This invention relates to tunable optical delay lines. More particularly it addresses the use of tunable delays in phased array antenna systems.
A phased array is a group of radio frequency antennas in which the relative phases of the respective signals feeding the antennas are varied in such a way that the effective radiation pattern of the array is reinforced in a desired direction and suppressed in undesired directions. In typical embodiments, they incorporate electronic phase shifters that provide a differential delay or phase shift to adjacent radiating elements to tilt the radiated phase front and thereby produce far-field beams in different directions depending on the differential phase shifts applied to the individual elements.
A number of embodiments of delay lines and antenna elements can be arranged in an RF antenna assembly. The antenna assembly may include an array of antenna elements. Such arrays of antenna elements may, in certain embodiments, be spatially arranged in either a non-uniform or uniform pattern to provide the desired antenna assembly characteristics. The configuration of the arrays of antenna elements may affect the shape, strength, operation, and other characteristics of the waveform received or transmitted by the antenna assembly.
The antenna elements may be configured to either generate or receive RF signals. The physical structure of the element for signal generation and reception is similar, and typically a single element is used for both functions. A phase shifter/true time delay (PS/TTD) device is a crucial part of the antenna element providing a differential delay or phase shift to adjacent elements to tilt the radiated/received phase front.
The active phased array antenna architecture is the most applicable to the use of the PS/TTD device. A schematic of one of the embodiments of an active phased array antenna unit is shown in
The tunable delay application is not limited to active phased array antennas. Alternatively, PS/TTDs can be implemented in passive phased array systems, where the power is shared passively between many antenna elements, each having its own PS/TTD device.
Photonics technologies offer significant advantages over RF and microwave electronics, which can be exploited in phased array systems. Optics offer tremendous inherent bandwidth for use in optical processing and communicating systems, due to the very high carrier frequencies (e.g. 200 THz) compared to the microwave signals (10 s GHz) upon which they operate. Photonic technologies offer much lower cost if efficiently integrated. Photonic devices are inherently small due to the short wavelength at which they operate (around 1 micron) compared to the cm and mm wavelengths of microwave integrated circuits in phased array systems. Photonic integration provides a path to massive parallelism, providing additional reductions in size and weight, together with the promise of much lower overall system cost.
Phased array antenna using photonic delay lines is shown in
The optical signal next gets spitted between individual elements, each element containing photonic delay line, detector and the antenna. At the detector the optical signal of frequency ω gets down converted back to the RF of frequency Ω. Coherent addition of RF signals with different delays results in directional emission at angle θ.
This invention relates to optical delay lines based on microresonator structures. One of the most promising delay line designs is a ‘side-coupled integrated spaced sequence of resonators’ (SCISSOR) shown in
Another configuration (
A multitude of phased array systems are used in many applications, varying from large surveillance systems to weapons guidance systems to guided missiles, plus many civil applications including weather monitoring radar systems, radio-astronomy and topography.
There is a need to provide more reliable and efficient devices for tunable delays to control phased array antennas. In the phased array antenna applications each frequency component of optical signal ω is down converted into an RF frequency component of angular frequency Ω with a phase delay ΦRF(Ω). The angle at which the phased array will emit the RF signal can be written as θ=sin−1(cωRF(Ω)/Ωd), where c is the speed of light and d is the distance between antenna elements.
In order to maintain the emission angle frequency-independent, it is required that ΦRF(Ω)/Ω=Td where Td is referred to as the true time delay that must be constant over the whole signal bandwidth. In the state of the art phased arrays the true time delay can be achieved only by using long propagation length, and it cannot be tuned easily. In this invention we propose a compact true time delay line that is also tunable over a wide range.
This invention provides a tunable delay for an optical signal having a carrier frequency and a single side band; these optical signals are used, for example, in microwave photonics systems such as a phased array radar.
In the preferred embodiment the device comprises at least three integrated microresonators having resonance frequencies ω1=ωr−Δω1, ω2=ωr+Δω1, and ω3=ω0±Δω2 respectively, ωr is a median frequency of the side band, ω0 is the carrier frequency, and Δω1,2 are deviations from those frequencies. The third resonator provides a phase delay difference between the phase at the optical carrier frequency Φ(ω0) and the phase at the median signal frequency Φ(ωr) equal to (ω0−ωr)Td, where Td is the time delay. The frequency ω3 is chosen to satisfy the relation Φ(ω0)=Φ(ωr)+Td(ωr)(ω0−ωr). The first two resonators in the group provide tunable group delay for the signal band, while the remaining at least one resonator provides tunable phase delay for the optical carrier. The first and the second resonators eliminate a third order group delay dispersion over the side band frequencies of the signal band using cancellation of the positive dispersion of the first loop resonator by the negative dispersion of equal magnitude of the second loop resonator. This arrangement allows one to operate as a true time delay line for very high frequency but relatively narrow band RF signals.
