CN111431598A - New inner and outer boundary calculation method for MAC capacity area in V L C network - Google Patents

New inner and outer boundary calculation method for MAC capacity area in V L C network Download PDF

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CN111431598A
CN111431598A CN202010243564.3A CN202010243564A CN111431598A CN 111431598 A CN111431598 A CN 111431598A CN 202010243564 A CN202010243564 A CN 202010243564A CN 111431598 A CN111431598 A CN 111431598A
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channel capacity
transmitter
capacity
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distribution
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马帅
张蕴琪
李世银
杜淳
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China University of Mining and Technology CUMT
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    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04BTRANSMISSION
    • H04B10/00Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
    • H04B10/11Arrangements specific to free-space transmission, i.e. transmission through air or vacuum
    • H04B10/114Indoor or close-range type systems
    • H04B10/116Visible light communication
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04BTRANSMISSION
    • H04B10/00Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
    • H04B10/07Arrangements for monitoring or testing transmission systems; Arrangements for fault measurement of transmission systems
    • H04B10/075Arrangements for monitoring or testing transmission systems; Arrangements for fault measurement of transmission systems using an in-service signal
    • H04B10/079Arrangements for monitoring or testing transmission systems; Arrangements for fault measurement of transmission systems using an in-service signal using measurements of the data signal
    • H04B10/0793Network aspects, e.g. central monitoring of transmission parameters
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04BTRANSMISSION
    • H04B10/00Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
    • H04B10/50Transmitters
    • H04B10/501Structural aspects
    • H04B10/502LED transmitters

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Abstract

The invention provides a new inner and outer boundary calculation method of MAC capacity region in V L C network, the invention establishes suggested inner boundary by using single user ability to realize input distribution of each user, and can obtain suggested outer boundary by determining single user capacity of each user and calculating total capacity upper limit by relaxing input constraint condition.

Description

New inner and outer boundary calculation method for MAC capacity area in V L C network
Technical Field
The invention relates to the field of visible light communication, in particular to a new inner and outer boundary calculation method for an MAC capacity area in a V L C network.
Background
By utilizing existing light emitting diodes (L ED) as transmitters, V L C systems can not only provide both illumination and Communication, but also have several other advantages, such as ultra-low electromagnetic radiation, strong transmission security and high energy efficiency.
The capacity region of a MAC can characterize the fundamental limitation of achievable rates and therefore can serve as a theoretical basis for other practical V L C network designs, the disadvantage of the prior art is that the exact capacity region and optimal input distribution of the V L C MAC are still unknown, without closed form expressions, and the complexity is relatively high.
Disclosure of Invention
The invention aims to solve the technical problems in the background art, and provides a new inner and outer boundary calculation method for an MAC (multiple access channels) capacity area in a V L C (visible light communication) network, which comprises the following steps:
step 1, establishing a V L C system, wherein the V L C system comprises two transmitters and a receiver, the two transmitters are respectively marked as a first transmitter and a second transmitter, each transmitter is provided with a light-emitting diode (L ED), and the receiver is provided with a single Photon Detector (PD);
step 2, limiting the peak light power and the average light power of the V L C system;
and 3, solving the channel capacity and the inner and outer boundaries of the V L C system.
In step 1, X is set1And X2Representing the transmitted signals of the first transmitter and the second transmitter, respectively. Since the information is embedded in the intensity of the optical signal, X1And X2Should be real, non-negative.
In step 2, according to eye safetyStandard and actual lighting requirements, limiting peak and average optical power: x is not less than 01≤A1,E{X1}≤μ1,0≤X2≤A2,E{X2}≤μ2Wherein A is1And A2Respectively representing the maximum value of the transmission signal of the first transmitter and the maximum value of the transmission signal of the second transmitter; e { X }1And E { X }2The mathematical expectations for the signals transmitted by the first and second transmitters, respectively; while mu1And mu2The maximum value of the expected value of the signal transmitted by the first transmitter and the second transmitter respectively. In the MAC channel, the received signal Y is represented as:
Y=X1+X2+Z (1)
where Z is the independent Gaussian noise with a mean of 0 and a variance of σ2
The step 3 comprises the following steps:
step 3-1, the MAC capacity field in the V L C system is a convex hull
Figure BDA0002433352910000021
Wherein R (X)1,X2) Indicating, for a fixed product distribution satisfying a given input constraint
Figure BDA0002433352910000022
The set of rate pairs (R)1,R2) The following conditions are satisfied:
Figure BDA0002433352910000023
wherein R is1And R2Respectively represent x1Transmission rate and x2The transmission rate of (c);
I(X1;Y|X2) Indicating the channel capacity of information about X1 obtained from Y when X2 is known to be known.
