Phase calibration in FMCW radar systems
11366199 · 2022-06-21
Assignee
Inventors
- Oliver Lang (Linz, AT)
- Michael GERSTMAIR (Langenstein, AT)
- Alexander Melzer (Neutillmitsch, AT)
- Alexander Onic (Linz, AT)
- Christian Schmid (Linz, AT)
Cpc classification
International classification
G01S13/00
PHYSICS
Abstract
A method for a radar system is described. In accordance with one example implementation, the method comprises generating a frequency-modulated RF oscillator signal and feeding the RF oscillator signal to a first transmitting channel and a second transmitting channel. The method further comprises generating a first RF transmission signal in the first transmitting channel based on the RF oscillator signal, emitting the first RF transmission signal via a first transmitting antenna, receiving a first RF radar signal via a receiving antenna, and converting the first RF radar signal to a baseband, as a result of which a first baseband signal is obtained, which has a first signal component having a first frequency and a first phase, where the first signal component is assignable to direct crosstalk from the first transmitting antenna. This procedure is repeated for the second transmitting channel.
Claims
1. A method comprising: generating a frequency-modulated radio frequency (RF) oscillator signal and providing the RF oscillator signal to a first transmitting channel and a second transmitting channel; generating a first RF transmission signal in the first transmitting channel based on the RF oscillator signal and emitting the first RF transmission signal via a first transmitting antenna; receiving a first RF radar signal via a receiving antenna and converting the first RF radar signal into a baseband, wherein a first baseband signal is obtained, which has a first signal component having a first frequency and a first phase, the first signal component being assignable to direct crosstalk from the first transmitting antenna; generating a second RF transmission signal in the second transmitting channel based on the RF oscillator signal and emitting the second RF transmission signal via a second transmitting antenna; receiving a second RF radar signal via the receiving antenna and converting the second RF radar signal into the baseband, wherein a second baseband signal is obtained, which has a second signal component having a second frequency and a second phase, the second signal component being assignable to direct crosstalk from the second transmitting antenna; determining the first phase based on the first baseband signal and determining the second phase based on the second baseband signal; and determining a value representing a difference between a phase shift caused by the first transmitting channel and a phase shift caused by the second transmitting channel, based on the first phase and the second phase and further based on parameters, representing a phase shift on account of the direct crosstalk from the first transmitting antenna and the direct crosstalk from the second transmitting antenna.
2. The method as claimed in claim 1, wherein converting the first RF radar signal and the second RF radar signal to the baseband is carried out in each case by mixing with an RF reference signal, wherein the RF reference signal and the RF oscillator signal are frequency-shifted with respect to one another by a frequency offset.
3. The method as claimed in claim 2, wherein the RF reference signal is generated by a local oscillator and the RF oscillator signal is generated from the RF reference signal using modulation with a modulation signal of constant frequency.
4. The method as claimed in claim 2, wherein the RF oscillator signal is generated by a local oscillator and the RF reference signal is generated from the RF oscillator signal by modulation with a modulation signal of constant frequency.
5. The method as claimed in claim 1, wherein the first baseband signal and/or the second baseband signal are/is frequency-shifted by a frequency offset using modulation.
6. The method as claimed in claim 1, further comprising: adapting a phase shift in the first transmitting channel and/or the second transmitting channel based on the value representing the difference between the phase shift caused by the first transmitting channel and the phase shift caused by the second transmitting channel.
7. The method as claimed in claim 6, wherein the first baseband signal has a further signal component having a third frequency and a third phase, the further signal component being assignable to indirect crosstalk from the first transmitting antenna; and wherein determining the first phase comprises: estimating the further signal component based on the first baseband signal; subtracting the estimated further signal component from the first baseband signal; and estimating the first signal component assignable to the direct crosstalk based on the first baseband signal remaining after subtracting the estimated further signal component.
