This Application is a Section 371 National Stage Application of International Application No. PCT/EP2018/084244, filed Dec. 10, 2018, which is incorporated by reference in its entirety and published as WO 2019/121122 A1 on Jun. 27, 2019, not in English.
The field of the invention is that of digital sample interpolation.
More precisely, the invention concerns a digital interpolation filter with a configurable frequency response.
Such a filter is particularly useful for changing the sampling rate of signals with a variable frequency environment. Thus, the invention has many applications, particularly, but not exclusively, in the field of radio-frequency signal reception or audio-frequency signal processing.
interpolation filters are digital filters that are used to calculate the value of a signal at instants when digital samples of the signal in question are not available.
For example, an interpolation filter has, as input, N available samples of the signal to be interpolated, as well as a parameter representative of the sampling instants at which samples of the signal are to be calculated. The filter then provides an approximation of the signal value at the desired instants as defined by the parameter in question.
Classically, the filters used to perform such a function are based on a polynomial interpolation of the input samples.
A commonly used structure to implement such a polynomial interpolation is the Farrow structure described in the article by Farrow, C. W. “A continuously variable digital delay element Circuits and Systems”, IEEE International Symposium on, 1988, 2641-2645 vol. 3. Indeed, the Farrow structure enables a polynomial interpolation to be implemented regardless of the nature of the polynomials considered, which partly explains its success.
In this case, the parameter representative of the sampling instants of the filter output signal usually defines a delay (e.g. a fraction of the sampling period) with respect to the sampling instants of the samples available at the filter input. If necessary, such a delay can be made variable and reprogrammable on-the-fly between two samples also to allow a change in sampling frequency. In practice, the delay in question can a priori be arbitrary, only the hardware implementation constraints limiting the granularity of this parameter.
However, such a Farrow structure has a significant computational complexity. This is why structures derived from the Farrow structure have been proposed to reduce computational complexity.
An example can be cited of the symmetric Farrow structure described in Valimaki, V. “A new filter implementation strategy for Lagrange interpolation”, Circuits and Systems, 1995. ISCAS '95, 1995 IEEE International Symposium on, Seattle, Wash., 1995, pp. 361-364 vol. 1. Such a structure keeps the advantage of being applicable to any type of polynomial, but provides little implementation gain. In particular, the complexity remains proportional to the square of the order of the implemented interpolation.
Alternatively, a structure called Newton's structure, described in the article by Tassart, S., Depalle, P. “Fractional delay lines using Lagrange interpolation”, Proceedings of the 1996 International Computer Music Conference, Hong Kong, April 1996, p 341-343, derived from Farrow's structure, makes it possible to obtain a reduced computational complexity, proportional to the order of the implemented interpolation. However, such a structure only allows interpolations based on Lagrange polynomials.
However, such a structure has been generalized into a Newton-like structure described in the article by Lamb, D., Chamon, L., Nascimento, V. “Efficient filtering structure for spline interpolation and decimation”, Electronics Letters, IET, 2015, 52, p 39-41. Such a quasi-Newton structure enables a computational complexity proportional to the order of the implemented interpolation to be kept, but for an interpolation based on Spline polynomials.
However, regardless of the filter structure considered, once the order and, where appropriate, the nature of the polynomials used for interpolation have been chosen, the filtering template is fixed.
However, some applications requiring such a change of rhythm would benefit from having an adaptive frequency response of the interpolation filter in question. For example, when implementing a multi-mode receiver, the environment of the signal to be received (in terms of interfering signals, etc.) depends on the standard in question.
The current solution is to completely reconfigure the interpolation filter response, particularly in terms of the nature of the interpolation polynomials, to adapt it to the new standard of the received signal when switching from one standard to another. In this case, this requires the use of a filter structure enabling any type of polynomial interpolation to be implemented. As discussed above, only the Farrow structure, whether symmetric or not, offers such flexibility. However, such a structure is complex in terms of computational load. Furthermore, such an approach requires calculating and/or storing a complete set of filter parameters for each reception configuration to be addressed. In practice, this limits such an approach to a few reception configurations.
