The present invention relates to the field of digital modulation, and more particularly very-high-bitrate APSK (Amplitude and Phase Shift Keying) modulations. It can in particular be used in the sub-THz communications envisaged in future telecommunication standards.
The growing demand for bandwidth from users has led to the emergence of new technological solutions in the last-generation mobile telecommunications networks, such as massive MIMO (Multiple Input Multiple Output), cellular densification via small cells, multi-RAT (Radio Access Technology) access using together the sub-6 GHz band and the millimetric band. More recently, it has been proposed to use spectral bands between 100 and 300 GHz, called sub-THz, for very-high-bitrate communications. These sub-THz communications are envisaged for example for the point-to-multipoint links in which a base station transmits data at a very high bitrate and low distance to a plurality of mobile terminals on the downstream connection or to establish point-to-point links between base stations in the backhaul network.
The use of the sub-THz bands involves, however, solving problems of energy consumption, of stability of the oscillators and of being able to reach high orders of modulation. The difficulty in producing stable oscillators in this frequency range as well as the necessity of using high orders of modulation to obtain ever-increasing data bitrates make it so that sub-THz communication systems are very sensitive to phase noise. This phase noise affects both the oscillator of the emitter and that of the receiver. To this phase noise is added the conventional problem of offset between the frequency of the oscillator of the receiver and that of the oscillator of the emitter or CFO (Frequency Offset). The symbol error rate can thus become very high.
Various strategies for optimization of modulation constellations have been proposed in the prior art to minimize the symbol error rate. In particular, the article of C. Hager et al. entitled “Design of APSK constellations for coherent optical channels with nonlinear phase noise”, IEEE Transactions on Communications, vol. 61, no 8, August 2013, discloses modulation constellations having good robustness to nonlinear phase noise in the case in which the receiver uses a sub-optimal detection module with two stages, a first stage carrying out a detection of amplitude and a phase correction, and a second stage carrying out a phase detection.
However, these strategies are not optimal insofar as they do not seek to minimize the bit error rate or BER (Bit Error Rate) but simply the symbol error rate or SEP (Symbol Error Probability). Moreover, the constellations obtained are not structured and thus difficult to use for high orders of modulation. Finally, these strategies do not address the way to adapt the link between the emitter and the receiver in the presence of phase noise, to obtain low bit error rates.
The present invention is defined by a method for adapting a link as claimed below. Alternative embodiments are specified in the dependent claims.
Other features and advantages of the invention will appear upon reading a preferred embodiment of the invention, described in reference to the appended drawings in which:
Below, communication over a transmission channel affected by phase noise between an emitter and a receiver will be considered. For example, the communication can be that between a base station and a mobile terminal in the sub-THz band. Recent measurement campaigns have shown that the direct path or LOS (Line Of Sight) dominated in such communications.
The signal received in the baseband at the time k can be expressed in the form:
r(k)=s(k)ejφ(k)+n(k) (1)
where s(k) is the symbol emitted at the time k, φ(k) is the phase noise representing the sum of the phase noise of the emitter and that of the receiver, n(k) is a sample of additive white Gaussian noise (AWGN) having a variance σn2.
The phase noise can be considered as the sum of a Gaussian random variable (having a variance σp2) and a Wiener (also called Wiener-Lévy) stochastic process, that is to say with stationary independent increments following a Gaussian distribution (having a variance σw2). It can be shown that the spectral density of the phase noise is the sum of a constant (white noise) and of a Lorentzian contribution (Wiener-Lévy process). The Lorentzian contribution is dominant at the low frequencies but becomes negligible with respect to the white-noise component above a cutoff frequency proportional to the ratio
When this cutoff frequency, fc, is less than
where B is the width of the band used for the transmission, N is the length of a frame transmitted and
the Lorentzian contribution can be ignored. Since this condition is generally verified in sub-THz communications, hereinafter it is supposed, unless otherwise mentioned, that the Lorentzian contribution can be ignored in the phase noise.
The digital modulation method used by the present invention transforms words of m bits into complex symbols belonging to a modulation constellation, C, of order M where M=2m, the complex symbols modulating a carrier wave via quadrature modulation.