I(X2;Y|X1) Indicating the channel capacity of information about X2 obtained from Y when X1 is known to be known.
I(X1,X2(ii) a Y) representsUnconditional mutual information, i.e., channel capacity of information on X1 and X2 obtained from Y.
Step 3-2, solving channel capacity I (X)i;Y|Xi) Wherein i is 1,2,
Figure BDA0002433352910000024
due to the finite amplitude (peak optical power constraint), the optimal input distribution of equation (2) should be a finite set of discrete points. Therefore, an effective method is proposed to estimate the channel capacity I (X) under discrete input distributioni;Y|Xi) And its inner and outer boundaries, where i is 1,2, and i is 3-i.
Step 3-3, solving channel capacity I (X)i;Y|Xi) The inner boundary of (a);
step 3-4, solving channel capacity I (X)i;Y|Xi) To the outer boundary of (a).
Step 3-2 comprises:
step 3-2-1 to obtain X1And X2Optimum distribution (X)1And X2Channel capacity distribution) of the channel, setting signal XiGet KiA non-negative real value to obey a discrete distribution
Figure BDA0002433352910000031
i is 1,2, as follows:
Figure BDA0002433352910000032
Figure BDA0002433352910000033
Figure BDA0002433352910000034
in the formula xi,jIs XiJ (th) point of (p)i,jRepresenting its corresponding probability; pr { Xi=xi,jIs means for Xi=xi,jThe probability of (d); sigma2Is the variance of the Gaussian noise Z, K1And K2Are respectively taken as
Figure BDA0002433352910000035
Step 3-2-2, based on step 3-2-1, obtaining:
Figure BDA0002433352910000036
Figure BDA0002433352910000037
Figure BDA0002433352910000038
Figure BDA0002433352910000039
wherein, P (X)i) Represents the probability density function of the signal Xi, h (Xi + Z) represents the entropy of Xi + Z,
Figure BDA00024333529100000310
since the noise Z follows a Gaussian distribution, its probability density (pdf)
Figure BDA00024333529100000311
Is written as:
Figure BDA00024333529100000312
step 3-2-3, obtaining the capacity expression of formula (4d) on the basis of step 3-2-1 and step 3-2-2, expressing as a mathematical problem subject to optimization, as follows:
Figure BDA0002433352910000041
s.t.(3a),(3b),(3c)
step 3-2-4, due to variable Ki
Figure BDA0002433352910000042
And
Figure BDA0002433352910000043
to overcome this difficulty, the problem (6) is difficult to solve by applying an imprecise descent gradient method (S.Boyd and L Vandenberghe, Convexoptimization Cambridge, U.K.: Cambridge Univ.Press,2004.) to obtain an optimal input distribution
Figure BDA0002433352910000044
Namely, it is
Figure BDA0002433352910000045
Sum channel capacity Ci
Figure BDA0002433352910000046
The number of non-negative real values taken when representing the optimal input distribution,
Figure BDA0002433352910000047
represents XiAt the point of the (j) th,
Figure BDA0002433352910000048
indicating its corresponding probability.
Step 3-3 comprises:
step 3-3-1, to obtain channel capacity C1,2Inner boundary of (3), define
Figure BDA0002433352910000049
Figure BDA00024333529100000410
Figure BDA00024333529100000411
Wherein the probability density function fY(y) is:
Figure BDA00024333529100000412
wherein x1,mRepresents X1M point of (1), p1,mRepresenting its corresponding probability;
x2,nrepresents X2N th point of (p)2,nRepresenting its corresponding probability;
y represents a received signal;
step 3-3-2, according to the parameters obtained in step 3-3-1, the capacity domain of V L C MAC comprises two variables
Figure BDA0002433352910000051
And
Figure BDA0002433352910000052
this makes the optimization problem difficult to solve. Therefore, a sub-optimal solution needs to be found. In particular, will distribute
Figure BDA0002433352910000053
And
Figure BDA0002433352910000054
put to the rightmost side of formula (7), the result obtained is C1,2The inner boundary of (a).