8. A radar device comprising: a first transmitting channel having an output for connection of a first transmitting antenna; a second transmitting channel having an output for connection of a second transmitting antenna; a local oscillator configured to generate a frequency-modulated radio frequency (RF) oscillator signal, wherein the local oscillator is connectable to the first transmitting channel and the second transmitting channel in order to provide the RF oscillator signal to the first transmitting channel and the second transmitting channel; a receiving channel connectable to a receiving antenna, wherein the receiving channel is configured to: receive a first RF radar signal belonging to the first transmitting channel and mix the first RF radar signal with a baseband, wherein a first baseband signal is obtained, which has a first signal component having a first frequency and a first phase, the first signal component being assignable to direct crosstalk from the first transmitting antenna; and receive a second RF radar signal belonging to the second transmitting channel and mix the second RF radar signal with a baseband, wherein a second baseband signal is obtained, which has a second signal component having a second frequency and a second phase, the second signal component being assignable to direct crosstalk from the second transmitting antenna; and a computing unit coupled to the receiving channel and configured to: determine the first phase based on the first baseband signal and determine the second phase based on the second baseband signal; and determine a value representing a difference between a phase shift caused by the first transmitting channel and a phase shift caused by the second transmitting channel, based on the first phase and the second phase and further based on parameters, representing a phase shift on account of the direct crosstalk from the first transmitting antenna and the direct crosstalk from the second transmitting antenna.
9. The radar device of claim 8, further comprising one or more processors configured to: adapt a phase shift in the first transmitting channel and/or the second transmitting channel based on the value representing the difference between the phase shift caused by the first transmitting channel and the phase shift caused by the second transmitting channel.
10. A device, comprising: one or more memories; and one or more processors, coupled to the one or more memories, configured to: generate a frequency-modulated radio frequency (RF) oscillator signal and providing the RF oscillator signal to a first transmitting channel and a second transmitting channel; generate a first RF transmission signal in the first transmitting channel based on the RF oscillator signal and emitting the first RF transmission signal via a first transmitting antenna; receive a first RF radar signal via a receiving antenna and converting the first RF radar signal into a baseband, wherein a first baseband signal is obtained, which has a first signal component having a first frequency and a first phase, the first signal component being assignable to direct crosstalk from the first transmitting antenna; generate a second RF transmission signal in the second transmitting channel based on the RF oscillator signal and emitting the second RF transmission signal via a second transmitting antenna; receive a second RF radar signal via the receiving antenna and converting the second RF radar signal into the baseband, wherein a second baseband signal is obtained, which has a second signal component having a second frequency and a second phase, the second signal component being assignable to direct crosstalk from the second transmitting antenna; determine the first phase based on the first baseband signal and determining the second phase based on the second baseband signal; and determine a value representing a difference between a phase shift caused by the first transmitting channel and a phase shift caused by the second transmitting channel, based on the first phase and the second phase and further based on parameters, representing a phase shift on account of the direct crosstalk from the first transmitting antenna and the direct crosstalk from the second transmitting antenna.
11. The device of claim 10, wherein converting the first RF radar signal and the second RF radar signal to the baseband is carried out in each case by mixing with an RF reference signal, wherein the RF reference signal and the RF oscillator signal are frequency-shifted with respect to one another by a frequency offset.
12. The device of claim 11, wherein the RF reference signal is generated by a local oscillator and the RF oscillator signal is generated from the RF reference signal using modulation with a modulation signal of constant frequency.
13. The device of claim 11, wherein the RF oscillator signal is generated by a local oscillator and the RF reference signal is generated from the RF oscillator signal by modulation with a modulation signal of constant frequency.
14. The device of claim 10, wherein the one or more processors are further configured to: adapt a phase shift in the first transmitting channel and/or the second transmitting channel based on the value representing the difference between the phase shift caused by the first transmitting channel and the phase shift caused by the second transmitting channel.
15. The device of claim 14, wherein the first baseband signal has a further signal component having a third frequency and a third phase, the further signal component being assignable to indirect crosstalk from the first transmitting antenna, and wherein the one or more processors, to determine the first phase, are configured to: estimate the further signal component based on the first baseband signal; subtract the estimated further signal component from the first baseband signal; and estimate the first signal component assignable to the direct crosstalk based on the first baseband signal remaining after subtracting the estimated further signal component.