There is therefore a need for an interpolation filter with a frequency and time response that can be configured for a reduced number of parameters.
There is also a need for such a filter to be simple in terms of hardware implementation.
In one embodiment of the invention, a digital fractional delay device is provided comprising a digital interpolation filter delivering a series of output samples approximating a signal x(t) at sampling instants of the form (n+d)Ts based on a series of input samples of the signal x(t) taken at sampling instants of the form nTs, with n being an integer, Ts a sampling period and d a real number. Such a filter implements a transfer function in the Z-transform domain, Hcd(Z−1), expressed as a linear combination between:
Hence, the invention proposes a new and inventive solution to allow a simple hardware implementation of an interpolation filter with a configurable frequency and time response.
To do this, the hardware structure implementing the second transfer function comprises at least the Newton structure implementing the first transfer function. The overall hardware implementation of the interpolation filter thus takes advantage of the synergy between the two structures and the efficiency of the implementation of the Newton structure.
Moreover, the linear combination allows the global response of the interpolation filter to be configured in a simple manner between the responses of the two polynomial interpolations in question.
According to one embodiment, the linear combination of the first H1d(Z−1) and second H2d(Z−1) transfer functions is expressed as:
Hcd(Z−1)=H1d(Z−1)+c(H2d(Z−1)−H1d(Z−1))
According to one embodiment, the other structure is a quasi-Newton structure (as defined in Part 5 of this patent application).
Thus, the hardware implementation of the second transfer function is also particularly efficient, and thus that of the global interpolation filter as well.
According to one embodiment, the other polynomial interpolation of the input samples belongs to the group comprising:
Thus, the quasi-Newton structure implementing the second transfer function is obtained directly and simply by using known synthesis methods.
According to one embodiment:
Thus, the first transfer function (representing a Lagrange interpolation) and the second transfer function are expressed at least partly on the same transform base corresponding to a hardware implementation in a particularly efficient form (i.e. according to a Newton structure).
In this way, reusing the Newton structure implementing the first transfer function to implement the second transfer function is simple and efficient.
According to one embodiment, the real number d is included in the segment [−N/2; 1−N/2[, the order of the Lagrange interpolation being equal to N−1, with N an integer. The second transfer function H2d(Z−1) is expressed as:
with qn,m elements of a matrix Q of N rows and N columns, the matrix Q expressed as a product of matrices:
Q=(TdT)−1PTz−1
where:
with pi,j a row index element i and a column index element j of the matrix P, the N polynomials βj (μ) verifying βj (μ)=+βN−j+1(μ) or βj(μ)=βN−j+1(μ).
Thus, an expression of the second transfer function on the transform base (i.e. based on polynomials of the form (1−Z−1)k, with k an integer) is easily obtained, regardless of the nature of the polynomial interpolation associated with the second transfer function. Indeed, a symmetric Farrow matrix can be obtained for a polynomial interpolation whatever the nature of the polynomials in question.
According to one embodiment, the transfer function H2μ(Z−1) represents a symmetric Farrow structure implementing a Spline or Hermit polynomial interpolation of the input samples.
According to one embodiment, the matrix Td is expressed as a product of matrices Td=T2dTd1, with Td1 and Td2 two matrices of N rows and N columns, at least one element, Td1[i,j], of row index i and column index j, of the matrix Td1, being proportional to
a binomial coefficient read j−1 among i−1. At least one element, Td2[i, j], of row index i and column index j of the matrix Td2, being proportional to a Stirling number of the first kind Sj−1(i−1).
According to one embodiment, at least one element, Tz[i,j], of row index i and column index j, of the matrix Tz, is proportional to
a binomial coefficient read j−1 among i−1.
Thus, the expression of the second transfer function on the transform base in question is obtained regardless of the order of the interpolation considered.
Depending on the embodiment, the real number d and/or the combination parameter c is/are variable.
Thus, the frequency and time response of the interpolation filter is reconfigurable.
