# An improved generalized Newton method for absolute value equations

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## Abstract

In this paper, we suggest and analyze an improved generalized Newton method for solving the NP-hard absolute value equations \(Ax-|x|=b\) when the singular values of A exceed 1. We show that the global and local quadratic convergence of the proposed method. Numerical experiments show the efficiency of the method and the high accuracy of calculation.

### Keywords

Absolute value equations Generalized Newton’s method Global and local convergence## Background

*x*| denotes a vector in \(R^n\), whose

*i*-th component is \(|x_i|\). A more general form of the AVEs, \(Ax+B|x|=b\), was introduced by Rohn (2004) and researched in a more general context in Mangasarian (2007a). Hu et al. (2011) proposed a generalized Newton method for solving absolute value equation \(Ax+B|x|=b\) associated with second order cones, and showed that the method is globally linearly and locally quadratically convergent under suitable assumptions. As was shown in Mangasarian and Meyer (2006) by Mangasarian, the general NP-hard linear complementarity problems (LCPs) (Cottle and Dantzing 1968; Chung 1989; Cottle et al. 1992) subsume many mathematical programming problems such as absolute value equations (AVEs) (1), which own much simpler structure than any LCP. Hence it has inspired many scholars to study AVEs. And in Mangasarian and Meyer (2006) the AVEs (1) was investigated in detail theoretically, the bilinear program and the generalized LCP were prescribed there for the special case when the singular values of

*A*are not less than 1. Based on the LCP reformulation, sufficient conditions for the existence and nonexistence of solutions are given in this paper. Mangasarian also has used concave minimization model (Mangasarian 2007b), dual complementarity (Mangasarian 2013), linear complementarity (Mangasarian 2014a), linear programming (Mangasarian 2014b) and a hybrid algorithm (Mangasarian 2015) to solve AVEs (1). Hu and Huang reformulated a system of absolute value equations as a standard linear complementarity problem without any assumption and gave some existence and convexity results for the solution set of the AVEs (1) in Hu and Huang (2010). Paper Zhang et al. (2015) presented a new algorithm which relaxes the absolute value equations into a convex optimization problem, Zhang et al. found the sparsest solution of AVEs by the minimum \(l_0\)-norm. Caccetta et al. proposed a globally and quadratically convergent method for AVEs in Caccetta et al. (2011). Rohn et al. gave an iterative method for AVEs (1) and analyzed the sufficient conditions of unique solvability by Rohn et al. (2014), Uniqueness is always a hot spot (Wu and Guo 2015), and Moosaei et al. gave the minimum norm solution of absolute value equations \(Ax-|x| = b\) which has multiple solutions (at most \(2^n\)) via simulated annealing algorithm in Moosaei et al. (2014). Salkuyeh (2014) put forward a hybrid algorithm which combined with skew-Hermitian and Picard-Hermitian splitting iteration method for solving AVEs (1), and gave the convergence analysis of the hybrid algorithm. Furthermore, Mangasarian (2009) clearly showed that generalized Newton method is a very effective method by solving some high dimensional examples in very few iterations. Haghani (2015) proposed an improved Newton method with two-step form, called Traub’s method, whose effectiveness is better than that of Mangasarian’s. Iqbal et al. (2015) proposed a Levenberg–Marquardt method for AVEs (1), which is the combination of steepest descent and the Gauss–Newton method. Paper Cruz et al. (2016) raised an inexact semi-smooth Newton algorithm for AVEs (1), and proved that the method is globally convergent. So, how to solve absolute value equations based on the classic Newton algorithm have been received many of the concerns. That have motivated us for trying to improve Newton method as the main aim of the present paper.

Now we describe our notation. The scalar product of two vectors *x* and *y* in the *n*-dimensional real space will be denoted by \(\langle x,y\rangle\). For \(x\in R^n\), the norm \(\Vert x\Vert\) will denote the two-norm \((x^T x)^{1/2}\) , and \({ sign}(x)\) will denote a vector with components equal to \(+1\), 0 or \(-1\), depending on whether the corresponding component of *x* is positive, zero or negative, respectively. In addition, diag(sign(*x*)) will denote a diagonal matrix corresponding to sign (*x*).