The ring resonators have radius ranging from about 2 μm to about 50 μm.
The resonator frequencies are tunable using, for example, a thermo-optical effect. In one embodiment the frequencies are tunable slowly using the thermo-optical effect followed by fast tuning using carrier injection or the Stark effect. Using fast tuning the frequencies may be tuned within a range of +/−0.1% within 10 microseconds.
In one embodiment the device consists of at least one cell. The cell contains at least three ring resonators. In another embodiment the device further comprises a fourth resonator, having the same angular frequency as the third resonator. In order to achieve a relatively large delay time, the device includes multiple cells, for example, ten or more cells, each having three or four resonators.
A phased array antenna comprising a tunable delay based on microresonator structures is another object of the present invention.
Yet another object of the present invention is a method for producing a tunable delay of an optical signal having a carrier frequency and a single side band. The method comprises: introducing an input optical signal in a waveguide; coupling the optical signal sequentially to a first loop resonator, a second loop resonator and a third loop resonator; wherein the first, second and third resonators have different resonant angular frequencies ω1, ω2, and ω3; outputting a delayed optical signal, wherein all frequencies of the output optical signal have the same group delay.
a) A ‘side-coupled integrated spaced sequence of resonators’ (SCISSOR) structure; (b) a SCISSOR structure with the resonators coupling on the opposite sides of the core waveguide (prior art).
Optical delay lines typically use near infrared (NIR) light, however the disclosure is not limited to this spectral range. The term “optical” in the present disclosure comprises visible, near infrared, infrared, far infrared and the near and far ultra-violet spectra.
The novel approach is applied to the processing of the optical signal for use in phased array antennas based on separate processing of the optical carrier, the upper sideband, and the lower sideband of the modulated optical signal. This technology has a number of potential implementations, which utilize the ideas of separately controlling the time delay of each signal, and also removing one of the sideband signals through optical filtering. The filtering and also separate control of each signal can be most easily implemented when the modulation frequency is high, so that separation between the optical carrier and sidebands is large. A good example of this would be a 60 GHz RF frequency modulated onto an optical carrier, providing sidebands at +/−60 GHz, also assuming some reasonable bandwidth for each sideband, e.g. 10 GHz. Such an optical signal is shown in
The optical signal in
One way to reduce the required bandwidth of the TTD device is to remove one of the sidebands from the optical signal. On an integrated photonic circuit it is possible to design an optical filter to simply remove one of the sidebands of the optical signal, which provides a single sideband (SSB) signal. SSB modulation cuts the bandwidth requirement of the TTD device almost in half, so that a system at 60 GHz requires only 75 GHz bandwidth, and a system at 35 GHz requires only 50 GHz. This is a significant reduction in required bandwidth, and so for systems operating at high frequencies it is extremely helpful to use SSB modulation.
The invention is focused on implementation of SSB modulation (
a) shows a single ‘cell’ of a microresonator design for a novel TTD device using the described approach. In this description it is assumed that the higher sideband has been filtered from the optical signal before entering the time delay ‘cells’. In this simplest case a cell may include two microresonator elements, one resonant with the sideband and one resonant with the optical carrier. The device is designed so that the delays to the sideband and to the optical carrier are individually tuned to the same value, to provide an overall signal with the correct true time delay. This can be achieved because each of the two microresonator elements is only resonant with one part of the signal—one with the optical carrier and the other with the sideband; the microresonators have little affect on the signal for which they are not resonant.
As can be seen in
The disadvantage of the design shown in
c) and (d) shows another embodiment of the invention. Each cell contains at least four resonators 1, 2, 3 and 4; two (1 and 2) for the signal side band and two (3 and 4) for the carrier. Calculations show that this arrangement allows longer delays to be achieved.
a) shows the basic cell of the proposed structure. Two rings with resonant angular frequencies ω1 and ω2 are tuned below (−) and above (+) the signal frequency ωr:
ω1=ωr+Δω1 and ω2=ωr−Δω1.
The third ring has resonant angular frequency ω3, which is close to the frequency of the optical carrier ωc.
In the relatively narrow region of frequencies within the optical signal side band the straight line (frequency independent delay) can be maintained using the “balanced scissor” arrangement of the parent patent U.S. application Ser. No. 12/205,368 filed Sep. 5, 2008, filed by the same inventive entity. The two resonators with resonant frequencies ω1=ωr+Δω1 and ω2=ωr−Δω1, round trip time τ and a coupling coefficient k=(1−p2)1/2 provide almost frequency independent time delay
Td=2τ(1+ρ)/(1−ρ)+τ3Δω12ρ(1+ρ)/(1−ρ)3
that can also be made tunable by changing Δω1.
