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Indefinite Sturm–Liouville Operators in Polar Form

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Abstract

We consider the indefinite Sturm–Liouville differential expression

$$\begin{aligned} {\mathfrak {a}}(f):= - \frac{1}{w}\left( \frac{1}{r} f' \right) ', \end{aligned}$$

where \({\mathfrak {a}}\) is defined on a finite or infinite open interval I with \(0\in I\) and the coefficients r and w are locally summable and such that r(x) and \(({\text {sgn}}\,x) w(x)\) are positive a.e. on I. With the differential expression \({\mathfrak {a}}\) we associate a nonnegative self-adjoint operator A in the Krein space \(L^2_w(I)\) which is viewed as a coupling of symmetric operators in Hilbert spaces related to the intersections of I with the positive and the negative semi-axis. For the operator A we derive conditions in terms of the coefficients w and r for the existence of a Riesz basis consisting of generalized eigenfunctions of A and for the similarity of A to a self-adjoint operator in a Hilbert space \(L^2_{|w|}(I)\). These results are obtained as consequences of abstract results about the regularity of critical points of nonnegative self-adjoint operators in Krein spaces which are couplings of two symmetric operators acting in Hilbert spaces.

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References

  1. Abasheeva, N.L., Pyatkov, S.G.: Counterexamples in indefinite Sturm–Liouville problems. Siberian Adv. Math. 7(4), 1–8 (1997)

    MathSciNet  Google Scholar 

  2. Akhiezer, N.I., Glazman, I.M.: Theory of Linear Operators in Hilbert Space, Two Volumes Bound as One. Dover Publications, New York (1993)

    Google Scholar 

  3. Akopjan, R.V.: On the regularity at infinity of the spectral function of a \(J\)-nonnegative operator. Izv. Akad. Nauk Arm. SSR Ser. Mat. 15(5), 357–364 (1980). (in Russian)

  4. Atkinson, F.V.: Some further estimates for the Titchmarsh–Weyl \(m\)-coefficient, preprint, University of Toronto (1985)

  5. Azizov, T.Y., Iokhvidov, I.S.: Linear Operators in Spaces with an Indefinite Metric. John Wiley & Sons, New York (1990)

    Google Scholar 

  6. Beals, R.: Indefinite Sturm–Liouville problems and half-range completeness. J. Differ. Equ. 56, 391–407 (1985)

    MathSciNet  Google Scholar 

  7. Belna, C.L.: Cluster sets of arbitrary real functions: a partial survey. Real Anal. Exch. 1, 7–20 (1976)

    MathSciNet  Google Scholar 

  8. Bennewitz, C.: The HELP inequality in the regular case, General inequalities, 5 (Oberwolfach, 1986), 337–346, Internat. Schriftenreihe Numer. Math., 80, Birkhäuser, Basel (1987)

  9. Bennewitz, C.: Spectral asymptotics for Sturm–Liouville equations. Proc. Lond. Math. Soc. 59, 294–338 (1989)

    MathSciNet  Google Scholar 

  10. Binding, P., Ćurgus, B.: Riesz bases of root vectors of indefinite Sturm–Liouville problems with eigenparameter dependent boundary conditions. I. Operator theory and indefinite inner product spaces. In: Operator Theory: Advances and Applications, vol. 163, pp. 75–95. Birkhäuser, Basel (2006)

  11. Binding, P., Ćurgus, B.: Riesz bases of root vectors of indefinite Sturm–Liouville problems with eigenparameter dependent boundary conditions. II. Integral Equ. Oper. Theory 63(4), 473–499 (2009)

    MathSciNet  Google Scholar 

  12. Bingham, N.H., Goldie, C.M., Teugels, J.L.: Regular Variation. Encyclopedia of Mathematics and its Applications, vol. 27. Cambridge University Press, Cambridge (1989)

    Google Scholar 

  13. Bognár, J.: Indefinite Inner Product Space. Springer-Verlag, Berlin (1974)

    Google Scholar 

  14. Buldygin, V.V., Pavlenkov, V.V.: Karamata theorem for regularly log-periodic functions. Ukrainian Math. J. 64, 1635–1657 (2013)

    MathSciNet  Google Scholar 

  15. Buldygin, V.V., Indlekofer, K.-H., Klesov, O.I., Steinebach, J.G.: Pseudo-Regularly Varying Functions and Generalized Renewal Processes. In: Probability Theory and Stochastic Modelling 91, Springer, Cham (2018)