According to one embodiment, the filter comprising a modified Newton structure comprising:
Thus, the adaptability of the response of the interpolation filter is achieved with a minimal modification of the Newton structure, and thus at a reduced material cost.
According to one embodiment, the modified Newton structure implements:
According to one embodiment, the combination parameter c is fixed and the filter comprises a modified Newton structure comprising, at least in part, the Newton structure.
In one embodiment of the invention, there is a sampling rhythm changing device comprising at least one digital device according to the invention (according to any one of its embodiments).
Thus, the characteristics and advantages of this device are the same as the digital interpolation filter described above. Consequently, they are not detailed further.
In one embodiment of the invention, there is an item of equipment for receiving a radio-frequency signal comprising at least one device for changing the sampling rhythm comprising at least one digital interpolation filter according to the invention (according to any one of its embodiments).
Other characteristics and advantages of the invention will emerge upon reading the following description, provided as a non-restrictive example and referring to the annexed drawings, wherein:
In all the figures in this document, identical elements and steps are designated by the same reference.
The general principle of the described technique consists in implementing a digital fractional delay device comprising a digital interpolation filter delivering a series of output samples approximating a signal x(t) at sampling instants of the form (n+d)Ts based on a series of input samples of the signal x(t) taken at sampling instants of the form nTs with n an integer, Ts a sampling period and d a real number representing the delay applied to the sampling instants.
In particular, the interpolation filter implements a transfer function in the Z-transform domain, Hcd(Z−1), expressed as a linear combination between:
The terminology “implement a transfer function according to a given structure” is used in this patent application to mean that the hardware implementation of the filter in question corresponds (in terms of the functionalities used) to the mathematical expressions explained in the transfer function considered. There is thus a direct relationship between the expression of the transfer function under consideration and the corresponding hardware implementation.
Moreover, the linear combination is a function of at least one real combination parameter c.
The overall hardware implementation of the digital device comprising the interpolation filter thus takes advantage of the synergy between the Newton structure implementing the first transfer function H1d(Z−1) and the structure implementing the second transfer function H2d(Z−1).
Moreover, the linear combination allows the global response of the interpolation filter to be configured in a simple manner between the responses of the two polynomial interpolations in question.
In one embodiment, the second transfer function H2d(Z−1) is expressed at least in part on a polynomial base in Z−1 corresponding to an implementation of the first transfer function H1d(Z−1) according to the Newton structure. This is to facilitate the reuse of the Newton structure in question. Such a base, called transform base in the following description, comprises polynomials of the form (1−Z−1)k with k an integer, as described below.
For this purpose, the method disclosed in the above-mentioned article by Lamb et al. is generalised to an interpolation of any order. Such a generalised method indeed enables an expression of the second transfer function H2d(Z−1) to be determined in the transform base from an expression of the same transfer function, but expressed in a base adapted to a symmetric Farrow implementation.
Such a method is thus of interest insofar as a Farrow structure, even symmetric, enables a polynomial interpolation to be implemented whatever the nature of the polynomials involved. An expression of the transfer function of any type of polynomial interpolation can thus be obtained in the transform base by such a method.
To do this, an expression of the impulse response h(t) of a filter implementing the polynomial interpolation under consideration must first be obtained in order to determine the corresponding Farrow matrix.
In particular, such an impulse response h(t) is expressed as a concatenation of N polynomial sections βj(μ)=Σi=1Npi,jμi−1, with μ∈[−1/2; 1/2[and i and j two integers each from 1 to N, the polynomials βj(u) being translated over successive time segments such that:
Further, according to the definition considered in this patent application, the impulse response h(t) is centred on the time axis so as to be symmetrical in t/Ts=(N+1)/2. In other words, the N polynomials βj(μ) verify βj(μ)=+βN−j+1(μ) or βj(μ)=−βN−j+1(μ) depending on whether the symmetry is even or odd.
Hence, the matrix P comprised of the elements pi,j is a symmetric Farrow matrix as introduced in the above-mentioned article by Valimaki.
