Research article Topical Sections

Effect of the incorporation of BiFeO3 on the structural, electrical and magnetic properties of the lead-free Bi0.5Na0.5TiO3

  • Received: 07 September 2021 Accepted: 26 October 2021 Published: 05 November 2021
  • Powders of the system (1–x)Bi0.5Na0.5TiO3xBiFeO3 (x = 0, 0.02, 0.08, 0.10) are synthesized by the combustion reaction method. The crystal structure and the particle size of Bi0.5Na0.5TiO3 are modified by the incorporation of BiFeO3, as can be seen from the infrared spectroscopy and X-ray diffraction results. The inclusion of iron and the increase in the molar percentage of bismuth in the BNT matrix generate new bonds with a different force constant. The structural analysis showed that the addition of BFO to the BNT does not induce any structural phase transition, preserving the rhombohedral symmetry of the Bi0.5Na0.5TiO3 system. The electrical measurements show that the incorporation of iron increases the conductivity of the system generated by an increase in the concentration of oxygen vacancies; alternatively, the addition of 10% of BiFeO3 generates ferrimagnetic behavior reflected in the magnetic hysteresis curves obtained at room temperature.

    Citation: Wolfgang Zúñiga-Mera, Sonia Gaona Jurado, Alejandra Isabel Guerrero Duymovic, Claudia Fernanda Villaquirán Raigoza, José Eduardo García. Effect of the incorporation of BiFeO3 on the structural, electrical and magnetic properties of the lead-free Bi0.5Na0.5TiO3[J]. AIMS Materials Science, 2021, 8(5): 792-808. doi: 10.3934/matersci.2021048

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  • Powders of the system (1–x)Bi0.5Na0.5TiO3xBiFeO3 (x = 0, 0.02, 0.08, 0.10) are synthesized by the combustion reaction method. The crystal structure and the particle size of Bi0.5Na0.5TiO3 are modified by the incorporation of BiFeO3, as can be seen from the infrared spectroscopy and X-ray diffraction results. The inclusion of iron and the increase in the molar percentage of bismuth in the BNT matrix generate new bonds with a different force constant. The structural analysis showed that the addition of BFO to the BNT does not induce any structural phase transition, preserving the rhombohedral symmetry of the Bi0.5Na0.5TiO3 system. The electrical measurements show that the incorporation of iron increases the conductivity of the system generated by an increase in the concentration of oxygen vacancies; alternatively, the addition of 10% of BiFeO3 generates ferrimagnetic behavior reflected in the magnetic hysteresis curves obtained at room temperature.



    A matrix A=[aij]Cn×n is called a strictly diagonally dominant (SDD) matrix if

    |aii|>ri(A) (1.1)

    for all iN:={1,,n}, where ri(A)=jN{i}|aij|.

    The concept of SDD originated from the well-known Lévy-Desplanques Theorem [1], which states that if condition (1.1) holds, then A is nonsingular, i.e., SDD matrices are nonsingular. It is well known that the class of SDD matrices has wide applications in many fields of scientific computing, such as the Schur complement problem [2,3], eigenvalue localizations [4,5,6,7,8,9,10], convergence analysis of the parallel-in-time iterative method [11], estimating the infinity norm for the inverse of H-matrices [12,13,14,15], error bound for linear complementarity problems [16,17], structure tensors [18,19], etc.

    Some well-known matrices have been presented and studied [4,7,20] by breaking the diagonal dominance condition (1.1). For instance, by allowing at most one row to be non-SDD, Ostrowski introduced the class of Ostrowski matrices [20] (also known as doubly strictly diagonally dominant (DSDD) matrices). Here, a matrix A=[aij]Cn×n is an Ostrowski matrix [20] if for all ji,

    |aii||ajj|>ri(A)rj(A).

    In addition, based on the partition-based approach that allows more than one row to be non-SDD, a well-known class of matrices called S-SDD matrices has been proposed and studied [7,21].

    Definition 1.1. [7,21] Let A=[aij]Cn×n and S be a nonempty proper subset of N. Then, a matrix A is called an S-SDD matrix if

    {|aii|>rSi(A),iS,(|aii|rSi(A))(|ajj|r¯Sj(A))>r¯Si(A)rSj(A),iS,j¯S,

    where rSi(A)=jS{i}|aij|.

    Besides DSDD matrices and S-SDD matrices, there are many generalizations of SDD matrices, such as Nekrasov matrices [22,23], DZ-type matrices [24], CKV-type matrices [25] and so on.

    Observe from Definition 1.1 that S-SDD matrices only consider the effect of "interaction" between iS and j¯S on the nonsingular. However, other "interaction, " such as the "constraint condition" between iS (i¯S) and jS (j¯S) with ij, might also affect the non-singularity of the matrix. Naturally, an interesting question arises: When we consider this "constraint condition, " can we get the non-singularity of the matrix? To answer this question, in this paper, we introduce a new class of nonsingular matrices arising from this "constraint condition" and show several benefits from this new class of matrices, which we will call partially doubly strictly diagonally dominant matrices.