16. A non-transitory computer-readable medium storing a set of instructions, the set of instructions comprising: one or more instructions that, when executed by one or more processors of a device, cause the device to: generate a frequency-modulated radio frequency (RF) oscillator signal and providing the RF oscillator signal to a first transmitting channel and a second transmitting channel; generate a first RF transmission signal in the first transmitting channel based on the RF oscillator signal and emitting the first RF transmission signal via a first transmitting antenna; receive a first RF radar signal via a receiving antenna and converting the first RF radar signal into a baseband, wherein a first baseband signal is obtained, which has a first signal component having a first frequency and a first phase, the first signal component being assignable to direct crosstalk from the first transmitting antenna; generate a second RF transmission signal in the second transmitting channel based on the RF oscillator signal and emitting the second RF transmission signal via a second transmitting antenna; receive a second RF radar signal via the receiving antenna and converting the second RF radar signal into the baseband, wherein a second baseband signal is obtained, which has a second signal component having a second frequency and a second phase, the second signal component being assignable to direct crosstalk from the second transmitting antenna; determine the first phase based on the first baseband signal and determining the second phase based on the second baseband signal; and determine a value representing a difference between a phase shift caused by the first transmitting channel and a phase shift caused by the second transmitting channel, based on the first phase and the second phase and further based on parameters, representing a phase shift on account of the direct crosstalk from the first transmitting antenna and the direct crosstalk from the second transmitting antenna.
17. The non-transitory computer-readable medium of claim 16, wherein converting the first RF radar signal and the second RF radar signal to the baseband is carried out in each case by mixing with an RF reference signal, wherein the RF reference signal and the RF oscillator signal are frequency-shifted with respect to one another by a frequency offset.
18. The non-transitory computer-readable medium of claim 17, wherein the RF reference signal is generated by a local oscillator and the RF oscillator signal is generated from the RF reference signal using modulation with a modulation signal of constant frequency.
19. The non-transitory computer-readable medium of claim 17, wherein the RF oscillator signal is generated by a local oscillator and the RF reference signal is generated from the RF oscillator signal by modulation with a modulation signal of constant frequency.
20. The radar device of claim 9, wherein the first baseband signal has a further signal component having a third frequency and a third phase, the further signal component being assignable to indirect crosstalk from the first transmitting antenna, and wherein the computing unit, to determine the first phase, are configured to: estimate the further signal component based on the first baseband signal; subtract the estimated further signal component from the first baseband signal; and estimate the first signal component assignable to the direct crosstalk based on the first baseband signal remaining after subtracting the estimated further signal component.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
(1) Example implementations are explained in greater detail below with reference to figures. The illustrations are not necessarily to scale and the example implementations are not restricted only to the aspects illustrated. Rather, the figures illustrate the principles underlying the example implementations.
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DETAILED DESCRIPTION
(16)
(17) In the present example, the radar device 1 comprises separate transmitting (TX) and receiving (RX) antennas 5 and 6 respectively (bistatic or pseudo-monostatic radar configuration). It should be noted, however, that a single antenna can also be used, which serves simultaneously as transmitting antenna and as receiving antenna (monostatic radar configuration). The transmitting antenna 5 emits a continuous RF signal s.sub.RF(t), which is frequency-modulated for example with a type of sawtooth signal (periodic, linear frequency ramp). The emitted RF radar signal s.sub.RF(t) is backscattered at the radar target T and the backscattered/reflected signal y.sub.RF(t) (echo signal) is received by the receiving antenna 6.
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(19) A radar echo signal y.sub.RF(t) received via an RX antenna is a temporally shifted (delay time τ) and scaled version of the radar signal s.sub.RF(t) emitted via the associated TX antenna (cf.
τ=Δf.Math.T.sub.CHIRP/B=Δf/k. (1)
The roundtrip delay time τ corresponds to a distance x=c.Math.τ (c denotes the speed of light) covered by the radar signal. The frequency offset Δf measured by the radar device (by down-converting the radar echo signal and spectral analysis) contains information about the round-trip delay time of the radar signal and thus also about the path distance x covered by the radar signal.