  16. Chisholm, R.S., Everitt, W.N.: On bounded integral operators in the space of integrable-square functions. Proc. R. Soc. Edinb. Sect. 69, 199–204 (1970/71)

  17. Ćurgus, B.: On the regularity of the critical point infinity of definitizable operators. Integral Equ. Oper. Theory 8, 462–488 (1985)

    MathSciNet  Google Scholar 

  18. Ćurgus, B., Derkach, V.: Partially fundamentally reducible operators in Krein spaces. Integral Equ. Oper. Theory 82, 469–518 (2015)

    MathSciNet  Google Scholar 

  19. Ćurgus, B., Derkach, V., Trunk, C.: Indefinite Sturm-Liouville operators in polar form. (2021) arXiv:2101.00104v2 [math.SP]

  20. Ćurgus, B., Fleige, A., Kostenko, A.: The Riesz basis property of an indefinite Sturm–Liouville problem with non-separated boundary conditions. Integral Equ. Oper. Theory 77, 533–557 (2013)

    MathSciNet  Google Scholar 

  21. Ćurgus, B., Langer, H.: A Krein space approach to symmetric ordinary differential operators with an indefinite weight function. J. Differ. Equ. 79, 31–61 (1989)

    MathSciNet  Google Scholar 

  22. Ćurgus, B., Najman, B.: A Krein space approach to elliptic eigenvalue problems with indefinite weights. Differ. Integral Equ. 7, 1241–1252 (1994)

    MathSciNet  Google Scholar 

  23. Ćurgus, B., Najman, B.: The operator \(({\rm sgn }\, x){d^{2}}/{dx^{2}}\) is similar to a self-adjoint operator in \(L^{2}({{\mathbb{R} }})\). Proc. Am. Math. Soc. 123, 1125–1128 (1995)

    Google Scholar 

  24. Ćurgus, B., Najman, B.: Positive differential operators in Krein space \(L^2(\mathbb{R})\). Recent developments in operator theory and its applications (Winnipeg, MB, 1994). In: Operator Theory: Advances and Applications, vol. 87, pp. 95–104. Birkhäuser, Basel (1996)

  25. Ćurgus, B., Najman, B.: Positive differential operators in the Krein space \(L^2({\mathbb{R}}^n)\). Contributions to operator theory in spaces with an indefinite metric (Vienna, 1995). In: Operator Theory: Advances and Applications, vol. 106, pp. 113–129. Birkhäuser, Basel (1998)

  26. Ćurgus, B., Read, T.: Discreteness of the spectrum of second-order differential operators and associated embedding theorems. J. Differ. Equ. 184, 526–548 (2002)

    MathSciNet  Google Scholar 

  27. Daho, K., Langer, H.: Sturm-Liouville operators with an indefinite weight function. Proc. R. Soc. Edinb. Sect. A 87, 161–191 (1977)

    MathSciNet  Google Scholar 

  28. Derkach, V.A.: On Weyl function and generalized resolvents of a Hermitian operator in a Krein space. Integral Equ. Oper. Theory 23, 387–415 (1995)

    MathSciNet  Google Scholar 

  29. Derkach, V.A.: On generalized resolvents of Hermitian relations in Krein spaces. J. Math. Sci. 97, 4420–4460 (1999)

    MathSciNet  Google Scholar 

  30. Derkach, V.A., Hassi, S., Malamud, M.M., de Snoo, H.S.V.: Generalized resolvents of symmetric operators and admissibility. Methods Funct. Anal. Topol. 6(3), 24–55 (2000)

    MathSciNet  Google Scholar 

  31. Derkach, V.A., Malamud, M.M.: Generalized resolvents and the boundary value problems for Hermitian operators with gaps. J. Funct. Anal. 95, 1–95 (1991)

    MathSciNet  Google Scholar 

  32. Derkach, V., Malamud, M.: Extension Theory of Symmetric Operators and Boundary Value Problems, Transactions of Institute of Mathematics NAS of Ukraine, vol. 104, Kyiv (2017)

  33. Derkach, V., Strelnikov, D., Winkler, H.: On a class of integral systems. Complex Anal. Oper. Theory 15(6), Paper No. 103 (2021)

  34. Derkach, V., Trunk, C.: Coupling of defnitizable operators in Krein spaces. Nanosystems Phys. Chem. Math. 8, 166–179 (2017)