    This paper is organized as follows. In Section 2, we present a new class of matrices called PDSDD matrices and prove that it is a subclass of nonsingular H-matrices, which is similar to, but different from, the class of S-SDD matrices. Section 3 gives a new eigenvalue localization set for matrices and presents an infinity norm bound for the inverse of PDSDD matrices. It is proved that the obtained bound is better than the well-known Varah's bound for SDD matrices. Based on this infinity norm bound, we also obtain a new pseudospectra localization for matrices and apply it to measure the distance to instability. Finally, we give concluding remarks in Section 4.

    We start with some preliminaries and definitions. Let Zn×n be the set of all matrices A=[aij]Rn×n with aij0 and ij. A matrix AZn×n is called a nonsingular M-matrix if its inverse is nonnegative, i.e., A10 [26]. A matrix A=[aij]Cn×n is called a nonsingular H-matrix [26] if its comparison matrix M(A)=[mij]Rn×n defined by

    mij={|aij|,i=j,|aij|,ij,

    is a nonsingular M-matrix. Let |N| be the cardinality of set N.

    In the following, we define a new class of matrices called PDSDD matrices.

    Definition 2.1. Let S be a subset of N and ¯S be the complement of S. Given a matrix A=[aij]Cn×n, for each subset Δ{S,¯S}, denote Δ:={iΔ|aiiri(A)} and Δ+:={iΔ|aii>ri(A)}. Then, a matrix A is called a partially doubly strictly diagonally dominant (PDSDD) matrix if for each Δ{S,¯S} either |Δ|=0 or |Δ|=1, and for iΔ,

    {|aii|>r¯Δi(A),(|aii|r¯Δi(A))(|ajj|rΔj(A)+|aji|)>rΔi(A)(r¯Δj(A)+|aji|),jΔ+, (2.1)

    where rΔi(A)=jΔ{i}|aij|.

    Note that the class of DSDD matrices allows at most one row to be non-SDD, whereas the class of matrices defined in Definition 2.1 allows at most one row to be non-SDD in each subset Δ{S,¯S}. For this reason, we call it the class of PDSDD matrices.

    The following theorem provides that the class of PDSDD matrices is a subclass of nonsingular H-matrices.

    Theorem 2.1. Every PDSDD matrix is a nonsingular H-matrix.

    Proof. According to the well-known result that SDD matrices are nonsingular H-matrices, it is sufficient to consider the case that A has one or two non-SDD rows. Assume, on the contrary, that A is a singular matrix, and then there exists a nonzero eigenvector x=[x1,x2,,xn]T corresponding to 0 eigenvalue such that

    Ax=0. (2.2)

    Let |xp|:=maxiN{|xi|}. Then, |xp|>0, and pΔ¯Δ, where Δ{S,¯S}. Without loss of generality, we assume that Δ=S. Next, we need only consider the case pS, and another case p¯S can be proved similarly. For pS, it follows from Definition 2.1 that pSS+, where S:={iS|aiiri(A)} and S+:={iS|aii>ri(A)}.

    If pS, then by Definition 2.1 we have

    |app|>r¯Sp(A), (2.3)

    and for all jS+,

    (|app|r¯Sp(A))(|ajj|rSj(A)+|ajp|)>rSp(A)(r¯Sj(A)+|ajp|). (2.4)

    Note that |S|=1. Then, S{p}=S+. Let |xq|:=maxkS{p}{|xk|}. Considering the p-th equality of (2.2), we have

    appxp=kp,kSapkxkkp,k¯Sapkxk.

    Taking the modulus in the above equation and using the triangle inequality yields

    |app||xp|kp,kS|apk||xk|+kp,k¯S|apk||xk|kp,kS|apk||xq|+kp,k¯S|apk||xp|=rSp(A)|xq|+r¯Sp(A)|xp|,

    which implies that

    (|app|r¯Sp(A))|xp|rSp(A)|xq|. (2.5)

    If |xq|=0, then |app|r¯Sp(A)0 as |xp|>0, which contradicts (2.3). If |xq|0, then from the q-th equality of (2.2), we obtain

    |aqq||xq|kq,kS|aqk||xk|+kq,k¯S|aqk||xk|(kq,kS|aqk||aqp|)|xq|+(kq,k¯S|aqk|+|aqp|)|xp|=(rSq(A)|aqp|)|xq|+(r¯Sq(A)+|aqp|)|xp|,

    i.e.,

    (|aqq|rSq(A)+|aqp|)|xq|(r¯Sq(A)+|aqp|)|xp|. (2.6)

    Multiplying (2.6) with (2.5) and dividing by |xp||xq|>0, we have

    (|app|r¯Sp(A))(|aqq|rSq(A)+|aqp|)rSp(A)(r¯Sq(A)+|aqp|),

    which contradicts (2.4).

    If pS+, then |app|>rp(A). Considering the p-th equality of (2.2) and using the triangle inequality, we obtain

    |app||xp|kp|apk||xk|rp(A)|xp|,

    i.e., |app|rp(A), which contradicts |app|>rp(A). Hence, we can conclude that 0 is not an eigenvalue of A, that is, A is a nonsingular matrix.

    We next prove that A is a nonsingular H-matrix. For any ε0, let

    Bε=M(A)+εI=[bij].