The steps 3-4 comprise:
step 3-4-1, defining a signal
Figure BDA0002433352910000055
Then sum signal
Figure BDA0002433352910000056
The peak optical power and the average optical power are respectively constrained to be
Figure BDA0002433352910000057
Wherein
Figure BDA0002433352910000058
Wherein
Figure BDA0002433352910000059
Represents an upper bound for the peak optical power,
Figure BDA00024333529100000510
represents the maximum value of the average optical power.
Step 3-4-2, setting signal
Figure BDA00024333529100000511
Subject to a discrete distribution, take
Figure BDA00024333529100000512
A non-negative real value
Figure BDA00024333529100000513
This gives:
Figure BDA00024333529100000514
Figure BDA00024333529100000515
Figure BDA00024333529100000516
in the formula
Figure BDA00024333529100000517
Step 3-4-3, according to step 3-4-2, obtaining C1,2Has an outer boundary of
Figure BDA00024333529100000518
To simplify it, C1,2Is written as
Figure BDA00024333529100000519
s.t.(9a),(9b),(9c)
Step 3-4-4, which is a discrete non-convex problem. The problem (10) can be solved by an inaccurate gradient descent method, and the channel capacity C can be obtained1,2To the outer boundary of (a). The method for analyzing the channel capacity of the two users can be directly extended to N users (N is more than or equal to 3) multiple access communication.
The present invention studies the capacity region of V L C MAC with peak and average power limitations, the optimal input follows a discrete distribution due to peak optical power limitations, formulating the exact channel capacity region of the found V L C MAC into a hybrid discrete optimization problem by assuming discrete inputs, which is non-convex because the objective function has no analytical expressions.
The method has the advantages that the obtained difference between the inner boundary and the outer boundary is smaller, and the system performance is better due to the new inner boundary and the new outer boundary of the capacity areas of the Multiple Access Channels (MAC) in the visible light communication (V L C) network.
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The foregoing and/or other advantages of the invention will become further apparent from the following detailed description of the invention when taken in conjunction with the accompanying drawings.
FIG. 1 shows the respective optimum input positions of V L C MAC under different SNRs
Figure BDA0002433352910000061
Schematic diagram of the variation curve of (2).
FIG. 2 shows the respective discrete distribution optimal inputs of V L C MAC under different SNR
Figure BDA0002433352910000062
Schematic diagram of the variation curve of (2).
Fig. 3 is a graph showing the inner and outer boundary variation curves of the V L C MAC capacity domain at low SNR.
Fig. 4 is a graph showing the inner and outer boundary variation curves of the V L C MAC capacity domain at high SNR.
FIG. 5 shows the rate R only under the constraint of peak optical power1And R2Schematic diagram of the variation curve of (2).
FIG. 6 shows the rate R only under the constraint of peak optical power1And R2Schematic diagram of the variation curve of (2).
FIG. 7 shows the rate and R for two users at a particular SNR (dB)1+R2Schematic diagram of the variation curve of (2).
Detailed Description
The invention provides a new inner and outer boundary calculation method of a MAC (multiple access channels) capacity area in a V L C (visible light communication) network, which comprises the following steps:
step 1, establishing a V L C system, wherein the V L C system comprises two transmitters and a receiver, the two transmitters are respectively marked as a first transmitter and a second transmitter, each transmitter is provided with a light-emitting diode (L ED), and the receiver is provided with a single Photon Detector (PD);
step 2, limiting the peak light power and the average light power of the V L C system;
and 3, solving the channel capacity and the inner and outer boundaries of the V L C system.
In step 1, X is set1And X2Representing the transmitted signals of the first transmitter and the second transmitter, respectively. Since the information is embedded in the intensity of the optical signal, X1And X2Should be real, non-negative.