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(21) The example illustrated shows a bistatic (or pseudo-monostatic) radar system comprising separate RX and TX antennas. In the case of a monostatic radar system, the same antenna would be used both for emitting and for receiving the electromagnetic (radar) signals. In this case, by way of example, a directional coupler (e.g. a circulator) can be used to separate the RF signals to be emitted from the received RF signals (radar echo signals). As mentioned, radar systems in practice usually comprise a plurality of transmitting and receiving channels having a plurality of transmitting and receiving antennas, respectively, which makes it possible, inter alia, to measure the direction (Direction of Arrival, DoA) from which the radar echoes are received. In Multiple-Input Multiple-Output (MIMO) systems of this type, the individual (physical) TX channels and RX channels are usually constructed identically or similarly in each case. From a plurality of TX antennas and RX antennas, it is possible to form so-called virtual antenna arrays, which can be used for implementing beamforming techniques. By way of example, a system comprising three TX antennas and four RX channels can be used to implement an antenna array comprising 12 (three times four) virtual antenna elements. The phase differences between the emitted antenna signals (or the RF output signals of the TX channels) are of importance for the application of beamforming techniques.
(22) In the case of an FMCW radar system, the RF signals emitted via the TX antenna(s) 5 can lie e.g. in the range of approximately 20 GHz to 100 GHz (e.g. around 77 GHz in some applications). However, this range is merely one example and other frequencies are also possible. As mentioned, the RF signal received by each RX antenna 6 comprises radar echoes (chirp echo signals), e.g. those signal components which are backscattered at one or at a plurality of radar targets. In each RX channel, the received RF signal y.sub.RF(t) is down-converted to the baseband and can be processed further in the baseband using analog signal processing (see
(23) The overall system is generally controlled via a system controller 50, which can likewise be implemented at least partly via software/firmware which is executed on a processor such as e.g. a microcontroller. The RF frontend 10 and the analog baseband signal processing chain 20 (optionally also the analog-to-digital convertor 30 and the computing unit 40) can be jointly integrated in a single MMIC (e.g. an RF semiconductor chip). Alternatively, the individual components can also be distributed among a plurality of integrated circuits (MMICs). In order to simplify the illustration, and since it is not necessary for the further explanations, hereinafter no distinction is drawn between “Single-Chip”radar systems and distributed radar systems and it goes without saying that the example implementations described here can be implemented both as single-chip systems and as distributed radar systems. The examples in
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(25) The RF frontend 10 comprises a local oscillator 101 (LO), which generates an RF oscillator signal s.sub.LO(t). The RF oscillator signal s.sub.LO(t) is frequency-modulated during operation, as described above with reference to
(26) The RF transmission signal s.sub.RF(t) (cf.
(27) The down-converted baseband signal (mixer output signal) is designated below by y.sub.BB(t). Said baseband signal y.sub.BB(t) is firstly processed further in analog fashion, wherein the analog baseband signal processing chain 20 substantially brings about further amplification and (e.g. bandpass or low-pass) filtering in order to suppress undesired sidebands and image frequencies. The resulting analog output signal of the receiving channel RX1, which is fed to an analog-to-digital convertor (see
(28) In the present example, the mixer 104 down-converts the preamplified RF reception signal g.Math.y.sub.RF(t) (e.g. the amplified antenna signal) to the baseband. The mixing can take place in one stage (that is to say from the RF band directly to the baseband) or via one or more intermediate stages (that is to say from the RF band to an intermediate frequency band and further to the baseband). In this case, the reception mixer 104 effectively comprises a plurality of individual mixer stages connected in series. The mixer 104 can be implemented in various ways. In some example implementations, an IQ demodulator (in-phase/quadrature-phase demodulator) can be used as the mixer 104, which has the consequence that the (digital) baseband signal y[n] is a complex-valued signal. Normal mixers that yield a real baseband signal y[n] are used in other example implementations. The concepts described here are applicable to both variants.
