modulated broad-spectrum hght beam.
  • the encoder 150 includes a diffraction grating 152 that spatially spreads the spectrum of the modulated light beam along an axis.
  • the spatially spread light beam is colhmated by a collimatmg lens 154 and then the collimated beam is passed through the encoding mask 156.
  • the encoding mask provides a spatially encoded, modulated beam of light that is collected by collimatmg lens 158 and combined back to a broad spectrum beam by a diffraction grating 160 for injection into the fiber 162, which may be a single mode optical fiber.
  • An optical coupler 164 such as a star coupler, a Y coupler or the like is used to couple the encoded beam into the fiber 162.
  • the light beam may be first encoded with the encoder 150 and then modulated by the modulator 144.
  • FIG. 7 shows a compatible decoder, which has two channels 170 and 172.
  • Light signals containing a potential plurality of spread spectrum signals are diverted from the fiber 162 using an optical coupler (not shown), and split into two beams through a beam separator 174.
  • the beam separator is most preferably a polanzation insensitive element like that illustrated in FIG. 15 and discussed below with reference to that figure.
  • One incoming beam is spread spatially along an axis by a diffraction grating 176 and is then colhmated by a collimatmg lens 180 before being passed through a detection or decoding mask 184.
  • the decoding mask 184 is, in this illustrated preferred embodiment, identical to the encoding mask 156.
  • this second decoding mask 188 is the bit-wise complement of the encoder mask 184.
  • the beam after being passed through the second decoding mask 186, is passed through the collimatmg lens 190 and a diffraction grating 194 to remove the spatial spreading.
  • the output of the first decoder channel 170 may then be supplied to a photodetector 196 to convert the light into an electncal signal.
  • the output from decoder channel 172 is supplied to a photo detector 198 to convert the light into an elect ⁇ cal signal.
  • the two elect ⁇ cal signals are then subtracted by the back-to-back anangement of the two detector diodes, 196 and 198 for being supplied to data and clock recovery hardware and/or software 200.
  • the two electncal signals may also be separately processed by two gam control circuits, respectively, to adjust for different losses in the two detector channels 170 and 172, before a difference calculation is performed.
  • the differential electncal signal is then detected for data recovery.
  • Data recovery for digital data streams may include, for example, integrating and square-law detecting the difference signal.
  • Data recovery for analog signals provided by analog code mask embodiments of the invention may include, for example, low-pass filtenng the difference signal.
  • FIG. 8 shows another embodiment of the decoder 210
  • the beam of light received from the fiber is not split into two channels with two masks, but is instead spread by the grating 212 and is colhmated by a lens 214.
  • the colhmated light is then intercepted by an a ⁇ ay of detectors 216.
  • the number of detectors in the array is equal to the number of bits in the encoder mask.
  • Each detector position corresponds to the encoder mask bit position.
  • the detector signal from each detector in the array is multiplied by either "1" or "- 1" depending on whether the corresponding encoder mask bit is a "transparent" or "opaque.” The results of all the multiplier outputs are then summed.
  • the sum is then compared with a threshold 218 for data recovery.
  • This digital processing can be performed in discrete logic hardware or in a DSP 220 using software
  • the outputs of the detectors may also be multiplied by numbers other than "1" or "-1". It should be noted that in both embodiments of FIGS. 6 and 7 only one encoder mask is used for transmitting data and no concatenated code is required in contrast with p ⁇ or art designs. The preferred encoding and decoding scheme according to the present invention is explained next.
  • unipolar codes means code sequences compnsing 1 's and 0's in the case of binary codes, or code functions having values between 0 and 1 in the case of analog codes
  • Bipolar codes means code sequences comp ⁇ sing -l's and l's in the case of binary codes, or code functions having values between -1 and 1 in the case of analog codes.
  • a complement of a unipolar binary code u is (1-u), i.e. its bit-wise complement in which 0's are substituted by l's and l's are substituted by 0's.
  • a complement of a unipolar analog code f is (1-f).
  • Unipolar binary codes are used as an example in the following descnption.
  • the basic requirement for a spectral encoding/decoding scheme is that the decoding apparatus at a receiving user be able to recover data signals from the conespondmg transmitting user while reducing or eliminating interference from signals from all other users.
  • the receiving masks will be fixed as a particular receiver always receives the same channel of data.
  • the receiving masks will be programmable so that different signal sources can be selected from the many possible sources.
  • a spread spectrum CDMA system using an incoherent light source because an incoherent optical system can only transmit positive signals (light intensities), and no phase information is available, only unipolar codes may be used for encoding.
  • the number of digits in the sequence, N is referred to as the length of the code.