In step 2, according to eye safety standard and actual lighting requirement, limiting peak light power and average light power: x is not less than 01≤A1,E{X1}≤μ1,0≤X2≤A2,E{X2}≤μ2Wherein A is1And A2Respectively representing the maximum value of the transmission signal of the first transmitter and the maximum value of the transmission signal of the second transmitter; e { X }1And E { X }2The mathematical expectations for the signals transmitted by the first and second transmitters, respectively; while mu1And mu2The maximum value of the expected value of the signal transmitted by the first transmitter and the second transmitter respectively. In the MAC channel, the received signal Y is represented as:
Y=X1+X2+Z (1)
where Z is the independent Gaussian noise with a mean of 0 and a variance of σ2
The step 3 comprises the following steps:
step 3-1, the MAC capacity field in the V L C system is a convex hull
Figure BDA0002433352910000071
Wherein R (X)1,X2) Indicating, for a fixed product distribution satisfying a given input constraint
Figure BDA0002433352910000072
The set of rate pairs (R)1,R2) The following conditions are satisfied:
Figure BDA0002433352910000073
wherein R is1And R2Respectively represent x1Transmission rate and x2The transmission rate of (c);
I(X1;Y|X2) Indicating the channel capacity of information about X1 obtained from Y when X2 is known to be known.
I(X2;Y|X1) Indicating the channel capacity of information about X2 obtained from Y when X1 is known to be known.
I(X1,X2(ii) a Y) represents unconditional mutual information, i.e., channel capacity of information on X1 and X2 obtained from Y.
Step 3-2, solving channel capacity I (X)i;Y|Xi) Wherein i is 1,2,
Figure BDA0002433352910000074
due to the finite amplitude (peak optical power constraint), the optimal input distribution of equation (2) should be a finite set of discrete points. Therefore, an effective method is proposed to estimate the channel capacity I (X) under discrete input distributioni;Y|Xi) And its inner and outer boundaries, where i is 1,2,
Figure BDA0002433352910000075
step 3-3, solving channel capacity I (X)i;Y|Xi) The inner boundary of (a);
step 3-4, solving channel capacity I (X)i;Y|Xi) To the outer boundary of (a).
Step 3-2 comprises:
step 3-2-1 to obtain X1And X2Optimum distribution (X)1And X2Channel capacity distribution) of the channel, setting signal XiGet KiA non-negative real value to obey a discrete distribution
Figure BDA0002433352910000081
i is 1,2, as follows:
Figure BDA0002433352910000082
Figure BDA0002433352910000083
Figure BDA0002433352910000084
in the formula xi,jIs XiJ (th) point of (p)i,jRepresenting its corresponding probability; pr { Xi=xi,jIs means for Xi=xi,jThe probability of (d); sigma2Is the variance of the Gaussian noise Z, K1And K2Are respectively taken as
Figure BDA0002433352910000085
Step 3-2-2, based on step 3-2-1, obtaining:
Figure BDA0002433352910000086
Figure BDA0002433352910000087
Figure BDA0002433352910000088
Figure BDA0002433352910000089
wherein, P (X)i) Represents the probability density function of the signal Xi, h (Xi + Z) represents the entropy of Xi + Z,
Figure BDA00024333529100000810
since the noise Z follows a Gaussian distribution, its probability density (pdf)
Figure BDA00024333529100000811
(yi) Is written as:
Figure BDA0002433352910000091
step 3-2-3, obtaining the capacity expression of formula (4d) on the basis of step 3-2-1 and step 3-2-2, expressing as a mathematical problem subject to optimization, as follows:
Figure BDA0002433352910000092
s.t.(3a),(3b),(3c)
step 3-2-4, due to variable Ki
Figure BDA0002433352910000093
And
Figure BDA0002433352910000094
to overcome this difficulty, the problem (6) is difficult to solve by applying an imprecise descent gradient method (S.Boyd and L Vandenberghe, Convexoptimization Cambridge, U.K.: Cambridge Univ.Press,2004.) to obtain an optimal input distribution
Figure BDA0002433352910000095
Namely, it is
Figure BDA0002433352910000096
Sum channel capacity Ci
Figure BDA0002433352910000097
The number of non-negative real values taken when representing the optimal input distribution,
Figure BDA0002433352910000098
represents XiAt the point of the (j) th,
Figure BDA0002433352910000099
indicating its corresponding probability.
