EP2980620A1 - Optisches Verzögerungselement - Google Patents

Optisches Verzögerungselement Download PDF

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Publication number
EP2980620A1
EP2980620A1 EP14002640.2A EP14002640A EP2980620A1 EP 2980620 A1 EP2980620 A1 EP 2980620A1 EP 14002640 A EP14002640 A EP 14002640A EP 2980620 A1 EP2980620 A1 EP 2980620A1
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EP
European Patent Office
Prior art keywords
filter
signal
signals
unit
delay element
Prior art date
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EP14002640.2A
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English (en)
French (fr)
Inventor
Jürg LEUTHOLD
Romain Bonjour
David Hillerkuss
Christian Hafner
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Eidgenoessische Technische Hochschule Zurich ETHZ
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Eidgenoessische Technische Hochschule Zurich ETHZ
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Priority to EP14002640.2A priority Critical patent/EP2980620A1/de
Publication of EP2980620A1 publication Critical patent/EP2980620A1/de
Withdrawn legal-status Critical Current

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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q3/00Arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system
    • H01Q3/26Arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system varying the relative phase or relative amplitude of energisation between two or more active radiating elements; varying the distribution of energy across a radiating aperture
    • H01Q3/2682Time delay steered arrays

Definitions

  • the invention is related to a delay element and to a method for delaying an input signal.
  • Delay elements are required for many applications, and especially tunable delay elements are desired in many technical fields.
  • a delay element comprises a filter unit for splitting an input signal into two or more signals referred to as filter signals.
  • One or more of the filter signals are then modulated in a modulation unit, and preferably are offset by a phase or a complex amplitude therein, before they are recombined in a combination unit into a single signal which is the output signal.
  • the combination unit recombines the modulated one or more filter signals and the one or more non-modulated filter signals into the output signal which represents the delayed input signal.
  • the filter unit splits the input signal with a frequency dependent splitting ratio or phase ratio.
  • each filter signal is derived from the input signal by applying a filter characteristic that changes over frequency, e.g. linear, or sinusoidal.
  • the filter unit splits the input signal in such a way, that the filter signals complement to a frequency spectrum of the input signal.
  • the filter signals provided by the filter unit may therefore be also referred to as filter signals.
  • the parameter of the at least one filter signal to be modulated is one or more a phase, an amplitude, a frequency, a polarization.
  • the parameter to be modulated is tunable in its magnitude.
  • a phase of the at least one filter signal is modulated while its amplitude preferably is maintained constant.
  • the phase modulation is responsible for the time delay in the output signal.
  • a phase shift to be applied to the at least one filter signal is adjustable. This characteristic makes the delay element be tunable in time.
  • an amplitude of the at least one filter signal is modulated while its phase preferably is maintained constant.
  • the amplitude modulation is responsible for the time delay in the output signal.
  • the amplitude is adjustable. This characteristic makes the delay element be tunable in time.
  • the modulation unit is configured to modulate a phase of exactly one of the filter signals.
  • the filter unit splits the input signal into exactly two filter signals.
  • the modulation unit preferably acts on only one of the filter signals while the other filter signal remains unaffected in phase.
  • the filter signal to be modulated preferably is phase-shifted by - n/2 ⁇ ⁇ ⁇ ⁇ /2.
  • This phase shift invokes, after a recombination of the modulated filter signal and the non-modulated filter signal a resulting output signal that represents the input signal delayed in time.
  • the delay element requires only one filter unit, one phase modulator in the modulation unit and one coupler in the combination unit and as such allows for an implementation with few elements only.
  • the filter unit can comprise any type of filter or filters depending on a desired frequency response of the delay element.
  • the shape and types of the one or more individual filters of the filter unit may have a frequency response which is linear or nonlinear with the frequency, and in case of multiple filters provided these filters may be cascaded, i.e. sequentially arranged, or come as a combination of parallel filters, e.g. in order to optimize a frequency response of the overall filter unit.