    Note that bii=|aii|+ε, bij=|aij|, and BεZn×n. Then, Δ(Bε)Δ(A), and Δ+(A)Δ+(Bε). If A is an SDD matrix, then Δ(A)=, and thus Δ(Bε)=, which implies that Bε is an SDD matrix. If A is not an SDD matrix, then |Δ(A)|=1 for some Δ{S,¯S}. For this case, |Δ(Bε)|=0 or |Δ(Bε)|=1. If |Δ(Bε)|=0 for each Δ{S,¯S}, then Bε is also an SDD matrix. If |Δ(Bε)|=1 for some Δ{S,¯S}, then Δ(Bε)=Δ(A) and Δ+(Bε)=Δ+(A). Hence, for iΔ(Bε),

    |bii|r¯Δi(Bε)=|aii|+εr¯Δi(A)>0,

    and for all jΔ+(Bε),

    (|bii|r¯Δi(Bε))(|bjj|rΔj(Bε)+|bji|)=(|aii|+εr¯Δi(A))(|ajj|+εrΔj(A)+|aji|)(|aii|r¯Δi(A))(|ajj|rΔj(A)+|aji|)>rΔi(A)(r¯Δj(A)+|aji|)=r¯Δi(Bε)(rΔj(Bε)+|bji|).

    Therefore, Bε is a PDSDD matrix and thus nonsingular for each ε0. This implies that M(A) is a nonsingular M-matrix (see the condition (D15) of Theorem 2.3 in [26, Chapter 6]). Therefore, A is a nonsingular H-matrix. The proof is complete.

    Proposition 2.1. Every DSDD matrix is a PDSDD matrix.

    Proof. If A is an SDD matrix, then A is a PDSDD matrix. If A is not an SDD matrix, then by the assumptions it holds that there exists i0N such that |ai0i0|ri0(A) and

    |ai0i0||ajj|>ri0(A)rj(A)for allji0.

    Taking S=N, we have r¯Si(A)=0 and rSi(A)=ri(A) for all iN. This implies that for all jS{i0},

    (|ai0i0|r¯Si0(A))(|ajj|rSj(A)+|aji0|)rSi0(A)(r¯Sj(A)+|aji0|)=|ai0i0|(|ajj|rj(A)+|aji0|)ri0(A)|aji0|=|ai0i0||ajj||ai0i0|(rj(A)|aji0|)ri0(A)|aji0||ai0i0||ajj|ri0(A)(rj(A)|aji0|+|aji0|)=|ai0i0||ajj|ri0(A)rj(A)>0.

    Hence, by Definition 2.1, we conclude that A is a PDSDD matrix. The proof is complete.

    Next, we give an example to show that neither PDSDD matrices nor S-SDD matrices are included in each other.

    Example 2.1. Consider the following matrices:

    A=[3130130801300008],B=[3003030300330008].

    By calculation, we know that A is a PDSDD matrix for S={1,3}, but it is not an S-SDD matrix for any nonempty proper subset S of N and thus not a DSDD matrix. Meanwhile, B is an S-SDD matrix for S={1,2,3}, but it is not a PDSDD matrix, because B has three non-SDD rows.

    According to Theorem 2.1, Proposition 2.1 and Example 2.1, the relations among DSDD matrices, PDSDD matrices, S-SDD matrices and H-matrices can be depicted as follows:

    {PDSDD}{H},{PDSDD}{S-SDD},{S-SDD}{PDSDD},

    and

    {DSDD}{PDSDD}{S-SDD}.

    It is well known that the non-singularity of matrices can generate the equivalent eigenvalue inclusion set in the complex plane [4,5,7,9,24]. By the non-singularity of PDSDD matrices, we in this section give a new eigenvalue localization set for matrices. Before that, an equivalent condition for the definition of PDSDD matrices is given, which can be proved immediately from Definition 2.1.

    Lemma 3.1. Let A=[aij]Cn×n and {S,¯S} be a partition of the set N. A matrix A is called a PDSDD matrix if and only if S is not empty unless S is empty, and ¯S is not empty unless ¯S is empty, where

    S:={iS:|aii|>r¯Si(A),andforalljS{i},|ajj|>rj(A)and(|aii|r¯Si(A))(|ajj|rSj(A)+|aji|)>rSi(A)(r¯Sj(A)+|aji|)},

    and

    ¯S:={i¯S:|aii|>rSi(A),andforallj¯S{i},|ajj|>rj(A)and(|aii|rSi(A))(|ajj|r¯Sj(A)+|aji|)>r¯Si(A)(rSj(A)+|aji|)}

    with rSi(A)=jS{i}|aij|.

    By Lemma 3.1, we can obtain the following theorem.

    Theorem 3.1. Let A=[aij]Cn×n and S be any subset of N. Then,

    σ(A)ΘS(A):=θS(A)θ¯S(A),

    where σ(A) is the set of all the eigenvalues of A,

    θS(A)=iS(Γ¯Si(A))(jS{i}(ˆV¯Sij(A)Γj(A)))

    and

    θ¯S(A)=i¯S(ΓSi(A))(j¯S{i}(ˆVSij(A)Γj(A)))

    with

    ΓSi(A):={zC:|zaii|rSi(A)},Γj(A):={zC:|zajj|rj(A)},

    and

    ˆVSij(A):={zC:(|zaii|rSi(A))(|zajj|r¯Sj(A)+|aji|)r¯Si(A)(rSj(A)+|aji|)}.