  • each of the code values corresponds to a fixed interval slot, either transparent or opaque, on the spatially patterned mask that in turn corresponds to a fixed frequency or wavelength interval in the spatially modulated broad spectrum beam of light.
  • the codes are preferably chosen such that they are orthogonal, or:
  • each transmitting user may transmit signals using a single encoding mask, and the corresponding receiving user may use a single decoding mask identical to the encoding mask to recover the signal from the corresponding transmitting user while rejecting mterfenng signals from all other users.
  • This desirable outcome occurs only when the codes are chosen to as the binary basis vectors:
  • This set of codes is undesirable in that, since only one digit of the entire code is 1 , only one frequency bin of mask passes power through it while the great majo ⁇ ty of the bins are blocked.
  • Such a system can be viewed as an incoherent wave division multiple access (WDMA) system.
  • WDMA wave division multiple access
  • a set of unipolar codes may be used such that although a code u, in the set is not orthogonal to other codes u, in the set according to the definition of orthogonality set forth above. Rather, the code u, is selected to be orthogonal to the difference between any other code u, and its complement u *, ⁇ e.
  • the decoders of embodiments of FIGS. 7 and 8 implement the p ⁇ nciple of Eq. (2).
  • the received light beam at a user j contains signals from all transmitting users l encoded with codes u,.
  • the first channel 170 having the mask 56 generates a light beam representing u,»U j
  • the second channel having the complementary mask 172 generates a light beam representing u, «U j *
  • the differentially arranged detectors 62 and 63 generates the difference signal u,*(u J -u J *).
  • the array of detectors 73 outputs signals representing u food and the DSP 74 calculates ⁇ •(U j -u,*) based on the outputs of the detector array 73.
  • the difference signal U,*(U J -U J *) is non-zero only for the signal from the user that uses a mask having a code u,. Consequently, such decoders are able to recover the signals from the transmitting user l and reject signals from all other users.
  • a set of unipolar code that satisfy Eq. (2) may be denved from a set of balanced bipolar binary orthogonal codes v, that satisfy the following conditions:
  • the bipolar code v is "balanced" in that they have equal numbers of l's and -l's (eq. (4)). These particularly preferred unipolar codes u, thus have equal numbers of 1 's and 0's. As a result, half of the light power may be transmitted as signals, thereby promoting the efficient utilization of the source power.
  • a Hadamard matnx is a square matnx the elements of which are l's or -l's such that all rows are orthogonal to each other and all columns are orthogonal to each other.
  • a 4x4 Hadamard matnx may be:
  • the column (or row) vectors except the first column (or row) of a Hadamard matnx provide a set of balanced bipolar binary orthogonal codes satisfying Eqs. (3) and (4).
  • a set of unipolar codes u tract u 2 , . . ., u n used m the uni-bipolar spread spectrum CDMA system prefened m accordance with the present invention may be constructed by first constructing a Hadamard matnx of size n+1 or greater. Except the first column (or row), every column (or row) of this Hadamard matrix may be used to generate a unipolar code u, by replacing all -1 's with 0's.
  • the above 4x4 Hadamard matnx may be used to generate the following codes:
  • Hadamard matnces having a size N that is a power of 2 may be constructed from H 2
  • Eqs. (3) and (4) indicate that the bipolar code set used to generate the unipolar codes should be orthogonal and balanced, in practice, it may be acceptable although not desired to use code sets that are "near orthogonal" or "near balanced.”
  • a code set is near orthogonal when, for example, u. ⁇ U j (I ⁇ J) is substantially smaller than u,»u,.
  • the codes are near balanced when, for example, u,» 1 is substantially smaller than N. For example, when the length N of the codes is large, changing a few digits of some codes in the set may result in a near orthogonal or near balanced code set.
  • the coding masks 156, 184, 186 in FIGS. 6 and 7 may be either transmissive or reflective. As a practical matter, however, the present inventors have observed that reflective masks are harder to make and do not usually have a desirably large extinction ratio.
  • the masks are made of liquid crystal matenal as shown in FIG. 9 divided into a plurality of cells "a" through "L", with L an arbitrary integer and being the maximum permitted length of the code.
  • Such LCD masks are commercially available or are readily made using known technology.
  • the cells form a one-dimensional anay arranged along the axis 230 of spatial spectrum spreading caused by the diffraction grating 152.
  • the control of the cells is analog, meaning that the opacity of each cell is either infinitely adjustable or is adjustable m at least three or more separately controllable stages. Preferably a large number of finite stages, preferably sixty-four or greater levels of opacity should be used.