In “Preliminary” section of the present work we give the notations and preliminary notes about AVEs. “The improved generalized Newton method” section gives an improved generalized Newton iterative algorithm which is globally and locally quadratic convergent under certain assumptions. In “Computational results” section some numerical reports show the efficiency of the proposed scheme. “Conclusions” section gives some concluding remarks to end the paper.

## Preliminary

*f*(

*x*) specified by the AVEs (1) as follows:

*f*at

*x*is

*A*are exceed 1. However, the computational time of (5) is a little less than that of (4), with a higher residual error precision than (4).

## The improved generalized Newton method

*R*, which give us some inspiration. We will promote this idea to the

*n*-dimensional space. The iterative method is as follows:

We shall need a few theoretical results to establish convergence of Algorithm 1, we first quote the following two results from Mangasarian and Meyer (2006).

**Lemma 1**

*The singular values of the matrix* \(A\in R^{n\times n}\) *exceed 1 if and only if the minimum eigenvalue of* \(A'A\) *exceeds 1*.

**Lemma 2**

*If the singular values of* \(A\in R^{n\times n}\) *exceed 1 for the method* (6), *then* \((A-D)^{-1}\) *exists for any diagonal matrix* *D* *whose diagonal elements are* \(\pm 1\) *or* 0.

Therefore, the sequence of vector iterates form (6) is well defined no matter how to choose the initial vector \(x^0\) in \(R^n\).

We now prove the proposed Newton direction \(d^k\) of (7) is a descent direction for the objective function \(\Vert f(x)\Vert ^2\).

**Lemma 3**

*If the singular values of* \(A\in R^{n\times n}\) *exceed 1, then the proposed Newton direction* \(d^k\) *of* (7) *is a descent direction for the objective function* \(F(x)=\frac{1}{2}\Vert f(x)\Vert ^2\).

*Proof*

Since \(f(x)=Ax-|x|-b, \partial f(x)=A-D(x)\), and \((A-D(x))^{-1}\) exists for any diagonal matrix *D* whose diagonal elements are \(\pm 1\) or 0.

*F*(

*x*). \(\square\)

**Lemma 4**

*Let the singular values of* *A* *exceed 1, then the sequence* \(\{x_k\}\) *generated by the improved generalized Newton method* (6) *is bounded, and there exists an accumulation point* \(\bar{x}\) *such that* \((A-\bar{D})\bar{x}=b+\bar{a} f(\bar{x})\) *for some diagonal matrixes* \(\bar{D}\) *with diagonal elements of* \(\pm 1\) *or* 0.

*Proof*

**Theorem 1**

(Global linear convergence) *If* \(\Vert (A-D)^{-1}\Vert <\frac{1}{3}\) *for any diagonal matrix* *D* *with diagonal elements of* \(\pm 1\) *or* 0, *then the improved generalized Newton method* (6) *converges linearly from any starting point* \(x^0\) *to a solution* \(\bar{x}\) *for any solvable AVEs* (1).

*Proof*

The proof is complete. \(\square\)

**Theorem 2**

*If* \(\Vert A^{-1}\Vert <\frac{1}{4}\) *and* \(D(x^k)\ne 0\) *for any diagonal matrix* \(D(x^k)\) *with diagonal elements of* \(\pm 1\) *or* 0, *then the Algorithm 1 converges linearly from any starting point* \(x^0\) *to a solution* \(\bar{x}\) *for any solvable AVEs* (1).

*Proof*

The proof directly from Mangasarian (2009, Proposition 7). It is hence omitted.

In the following, we use Eq. (7) to prove the locally quadratic convergence of the Algorithm 1. \(\square\)

**Lemma 5**

*If* \(A-D\) *is nonsingular for any diagonal matrix* *D* *with diagonal elements of* \(\pm 1\) *or* 0, *then the Algorithm 1 is approximately Newton’s method*.