However, near the carrier frequency the phase curve deviates significantly from the desired straight line. It is important that the phase curve does not need to follow the dashed line over the entire range between signal and carrier, since there is no power carried in most of that frequency range. It is only necessary for the phase curve to cross the dashed line at the carrier frequency to satisfy the condition Φ(ω0)−Φ(ωr)=(ω0−ωr)Td This condition can be stated as following: the group delay of the signal envelope is equal to the phase delay of the RF carrier and is accomplished in curve (b). This result is achieved by separate control of the ring resonators 3 and 4 to tune them near the carrier frequency and thus change the phase delay there without affecting the phase delay near the signal.
If we introduce a separate resonator of resonant frequency ω3=ω0+Δω2 the phase at the optical carrier frequency becomes
Φ(ω0)=2 tan−1((k2 sin Δω2τ)/(1+ρ2)/(cos Δω2τ−2ρ))
By adjusting Δω2 we can satisfy the equality of envelope and RF carrier delays.
One can introduce a fourth resonator identical to the third resonator in which case
Φ(ω0)=2 tan−1((k2 sin Δω2τ)/(1+ρ2)/(cos Δω2τ−2ρ))
By adjusting Δω2 we can satisfy the equality of envelope and RF carrier delays with smaller Δω2.
Essentially the new configuration looks like a ‘Balanced SCISSOR’ structure from the co-pending U.S. patent application Ser. No. 12/205,368, but differs in the control. Instead of two separate values of index shift it requires three: two of opposite sign±Δn1 for the signal and one separate (hence the name) αn2 for the carrier. Using this structure, rings with smaller coupling coefficients (large finesse) can be used, leading to significantly larger time delay tunability. Results shown in this application are for a tunable delay line that was designed for a 60 GHz RF carrier frequency and using a small coupling coefficient of κ=0.2, however any other parameters can be used.
A variety of technologies could be used for the tunable delay fabrication. In the preferred embodiment an active device is provided including a silicon substrate, an insulator layer, and a top silicon layer, in which the device is fabricated. The device is electronically controlled by injected carriers or by applying an electric field. In another embodiment another (slower) technology is used, which includes silica waveguides on a silicon wafer. These devices use thermal tuning by applying a heater on the resonator or waveguide structure. “Hydex” material, produced by Infinera, CA can be used for this kind of thermally tuned devices; this material has a refractive index between that of silicon and silica. Devices could also be fabricated in III-V compound semiconductors, such as InP or GaAs.
In the preferred embodiment of the present invention, a series of ring resonators is used in the device design. However, the invention is not limited to such configuration. Other embodiments include all variety of resonator types. The invention addresses an assembly of one or more pairs of tunable resonators or filters (or just responses), which when combined together provide the required overall tuning response, that is, a broad range of tunability of the overall group delay (time delay) with limited distortion. The resonators/filters are tuned in opposite directions (in wavelength) so that the combined group delay at the center wavelength between the two resonators/filters is tuned up or down as the responses move away from or towards each other. This approach is applicable to any types of resonators or filters than can be combined (amplitude and phase responses) to give the desired response, which includes micro-ring resonators, Bragg gratings, photonic crystals, free space resonators or some other form of optical resonator or filter of some sort. The device does not need to be flat, and it can also be in 3D—some resonators are spherical, and any kind of 2D or 3D structure could potentially be used. The refractive index is changed in one implementation, but it is also possible to change the coupling coefficient to tune the rings through a physical mechanical movement using MEMS. In another embodiment, the refractive index is kept unchanged while the device is tuned by changing its size.
While the above invention has been described with reference to specific embodiments, these embodiments are intended to be illustrative and not restrictive. The scope of the invention is indicated by the claims below, and all changes that come within the meaning and range of equivalents thereof are intended to be embraced therein.
The application claims priority of U.S. Provisional Patent Application Ser. No. 60/974,502 filed Sep. 24, 2007. This application is also a Continuation-in-part of U.S. patent application Ser. No. 12/205,368 filed Sep. 5, 2008.
This invention was made with U.S. Government support under Contract W31P4Q-07-CO150 with DARPA MTO SBIR Project, and the U.S. Government has certain rights in the invention.
Number | Name | Date | Kind |
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7110632 | Abeles | Sep 2006 | B2 |
Number | Date | Country | |
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20090067772 A1 | Mar 2009 | US |
Number | Date | Country | |
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60974502 | Sep 2007 | US |
Number | Date | Country | |
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Parent | 12205368 | Sep 2008 | US |
Child | 12234614 | US |