    Proof. Without loss of generality, we assume that S is a nonempty subset of N. For the case of S=, we have ΘS(A)=θ¯S(A), and the conclusion can be proved similarly. Suppose, on the contrary, that there exists an eigenvalue λ of A such that λΘS(A), that is, λθS(A) and λθ¯S(A). For λθS(A), there exists an index iS such that λΓ¯Si(A), and for all jS{i}, λΓj(A) and λˆV¯Sij(A), that is, |λaii|>r¯Si(A), |λajj|>rj(A), and

    (|λaii|r¯Si(A))(|λajj|rSj(A)+|aji|)>rSi(A)(r¯Sj(A)+|aji|).

    Similarly, for λθ¯S(A), there exists an index i¯S such that λΓSi(A), and for all j¯S{i}, λΓj(A) and λˆVSij(A), that is, |λaii|>rSi(A), |λajj|>rj(A), and

    (|λaii|rSi(A))(|λajj|r¯Sj(A)+|aji|)>r¯Si(A)(rSj(A)+|aji|).

    These imply that S(λIA) and ¯S(λIA) are not empty. It follows from Lemma 3.1 that λIA is a PDSDD matrix. Then, by Theorem 2.1, λIA is nonsingular, which contradicts that λ is an eigenvalue of A. Hence, λΘS(A). This completes the proof.

    Remark 3.1. Take the intersection over all possible subsets S of N, and we can get a satisfactory eigenvalue localization although it has more computation costs:

    σ(A)Θ(A):=SNΘS(A).

    To compare our set Θ(A) with the Geršgorin disks Γ(A) in [8], Brauer's ovals of Cassini K(A) in [27] and the Cvetković-Kostić-Varga eigenvalue localization set C(A) in [7], }let us recall the definitions of Γ(A), K(A) and C(A) as follows.

    Theorem 3.2. [8] Let A=[aij]Cn×n and σ(A) be the set of all eigenvalues of A. Then,

    σ(A)Γ(A):=iNΓi(A),

    where Γi(A)={zC:|aiiz|ri(A)}.

    Theorem 3.3. [27] Let A=[aij]Cn×n and σ(A) be the set of all eigenvalues of A. Then,

    σ(A)K(A):=i,jN,ijKij(A),

    where Kij(A)={zC:|aiiz||ajjz|ri(A)rj(A)}.

    Theorem 3.4. [7] Let S be any nonempty proper subset of N, and n2. Then, for any A=[aij]Cn×n, all the eigenvalues of A belong to set

    CS(A)=(iSΓSi(A))(iS,j¯SVSij(A)),

    and hence

    σ(A)C(A):=SN,S,SNCS(A),

    where ΓSi(A) is given by Theorem 3.1, and

    VSij(A):={zC:(|zaii|rSi(A))(|zajj|r¯Sj(A))r¯Si(A)rSj(A)}.

    Remark 3.2. Observe that the class of SDD matrices is a subclass of DSDD matrices, which is a subclass of of PDSDD matrices. Hence, the corresponding set Θ(A) will contain Brauer's ovals of Cassini K(A), which contains the Geršgorin disks Γ(A), that is,

    Θ(A)K(A)Γ(A).

    In addition, because PDSDD class and S-SDD class do not contain each other, it follows that the relation between Θ(A) and C(A) is

    Θ(A)C(A)andC(A)Θ(A).

    In this section, we consider the infinity norm bounds for the inverse of PDSDD matrices, since it might be used for the convergence analysis of matrix splitting and matrix multi-splitting iterative methods for solving large sparse systems of linear equations, linear complementarity problems and pseudospectra localizations.

    Theorem 3.5. Let A=[aij]Cn×n be a PDSDD matrix. Then,

    ||A1||max{miniSmax{1|aii|r¯Si(A),φSi(A)},mini¯Smax{1|aii|rSi(A),φ¯Si(A)}}, (3.1)

    where S and ¯S are defined by Lemma 3.1,

    φSi(A):=maxjS{i}{XSij(A),1|ajj|rj(A)}

    with

    XSij(A):=|ajj|rSj(A)+|aji|+rSi(A)(|aii|r¯Si(A))(|ajj|rSj(A)+|aji|)rSi(A)(r¯Sj(A)+|aji|).

    Proof. According to a well-known fact (see [10,30]),

    ||A1||1=infx0||Ax||||x||=min||x||=1||Ax||=||Ax||=maxiN|(Ax)i|

    for some x=[x1,x2,,xn]T such that ||x||=1. Denote |xp|=||x||=1. It follows that

    ||A1||1|(Ax)p|.

    Consider the p-th row of Ax, and we have

    (Ax)p=appxp+jpapjxj. (3.2)

    Since A is a PDSDD matrix, it follows from Lemma 3.1 that S is not empty unless S is empty, and ¯S is not empty unless ¯S is empty. We only consider the case both S and ¯S are not empty, and the case of S= or ¯S= can be proved similarly.

    The first case. Suppose that either S or ¯S is a singleton set. We assume that S={k}. Then, ¯S=N{k}, and from Lemma 3.1 it holds that S is not empty and ¯S is not empty, that is,

    |akk|>r¯Sk(A)=rk(A).