Step 3-3 comprises:
step 3-3-1, to obtain channel capacity C1,2Inner boundary of (3), define
Figure BDA00024333529100000910
Figure BDA00024333529100000911
Figure BDA00024333529100000912
Wherein the probability density function fY(y) is:
Figure BDA00024333529100000913
wherein x1,mRepresents X1M point of (1), p1,mRepresenting its corresponding probability;
x2,nrepresents X2N th point of (p)2,nRepresenting its corresponding probability;
y represents a received signal;
step 3-3-2, according to the parameters obtained in step 3-3-1, the capacity domain of V L C MAC comprises two variables
Figure BDA0002433352910000101
And
Figure BDA0002433352910000102
this makes the optimization problem difficult to solve. Therefore, a sub-optimal solution needs to be found. In particular, will distribute
Figure BDA0002433352910000103
And
Figure BDA0002433352910000104
put to the rightmost side of formula (7), the result obtained is C1,2The inner boundary of (a).
The steps 3-4 comprise:
step 3-4-1, defining a signal
Figure BDA0002433352910000105
Then sum signal
Figure BDA0002433352910000106
The peak optical power and the average optical power are respectively constrained to be
Figure BDA0002433352910000107
Wherein
Figure BDA0002433352910000108
Wherein
Figure BDA0002433352910000109
Represents an upper bound for the peak optical power,
Figure BDA00024333529100001010
represents the maximum value of the average optical power.
Step 3-4-2, setting signal
Figure BDA00024333529100001011
Subject to a discrete distribution, take
Figure BDA00024333529100001012
A non-negative real value
Figure BDA00024333529100001013
This gives:
Figure BDA00024333529100001014
Figure BDA00024333529100001015
Figure BDA00024333529100001016
in the formula
Figure BDA00024333529100001017
Step 3-4-3, according to step 3-4-2, obtaining C1,2Has an outer boundary of
Figure BDA00024333529100001018
To simplify it, C1,2Is written as
Figure BDA00024333529100001019
s.t.(9a),(9b),(9c)
Step 3-4-4, which is a discrete non-convex problem. Can be applied with an imprecise gradientThe down method solves the problem (10) and obtains the channel capacity C1,2To the outer boundary of (a). The method for analyzing the channel capacity of the two users can be directly extended to N users (N is more than or equal to 3) multiple access communication.
Examples
FIGS. 1 and 2 illustrate the respective optimum input positions of V L C (V L C, Visible L illumination communication) MAC (MAC, Multiple Access Channel model) under different SNR (signal-to-NOISE RATIO, SIGNA L NOISE RATIO, SNR) when using the method of the present invention
Figure BDA0002433352910000111
(xi,jJ-th point representing Xi) and a discrete distribution optimal input
Figure BDA0002433352910000112
(pi,jRepresents piThe j point of (1), i.e. xi,jProbability) of in which
Figure BDA0002433352910000113
For SNR ≦ 10dB, the optimal input position has two discrete points {0, A } for different probabilities, i.e., {0.8,0.2 }. therefore, OOK modulation system can also get the capacity of V L C MAC at low SNR>At 10dB, there are more than two discrete points at the optimal input position, which indicates that a PAM Modulation system (PAM) can obtain the capacity of the V L C MAC.
Fig. 3 and 4 of the method diagram according to the invention illustrate, respectively, that at low SNR, i.e. at low SNR
Figure BDA0002433352910000114
(A1 denotes the peak optical power of emitter 1) and
Figure BDA0002433352910000115
(A2 denotes the peak optical power of emitter 2, σ is the standard deviation of Gaussian noise Z), and at high SNR, i.e., at
Figure BDA0002433352910000116
And
Figure BDA0002433352910000117
inner and outer boundaries of the V L C MAC capacity domain, where
Figure BDA0002433352910000118
As can be seen from fig. 3, the proposed outer boundary is lower than the existing outer boundary, i.e. it is lower than the existing outer boundary
Figure BDA0002433352910000119
And
Figure BDA00024333529100001110
and the proposed inner boundary is larger than the maximum discrete entropy inner boundary.
Fig. 5 and 6 of the method diagram according to the invention illustrate the special case, i.e. only under the constraint of peak optical power, where
Figure BDA00024333529100001111
Figures 3, 4 and 5, 6 all show that the proposed outer boundary is lower than the existing outer boundary, whereas the proposed inner boundary is lower than the outer boundary except for
Figure BDA00024333529100001112
The other existing inner boundaries on the high SNR side are all high, i.e., in FIG. 6
Figure BDA00024333529100001113
Sum rate R1+R2(transmission rate).