    Google Scholar 

  35. Edmunds, D., Evans, W.: Spectral Theory and Differential Operators. Oxford University Press, Oxford (1987)

    Google Scholar 

  36. Evans, W.D., Everitt, W.N.: HELP inequalities for limit-circle and regular problems. Proc. Roy. Soc. Lond. A 432, 367–390 (1991)

    MathSciNet  Google Scholar 

  37. Everitt, W.N.: On an extension to an integro-differential inequality of Hardy, Littlewood and Polya. Proc. Roy. Soc. Edinb. A 69, 295–333 (1972)

    MathSciNet  Google Scholar 

  38. Faddeev, M.M., Shterenberg, R.G.: On the similarity of some singular differential operators to self-adjoint operators. (Russian) Zap. Nauchn. Sem. S.-Peterburg. Otdel. Mat. Inst. Steklov. (POMI) 270 (2000), Issled. po Linein. Oper. i Teor. Funkts. vol. 28, pp. 336–349, 370–371; translation in J. Math. Sci. (N. Y.) 115, 2279–2286 (2003)

  39. Fleige, A.: The turning point condition of Beals for indefinite Sturm–Liouville problems. Math. Nachr. 172, 109–112 (1995)

    MathSciNet  Google Scholar 

  40. Fleige, A.: A counterexample to completeness properties for indefinite Sturm–Liouville problems. Math. Nachr. 190, 123–128 (1998)

    MathSciNet  Google Scholar 

  41. Fleige, A.: The Riesz basis property of an indefinite Sturm–Liouville problem with a non odd weight function. Integral Equ. Oper. Theory 60, 237–246 (2008)

    MathSciNet  Google Scholar 

  42. Fleige, A.: The critical point infinity associated with indefinite Sturm–Liouville problems. In: Alpay, D. (ed.) Operator Theory. Springer, Basel (2015)

    Google Scholar 

  43. Fleige, A., Najman, B.: Perturbations of Krein spaces preserving the nonsingularity of the critical point infinit. Contributions to operatot theory in spaces with and idenfinite metric (Vienna, 1995), In: Operator Theory: Advances and Applications, vol. 106, pp. 147–155, Birkhäuser, Basel (1998)

  44. Glazman, I.M.: On the theory of singular differential operators. Uspekhi Mat. Nauk 5(6), 102–135 (1950)

    MathSciNet  Google Scholar 

  45. Gorbachuk, V.I., Gorbachuk, M.L.: Boundary Value Problems for Operator Differential Equations. Kluwer Academic Publishers Group, Dordrecht (1991)

    Google Scholar 

  46. de Haan, L.: On Regular Variation and its Application to the Weak Convergence of Sample Extremes. Mathematical Centre Tracts, vol. 32. Mathematisch Centrum, Amsterdam (1970)

  47. Hille, E.: Non-oscillation theorems. Trans. Am. Math. Soc. 64, 234–252 (1948)

    MathSciNet  Google Scholar 

  48. Horning, A., Townsend, A.: FEAST for differential eigenvalue problems. SIAM J. Numer. Anal. 58, 1239–1262 (2020)

    MathSciNet  Google Scholar 

  49. Jonas, P.: Compact perturbations of definitizable operators II. J. Oper. Theory 8, 3–18 (1982)

    MathSciNet  Google Scholar 

  50. Jonas, P.: Regularity criteria for critical points of definitizable operators. In: Operator Theory: Advances and Applications, vol. 14, pp. 179–195. Birkhäuser (1984)

  51. Jonas, P., Langer, H.: Compact perturbations of definitizable operators. J. Oper. Theory 2, 63–77 (1979)

    MathSciNet  Google Scholar 

  52. Kac, I.S., Krein, M.G.: Criteria for the discreteness of the spectrum of a singular string, (Russian). Izv. Vysš. Učebn. Zaved. Mat. 2, 136–153 (1958)

    Google Scholar 

  53. Kac, I.S.: A generalization of the asymptotic formula of V. A. Marčenko for the spectral functions of a second order boundary value problem. (Russian) Izv. Akad. Nauk SSSR Ser. Mat. 37, 422–436. English transl. in: Math USSR Izv. 7(1973), 424–436 (1973)

  54. Kac, I.S., Krein, M.G.: \(R\)-functions-analytic functions mapping the upper halfplane into itself. Am. Math. Soc. Transl. Ser. (2) 103, 1–18 (1974)