*Proof*

*k*, \(f(y^k) =O(\Vert y^k-\bar{x}\Vert ^2)\), thus

*k*is sufficiently large and \((A-D(x^k)\) is uniformly bounded \((|A-D(x^k)|<|A|+|D(x^k)|<|A|+1)\), \(d^k=O(f(x^k))\). Then, \(f(y^k)-f(x^k)=-f(x^k)+O(\Vert f(x^k)\Vert ^2)\), we also have \(\Vert f(x^k)\Vert =\Vert (A-D(\overline{}\overline{x}))(x^k-\overline{x})\Vert =O(\Vert x^k-\overline{x}\Vert )=:O(\Vert c^k\Vert )\), where \(c^k:=x^k-\overline{x}\). Thus, \(f(y^k)=O(\Vert c^k\Vert ^2)\), and

**Theorem 3**

(Locally quadratic convergence) *If* \(A-D\) *is nonsingular for any diagonal matrix* *D* *with diagonal elements of* \(\pm 1\) *or* 0, *then the sequence* \(\{x^k\}\) *from improved generalized Newton’s method* (7) *converges to* \(\bar{x}\) *and* \(\Vert x^{k+1}-\bar{x}\Vert =O(\Vert x^k-\bar{x}\Vert ^2)\).

## Computational results

To illustrate the implementation and efficiency of the proposed method, we test the following two examples. All the experiments are performed by MATLAB R2010a. In comparisons, NM, TM and INM denote the generalized Newton’s method (4), the generalized Traub’s method (5) and the improved generalized Newton’s method (6), respectively.

*Example 1*

*A*according to the following formula:

*n*. To ensure that the minimum singular value of each A exceeds 1, we compute the minimum singular value of

*A*and reseal

*A*by the minimum singular value multiply by a random number in the interval [1, 2], The results are shown in Table 1.

The comparison of NM, TM and INM in Example 1

Dim | NM | TM | INM | ||||||
---|---|---|---|---|---|---|---|---|---|

K | ACC | T | K | ACC | T | K | ACC | T | |

100 | 3 | \(1.6125\times 10^{-10}\) | 0.0036 | 3 | \(1.8416\times 10^{-11}\) | 0.0031 | 3 | \(1.6168\times 10^{-11}\) | 0.0027 |

200 | 3 | \(6.0215\times 10^{-10}\) | 0.0097 | 3 | \(7.0496\times 10^{-11}\) | 0.0095 | 3 | \(6.2749\times 10^{-11}\) | 0.0084 |

300 | 3 | \(1.2931\times 10^{-9}\) | 0.0216 | 3 | \(1.6284\times 10^{-10}\) | 0.0071 | 3 | \(4.5510\times 10^{-10}\) | 0.0217 |

400 | 3 | \(2.5705\times 10^{-9}\) | 0.0567 | 3 | \(2.6186\times 10^{-10}\) | 0.0517 | 3 | \(7.6406\times 10^{-10}\) | 0.0321 |

500 | 3 | \(4.3078\times 10^{-8}\) | 0.0831 | 3 | \(4.7102\times 10^{-10}\) | 0.0944 | 3 | \(3.5408\times 10^{-10}\) | 0.0512 |

600 | 4 | \(6.3700\times 10^{-8}\) | 0.1365 | 3 | \(5.5877\times 10^{-10}\) | 0.1576 | 3 | \(4.1326\times 10^{-10}\) | 0.0906 |

700 | 4 | \(7.0085\times 10^{-8}\) | 0.2227 | 3 | \(1.0945\times 10^{-9}\) | 0.2304 | 3 | \(8.8369\times 10^{-10}\) | 0.1278 |

800 | 4 | \(2.1838\times 10^{-7}\) | 0.3766 | 4 | \(2.0634\times 10^{-9}\) | 0.3103 | 4 | \(2.5631\times 10^{-9}\) | 0.1788 |

