Research article

The Hermitian solution to a matrix inequality under linear constraint

  • Received: 29 April 2024 Revised: 31 May 2024 Accepted: 12 June 2024 Published: 20 June 2024
  • MSC : 15A24, 15A57

  • In this paper, the necessary and sufficient conditions under which the matrix inequality CXCD (>D) subject to the linear constraint AXA=B is solvable are deduced by means of the spectral decompositions of some matrices and the generalized singular value decomposition of a matrix pair. An explicit expression of the general Hermitian solution is also provided. One numerical example demonstrates the effectiveness of the proposed method.

    Citation: Yinlan Chen, Wenting Duan. The Hermitian solution to a matrix inequality under linear constraint[J]. AIMS Mathematics, 2024, 9(8): 20163-20172. doi: 10.3934/math.2024982

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  • In this paper, the necessary and sufficient conditions under which the matrix inequality CXCD (>D) subject to the linear constraint AXA=B is solvable are deduced by means of the spectral decompositions of some matrices and the generalized singular value decomposition of a matrix pair. An explicit expression of the general Hermitian solution is also provided. One numerical example demonstrates the effectiveness of the proposed method.



    Throughout this paper, we denote the complex m×n matrix space by Cm×n, the set of all Hermitian matrices in Cm×m by Cm×mH, the conjugate transpose, the range space, and the Moore-Penrose generalized inverse of a matrix A by A, R(A) and A, respectively. In is the n×n identity matrix and A0 (>0) means that ACn×n is Hermitian nonnegative definite (positive definite). PL represents the orthogonal projector on the subspace L. Given a matrix ACm×n, EA=ImAA and FA=InAA are two orthogonal projectors. Besides, F stands for the Frobenius norm.

    A lot of work with the Hermitian solutions of the matrix equations have been published [1,2,3,4,5,6,7]. However, the problem of solving the Hermitian solution of the matrix inequality under the symmetric matrix equation constraint is considered by only a few authors. To the best of our knowledge, the constrained matrix inequality:

    CXCD (>D), s.t. AXA=B, (1.1)

    where ACm×n, BCn×n, CCm×p and DCp×p, and XCm×mH is an unknown matrix to be determined, was first investigated by Liu [8]. Observe that Liu derived the necessary and sufficient conditions for the solvability of (1.1) using the maximal and minimal ranks and inertias of the matrix polynomials. In this paper, we provide an alternative approach to find the Hermitian solution of (1.1). Compared with the approach proposed by Liu [8], the method used in this paper is from a new perspective, using the decompositions of matrices to reduce the calculations of the rank and inertia, which makes it easier to obtain the representation of the Hermitian solution of (1.1).

    In what follows, we discuss the necessary and sufficient conditions for the solvability of (1.1) using the spectral decompositions (SDs) and the generalized singular value decomposition (GSVD) of some matrices, and give an explicit representation of the general Hermitian solution of (1.1) when the consistent conditions are satisfied. Further, one numerical example shows that the introduced method is correct.

    In order to solve the Hermitian solution of (1.1), we need the following lemmas.

    Lemma 1. ([9]) If ACm×n and BCn×nH, then the matrix equation AXA=B has a solution XCm×mH if and only if

    R(B)R(A). (2.1)

    In which case, the general Hermitian solution can be expressed as

    X=(A)BA+EAZ+ZEA, (2.2)

    where ZCm×m is an arbitrary matrix.

    Lemma 2. ([10,11]) Assume that A1Cp×m, A2Cn×p and A3Cp×pH. Then the matrix equation A1XA2+(A1XA2)=A3 has a solution if and only if

    EA1A3EA1=0,  FA2A3FA2=0,  [A1, A2][A1, A2]A3=A3.

    In this case, the general solution with respect to XCm×n gives

    X=A1(Γ+F˜LSXF˜LA1A1)A2+YA1A1YA2A2,

    where ˜L=FA2A1A1, Γ=12A3(2IpA1A1)+12(ΨΨ)A1A1, and Ψ=2˜LFA2A3+(Ip˜LFA2)A3˜L˜L, YCm×n and SXCp×p are arbitrary matrices with SX=SX.

