Abstract
It is a classical result that the Weyl function of a simple symmetric operator in a Hilbert space determines a boundary triple uniquely up to unitary equivalence. We generalize this result to a simple symmetric operator in a Pontryagin space, where unitary equivalence is replaced by the similarity realized via a standard unitary operator.
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References
Albeverio, S., Günther, U., Kuzhel, S.: J-self-adjoint operators with C-symmetries: an extension theory approach, J. Phys. A: Math. Theor. 42 (2009), no. 10, 105205
Azizov, T., Ćurgus, B., Dijksma, A.: Standard symmetric operators in Pontryagin spaces: a generalized von Neumann formula and minimality of boundary coefficients. J. Func. Anal. 198(2), 361–412 (2003)
Azizov, T., Iokhvidov, I.: Linear operators in spaces with an indefinite metric and their applications. Itogi nauki i mech. Ser. Mat. 17, 113–205 (1979)
Azizov, T., Iokhvidov, I.: Linear operators in spaces with an indefinite metric, Wiley (1989)
Behrndt, J.: Realization of nonstrict matrix Nevanlinna functions as Weyl functions of symmetric operators in Pontryagin spaces. Proc. Amer. Math. Soc. 137(8), 2685–2696 (2009)
Behrndt, J., Derkach, V.A., Hassi, S., de Snoo, H.: A realization theorem for generalized Nevanlinna families. Oper. Matrices 5(4), 679–706 (2011)
Behrndt, J., Hassi, S., de Snoo, H.: Boundary Value Problems, Weyl Functions, and Differential Operators., Birkhauser, (2020)
Bognár, J.: Indefinite inner product spaces. Springer-Verlag, Berlin Heidelberg New York (1974)
Calkin, J.: Abstract symmetric boundary conditions. Trans. Amer. Math. Soc. 45(3), 369–442 (1939)
Coddington, E.A.: Extension theory of formally normal and symmetric subspaces. Mem. Amer. Math. Soc. 134, 1–80 (1973)
Coddington, E.A.: Self-adjoint subspace extensions of nondensely defined symmetric operators. Bullet. Amer. Mac. Soc. 79(4), 712–715 (1973)
Coddington, E.A.: Self-adjoint subspace extensions of nondensely defined symmetric operators. Adv. Math. 14(3), 309–332 (1974)
Derkach, V.: On generalized resolvents of Hermitian relations in Krein spaces. J. Math. Sci. 97(5), 4420–4460 (1999)
Derkach, V.: Boundary Triplets, Weyl Functions, and the Kreĭn Formula, Operator Theory (2015), 183–218
Derkach, V., Hassi, S., Malamud, M.: Generalized boundary triples, II. Some applications of generalized boundary triples and form domain invariant Nevanlinna functions, Math. Nachr. 295 (2022), no. 6, 1113–1162
Derkach, V., Hassi, S., Malamud, M., de Snoo, H.: Boundary relations and their Weyl families. Trans. Amer. Math. Soc. 358(12), 5351–5400 (2006)
Derkach, V., Hassi, S., Malamud, M., de Snoo, H.: Boundary relations and generalized resolvents of symmetric operators. Russ. J. Math. Phys. 16(1), 17–60 (2009)
Derkach, V., Malamud, M.: Generalized resolvents and the boundary value problems for hermitian operators with gaps. J. Func. Anal. 95(1), 1–95 (1991)
Derkach, V., Malamud, M.: Weyl function of a Hermitian operator and its connection with characteristic function, arXiv:1503.08956 (2015)
Derkach, V.A., Malamud, M.M.: Extension theory of symmetric operators and boundary value problems, vol. 104. Institute of Mathematics of NAS of Ukraine, Kiev (2017). (in Russian)
Derkach, V., Hassi, S., Malamud, M.M.: Generalized boundary triples, I. Some classes of isometric and unitary boundary pairs and realization problems for subclasses of Nevanlinna functions. Math. Nachr. 293(7), 1278–1327 (2020)
Dijksma, A., Langer, H., de Snoo, H.: Eigenvalues and pole functions of Hamiltonian systems with eigenvalue depending boundary conditions. Math. Nachr. 161, 107–154 (1993)
Dijksma, A., Langer, H., Luger, A., Shondin, Yu.: Minimal realizations of scalar generalized Nevanlinna functions related to their basic factorization, spectral methods for operators of mathematical physics. Operator Theory: Advances and Applications (2004)