  • the control is binary, and Walsh codes (unipolar Hadamard) are used. These masks can be implemented by LCD pixel a ⁇ ays or by a photonic integrated circuit such as a solid state amplifier a ⁇ ay. Alternately, and presently preferred for systems where multiplexing of signals onto a fiber is most desirable, the masks may be fixed and formed on glass blanks. Such fixed masks are most preferably binary masks embodying unipolar Hademard codes.
  • the glass may be BK7 or quartz and the reflective regions could be gold.
  • the glass may still be BK7 or quartz and the blocking regions could be chrome.
  • masks are on the order of one to two inches across so that readily available technology can be used to define a mask having 128 different, equal sized and contiguous positions on the mask, as is presently contemplated for an OC-12 application of the present invention. Masks with finer granulanty with 256 or 512 positions are readily defined using available technology.
  • Eqs. (2) - (4) which are illustrated m the context of binary codes, apply equally to analog codes.
  • the wavelet functions are discrete harmonic spatial sine waves (represented for purposes of illustration as continuous functions) as shown in FIG. 5.
  • the ordmate axis is the axis along which the frequencies of the beam are spread and the abscissa is the relative transparency of the beam passing through a cell.
  • a first encoder mask transparency function shown in FIG. 10A may have a spatial frequency of 1/L, where L is the number of cells.
  • the mask of that first encoder is a discrete (as opposed to continuous) cosine wave m terms of transparency having one cycle over the frequency spectrum of L, such that the lowest and highest frequency portion of the encoded spectrum have the maximum intensity and the mid-range spectral frequencies have the lowest intensity.
  • a second encoder mask may for example have a spatial frequency intensity mask of twice the frequency of the first encoder with two full cycles across the length of the encoder L of FIG. 10B.
  • Still further a third encoder may have a frequency three times the frequency of the first encoder as shown in FIG. IOC.
  • the maximum number of codes should be over one hundred and preferably over several hundred for higher usage systems.
  • the maximum number of harmonics or Walsh code bits (and therefore, the maximum number of codes) is limited only by the number of cells in the mask. For the analog mask, the number of different levels of opacity permitted m the mask, results in the quantization noise in the encoder.
  • Chebyshev polynomials could also be used as they are orthogonal with respect to each other.
  • cosme waves for the encoding function also permits an easier decoder design.
  • the received signal can be separated through a spatial filter for the frequency of the desired signal and then that signal can be recovered.
  • FIG. 11 shows the Fou ⁇ er transform of a signal received from a fiber where the separate encoded signals include 1 L, 2 L, 4/L and 8/L. Any one of these signals may be readily obtained by filtenng for that particular spatial frequency m the received signal.
  • an alternative method may be used for modulating signals using two codes as is shown in FIG. 12 A.
  • the optical path for the spatially spread light source 240 is switched between a first mask 242 and a second mask 244, which is complementary to the first mask 242, by a switcher 246 responsive to data from a data source 248, the first mask encoding the light to provide a digital "one" signal and the second mask encoding the light to provide a digital "zero" signal for the same code channel.
  • the modulator switches the light path between two different encoder masks using one liquid crystal in a manner similar to the binary mask receiver embodiment.
  • the light from both masks is then summed by a summer 250 and then provided to the optical communications channel such as a optical fiber (not shown).
  • Receiving data proceeds m the converse manner as shown in FIG. 12B.
  • a decoder 260 receives light from the communications channel and generates the spatially spread spectrum of the received light with receiving input optics 262 through masks 264, 266 which are identical to the mask 242 and the mask 244, respectively.
  • the light from the masks 264 and 266 is then provided to a differential receiver 268 in the manner descnbed above m the binary receiver embodiment.
  • the signal from the receiver 268 may then be processed by a digital signal processor 270 for recovery of the data.
  • FIG. 13A shows one alternative embodiment of the masks appropnate for coding where two different masks are used for transmitting ones and zeros.
  • the mask formed of L cells m a liquid crystal mask 280 is divided into four parts, 282, 284, 286 and 288.
  • Parts 282 and 284 compnse L/2 cells each along a first linear array arranged along the axis of spreading of the spectrum on a first row to encode a "one" for this particular code channel and at a second column, cells 286 and 288 also compnse L/2 cells ananged along the same axis for encoding a "zero" for this same channel.
  • the discrete transparency functions for parts 282, 284 are the complements of each other such as shown in FIG. 13B, where the ordmate represents spatial frequency and the abscissa represents intensity.
  • the ordmate represents spatial frequency
  • the abscissa represents intensity.
  • the complements of the discrete intensity functions for parts 286 and 288 are reversed.
  • the portion of the mask in section 282 is identical to the portion of the mask in 288 and the portion of the mask in 284 is identical to the portion of the mask m 286.