(29) In the case of radar systems comprising a plurality of TX channels and a plurality of RX channels (so-called Multi-Input/Multi-Output (MIMO) systems), it is beneficial for the phases of radar signals emitted via different TX channels to correspond to a specified value. As mentioned in the introduction, a virtual antenna array comprising a plurality of virtual receiving antennas/channels can be formed in a MIMO radar system. For this purpose, it may be beneficial that, in particular, the relative phases (e.g. the respective phase differences) of the radar signals emitted via different TX channels have defined values. However, the phase shift ΔΦ caused by a TX channel is dependent on unavoidable tolerances during production and additionally has cross-sensitivities, e.g. in relation to temperature. Furthermore, aging effects can alter the phase over the course of time. For this reason, modern radar systems comprise circuit components that allow a setting of the phases of the radar signals emitted via the different TX channels. For this purpose, the TX channels can have phase shifters (cf.
(30) The example implementations described here utilize the unavoidable crosstalk between TX channels and RX channels to carry out a phase calibration.
(31) Assuming that s.sub.LO(t)=cos(2πf.sub.LOt) holds true for the LO signal fed to the modulator, then s.sub.LO′(t)=cos(2π(f.sub.LO−f.sub.MOD)t) holds true for the output signal s.sub.LO′(t) of the modulator. The amplitude of the LO signal is assumed to be one, without restricting the generality. In a simplified consideration, possible phase shifts can be ascribed to the phase shifts ΔΦ.sub.1, ΔΦ.sub.2 of the TX channels TX1 and TX2, respectively. For the radar signals emitted by the TX antennas 5 it thus holds true that
s.sub.RF,k(t)=A.sub.k cos(2π(f.sub.LO−f.sub.MOD)t+ΔΦ.sub.k), (2)
wherein the index k denotes the channel, e.g. k={1, 2} in the present example with two channels. The output of the modulator 106 is connected to the TX channels TX1, TX2 via the RF switch SW. During a frequency ramp, the frequency f.sub.LO is not constant, but rather rises (in the case of an up-chirp) linearly, e.g.
f.sub.LO=f.sub.START+k.Math.t (3)
and from this it follows (cf. Equation 2) for the output signal of the k-th channel TXk that:
s.sub.RF,k(t)=A.sub.k COS(2π(f.sub.START−f.sub.MOD)t+kπt.sup.2+ΔΦk). (4)
The time derivative of the argument of the cosine function from equation 4 divided by 2 π yields the instantaneous frequency in accordance with equation 3. The modulated (frequency-shifted) LO signal s.sub.LO′(t) is fed to one of the TX channels depending on the switch position. The ADC 30 has been omitted in
(32) As mentioned, crosstalk is always present in FMCW radar systems. Direct crosstalk denotes the effect that a transmission signal emitted via a transmitting antenna is received again by a receiving antenna directly—e.g. without reflection at an object.
