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Spectrum perturbations of compact operators in a Banach space

  • Michael Gil’ EMAIL logo
Published/Copyright: September 14, 2019

Abstract

For an integer p ≥ 1, let Γp be an approximative quasi-normed ideal of compact operators in a Banach space with a quasi-norm NΓp(.) and the property

k=1|λk(A)|papNΓpp(A)(AΓp),

where λk(A) (k = 1, 2, …) are the eigenvalues of A and ap is a constant independent of A. Let A, ÃΓp and

Δp(A,A~):=NΓp(AA~)expapbpp1+12(NΓp(A+A~)+NΓp(AA~))p,

where bp is the quasi-triangle constant in Γp. It is proved the following result: let I be the unit operator, IAp be boundedly invertible and

Δp(A,A~)expapNΓpp(A)ψp(A)<1,

where ψp(A) = infk=1,2,… |1 – λkp (A)|. Then IÃp is also boundedly invertible. Applications of that result to the spectrum perturbations of absolutely p-summing and absolutely (p, 2) summing operators are also discussed. As examples we consider the Hille-Tamarkin integral operators and matrices.

MSC 2010: 47A10; 47A55; 47B10; 47A75

1 Introduction and statement of the main result

Roughly speaking, the spectrum perturbation theory for linear operators consists of two approaches. In the framework of the first one some structure on the error is imposed; for example, they may be analytic functions of a complex variable. The problem is then to determine how this structure affects the perturbed spectrum: e.g., when are they analytic functions of the variable, what kind of paths do they follow in the complex plane? That approach is well developed. For various results of this kind see for instance the book by Kato [1]. In the framework of the second approach the errors are unstructured and perturbations are bounded in terms of some norm of the errors. That approach in the case of operators in a Banach space to the best of our knowledge is at an early stage of development. Below we suggest perturbation results for compact operators in a Banach space, which are connected with the second approach.

Throughout this paper 𝓧 is a Banach space with the approximation property [2], the unit operator I and norm ∥.∥𝓧 = ∥.∥, (𝓑(𝓧)) is the algebra of all bounded linear operators in 𝓧. For a compact operator A, λk(A) (k = 1, 2, …) are the eigenvalues counted with their algebraic multiplicities. A point λ ∈ ℂ is said to be Φ-regular for A if IλA is boundedly invertible; σΦ(A) denotes the Fredholm spectrum (the complement of all Φ-regular points in the closed complex plane).

For an integer p ≥ 1 introduce the two-sided quasi-normed ideal Γp of compact operators in (𝓑(𝓧)) with a quasi-norm NΓp(.) and the property

k=1|λk(A)|papNΓpp(A)(AΓp), (1.1)

where ap is a constant independent of A, and Γp is approximative (i.e. the set of all finite rank operators is dense in Γp). Below bp denotes the quasi-triangle constant in Γp:

NΓp(A+A~)bp(NΓp(A)+NΓp(A~))(A,A~Γp). (1.2)

For the theory of the approximative normed and quasi-normed ideals see [2, 3] and references given therein. In the sequel constant ap in (1.1) will be called the eigenvalue constant.

Put

Δp(A,A~):=NΓp(AA~)expapbpp1+12(NΓp(A+A~)+NΓp(AA~))p

and

ψp(A)=infk=1,2,...|1λkp(A)|.

Now we are in a position to formulate the main result of the paper.

Theorem 1.1

For an integer p ≥ 1, let A, ÃΓp and IAp be boundedly invertible. If, in addition,

Δp(A,A~)expapNΓpp(A)ψp(A)<1,

then IÃp is also boundedly invertible.

The proof of this theorem is presented in the next section. Replacing in Theorem 1.1 A and à by λA and λÃ, respectively, we get the following result.

Corollary 1.2

Let A, ÃΓp and λpσΦ(Ap). If, in addition,

Δp(λA,λA~)expapNΓpp(λA)ψp(λA)<1,

then λp is Φ-regular also for Ãp.

From this corollary it follows

Corollary 1.3

Let A, ÃΓp and μpσΦ(Ãp). Then either μpσΦ(Ap), or

Δp(μA,μA~)expapNΓpp(μA)ψp(μA)1. (1.3)

Note that (1.3) can be rewritten as

|μ|NΓp(AA~)expap|μ|pNΓpp(A)ψp(μA)+apbpp1+|μ|2(NΓp(A+A~)+NΓp(AA~))p1. (1.4)

2 Proof of Theorem 1.1

For an AΓ1 introduce the determinant by

det(IA)=k=1(1λk(A)).