  • first portion 282 of the mask is the orthogonal wave function and the second half is all opaque for a "zero" 284 and the second level, the first half 286 is all opaque and the second half is the same pattern as the first half 282 to make a "one.”
  • first halves 282, 286 can be a first polynomial such as a sine wave and the second halves 284, 288 can be a second polynomial such as a Chebyshev function.
  • optical systems 150, 170 and 172 in the encoder of FIG. 6 and decoder of FIG. 7 may be generally refe ⁇ ed to as optical chambers.
  • An optical chamber which may be a set of discrete optics or an integrated optical device, spectrally encodes an input broad band optical signal by selectively attenuating the spectral components of the signal according to a "code.”
  • the code which may be binary or analog, determines the degree of attenuation of each spectral components of the input signal.
  • the optical chambers are implemented with diffraction gratings, collimatmg lenses and an optical mask having a code, but other implementations are also possible.
  • encoders and decoders could also be applied to analog modulation of the optical signal.
  • CDMA techniques have been descnbed above, those of ordinary skill m the field will readily understand that depending upon system parameters, the system may also be used with wavelength (frequency) division multiplexing and time division multiplexing. For example, different coding schemes may be used for different portions of the optical spectrum so that wavelength division multiplexing may be used.
  • the codes may be shared on a time shanng basis to provide for time division multiplexing.
  • optical spatial (frequency domain) CDMA can be combined with time-domain optical CDMA to increase the number of codes and the users in the network.
  • time domain spread spectrum embodiments several users are provided with different time domain spread spectrum codes for encoding the data before the data is provided to the optical encoder. However, these users can share the same wavelength encoding schemes discussed above. Of course, at the decoder, once the received optical information is converted back into the electncal digital domain, the digital signal must be processed according to the time domain spread spectrum code to recover the desired transmitted information.
  • vanous network algo ⁇ thms may also be implemented.
  • the present invention may be applied to vanous fiber communication system architecture, such as a network environment shown in FIG. 5, in which a plurality of users s su s 2 , . . . s N are connected to an optical fiber medium 130 and each user s ; may communicate with any other user s, over the optical fiber.
  • Each user or node s is assigned a code U j for receiving data from other users, and different users are preferably assigned different codes.
  • any one node may be assignable from one or more master nodes distributed throughout the network. Hence, when a node in a network comes on line, it requests a code or codes for encoding for selecting one of the possible spread spectrum channels over which to communicate. When that node leaves the network, the code that had been used by that particular node may be reassigned to a different node in the network. Vanous schemes may be used for making such requests such as CSMA/CD technique or token passing on a permanently assigned channel.
  • token passing techniques may be used for gaining codes for secunng one of the code division channels.
  • the disclosed embodiments permit an increase in the number of simultaneous users.
  • the maximum number of simultaneous users that are permitted for the same number of codes is 2 N 2 where N is the maximum number of codes.
  • the maximum number of codes with holding everything else constant is 2 N .
  • total system throughput is dramatically increased, thereby permitting a system throughput of at least one half of a terabit, with the total system throughput being determined by the maximum number of simultaneous users, and the users data rate.
  • FIG. 14 illustrates a preferred apparatus for generating a plurality of broad-spectrum sources in a cost effective manner using a single erbium-doped fiber source and a hierarchy of erbium- doped fiber amplifiers to provide enough channels of sources, each with sufficient intensity for dnvmg a channel of the optical communications system.
  • a single erbium-doped fiber source 300 outputs light with an acceptably broad spectrum, generally providing a bandwidth of about 28 nanometers in wavelength over which the intensity of the source vanes by less than about 5 dB.
  • the 28-nanometer bandwidth corresponds to a system bandwidth of about 3.5 THz.
  • the output of the erbium-doped fiber source also known as a super luminescent fiber source, is provided over a fiber to a splitter such as a star coupler 302 which splits the input source signal and provides the output over four fibers to an anay of four fiber amplifiers 304.
  • the intensity drops m the expected manner.
  • Each of the four split off sources is thus amplified by the four fiber amplifiers to provide four broad-spectrum light beams preferably each having an intensity approximately equal to the o ⁇ ginal source 300 intensity.
  • this process is repeated through several further hierarchical stages.
  • the outputs from the four fiber amplifiers 304 are provided over fibers to a corresponding set of four splitters 306, which may also be star couplers.
  • the splitters 306 split the output from the fiber amplifiers into a plurality of outputs also of reduced intensity.
  • the split off output from the splitters 306 are then provided to a further array of fiber amplifiers 308, which preferably amplify the intensity of the plural channels of broad-spectrum light to provide a next set of source light beams 310 having an appropnate intensity.
