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International Journal of Research in Advent Technology, Vol.2, No.6, June 2014 
E-ISSN: 2321-9637 
233 
Design and Implementation of SD for MIMO System 
Using FPGA 
Rashmi Pahal1, Dinesh Kumar Verma2Ajay sharma3 
Electronics and communication Department1,2,3 
P.D.M college of Engg1,2, DKOP Labs Pvt. Ltd.3 
Rashmipahal04@gmail.com1, erdineshverma@gmail.com2,ajay@dkoplabs.com3 
Abstract-This paper has shown the use of Newton Iterative Method for matrix inversion, it reduces the complexity 
of calculating the unconstrained solution in Sphere Decoding for Multiple input Multiple output system. The paper 
purposes the initialization procedure for Newton Iterative method and Q-Cholskey method for decomposition of 
matrix to upper triangular matrix. This paper has shown the result of minimum Euclidian distance for a 2×2 MIMO 
with 4-QAM. 
Index Term- FPGA, Newton Iterative Method, MIMO, QAM 
1. INTRODUCTION 
MIMO system is a wireless system employing 
multiple transmit and receive antennas[1].As the 
capacity increase with the minimum number of 
transmit and receive antenna[2], in the last years 
significant interest in large MIMO 
schemes[3][4][5].Hence low complexity detection 
technique for such system are crucial for practical 
application. A high performance detection method 
Sphere Decoding (SD) [6] and its variation. Sphere 
Decoding demands the inversion of channel matrix, 
so an approximate inversion method is used to get the 
approximate inverse[7][12]. The Sphere Decoding 
algorithm was first introduced in[8] as a method for 
finding lattice vectors of short length, and its 
complexity is polynomial in dimension of the 
lattice[9]. Sphere decoding was first applied to 
communication problems in a paper on lattice code 
decoding[10]. The use of newton-iterative method [7] 
of inversion of matrix for SD target MIMO systems, 
and focuses on minimum Euclidean Distance Vector. 
This technique can be interested also to other MIMO 
detection scheme that require inversion of large 
matrices. 
In this paper, we introduce a SD for measurement of 
minimum Euclidean distance vector, Newton 
algorithm for the calculation of matrix inversion. In 
section II, we review the system Model and decoding 
algorithm for Sphere Decoder. In section III, we 
show our stimulation result for considered MIMO 
system. Section IV show the conclusion of SD 
Algorithm. 
2. SYSTEM MODEL AND DECODING 
ALGORITHM 
Consider a multiple antenna system with nT transmit 
antennas and nR receive antennas over a flat fading 
Rayleigh channel. Such a system is represented by 
̂=  
+	, … (1) 
The case in which nT = nR. The baseband signal 
vector transmitted is denoted as  = [1,2,……,nT], 
where each component of the vector is independently 
matrix whose elements mij represent the complex 
transfer functions from the jth transmit drawn from a 
complex constellation such as QAM or PSK, our 
work is on 4-QAM. M is nT×nR channel antenna to 
the ith receive antenna. Each element of M is an 
independently identically distributed (i.i.d) zero mean 
circular complex Gaussian random variable of unit 
variance. Noise vector,	 is an i.i.d. complex 
Gaussian random variable of variance N0 that is 
independent of M and u. 