Referring to the above-mentioned article by Lamb et al, the change of base from the Farrow base to the transform base is obtained by the matrix operation:
Q=(TdT)−1PTz−1 (Eq-2)
where:
In particular, the matrix Td is expressed as a product of matrices Td=Td2Td1 With Td1 and Td2 two matrices of N rows and N columns. The element Td1[i,j], of row index i and column index j, of the matrix Td1 is equal to
the binomial coefficient read j−1 among i−1. Similarly, the element Td2[i,j], of row index i and column index j, of the matrix Td2, is equal to the Stirling number of the first kind Sj−1(i−1).
Further, the element Tz[i,j], of row index i and column index j, of the matrix Tz is equal to
the binomial coefficient read j−1 among i−1.
The change of base in question thus makes it possible to obtain the transfer function Hd (Z−1) of the filter implementing the polynomial interpolation considered in the transform base in the form:
with qn,m the elements of the matrix Q of N rows and N columns.
In particular, the transfer function Hd(Z−1) of an interpolation filter implementing a Lagrange interpolation expressed in the transform base corresponds to an implementation according to a Newton structure as discussed in the above-mentioned article by Lamb et al. and as illustrated below in relation to
Indeed, a known interpolation filter implementing a third-order Lagrange interpolation implemented according to a Newton structure 100 is now described in relation to
In order to obtain an expression of the transfer function HLd(Z−1) of the interpolation filter in question in the transform base, the base change method described above is applied for example.
In particular, an expression of the impulse response h(t) of the filter in question is first obtained in order to determine the corresponding symmetric Farrow matrix PL.
To do so, it is noted that such an interpolation seeks to construct the polynomial y(t) that goes through the N samples x[j], j from 1 to N, of the input signal x(t) such that:
where t/Ts∈[N/2−1; N/2[.
The Lagrange polynomials are known and defined as follows:
In order to obtain an impulse response centred on the time axis so as to present symmetry, here even, in t/Ts=(N+1)/2, the polynomials
as defined above are translated along the time axis by a value of Ts(N−1)/2. In this way, the polynomials βj(μ) required to define the matrix PL are obtained according to:
where μ∈[−½; ½[.
In this manner, for N=4, one obtains:
Thus, the symmetric Farrow matrix PL corresponding to the third-order Lagrange interpolation is expressed according to our definitions as:
It is noted that this expression differs from equation (3) in the above-mentioned publication by Lamb et al. due to a different choice in the definition of the parameter μ (chosen here as the opposite of the publication in question).
Furthermore, on the basis of the general expressions of the elements of the matrices Td and Tz data above, the matrices (TdT)−1 and Tz−1 are expressed in the case N=4 as:
In this way, the matrix QL obtained by the equation (Eq-2) is expressed in this case as:
As expected, the base change made leads to an expression of the diagonal matrix QL. The associated transfer function HLd(Z−1) obtained from the matrix QL via the equation (Eq-3), then corresponds to an implementation in the form of a structure 100 implementing only three delay lines 110_1, 110_2, 110_3 of the form (1−Z−1)k, where k is an integer from 1 to 3.
The transform base used to express the transfer function HLd(Z−1) of the Lagrange interpolation thus leads to a particularly efficient implementation in computational terms, known as the Newton structure 100.
A known interpolation filter implementing a third-order Spline interpolation with a quasi-Newton structure 200 is now described in relation to
In particular, such a structure 200 corresponds to an expression of the transfer function HSd(Z−1) of the interpolation filter in question in the transform base.
As such, the base-change method described above is applied, for example, to obtain the expression of the transfer function in question.
Again, an expression of the impulse response h(t) of the filter in question is first obtained in order to determine the corresponding symmetric Farrow matrix PS.
To do so, it is noted that such an interpolation seeks to construct the polynomial y(t) that goes through the N samples x[j], j from 1 to N, of the input signal x(t) such that:
where t/Ts∈[N/2−1; N/2[.
The Spline polynomials
considered here are determine for example by the method described in the article by Gradimir V. Milovanović and Zlatko Udovičić, “Calculation of coefficients of a cardinal B-spline”, in Applied Mathematics Letters, Volume 23, Issue 11, 2010, Pages 1346-1350.