  • the filter unit may preferably comprise a spatial light modulator - such as a WaveshaperTM from FinisarTM (trademarks of Finisar or another third party) - providing a very flexible all-purpose implementation which can be tuned to form any possible filter characteristic.
  • the filter could e.g comprise of a delay interferometer, a Fabry-Perot Etalon filter, a thin film filter, a Bragg-Grating filter, a prism filter, an arrayed waveguide grating router filter, etc., which all have a frequency dependent response when tuned to the edge of the passband. Any of these filters can be implemented in different ways. E.g.
  • the delay interferometer can be implemented as a free space delay interferometer, as a fiber interferometer, as an integrated optic interferometer, as a birefringent material interferometer in a fiber, a crystal, etc. Many other implementations can be considered for those skilled in the art.
  • the modulation unit comprises one or more optical modulators, and in particular one or more phase-shifter elements based on a linear electro-optic effect.
  • Such elements typically offer an ultra-fast phase tuning, i.e. a ultra-fast response / low settling time to a tuning of the phase as small as 0.1 ns given a tunability of the modulation unit of e.g. 10 GHz.
  • the tunable time delay element as such is tunable ultra-fast as well.
  • the modulation unit can be based on the Kerr-effect, the quantum confined Stark effect, the plasma dispersion effect, the Franz-Keldysh effect, cross-phase or cross-gain modulation effects, nematic liquid or thermal effects or many other physical effects.
  • a modulator of the modulation unit can be arranged as a single unit phase-modulator or arranged in a Mach-Zehnder or Michelson Interferometer or ring filter configurations. Again, many configurations can be used to modulate the phase or magnitude of a signal. If the filter signal that is fed into the modulation unit is an electrical signal the modulator preferably is based on a mechanical delay element.
  • the combination unit can comprise an electrical or an optical coupler, or any other means for summing up signals, in particular by interference effects.
  • the delay element may also be referred to as complementary phase shifted spectrum delay element.
  • the input signal and the output signal are one of an electrical signal, and in particular a radio-frequency signal, and an optical signal.
  • Embodiments of the present delay elements offer tunability as to the delay time, an ultra-fast settling time and a large bandwidth at the same time. This offers a wide range of new applications where a fast switching between different modulation parameters, e.g. resulting in a fast switching between different delay times, is crucial.
  • the switching time may be defined as a settling time to change from one phase shift to another phase shift resulting in the case of phase modulation, for example.
  • a delay element according to an embodiment of the present invention may be used in a phase array feeder, and especially in a beam array feeder, e.g. employable in next generation wireless networks and allowing new utilizations owed to an ultra-fast tunability of steering directions, and / or an ultra-fast beam stabilization for long range communication and / or a space-time division multiplexing.
  • a long range stabilization such a system would have the ability to overcome the effect of the atmosphere on the transmission channel allowing a longer transmission distance, a faster speed and / or an advanced modulation format.
  • a -delay element according to an embodiment of the present invention may also be employed in a tunable filter for communications, or for the generation of flexible modulation formats such as e.g. pulse position modulation, space division multiplexing etc.
  • exemplary implementations may be in radar or sensing, in radio-frequency and optical signal processing, in multiplexing/de-multiplexing signals, etc.
  • the delay element according to an embodiment of the present invention allows an all-optical system with ultra-fast stabilization of the input signal. Such an implementation would therefore provide real time synchronization without digital signal processing.
  • the delay element comprises one or more or all units implemented in either an optical free space technology in which optical signals are transmitted in free space, or as bulk components comprising of waveguides and / or fibers (RF waveguides, optical fibers, etc.), or in an integrated technology.
  • the individual units of the delay element may be implemented by cascades, i.e. sequentially arranged filters, modulators, etc. for achieving an optimized frequency response for generating a true time delay element.
  • the delay element is generated by using an optical interference technique.
  • an interferometer system may also be implemented as a photonic integrated circuit (PIC) using ring resonators, a delay line or any other component able to generate the requested filter unit in an integrated system.
  • PIC photonic integrated circuit
  • a similar system could be based on free space optic.
  • the two filter signals propagate in the same single waveguide or fiber and have different polarizations, i.e. polarization multiplexing is applied to remove phase noise.