Gokhberg, I., Krein, M.: Fundamental aspects of defect numbers, root numbers and indexes of linear operators. Uspekhi Mat. Nauk 12(2), 43–118 (1957)
Gorbachuk, V., Gorbachuk, M.: Boundary Value Problems for Operator Differential Equations, vol. 48. Kluwer Academic Publishers, Dordrecht (1991)
Hassi, S., de Snoo, H., Woracek, H.: Some interpolation problems of Nevanlinna-Pick type. The Krein-Langer method, Operator Theory: Advances and Applications 106, 201–216 (1998)
Hassi, S., de Snoo, H.S.V., Szafraniec, F.H.: Componentwise and Cartesian decompositions of linear relations. Dissert. Math. 465, 1–59 (2009)
Hassi, S., de Snoo, H.S.V., Szafraniec, F.H.: Infinite-dimensional perturbations, maximally nondensely defined symmetric operators, and some matrix representations. Indag. Math. 23(4), 1087–1117 (2012)
Hassi, S., Kuzhel, S.: On J-self-adjoint operators with stable C-symmetries. Proc. Edinburgh Math. Soc. 143(1), 141–167 (2013)
Hassi, S., Malamud, M., Mogilevskii, V.: Unitary equivalence of proper extensions of a symmetric operator and the Weyl function. Integr. Equ. Oper. Theory 77(4), 449–487 (2013)
Hassi, S., Sebestyén, Z., de Snoo, H.S.V., Szafraniec, F.H.: A canonical decomposition for linear operators and linear relations. Acta Math. Hungar. 115(4), 281–307 (2007)
Hassi, S., Wietsma, H.: Minimal realizations of generalized Nevanlinna functions. Opuscula Math. 36(6), 749–768 (2016)
Iokhvidov, I., Krein, M.: Spectral theory of operators in space with indefinite metric. I, Tr. Mosk. Mat. Obs. 5 (1956), 367–432
Jonas, P., Langer, H.: Self-adjoint extensions of a closed linear relation of defect one in a Krein space, Operator theory and boundary eigenvalue problems, pp. 176–205, (1995)
Juršėnas, R.: Weyl families of transformed boundary pairs, Math. Nachr. (2023)
Kochubei, A.N.: Extensions of symmetric operators and symmetric binary relations. Mat. Zametki 17(1), 41–48 (1975)
Krein, M., Langer, H.: Defect subspaces and generalized resolvents of an Hermitian operator in the space \(\Pi _k\). Funktsional. Anal. i Prilozhen. 5(2), 59–71 (1971)
Kuzhel, S., Trunk, C.: On a class of J-self-adjoint operators with empty resolvent set. J. Math. Anal. Appl. 379(1), 272–289 (2011)
Langer, H., Luger, A.: A class of 2 \(\times \) 2-matrix functions, Glasnik Matematički 35(55), 149–160 (2000)
Langer, H., Textorius, B.: On generalized resolvents and Q-functions of symmetric linear relations (subspaces) in Hilbert space. Pacific. J. Math. 72(1), 135–165 (1977)
Malamud, M., Mogilevskii, V.: Krein type formula for canonical resolvents of dual pairs of linear relations. Methods Func. Anal. Topology 8(4), 72–100 (2002)
Mogilevskii, V.: Boundary triplets and Krein type resolvent formula for symmetric operators with unequal defect numbers. Methods Func. Anal. Topology 12(3), 258–280 (2006)
Mogilevskii, V.: Boundary triplets and Titchmarsh.Weyl functions of differential operators with arbitrary deficiency indices. Methods Func. Anal. Topology 15(3), 280–300 (2009)
Mogilevskii, V.: Description of generalized resolvents and characteristic matrices of differential operators in terms of the boundary parameter. Math. Notes 90(4), 558–583 (2011)
Popovici, D., Sebestyén, Z.: Factorizations of linear relations. Adv. Math. 233, 40–55 (2013)
Sandovici, A., Sebestyén, Z.: On operator factorization of linear relations. Positivity 17(4), 1115–1122 (2013)
Shmul’yan, Yu.L.: Extension theory for operators and spaces with indefinite metric. Izv. Akad. Nauk. 38(4), 896–908 (1974)
Strauss, V.A., Trunk, C.: Some Sobolev spaces as Pontryagin spaces. Vestn. Yuzhno-Ural. Gos. Un-ta. Ser. Matem. Mekh. Fiz. 6, 14–23 (2012)
Wietsma, H.L.: On unitary relations between Krein spaces. Acta Wasaensia, Vaasan Yliopisto (2012)
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Appendix A.