In particular, the temporal support of the polynomial
obtained by this method extends over the interval [j−1;j]. In this way, the polynomials βj(μ), with μ∈[−1/2; 1/2[, defining the impulse response sought via the equation (Eq-1) are obtained via temporal translation:
The result in the example that interests us, i.e. for N=4, is that:
Thus, the symmetric Farrow matrix PS corresponding to the third-order Spline interpolation is expressed according to our definitions as:
It is noted here again that this expression differs from equation (8) in the above-mentioned publication by Lamb et al. due to a different choice in the definition of the parameter μ (chosen here as the opposite of the publication in question).
Further, on the basis of the expressions of the matrices (TdT)−1 and Tz−1 given respectively by equations (Eq-4) and (Eq-5), the matrix QS obtained by equation (Eq-2) is expressed in this case as:
It is observed that:
These two characteristics of the matrix QS are found in the implementation of the associated transfer function, HSd(Z−1), where this implementation is based on the use of delay lines of the form (1−Z−1)k corresponding to an expression of HSd(Z−1) in the transform base (HSd(Z−1) being obtained from the matrix QS via equation (Eq-3)).
More specifically, the implementation in question includes:
Due to the small number of additional return loops 210_1, 210_2, 210_3 (i.e. the matrix QS is hollow), such an implementation corresponds to a quasi-Newton structure 200.
A digital fractional delay device comprising an interpolation filter resulting from a linear combination of the filters of
In particular, the interpolation filter according to this embodiment implements a third-order polynomial interpolation including a transfer function in the Z-transform domain, HLSd(Z−1), expressed as a linear combination between:
More specifically, in this embodiment, the transfer function HLSd(Z−1) is expressed as:
HLSd(Z−1)=HLd(Z−1)+c(HSd(Z−1)−HLd(Z−1))
Thus, the transfer function HLSd(Z−1) appears as configurable according to the combination parameter c. In particular, the magnitude of the transfer function HLSd(Z−1) of the filter according to the invention varies between the amplitude of the transfer function HLd(Z−1) of the third-order Lagrange interpolation for c=0 and that of the transfer function HSd(Z−1) of the Spline interpolation of the same order for c=1 as shown in
Equivalently, it is obtained by linearity of the equation (Eq-3) that the matrix QLS, representing the function HLSd(Z−1) in the transform base, expresses itself as:
QLS=QL+c(QS−QL)
From matrix expressions QL and QS obtained above in relation to
The corresponding structure 300 (
Specifically, structure 300 appears as a modified Newton structure that implements:
A known interpolation filter implementing a third-order Hermite interpolation with a quasi-Newton structure 400 is now described in relation to
In particular, such a structure 400 corresponds to an expression of the transfer function HHd(Z−1) of the interpolation filter in question in the transform base.
As such, the base-change method described above is applied, for example, to obtain the expression of the transfer function in question.
Again, an expression of the impulse response h(t) of the filter in question is first obtained in order to determine the corresponding symmetric Farrow matrix PS. However, in the case of Hermite interpolation, the derivative of the polynomials must also be estimated at the sampling points of the signal in addition to the polynomials themselves.
In particular, such an interpolation seeks to construct the polynomial y(t) that goes through the NP samples x[j], j from 1 to NP, of the input signal x(t), while imposing the equality of the derivatives of y(t) and the interpolated signal x(t) at the same sampling points x[j]. In other words, NH=NP(p+1) constraints of the form are obtained:
y(i)(jTs)=x(i)[j]
where i∈{0, 1, 2, . . . , p}, j∈{1, 2, . . . , NP} and .(i) which indicates the i-order derivative.