  • a polarization maintaining fiber may be comprised in the filter unit to generate an interferometer delay.
  • a polarization dependent modulator may be comprised in the modulation unit to apply a phase shift on only one of the complementary spectrums.
  • a reference signal which may be used as an up or down-conversion of the input signal with respect to frequency.
  • the reference signal is frequency offset compared to the input signal.
  • the reference signal may in a preferred embodiment be shifted in phase.
  • the reference signal is an optical signal, and in particular a laser signal such that the phase shift may delay a baseband signal and a carrier of the reference signal.
  • the phase shift may be applied at any point using de-multiplexing if requested, and in particular may be applied after the mixing of the two signals.
  • a control for the modulation of the filter signal and the reference signal may be coupled such that both modulators may be driven by the same control signal. This can be achieved either by applying modulators with different properties, such as different length, doping, structure, in order to have different effects in response to the same control signal, or by adding introducing an amplifier with a gain corresponding to a requested difference in length between the modulators.
  • multiple instances of the present embodiments may be cascaded. Even more than two complementary signals may be used.
  • the present delay element may be embodied in one or more of a phased array feeder, a clock recovery system, or a multiplexer.
  • the phase array feeder When applied in a phase array feeder for processing signals to be supplied to an array of n antennas, the phase array feeder comprises a delay element according to any one of the embodiments for supplying the output signal of which delay element to one of the n antennas of the array.
  • n-1 additional modulation units and n-1 additional combination units are provided.
  • a splitter is provided to distribute the filter signals supplied by the filter unit to all of the additional modulation units, too.
  • the present embodiment virtually provides n delay elements while these delay elements share a common filter unit.
  • the splitter may in a more general sense be regarded as a unit for supplying the filter signals provided by the filter unit to each of the additional modulation units.
  • This unit may be considered as a power divider to generate as many copies of the input signal as requested for the given array size.
  • Each modulation unit then modulates at least one of the filter signals supplied thereto.
  • all the modulation units are configured to modulate by a different phase offset.
  • Each additional combining unit is configured to combine at least one modulated filter signal of the assigned additional modulation unit and any filter signal not modulated by the assigned additional modulation unit into a corresponding output signal to be supplied to an associate antenna of array.
  • Each additional modulation unit may comprise a phase modulator for driving both the filter signal phase modulation and an offset phase modulation applied to a reference signal if any.
  • the phase modulator may be implemented in parallel, in series or a combination of both.
  • an azimuth and an elevation angle in the phase are driven by two different control signals.
  • the filter unit, the modulation unit, and the combining unit are integrated on a common substrate.
  • a method for delaying an input signal having a frequency spectrum.
  • the input signal is split into at least two signals filter to the frequency spectrum of the input signal.
  • At least one of the filter signals is modulated, and at least one modulated filter signal and any non-modulated filter signal are combined into an output signal representing the input signal delayed in time.
  • a frequency response of the delay element is generated by means of an interference effect between complementary signal spectra at least one of which is tunable by means of a modulation unit acting on one of magnitude, phase, polarization or frequency.
  • the delay element may be operated sequentially, i.e. it may process several input signals at different frequencies consecutively. In another embodiment, several input signals at different frequencies may be processed at the same time.
  • ⁇ t is the time delay
  • g(t) is an unknown function g in time domain t, also referred to as input signal
  • ⁇ (f) is the Fourier transform in the frequency domain f corresponding to g(t), also referred to as output signal.
  • This frequency response can be understood as a phase shift that changes linearly with the frequency f.
  • Figure 1 depicts the effect of a perfect delay element onto a signal.
  • An input signal Sigin in diagram L exemplary chosen as Nyquist signal, is depicted using a magnitude (absolute value of the complex amplitude) and phase versus frequency representation and using a complex domain representation.
  • an output signal Sig out exhibits the characteristic depicted in diagram M.
  • the effect of a delay element is thus, in the frequency representation, a linear phase versus frequency and no changes on the amplitude. In the complex domain representation, this corresponds to different angles for the different phasors while their lengths stay constant.