To obtain a lattice representation of this multiple 
antenna system, we begin by transforming the 
complex matrix equation into the real matrix 
equation. This lattice representation is given as: 
r = [
{̂ᵀ} {̂ᵀ}]T …(2) 
M =
{ 
ᵀ} −{ 
ᵀ} 
{ 
ᵀ}
{ 
ᵀ} 
…(3) 
u = [

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Paper id 26201482

  • 1. International Journal of Research in Advent Technology, Vol.2, No.6, June 2014 E-ISSN: 2321-9637 233 Design and Implementation of SD for MIMO System Using FPGA Rashmi Pahal1, Dinesh Kumar Verma2Ajay sharma3 Electronics and communication Department1,2,3 P.D.M college of Engg1,2, DKOP Labs Pvt. Ltd.3 Rashmipahal04@gmail.com1, erdineshverma@gmail.com2,ajay@dkoplabs.com3 Abstract-This paper has shown the use of Newton Iterative Method for matrix inversion, it reduces the complexity of calculating the unconstrained solution in Sphere Decoding for Multiple input Multiple output system. The paper purposes the initialization procedure for Newton Iterative method and Q-Cholskey method for decomposition of matrix to upper triangular matrix. This paper has shown the result of minimum Euclidian distance for a 2×2 MIMO with 4-QAM. Index Term- FPGA, Newton Iterative Method, MIMO, QAM 1. INTRODUCTION MIMO system is a wireless system employing multiple transmit and receive antennas[1].As the capacity increase with the minimum number of transmit and receive antenna[2], in the last years significant interest in large MIMO schemes[3][4][5].Hence low complexity detection technique for such system are crucial for practical application. A high performance detection method Sphere Decoding (SD) [6] and its variation. Sphere Decoding demands the inversion of channel matrix, so an approximate inversion method is used to get the approximate inverse[7][12]. The Sphere Decoding algorithm was first introduced in[8] as a method for finding lattice vectors of short length, and its complexity is polynomial in dimension of the lattice[9]. Sphere decoding was first applied to communication problems in a paper on lattice code decoding[10]. The use of newton-iterative method [7] of inversion of matrix for SD target MIMO systems, and focuses on minimum Euclidean Distance Vector. This technique can be interested also to other MIMO detection scheme that require inversion of large matrices. In this paper, we introduce a SD for measurement of minimum Euclidean distance vector, Newton algorithm for the calculation of matrix inversion. In section II, we review the system Model and decoding algorithm for Sphere Decoder. In section III, we show our stimulation result for considered MIMO system. Section IV show the conclusion of SD Algorithm. 2. SYSTEM MODEL AND DECODING ALGORITHM Consider a multiple antenna system with nT transmit antennas and nR receive antennas over a flat fading Rayleigh channel. Such a system is represented by ̂= + , … (1) The case in which nT = nR. The baseband signal vector transmitted is denoted as = [1,2,……,nT], where each component of the vector is independently matrix whose elements mij represent the complex transfer functions from the jth transmit drawn from a complex constellation such as QAM or PSK, our work is on 4-QAM. M is nT×nR channel antenna to the ith receive antenna. Each element of M is an independently identically distributed (i.i.d) zero mean circular complex Gaussian random variable of unit variance. Noise vector, is an i.i.d. complex Gaussian random variable of variance N0 that is independent of M and u. To obtain a lattice representation of this multiple antenna system, we begin by transforming the complex matrix equation into the real matrix equation. This lattice representation is given as: r = [
  • 3. { ᵀ} −{ ᵀ} { ᵀ}
  • 7. International Journal of Research in Advent Technology, Vol.2, No.6, June 2014 E-ISSN: 2321-9637 234 Since the elements of M are i.i.d. complex Gaussian, the rank of the matrix M is almost always 2nT, so we can think of the 2nT columns of M as basis vectors {mi} of a lattice lying in a 2nR-dimensional space. The vector acts as the “coordinates” of a lattice point. Receiver is familiar with the channel matrix, so maximum likelihood (ML) detection is achieved by searching for a possible transmitted that generate the smallest Euclidean distance dML =arg mind ǁr – Mu ǁ2 …. (6) An efficient method of solving (6) is provide by SD[6][11] that requires an equivalent from of (1). It is easily shown that (7) is equivalent to dML =arg mind ǁ R(u-) ǁ 2 …(7) where, R is the upper triangle matrix obtained from the Q-Cholesky factorization, and the unconstrained solution is given by =(CHC)-1 CHr[6]. For an invertible channel matrix C. =M-1 r …(8) This form is the basic of scheme implemented in[17][18]. The implemented scheme [17] is attractive for large MIMO systems. We term the process of calculating the unconstrained solution and upper triangular matrix R as preprocessing and determining the ML solution. The SD algorithm employs depth first tree searching[16] for finding the ML data vector. The unconstrained solution is calculated during the preprocessing, a task that can contribute significantly to complexity if no of antennas at any of the end is large. We use Newton iterative approach for obtaining the matrix inverse, as it is massively parallelizable with good numerical stability and requires O(log2n) parallel time units to achieve an accuracy of 2-O(log2n) when N is large[15]. Other method used for approximate matrix inverse Jacobi iteration [13][14] converges linearly, while Newton Iterative method converges Quadratically. The Newton algorithm for inverting M is given by[12][7] XK+1=XK(2I–MXK) …(9) Theorem 2 in [12] shows the initialization X0 = α0MT , With α0 positive and sufficiently small. Initial choice of α0 is crucial in the convergence process for calculating the inverse of matrix. The residual matrix, EK is a measure of deviation of computed inverse from the actual inverse of given matrix A. The Residual matrix EK after k iteration is given as EK=I–M M+ …(10) It is easy to show that in this method we have XK+1 = XK 2 revealing quadratical convergence. By increasing the number of iteration , accuracy of generalized inverse matrix also increases. Q-Cholesky algorithm is followed for decomposition of matrix to upper triangular matrix[11]. 3. SIMULATION RESULTS The objective of the computer stimulation is to investigate the effect of Newton iteration in calculation of Unconstrained solutions on the overall MIMO system. We have done all of our work on Xilinx ISE tool for analysis of unconstrained solution obtained by SD by use of Newton iterative method for matrix inversion. We analyze the result of Newton algorithm and observe that the result obtained at 4th iteration are not accurate while result obtained at 7th iteration are converging to zero. So we use the result of 7th iteration for SD algorithm. The analysis of Newton result is by comparing the residue matrix at 4th and 7th iteration. We implement the SD for 2 × 2 MIMO with 4 QAM. Considering the 4 QAM with average symbol energy ,Es of 42, so the possible lattice coordinates are S4 = [-3,-1,1,3]. Fig 1 The stimulation of Newton Iterative method for matrix Inversion.