The polynomial y(t) is thus generally expressed as:
The NH constraints applied to the NH unknown ai lead to a linear system of NH equations whose resolution can express the coefficients ai depending on the values of the samples x[j]. Based on the expression in question of the coefficients ai, it appears that the polynomial y(t) can be generally rewritten as:
In order to describe a third-order interpolation filter whose transfer function can be modelled by matrices PS and QS that are square and of a size 4×4 (so that they can be combined with the matrices PL and QL of the filter of
In this way, the following values of the polynomials αi,j(t) are obtained:
α0,1i(t)=2t3−3t2+1
α1,1(t)=−2t3−3t2
α0,2(t)=t3−2t2+t
α1,2(t)=t3−t2
Further, the second-order derivative estimation method as used for example in the article by Soontornwong, P., Chivapreecha, S. & Pradabpet, C. “A Cubic Hermite variable fractional delay filter Intelligent Signal Processing and Communications Systems” (ISPACS), 2011 International Symposium on, 2011, pp 1-4, is implemented to estimate derivatives x(i)[j] of the signal x(t) at sampling points x[j]. Thus, γ=2 two samples are used to estimate the value of a derivative at a given point.
In this manner, the Hermit polynomials
are finally determined so that y(t) is expressed as:
where t/Ts∈[NP/2−1; NP/2 [and N=NP+γ=4.
The polynomials βj(μ), with μ∈[−1/2; 1/2 [, defining the impulse response sought via the equation (Eq-1) are obtained via time translation:
The result in the example that interests us, i.e. for N=NP+γ=4, is that:
Thus, the symmetric Farrow matrix PH corresponding to the third-order Hermite interpolation considered is expressed according to our definitions as:
Further, on the basis of the expressions of the matrices (TdT)−1 and Tz−1 given respectively by equations (Eq-4) and (Eq-5), the matrix QH obtained by equation (Eq-2) is expressed in this case as:
It is observed that:
the diagonal of the matrix QH is expressed as that of the matrix QL (obtained above for a third-order third-order Lagrange interpolation) to which the term ⅓ is added to the last value of the diagonal; and
only three extra-diagonal elements of the matrix QH are non null. In other words, the matrix QH is also hollow, as is the matrix QS obtained above in relation to
These two characteristics of the matrix QH are found in the implementation of the associated transfer function, HHd(Z−1), where this implementation is based on the use of delay lines of the form (1−Z−1)k, corresponding to an expression of HHd(Z−1) in the transform base (HHd(Z−1) being obtained from the matrix QH via equation (Eq-3)).
More specifically, the implementation in question includes:
the Newton structure 100, implementing the Lagrange interpolation filter described in relation to
four additional return loops 410_1 to 410_3 (dotted arrows in
Due to the small number of additional return loops 410_1, 410_2, 410_3 (i.e. the matrix QH is hollow and consists of only three extra-diagonal elements, such as the matrix QS discussed above in relation to
A digital fractional delay device comprising an interpolation filter resulting from a linear combination of the filters of
In particular, the interpolation filter according to this embodiment implements a third-order polynomial interpolation including a transfer function in the Z-transform domain, HLHd(Z−1), expressed as a linear combination between:
More specifically, in this embodiment, the transfer function HLHd(Z−1) is expressed as:
HLHd(Z−1)=HLd(Z−1)+c(HHd(Z−1)−HLd(Z−1))
Thus, the transfer function HLHd(Z−1) appears as configurable according to the combination parameter c. In particular, the amplitude of the transfer function HLHd(Z−1) of the filter according to the invention varies between the amplitude of the transfer function HLd(Z−1) of the third-order Lagrange interpolation for c=0 and that of the transfer function HHd(Z−1) of the Hermite interpolation of the same order for c=1 as shown in
Equivalently, it is obtained by linearity of the equation (Eq-3) that the matrix QLH, representing the function HLHd(Z−1) in the transform base, expresses itself as:
QLH=QL+c(QH−QL)
From matrix expressions QL and QH obtained above in relation to
The corresponding structure 500 (
Specifically, structure 500 appears as a modified Newton structure that implements:
A digital fractional delay device comprising an interpolation filter resulting from a linear combination of the filters of
In particular, the interpolation filter according to this embodiment implements a third-order polynomial interpolation, of which a transfer function HLH,1/4d(Z−1) in the Z-transform domain corresponds to the transfer function HLHd(Z−1) of the filter in
From the transfer function HLHd(Z−1) obtained above in relation to