Fig. 7, which is a graphical representation of the method according to the invention, shows the proposed inner and outer boundaries, maximizing the discrete entropy inner boundary,
Figure BDA00024333529100001114
Figure BDA0002433352910000121
and
Figure BDA0002433352910000122
rate sum of two users at a particular SNR (dB)R1+R2(bits/s/Hz), i.e. when only the peak optical power is constrained, wherein
Figure BDA0002433352910000123
It can be seen that at low SNR the proposed inner boundary is very close to the maximum discrete entropy inner boundary, whereas at high SNR the proposed inner boundary is higher than the maximum discrete entropy inner boundary. This is because, maximizing the discrete entropy inner boundary is to separate the input entropy H (X) into discrete entropy1)+H(X2) Maximized, this is only the difference entropy h (X)1+X2+ Z) is an approximation. At low and medium SNR, the proposed inner boundary ratio
Figure BDA0002433352910000124
The inner boundary is high. At the time of a high SNR, it is,
Figure BDA0002433352910000125
highest (only peak optical power constraint). Furthermore, the proposed outer boundary is higher than the existing outer boundary
Figure BDA0002433352910000126
And
Figure BDA0002433352910000127
the relevant english explanations in fig. 3 to 7 are as follows:
the deployed Outer represents the Outer boundary proposed by the method of the present invention;
the deployed inner means represents the inner boundary proposed by the method of the present invention;
max Entry denotes the maximum inner boundary of discrete Entropy proposed in the paper "Channel capacity and non-uniform signalling for free-space optical intensities channels" (A.A.F. and S.Hranilvic, "Channel capacity and non-uniform signalling for free-space optical intensities channels," IEEE J.Sel.areas Commun., vol.17, No.9, pp.1553-1563, Dec.2009.)
Outer
Figure BDA0002433352910000128
Denotes the outer boundary set forth in the paper "On the capacity of free space optical fibres
Figure BDA0002433352910000129
(A.Lapidoth,S.M.Moser,and M.Wigger,“On the capacityof freespace optical intensity channels,”IEEE Trans.Inf.Theory,vol.55,no.10,pp.4449–4461,Oct.2009.)
Outer
Figure BDA00024333529100001210
Denotes the outer boundary set forth in the paper "Free-space optical communications," capacity centers, approximations, and a new propagating property
Figure BDA00024333529100001211
(A.Chaaban,J.-M.Morvan,and M.-S.Alouini,“Free-space optical communications:capacity bounds,approximations,and a new spherepacking perspective,”IEEETrans.Commun.,vol.64,no.3,pp.1176–1191,Mar.2016.)
Outer
Figure BDA00024333529100001212
Denotes the outer boundary set forth in the paper "On the capacity of free space optical fibres
Figure BDA0002433352910000131
(A.Lapidoth,S.M.Moser,and M.Wigger,“On the capacityof freespace optical intensity channels,”IEEE Trans.Inf.Theory,vol.55,no.10,pp.4449–4461,Oct.2009.)
Outer
Figure BDA0002433352910000132
Denotes the outer boundary set forth in the paper "Bounds on the capacity region of the optical intensitymultiple access channel
Figure BDA0002433352910000133
(J.Zhou and W.Zhang,“Bounds on the capacity region of the optical intensity multiple accesschannel,”accepted by IEEE Trans.Commun.,2019.)
Inner
Figure BDA0002433352910000134
Denotes the outer boundary set forth in the paper "Bounds on the capacity region of the optical intensitymultiple access channel
Figure BDA0002433352910000135
(J.Zhou and W.Zhang,“Bounds on the capacity region of the optical intensity multiple accesschannel,”accepted by IEEE Trans.Commun.,2019.
It is noted that the outer boundary
Figure BDA0002433352910000136
And an inner boundary
Figure BDA0002433352910000137
Only for the specific case, i.e. with only peak optical power constraints, and the discrete Entropy maximizing inner boundary of Max entry is first extended to the V L C MAC scheme in the present invention.