  • 8. International Journal of Research in Advent Technology, Vol.2, No.6, June 2014 E-ISSN: 2321-9637 235 Fig 2 The stimulation of Q-cholesky Fig. 3 The stimulation result of Sphere Decoding algorithm. 4. CONCLUSION In stimulation nT =2 transmit antennas and nR =2 receiving antennas, the average symbol energy was 42. The complexity face while doing the work is, selection of initial choice of sphere radius. As if radius chosen in small then it will leave some of the lattice points, while if radius chosen is large then it will search the points which are not present in constellation, thus making the system divergent. Second problem we faces is the usage of divider and square Root in SD algorithm, as it is very difficult for Verilog to code the divider and Square Root. Our thesis has shown the stimulation only not the synthesis. This work has a future scope that one can use the IP CORE processor for Divider and Square Root and can synthesis the SD. REFERENCE [1] A. J. Paulraj, D. A. Gore, R. U. Nabar, and H. Bolcskei, “An overview of MIMO communication: a key to gigabit wireless,” Proc. IEEE, vol. 92, no. 2, pp. 198–218, Feb. 2004. [2] E. Telatar, “Capacity of multi-antenna Gaussian channels,” European Trans. Telecommun., vol. 10, no. 6, pp. 585–595, Nov. 1995. [3] F. Rusek, D. Persson, B. K. Lau, E. G. Larsson, T. L. Marzetta, O. Edfors, and Tufvesson, “Scalling up MIMO: opportunities and challenges with very large arrays,” Available: arXiv:1201.321v1 [cs.IT], pp. 1–30, 16 Jan. 2012. [4] Y. C. Liang, S. Sun, and C. K. Ho, “Block-iterative generalized decision feedback equalizers for large MIMO systems: algorithm design and asymptotic performance analysis,” IEEE Trans. Signal Process., vol. 54, no. 6, pp. 2035–2048, June 1995. [5] K. V. Vardham, S. K. Mohammad, A. Chockalingam, and B. S. Rajan, “A low-complexity detector for large MIMO systems and multicarrier CDMA systems,” IEEE J. Sel. Areas Commun., vol. 26, no. 3, pp. 473– 485, Apr. 2008. [6] B. M. Hochwald and S. ten Brink, “Achieving near-capacity on a multiple-antenna channel,” IEEE Trans. Commun., vol. 51, no. 3, pp.389– 399, Mar. 2003. [7] V. Pan and R. Schreiber, “An improved Newton iteration for the generalized inverse of a matrix, with applications,” SIAM J. Scientific and Statistical Computing, vol. 12, no. 5, pp. 1109– 1130, Sep. 1991. [8] M. Pohst, “On the computation of lattice vectors of minimal length, successive minima and reduced basis with applications,” ACM SIGSAM Bull., vol. 15, pp. 37–44, 1981. [9] U. Fincke and M. Pohst, “Improved methods for calculating vectorsof short length in a lattice, including a complexity analysis,” Math. Comput., vol 44, pp. 463–471, Apr. 1985. [10] E.Viterbo and E.Biglieri,“A universal lattice decoder,”in 14eme Colloq.GRETSI, Juan-les- Pins, France, Sept.1993, pp. 611-614.
  • 9. International Journal of Research in Advent Technology, Vol.2, No.6, June 2014 E-ISSN: 2321-9637 236 [11] A. M. Chan and I. Lee, “A new reduced-complexity sphere decoder for multiple antenna systems,” in Proc. 2002 IEEE International Conferenceon Communications, vol. 1, pp. 460–464.