Equally, the matrix QLH,1/4, representing the function HLH,1/4d(Z−1) in the transform base, is expressed as:
or, from the expression of the matrix QLH obtained above in relation to
It thus appears that the corresponding structure 500′ is not only a simple copy of the structure 500 of the filter in
A digital fractional delay device comprising an interpolation filter according to one embodiment of the invention is now described in relation to
In particular, the interpolation filter according to this embodiment implements a third-order polynomial interpolation including a transfer function in the Z-transform domain, HLPd(Z−1), expressed as a linear combination between:
For example, the transfer function HPd(Z−1) is generated using the filter synthesis method described in the thesis of Hunter, M. T. “Design of Polynomial-based Filters for Continuously Variable Sample Rate Conversion with Applications in Synthetic Instrumentation and Software Defined Radio”, University of Central Florida Orlando, Florida, 2008 to verify the following constraints:
Furthermore, the parameters Wpass and Wstop of the above-mentioned synthesis method are set at 25 so as to give the same importance to the optimisation of the transfer function of the filter in question within its bandwidth and outside its bandwidth. This provides both a good flatness in the bandwidth and a good attenuation of the side lobes. As shown in
Based on these constraints, the synthesis method directly provides an expression for the corresponding symmetric Farrow matrix Pp:
Further, on the basis of the expressions of the matrices (TdT)−1 and Tz−1 given respectively by equations (Eq-4) and (Eq-5), the matrix Qp obtained by equation (Eq-2) is expressed in this case as:
In this embodiment, the transfer function HLPd(Z−1) is expressed as:
HLPd(Z−1)=HLd(Z−1)+c(HPd(Z−1)−HLd(Z−1))
Hence, the magnitude of the transfer function HLPd(Z−1) of the filter according to the invention varies between the amplitude of the transfer function HLd(Z−1) of the third-order Lagrange interpolation for c=0 and that of the transfer function HPd(Z−1) of the personalised interpolation of the same order for c=1 as shown in
Equivalently, it is obtained by linearity of the equation (Eq-3) that the matrix QLP, representing the function HLPd(Z−1) in the transform base, expresses itself as:
QLP=QL+c(QP−QL)
From the expression of the matrix QL obtained above in relation to
with qi,j the elements of the matrix Qp.
In particular, the corresponding structure 600 (
the Newton structure 100, implementing the Lagrange interpolation filter described in relation to
fifteen additional return loops (dotted arrows in
Specifically, the fifteen additional 610 return loops correspond to the fifteen elements of the matrix QLP that are weighted by the combination parameter c. In practice, such weighting is performed by multipliers (also dotted in
A multi-mode radio frequency 700 receiving equipment comprising two sampling rhythm changing devices 730_1, 730_2 each implementing the digital fractional delay device in
More specifically, the receiving equipment 700 includes an antenna 710 delivering the radio frequency signal to a low noise amplifier LNA. The low noise amplifier LNA delivers the amplified radio frequency signal to two mixers 720_1, 720_2 sequenced by two signals in quadrature delivered by a local oscillator OL. The two baseband I and Q signals thus obtained are filtered by analogue filters 730_1, 730_2 before being sampled at a sampling frequency of Fin by two analogue-to-digital converters 740_1, 740_2.
The I and Q signals sampled at the sampling frequency Fin are then processed respectively by two sampling rhythm changing devices 750_1, 750_2 each implementing the interpolation filter of
Moreover, the receiving equipment 700 is configured to operate according to two reception modes. In a first mode, the receiving equipment 700 receives, for example, an LoRa® signal with a bandwidth of 125 kHz. In a second mode, the receiving equipment 700 receives, for example, a SigFox® signal with a bandwidth of 100 Hz.
To do this, devices 750_1, 750_2 each implement the filter in
When c=0, the Lagrange-type transfer function is adapted to the attenuation of the first 770_1 and second 770_2 replicas of the LoRa Signal® sampled at the frequency Fin while preserving the useful signal centred on the zero frequency (
Conversely, when c=1, the Spline transfer function is better adapted to the attenuation of the first 780_1 and second 780_2 replicas of the SigFox® signal sampled at the frequency Fin while preserving the useful signal centred on the null frequency (
In this manner, the anti-aliasing filtering function of the 730_1, 730_2 devices is obtained in a simple and configurable way in order to address both standards.