Appendix A.
Lemma A.1
Let \({\mathfrak {H}}=({\mathfrak {H}},[\cdot ,\cdot ])\) be a Krein space with fundamental symmetry J, and consider relations G and H in \({\mathfrak {H}}\) such that \(H\subseteq G^+\cap G^\bot \). Then:
-
(a)
If \({{\,\textrm{dom}\,}}G\bot {{\,\textrm{dom}\,}}H\) then
$$\begin{aligned} \begin{aligned}&{{\,\textrm{ran}\,}}(JH+zI)\subseteq {\mathfrak {N}}_z(JG^+)\\&\text {or equivalently}\\&{{\,\textrm{ran}\,}}(JG+zI)\subseteq {\mathfrak {N}}_z(JH^+) \end{aligned} \end{aligned}$$(A.1)for all \(z\in {\mathbb {C}}\).
-
(b)
If \(G\,\widehat{\oplus }\,H\) is a neutral subset of \({\mathfrak {K}}\) then:
-
(i)
The inclusions in (A.1) hold for both \(z=\textrm{i}\) and \(z=-\textrm{i}\).
-
(ii)
The inclusions in (A.1) become the equalities for \(z=\textrm{i}\) or \(z=-\textrm{i}\) (resp. for both \(z=\textrm{i}\) and \(z=-\textrm{i}\)) iff \(G\,\widehat{\oplus }\,H\) is maximal (resp. hyper-maximal) neutral.
-
(i)
Remark A.2
In (b), \({{\,\textrm{dom}\,}}G\bot {{\,\textrm{dom}\,}}H\) is not assumed. As in the body of the text, the symbol \(\bot \) indicates the orthogonality with respect to a Hilbert space metric \([\cdot ,J\cdot ]\), while \([\bot ]\) refers to the orthogonality with respect to \([\cdot ,\cdot ]\).
Proof
(a) \({{\,\textrm{dom}\,}}G\bot {{\,\textrm{dom}\,}}H\) implies that
Since \(G\bot H\), this implies that also
Consider \((f,f^\prime )\in JH\), so that \(f^\prime +zf\in {{\,\textrm{ran}\,}}(JH+zI)\) for all \(z\in {\mathbb {C}}\). Then
Since \((f,f^\prime )\), \((f^\prime ,0)\), and (0, f) are all the elements from \(JG^+\), \(f^\prime +zf\in {\mathfrak {N}}_z(JG^+)\).
(b)(i) Let \(K\mathrel {\mathop :}=G\,\widehat{\oplus }\,H\) be neutral. Since \(JH=JK\cap (JG)^\bot \), the range \({{\,\textrm{ran}\,}}(JH+zI)\), for all \(z\in {\mathbb {C}}\), consists of those \(k^\prime +zk\) such that \((k,k^\prime )\in JK\) and \((k^\prime ,-k)\in JG^+\). If \(z=\textrm{i}\) then
Since \(JK\subseteq JG^+\), this shows \(k^\prime +\textrm{i}k\in {\mathfrak {N}}_\textrm{i}(JG^+)\). The case \(z=-\textrm{i}\) is treated analogously.
(b)(ii) Sufficiency: Let K be either maximal or hyper-maximal neutral; that is, either \(P_+(K)={\mathfrak {K}}\) or \(P_-(K)={\mathfrak {K}}\) if K is maximal and \(P_\pm (K)={\mathfrak {K}}\) if K is hyper-maximal. We consider the case \(P_+(K)={\mathfrak {K}}\), since the case \(P_-(K)={\mathfrak {K}}\) is treated analogously. In view of (b)(i) it suffices to show that \({\mathfrak {N}}_\textrm{i}(JG^+)\subseteq {{\,\textrm{ran}\,}}(JH+\textrm{i}I)\).
