Optical demultiplexing system

Abstract: Optical demultiplexing system, wherein from an optical carrier modulated by a TDM data flow the wanted tributary is extracted as an optical signal. The system makes use of a semiconductor optical amplifier, whose gain is modulated due to saturation effect. The amplifier receives both the modulated optical carrier and one or a plurality of sampling optical carriers, with wavelengths different from that of the modulated carrier. One or a plurality of optical filters supply at the output the tributaries by extracting from the amplifier output the sampling carriers modulated by data signals.

Description: The present invention concerns high bit-rate digital signal transmission systems, wherein a plurality of channels are transmitted in time division on an optical fibre by modulating a coherent light radiation, and more particularly it relates to an optical demultiplexing system. When a digital signal flow composed of a plurality of time-division multiplexed channels (TDM=Time Division Multiplex) arrives at a receiving terminal, it must undergo a demultiplexing operation allowing the extraction of bits belonging to a determined channel or tributary. If the transmission is carried out by sending on an optical fibre a light radiation amplitude-modulated by the digital TDM flow, the demultiplexing at the receiving terminal can be carried out according to two different methods: by converting the whole TDM data flow from optical into electrical signal and hence by demultiplexing the signal obtained by suitable electronic circuits, of the type commonly used in digital telecommunication apparatus; by extracting by optical devices from the TDM data flow the only tributary desired and then converting it into an electric signal for the successive processing operations. The first method, which is presently the most widely used, requires a broadband optical receiver and demultiplexing electronic circuits operating at the bit rate of the TDM data flow. Good performances in terms of sensitivity are difficult to achieve by the use of wide-band optical receivers and the electronic circuits are particularly critical, especially by operating at bit rates of some Gbit/s. The second method demands a suitable device which allows the optical signal to be deviated to the receiver exclusively at the instants corresponding to the passage of the bits belonging to the channel to be extracted. Such a device must be capable of operating at a rate comparable with TDM data flow bit rate, requiring as low as possible optical power levels. Different methods using devices adapted to this aim have been described in the literature. Among them the following methods are worth noticing; they use: an electro-optical switch, of the type described by R.S.Tucker et al in "16 Gbit/s fibre transmission experiment using optical time-division multiplexing", issued in Electronic Letters, Vol. 23, n.24, pages 1270-1271; a semiconductor optical amplifier, switched on only in correspondence with the tributary to be extracted, according to the method described by P.B.Hansen et al in "Optical Demultiplexing at 6 Gbit/s Using a Semiconductor Laser Amplifier as an Optical Gate" issued in IEEE Fhotonics Technology Letters Vol. 3, NO. 11, November 1991, pages 1018-1020; an optical fibre trunk, whereto the TDM data flow and a suitable sampling signal are sent at the same time and wherefrom the relevant conversion products, generated by non-linearity phenomena, are extracted by a suitable optical filtering operation. This method is cescribed by P.A. Andrekson et al in "All-Optical Demultiplexing at 16 Gbit/s using Four-Wave Mixing", issued in Technical Digest of OFC'91, San Diego 1991, pages 19-22. and in "16Gbit/s All-Optical Demultiplexing using Four-Wave Mixing", issued in Electronic Letters. 23 May, 1991. Vol. 27 No. 11, pages 922-924. The first two methods dramatically degrade TDM data flow integrity, rendering it non-available for further processing operations, while the third requires high signal powers, of the order of 100 mW, and optical signals with wavelengths very close to one another, so as to obtain the desired non-linearity effects in the fibre. The latter requirement demands also the use of very narrow optical filters and highly wavelength-stabilized optical-carriers. The disadvantages above are overcome by the optical demultiplexing system, provided by the present invention, which does not require high power optical signals, is not critical as to the difference between optical signal wavelengths and does not dramatically degrade TDM data flow, thus allowing its further use for successive processing operations. It can operate at high bit rates, while the optical receivers and the electronic circuits can operate at the demultiplexed signal rate. The present invention provides an optical demultiplexing system, wherein from an optical carrier at a first wavelength, modulated by a TDM data flow, one or more tributaries are extracted to be forwarded to relevant optical receivers for successive processing operations, which comprises: one or more sources, apt to generate sampling optical carriers reaching their maximum amplitude only in the time intervals wherein the relevant tributary to be extracted is present; an optical coupler, whereto said optical carrier at the first wavelength and the sampling optical carrier(s) at different wavelength(s) are sent; an optical non-linear interaction means, whose input receives the sum of said optical carriers, present at the output of said optical coupler; a second optical coupler, which subdivides the power supplied at the output by said optical non-linear interaction means; optical filters, to whose input there is sent the signal supplied by said second optical coupler, characterized in that the optical non-linear interaction means, the interaction therein varying with the increasing of the total power of the input carriers, is a semiconductor optical amplifier whose amplifier gain decreases with the increasing of the total power, and in that said optical filters have pass bands centred on said first wavelength for extracting said optical carrier modulated by the TDM data flow, and centred on the wavelength of one of the sampling optical carriers for supplying said one or more tributaries to the receivers, respectively. The foregoing and other characteristics of the present invention will be made ciearer by the following description of a preferred embodiment thereof given by way of non-limiting example, and by the annexed drawing which shows a block diagram of the optical demultiplexing system. The system uses a semiconductor optical amplifier, whose gain is modulated as an effect of the saturation due to the algebraic sum of the powers of the input optical signals, independent of how the power is distributed among the different wavelengths. As a consequence, if an intensity-modulated and an unmodulated optical carrier are sent at the same time to the amplifier, even the second carrier is modulated by saturation effect. If the carriers have different wavelengths, they can be afterwards easily separated. In the block diagram shown in the figure, a source SD sends to a fibre end OF1 an optical carrier at a wavelength L1, amplitude-modulated by TDM data flow. At the same time, a source SC sends to a fibre end OF2 a sampling optical carrier, i.e. a carrier which reaches its maximum amplitude only in the time intervals wherein the tributary to be extracted is present. This second carrier has a wavelength 12 different from L1. The two signals at the outputs of the opposite fibre ends are summed in a coupler OC1 and sent to a semiconductor optical amplifier SA. The amplifier gain decreases when the algebraic sum of the powers of the input optical signals increases, therefore, when the sampling carrier is present and the TDM data signal reaches its maximum power (high logic level), the amplifier gain is lower than at the instants the power of TDM data signal is minimum (low logic level). The sampling signal at the amplifier output is thus modulated with inverted logic with regard to the wanted tributary. A coupler OC2 splits the optical signal at the output of the amplifier SA and sends the two parts to two optical fibres OF3 and OF4. An optical filter F12, having its passband centred on wavelength L2, allows the forwarding to the optical receiver RX of the only sampling signal modulated by the wanted tributary and rejects the TDM data signal at wavelength L1. The latter signal, present on fibre OF3, can be picked up for successive processing operations by a filter Fl1 with passband centred on wavelength L1. Within receiver RX the optical signal relevant to the only wanted tributary is then detected, electronically amplified and possibly inverted to obtain the original digital signal. If a plurality of tributaries is to be extracted, it is sufficient to utilize a plurality of sources like SC, each of them capable of generating a sampling carrier with different wavelength L3, L4, etc, and, by using a coupler OC1 with a plurality of inputs, to send at the same time all the optical carriers to optical amplifier SA. Analogously, at SA output a coupler like OC2, with a plurality of outputs, sends to a plurality of optical filters, each of them having a passband centred on the wavelength of one of the sampling carriers, the global optical signal. A corresponding receiver like RX can be placed at the output of each filter.