(33) In addition to direct crosstalk, in practice indirect crosstalk often occurs, in the case of which the emitted radar signal is reflected at an obstacle situated very near the antenna. Such obstacles are sometimes also referred to as Short-Range Targets, and the (indirect) crosstalk associated therewith is often also referred to as “Short-Range Leakage”. In applications in the automotive field, such a Short-Range Target can be formed for example by the fender of an automobile. In
(34) Both direct crosstalk and indirect crosstalk have an effect in the resulting baseband signal y.sub.BB(t) that is similar to the effect of a radar target situated very near the antennas. The round-trip delay times τ.sub.1 and τ.sub.2 and also τ.sub.B1 and τ.sub.B2 are so short that the resulting frequency offsets in accordance with equation 1 are very small (e.g. close to zero hertz, designated as Δf in equation 1). In many applications, radar frontends are usually implemented in such a way that such small frequencies are eliminated by the analog baseband signal processing chain 20 (e.g. high-pass filter or bandpass filter). Accordingly, the output signal y(t) and the digital baseband signal y[n] no longer contain these small frequencies. As a result of the frequency shift by the modulation frequency f.sub.MOD that is brought about by the modulator 106, the frequency offsets mentioned are increased by the value f.sub.MOD. In the example illustrated in
f.sub.1=τ.sub.1k+f.sub.MOD≈f.sub.MOD, (5)
f.sub.B1=τ.sub.B1k+f.sub.MOD, (6)
f.sub.2=τ.sub.2k+f.sub.MOD≈f.sub.MOD and (7)
f.sub.B2=τ.sub.B2k+f.sub.MOD, (8)
for the crosstalk from the transmitting channel TX1 to the receiving channel RX1 and respectively the crosstalk from the transmitting channel TX2 to the receiving channel RX1. However, the round-trip delay times τ.sub.1 and τ.sub.2 are so small (in comparison with f.sub.MOD) that the frequencies f.sub.1 and f.sub.2 are practically equal to the modulation frequency f.sub.MOD. The phase values φ.sub.1, and φ.sub.2 associated with the frequencies f.sub.1 and f.sub.2 can be measured based on the digital radar signal y[n]. For this purpose, the modulated (frequency-shifted) LO signal s.sub.LO′(t) is firstly passed through the TX channel TX1 and the resulting output signal y[n] of the RX channel RX1 is measured. Using spectral analysis, the phase φ.sub.1 at the frequency f.sub.1 can be determined from this digital radar signal y[n]. This process is repeated with the TX channel TX2 in order to determine a value for the phase φ.sub.2. In the case of a general MIMO system, this process can be repeated for every available TX channel/RX channel pair.
(35) The modulator 106 can be inactive during normal radar operation (e.g. for the measurement of position and speed of a radar target). By way of example, during normal radar operation, the modulator 106 can be bypassed, or the modulation frequency f.sub.MOD can be set to zero. The modulator 106 also need not necessarily be in the signal path from the local oscillator to the TX channel under consideration. Alternatively, the modulator can also be arranged in the signal path from the local oscillator to the RX path (cf. e.g.
(36) It can be shown that the phase shifts φ.sub.1 and φ.sub.2 (measurement values) assigned to the frequencies f.sub.1 and f.sub.2 are constituted as follows:
φ.sub.1=Φ.sub.1−ΔΦ.sub.1+Φ.sub.RX and (9)
φ.sub.2=Φ.sub.2−ΔΦ.sub.2+Φ.sub.RX. (10)
In this case, ΔΦ.sub.1 and ΔΦ.sub.2 denote the unknown phase shifts in the TX channels TX1 and TX2, respectively, Φ.sub.1 and Φ.sub.2 denote the phases on account of the round-trip delay times τ.sub.1 and τ.sub.2 between the respective antennas, and Φ.sub.RX denotes a constant phase offset in the RX channel. The phases Φ.sub.1 and Φ.sub.2 can be calculated as follows
Φ.sub.1=2π(f.sub.START−f.sub.MOD)τ.sub.1−πkτ.sub.1.sup.2 and (11)
Φ.sub.2=2π(f.sub.START−f.sub.MOD)τ.sub.2−πkτ.sub.2.sup.2, (12)
wherein τ.sub.1=d.sub.1/c and τ.sub.2=d.sub.2/c hold true for the round-trip delay times. The phases Φ.sub.1 and Φ.sub.2 are thus system parameters (design parameters) known a priori for a specific radar system in which the distances d.sub.1 and d.sub.2, respectively, between the antennas are known.
(37) The difference ΔΦ.sub.2−ΔΦ.sub.1 can be calculated based on equations (9) and (10) as follows (equations 9 and 10 are subtracted):
ΔΦ.sub.2−ΔΦ.sub.1=(φ.sub.1−Φ.sub.1)−(φ.sub.2−Φ.sub.2)=(φ.sub.1−φ.sub.2)−(Φ.sub.1−Φ.sub.2). (13)
Based on this phase difference ΔΦ.sub.2−ΔΦ.sub.1 calculated from measurement values (e.g. φ.sub.1 and φ.sub.2) and known system parameters (e.g. Φ.sub.1 and Φ.sub.2), the phase shift ΔΦ.sub.2 can be altered for example using the phase shifter 105 arranged in the TX channel TX2 in such a way that the phase difference ΔΦ.sub.2−ΔΦ.sub.1 corresponds to a desired setpoint value. The phase offset Φ.sub.RX in the RX channel cancels out on account of the difference formation.