  • Figure 2 depicts in diagram a) a magnitude and in diagram b) a phase response over frequency f of an ideal time delay element for different delay times ⁇ t . Any device aiming to act as a tunable time delay element needs therefore a similar set of frequency responses.
  • Figure 3 depicts a delay element according to an embodiment of the invention.
  • the tunable time delay element comprises: A first section 101 with a filter unit 120 generating two signals B and C filter to an input signal 110 depicted in A, that is supplied to the filter unit 120 A second section 102 where one or more of the filter signals B and C - and in the present example only the filter signal C - are modulated by a modulation unit 130 by an exemplary phase, to form modulated filter signals, and in the present embodiment one modulated filter signal E and another non-modulated filter signal D .
  • the modulated filter signal E is combined with the non-modulated filter signal D by a combining unit 140 to generate by superposition an output signal 150 depicted in F.
  • the superposition after phase modulation will exhibit a phase shift that changes with frequency.
  • This effect can be better understood by looking at the complex domain representation of the signals D, E and F.
  • the phasors can be considered having an angle of zero as they are used as reference.
  • the phasors are at an angle or phase corresponding to the applied phase shift in the modulation unit 130, here exemplary of ⁇ /2.
  • the output signal 150 according to F is a vectorial sum of the different frequency components from both signals D and E.
  • the resulting phasors of the output signal 150 have different angles for different frequencies as an amplitude ratio of the filter signals B and C are not constant.
  • the output signal 150 in F exhibits therefore a similar characteristic as with the theoretical time delay element depicted in Figure 1 such that this embodiment can be considered as an approximation of a true time delay element.
  • Figure 4 illustrates a part of the delay element of Figure 3 to demonstrate the tunable nature of the delay element of Figure 3 .
  • the modulator now applies a phase shift of n/4 instead of n/2 to form the modulated filter signal E while the non- modulated filter signal D is not changed compared to Figure 3 .
  • the result of the complex addition in the combining unit 140 exhibits thereby a different relation leading to a different phase versus frequency i.e. another time delay.
  • the phase modulator is thus acting as a tunable element to generate different time delays and can be tuned between - n/2 ⁇ 0 ⁇ n/2 without strong signal deterioration.
  • Figure 5 depicts a set of frequency responses with different applied phase shifts.
  • the complementary spectrums in this example are plotted for the filter units of Figure 3 and 4 , i.e. they correspond to triangular spectrums.
  • the frequency response depicted in Figure 5 may mathematically be computed using the following principles exemplary applied to the embodiments of Figure 3 and 4 .
  • the frequency response of a tunable time delay element at least depends on the type of filter used in the filter unit for splitting the input signal into the two or more complementary signals.
  • a filter unit generating complementary signals may preferably have the following characteristics: the resulting filter signals share the same bandwidth and their amplitudes correspond to a frequency dependent splitting ratio of the input signal.
  • the frequency dependent splitting ratio depicted in for the filter units 120 of Figures 3 and 4 is exemplarily generating a triangle spectrum but any other shapes to optimize the frequency responses of the tunable time delay element would work according to the same principle.
  • FIG. 6 illustrates a block diagram 100a of a tunable time delay element according to an embodiment of the present invention.
  • An input signal 110 is split in a first section 101 by a filter unit 120 into two or more filter signals, the set of filter signals complement to the frequency spectrum of the input signal 110.
  • a frequency dependent splitting ratio is applied in the filter unit 120 across the signal spectrum.
  • One or more of the filter signals supplied at output ports of the filter unit 120 are then offset by phase or complex amplitude by modulators in combination representing a modulation unit 130 - although in the present and other embodiments the individual modulators are referred to by 130 - in a second section 102 before they are recombined into a single output signal 150 in a combination unit 140 of a third section 103.
  • Figure 7 illustrates a block diagram of a tunable time delay element according to another embodiment of the present invention.
  • the filter unit 120 comprises an interferometer such as one of a Mach-Zehnder, a delay-interferometer, a Michelson, a ring filter etc. for generating two filter signals from the input signal.