If \(P_+(K)={\mathfrak {K}}\) then a maximal symmetric relation JK in a Hilbert space \(({\mathfrak {H}},[\cdot ,J\cdot ])\) satisfies \({{\,\textrm{ran}\,}}(JK+\textrm{i}I)={\mathfrak {H}}\). Thus, if \(g\in {\mathfrak {N}}_\textrm{i}(JG^+)\) then \((\exists (k,k^\prime )\in JK)\) \(g=k^\prime +\textrm{i}k\). Then
Since \(JK\subseteq JG^+\), this shows \((k^\prime ,-k)\in JG^+\), i.e. \(g\in {{\,\textrm{ran}\,}}(JH+\textrm{i}I)\).
Necessity: Let \(K=G\,\widehat{\oplus }\,H\) be neutral and \({{\,\textrm{ran}\,}}(JH\pm \textrm{i}I)={\mathfrak {N}}_{\pm \textrm{i}}(JG^+)\). Then \({{\,\textrm{ran}\,}}(JK\pm \textrm{i}I)={\mathfrak {H}}\), thus showing \(P_\pm (K)={\mathfrak {K}}\). \(\square \)
Lemma A.3
Let G and H be relations in a Krein space \(({\mathfrak {H}},[\cdot ,\cdot ])\) with fundamental symmetry J.
-
(a)
The eigenspace
$$\begin{aligned} \begin{aligned} {\mathfrak {N}}_z(G\,\widehat{+}\,H)=&{{\,\textrm{ran}\,}}((G-zI)^{-1}(zI-H)+I)\\ =&{{\,\textrm{ran}\,}}((G-zI)^{-1}-(H-zI)^{-1})\\ \supseteq&{\mathfrak {N}}_z(G)+{\mathfrak {N}}_z(H) \end{aligned} \end{aligned}$$(A.2)for all \(z\in {\mathbb {C}}\).
-
(b)
Let \(O=O(G,H)\) be the set of all those \(z\in {\mathbb {C}}\) such that
$$\begin{aligned} {{\,\textrm{ran}\,}}(G-zI)\cap {{\,\textrm{ran}\,}}(H-zI)=\{0\}. \end{aligned}$$(Equivalently, O is the set of all those \(z\in {\mathbb {C}}\) such that \((G-zI)^{-1}(H-zI)\subseteq {\mathfrak {N}}_z(H)\times {\mathfrak {N}}_z(G)\).) Then the inclusion \(\supseteq \) in (A.2) becomes the equality for all \(z\in O\); hence
$$\begin{aligned} O\cap \sigma _p(G\,\widehat{+}\,H)= O\cap (\sigma _p(G)\cup \sigma _p(H) ). \end{aligned}$$(A.3) -
(c)
Suppose \(G\bot H\) as linear subsets of \({\mathfrak {K}}\). Let O be as in (b). Then
$$\begin{aligned} \sigma _p(G\,\widehat{\oplus }\,H)= ( O\cap (\sigma _p(G)\cup \sigma _p( H) ) )\amalg ({\mathbb {C}}\smallsetminus O). \end{aligned}$$(A.4)(The symbol \(\amalg \) denotes the union of disjoint sets.) In particular:
-
(i)
\(\sigma _p(G\,\widehat{\oplus }\,H)=\emptyset \) (resp. \(\sigma ^0_p(G\,\widehat{\oplus }\,H)=\emptyset \)) iff \(O={\mathbb {C}}\) and \(\sigma _p(G)=\sigma _p(H)=\emptyset \) (resp. \(O\supseteq {\mathbb {C}}_*\) and \(\sigma ^0_p(G)=\sigma ^0_p(H)=\emptyset \)).
-
(ii)
\(\sigma _p(G\,\widehat{\oplus }\,H)={\mathbb {C}}\) (resp. \(\sigma ^0_p(G\,\widehat{\oplus }\,H)={\mathbb {C}}_*\)) iff \(O\subseteq \sigma _p(G)\cup \sigma _p(H)\) (resp. \({\mathbb {C}}_*\cap O\subseteq \sigma ^0_p(G)\cup \sigma ^0_p(H)\)).