(38) As mentioned, the measurement values φ.sub.1 and φ.sub.2 can be determined based on the output signals y(t) and y[n], respectively, of the RX channel. The left-hand diagram (a) in
(39) In the example described above, the phases Φ.sub.1 and Φ.sub.2 on account of the round-trip delay times τ.sub.1 and τ.sub.2, respectively, are known system parameters that can be calculated based on the distances d.sub.1 and d.sub.2 of the antennas (cf. equations 11 and 12). A possibility that enables these phases Φ.sub.1 and Φ.sub.2 also to be ascertained using measurements is explained below. These measurements can be carried out e.g. in the context of an end-of-line (EOL) test.
(40) The measured phase φ.sub.R is constituted as follows (cf. equations 9 and 10)
φ.sub.R=Φ.sub.R−ΔΦ.sub.1+Φ.sub.RX, (14)
wherein the phase Φ.sub.R on account of the round-trip delay time τ.sub.R can be calculated as follows (cf. equations 11 and 12)
Φ.sub.R=2π(f.sub.START−f.sub.MOD)τ.sub.R−πkτ.sub.R.sup.2. (15)
The phase shift ΔΦ.sub.1 in turn denotes the phase shift in the TX channel TX1. The round-trip delay time τ.sub.R can be calculated simply from the distance of the radar reflector (doubled distance divided by the speed of light), and the phase Φ.sub.R follows directly from the round-trip delay time τ.sub.R in accordance with equation 15.
(41) Direct crosstalk causes, in the spectrum of the digital radar signal y[n], a spectral line at the frequency f.sub.1=τ.sub.1k+f.sub.MOD(see equation 5) with an associated phase φ.sub.1. From equations (9) and (14), the following arises for the phase difference φ.sub.1−φ.sub.R
φ.sub.1−φ.sub.R=Φ.sub.1−Φ.sub.R. (16)
The sought phase shift Φ.sub.1 which can be assigned to the round-trip delay time τ.sub.1 follows directly from equations 15 and 16
Φ.sub.1=(φ.sub.1−φ.sub.R)+2π(f.sub.START−f.sub.MOD)τ.sub.R−πkτ.sub.R.sup.2. (17)
The same procedure can be used for the TX channel TX2 in order to determine the phase Φ.sub.2. These values Φ.sub.1 and Φ.sub.2 can be stored and used later in a real application (e.g. in the example explained above with reference to
(42) The method just described (represented by equations 14 to 17) for ascertaining Φ.sub.1 and Φ.sub.2 uses an exact determination of the round-trip delay time τ.sub.R of the radar signal to the radar reflector 7 and back again. Under certain circumstances, this round-trip delay time, which is proportional to the distance between the antennas and the reflector 7, is not always determinable with sufficient accuracy. This problem can be avoided with the following approach. The overriding goal is to ascertain the difference between the phase delays ΔΦ.sub.2−ΔΦ.sub.1 in the TX channels TX1 and TX2. According to equation 13, for this only the difference Φ.sub.1−Φ.sub.2 is used; the individual values of the phase shifts Φ.sub.1 and Φ.sub.2 are not relevant. This difference Φ.sub.1−Φ.sub.2 can be determined as follows. A radar reflector 7 is positioned in front of the radar system such that it is at a horizontal angle (azimuth angle) and a vertical angle (elevation angle) of zero degrees with respect to the radar system. The round-trip delay times (RTDTs) of the radar signals of all the TX channels to the radar reflector 7 and back to the RX antenna are thus approximately identical (applying the far-field assumption). Given an identical round-trip delay time, the phase delays Φ.sub.R caused by the round-trip delay time τ.sub.R are also identical for all the TX antennas. In the case of a single measurement (e.g. via the TX channel TX1), a phase of φ.sub.R,1=Φ.sub.R−ΔΦ.sub.1+Φ.sub.RX can be observed for the spectral line at the frequency f.sub.R=kτ.sub.R+f.sub.MOD. In the case of a further measurement (e.g. via the TX channel TX2), a phase of φ.sub.R,2=Φ.sub.R−ΔΦ.sub.2+Φ.sub.RX can be observed at the same spectral line. Subtracting these two measurement values φ.sub.R,1 and φ.sub.R,2 yields the difference between the phase delays