    For each i0¯S, |ai0i0|>rSi0(A), and for all j¯S{i0},

    (|ai0i0|rSi0(A))(|ajj|r¯Sj(A)+|aji0|)>r¯Si(A)(rSj(A)+|aji0|). (3.3)

    Note that pS¯S. If pS={k}, then

    |app||(Ax)p|+rp(A),

    and

    ||A1||1|(Ax)p||app|rp(A)>0.

    Hence,

    ||A1||1|app|rp(A)=1|akk|r¯Sk(A). (3.4)

    If p¯S, then p=i0 or pi0, where i0¯S. If p=i0, then let |xq|=maxj¯S{p}{|xj|}. By (3.2), it follows that

    appxp=(Ax)pjp,jSapjxjjp,j¯Sapjxj,

    and taking absolute values on both sides and using the triangle inequality, we get

    |app||xp||(Ax)p|+jp,jS|apj||xj|+jp,j¯S|apj||xj||(Ax)p|+jp,jS|apj||xp|+jp,j¯S|apj||xq|||A1||1+rSp(A)|xp|+r¯Sp(A)|xq|,

    which implies that

    |app|||A1||1rSp(A)r¯Sp(A)|xq|. (3.5)

    Consider the q-th row of Ax, and we have

    (Ax)q=aqqxq+jqaqjxj.

    It follows that

    |aqq||xq||(Ax)q|+(jq,j¯S|aqj||aqp|)|xq|+(jq,jS|aqj|+|aqp|)|xp|||A1||1+(r¯Sq(A)|aqp|)|xq|+(rSq(A)+|aqp|),

    i.e.,

    (|aqq|r¯Sq(A)+|aqp|)|xq|||A1||1+(rSq(A)+|aqp|). (3.6)

    Then, from (3.5) and (3.6), we get that

    |app|||A1||1rSp(A)r¯Sp(A)|xq|||A1||1+rSq(A)+|aqp||aqq|r¯Sq(A)+|aqp|,

    which implies that

    ||A1|||aqq|r¯Sq(A)+|aqp|+r¯Sp(A)(|app|rSp(A))(|aqq|r¯Sq(A)+|aqp|)r¯Sp(A)(rSq(A)+|aqp|)maxj¯S{i0}|ajj|r¯Sj(A)+|aji0|+r¯Si0(A)(|ai0i0|rSi0(A))(|ajj|r¯Sj(A)+|aji0|)r¯Si0(A)(rSj(A)+|aji0|):=maxj¯S{i0}X¯Si0j(A). (3.7)

    If pi0, then |app|>rp(A). Similarly to the proof of (3.4), we obtain

    ||A1||1|app|rp(A)maxj¯S{i0}1|ajj|rj(A).

    Hence,

    ||A1||maxj¯S{i0}{X¯Si0j(A),1|ajj|rj(A)}.

    Since i0 is arbitrary in ¯S, it follows that

    ||A1||mini¯Smaxj¯S{i}{X¯Sij(A),1|ajj|rj(A)}. (3.8)

    By (3.4) and (3.8), it holds that

    ||A1||max{miniS1|aii|r¯Si(A),mini¯Smaxj¯S{i}{X¯Sij(A),1|ajj|rj(A)}}.

    If ¯S is a singleton set, then similar to the above case, we obtain

    ||A1||max{miniSmaxjS{i}{XSij(A),1|ajj|rj(A)},mini¯S1|aii|rSi(A)}.

    The second case. Suppose that both S and ¯S are singleton sets. By Lemma 3.1, it follows that S is not empty, and ¯S is not empty. Then, similar to the proof of the first case, we have

    ||A1||miniSmaxjS{i}{XSij(A),1|ajj|rj(A)},

    and

    ||A1||mini¯Smaxj¯S{i}{X¯Sij(A),1|ajj|rj(A)}.

    Now, the conclusion follows from the above two cases.

    In [15], an elegant upper bound for the inverse of SDD matrices is presented.

    Theorem 3.6. [15] Let A=[aij]Cn×n be an SDD matrix. Then,

    ||A1||maxiN1|aii|ri(A).

    This bound is usually called Varah's bound and plays a critical role in numerical algebra [11,16,28,29]. As discussed before, an SDD matrix is a PDSDD matrix as well. Thus, Theorem 3.5 can be applied to SDD matrices. In the following, we show that bound (3.1) of Theorem 3.5 works better than Varah's bound of Theorem 3.6.

    Theorem 3.7. Let A=[aij]Cn×n be an SDD matrix and S be any subset of N. Then,

    ||A1||φS(A)maxiN1|aii|ri(A),

    where

    φS(A):=max{miniSmax{1|aii|r¯Si(A),φSi(A)},mini¯Smax{1|aii|rSi(A),φ¯Si(A)}}

    and φSi(A) is given by Theorem 3.5.

    Proof. Since A is an SDD matrix, it follows from Lemma 3.1 that S=S for any subset S of N. Hence, by Theorem 3.5, it follows that

    ||A1||φS(A).

    We next prove that φS(A)maxiN1|aii|ri(A). Define |ai0i0|ri0(A):=miniN{|aii|ri(A)}. Obviously, for each iN,

    1|aii|rSi(A)1|ai0i0|ri0(A)and1|aii|r¯Si(A)1|ai0i0|ri0(A).