  • the filter unit 120 may contain a WDM de-multiplexer or any filter leading to sinusoidal magnitude frequency responses.
  • a free spectral range (FSR) preferably is chosen to be about twice the bandwidth of the input signal 110 in order to improve the working range and the tuning of the time delay.
  • the outputs of the interferometer 121 i.e. the filter signals are cosine and sinusoidal functions in frequency instead of being linear in frequency, but similar frequency responses occur as shown for the previous embodiment.
  • the frequency responses of the filters 121 generating the filter signals are depicted as 121a and 121b as insets of Figure 7 .
  • Figure 8 depicts a corresponding frequency response for different phase shifts of a tunable time delay element comprising an interferometer 121 such as shown in Figure 7 . While the magnitude is not flat in all the cases, the phase is almost linear in any of the situations. Therefore, this embodiment with the delay interferometer filter represents an ultra-fast tunable time delay element.
  • the filter units of Figure 6 and / or Figure 7 may be cascaded.
  • FIG. 9 depicts a block diagram of a tunable time delay element according to another embodiment of the present invention.
  • the present filter unit comprises a fiber based delay interferometer.
  • an input signal 210 is tuned in a polarization controller 211 to have a 45° polarization before entering a polarization maintaining fiber 222 leading to a delay of signals at two outputs of the fiber 222 due to fiber birefringence between the slow and fast fiber axis.
  • the two signals are then again rotated by 45° degrees so that interferences can take place on the vertical and horizontal polarization to generate two filter signals at the filter unit outputs.
  • the filter unit may preferably contain a sequential arrangement of a polarization controller 211, a fiber 222, and another polarization controller 223.
  • a different setup could be used achieving the same functions.
  • a modulation unit that is embodied as polarization sensitive phase modulator 230 which is configured to allow offsetting the phase in one polarization only.
  • a combination unit contains a polarization controller 241 in which the signals in the two polarizations, i.e. one filter signal and one phase modulated filter signal, are rotated again in order to generate the desired output signal 250 after the polarizer 242.
  • the output signal 250 could thus be used directly or enter a photodiode.
  • all signals are optical signals and the filtering unit, the modulation unit and the combination unit are acting on the various optical signals in a single waveguide used for propagating.
  • the interferometer system could also be implemented as a photonic integrated circuit (PIC) using a ring resonator, an optical delay element arrangement, or any other component able to generate the requested filter unit in an integrated system.
  • PIC photonic integrated circuit
  • the modulation unit may be implemented depending on the specific application.
  • a free space optical unit may be used for implementing the filter unit and / or the modulation unit, such that a free spectral range FSR may be changed easily.
  • Such an embodiment may allow to be used for signals of different bandwidth just by tuning.
  • Figure 10 shows a block diagram of a tunable time delay element according to another embodiment of the present invention which in addition allows RF or microwave signal generation by photonics mixing.
  • This embodiment contains as additional feature a down- or up-converter 380, where the signal from the tunable time delay element is combined with a reference signal 360 having a different frequency, i.e. having a frequency difference with respect to the input signal 310.
  • a phase modulator 370 might be needed to adjust the phase of the reference signal 360.
  • an input signal 310 is split into one or more filter signals by means of a filter unit 320. Then one or more filter signals at the outputs of the filter unit 320 are phase shifted in a modulation unit 330 in a second section 302 before being recombined in a coupler 340.
  • the recombined signal at the output of the coupler 340 - i.e. the signal carrying information- is combined with the reference signal 360 or the phase shifted reference signal in the down- or up-converter 380.
  • An output signal 350 of the down- or up-converter 380 can thereafter be fed into a mixer not shown providing a signal showing the frequency difference between the input signal 110 and the reference signal 350.
  • the input signal 310 may comprise a baseband signal, i.e. the signal to be delayed in time, that is modulated to a high frequency wave e.g. in the THz range, and the reference signal 360 may have a slightly different frequency than the high frequency wave of the input signal.