    Lemma 3. ([12,13]) Given matrices ˜ACp×m and ˜DCp×m. Let the singular value decomposition (SVD) of the matrix ˜A be ˜A=˜P[Σ000]˜Q, where Σ=diag(α1, , αr)>0, r=rank(˜A) and ˜P=[˜P1, ˜P2]Cp×p, ˜Q=[˜Q1, ˜Q2]Cm×m are unitary matrices with ˜P1Cp×r, ˜Q1Cm×r and ˜Q2Cm×(mr). Then:

    (ⅰ) The matrix equation ˜AY=˜D has a Hermitian nonnegative definite solution YCm×mH if and only if ˜D˜A0, R(˜D)=R(˜D˜A), and the general nonnegative definite solution can be expressed as

    Y=Y0+F˜AKF˜A,

    where Y0=˜A˜D+F˜A(˜A˜D)+F˜A˜D(˜D˜A)˜DF˜A, and KCm×mH is an arbitrary nonnegative definite matrix.

    (ⅱ) The matrix equation ˜AY=˜D has a Hermitian positive definite solution if and only if ˜A˜A˜D=˜D, ˜P1˜D˜A˜P1>0, and the general positive definite solution is

    Y=Y0+F˜AKF˜A,

    where Y0=˜A˜D+F˜A(˜A˜D)+F˜A˜D(˜D˜A)˜DF˜A, and KCm×mH is an arbitrary positive definite matrix.

    According to Lemma 1, we know that the matrix equation AXA=B has a Hermitian solution if and only if the condition (2.1) holds, then the general solution is given by (2.2), where ZCm×m is an arbitrary matrix. Substituting (2.2) into the first matrix inequality of (1.1) yields

    CEAZC+CZEACDC(A)BAC (>DC(A)BAC). (3.1)

    Clearly, the inequality (3.1) can be equivalently written as

    GZC+CZG=K˜D, (3.2)

    where ˜D=D+C(A)BAC, G=CEA and K0 (>0) is an unknown matrix to be determined. By utilizing Lemma 2, we see that Eq (3.2) with respect to Z is solvable if and only if the following three matrix equations hold simultaneously:

    EGKEG=EG˜DEG, (3.3)
    FCKFC=FC˜DFC, (3.4)
    [G, C][G, C](K˜D)=K˜D. (3.5)

    Now, we will seek the solvability conditions with respect to K0 (>0) such that (3.3)–(3.5) are consistent. If let PL=[G, C][G, C], Eq (3.5) can be equivalently written as

    (IpPL)K=(IpPL)˜D. (3.6)

    From Lemma 3, Eq (3.6) has a Hermitian nonnegative definite solution KCp×p if and only if

    (IpPL)˜D(IpPL)0,  R((IpPL)˜D)=R((IpPL)˜D(IpPL)), (3.7)

    in this case, the general Hermitian nonnegative definite solution can be expressed as

    K=K0+PLSPL, (3.8)

    where

    K0=˜DPL˜DPL+PL˜D(IpPL)[(IpPL)˜D(IpPL)](IpPL)˜DPL, (3.9)

    and SCp×pH is an arbitrary nonnegative matrix.

    Assume that the SD of IpPL is

    IpPL=Q[Is000]Q=Q1Q1, (3.10)

    where s=rank(IpPL) and Q=[Q1, Q2] is a unitary matrix with Q1Cp×s and Q2Cp×(ps). By Lemma 3, Eq (3.6) has a Hermitian positive definite solution if and only if

    Q1˜DQ1>0, (3.11)

    then the general Hermitian positive definite solution can be formulated as

    K=K0+PLSPL, (3.12)

    where K0 is given by (3.9), and S is an arbitrary Hermitian positive definite matrix. Due to L=R(G)+R(C), then

    PLGG=GG=GGPL, PLCC=CC=CCPL.