In life, from the viewpoint of eye safety, instantaneous optical power, that is, amplitude needs to be considered. The average light power is also limited according to the actual lighting requirements, and
Figure BDA0002433352910000138
and
Figure BDA0002433352910000139
only the peak value constraint is considered, and the method is not applicable to actual life. Second, it is used for
Figure BDA00024333529100001310
And
Figure BDA00024333529100001311
the external environment of the method is worse than that of the method, the limit of the method is stricter, and the method is suitable for actual usersGrouping, power allocation, interference management and energy efficiency are all greatly facilitated, and are key to improving industrial efficiency.
The present invention provides a new method for calculating the inner and outer boundaries of the MAC capacity region in the V L C network, and a plurality of methods and approaches for implementing the method, and the above description is only a preferred embodiment of the present invention, and it should be noted that, for those skilled in the art, without departing from the principle of the present invention, several improvements and modifications may be made, and these improvements and modifications should be regarded as the protection scope of the present invention.

Claims (7)

1. A new inner and outer boundary calculation method of a MAC capacity area in a V L C network is characterized by comprising the following steps:
step 1, establishing a V L C system, wherein the V L C system comprises two transmitters and a receiver, the two transmitters are respectively marked as a first transmitter and a second transmitter, each transmitter is provided with a light emitting diode L ED, and the receiver is provided with a single photon detector PD;
step 2, limiting the peak light power and the average light power of the V L C system;
and 3, solving the channel capacity and the inner and outer boundaries of the V L C system.
2. The method of claim 1, wherein in step 1, X is set1And X2Representing the transmitted signals of the first transmitter and the second transmitter, respectively.
3. The method according to claim 2, wherein in step 2, the peak and average optical powers are limited according to eye safety standards and actual lighting requirements: x is not less than 01≤A1,E{X1}≤μ1,0≤X2≤A2,E{X2}≤μ2Wherein A is1And A2Representing the maximum value of the first transmitter transmission signal and the maximum value of the second transmitter transmission signal, respectivelyA large value; e { X }1And E { X }2The mathematical expectations for the signals transmitted by the first and second transmitters, respectively; while mu1And mu2The maximum value of the expected value of the signals transmitted by the first transmitter and the second transmitter respectively;
in the MAC channel, the received signal Y is represented as:
Y=X1+X2+Z (1)
where Z is the independent Gaussian noise with a mean of 0 and a variance of σ2
4. The method of claim 3, wherein step 3 comprises:
step 3-1, the MAC capacity field in the V L C system is a convex hull
Figure FDA0002433352900000011
Wherein R (X)1,X2) Indicating, for a fixed product distribution satisfying a given input constraint
Figure FDA0002433352900000012
The set of rate pairs (R)1,R2) The following conditions are satisfied:
Figure FDA0002433352900000013
wherein R is1And R2Respectively represent x1Transmission rate and x2The transmission rate of (c);
I(X1;Y|X2) Channel capacity representing information about X1 obtained from Y when X2 is known to be known;
I(X2;Y|X1) Channel capacity representing information about X2 obtained from Y when X1 is known to be known;
I(X1,X2(ii) a Y) represents unconditional mutual information, i.e., channel capacity of information on X1 and X2 obtained from Y;
step 3-2, solving channel capacity
Figure FDA0002433352900000021
Wherein the ratio of i to 1,2,
Figure FDA0002433352900000022
step 3-3, solving channel capacity
Figure FDA0002433352900000023
The inner boundary of (a);
step 3-4, solving channel capacity
Figure FDA0002433352900000024
To the outer boundary of (a).