    Google Scholar 

  55. Kac, I.S., Krein, M.G.: On the spectral functions of the string, Supplement II to the Russian edition of F.V. Atkinson, Discrete and continuous boundary problems, Mir, Moscow: (Russian) (English translation: Am. Math. Soc. Transl. (2) 103(1974), 19–102 (1968)

  56. Kalf, H.: Remarks on some Dirichlet type results for semibounded Sturm–Liouville operators. Math. Ann. 210, 197–205 (1974)

    MathSciNet  Google Scholar 

  57. Karabash, I.M.: \(J\)-self-adjoint ordinary differential operators similar to self-adjoint operators. Methods Funct. Anal. Topol. 6, 22–49 (2000)

    Google Scholar 

  58. Karabash, I.M.: A functional model, eigenvalues, and finite singular critical points for indefinite Sturm–Liouville operators. In: Operator Theory: Advances and Applications, vol. 203, pp. 247–287 (2009). arXiv:0902.4900

  59. Karabash, I.M., Kostenko, A.: Indefinite Sturm–Liouville operators with the singular critical point zero. Proc. Roy. Soc. Edinb. Sect. A 138, 801–820 (2008)

    MathSciNet  Google Scholar 

  60. Karabash, I.M., Kostenko, A., Malamud, M.M.: The similarity problem for \(J\)-nonnegative Sturm–Liouville operators. J. Differ. Equ. 246, 964–997 (2009)

    MathSciNet  Google Scholar 

  61. Karabash, I.M., Malamud, M.M.: Indefinite Sturm–Liouville operators with finite zone potentials. Oper. Matrices 1, 301–368 (2007)

    MathSciNet  Google Scholar 

  62. Karabash, I., Trunk, C.: Spectral properties of singular Sturm–Liouville operators. Proc. Roy. Soc. Edinb. Sect. A 139, 483–503 (2009)

    Google Scholar 

  63. Karabash, I.M., Kostenko, A.S.: On the similarity of operators of the type \({\rm sgn }\, x \bigl (-\frac{d^2}{dx^2} + c\delta \bigr )\) to a normal and a selfadjoint operator. Math. Notes 74(1–2), 127–131 (2003)

    MathSciNet  Google Scholar 

  64. Karamata, J.: Sur un mode croissance régulière des fonctions. Mathematica (Cluj) 4, 38–53 (1930)

    Google Scholar 

  65. Kasahara, Y.: Spectral theory of generalized second order differential operators and its applications to Markov processes, Japan. J. Math. (N.S.) 1(1), 67–84 (1975/76)

  66. Kochubei, A.N.: Extensions of \(J\)-symmetric operators (Russian). Teor. Funkciĭ Funkcional. Anal. i Prilozhen. 31, 74–80 (1979)

    Google Scholar 

  67. Korevaar, J.: Tauberian Theory: A Century of Developments. Grundlehren der Mathematischen Wissenschaften. Springer, Berlin (2004)

    Google Scholar 

  68. Kostenko, A.: The similarity problem for indefinite Sturm–Liouville operators with periodic coefficients. Oper. Matrices 5, 707–722 (2011)

    MathSciNet  Google Scholar 

  69. Kostenko, A.: The similarity problem for indefinite Sturm–Liouville operators and the HELP inequality. Adv. Math. 246, 368–413 (2013)

    MathSciNet  Google Scholar 

  70. Kostenko, A.: On a necessary aspect for the Riesz basis property for indefinite Sturm-Liouville problems. Math. Nachr. 287(14–15), 1710–1732 (2014)

    MathSciNet  Google Scholar 

  71. Langer, H.: Spectral functions of definitizable operators in Krein spaces. In: Functional analysis (Dubrovnik, 1981), Lecture Notes in Mathematics, vol. 948, pp. 1–46. Springer (1982)

  72. Marčenko, V.A.: Some questions of the theory of one-dimensional linear differential operators of the second order. I. (Russian). Trudy Moskov. Mat. Obšč. 1, 327–420 (1952)

    MathSciNet  Google Scholar 

  73. Maz’ja, V.G.: Sobolev Spaces. Springer-Verlag, Berlin Heidelberg New York (1985)

    Google Scholar 

  74. Muckenhoupt, B.: Weighted norm inequalities for the Hardy maximal function. Trans. Am. Math. Soc. 165, 207–226 (1972)