    Substituting (3.8) ((3.12)) into (3.3) and (3.4), we can obtain that

    (PLGG)S(PLGG)=(IpGG)W(IpGG), (3.13)
    (PLCC)S(PLCC)=(IpCC)W(IpCC), (3.14)

    where W=˜DK0. According to (3.9), it follows that

    (PLGG)W(PLGG)=(IpGG)W(IpGG), (3.15)
    (PLCC)W(PLCC)=(IpCC)W(IpCC). (3.16)

    By Eqs (3.15) and (3.16), Eqs (3.13) and (3.14) are equivalent to

    (PLGG)S(PLGG)=(PLGG)W(PLGG), (3.17)
    (PLCC)S(PLCC)=(PLCC)W(PLCC). (3.18)

    It is easily verified that PLGG and PLCC are orthogonal projection operators, then there exists unitary matrices U and V such that

    PLGG=U[Ia000]U=U1U1,  PLCC=V[Ib000]V=V1V1, (3.19)

    where a=rank(PLGG), b=rank(PLCC), U1Cp×a and V1Cp×b are full column rank unitary matrices. Substituting (3.19) into (3.17) and (3.18), we can get that

    U1SU1=U1WU1,  V1SV1=V1WV1. (3.20)

    Let the GSVD [14] of the matrix pair [U1, V1] be:

    U1=MΔ1N1,  V1=MΔ2N2, (3.21)

    where MCp×p is a nonsingular matrix, and N1Ca×a, N2Cb×b are unitary matrices, and

    Δ1=[I00Υ0000]aeefapf,     aeeΔ2=[00Θ00I00]aeefapf,           ebe

    f=rank([U1, V1])=a+be, Υ=diag(δ1, δ2, , δe) and Θ=diag(ϑ1, ϑ2, , ϑe) with 1>δ1δ2δe>0, 0<ϑ1ϑ2ϑe<1, δ2i+ϑ2i=1, i=1, 2, , e. Substituting (3.21) into (3.20) and partitioning the matrix MWM as:

    MWM=[M11 M12 M13 M14M12 M22 M23 M24M13 M23 M33 M34M14 M24 M34 M44]aeefapf.            ae e fapf (3.22)

    Then, it follows from Lemma 2.6 of [15] that:

    (i) Equation (3.20) has a solution S0 if and only if

    [M11 M12M12 M22]0,[M22 M23M23 M33]0, (3.23)

    and the general Hermitian nonnegative definite solution of Eq (3.20) is

    S=(M)1[Ω(S13)Ω(S13)J1J1Ω(S13)J2+J1Ω(S13)J1]M1, (3.24)

    where

    Ω(S13)[M11 M12 S13M12 M22 M23S13 M23 M33], (3.25)

    with

    S13=M12M22M23+(M11M12M22M12)12J3(M33M23M22M23)12, (3.26)

    and J1Cf×(pf), J2C(pf)×(pf) are arbitrary matrices with J20, and J3C(ae)×(fa) is an arbitrary contraction matrix (that is, the maximum singular value with respect to J3 cannot exceed 1).

    (ii) Equation (3.20) has a Hermitian positive solution of S if and only if

    [M11 M12M12 M22]>0,[M22 M23M23 M33]>0, (3.27)

    and the representation of the general solution for Eq (3.20) can be expressed as

    S=(M)1[Ω(S13)J4J4J5+J4[Ω(S13)]1J4]M1, (3.28)

    where Ω(S13) is given by (3.25) with

    S13=M12M122M23+(M11M12M122M12)12J6(M33M23M122M23)12, (3.29)

    and J4Cf×(pf), J5C(pf)×(pf) are arbitrary matrices with J5>0, and J6C(ae)×(fa) is an arbitrary strict contraction matrix (that is, the maximum singular value with respect to J6 is less than 1).

    Furthermore, when the conditions (3.3)–(3.5) hold simultaneously, the general expression with respect to Z in Eq (3.2) is

    Z=G(Γ+F˜LNXF˜LGG)C+YGGYCC, (3.30)

    where

    Γ=12(PLSPLW)(2IpGG)+12(ΨΨ)GG, (3.31)

    with

    Ψ=2˜LFC(PLSPLW)+(Ip˜LFC)(PLSPLW)˜L˜L, (3.32)

    and S is given by Eq (3.24) ((3.28)), ˜L=FCGG, and YCm×m, NXCp×p are arbitrary matrices with NX=NX. By substituting (3.30) into (2.2), we can get the Hermitian solution of (1.1).