5. The method of claim 4, wherein step 3-2 comprises:
step 3-2-1 to obtain X1And X2Setting the signal X to an optimum distributioniGet KiA non-negative real value to obey a discrete distribution
Figure FDA0002433352900000025
As follows:
Figure FDA0002433352900000026
Figure FDA0002433352900000027
Figure FDA0002433352900000028
in the formula xi,jIs XiJ (th) point of (p)i,jRepresenting its corresponding probability; pr { Xi=xi,jIs means for Xi=xi,jThe probability of (d); sigma2Is the variance of the gaussian noise Z; k1And K2Are respectively taken as
Figure FDA0002433352900000029
Step 3-2-2, based on step 3-2-1, obtaining:
Figure FDA00024333529000000210
wherein, P (X)i) Represents the probability density function of the signal Xi, h (Xi + Z) represents the entropy of Xi + Z,
Figure FDA0002433352900000031
since the noise Z follows a Gaussian distribution, its probability density
Figure FDA0002433352900000032
Is written as:
Figure FDA0002433352900000033
step 3-2-3, obtaining the capacity expression of formula (4d) on the basis of step 3-2-1 and step 3-2-2, expressing as a mathematical problem subject to optimization, as follows:
Figure FDA0002433352900000034
s.t.(3a),(3b),(3c)
3-2-4, obtaining the optimal input distribution x by applying an inaccurate descending gradient methodiIs/are as follows
Figure FDA0002433352900000035
Namely, it is
Figure FDA0002433352900000036
And xiChannel capacity C ofi
Figure FDA0002433352900000037
The number of non-negative real values taken when representing the optimal input distribution,
Figure FDA0002433352900000038
represents XiAt the point of the (j) th,
Figure FDA0002433352900000039
indicating its corresponding probability.
6. The method of claim 5, wherein step 3-3 comprises:
step 3-3-1, in order to obtain the inner boundary of the channel capacity, defining the channel capacity
Figure FDA00024333529000000310
Figure FDA00024333529000000311
Obtaining:
Figure FDA00024333529000000312
wherein the probability density function fY(y) is:
Figure FDA00024333529000000313
wherein x1,mRepresents X1M point of (1), p1,mRepresenting its corresponding probability;
x2,nrepresents X2N th point of (p)2,nRepresenting its corresponding probability;
y represents a received signal;
step 3-3-2, distribution
Figure FDA0002433352900000041
And
Figure FDA0002433352900000042
put to the rightmost side of formula (7), the result obtained is C1,2The inner boundary of (a).
7. The method of claim 6, wherein steps 3-4 comprise:
step 3-4-1, defining a signal
Figure FDA0002433352900000043
Then sum signal
Figure FDA0002433352900000044
The peak optical power and the average optical power are respectively constrained to be
Figure FDA0002433352900000045
Wherein
Figure FDA0002433352900000046
Wherein
Figure FDA0002433352900000047
Represents an upper bound for the peak optical power,
Figure FDA0002433352900000048
represents the maximum value of the average optical power;
step 3-4-2, setting signal
Figure FDA0002433352900000049
Subject to a discrete distribution, take
Figure FDA00024333529000000410
A non-negative real value
Figure FDA00024333529000000411
This gives:
Figure FDA00024333529000000412
Figure FDA00024333529000000413
Figure FDA00024333529000000414
in the formula
Figure FDA00024333529000000415
Step 3-4-3, according to step 3-4-2, obtaining C1,2Has an outer boundary of
Figure FDA00024333529000000416
To simplify it, C1,2The outer boundary of (a) is written as:
Figure FDA00024333529000000417
s.t.(9a),(9b),(9c)
step 3-4-4, solving the problem (10) by an inaccurate gradient descent method and obtaining the channel capacity C1,2To the outer boundary of (a).
CN202010243564.3A 2020-03-31 2020-03-31 New inner and outer boundary calculation method for MAC capacity area in V L C network Pending CN111431598A (en)

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Publication number Priority date Publication date Assignee Title
CN108270485A (en) * 2016-12-30 2018-07-10 徐州坤泰电子科技有限公司 Visible ray is point-to-point and broadcast communication system signal generates and capacity calculation methods
CN109150304A (en) * 2018-11-01 2019-01-04 中国矿业大学 A kind of calculation method of free space light intensity channel up to capacity
CN110808780A (en) * 2019-11-19 2020-02-18 中国矿业大学 New boundary calculation method for capacity region of visible light communication multiple access channel

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108270485A (en) * 2016-12-30 2018-07-10 徐州坤泰电子科技有限公司 Visible ray is point-to-point and broadcast communication system signal generates and capacity calculation methods
CN109150304A (en) * 2018-11-01 2019-01-04 中国矿业大学 A kind of calculation method of free space light intensity channel up to capacity
CN110808780A (en) * 2019-11-19 2020-02-18 中国矿业大学 New boundary calculation method for capacity region of visible light communication multiple access channel

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