Obviously,

|det(IA)|k=1(1+|λk(A)|)expk=0|λk(A)|.

So from (1.1) we have

|det(IA)|expa1NΓ1(A).

Hence, the convergence of the product follows. Since Γ1 is approximative, we get

limndet(IAn)=det(IA)

for a sequence {An} of n-dimensional operators (n < ∞) converging to A in NΓ1(.).

Various approaches to the determinants of operators in a Banach space can be found, in particular, in the well-known publications [2, 4, 5].

Similarly, if AΓp for p > 1, we can write

det(IAp)=k=1(1λkp(A))

and according to (1.1)

|det(IAp)|exp[apNΓpp(A)]. (2.1)

Lemma 2.1

Let A, ÃΓp. Then

|det(IAp)det(IA~p)|Δp(A,A~). (2.2)

Proof

Let A and à be n-dimensional (n < ∞). Consider the function

f(λ)=det(I[12(A+A~)+λ(AA~)]).

First assume that I 12 (A + Ã) is invertible. Then

f(λ)=detI12(A+A~))(Iλ(I12(A+A~))1(AA~))=det(I12(A+A~))det(IλC),

where C = (I 12 (A + Ã))–1 (AÃ). But

det(IλC)=k=1n(1λλk(C))

is a polynomial. So f(λ) is a polynomial. Similarly, we can prove that

det(I[12(Ap+A~p)+λ(ApA~p)])

is a polynomial, if I 12 (Ap + Ãp) is invertible. Making use of Lemma 1.4.1 [6] (see also [7]), according to (2.1) we get (2.2). If I 12 (Ap + Ãp) is not invertible, then (2.2) can be proved by a small perturbation of the considered operators and continuity of determinants. So for finite dimensional operators the lemma is proved. The approximativity of Γp implies the required result.□

Corollary 2.2

Let A, ÃΓp and

|det(IAp)|>Δp(A,A~).

Then

|det(IA~p)||det(IAp)|Δp(A,A~)>0.

Lemma 2.3

If the condition

k=1|λk(A)|< (2.3)

holds and 1 ∉ σΦ(A), then

|det(IA)|exp[1ψ1(A)k=1|λk(A)|].

Proof

By the usual procedure for the calculations of an extremum we find that maxx≥0 exx = 1/e. Hence

1|1z|e1|1z|1/e(zC)

and

|1z|e11|1z|=e(|1z|1)/|1z|e(1|z|1)/|1z|=e|z||1z|.

So if 1 ∉ σΦ(A), then

|1λk(A)|exp[|λk(A)||1λk(A)|]exp[|λk(A)|ψ1(A)].

Hence

|det(IA)|=k=1|1λk(A)|exp[1ψ1(A)k=1|λk(A)|],

as claimed.□

Now let AΓp. From the previous lemma, due to (1.1)

|det(IAp)|expapNΓpp(A)ψp(A)(1σΦ(Ap)). (2.4)

Corollary 2.2 implies

Corollary 2.4

Let A, ÃΓp for an integer p ≥ 1. If, 1 ∉ σΦ (Ap) and

expapNΓpp(A)ψp(A)>Δp(A,A~), (2.5)

then

|det(IA~p)|expappNΓpp(A)ψp(A)Δp(A,A~)>0.

The assertion of Theorem 1.1 directly follows from Corollary 2.4.□

3 Particular cases

3.1 Absolutely p-summing operators

An operator A ∈ (𝓑(𝓧)) is said to be absolutely p-summing (1 ≤ p < ∞), if there is a constant ν, such that regardless of a natural number m and regardless of the choice x1, …, xm ∈ 𝓧 we have

[k=1mAxkp]1/pνsup{[k=1m|x,xk|p]1/p:xX,x=1}.

Here 〈 ., .〉 means the functional on 𝓧, 𝓧* means the space adjoint to 𝓧[2, 3, 8, 9]. The least ν for which this inequality holds is a norm and is denoted by πp(A). The set of absolutely p-summing operators in 𝓧 with the finite norm πp is a normed ideal in the set of bounded linear operators, which is denoted by Πp, cf. [2].