  • This process is repeated until a sufficient number of broad-spectrum sources having an appropnate intensity are generated, for example 128 independent sources for the illustrative 128-channel fiber communication system.
  • This hierarchical arrangement is preferred as using a single ongmating source and a number of fiber amplifiers to obtain the desired set of broad-spectrum light sources, which advantageously takes advantage of the lower p ⁇ ce of fiber amplifiers as compared to the fiber source.
  • each of the 128 masks uses a 128-bm mask to spatially encode the input light signal, with each of the 128 masks presenting a different one of a unipolar Hadamard code vector generated m the manner discussed above.
  • each of the masks is a fixed mask for use in a transmission mode, with the mask having a total of 128 equal sized bins, with the bins spanning the usable width of the linear mask.
  • the 128 bins span a total of about 3.5 THz (28 nanometers) m bandwidth, with each adjacent bin defining a subsequent frequency interval providing about 25 GHz of bandwidth.
  • Each of the equal sized bins of the fixed mask is assigned according to the code vector to have one or the other of two binary values. One of the two binary values is identified by a blocking chrome stripe on the glass substrate of the mask and the other binary value is identified by an unblocked, transparent st ⁇ pe on the glass substrate.
  • Each of the 128 channels of the communication system is then defined by a distinct spatial encoding function and each of the channels is also modulated with a time-domain signal, for example using a modulator 144 like that shown in FIG. 6.
  • the vanous channels are modulated both spatially (equivalently, frequency) and temporally, the 128 channels are combined and injected into a fiber.
  • Long distance transmission for this fiber communication system is managed in a manner similar to the manner other conventional fiber communication systems are managed.
  • the signals on the fiber will undergo dispersion and losses. It is preferable that the signals on the fiber be amplified using a conventional fiber doped amplifier at regular intervals, for example, every forty to eighty kilometers.
  • the combined light signals are split, amplified, and provided to an array of 128 receivers, each corresponding to one of the fixed mask channels defined by the 128 transmitters coupled mto the fiber.
  • the pn ary purpose of the illustrated embodiment is to expand the usage or loading on the fiber, so the receivers also include fixed masks so that each receiver is dedicated to a single one of the 128 channels.
  • the receivers which may have the structure shown in FIG. 7, are each dedicated to a particular channel defined by a particular transmitter by including within the receiver one mask identical to the transmitter mask and a second mask that is the bit-wise complement of the transmitter mask.
  • va ⁇ able mask such as one using a programmable LCD element.
  • the use of fixed masks on both the transmitting and receiving ends of the communication system provides a reduced cost system that provides significantly improved bandwidth for a high volume fiber link.
  • FIG. 15 shows a beam separator that is preferably used at the input to the receiver.
  • a beam separator m accordance with the present invention is capable of separating the received light beam into two beams of sufficiently equal power levels to allow the preferred differential detection scheme of the optical CDMA receivers to effectively detect a desired user channel.
  • An embodiment of a polanzation insensitive beam separator might consist of a first polanzation sensitive element that divides the received light beam into first and second channels of light with each channel having a different one of two orthogonal polanzations.
  • one channel of light might include the vertically pola ⁇ zed component of the received light beam and the other channel might include the ho ⁇ zontally polanzed component of the received light beam.
  • the polanzation of one of the channels is then converted to the polanzation of the other light beam.
  • linearly polanzed light this might consist of rotating the polanzation of the hght.
  • the two channels of light are then recombmed and provided to a beam splitter.
  • This beam splitter is typically a polanzation sensitive element that accurately splits the combined beams into two beams of substantially equal power because the polanzation of the combined beams is well defined and predictable.
  • a specific embodiment is desc ⁇ bed m which light is received from a single mode fiber 350 Since the fiber 350 is generally not polanzation preserving and the light within the fiber 350 is likely linearly pola ⁇ zed in an arbitrary direction, it is convenient to use a conventional linear pola ⁇ zer as a beam splitter 352 or polanzation analyzer.
  • the polanzation sensitive element 352 preferably separates the input light beam into two orthogonal polanzation components and provides those two components to two different optical paths 354, 356. Generally different power levels will be present along each path.
  • the illustrated optical paths may propagate through free space or may proceed through polanzation preserving fibers. In either case, the polanzation of the light within each arm will be of a uniform polanzation until the polanzation is altered.
  • One component of the light is provided along optical path 354 and maintains a vertical linear polanzation 358 throughout the optical path 354.
  • the polanzation is initially honzontal 360 and then the polanzation is rotated by 90° by a rotation element 362 so that the polanzation of the second optical path's light becomes linear vertical as indicated at 364 in FIG. 15.