-
(i)
Proof
(a) Let \(f\in {\mathfrak {N}}_z(G\,\widehat{+}\,H)\), i.e. \((f,zf)\in G\,\widehat{+}\,H\). Then \(f=g+h\) with \((g,g^\prime )\in G\) and \((h,h^\prime )\in H\) such that \(g^\prime +h^\prime =z(g+h)\), i.e. \((\exists u)\) \((g,u)\in G-zI\) and \((h,u)\in zI- H\), i.e. \((h,g)\in (G-zI)^{-1}(zI-H)\). Since the arguments are reversible, this proves (A.2).
(b) First we show that \(z\in O\) iff \(z\in {\mathbb {C}}\) satisfies \((G-zI)^{-1}(H-zI)\subseteq {\mathfrak {N}}_z(H)\times {\mathfrak {N}}_z(G)\). This will follow from a general claim: If X and Y are relations in \({\mathfrak {H}}\) then \({{\,\textrm{ran}\,}}X\cap {{\,\textrm{ran}\,}}Y\) is trivial iff \(X^{-1}Y\subseteq \ker Y\times \ker X\). (Notice that always \(X^{-1}Y\supseteq \ker Y\times \ker X\).) Indeed, \({{\,\textrm{ran}\,}}X\cap {{\,\textrm{ran}\,}}Y\) consists of those u such that \((\exists x)\) \((\exists y)\) \((x,u)\in X\) and \((y,u)\in Y\), while \(X^{-1}Y\) is the set of those (y, x) such that \((\exists u)\) \((x,u)\in X\) and \((y,u)\in Y\). Therefore, if \({{\,\textrm{ran}\,}}X\cap {{\,\textrm{ran}\,}}Y\) is trivial then \((y,x)\in X^{-1}Y\) implies \((y,x)\in \ker Y\times \ker X\). And conversely, if \(X^{-1}Y=\ker Y\times \ker X\) then \(u\in {{\,\textrm{ran}\,}}X\cap {{\,\textrm{ran}\,}}Y\) implies \(u=0\).
This shows in particular that the inclusion \(\supseteq \) in (A.2) becomes the equality for all \(z\in O\).
(c) Let
By (a), \({\mathfrak {N}}_z(G\,\widehat{\oplus }\,H)\) is trivial iff so is \({{\,\textrm{ran}\,}}L_z\), i.e.iff \(L_z\subseteq {\mathfrak {H}}\times \{0\}\). We show that \(\ker L_z\) is trivial, meaning that the last inclusion is equivalent to \(L_z=\{0\}\), which in turn is equivalent to \((G-zI)^{-1}(zI-H)=\{0\}\).
The relation \(L_z\) consists of the pairs \((h,g+h)\) such that \((\exists u)\) \((g,zg+u)\in G\) and \((h,zh-u)\in H\). Since \(G\bot H\)
where the scalar product \(\left\langle x,y\right\rangle \mathrel {\mathop :}=[x,Jy]\) and the norm \(\Vert x\Vert ^2\mathrel {\mathop :}=\left\langle x,x\right\rangle \) for all x, \(y\in {\mathfrak {H}}\). If \(g+h=0\) then by the above
But by Cauchy–Schwarz
so that then \(g=0=u\) and \(h=0\).
Suppose now \((G-zI)^{-1}(zI-H)=\{0\}\). Multiplying both sides by \(G-zI\) from the left implies that
Then
and then \(R=\{0\}\), since
by \(G\bot H\). In particular
This shows that \({\mathbb {C}}\smallsetminus \sigma _p(G\,\widehat{\oplus }\,H)\subseteq O\). The latter combined with (A.3) yields (A.4), which in turn yields (i) and (ii). \(\square \)
Remark A.4
For closed relations G and H and for \(z\in \rho (G)\cap \rho (H)\), the second equality in (A.2) is given in [7, Lemma 1.7.2].
Lemma A.5
Let G be a relation in a Krein space \({\mathfrak {H}}\). In order that the eigenspaces corresponding to distinct eigenvalues of the adjoint \(G^+\) should be mutually disjoint, that is, \((\forall z,z_0\in {\mathbb {C}})\)
it is necessary and sufficient that \({{\,\textrm{dom}\,}}G+{{\,\textrm{ran}\,}}G\) should be dense in \({\mathfrak {H}}\).
