OPTICAL LINEWIDTH INDEPENDENT HIGH PURITY MMW/THZ GENERATOR EMPLOYING CASCADED DEMULTIPLEXING

20230370165 · 2023-11-16

    Inventors

    Cpc classification

    International classification

    Abstract

    The invention provides an optical generator and method comprising an Optical Frequency Comb configured to generate a plurality of frequency tones and fed to a first demultiplexer, wherein the first demultiplexer is configured to injection lock at least one desired frequency tone; and a second demultiplexer connected to the first demultiplexer and configured to injection lock a second frequency tone from said plurality of frequency tones wherein the output of the second demultiplexer comprise two injection locked frequency tones separated by a desired frequency. The invention enables the generation of high frequency signals (>30 GHz) that exhibit high levels of purity (required for many applications). Moreover, the invention simplifies the architecture, by reducing the real estate occupied by the components. This is most important when all the devices involved are integrated onto a single chip.

    Claims

    1. An optical high frequency RF generator comprising an Optical Frequency Comb configured to generate a plurality of frequency tones and fed to a first demultiplexer, wherein the first demultiplexer is configured to injection lock at least one desired frequency tone; a second demultiplexer connected to the first demultiplexer and configured to injection lock a second frequency tone from said plurality of frequency tones wherein the output of the second demultiplexer comprise two injection locked frequency tones separated by a desired frequency; and a modulator configured to modulate the second demultiplexer with a data signal, such that a desired data signal is applied to a second demultiplexed tone.

    2. The optical high frequency RF generator of claim 1 wherein the at least one desired frequency tone is amplified.

    3. The optical high frequency RF generator of claim 1 comprising a photodetector configured to heterodyne the two injection locked frequency tones to generate an electrical signal.

    4. The optical high frequency RF generator of claim 1 wherein the first demultiplexer and the second demultiplexer comprises two active demultiplexers connected in series and configured such that two tones required for high frequency generation can be filtered out.

    5. The optical high frequency RF generator of claim 1 wherein a heterodyning process generates a high purity mmW/THz frequency.

    6. The optical high frequency RF generator of claim 1 wherein the first demultiplexer comprises a semiconductor laser.

    7. The optical high frequency RF generator of claim 1 wherein the second demultiplexer comprises a semiconductor laser.

    8. The optical high frequency RF generator of claim 1 wherein at the output of the demultiplexer the two amplified tones are separated by a desired mmW/THz frequency are obtained.

    9. A transmitter for use in an optical communications system comprising the optical high frequency RF generator as claimed in claim 1.

    10. A method of generating a high frequency signal using an optical generator comprising the steps of: configuring an Optical Frequency Comb to generate a plurality of frequency tones and inputting to a first demultiplexer, wherein the first demultiplexer is configured to injection lock at least one desired frequency tone; connecting a second demultiplexer connected to the first demultiplexer; configuring the second demultiplexer to injection lock a second frequency tone from said plurality of frequency tones; and outputting two injection locked frequency tones separated by a desired frequency.

    11. The method of claim 10 comprising the step of modulating the second demultiplexer with a data signal, such that a desired data signal is applied to a second demultiplexed tone.

    Description

    BRIEF DESCRIPTION OF THE DRAWINGS

    [0044] The invention will be more clearly understood from the following description of an embodiment thereof, given by way of example only, with reference to the accompanying drawings, in which:

    [0045] FIG. 1 illustrates a schematic of (a) a mmW/THz generator employing a cascaded demultiplexer, (b) its functionality as a data modulator. Line graph illustrates the principle of operation;

    [0046] FIG. 2 illustrates (a) a traditional comb based mmW/THz generator consisting of passive filters, external modulators, passive splitters and combiners, and (b) a mmW/THz generator employing active demultiplexers according to one aspect of the invention; and

    [0047] FIG. 3 illustrates (a) an experimental setup of the A-RoF transmission system employing dual-stage active demultiplexer, (b) line-graph illustration of the principle operation, (c) electrical spectrum of the down converted UF-OFDM data after 25 km fibre transmission. where BBU: baseband processing unit; RRU: remote radio unit; VOA: variable optical attenuator; AWG: arbitrary waveform generator; PD: photodetector; EBPF: electrical band pass filter; LO: local oscillator; RTS: real time oscilloscope.

    DETAILED DESCRIPTION OF THE DRAWINGS

    [0048] The invention provides a cascaded demultiplexer (for mmW/THz generation), in combination with an optical frequency comb, which works on the principle of using a pair of active demultiplexers based on optical injection locking. The invention provides a means to filter and amplify individual comb lines generated from the optical comb.

    [0049] An optical generator comprising an optical comb source and utilises two active demultiplexers in series, configured such that two tones required for the mmW/THz generation can be filtered out without the need for splitting/recombining signals. In other words, the invention provides a dual stage active demultiplexing of an optical frequency comb source. As a result, the invention avoids any potential phase decorrelation, preserves the optical power and reduces the device footprint since the entire generator can be realised as a single small photonically integrated chip.

