The present invention relates to a method and circuit arrangement for transmitting messages, the messages being coded by orthogonal functions to form a signal.
Methods for transmitting messages using coding by orthogonal functions have been used. Thus, in practice, frequent use is made of sinusoidal and cosinusoidal functions as orthogonal base functions for coding a number of messages to form a common signal. Reference is made to the book entitled “Principles of Communication Engineering”, Wozencraft, Jacobs, Wiley, New York 1965, which is herewith incorporated by reference herein, for the theory of these methods.
A method and a device for transmitting messages using Hermite functions as orthogonal functions are described in European Patent Document No. EP 0 340 853.
The aim in transmitting messages is to make the signals to be transmitted immune to interference and to provide means at the receiving side which filter out interference.
An object of the present invention is to specify a method and circuit arrangement which permits a high transmission rate in conjunction with a reduction in the interference susceptibility.
The present invention provides a method for transmitting at least one message, the method including coding each of the at least one message using a respective orthogonal function so as to form a transmission signal, each respective orthogonal function being an approximation of a respective Hermite function. A Fourier transform is performed on a received signal, and then the Fourier transformed received signal is decoded using the respective orthogonal function so as to obtain the at least one message. Use is made of the property that, except for a multiplicative constant, Hermite functions do not change during a Fourier transform.
In an advantageous further development of the present invention, the received signal is subjected to a Fourier transform and subsequently decoded with the aid of the Hermite functions. In this case, use is made of the property that, except for a multiplicative constant, Hermite functions do not change during a Fourier transform.
An advantageous further development of the present invention provides for the received signal to be filtered before and/or after the Fourier transform, in order to eliminate possibly included interference components.
In one advantageous further development of the invention, the received signal is decoded both in the time domain and in the frequency domain. That is to say, on the one hand, the received signal is fed directly to the decoding and, on the other hand, is first of all subjected to a Fourier transform and then decoded.
In an advantageous further development of the invention, in each case one of the two decoded signals in the time domain and in the frequency domain, respectively, is selected.
One advantageous further development of the invention provides for one of the two signals present in the time domain and in the frequency domain to be selected on the basis of all signals present.
The present invention also provides a circuit arrangement for transmitting at least one message, the circuit arrangement including a coding device at a transmission side for coding each of the at least one message using a respective orthogonal function so as to form a transmission signal, each respective orthogonal function being an approximation of a respective Hermite function. A demodulation device is included at a receiving side for recovering the at least one message from a received signal via a decoding using the respective Hermite function. The demodulation device includes a Fourier-transform device for performing a Fourier transform on the received signal before the decoding.
In an advantageous further development of the present invention, the demodulation device has a number of multipliers, integrators and discriminators corresponding to the number of dimensions or linear factors, one multiplier, one integrator and one discriminator, respectively, being connected in series to form an evaluation unit. A multiplier and an integrator form a correlator.
In one advantageous further development of the invention, provision is made for a Fourier-transform device which subjects the received signal to a Fourier transform and the time domain, and the other evaluation unit is fed the signal in the frequency domain. Instead of two evaluation units, it is optionally possible to use only one with a multiplex technique.
The invention will now be explained in more detail on the basis of exemplary embodiments with reference to the drawing, in which:
s(t)=m0f0(t)+m1f1(t)+ . . . +mL-1fL-1(t).
Functions f0(t) to fL-1(t) are orthogonal functions which satisfy the following rule:
T being the orthogonality interval. Since the orthogonality interval of the Hermite functions extends over an infinite time interval, the Hermite functions must be approximated by technically realizable functions.
Functions f(t) are usually standardized in such a way that the constant is equal to 1. The term orthonormal functions is also used in this case.
It is indicated in
Receiving device 7 includes a number of decoder units 13 corresponding to the number of the dimensions contained in signal s(t). In the present exemplary embodiment, a number L of decoder units 13 is provided. Each of decoder units 13 includes a multiplier 15, an integrator 17 and a discriminator 19. The aforesaid subassemblies are connected in series, the output signal of multiplier 15 being fed to the integrator, and the output signal of the integrator being fed to discriminator 19, which then provides the decoded component {circumflex over (m)}j.
Each of decoder units 13 is fed a signal r(t) which is composed of transmitted signal s(t) and interference signal e(t). Owing to the orthogonality of the functions used for modulation, components mj can be recovered from transmitted signal s(t) in a simple manner by calculating the integral
This integration is carried out by integrators 17. Since signal r(t) received by receiving device 7 has an interference component e(t), the signal made available by integrators 17 in accordance with the equation
In addition to the already mentioned property of orthogonality, functions f0(t) to fL-1(t) used for modulation are distinguished by the fact that they remain unchanged in the case of a Fourier transform, except for a multiplicative constant. Such functions are the Hermite functions, and are defined as follows:
Hn(x) being the Hermite polynomials, for which it holds that:
A graphical representation of the first five Hermite functions is shown in
The strong exponential decay of the functions is clearly to be seen. This property permits, in a simple way, a technically realizable approximation of the functions which are then fed to multipliers 9 and 15. A detailed description of the mentioned Hermite functions can be found in the book entitled “The Fourier Integral and Certain of Its Applications”, N. Wiener, Cambridge University Press, Cambridge 1933, reprinted 1988 which is herewith incorporated by reference herein.
Because signal s(t) containing the message is represented in the base band as a linear combination of Hermite functions, this signal s(t) is essentially not changed by the Fourier transform of Fourier-transform device 21. The result of this is that decoder units 13 can be designed in accordance with the decoder units specified in
Other definitions of the Fourier transform are likewise possible, mutatis mutandis. The definition used here is the mathematically simplest one in this case. Note, however, that the symbol f differs by a factor from the customary frequency.
The interference e(t) contained in received signal r(t) can be filtered out to a certain extent by filter 22.1 upstream of Fourier-transform device 21, the signal components of the orthogonal Hermite functions remaining essentially unchanged. A contribution to further reducing the interference component is made by second filter 22.2, which is connected downstream of Fourier-transform device 21 and eliminates further interference components by a further filtering operation.
A further exemplary embodiment of a receiving device 7 is shown in
Shown in
It is common to all the above-mentioned exemplary embodiments that an additional filtering can be performed in the frequency domain owing to the use of Hermite functions to code the message, because these Hermite functions are not essentially changed by the Fourier transform. Thus, interference in the decoded messages is reduced.
Of course, it is possible to combine individual exemplary embodiments; for example, the two filters 22.1, 22.2 shown in
Number | Date | Country | Kind |
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197 35 097 | Aug 1997 | DE | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/EP98/04434 | 7/16/1998 | WO | 00 | 10/16/2000 |
Publishing Document | Publishing Date | Country | Kind |
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WO99/09656 | 2/25/1999 | WO | A |
Number | Name | Date | Kind |
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4730344 | Saha | Mar 1988 | A |
5175743 | Crespo et al. | Dec 1992 | A |
5761346 | Moody | Jun 1998 | A |
5862182 | Awater et al. | Jan 1999 | A |
6169723 | Fertner et al. | Jan 2001 | B1 |
6356555 | Rakib et al. | Mar 2002 | B1 |
Number | Date | Country |
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0 340 853 | Nov 1989 | EP |