900 | 4 | \(3.6958\times 10^{-7}\) | 0.4706 | 4 | \(6.9784\times 10^{-9}\) | 0.4173 | 4 | \(2.9899\times 10^{-9}\) | 0.2325 |

1000 | 5 | \(6.3484\times 10^{-7}\) | 0.6973 | 4 | \(1.7392\times 10^{-8}\) | 0.5221 | 4 | \(6.3255\times 10^{-9}\) | 0.3063 |

*Example 2*

*A*of which all the singular values are greater than 1 is generated by the following MATLAB procedure:

The comparison of NM, TM and INM in Example 2

Dim | NM | TM | INM | ||||||
---|---|---|---|---|---|---|---|---|---|

K | ACC | T | K | ACC | T | K | ACC | T | |

100 | 3 | \(1.7851\times 10^{-11}\) | 0.0042 | 3 | \(1.1360\times 10^{-11}\) | 0.0333 | 3 | \(1.2528\times 10^{-11}\) | 0.0029 |

200 | 3 | \(3.3603\times 10^{-10}\) | 0.0146 | 3 | \(8.0510\times 10^{-11}\) | 0.0132 | 3 | \(6.7278\times 10^{-11}\) | 0.0069 |

300 | 3 | \(3.9958\times 10^{-9}\) | 0.0392 | 3 | \(2.8067\times 10^{-10}\) | 0.0301 | 3 | \(2.6026\times 10^{-10}\) | 0.0203 |

400 | 3 | \(7.3587\times 10^{-9}\) | 0.0857 | 3 | \(6.8738\times 10^{-10}\) | 0.0681 | 3 | \(5.7847\times 10^{-10}\) | 0.0444 |

500 | 3 | \(2.1626\times 10^{-9}\) | 0.1411 | 3 | \(1.1259\times 10^{-9}\) | 0.1085 | 3 | \(1.1792\times 10^{-9}\) | 0.0679 |

600 | 4 | \(1.1403\times 10^{-8}\) | 0.2356 | 3 | \(2.1310\times 10^{-9}\) | 0.1595 | 3 | \(2.4023\times 10^{-9}\) | 0.1055 |

700 | 4 | \(4.6354\times 10^{-8}\) | 0.3993 | 3 | \(2.9880\times 10^{-9}\) | 0.2681 | 3 | \(3.6051\times 10^{-9}\) | 0.1704 |

800 | 4 | \(5.7742\times 10^{-8}\) | 0.4829 | 4 | \(5.1658\times 10^{-9}\) | 0.3543 | 3 | \(3.8475\times 10^{-9}\) | 0.2239 |

900 | 5 | \(6.4563\times 10^{-8}\) | 0.5749 | 4 | \(6.9541\times 10^{-9}\) | 0.4665 | 3 | \(7.0228\times 10^{-9}\) | 0.3076 |

1000 | 5 | \(8.6322\times 10^{-8}\) | 0.7589 | 4 | \(8.8558\times 10^{-9}\) | 0.6615 | 3 | \(7.3382\times 10^{-9}\) | 0.4127 |

In Tables 1 and 2, Dim, K, ACC and T denote the dimensions of the problem, the number of iterations, \(\Vert Ax^k-|x^k|-b\Vert _2\) and times(s), respectively. It is evident from Tables 1 and 2 that the improved generalized Newton’s method is very effective for solving large problems.

## Conclusions

In this paper, we have proposed the generalized Newton’s method with special search direction for solving the NP-hard absolute value equations under certain assumptions on *A*. The method have some nice convergence properties and calculation results. Further work is to find more effective methods for AVEs.

## Notes

### Authors’ contributions

Analysis is done by FJM and LSY. Algorithm design and data simulation are carried out by FJM. Manuscript is drafted by FJM with contribution from LSY. Both authors read and approved the final manuscript.

### Acknowledgements

The authors thank the referee for helpful suggestions, which have greatly improved the earlier version of our paper. The research are supported by the National Natural Science Foundation of China (Grant Nos. 11301409, 61373174).

### Competing interests

Both authors declare that they have no competing.

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