As is well-known,

k=1|λk(A)|pπpp(A)(AΠp;2p<), (3.1)

cf. Theorem 17.4.3 from [9] (see also Theorem 3.7.2 from [2, p. 159]). Thus, Πp (p ≥ 2) has the properties of ideal Γp. Besides, NΓp(A) = πp(A), bp = 1 and ap = 1.

3.2 Ideal 𝓔p and absolutely (p, 2)-summing operators

Recall [2, p. 79] that sn(T) (n = 1.2, …) is called the n-th s-number (n-th singular number) of T ∈ (𝓑(𝓧)), if the following conditions are satisfied:

(S1)T=s1(T)s2(T)...0;(S2)sn+m1(S+T)sm(T)+sn(S)(S(B(X)));(S3)sn(A1TA2)A1sn(T)A2(A1,A2(B(X)));(S4) If rank(T)<n, then sn(T)=0;(S5)sn(Iln2)=1.

Here Iln2 is the unit operator in the n-dimensional Hilbert space ln2 with the traditional scalar product.

Let L(l2, 𝓧) denote the space of linear operators acting from the Hilbert space l2 with the traditional scalar product into 𝓧. The n-th Weyl number of T ∈ (𝓑(𝓧))) is defined by

xn(T):=sup{an(TZ):ZL(l2,X),Z=1},

where an(T) is the n-th approximation number defined by

an(T):=inf{TTn:Tn(B(X)),rankTn<n}.

xn(T) is an s-number with the sub-multiplicative property

(S6)xn+m1(TS)xn(T)xm(S)(S,T(B(X))),

cf. [2, Theorem 2.4.14] and [2, Proposition 2.4.17]. For an integer p ≥ 1, let 𝓔p. be the set of compact operators A acting in 𝓧 and satisfying

NEp(A):=(k=1xkp(A))1/p<.

Since xk(A) ≤ xk–1(A) and x2k–1(A + Ã) ≤ xk(A) + xk(Ã), we have

k=1xkp(A+A~)=j=1x2j1p(A+A~)+x2jp(A+A~)2j=1x2j1p(A+A~)2j=1(xj(A)+xj(A~))p.

By the Minkovsky inequality

(j=1(xj(A)+xj(A~))p)1/p(j=1xjp(A))1/p+(j=1xjp(A~))1/p.

Then

NEp(A+A~)21/p(NEp(A)+NEp(A~)). (3.2)

So 𝓔p is a quasinormed ideal with the quasi-triangular constant bp = 21/p. It is approximative, cf. [2, 3]. We need the following Weyl type inequality:

k=1|λk(A)|pcppk=1xkp(A)=cppNEpp(A) (3.3)

with

cp=21/p2e.

cf. [3, Theorem 2.a.6, p. 85].

So 𝓔p is an example of ideal Γp with NΓp(A) = N𝓔p(A), ap = cpp and bp = 21/p.

About the recent investigations of the singular numbers and Weyl type inequalities see [10]-[16].

Let us point an estimate for N𝓔p(A). To this end recall that an A ∈ (𝓑(𝓧)) is said to be absolutely (p, q)-summing (pq), if there is a constant ν such that regardless a natural number m and regardless of the choice x1, …, xm ∈ 𝓧 we have

[k=1mAxkp]1/pνsup{[k=1m|x,xk|q]1/q:xX,x=1}

cf. [2, 3, 8, 9]. The least ν for which this inequality holds is denoted by πp,q(A). The set of absolutely (p, q)-summing operators is denoted by Πp,q.

Due to [9, Theorem 16.3.1] πp,q is a norm and Πp,q with that norm is a Banach space. If AΠp,q, then ∥A∥ ≤ πp,q(A), since

Ax=[Axp]1/pπp,q(A)sup{[|x,x|q]1/q:xX,x=1}πp,q(A)x

for any x ∈ 𝓧. If, in addition R and S are bounded operators acting in 𝓧, then πp,q(SAR) ≤ ∥R𝓧S𝓧 πp,q(A).