    Note that for each iS,

    φSi(A):=maxjS{i}{XSij(A),1|ajj|rj(A)} (3.9)

    and

    XSij(A):=|ajj|rSj(A)+|aji|+rSi(A)(|aii|r¯Si(A))(|ajj|rSj(A)+|aji|)rSi(A)(r¯Sj(A)+|aji|).

    If |aii|ri(A)|ajj|rj(A), then

    (|aii|r¯Si(A))(|ajj|rSj(A)+|aji|)rSi(A)(r¯Sj(A)+|aji|)=(|aii|ri(A))(|ajj|rSj(A)+|aji|)+rSi(A)(|ajj|rj(A))(|ajj|rj(A))(|ajj|rSj(A)+|aji|)+rSi(A)(|ajj|rj(A))=(|ajj|rj(A))(|ajj|rSj(A)+|aji|+rSi(A)),

    which implies that

    XSij(A)1|ajj|rj(A)1|ai0i0|ri0(A). (3.10)

    If |aii|ri(A)<|ajj|rj(A), then

    (|aii|r¯Si(A))(|ajj|rSj(A)+|aji|)rSi(A)(r¯Sj(A)+|aji|)=(|aii|ri(A))(|ajj|rSj(A)+|aji|)+rSi(A)(|ajj|rj(A))>(|aii|ri(A))(|ajj|rSj(A)+|aji|)+rSi(A)(|aii|ri(A))=(|aii|ri(A))(|ajj|rSj(A)+|aji|+rSi(A)),

    which implies that

    1|ajj|rj(A)<XSij(A)<1|aii|ri(A)1|ai0i0|ri0(A). (3.11)

    By (3.9), (3.10) and (3.11), it follows that for each iS,

    φSi(A)1|ai0i0|ri0(A).

    Similarly, for each i¯S, we can see that

    φ¯Si(A)1|ai0i0|ri0(A).

    This completes the proof.

    Remark 3.3. For SDD matrices, consider the intersection over all possible subsets S of N, and a tighter upper bound for ||A1|| can be obtained from Theorem 3.7:

    ||A1||minSNφS(A)φS(A)maxiN1|aii|ri(A).

    Besides SDD matrices, for other subclasses of H-matrices, such as DSDD matrices, S-SDD matrices and Nekrasov matrices, various infinity norm bounds for their inverse have also been derived. For details, see [12,23,28,29,30,31,32,33] and references therein. A numerical example is given to illustrate the advantage of the proposed bound in Theorem 3.6.

    Example 3.1. Consider the matrix in Example 2.1:

    A=[3130130801300008].

    By computation, we know that A is a PDSDD matrix for S={1,3} but neither SDD nor a Nekrasov matrix. Moreover, it is easy to verify that there is no nonempty proper subset S of N such that A is an S-SDD matrix, and so it is not a DSDD matrix. Therefore, neither of the existing bounds for SDD, DSDD, S-SDD, and Nekrasov matrices can be used to estimate ||A1||. However, by our bound (3.1), we have

    ||A1||2.

    The exact value of the infinity norm of the inverse of A is ||A1||=1.

    For a given ε>0, denoted by

    Λε(A)={λC:xCn{0},ECn×n,||E||εsuchthat(A+E)x=λx},

    the ε-pseudospectrum of a matrix A consists of all eigenvalues of matrices [30], which is equivalent to

    Λε(A)={zC:||(AzI)1||1ε}, (3.12)

    where the convention is ||A1||1=0 if A is singular [30]. This implies that the infinity norm bounds of the inverse of a given matrix could be used to generate new pseudospectra localizations. For details, see [13,25,30]. So, in this section, we shall give a new pseudospectra localization using the obtained bound in Section 3.2. Before that, a useful lemma is given that will be used later.

    Lemma 3.2. Let A be an arbitrary matrix and S be any subset of N. Then,

    ||A1||1μ(A):=min{f(A),g(A)},

    where

    f(A):=maxiSmin{|aii|r¯Si(A),minjS{i}{μSij(A),|ajj|rj(A)}}

    and

    g(A):=maxi¯Smin{|aii|rSi(A),minj¯S{i}{μ¯Sij(A),|ajj|rj(A)}}

    with the convention ||A1||1 if A is singular, and μSij(A)=0 if |ajj|rSj(A)+|aji|+rSi(A)=0; otherwise,

    μSij(A)=(|aii|r¯Si(A))(|ajj|rSj(A)+|aji|)rSi(A)(r¯Sj(A)+|aji|)|ajj|rSj(A)+|aji|+rSi(A).

    Proof. For any given subset S of N, if A is a PDSDD matrix, then it follows from Lemma 3.1 and Theorem 3.5 that

    ||A1||1min{maxiSmin{|aii|r¯Si(A),minjS{i}{μSij(A),|ajj|rj(A)}},maxi¯Smin{|aii|rSi(A),minj¯S{i}{μ¯Sij(A),|ajj|rj(A)}}}=μ(A).