  • the rotation element may be a '/. waveplate or an appropnate Faraday rotator.
  • the rotation element 362 is most preferably effected by a mechanical rotation of the fiber by 90°. Most generally the rotation of the fiber will proceed continuously over a length of the fiber. Of course, it is possible to perform the rotation through other means, such as by inserting a rotation element at an end of the fiber of the second optical path.
  • the two beams on the two optical paths have had their pola ⁇ zations properly o ⁇ ented, the two beams are recombined and then split into a pair of substantially equal power beams to propagate along two additional beam paths.
  • a typical polanzation sensitive beam splitter 366 to divide the beams into two substantially equal power beams.
  • the two desired output beams are provided along optical paths 368 and 370 preferably through single mode optical fiber with linear polanzations in the illustrated embodiment.
  • the input fiber 350 of FIG. 15 may correspond to the input fiber 162 of FIG. 7 and the output beams along optical fiber paths 368, 370 (FIG. 15) correspond to the two optical paths shown propagating from element 174 of the FIG. 7 embodiment.
  • the split, received beams are then provided to the filtenng elements 170, 172 of FIG. 7 where the two channels are analyzed through the masks shown in FIG. 7.
  • the preferred electncal system illustrated schematically in FIG. 16, also provides a mechanism for reducing interference.
  • the subsystem illustrated m FIG. 16 provides further detail on the back-to-back diode arrangement indicated at 196, 198 m FIG. 7.
  • the two complementa ⁇ ly filtered optical signals are provided to the back-to-back diodes 196, 198, which effect both a square law optical detection but also a differential amplification function.
  • Other combinations of optical detectors, difference detection and elect ⁇ cal amplification are known and might well be substituted for these functions.
  • the electncal output signal 200 from the diode pair 196, 198 and is then low pass filtered by filter 380.
  • the low pass filtenng is performed to remove high frequency noise signals.
  • the filtenng might pass frequencies of 630-650 MHz.
  • the filtered electncal signal is then provided to an electncal square law circuit element 382 such as a diode.
  • This square law element or limiter preferably removes the negative going portions of the received elect ⁇ cal signal and might also be used to amplify the positive going portions of the received elect ⁇ cal signal.
  • the negative going portions of the elect ⁇ cal signal are immediately identifiable as noise and so can be removed to improve the signal to noise ratio of the overall system.
  • the elect ⁇ cal signal output from the limiter 382 is then analyzed to detect signals above a threshold value, which signals are recognized as transmitted ones.
  • a particularly desirable and particularly economical implementation of multiple sources having desirable spectral similanties is to provide a single onginatmg light source that is coupled to a fiber, where the output of the source is split, for example into four components by a star splitter. Each of the split off components are then amplified to an appropnate level and then each of the split off and amplified components is provided to a separate start splitter.
  • a hierarchical structure of an ongmal source that is split and amplified, with each successive source channel being split and amplified, can be used to develop a great many sources having essentially identical spectral charactenstics. Another method of reducing interference is to reduce the correlation between different ones of the noise signals.
  • a difficulty observed by the present inventors when implementing the source strategy shown in FIG. 14 is an undesired level of temporal conelation between the different sources.
  • This level of correlation can give nse to undesirable levels of correlation of noise sources or of co ⁇ elation between the different communication channels associated with the different sources. Consequently, preferred embodiments deconelate the different sources. This might be accomplished by inserting different optical delays along each of the output paths of the different source channels.
  • One simple mechanism for accomplishing this is illustrated in FIG. 18.
  • a large number of distinct sources 400-403 are defined, for example using the technique illustrated m FIG. 14 and discussed above, so that the sources provide similar optical outputs with similar spectral bandwidths and spectral power distribution. While four sources are shown, the system will typically include 128 or more total sources corresponding to 128 or more users.
  • the outputs of each of the sources 400-403 are passed through a delay to reduce the temporal correlation between the different sources.
  • Such optical delays could consist of optical delay lines or extended optical propagation paths. Causing each of the sources to pass through different lengths of fiber delay lines is the most preferred mechanism for providing appropnate delays. Delays might alternately be generated using free space propagation through different optical paths. Fiber delays are preferred since they can be implemented using only minimal space, so that the overall optical system can be provided in a sufficiently small space as to allow a wider range of implementations for systems embodying this aspect of the present invention. Refer ⁇ ng once again to FIG. 17, appropnate delays are effected by passing the output of each of the sources 400-403 through different lengths of single mode fibers 404-407.