    [0050] As the active demultiplexer is preferably a semiconductor laser, the second demultiplexer can be directly modulated with the data, thus eliminating the need for an external modulator, further simplifying the design of a mmW/THz generator (further insertion loss, path mismatch, polarisation management etc.).

    [0051] FIG. 1(a) illustrates schematic of a mmW/THz generator employing cascaded demultiplexer, laser 1 and laser 2 according to one embodiment of the invention. FIG. 1(b), similar to FIG. 1(a) illustrates an additional functionality, where a data modulation can be applied to the second demultiplexer, laser 2 which is arranged in series with the first demultiplexer. Line graph illustrates the principle of operation.

    [0052] A high purity mmW and THz radio frequency can be generated by employing at least two multifunctional active demultiplexers in a cascaded configuration. The operational principle of FIG. 1(a) is as follows: an Optical Frequency Comb is (OFC) 10 is configured to generate highly coherent tones with a free spectral range (FSR) ‘w’, is injected into demultiplexer 11. The wavelength of the demultiplexer 11, λ.sub.d1, is thermally tuned to match the wavelength of a desired comb tone λ.sub.1. Consequently, the demultiplexer 11 is injection locked by the tone (i.e. inherits its frequency and phase). Since the output power of the demultiplexer 11 is much higher than that of the input tone, the selected line is also amplified. The remaining, unsuppressed OFC tones also pass through Demultiplexer 11, but without any amplification.

    [0053] The output of the demultiplexer 11 is injected into demultiplexer 12. In a similar fashion, the wavelength of demultiplexer 2, λ.sub.d2, is matched with the comb tone (unsuppressed) separated from λ.sub.1, by a frequency of the mmW/THz that is to be generated. While the power of these unsuppressed tones is typically low, it is still sufficient to achieve stable injection locking of the demultiplexer 12. As a consequence, demultiplexer 12 is injection locked by the desired unsuppressed tone, thus amplifying it and inheriting its phase and frequency.

    [0054] Thus, at the output of the demultiplexer 12, the two amplified tones separated by the desired mmW/THz frequency are obtained. The line graph shown in FIG. 1 (a), illustrates the principle operation of the mmW/THz generator.

    [0055] In addition, as the active demultiplexers are standard semiconductor lasers, it is possible to encode the electrical data on the mmW/THz signal, by directly modulating the demultiplexer 12 using a modulator device 13 (as shown in FIG. 1 (b)).

    [0056] As a result, heterodyning of the two demultiplexed tones on a photodetector 14 generates the desired high spectral purity mmW/THz tone modulated with the data. The arrangement of the active demultiplexers enables enhanced immunity to the phase noise and improved power of the mmW/THz signal. In addition, the photonic integration of the architecture of FIG. 1(a) and FIG. 1(b) is easier, cost efficient and results in a smaller footprint.

    [0057] FIG. 2 illustrates (a) traditional comb based mmW/THz generator consisting of passive demultiplexer, external modulators, passive splitters and combiners, and FIG. 2(b) illustrates proposed mmW/THz generator employing active demultiplexers.

    [0058] According to one embodiment of the invention, the mmW/THz generator can significantly simplify the way RF frequencies that are generated, as illustrated in FIG. 2(b). The schematic of a standard mmW/THz photonic generator is shown in FIG. 2(a), where an OFC can be demultiplexed using either a passive or an active demultiplexer, into individual comb tones that are then grouped in pairs, separated by the desired frequency. If the mmW/THz signal is to convey information, one tone out of the pair is then externally modulated with an electronic data signal. Finally, the pair of comb tones are recombined and detected (mixed) at the photodiode to generate the electrical signal. Such an architecture of the transmitter suffers from several problems: [0059] 1. Since the two tones travel different paths, phase decorrelation occurs. Maintaining the path lengths is particularly difficult if one of the tones needs to be modulated with data (different number of components in each path). The phase decorrelation reduces the quality of the generated tone, degrading the overall performance of the system employing such a transmitter. In order to minimise the impact of the path mismatch an expensive, ultra-low linewidth comb source needs to be used, which increases the cost of the generator. [0060] 2. The comb needs to be split as many times as the total number of comb tones required and then each pair of tones needs to be recombined. This introduces a loss of at least 6 dB per pair. If an external modulator is used, further loss is incurred in the modulated line. [0061] 3. Even when realised as a photonic integrated circuit (PIC), splitters and combiners occupy a large amount of space. The larger footprint also leads to an increased level of complexity e.g. of the temperature control of the device.