Claims: Optical demultiplexing system, wherein from an optical carrier at a first wavelength (L1), modulated by a TDM data flow, one or more tributaries are extracted to be forwarded to relevant optical receivers (RX) for successive processing operations, which comprises: one or more sources (SC), apt to generate sampling optical carriers reaching their maximum amplitude only in the time intervals wherein the relevant tributary to be extracted is present; an optical coupler (OC1), whereto said optical carrier at the first wavelength and the sampling optical carrier(s) at different wavelength(s) (L2, L3, L4,...) are sent; an optical non-linear interaction means (SA), whose input receives the sum of said optical carriers, present at the output of said optical coupler (OC1); a second optical coupler (OC2), which subdivides the power supplied at the output by said optical non-linear interaction means (SA); optical filters (FI1, FI2), to whose input there is sent the signal supplied by said second optical coupler, characterized in that the optical non-linear interaction means, the interaction therein varying with the increasing of the total power of the input carriers, is a semiconductor optical amplifier (SA) whose amplifier gain decreases with the increasing of the total power, and in that said optical filters (FI1, FI2) have pass bands centred on said first wavelength (L1) for extracting said optical carrier modulated by the TDM data flow, and centred on the wavelength (L2, L3, L4,...) of one of the sampling optical carriers for supplying said one or more tributaries to the receivers (RX), respectively.

Inventors: CAVACIUTI ALESSANDRO, PULEO MARIO, CAVACIUTI, ALESSANDRO, PULEO, MARIO
Applicants: CSELT CENTRO STUDI LAB TELECOM, CSELT CENTRO STUDI E LABORATORI TELECOMUNICAZIONI S.P.A.
Application year: 1993
Main classification: H04J14
IPC codes: H04J14, H01S5