    With the above discussion, we can obtain the following theorem.

    Theorem 1. Given matrices ACm×n, BCn×n, CCm×p and DCp×p. Let ˜D=D+C(A)BAC, G=CEA, L=R(G)+R(C), and let the SDs of the matrices IpPL, PLGG and PLCC be respectively given by (3.10) and (3.19). Suppose that the GSVD of the matrix pair [U1, V1] is given by (3.21), and the partition of the matrix MWM is given by (3.22). Then,

    (i) The matrix inequality CXCD s.t. AXA=B has a Hermitian solution if and only if the conditions (2.1), (3.7) and (3.23) hold, in which case, the general Hermitian solution XCm×mH can be expressed as

    X=(A)BA+EAG(Γ+F˜LNXF˜LGG)C+EAYEAGGYCC+(C)(ΓGGF˜LNXF˜L)(G)EA+YEACCYGGEA, (3.33)

    where W=˜DK0, ˜L=FCGG, and K0, S, Ω(S13), S13, Γ and Ψ are respectively given by (3.9), (3.24)–(3.26), (3.31) and (3.32), and NXCp×p, YCm×m, J1Cf×(pf) and J2C(pf)×(pf) are arbitrary matrices with NX=NX and J20, and J3C(ae)×(fa) is an arbitrary contraction matrix.

    (ii) The matrix inequality CXC>D s.t. AXA=B has a Hermitian solution XCm×mH if and only if the conditions (2.1), (3.11) and (3.27) are satisfied, in this case, the Hermitian solution can be expressed as

    X=(A)BA+EAG(Γ+F˜LNXF˜LGG)C+EAYEAGGYCC+(C)(ΓGGF˜LNXF˜L)(G)EA+YEACCYGGEA, (3.34)

    where W=˜DK0, ˜L=FCGG, and K0, S, Ω(S13), S13, Γ and Ψ are respectively given by (3.9), (3.28), (3.25), (3.29), (3.31) and (3.32), and NXCp×p, YCm×m, J4Cf×(pf) and J5C(pf)×(pf) are arbitrary matrices with NX=NX and J5>0, and J6C(ae)×(fa) is an arbitrary strict contraction matrix.}$

    According to Theorem 1, we can describe the numerical algorithm to solve the Hermitian solution of (1.1) as follows.

    Algorithm 1.

    (1) Input matrices A, B, C and D.

    (2) If the condition (2.1) holds, then continue; or else, (1.1) has no solution XCm×mH.

    (3) Compute matrices ˜D, G and IpPL.

    (4) If the condition (3.7) holds, then continue; or else, the matrix inequality CXCD s.t. AXA=B has no solution X.

    (5) Compute the SD of the matrix IpPL by (3.10).

    (6) If the condition (3.11) holds, then continue; or else, the matrix inequality CXC>D s.t. AXA=B has no solution X.

    (7) Compute the matrices K0 and W in the light of (3.9), (3.13) and (3.14), respectively.

    (8) Compute the SDs of the matrices PLGG and PLCC by (3.19).

    (9) Compute the GSVD of the matrix pair [U1, V1] by (3.21).

    (10) Compute the matrix MWM by (3.22).

    (11) (ⅰ) If the condition (3.23) holds, then continue; or else, the matrix inequality CXCD s.t. AXA=B has no solution X.

    (ⅱ) If the condition (3.27) holds, then continue; or else, the matrix inequality CXC>D s.t. AXA=B has no solution X.

    (12) (ⅰ) Select matrices J1, J20 and a contraction matrix J3, compute matrices S, Ω(S13) and S13 based on (3.24)–(3.26), respectively.

    (ⅱ) Select matrices J4, J5>0 and a strict contraction matrix J6, compute matrices S, Ω(S13) and S13 by (3.28), (3.25) and (3.29), respectively.

    (13) Calculate matrices Z, \  Γ and Ψ on the basis of (3.30)–(3.32), respectively.