Moreover, the delay d is variable here and can be reprogrammed on-the-fly between two samples of the input signal in order also to enable the change of the sampling frequency from Fin to Fout.
Similarly, the parameter c has the values 0 or 1 here. In this way, the transfer function HLSd(Z−1) is switched between the transfer function HLd(Z−1) and the transfer function HSd(Z−1) depending on the reception mode considered.
In other embodiments addressing other applications, the parameter d is static and only a delay to the sampling instants is obtained. In this case Fout=Fin.
In still other embodiments, the parameter c is made variable and reprogrammable on-the-fly over a range of values in order to enable a continuous variation of the amplitude of the transfer function of the filter according to the invention between the amplitude of the first transfer function H1d(Z−1) and the amplitude of the second transfer function H2d(Z−1).
In still other embodiments, the parameter c is static and has a predetermined value such that the amplitude of the transfer function of the filter according to the invention results from the desired linear combination between the amplitude of the first transfer function H1d(Z−1) and the amplitude of the second transfer function H2d(Z−1).
The various above-mentioned structures 100, 200, 300, 400, 500, 600 of digital filtering devices according to the invention may be implemented indifferently on a reprogrammable computing machine (a PC computer, a DSP processor or a microcontroller) executing a program comprising a sequence of instructions, or on a dedicated computing machine (for example a set of logic gates such as an FPGA or an ASIC, or any other hardware module) in order to implement digital interpolation according to the invention.
In the case where the above-mentioned filtering structures are realised with a reprogrammable computing machine, the corresponding program (i.e. the sequence of instructions) can be stored in a removable (such as, for example, a floppy disk, CD-ROM or DVD-ROM) or non-removable (a memory, volatile or not) storage medium, this storage medium being partially or totally readable by a computer or a processor. At initialisation, the code instructions of the computer program are for example loaded into a volatile memory before being executed by the processor of the processing unit.
A device 810 for controlling a digital fractional delay device 800 according to the invention is now described in relation to
For example, the digital device 800 is one of the digital devices in
According to the embodiment shown in
Table 1 below gives examples of parameter c values for some LoRa® or Sigfox® signals.
According to the embodiment shown in
Another device 910 for controlling a digital fractional delay device 900 according to the invention is now described in relation to
For example, the digital device 900 is one of the digital devices in
According to the embodiment shown in
More specifically, the controller 910c determines the parameter c suitable for the processed signal based on all or some of the following information:
the spectrum characteristics (useful signal band, existence of blocking signals, etc.) of the input signal x(t). The spectrum in question is, for example, delivered by the spectral analysis block 910f (implementing for example a discrete Fourier transform of the samples x(nTs) of the input signal);
the real number d defining fractional sampling instants; and
the configuration of other signal processing modules arranged either upstream or downstream of the digital device 900. For example, a filter module (e.g. an FIR filter) placed upstream of the digital device 900 can be used to implement pre-distortion of the signal having to be processed by the digital device 900. In this manner, it is possible to consider more aggressive filtering at the level of the digital device 900. Indeed, such a more aggressive filtering is at the expense of reducing the width of the filter bandwidth included in the digital device 900. However, the above-mentioned pre-distortion can in this case compensate for all or part of the distortion related to the reduction of the bandwidth in question. For example, when the digital device 900 corresponds to the digital device in
Further, in the embodiment shown in
Number | Date | Country | Kind |
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1762632 | Dec 2017 | FR | national |
Filing Document | Filing Date | Country | Kind |
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PCT/EP2018/084244 | 12/10/2018 | WO |
Publishing Document | Publishing Date | Country | Kind |
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WO2019/121122 | 6/27/2019 | WO | A |
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Number | Date | Country | |
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20210111707 A1 | Apr 2021 | US |