    MathSciNet  Google Scholar 

  75. Nehari, Z.: Oscillation criteria for second-order linear differential equations. Trans. Am. Math. Soc. 85, 428–445 (1957)

    MathSciNet  Google Scholar 

  76. Oinarov, R., Otelbaev, M.: A criterion for a general Sturm–Liouville operator to have a discrete spectrum. Differ. Equ. 24, 402–408 (1988)

    Google Scholar 

  77. Parfenov, A.I.: On an embedding criterion for interpolation spaces and application to indefinite spectral problems. Sib. Math. J. 44, 638–644 (2003)

    MathSciNet  Google Scholar 

  78. Parfenov, A.I.: The Ćurgus condition in indefinite Sturm–Liouville problems. Sib. Adv. Math. 15, 68–103 (2005)

    Google Scholar 

  79. Protter, M.H., Morrey, C.B.: A first Course in Real Analysis. Undergraduate Texts in Mathematics, 2nd edn. Springer-Verlag, New York (1991)

    Google Scholar 

  80. Pyatkov, S.G.: Interpolation of some function spaces and indefinite Sturm–Liouville problems. In: Differential and Integral Operators (Regensburg, 1995), Operator Theory: Advances and Applications, vol. 102, pp. 179–200. Birkhäuser, Basel (1998)

  81. Pyatkov, S.G.: Indefinite elliptic spectral problems. Sib. Math. J. 39, 358–372 (1998)

    MathSciNet  Google Scholar 

  82. Reed, M., Simon, B.: Methods of Modern Mathematical Physics. IV. Analysis of Operators. Academic Press, New York (1978)

    Google Scholar 

  83. Remling, C., Scarbrough, K.: The essential spectrum of canonical systems. J. Approx. Theory 254, 105395 (2020)

    MathSciNet  Google Scholar 

  84. Resnick, S.I.: Extreme Values, Regular Variation, and Point Processes. Applied Probability. A Series of the Applied Probability Trust, vol. 4. Springer-Verlag, New York (1987)

    Google Scholar 

  85. Romanov, R., Woracek, H.: Canonical systems with discrete spectrum. J. Funct. Anal. 278, 108318 (2020)

    MathSciNet  Google Scholar 

  86. Shmuljan, J.L.: Operator extension theory and spaces with indefinite metric Izv (Russian). Akad. Nauk SSSR Ser. Mat. 38, 896–908 (1974)

    MathSciNet  Google Scholar 

  87. Seneta, E.: Regularly Varying Functions. Lecture Notes in Mathematics, vol. 508. Springer-Verlag, Berlin-New York (1976)

    Google Scholar 

  88. Simon, B.: Operator Theory. A Comprehensive Course in Analysis, Part 4. American Mathematical Society, Providence (2015)

    Google Scholar 

  89. Stone, M.H.: Linear Transformations in Hilbert Space and their Applications to Analysis, AMS Colloquium Publ. American Mathematical Society, New York (1979)

    Google Scholar 

  90. Stuart, C.A.: The measure of non-compactness of some linear integral operators. Proc. Roy. Soc. Edinb. (A) 71, 167–179 (1972/73)

  91. Thomson, B.S., Bruckner, J.B., Bruckner, A.M.: Elementary Real Analysis, 2nd ed. www.classicalrealanalysis.com (2008)

  92. Titchmarsh, E.C.: Eigenfunction Expansions Associated with Second-Order Differential Equations. Part I, 2nd edn. Clarendon Press, Oxford (1962)

    Google Scholar 

  93. Veselić, K.: On spectral properties of a class of \(J\)-self-adjoint operators, I, II. Glasnik Mat. Ser. III 7(27), 229–248 (1972); ibid. 7(27), 249–254 (1972)

  94. Volkmer, H.: Sturm-Liouville problems with indefinite weights and Everitt’s inequality. Proc. Roy. Soc. Edinb. Sect. A 126, 1097–1112 (1996)

    MathSciNet  Google Scholar 

  95. Weyl, H.: Das asymptotische Verteilungsgesetz der Eigenwerte linearer partieller Differentialgleichungen (mit einer Anwendung auf die Theorie der Hohlraumstrahlung). Math. Ann. 71, 441–479 (1912)

    MathSciNet  Google Scholar 

  96. Wheeden, R.L., Zygmund, A.: Measure and Integral. An Introduction to Real Analysis. Pure and Applied Mathematics, 2nd edn. CRC Press, Boca Raton (2015)

    Google Scholar 

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Acknowledgements

The authors thank Aleksey Kostenko for fruitful discussions and literature hints. The authors thank the anonymous reviewer for very careful reading of our paper, a number of valuable comments and several literature suggestions.