We need Corollary 2.a.3 from [3, p. 81] (see also Corollary 17.2.2 from [9, p. 293]), which asserts the following: if AΠp0,2 (2 ≤ p0 < ∞), then

xn(A)πp0,2(A)n1/p0(n=1,2,...). (3.4)

Hence, for any p > p0 we have

NEp(A)=(k=1xnp(A))1/pπp0,2(A)(k=11kp/p0)1/p=ζ1/p(p/p0)πp0,2(A)(AΠp0,2), (3.5)

where

ζ(z)=k=11kz(z>1)

is the Riemann zeta-function.

4 Additional upper bounds for determinants

Lemma 4.1

For an integer p ≥ 1 and AΓp one has

|det(IAp)|ψp(A)exp[apNΓpp(A)].

Proof

Evidently,

|det(IAp)|=|1λmp(A)|k=1,km|1λkp(A)||1λmp(A)|exp[k=1|λk(A)|p]

for any m ≥ 1. Taking into account (1.1) and choosing m in such a way that |1 – λmp (A)| = ψp(A), we prove the lemma.□

Furthermore, let Ep(z) be the Weierstrass primary factor:

E1(z)=(1z);Ep(z)=(1z)exp[m=1p1zmm](p=2,3,...;zC).

Put

γp:=p1p(p1;p3) and γ1=γ3=1.

According to Theorem 1.5.3 [6],

|Ep(z)|exp[γp|z|p](zC). (4.1)

For an AΓp, p ≥ 2, introduce the p-regularized determinant by

detp(IA):=k=1Ep(λk(A)).

Due to (1.1) and (4.1)

|detp(IA)|exp[γpk=1|λk(A)|p]exp[a0γpNΓpp(A)](p2), (4.2)

and therefore the product converges.

Lemma 4.2

For an integer p ≥ 2 and any AΓp one has

|detp(IA)|ψ1(A)exp[k=1p1rsk(A)k]exp[apγpNΓpp(A)],

where rs(A) is the spectral radius of A.

Proof

By (4.1) and (1.1),

|detp(IA)|=|E(λm(A))|k=1,km|E(λk(A))||E(λm(A))|exp[γpk=1,km|λk(A)|p]|E(λm(A))|exp[apγpNΓpp(A)]

for any m ≥ 1. But

|Ep(λm(A))|=|1λm(A)||exp[k=1p1λm(A)kk]||1λm(A)|exp[k=1p1rsk(A)k].

So

|detp(IA)||1λm(A)|exp[k=1p1rsk(A)k]exp[apγpNΓpp(A)].

Hence, choosing m in such a way that |1 – λm(A)| = ψ1(A), we prove the lemma.□

5 Hille-Tamarkin integral operators “close” to Volterra ones

In this section and in the next one, we consider some concrete integral and matrix operators. We need the following result.

Corollary 5.1

Let WΓp be a quasi-nilpotent operator (i.e. its spectrum is {0}). Then for an arbitrary ÃΓp one has

|det(IA~p)1|Δp(W,A~).

Indeed, this result is due to Lemma 2.1 and the equality det(IWp) = 1.

Let Lp = Lp(0, 1) (2 ≤ p < ∞) be the space of scalar functions f defined on [0, 1] and endowed the norm

f=[01|f(t)|pdt]1/p.

Let K : LpLp be the operator defined by

(Kf)(t)=01k(t,s)f(s)ds(fLp,0t1),

whose kernel k defined on [0, 1]2 satisfies the condition

k^p(K):=[01(01|k(t,s)|pds)p/pdt]1/p<, (5.1)

where 1/p + 1/p′ = 1. Then K is called a (p, p′)-Hille-Tamarkin integral operator.

As is well known, [8, p. 43], any (p, p′)-Hille-Tamarkin operator K is an absolutely p-summing operator with πp(K) ≤ p(K). Let the operator V be defined by

(Vf)(t)=0tk(t,s)f(s)ds(fLp).

This operator is quasi-nilpotent. With Γp = Πp we have

Δp(K,V)=πp(KV)exp1+12(πp(K+V)+πp(KV))pΔ^p(K,V),

where

Δ^p(K,V):=k^p(KV)exp1+12(k^p(K+V)+k^p(KV))p.

Note that

((KV)f)(t)=x1k(t,s)f(s)ds.