  • the different length fibers are selected to impose a delay of between about one and about two or more times the data rate on successive sources. Considenng a data rate of approximately 622 Mbt sec, an appropnate delay can be fashioned by adding about one and a half feet of optical fiber (equivalent to -1.5 GHz) for each desired delay. Thus, for the first source 400, no addition fiber would be added as this represents the baseline. For the second source 401, 1.5 feet of additional fiber 405 would be included in the output path and for the third source 402, a three foot length of fiber 406 beyond the baseline length of fiber 404 is provided. Similarly, the output from source 403 is coupled through a fiber 407 that is about 4.5 feet ( ⁇ 4.5 GHz) longer than fiber 404.
  • Each of the users within a system which may total 128 users or more or equivalently might total 128 channels of multiplexed data, is provided with a source ongmatmg from a central source and delayed by an amount different from all of the other sources. It will of course be appreciated that different mechanisms for achieving optical delays are known and could be practiced to achieve similar results.
  • Time domain modulated data are provided to the optical communication system by modulating the sources.
  • Sources may be directly modulated or may be modulated by passing the source light through an element that can modulate the source.
  • modulation is accomplished so that a light pulse of predetermined intensity is provided to the optical system when one binary value is to be transmitted and no light is provided to the optical system when the other binary value is to be transmitted.
  • FIG. 6 A schematic example of the modulation of a source with a data stream is shown in FIG. 6.
  • a clock In a modulating data stream, there is typically a clock defining a data rate for modulated binary data and these binary data streams are typically charactenzed by a duty cycle.
  • vanous data streams (a)-(c) are shown on a background of clock cycle starts identified by the vertical dashed lines
  • each clock cycle defines a data penod and the data can consume some or all of the clock cycle. If all of the clock cycle is consumed by the data, then the duty cycle is said to be 100%. If the data consumes only half of the clock cycle, then the duty cycle is said to be 50%. This is shown in FIG. 18(a) and consists of an signal that may be "ON" as much as one half of the time.
  • the use of shortened duty cycles reduces the amount of light within the system, thereby reducing the noise signals and the amount of interference expe ⁇ enced by a desired signal.
  • Circuitry exists for reducing duty cycles considerably. As a practical matter, however, the reduction in duty cycle must be limited in extent so that the optical signal remains detectable.
  • the amplification of the input source or the amplification of the detection scheme must be increased in proportion to the reduction in the data duty cycle.
  • the noise floor associated with the amplifier then establishes the limit on how small the duty cycle might be reduced. The duty cycle cannot be reduced below the level at which amplifier noise comes to dominate the signal.
  • the data source (146 in FIG. 6) might be selected to provide data streams with the desired duty cycle charactenstics. On the other hand, it is typically preferable to provide greater flexibility so that any input data stream, for example the 50% duty cycle stream illustrated in FIG. 18(a), can be converted into a comparatively short duty cycle pulse.
  • FIG. 19 schematically illustrates a device for converting a input data stream like that of FIG. 18(a) into a data stream like that shown in FIGS. 18(b) or 18(c).
  • the circuit of FIG. 19 is placed between the data source 146 and the modulator 144 in FIG. 6.
  • a data stream is input from the data source 146 to the pulse modifier 420 shown m FIG. 19.
  • the electncal signal travels along two paths so that a portion of the signal passes through a delay element 422.
  • Delay element 422 creates a delay with respect to other path's undelayed signal.
  • the two signals are recombmed by a recombiner 424 in a manner that produces a positive pulse only while the undelayed and the delayed signals are both "1".
  • the delay circuit 422 may be a programmable delay or it might consist of a senes of inverters.
  • the recombiner might, for example, be an exclusive OR gate.

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  • Optical Communication System (AREA)

Abstract

La présente invention concerne un système de communications par fibre optique multi-utilisateurs utilisant des techniques d'accès multiple par étalement du spectre afin de permettre une meilleure utilisation de largeur de bande. Chaque voie du système est équipée d'une source de lumière temporellement et spectralement modulée à l'aide d'un codeur. La modulation s'accomplit en faisant d'abord passer les données via un modificateur d'impulsion afin d'obtenir un flux d'impulsions raccourcies avec un facteur de marche réduit. La lumière modulée est couplée à une fibre et les données sont récupérées par le décodeur. La source comprend une source de fibre superluminescente scindée de multiples fois et amplifiée d'une manière hiérarchique afin de produire une pluralité de sources semblables. L'adjonction de retard permet de décorréler ces sources semblables. Chacun des codeurs comprend un masque de codage présentant un premier code qui code le signal optique. La lumière, codée spatialement par le masque et temporellement modulée avec les données est émise sur une liaison de fibre avec les signaux d'autres utilisateurs et reçue par un décodeur. Dans chaque décodeur, un séparateur insensible à la polarisation scinde la lumière reçue en deux composants de puissance égale dirigés vers deux masques de décodage utilisés afin de décoder le signal. L'un des masques possède un deuxième code identique au premier code et l'autre masque possède un troisième code complémentaire du premier code. Les rayons lumineux de sortie, filtrés par les masques, sont détectés différentiellement afin de générer un signal de sortie, ultérieurement traité afin de récupérer des données. Le signal électrique passe par un filtre passe-bas et par un détecteur quadratique électrique. Les premiers codes sont choisis parmi un ensemble de codes unipolaires dérivés d'un ensemble de codes orthogonaux bipolaires équilibrés. Les codes peuvent être ou bien binaires ou analogiques.
