The present invention relates to a method and device for digitising an electrical signal, preferably a microwave signal. More particularly, but not exclusively, the present invention relates to a method of digitising a microwave signal comprising the steps of providing a plurality of laser pulse trains of different wavelengths, introducing a time delay between each of the pulse trains, passing each of the pulse trains through a modulator where they are modulated by an optical microwave signal, splitting the modulated signals into a plurality of wavelength dependent paths and digitising the received signal in each path. The present invention also relates to a device for performing such a method.
Devices for digitising microwave signals are known. Such devices use either time division multiplexing (TDM) or wavelength division multiplexing (WDM). TDM systems provide a succession of optical pulses. These are modulated by the microwave signal. A high speed RF driven optical switching element sends successive pulses along different optical paths. An analogue to digital converter in each path digitises the received pulses. The high speed optical element is difficult and expensive to manufacture and is also difficult to drive electrically.
WDM systems provide a series of pulses of different wavelengths. These are modulated by the microwave signal before being split into different optical paths by an arrayed waveguide grating before being digitised. It is difficult to generate a series of pulses with different wavelengths from one pulse to the next. Such WDM systems are complex and difficult to manufacture.
Accordingly, a first aspect of the invention provides a device for digitising an electrical signal comprising
Using this approach to make a photonic analogue to digital converter (ADC) enables sampling and digitisation of arbitrary electronic, preferably microwave signals to be achieved at significantly higher sampling rates and microwave signal bandwidths than can be achieved with purely electronic ADCs.
The use of continuous wave lasers allows the device to sample signals with higher precision than other wavelength division multiplexed architectures. Other WDM systems require a short pulsed (mode locked) laser which may not have a stable enough pulse to pulse power jitter to give a high enough effective number of bits (ENOB) or spurious free dynamic range (SFDR).
In addition the device according to the invention allows a complex sampling function to be achieved using simple passive photonic components. The device according to the invention is reliable and lightweight and is particularly suitable for use in high performance avionic and naval electronic warfare applications. Other applications include high speed single shot oscilloscopes and spectrum analysers.
Preferably the dispersive optical chopper comprises an optical combiner having a plurality of input ports each adapted to receive the output of a laser and an output port, the optical combiner being adapted to combine the optical signals received at the plurality of input ports at the output port.
Preferably, the dispersive optical chopper comprises at least one optical pulse generator adapted to receive continuous optical signals at one or more wavelengths and to convert these to one or more optical pulse trains at these wavelengths.
The pulse generator can be adapted to receive the output of the optical combiner.
The device can further comprise a dispersive optical element connected between the pulse generator and the port of the optical modulator to introduce a wavelength dependent delay between optical pulse trains received from the optical pulse generator.
The device can comprise a plurality of optical pulse generators, one being connected between each of the lasers and a corresponding input port of the optical combiner.
The device can comprise a dispersive optical element connected between the output of the optical combiner and the modulator.
Alternatively, the device can comprise a plurality of delay elements, one being connected between each optical pulse generator and the corresponding input of the optical combiner, each delay element being adapted to introduce a predetermined delay in the optical signal passing through the delay element.
The dispersive optical element can comprise an optical fibre, preferably a fibre optic cable.
The dispersive optical element can be a fibre bragg grating.
The dispersive optical element can be an echelle grating.
The dispersive optical element can comprise
The delay element can comprise an optical fibre, preferably a fibre optic cable.
The at least one optical splitter can be an arrayed waveguide grating.
The at least one optical splitter can be a thin film filter.
The at least one optical splitter can be a planar waveguide echelle grating.
The at least one optical combiner can be an arrayed waveguide grating.
The at least one optical combiner can be a thin film filter.
The at least one optical combiner can be a planar waveguide echelle grating.
In a further aspect of the invention there is provided
a method of digitising an electrical signal comprising the steps of
The output of the plurality of lasers can be combined into a single path before modulation.
The combination can be performed by an arrayed waveguide grating.
Alternatively, the combination can be performed by a thin film filter.
The combination can be performed by an echelle grating.
Preferably, each of the outputs is converted to an optical pulse train before combination.
The predetermined time delay can be introduced between the optical pulse trains before combination.
The time delay can be introduced by passing the optical pulse trains through at least one dispersive optical element, preferably an optical fibre, more preferably a fibre optic cable
The dispersive optical element can be an echelle grating or fibre Bragg grating.
Each of the outputs of the plurality of lasers can be converted to a optical pulse train after combination.
A predetermined delay can be introduced between the optical pulse trans after combination.
The present invention will now be described by way of example only and not in any limitative sense with reference to the accompanying drawings in which
Shown in
Connected to the output port 8 of the AWG 4 is the pulse generator 5. The pulse generator 5 receives the continuous wave output of the AWG 4 at a plurality of wavelengths and converts these into optical pulse trains at the same wavelengths. The optical pulse trains may be several wavelengths long. Typically the pulse is less than 1 ns but longer than ifs. The pulse generator of the embodiment is a stable low jitter electro-refractive pulse generator.
Extending from the output of the pulse generator 5 is the dispersive optical element 6 comprising fibre optic cable 6. A dispersive fibre optic cable 6 is one where the speed of light through the cable varies with the wavelength of the light. The dispersive fibre optic cable 6 introduces a very accurately known timing separation between the different wavelength optical pulse trains as they exit the fibre optic cable 6.
The dispersed optical pulse trains are received by a modulator 9. As the optical pulse trains pass through the modulator 9 they are modulated by a received analogue microwave signal 10. The amplitude of the signal output from the modulator 9 depends upon the amplitude of the microwave signal. The operation of such modulators 9 is well known and will not be described further.
The output from the modulator 9 is received by an optical splitter 11 comprising an AWG 11. The AWG 11 splits the modulator output into a plurality of wavelength dependent optical paths 12. Each of the optical paths 12 receives the optical pulse train from one of the CW lasers 2.
A plurality of photodetectors 13 are connected one to each of the outputs 12 of the AWG splitter 11. Filters (not shown) are connected to the outputs of the photodetectors 13 to broaden the received optical pulses which are in turn read by electronic analogue to digital converters (ADCs) (not shown).
The device according to the invention has the advantage that the microwave signal can be sampled at very short time intervals—the time between the different wavelength optical pulse trains as they leave the optical fibre 6. The analogue to digital converter however need only digitise the received signals at the rate the pulse generator 5 generates optical pulse trains
Shown in
The embodiment of
Shown in
This embodiment has the advantage that different pulse generators 19 can be driven at different clock rates for recovering the original frequency in under-sampled analogue microwave signals.
Shown in
The embodiments of
In a further embodiment of the invention (not shown) at least one of the ADCs is connected to a plurality of photodetectors each connected to an output from the final optical splitter. This increases the rate at which the ADCs must digitise the received optical signals but reduces the number of ADCs required.
Shown in
Shown in
The devices of
Number | Date | Country | Kind |
---|---|---|---|
0524461.1 | Dec 2005 | GB | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
---|---|---|---|---|
PCT/GB06/04450 | 11/28/2006 | WO | 00 | 11/16/2009 |