    [0062] In contrast, the method of mmW/THz generation according the present invention overcomes all of the mentioned difficulties. As showed in FIG. 2(b) an OFC comb 10 outputs to two pairs of demultiplexers, where the first pair comprise two demultiplexers 11a, 12a arranged in series and demultiplexer 12a is modulated by modulator 13a. The second pair also comprises two demultiplexers 11b, 12b arranged in series and demultiplexer 12b is modulated by modulator 13b. The architecture provides the following advantages: [0063] No path length mismatch: two tones traverse the same path [0064] Tolerance to a large optical linewidth (cheaper and simpler OFC) [0065] Reduced loss: split ratio reduced by a factor of two in comparison to the standard architecture, no need for a combiner [0066] Reduced footprint: smaller split ratio and elimination of combiners and external modulator allows for much smaller size of the device. [0067] Multifunctionality of the active demultiplexer: performs demultiplexing, amplification and modulator functionalities. [0068] Tunability: the mmW/THz frequencies can be tuned as multiples of the OFCs FSR [0069] Photonically integratable, further reducing cost, footprint and energy consumption

    Example Embodiment

    [0070] FIG. 3 (a) illustrates an example setup of an A-RoF transmission system employing dual-stage active demultiplexer, (b) line graph illustration of the principle operation, (c) electrical spectrum of the down-converted UF-OFDM data after 25 km fibre transmission. BBU: baseband processing unit; RRU: remote radio unit; VOA: variable optical attenuator; AWG: arbitrary waveform generator; PD: photodetector; EBPF: electrical band pass filter; LO: local oscillator; RTS: real time oscilloscope.

    [0071] The schematic of the proposed transmitter is shown in FIG. 3(a) as a baseband processing unit (BBU) 20. The BBU transmitter 20 comprises an Optical Frequency Comb (OFC 10), generating highly coherent tones, followed by a semiconductor laser based dual-stage active demultiplexer 11, 12. A spectral line graph, illustrating the principle of operation of the transmitter, is shown in FIG. 3(b).

    [0072] The output of the OFC 10 is injected, via an optical circulator 21, to the first stage of the demultiplexer (Demux 1) 11, whose wavelength is then tuned (using the bias current and the temperature) to match the wavelength of the desired comb line. Once the alignment is achieved, Demux 11 becomes injection locked by the comb line. As a result, Demux 11 inherits the frequency and phase characteristics of the OFC, while at the same time amplifying the selected comb tone (the power of Demux 11 is much higher than that of the comb line). The remaining, unsuppressed OFC tones also pass through Demux 11, but without any amplification.

    [0073] The difference between the power of the demultiplexed and the remaining comb tones can be defined as the comb line suppression ratio (CLSR). While the power of these spurious tones is low, it is sufficient to enable a stable injection locking of the second demultiplexing stage (Demux 2) 12. Therefore, a second OFC tone can be demultiplexed, by injecting the output of Demux 11 into Demux 12, via optical circulator 22. The wavelength of the latter is then tuned to match that of an unsuppressed comb tone, separated from the tone selected by Demux 11, by a frequency of the mmW signal that is to be generated.

    [0074] As a result, Demux 12 is injection locked by this second comb tone, thus also inheriting the spectral characteristics of the OFC 10 and providing amplification to the selected comb tone. Hence, the output of Demux 12 consists of the two selected high power spectral components (tone selected by Demux 11 and 12), separated by the desired mmW frequency.

    [0075] Since the active demultiplexer is a standard semiconductor laser, it is possible imprint the electrical data that is to be transmitted on the mmW signal, by directly modulating Demux 12 by using a modulator 23, such as an arbitrary waveform generator.

    [0076] The invention provides a transmitter based on an OFC and a dual-stage active demultiplexer. Unlike other OFC-based schemes, the architecture features a single optical path, alleviating the need for optical splitters, combiners, an external modulator as well as careful path length matching mechanisms.

    [0077] Furthermore, the inherent amplification provided by the active demultiplexer, removes the requirements for an external optical amplifier. As a result, the invention offers a significant cost, complexity and footprint reduction. Finally, as all the components of the transmitter can be realised in InP, the entire device can be realised within a single photonically integrated chip, providing further cost and footprint savings.

    [0078] The optical generator as hereinbefore described provides a solution for a range of applications, including communications, sensing (medical and industrial) and imaging.

    [0079] The embodiments in the invention described with reference to the drawings comprise a computer apparatus and/or processes performed in a computer apparatus. However, the invention also extends to computer programs, particularly computer programs stored on or in a carrier adapted to bring the invention into practice. The program may be in the form of source code, object code, or a code intermediate source and object code, such as in partially compiled form or in any other form suitable for use in the implementation of the method according to the invention. The carrier may comprise a storage medium such as ROM, e.g. a memory stick or hard disk. The carrier may be an electrical or optical signal which may be transmitted via an electrical or an optical fiber cable or by radio or other means.

    [0080] In the specification the terms “comprise, comprises, comprised and comprising” or any variation thereof and the terms “include, includes, included and including” or any variation thereof are considered to be totally interchangeable and they should all be afforded the widest possible interpretation and vice versa.

    [0081] The invention is not limited to the embodiments hereinbefore described but may be varied in both construction and detail.