Corollary 5.1 implies

Corollary 5.2

Let K be a (p, p′)-Hille-Tamarkin integral operator in Lp(0, 1) for an integer p ≥ 2 and 1/p + 1/p′ = 1. If Δ̂p(K, V) < 1, then

|det(IKp)1|Δ^p(K,V)

and therefore 1pσΦ(K), provided Δ̂p(K, V) < 1.

6 Hille-Tamarkin infinite matrices “close” to triangular ones

Let us consider the linear operator T in lp (2 ≤ p < ∞) generated by an infinite matrix (tjk)j,k=1, satisfying the condition

τp(T):=[j=1(k=1|tjk|p)p/p]1/p<, (6.1)

where 1/p + 1/p′ = 1.

Then T is called a (p, p′)-Hille-Tamarkin matrix. As is well known, any (p, p′)-Hille-Tamarkin matrix T is an absolutely p-summing operator with πp(T) ≤ τp(T), cf. [8, p. 43], [2, Sections 5.3.2 and 5.3.3, p. 230]). So according to (3.1),

k=1|λk(T)|pτpp(T)(2p<). (6.2)

Let T+=(τjk)j,k=1 be the upper-triangular part of T : τjk = tjk for 1 ≤ jk ≤ ∞ and τjk = 0 otherwise. Since p > p′, we obtain

(k=1|tjk|p)p/pk=1|tjk|p

and thus

j=1k=1|tjk|p<.

Since T+ is triangular, its eigenvalues are the diagonal entries and

det(IT+p)=d+,p:=k=1(1tkkp).

Under consideration,

Δp(T,T+)=πp(TT+)exp1+12(πp(T+T+)+πp(TT+))pΔ^p(T,T+),

where

Δ^p(T,T+):=τp(TT+)exp1+12(τp(T+T+)+τp(TT+))p.

Note that TT+ is the strictly lower part of T.

Making use of Lemma 2.1, we arrive at

Corollary 6.1

Let T be a (p, p′)-Hille-Tamarkin matrix for an integer p ≥ 2 and 1/p + 1/p′ = 1. Then |det(ITp) – d+,p| ≤ Δ̂p(T, T+), and therefore 1pσΦ(T), provided |d+,p| > Δ̂p(T, T+).

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Received: 2018-09-18
Accepted: 2019-08-12
Published Online: 2019-09-14

© 2019 Michael Gil’, published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 Public License.