Said complex symbols are distributed over Γ=2n equidistant concentric circles where m>n+1 and n>1, each of the concentric circles carrying the same plurality M/Γ of symbols. The angular distribution of the complex symbols is uniform and identical on each of the concentric circles. More precisely, the constellation C is defined by the set of complex symbols:
where
is the radial distance between consecutive concentric circles, Es is the average power of the symbols of the constellation, and where
is the angular offset between two consecutive symbols on the same concentric circle. Thus the modulation constellation is parameterized by the order of modulation, M, and the number of concentric circles, Γ. Hereinafter it will therefore be noted as C(M,Γ).
The successive symbols of a circle corresponding to two words of m bits having a Hamming distance equal to 1. Likewise, two symbols disposed on the same radius, that is to say aligned in the same angular direction, and belonging to two successive concentric circles, correspond to two words of m bits having a Hamming distance equal to 1. In other words, two adjacent modulation symbols, whether they are located on the same circle or on the same radius of the constellation, represent words only differing by a single bit.
For this purpose, each word of m bits to be modulated is coded into a word of a first Gray code having a size n and into a word of a second Gray code having a size (m−n). In other words, the word to be modulated bw can be represented by:
bw=(b1ρ, . . . ,bnρ,b1θ, . . . ,bm-nθ) (3)
It consists of a first portion, b1ρ, . . . , bnρ, giving the index of the concentric circle on which the modulation symbol is located and of a second portion, b1θ, . . . , bm-nθ, giving the index of the argument of this complex symbol.
Finally, the digital modulation used by the present invention can be considered as a bijective function F of {0,1}m in C(M,Γ) such that:
where q is the integer corresponding to the word of the first Gray code b1ρ, . . . , bnp and p is the integer corresponding to the word of the second Gray code b1θ, . . . , bm-nθ. This modulation method will conventionally be called PQAM (Polar-QAM).
More precisely, the constellation shown is the constellation C(16,4), that is to say of order M=16 (m=4) and having a number of concentric circles Γ=4 (n=2). The radial distance between concentric circles is indicated by δρ and the angular offset between successive symbols of the same circles is noted as δθ (here δθ=π/2). In the present case, the two most significant bits (MSB) form a first Gray code indexing the concentric circles. The two most significant bits (LSB) form a second Gray code indexing the symbols on the same circle.
Upon reception, the decisions on the symbols are taken on the basis of the polar coordinates (ρr, θr) of the received signal r. Hereinafter, the notation (ρs, θs) will be used to designate the polar coordinates of a symbol s.
In the absence of coding, the bits can be estimated by taking a hard decision on the basis of the received signal. More precisely, the symbol transmitted is advantageously estimated by the receiver via:
The bits transmitted then being estimated by ({circumflex over (b)}1, . . . , {circumflex over (b)}m)=F−1 (ŝ). The term in brackets is a distance defined in polar coordinates, dγ (s,r), defined by:
where
is the ratio between the power of the phase noise and that of the additive (thermal) noise on the channel, and Es is the average energy of the symbols of the constellation.
In the presence of coding with probabilistic input, for example LDPC coding, the bits transmitted can be estimated by soft decision by calculating the logarithmic likelihood ratios:
where p(bi=η|r) represents the probability that the bit bi equals η given that the received signal is the complex value r. The logarithmic likelihood ratios can be calculated by:
where C0i (resp. C1i) is a subset of symbols of C(M,Γ) satisfying bi=0 (resp. bi=1). The previous expression can be simplified via the max-log sum approximation (also called max-log), according to which the sums are approached by the dominant probability terms:
LLR(bi)≈log(p(r|s1))−log(p(r|s0)) (9)
or:
LLR(bi)≈(dγ2(r,s0))−(dγ2(r,s1)) (10)
The signal-to-noise ratio is equal to Es/(N0/2) where Es=mEb is the energy per symbol, Eb is the energy per bit and N0 the bilateral spectral density of noise.
The curves are given for a phase-noise power σp2=0.1.
In the case of
The words subject to the digital modulation come from LDPC coding with a rate of ⅔ with length of blocks of 1944 bits and soft decoding of the min-sum type and 50 decoding iterations.
It is noted that the level of BER obtained via the PQAM (or Polar-QAM in the drawings) modulation method is substantially less than that of a conventional QAM modulation of the same order, the difference occurring for an SNR of 13 dB when M=64 and of 20 dB when M=256.