Proof
Let \(f\in {\mathfrak {N}}_z(G^+)\cap {\mathfrak {N}}_{z_0}(G^+)\), \(z\ne z_0\). Then \((f,zf)\in G^+\) and \((f,z_0f)\in G^+\) implies \(f\in {{\,\textrm{mul}\,}}G^+\cap \ker G^+\). Conversely, if \(f\in {{\,\textrm{mul}\,}}G^+\cap \ker G^+\) then \((\forall w\in {\mathbb {C}})\) \((f,wf)\in G^+\); hence in particular \(f\in {\mathfrak {N}}_z(G^+)\cap {\mathfrak {N}}_{z_0}(G^+)\). Therefore, \({\mathfrak {N}}_z(G^+)\cap {\mathfrak {N}}_{z_0}(G^+)\) for \(z\ne z_0\) is trivial iff \({{\,\textrm{mul}\,}}G^+\cap \ker G^+= ({{\,\textrm{dom}\,}}G+{{\,\textrm{ran}\,}}G)^{[\bot ]}\) is trivial. \(\square \)
Lemma A.6
A closed symmetric operator in a Hilbert space has property (P), see Definition 6.10, iff it is densely.
Proof
Step 1. Let T be a closed symmetric relation in a Hilbert space \({\mathfrak {H}}\). Then \((\forall z\in {\mathbb {C}}_*)\) \({\mathfrak {N}}_z(T^*)\cap {{\,\textrm{dom}\,}}T=\{0\}\). For, if \(f\in {\mathfrak {N}}_z(T^*)\) then \((f,zf)\in T^*\) and if also \(f\in {{\,\textrm{dom}\,}}T\) then \((\exists f^\prime )\) \((f,f^\prime )\in T\), i.e. \(f^\prime -zf\in {{\,\textrm{ran}\,}}(T-zI)\cap {{\,\textrm{mul}\,}}T^*\); but the latter set is trivial, see e.g.[28, Eq. (2.4)].
Step 2. We use the first von Neumann formula
Since \({\mathfrak {N}}_{\pm \textrm{i}}(T^*)\cap {{\,\textrm{dom}\,}}T=\{0\}\), \({{\,\textrm{mul}\,}}T^*\) consists of the elements \(f^\prime +\textrm{i}f_\textrm{i}-\textrm{i}f_{-\textrm{i}}\), where \((f,f^\prime )\in T\), \(f_{\pm \textrm{i}}\in {\mathfrak {N}}_{\pm \textrm{i}}(T^*)\), and \(f+f_\textrm{i}+f_{-\textrm{i}}=0\); hence \(f=0\), \(f^\prime \in {{\,\textrm{mul}\,}}T=\{0\}\), and \(f_{-\textrm{i}}=-f_{\textrm{i}}\in {\mathfrak {N}}_{\textrm{i}}(T^*)\cap {\mathfrak {N}}_{-\textrm{i}}(T^*)\). By Lemma A.5\({\mathfrak {N}}_{\textrm{i}}(T^*)\cap {\mathfrak {N}}_{-\textrm{i}}(T^*)= {{\,\textrm{mul}\,}}T^*\cap \ker T^*\), so \({{\,\textrm{mul}\,}}T^*\subseteq {{\,\textrm{mul}\,}}T^*\cap \ker T^*\) implies that \({{\,\textrm{mul}\,}}T^*\cap \ker T^*=\{0\}\) iff \(T^*\) is an operator. \(\square \)
Remark A.7
In Step 1 one could instead use that \((\forall z\in {\mathbb {C}})\)
and that \(T^*\cap ({{\,\textrm{dom}\,}}T)^2\) is a symmetric relation in a Hilbert space \(\overline{{{\,\textrm{dom}\,}}}T\).
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Juršėnas, R. On the Similarity of Boundary Triples of Symmetric Operators in Krein Spaces. Complex Anal. Oper. Theory 17, 72 (2023). https://doi.org/10.1007/s11785-023-01361-9
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DOI: https://doi.org/10.1007/s11785-023-01361-9