Funding

Volodymyr Derkach gratefully acknowledges financial support by the Ministry of Education and Science of Ukraine (project # 0121U109525), by the German Research Foundation (DFG), grant TR 903/22-1, by the Fulbright Program, and travel support by the David and Darla Kennerud Visiting Math Scholars Fund at Western Washington University. The other two authors did not receive support from any organization for the submitted work.

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Appendix A: Some Results from Karamata’s Theory

Appendix A: Some Results from Karamata’s Theory

In Appendix we present the definitions and the results from Karamata’s theory of regularly varying functions that we use in the paper. Standard references for Karamata’s theory are [12] and [87]. For completeness we include a few standard results from Karamata’s theory and some of them are reformulated to fit our needs. In addition, we present Theorem A.6 and Corollary A.7 that seem to be new.

1.1 Definitions and basic results

First we give definitions of regularly varying functions.

Definition A.1

Let \(a,\alpha \in {\mathbb {R}}\) with \(a > 0\). A measurable function \(f:(0,a]\rightarrow {\mathbb {R}}_+\) is called regularly varying at 0 from the right with index \(\alpha \) if the following condition is satisfied:

$$\begin{aligned} \text {for all} \quad \lambda \in {\mathbb {R}}_+ \qquad \text {we have} \qquad \lim _{x\downarrow 0} \frac{f(\lambda x)}{f(x)} = \lambda ^{\alpha }. \end{aligned}$$

When \(\alpha = 0\) the function f is called slowly varying at 0 from the right.

A measurable function \(g:[a,+\infty ) \rightarrow {\mathbb {R}}_+\) is called regularly varying at \(+\infty \) with index \(\alpha \) if the following condition is satisfied:

$$\begin{aligned} \text {for all} \quad \lambda \in {\mathbb {R}}_+ \qquad \text {we have} \qquad \lim _{x\rightarrow +\infty } \frac{g(\lambda x)}{g(x)} = \lambda ^{\alpha }. \end{aligned}$$

When \(\alpha = 0\) the function g is called slowly varying at \(+\infty \).

A measurable function \(g:[-a,0) \rightarrow {\mathbb {R}}_-\) is called regularly varying at 0 from the left with index \(\alpha \) if the function \(f(x) = -g(-x)\) where \(x \in (0,a]\) is regularly varying at 0 from the right with index \(\alpha \). When \(\alpha = 0\) the function g is called slowly varying at 0 from the left.

We will often use “at \(0_+\)” as an abbreviation for the phrase “at 0 from the right” and “at \(0_-\)” as an abbreviation for the phrase “at 0 from the left.”

The Karamata’s theory of regular variation is commonly presented for functions regularly varying at \(+\infty \). The results for functions regularly varying at \(0_+\) follow from the following equivalence. Let f and g be measurable functions such that \(g(x) = f(1/x)\) for all x in the domain of g for which 1/x is in the domain of f. Then g is regularly varying at \(+\infty \) with index \(\alpha \) if and only if f is regularly varying at \(0_+\) with index \(-\alpha \).

In this section some results will be presented at \(0_+\) and some at \(+\infty \). This choice is sometimes made based on our needs in this paper and sometimes on convenience.

Slow variation plays the central role in the theory of regular variation. That centrality is expressed in the following proposition that follows immediately from the definition.

Proposition A.2

Let \(a, \alpha \in {\mathbb {R}}\) with \(a > 0\) and let \(f, g:(0,a]\rightarrow {\mathbb {R}}_+\) be measurable functions such that \(g(x) = x^\alpha f(x)\) for all \(x\in (0,a]\). The function g is regularly varying at \(0_+\) with index \(\alpha \) if and only if f is slowly varying at \(0_+\).

The next theorem is Karamata’s Representation Theorem, see [12, Theorem 1.3.1] or [64] for Karamata’s original paper.