    (14) (ⅰ) Select matrices NX and Y, compute the Hermitian solution of CXCD s.t. AXA=B in the light of (3.33).

    (ⅱ) Select matrices NX and Y, compute the Hermitian solution of CXC>D s.t. AXA=B based on (3.34).

    Remark 1. Through careful statistics, the amount of computations required by Algorithm 1 is about 146p3+84m3+46m2p+22mp2+2mnp+n2p+9n3+9mn2+5m2n flops, where the generalized inverse matrices C, G and ˜L are calculated by the SVDs of the matrices C, G and ˜L. Further, to compute the time complexity of Algorithm 1, the readers can see a survey [16].

    Example 1. Let m=6, n=5 and p=7. The matrices A, B, C and D are presented by

    A=[0.69370.44210.25100.56620.89730.39210.55090.26580.41140.49820.80971.01340.72900.69780.80020.38210.75600.29890.80280.71990.98981.25021.05751.26971.11790.97041.11410.56951.11981.3391],B=[5.01196.07433.95095.86276.27976.07437.35514.78277.10497.61403.95094.78273.10964.62124.95315.86277.10494.62126.85797.34606.27977.61404.95317.34607.8667],C=[0.79910.65640.44840.55500.44100.22780.47401.05140.78191.64300.59191.76051.16201.23370.85630.78620.88610.55200.77990.45980.89680.60530.48500.84880.32910.75180.58470.73470.71850.72180.92060.44740.75710.45320.95631.15490.87731.35600.63281.12600.98941.1950],D=[5.26367.98192.63352.25061.240110.02300.19727.981911.16375.68973.84713.801312.99622.35912.63355.68970.21580.87590.98467.53191.96552.25063.84710.87591.01090.17075.12240.36191.24013.80130.98460.17071.65955.55332.667310.023012.99627.53195.12245.553315.51514.07970.19722.35911.96550.36192.66734.07973.0450].                                                   

    It is easy to validate that the stated conditions (2.1), (3.7) and (3.23) are satisfied. In fact, FABF=1.6310×1015, the eigenvalues of the matrix (IpPL)˜D(IpPL) are 0.0000, 0.0000, 0.0000, 0.0000, 0.1016, 0.2585, 4.3461, E(IpPL)˜D(IpPL)˜D(IpPL)F=1.3311×1015, and E(IpPL)˜D(IpPL)(IpPL)˜DF=1.8544×1015, the eigenvalues of the matrix [M11 M12M12 M22]=[0.40790.28130.28130.1940] are 0.6018, 2.1184×105, and the matrix [M22 M23M23 M33] is 0. According to Algorithm 1 and choosing the matrices J1=0, J2=I5, NX=0 and Y=I6, we can obtain that

    X=[3.70606.020315.48709.26708.145012.59266.020312.77484.597949.286910.989916.323815.48704.597916.35030.53031.407721.24189.267049.28690.53037.48632.677623.51018.145010.98991.40772.67761.720512.619012.592616.323821.241823.510112.619032.0736].                                                   

    The absolute error is estimated by

    AXABF=2.6065×1014,

    and the eigenvalues of (CXCD) are 0.0000, 0.1172, 0.1505, 0.3321, 0.5119, 4.4760, 72.3055, which implies that X is the Hermitian solution of the matrix equality CXCD s.t. AXA=B.

    In this paper, we have established the necessary and sufficient conditions (see (2.1), (3.7), (3.23), and (2.1), (3.11), and (3.27)) for the Hermitian solution of (1.1), and achieve the explicit representation of the general Hermitian solution by the SD and the GSVD when the stated conditions are satisfied. One numerical example verifies the correctness of the introduced method.

    Yinlan Chen: Conceptualization, Methodology, Project administration, Supervision, Writing-review & editing; Wenting Duan: Investigation, Software, Validation, Writing-original draft, Writing-review & editing. All authors have read and approved the final version of the manuscript for publication.

    The authors declare that they have not used Artificial Intelligence (AI) tools in this article.

    The authors would like to express their gratitude to the anonymous reviewers for their valuable suggestions and comments that improved the presentation of this manuscript.

    The authors declare no conflicts of interest in this article.



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