The PQAM modulation disclosed above is used in a mechanism for adapting a link according to an embodiment of the invention. It is recalled that the adaptation of a link involves modifying, in an adaptive manner, the modulation and coding scheme (MCS scheme) of the bits of information according to the quality of the channel (in particular its signal-to-noise ratio), to obtain a target BER for a given bitrate, or inversely to obtain a target bitrate on the basis of a given BER.
In the present case, and in an original manner, the phase noise is also taken into account in the adaptation of the link.
The bit error rate,
can be calculated analytically via:
the decision region ML ŝ=s being defined by the ranges δρ,δθ around the symbol s.
where
is the complementary distribution function of the reduced centered normal distribution, N(0,1). Taking into account the expressions of δρ and δθ according to M and Γ, and the fact that Eb=Es/m:
where
More precisely, this diagram gives, for a target bit error rate (here BER<10−4), the modulation constellations compatible with a given level of phase noise and a given level of thermal noise. The abscissae show the signal-to-noise ratio, Eb/N0, and the ordinates show the inverse of the power of the phase noise,
This diagram is obtained by calculating the BER from the expression (14), according to the signal-to-noise ratio Eb/N0 and the phase-noise power, σp2, for various values of M and Γ. The values of M and Γ compatibles with the target BER are indicated in the diagram.
In step 410, the emitter transmits a plurality N of control symbols, for example in a header of a transmission frame. These control symbols are by definition known to the receiver and are not necessarily part of a constellation C(M,Γ) in the sense defined above. For example, symbols having the same amplitude √{square root over (Es)} are chosen.
In step 420, the receiver estimates, on the basis of the received signal, the variances in thermal noise (or additive noise) and in phase noise affecting the transmission channel. More precisely:
and
where sk, k=1, . . . , N are the control symbols, and r(k)=ρkejθk, k=1, . . . , N the signals received in the baseband, corresponding to these control symbols.
In step 430, the receiver returns to the emitter a piece of channel state information or CSI (Channel State Information) comprising an estimation of the phase-noise variance and an estimation of the variance in the thermal noise (or of the SNR,
In step 440, the emitter consults a table, the inputs of which (discretized) are the target bit error rate (BER) and the variances in thermal noise and phase noise. This table gives the optimal values of the parameters M,Γ compatible with the triplet of inputs provided (namely the variance in additive noise, the variance in the phase noise and the target bit error rate).
If necessary, this table also includes as an input the parameters of various types of channel coding with various rates. In all cases, the table in question has been precalculated and stored in a memory of the emitter. It contains the values M,Γ of the constellations C(M,Γ) compatible with the triple of inputs provided. More particularly, it contains the optimal values M,Γ satisfying the constraint:
with the same notation conventions as in the expression (14).
In step 450, the emitter modulates the binary data (if necessary after having coded them via channel coding) by grouping by blocks of log2 (M) bits to generate the corresponding modulation symbols of the constellation C(M,Γ). These modulation symbols then modulate a carrier via quadrature modulation, in a manner known per se.
Number | Date | Country | Kind |
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19 02720 | Mar 2019 | FR | national |
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5828695 | Webb | Oct 1998 | A |
20050074068 | Borran | Apr 2005 | A1 |
20160056989 | Murakami | Feb 2016 | A1 |
Number | Date | Country |
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WO 2018116411 | Jun 2018 | WO |
Entry |
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French Preliminary Search Report dated Jan. 9, 2020 in French Application 19 02720 filed on Mar. 15, 2019 (with English Translation of Categories of Cited Documents), 2 pages. |
Lianjun Deng, et al., “Performance of Circular QAM Constellations Using Partial Channel Coding with Parallel Double Gray Mapping”,19th International Symposium on Wireless Personal Multimedia Communications (WPMC), National Institute of Information and Communications Technology (NICT), Nov. 4, 2016, XP033106608, pp. 400-405. |
Bernhard Goebel, et al.,“Calculation of Mutual Information for Partially Coherent Gaussian Channels With Applications to Fiber Optics”, IEEE Transactions on Information Theory, vol. 57, No. 9, Sep. 1, 2011, XP011382281, pp. 5720-5736. |
Christian Hager, et al., “Design of APSK constellations for Coherent Optical Channels with Nonlinear Phase Noise”, IEEE Transactions on Communications, vol. 61, No. 8, Aug. 2013, 11 pages. |
U.S. Appl. No. 16/781,000, filed Feb. 4, 2020, Demmer et al. |
Number | Date | Country | |
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20200351141 A1 | Nov 2020 | US |