Theorem A.3

Let \(a \in {\mathbb {R}}\). A function \(f:[a,+\infty )\rightarrow {\mathbb {R}}_+\) is slowly varying at \(+\infty \) if and only if there exist \(b \in [a,+\infty )\), a measurable function \(m: [b,+\infty ) \rightarrow {\mathbb {R}}_+\) and a continuous function \(\varepsilon : [b,+\infty ) \rightarrow {\mathbb {R}}\) such that

$$\begin{aligned} \lim _{x\rightarrow +\infty } m(x) = M \in {\mathbb {R}}_+, \qquad \lim _{x\rightarrow +\infty } \varepsilon (x) = 0, \end{aligned}$$

and for all \(x \ge b\) we have

$$\begin{aligned} f(x) = m(x) \exp \left( \int _{b}^{x} \frac{\varepsilon (t)}{t} dt \right) . \end{aligned}$$

The following property of regularly varying functions follows from Proposition A.2 and Theorem A.3, see [87, 1\(^\circ \) on page 18].

Corollary A.4

If g is a regularly varying function at \(+\infty \) with a positive (negative, respectively) index, then

$$\begin{aligned} \lim _{x\rightarrow +\infty } g(x) = +\infty \qquad \text {(} \lim _{x\rightarrow +\infty } g(x) = 0, \ \text {respectively)}. \end{aligned}$$

If f is a regularly varying function at \(0_+\) with a positive (negative, respectively) index, then

$$\begin{aligned} \lim _{x\downarrow 0} f(x) = 0 \qquad \text {(} \lim _{x\downarrow 0} f(x) = +\infty , \ \text {respectively)}. \end{aligned}$$

1.2 Karamata’s Characterization and Consequences

The following theorem is our restatement of Karamata’s characterization of regular variation as it appears in [46, Theorem 1.2.1], [67, Theorems IV.5.2 and IV.5.3], [12, Theorems 1.5.11 and 1.6.1] and [14]. In [12, 14, 46, 67] regular variation at \(+\infty \) is considered. Here we characterize regular variation at \(0_+\).

Theorem A.5

Let \(a\in {\mathbb {R}}_+\) and let \(f:(0,a] \rightarrow {\mathbb {R}}_+\) be a locally integrable function on (0, a]. Let \(\alpha , \gamma \in {\mathbb {R}}\) be such that \(\gamma + \alpha \ne 0\) and consider the following two conditions:

$$\begin{aligned}{} & {} \int _{0}^{a} s^{\gamma -1} f(s) ds \quad \text {exists as an improper integral at }0, \end{aligned}$$
(A.1)
$$\begin{aligned}{} & {} \lim _{v \downarrow 0} \frac{1}{v^\gamma f(v)} \int _{0}^{v} s^{\gamma -1} f(s) ds = \frac{1}{\gamma + \alpha }. \end{aligned}$$
(A.2)

The following statements are equivalent:

  1. (a)

    f is regularly varying at \(0_+\) with index \(\alpha \).

  2. (b)

    For all \(\gamma \in {\mathbb {R}}\) such that \(\gamma + \alpha > 0\) conditions (A.1) and (A.2) hold.

  3. (c)

    There exists \(\gamma \in {\mathbb {R}}\) such that \(\gamma + \alpha > 0\) and (A.1) and (A.2) hold.

The next theorem is a reformulation of the preceding one in terms of the differential of the function under consideration.

Theorem A.6

Let \(a, \hspace{1.111pt}\alpha , \hspace{1.111pt}\gamma \in {\mathbb {R}}\) be such that \(a > 0, \hspace{1.111pt}\gamma \ne 0\hspace{1.111pt}\) and \(\hspace{1.111pt}\gamma + \alpha \ne 0\). Let \({f:(0,a] \rightarrow {\mathbb {R}}_+}\) be a measurable function which is of bounded variation on each closed interval contained in (0, a]. Consider the following three conditions:

$$\begin{aligned}{} & {} \int _{0}^{a} s^\gamma df(s) \quad \text {exists as an improper Riemann-Stieltjes integral at }0, \nonumber \\ \end{aligned}$$
(A.3)
$$\begin{aligned}{} & {} \lim _{v \downarrow 0} v^\gamma f(v) = 0, \end{aligned}$$
(A.4)
$$\begin{aligned}{} & {} \lim _{v \downarrow 0} \frac{1}{v^\gamma f(v)} \displaystyle \int _{0}^{v}\! s^\gamma df(s) = \frac{\alpha }{\gamma + \alpha }. \end{aligned}$$
(A.5)

The following statements are equivalent:

  1. (i)

    f is regularly varying at \(0_+\) with index \(\alpha \).