    If A is not a PDSDD matrix, then it follows from Lemma 3.1 that at least one of the following conditions holds: (i) |aii|r¯Si(A) for all iS; (ii) |aii|>r¯Si(A) for some iS; but for some jS{i}, |ajj|rj(A) or

    (|aii|r¯Si(A))(|ajj|rSj(A)+|aji|)rSi(A)(r¯Sj(A)+|aji|);

    (iii) |aii|rSi(A) for all i¯S; (iv) |aii|>rSi(A) for some i¯S; but for some j¯S{i}, |ajj|rj(A) or

    (|aii|rSi(A))(|ajj|r¯Sj(A)+|aji|)r¯Si(A)(rSj(A)+|aji|).

    This implies that μ(A)0||A1||1. The proof is complete.

    Now, a new pseudospectra localization for matrices is given based on Lemma 3.2.

    Theorem 3.8. (ε-pseudo PDSDD set) Let A=[aij]Cn×n and S be any subset of N. Then,

    Λε(A)ΘS(A,ε):=θS(A,ε)θ¯S(A,ε),

    where

    θS(A,ε):=iS(Γ¯Si(A,ε)(jS{i}(ˆV¯Sij(A,ε)Γj(A,ε))))

    and

    θ¯S(A,ε):=i¯S(ΓSi(A,ε)(j¯S{i}(ˆVSij(A,ε)Γj(A,ε))))

    with

    ΓSi(A,ε):={zC:|zaii|rSi(A)+ε},
    Γj(A,ε):={zC:|zajj|rj(A)+ε},

    and

    ˆVSij(A,ε):={zC:(|zaii|rSi(A)ε)(|zajj|r¯Sj(A)+|aji|)r¯Si(A)(rSj(A)+|aji|+ε)}.

    Proof. From Lemma 3.2 and (3.12), we immediately get

    Λε(A)={zC:||(AzI)1||1ε}{zC:μ(AzI)ε}, (3.13)

    where μ(AzI) is defined as in Lemma 3.2. Note that rSi(AzI)=rSi(A) and r¯Si(AzI)=r¯Si(A). Therefore, for any λΛε(A), it follows from (3.13) that

    f(AλI)εorg(AλI)ε,

    where f(AλI) and g(AλI) are given by Lemma 3.2.

    Case Ⅰ. If f(AλI)ε, then for all iS, |aiiλ|r¯Si(A)+ε or |aiiλ|>r¯Si(A)+ε for some iS; but for some jS{i}, |ajjλ|rj(A)+ε or μSij(AλI)ε, i.e.,

    (|aiiλ|r¯Si(A))(|ajjλ|rSj(A)+|aji|)rSi(A)(r¯Sj(A)+|aji|)|ajjλ|rSj(A)+|aji|+rSi(A)ε. (3.14)

    If |ajjλ|rSj(A)>0, then it follows from (3.14) that

    (|aiiλ|r¯Si(A)ε)(|ajjλ|rSj(A)+|aji|)rSi(A)(r¯Sj(A)+|aji|+ε).

    If |ajjλ|rSj(A)0, then |ajjλ|rSj(A)+εrj(A)+ε. These imply that λθS(A,ε).

    Case Ⅱ. If g(AλI)ε, then for all i¯S, |aiiλ|rSi(A)+ε or |aiiλ|>rSi(A)+ε for some i¯S; but for some j¯S{i}, |ajjλ|rj(A)+ε or μ¯Sij(AλI)ε, i.e.,

    (|aiiλ|rSi(A))(|ajjλ|r¯Sj(A)+|aji|)r¯Si(A)(rSj(A)+|aji|)|ajjλ|r¯Sj(A)+|aji|+r¯Si(A)ε. (3.15)

    If |ajjλ|r¯Sj(A)>0, then it follows from (3.15) that

    (|aiiλ|rSi(A)ε)(|ajjλ|r¯Sj(A)+|aji|)r¯Si(A)(rSj(A)+|aji|+ε).

    If |ajjλ|r¯Sj(A)0, then |ajjλ|r¯Sj(A)+εrj(A)+ε. These imply that λθ¯S(A,ε).

    From Case Ⅰ and Case Ⅱ, the conclusion follows.

    As an application, using Theorem 3.8, we next give a lower bound for distance to instability. Denote by Red(A)Rn×n the real matrix associated with a given matrix A=[aij]Cn×n in the following way:

    (Red(A))ij={Re(aii),j=i,|aij|,ji.

    Theorem 3.9. Consider A=[aij]Cn×n, such that Red(A) is a PDSDD matrix with all diagonal elements negative. Then, μ(Red(A))>0 and

    Λε(A)ΘS(A,ε)Cforall0<ε<μ(Red(A)), (3.16)

    where C is the open left half plane of C, μ(Red(A)) is defined as in Lemma 3.2, and Λε(A) denotes the infinity norm ε-pseudospectrum of A.