ΔΦ.sub.2−ΔΦ.sub.1=φ.sub.R,1−φ.sub.R,2 (18)
(43) In a further step, the phases on account of direct crosstalk are measured as described further above (cf. equations 9 to 13). In this measurement, the phases φ.sub.1 and φ.sub.2 are obtained as measurement values. Rearranging equation 13 and substituting the difference ΔΦ.sub.2−ΔΦ.sub.1 in accordance with equation 18 yields
Φ.sub.1−Φ.sub.2=(φ.sub.1−φ.sub.2)−(ΔΦ.sub.2−ΔΦ.sub.1)=(φ.sub.1−φ.sub.2)−(φ.sub.R,1−φ.sub.R,2). (19)
After the conclusion of the calibration procedure carried out with the aid of the radar reflector 7, this difference Φ.sub.1−Φ.sub.z can be stored and used later in a real application (such as e.g. in the example explained above with reference to
(44) RELAX algorithm—As mentioned above with reference to
(45) The RELAX algorithm makes use of an iterative method. In accordance with
(46) The method shown in
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(48)
(49) Unlike in the example from
(50) The example from
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(52)
(53) The example from
(54) In the present example, the digital radar signal y[n] can be used to detect radar targets. Various signal processing techniques are known for this purpose, for example range Doppler analysis. The digital radar signal y′[n] can be used for the phase monitoring, wherein the calculation of the phase shifts ΔΦ.sub.1 and ΔΦ.sub.2 in the TX channels TX1 and TX2, respectively, can be separately determined and monitored as explained above with reference to
(55)
(56) The method further comprises generating a first RF transmission signal in the first transmitting channel (see e.g.
(57) The method further comprises determining the first phase φ.sub.1 based on the first baseband signal and determining the second phase φ.sub.2 based on the second baseband signal (see
(58) Once the difference ΔΦ.sub.2−ΔΦ.sub.1 has been determined, the phase shifts ΔΦ.sub.1, ΔΦ.sub.2 of the transmitting channels TX1, TX2 can be set (calibrated) such that the difference ΔΦ.sub.2−ΔΦ.sub.1 assumes a desired value. This calibrating can be carried out e.g. with the aid of the phase shifters 105, contained in the transmitting channels (cf.
(59) Even though particular combinations of features are recited in the claims and/or disclosed in the specification, these combinations are not intended to limit the disclosure of various implementations. In fact, many of these features may be combined in ways not specifically recited in the claims and/or disclosed in the specification. Although each dependent claim listed below may directly depend on only one claim, the disclosure of various implementations includes each dependent claim in combination with every other claim in the claim set.
(60) No element, act, or instruction used herein should be construed as critical or essential unless explicitly described as such. Also, as used herein, the articles “a” and “an” are intended to include one or more items, and may be used interchangeably with “one or more.” Further, as used herein, the article “the” is intended to include one or more items referenced in connection with the article “the” and may be used interchangeably with “the one or more.” Furthermore, as used herein, the term “set” is intended to include one or more items (e.g., related items, unrelated items, a combination of related and unrelated items, etc.), and may be used interchangeably with “one or more.” Where only one item is intended, the phrase “only one” or similar language is used. Also, as used herein, the terms “has,” “have,” “having,” or the like are intended to be open-ended terms. Further, the phrase “based on” is intended to mean “based, at least in part, on” unless explicitly stated otherwise. Also, as used herein, the term “or” is intended to be inclusive when used in a series and may be used interchangeably with “and/or,” unless explicitly stated otherwise (e.g., if used in combination with “either” or “only one of”).