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  60. Nonfragile observer-based guaranteed cost finite-time control of discrete-time positive impulsive switched systems
  61. Empirical likelihood confidence regions of the parameters in a partially single-index varying-coefficient model
  62. Algebraic loop structures on algebra comultiplications
  63. Two weight estimates for a class of (p, q) type sublinear operators and their commutators
  64. Dynamic of a nonautonomous two-species impulsive competitive system with infinite delays
  65. 2-closures of primitive permutation groups of holomorph type
  66. Monotonicity properties and inequalities related to generalized Grötzsch ring functions
  67. Variation inequalities related to Schrödinger operators on weighted Morrey spaces
  68. Research on cooperation strategy between government and green supply chain based on differential game
  69. Extinction of a two species competitive stage-structured system with the effect of toxic substance and harvesting
  70. *-Ricci soliton on (κ, μ)′-almost Kenmotsu manifolds
  71. Some improved bounds on two energy-like invariants of some derived graphs
  72. Pricing under dynamic risk measures
  73. Finite groups with star-free noncyclic graphs
  74. A degree approach to relationship among fuzzy convex structures, fuzzy closure systems and fuzzy Alexandrov topologies
  75. S-shaped connected component of radial positive solutions for a prescribed mean curvature problem in an annular domain
  76. On Diophantine equations involving Lucas sequences
  77. A new way to represent functions as series
  78. Stability and Hopf bifurcation periodic orbits in delay coupled Lotka-Volterra ring system
  79. Some remarks on a pair of seemingly unrelated regression models
  80. Lyapunov stable homoclinic classes for smooth vector fields
  81. Stabilizers in EQ-algebras
  82. The properties of solutions for several types of Painlevé equations concerning fixed-points, zeros and poles
  83. Spectrum perturbations of compact operators in a Banach space
  84. The non-commuting graph of a non-central hypergroup
  85. Lie symmetry analysis and conservation law for the equation arising from higher order Broer-Kaup equation
  86. Positive solutions of the discrete Dirichlet problem involving the mean curvature operator
  87. Dislocated quasi cone b-metric space over Banach algebra and contraction principles with application to functional equations
  88. On the Gevrey ultradifferentiability of weak solutions of an abstract evolution equation with a scalar type spectral operator on the open semi-axis
  89. Differential polynomials of L-functions with truncated shared values
  90. Exclusion sets in the S-type eigenvalue localization sets for tensors
  91. Continuous linear operators on Orlicz-Bochner spaces
  92. Non-trivial solutions for Schrödinger-Poisson systems involving critical nonlocal term and potential vanishing at infinity
  93. Characterizations of Benson proper efficiency of set-valued optimization in real linear spaces
  94. A quantitative obstruction to collapsing surfaces
  95. Dynamic behaviors of a Lotka-Volterra type predator-prey system with Allee effect on the predator species and density dependent birth rate on the prey species
  96. Coexistence for a kind of stochastic three-species competitive models
  97. Algebraic and qualitative remarks about the family yy′ = (αxm+k–1 + βxmk–1)y + γx2m–2k–1
  98. On the two-term exponential sums and character sums of polynomials
  99. F-biharmonic maps into general Riemannian manifolds
  100. Embeddings of harmonic mixed norm spaces on smoothly bounded domains in ℝn
  101. Asymptotic behavior for non-autonomous stochastic plate equation on unbounded domains
  102. Power graphs and exchange property for resolving sets
  103. On nearly Hurewicz spaces
  104. Least eigenvalue of the connected graphs whose complements are cacti
  105. Determinants of two kinds of matrices whose elements involve sine functions
  106. A characterization of translational hulls of a strongly right type B semigroup
  107. Common fixed point results for two families of multivalued A–dominated contractive mappings on closed ball with applications
  108. Lp estimates for maximal functions along surfaces of revolution on product spaces
  109. Path-induced closure operators on graphs for defining digital Jordan surfaces
  110. Irreducible modules with highest weight vectors over modular Witt and special Lie superalgebras
  111. Existence of periodic solutions with prescribed minimal period of a 2nth-order discrete system
  112. Injective hulls of many-sorted ordered algebras
  113. Random uniform exponential attractor for stochastic non-autonomous reaction-diffusion equation with multiplicative noise in ℝ3
  114. Global properties of virus dynamics with B-cell impairment
  115. The monotonicity of ratios involving arc tangent function with applications
  116. A family of Cantorvals
  117. An asymptotic property of branching-type overloaded polling networks
  118. Almost periodic solutions of a commensalism system with Michaelis-Menten type harvesting on time scales
  119. Explicit order 3/2 Runge-Kutta method for numerical solutions of stochastic differential equations by using Itô-Taylor expansion
  120. L-fuzzy ideals and L-fuzzy subalgebras of Novikov algebras
  121. L-topological-convex spaces generated by L-convex bases
  122. An optimal fourth-order family of modified Cauchy methods for finding solutions of nonlinear equations and their dynamical behavior
  123. New error bounds for linear complementarity problems of Σ-SDD matrices and SB-matrices
  124. Hankel determinant of order three for familiar subsets of analytic functions related with sine function
  125. On some automorphic properties of Galois traces of class invariants from generalized Weber functions of level 5
  126. Results on existence for generalized nD Navier-Stokes equations
  127. Regular Banach space net and abstract-valued Orlicz space of range-varying type
  128. Some properties of pre-quasi operator ideal of type generalized Cesáro sequence space defined by weighted means
  129. On a new convergence in topological spaces
  130. On a fixed point theorem with application to functional equations
  131. Coupled system of a fractional order differential equations with weighted initial conditions
  132. Rough quotient in topological rough sets
  133. Split Hausdorff internal topologies on posets
  134. A preconditioned AOR iterative scheme for systems of linear equations with L-matrics
  135. New handy and accurate approximation for the Gaussian integrals with applications to science and engineering
  136. Special Issue on Graph Theory (GWGT 2019)
  137. The general position problem and strong resolving graphs
  138. Connected domination game played on Cartesian products
  139. On minimum algebraic connectivity of graphs whose complements are bicyclic
  140. A novel method to construct NSSD molecular graphs
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