    Proof. Since Red(A) is a PDSDD matrix, it follows from Lemma 3.2 that μ(Red(A))>0. To prove (3.16), for 0<ε<μ(Red(A)), it suffices to show that Re(z)<0 for each zΘS(A,ε). It follows from Theorem 3.8 that zθS(A,ε) or zθ¯S(A,ε). We only consider the case of zθS(A,ε), and the case of zθ¯S(A,ε) can be proved similarly. Since zθS(A,ε), it follows that for all iS, either (i) |aiiz|r¯Si(A)+ε or (ii) |aiiz|>r¯Si(A)+ε for some iS; but for some jS{i}, |ajjz|rj(A)+ε or

    (|aiiz|r¯Si(A)ε)(|ajjz|rSj(A)+|aji|)rSi(A)(r¯Sj(A)+|aji|+ε). (3.17)

    Note that

    μ(Red(A))=min{f(Red(A)),g(Red(A))},

    where

    f(Red(A)):=maxiSmin{|Re(aii)|r¯Si(Red(A)),minjS{i}{μSij(Red(A)),|Re(ajj)|rj(Red(A))}}

    and

    g(Red(A)):=maxi¯Smin{|Re(aii)|rSi(Red(A)),minj¯S{i}{μ¯Sij(Red(A)),|Re(ajj)|rj(Red(A))}}

    with μSij(Red(A)) defined as in Lemma 3.2.

    For case (i), i.e., |aiiz|r¯Si(A)+ε for all iS, we have

    Re(z)Re(aii)|Re(z)Re(aii)|=|Re(zaii)||zaii|r¯Si(A)+ε<r¯Si(A)+|Re(aii)|r¯Si(A)=Re(aii),

    which implies that Re(z)<0.

    For case (ii), i.e., |zaii|>r¯Si(A)+ε for some iS, if |ajjz|rj(A)+ε, then

    Re(z)Re(ajj)|Re(z)Re(ajj)|=|Re(zajj)||zajj|rj(A)+ε<rj(A)+|Re(ajj)|rj(A)=Re(ajj),

    which implies that Re(z)<0. If (3.17) holds, then

    Re(z)Re(ajj)|Re(z)Re(ajj)|=|Re(zajj)||zajj|r¯Si(A)(rSj(A)+|aji|+ε)|zaii|rSi(A)ε+rSj(A)|aji|. (3.18)

    {If |zaii|<|Re(aii)|, then Re(z)Re(aii)|zaii|<|Re(aii)|, which leads to Re(z)<0. Otherwise, since}

    0<ε<(|Re(aii)|r¯Si(A))(|Re(ajj)|rSj(A)+|aji|)rSi(A)(r¯Sj(A)+|aji|)|Re(ajj)|rSj(A)+|aji|+rSi(A)(|zaii|r¯Si(A))(|Re(ajj)|rSj(A)+|aji|)rSi(A)(r¯Sj(A)+|aji|)|Re(ajj)|rSj(A)+|aji|+rSi(A),

    it follows that

    r¯Si(A)(rSj(A)+|aji|+ε)|zaii|rSi(A)ε+rSj(A)|aji|<|Re(ajj)|,

    which together with (3.18) yields that

    Re(z)Re(ajj)<|Re(ajj)|=Re(ajj),

    and thus Re(z)<0. This completes the proof.

    The following example shows that the bound μ(Red(A)) in Theorem 3.9 is better than those of [13] and [30] in some cases.

    Example 3.2. Consider the matrix AR10×10 in [13], where

    A=[7871051083517495933535524458681344697887256883024290172671093638082699654878671107917734931131084435644554221099210347].

    It follows from [13] that A is a DZ-type matrix, and ε=μ(Red(A))=0.66. On the other hand, it is easy to verify that A is also a PDSDD matrix for S={1,2,3,4,9}. Hence, from Theorem 3.9, we can get a new lower bound for distance to instability ε=μ(Red(A))=4.17 and plot the corresponding pseudospectrum as shown in Figure 1, where Γε(A), D(A,ε), ΘS(A,ε), the pseudospectrum Λε(A) and the eigenvalues of A are represented by a blue solid boundary, a green dotted boundary, a red solid boundary, a gray area, and a black "×, " respectively.

    Figure 1.  Localization sets for ε-pseudospectrum for ε=μ(Red(A))=4.17.

    As can be seen from Figure 1, the sets Γε(A) of [30] and D(A,ε) of [13] propagate far into the right half-plane of C, but the localization set ΘS(A,ε) touches the y-axis. This implies that we cannot use Γε(A) and D(A,ε) to determine the stability of A. However, using the localization set ΘS(A,ε), we can determine that A is a stable matrix.

    This paper proposes a new class of nonsingular H-matrices called PDSDD matrices, which is similar to but different from S-SDD matrices. By its non-singularity, a new eigenvalue localization set for matrices is presented, which improves some existing results in [8] and [27]. Furthermore, an infinity norm bound for the inverse of PDSDD matrices is obtained, which improves the well-known Varah's bound for strictly diagonally dominant matrices. Meanwhile, utilizing the proposed infinity norm bound, a new pseudospectra localization for matrices is given, and a lower bound for distance to instability is provided as well. In addition, applying the proposed infinity norm bound to explore the error bounds for linear complementarity problems of PDSDD matrices is also an interesting problem. It is worth studying in the future.

    The authors would like to thank the editor and the anonymous referees for their valuable suggestions and comments. This work was partly supported by the National Natural Science Foundations of China (61962059 and 31600299), the Young Science and Technology Nova Program of Shaanxi Province (2022KJXX-01), the Science and Technology Project of Yan'an (2022SLGYGG-007), the Scientific Research Program Funded by Yunnan Provincial Education Department (2022J0949).

    The authors declare there are no conflicts of interest.



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