  • a combination of the reference signal and the input signal in a mixer such as a photodiode may later on result in a signal showing the frequency difference between the two THz waves, e.g. a signal in the GHz range such that a microwave signal is generated as a carrier for time shifted baseband signal.
  • the optical reference signal 360 of Figure 10 may not necessarily require a phase shifter 370 but may in a preferred embodiment be delayed in its baseband signal on its carrier but not in the carrier.
  • a phase offset constant in frequency is preferably added onto the carrier. This phase offset can be implemented on the reference signal 360 directly using another phase modulator 370.
  • the phase shifter of the modulation unit 330 and the phase shifter 370 can e.g. be driven with a very same control signal by designing the phase shifters such that they provide different phase shifts for the same drive voltage, or by implementing different electronic amplifiers.
  • FIG 11 another tunable time delay element is presented according to an embodiment of the present invention. This embodiment makes use of the basic components of the embodiment shown in Figure 10 .
  • an input signal 410 is supplied to a filter unit and tuned in a polarizer 411 of the filter unit to have a 45° degree polarization before entering a polarization maintaining fiber 422 leading to a delay of signals at two outputs of the fiber 422 due to a fiber birefringence between the slow and fast axis.
  • the two signals are then again rotated by 45° degrees so that interferences can take place on the vertical and horizontal polarization to generate two filter signals at the filter unit outputs that lie in two orthogonal polarizations.
  • a reference signal 460 e.g. in form of a reference laser signal, is polarized by a polarizer 461 to lay at 45° degrees in order to avoid losses in the last section 403.
  • a coupler 462 combines the complementary spectrum signals lying in two polarizations with the polarized reference signal in order to have a single interconnection between sections 401 and 402 avoiding therefore phase noise.
  • wavelength de-multiplexer 431 is used for splitting the signals again.
  • the filter signals can thus enter a polarization dependent phase modulation unit 430 in order to add the phase shift to one of the polarizations while the reference signal is supplied to an offset phase modulator 470.
  • a polarization beam splitter may be used before the modulation unit 430 in order to simplify the setup.
  • a common control signal 432 can directly drive both modulation unit 430 and modulator 470 as explained earlier.
  • the signals from the modulation unit 430 and the modulator are finally combined in a coupler 433 - which in one embodiment may be a WDM coupler as depicted - before entering a last section 403.
  • the components 441 and 442 correspond to the components 241 and 242 of Figure 10 in form of a coupler and a mixer, wherein the mixer supplies the output signal 450.
  • the polarizer 461 may be arranged after the modulator 470.
  • a tunable time delay element according to any of the embodiments is used in a phase array feeder for supplying signals with different delay times to individual antennas of an antenna array, such that a radiation pattern of such phase array takes a desired shape, i.e. a desired direction.
  • Figure 12 depicts the building blocks of a phase array feeder according to an embodiment of the present invention.
  • signal generation and filtering is performed with any filter unit as proposed in the previous embodiments, e.g. such as a filter unit 301 or 401 as comprised in Figures 11 or 12 .
  • the filter unit 301 supplies filter signals to a splitter 504.
  • the filter signals are split / de-multiplexed into a number of filter signal pairs corresponding to the number of antennas to be driven by the present phase array feeder, e.g. 16 signal pairs for a 4x4 antenna array, or into any desired number.
  • each modulation unit 302 of section 502 a phase shift is applied in each modulation units 302 of section 502 to one of the filter signals. If applicable, a phase offset may be applied to a frequency shifted reference signal in these modulation units 302 as well.
  • the signal pairs supplied by each modulation unit 302 are combined in a combination unit 303 each in order to generate output signals, preferably by using photonic mixing in order to generate microwave output signals.
  • each output signal drives a corresponding antenna.
  • each modulation unit 302 applies a modulation of different magnitude, e.g. a different phase shift to one of the filter signals, the output signals differ in the delay time such that the antennas may generate a directed electromagnetic field.
  • FIG. 13 illustrates a block diagram in section 602 with a corresponding modulation unit such as preferably used in each of the modulation units 302 of Figure 12 .