PCT/US1999/017258 1998-07-30 1999-07-29 Procede et dispositif de reduction d'interference en amcr optique WO2000007317A1 (fr)

Priority Applications (6)

Application Number Priority Date Filing Date Title
CA002339113A CA2339113A1 (fr) 1998-07-30 1999-07-29 Procede et dispositif de reduction d'interference en amcr optique
EP99938889A EP1101309A1 (fr) 1998-07-30 1999-07-29 Procede et dispositif de reduction d'interference en amcr optique
AU53278/99A AU5327899A (en) 1998-07-30 1999-07-29 Method and apparatus for reduced interference in optical cdma
KR1020017001291A KR20010072120A (ko) 1998-07-30 1999-07-29 광학 ｃｄｍａ에서 간섭을 감소시키기 위한 방법 및 장치
JP2000563022A JP2002521957A (ja) 1998-07-30 1999-07-29 光学ｃｄｍａにおいて干渉を減少する方法および装置
BR9912598-6A BR9912598A (pt) 1998-07-30 1999-07-29 Método de aparelho para uma interferência reduzida em um cdma ótico

Applications Claiming Priority (2)

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US12734398A 1998-07-30 1998-07-30
US09/127,343 1998-07-30

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JP (1) JP2002521957A (fr)
KR (1) KR20010072120A (fr)
AU (1) AU5327899A (fr)
BR (1) BR9912598A (fr)
CA (1) CA2339113A1 (fr)
RU (1) RU2001105929A (fr)
WO (1) WO2000007317A1 (fr)

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EP1286483A2 (fr) * 2001-08-23 2003-02-26 Alcatel Modulateur optique amélioré permettant une optimisation de la modulation NRZ
US6853445B2 (en) 2002-01-07 2005-02-08 Motorola, Inc. Two-dimensional angle of arrival detection device
CN102135698A (zh) * 2011-03-15 2011-07-27 中国工程物理研究院激光聚变研究中心 透射式全光纤光脉冲编码器
US8078059B2 (en) 2004-08-20 2011-12-13 Panasonic Corporation Multimode optical transmission device

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KR100488415B1 (ko) * 2002-10-29 2005-05-11 한국전자통신연구원 양극성 데이터를 송신하는 파장영역 광 코드분할다중접속 송신장치 및 그 방법
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Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2000070804A1 (fr) * 1999-05-17 2000-11-23 Codestream Technologies Corporation Circuit photonique integre pour amrc optique
EP1286483A2 (fr) * 2001-08-23 2003-02-26 Alcatel Modulateur optique amélioré permettant une optimisation de la modulation NRZ
FR2828943A1 (fr) * 2001-08-23 2003-02-28 Cit Alcatel Modulateur optique ameliore permettant une optimisation de la modulation nrz
US6661553B2 (en) 2001-08-23 2003-12-09 Alcatel Optical modulator which optimizes NRZ modulation
EP1286483A3 (fr) * 2001-08-23 2005-09-14 Alcatel Modulateur optique amélioré permettant une optimisation de la modulation NRZ
CN100340073C (zh) * 2001-08-23 2007-09-26 阿尔卡塔尔公司 优化不归零调制的改进的光调制系统
US6853445B2 (en) 2002-01-07 2005-02-08 Motorola, Inc. Two-dimensional angle of arrival detection device
US8078059B2 (en) 2004-08-20 2011-12-13 Panasonic Corporation Multimode optical transmission device
CN102135698A (zh) * 2011-03-15 2011-07-27 中国工程物理研究院激光聚变研究中心 透射式全光纤光脉冲编码器

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BR9912598A (pt) 2002-01-02
RU2001105929A (ru) 2003-01-27
KR20010072120A (ko) 2001-07-31
CA2339113A1 (fr) 2000-02-10
AU5327899A (en) 2000-02-21
EP1101309A1 (fr) 2001-05-23
JP2002521957A (ja) 2002-07-16

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