  • a corresponding modulation unit such as preferably used in each of the modulation units 302 of Figure 12 .
  • each modulation unit preferably contains two modulation sub-units.
  • Control signals 632x and 632y for the azimuth and elevation angle respectively drive separate phase modulators 630x and 630y for modulating at least one of the filter signals, and possibly in addition drive separate phase modulators 670x and 670y for modulating a reference signal.
  • each antenna preferably is supplied with an output signal of a different delay in time - which preferably are multiples of a basic delay time - depending on the antenna position.
  • the corresponding modulator length - or amplifier gain - is changed depending on the position on the array while keeping a ratio between the modulation of the filter signal and a modulation of the reference signal constant.
  • the size of the azimuth modulators 630x and 670x will change along one direction of the array, e.g.
  • the system can be driven with only one voltage for X and one voltage for Y.
  • the different time delays for the different antenna elements are then created owed to the different sizes.
  • Another improvement of the array driving structure may be to change a sign of the modulator's effect between the left and right side of the array, for e.g. the azimuth modulator, and the upper and lower side, for e.g. the azimuth modulator, in order to reduce maximum delays requested thought the array, e.g. 2 ⁇ t would be replaced by ⁇ ⁇ t .
  • a wavelength division multiplexing scheme preferably is implemented.
  • FIG 14 depicts an application of one or more tunable time delay elements according to an embodiment of the present invention, where a phase array 701 containing a phase array feeder according to Figure 13 , for example, is used to combine space-division multiple access (SDMA) with a time division multiplexing (TDM) scheme into a space-time division multiplexing.
  • SDMA space-division multiple access
  • TDM time division multiplexing
  • a transmitter array in the form of an array of antennas comprised in the phase array 701 sends short-pulses to different receivers 702 to 704, e.g. represented by mobile phones of users, each receiver 702 to 704 receiving only one symbol of information at the time.
  • the bandwidth of an electronic in the receiver can be dimensioned smaller than the bandwidth to be provided in the transmitter, i.e. the phase array 701, thereby avoiding waste of resources as it is nowadays often the case.
  • a very similar structure as the one proposed for the phase array embodiments but with a different distribution of the control signals preferably is used to generate an orbital angular momentum (OAM).
  • OAM orbital angular momentum
  • a size of the phase shifter - or a gain of an amplifier - may not change along the Cartesian coordinates, e.g. along x and y but along the polar coordinates, e.g. along radius and angle, in order to generated different OAM modes depending on the applied voltage.
  • Such a system could for example be used to encode information not only on the amplitude and phase of the signal - advanced modulation format - but also on a third axis corresponding to the different OAM modes.

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  • Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)
EP14002640.2A 2014-07-29 2014-07-29 Optisches Verzögerungselement Withdrawn EP2980620A1 (de)

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US4976518A (en) * 1989-09-13 1990-12-11 The United States Of America As Represented By The Secretary Of The Navy Fiber optic transversal filter/variable delay line
US5222162A (en) * 1991-11-27 1993-06-22 Hughes Aircraft Company Monolithic integrated optical time delay network for antenna beam steering
EP1326131A1 (de) * 2002-01-08 2003-07-09 Alcatel Variable optische Verzögerungsleitung und Verwendung der variablen optischen Verzögerungsleitung
US20110096338A1 (en) * 2009-10-27 2011-04-28 Fujitsu Optical Components Limited Delay interferometer using magneto-optic effect

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4976518A (en) * 1989-09-13 1990-12-11 The United States Of America As Represented By The Secretary Of The Navy Fiber optic transversal filter/variable delay line
US5222162A (en) * 1991-11-27 1993-06-22 Hughes Aircraft Company Monolithic integrated optical time delay network for antenna beam steering
EP1326131A1 (de) * 2002-01-08 2003-07-09 Alcatel Variable optische Verzögerungsleitung und Verwendung der variablen optischen Verzögerungsleitung
US20110096338A1 (en) * 2009-10-27 2011-04-28 Fujitsu Optical Components Limited Delay interferometer using magneto-optic effect

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