  2. (ii)

    For all \(\gamma \in {\mathbb {R}}\!\setminus \!\{0\}\) such that \(\gamma + \alpha > 0\) conditions (A.3), (A.4) and (A.5) hold.

  3. (iii)

    There exists \(\gamma \in {\mathbb {R}}\!\setminus \!\{0\}\) such that \(\gamma + \alpha > 0\) and conditions (A.3), (A.4) and (A.5) hold.

Proof

Let \(u, v \in (0,a]\) such that \(u < v\). First notice that since f is of bounded variation on [uv], see [96, Theorems 2.21 and 2.24], the integration by parts yields

$$\begin{aligned} \int _{u}^{v} s^\gamma df(s) = v^{\gamma } f(v) - u^{\gamma } f(u) - \gamma \int _{u}^{v} s^{\gamma -1} f(s) ds. \end{aligned}$$
(A.6)

Assume (i). Let \(\gamma \in {\mathbb {R}}{\setminus }\{0\}\) be such that \(\gamma + \alpha > 0\). Since by Definition A.1 the function \(x\mapsto x^\gamma f(x)\) is regularly varying at \(0_+\) with index \(\gamma +\alpha \), Corollary A.4 yields (A.4).

Theorem A.5 implies that (A.1) and (A.2) hold. Letting \(u\downarrow 0\) in (A.6) and using (A.1) yields (A.3) and

$$\begin{aligned} \frac{1}{v^{\gamma } f(v)} \int _{0}^{v} s^\gamma df(s) = 1 - \frac{\gamma }{v^{\gamma } f(v)} \int _{0}^{v} s^{\gamma -1} f(s) ds. \end{aligned}$$
(A.7)

Now letting \(v\downarrow 0\) and using (A.2) we deduce (A.5), proving (ii).

The fact that (ii) implies (iii) is trivial. Now assume (iii). Letting \(u\downarrow 0\) in (A.6) and using (A.3) yields (A.1), and we again deduce (A.7). Together (A.7) and (A.5) imply (A.2) in Theorem A.5. Thus, (c) in Theorem A.5 holds and (i) follows from Theorem A.5. \(\square \)

Let \(\gamma > 0\). With the substitution \(t = v^\gamma \), conditions (A.3), (A.4) and (A.5) can be rewritten as (see [79, Theorem 12.11] for the change of variables formula in Riemann-Stieltjes integral)

$$\begin{aligned}{} & {} \int _{0}^{a^\gamma } t\hspace{0.83328pt}df(t^{1/\gamma }) \quad \text {exists as an improper Riemann-Stieltjes integral at }0, \\{} & {} \lim _{t \downarrow 0} t f(t^{1/\gamma }) = 0, \\{} & {} \lim _{t \downarrow 0} \frac{1}{t f(t^{1/\gamma })} \displaystyle \int _{0}^{t} s\hspace{0.83328pt}df\bigl (s^{1/\gamma }\bigr ) = \frac{\alpha /\gamma }{1 + \alpha /\gamma }. \end{aligned}$$

This observation and Theorem A.6 (with \(\gamma \) being 1 and \(\alpha \) being \(\alpha /\gamma \)) yield the following equivalence: The function \(t\mapsto f(t^{1/\gamma })\) with \(t\in (0,a^\gamma ]\) is regularly varying at \(0_+\) with index \(\alpha /\gamma > -1\) if and only if conditions (A.3), (A.4), (A.5) hold. Here it is convenient to read the last fraction in (A.5) as \((\alpha /\gamma )/\bigl (1+(\alpha /\gamma )\bigr )\).

The next corollary generalizes the preceding equivalence to any increasing bijection on [0, a].

Corollary A.7

Let \(\alpha , a, b \in {\mathbb {R}}\) be such that \(a, b > 0\) and \(\alpha > -1\). Let \({f:(0,b] \rightarrow {\mathbb {R}}_+}\) be a function of bounded variation on every closed subinterval of (0, b] and let \(g:[0,b] \rightarrow [0,a]\) be an increasing bijection. The function is regularly varying at \(0_+\) with index \(\alpha > -1\) if and only if the following three conditions are satisfied:

$$\begin{aligned}{} & {} \int _{0}^{b}\! g(s)\hspace{0.83328pt}df(s) \quad \text {exists as an improper Riemann-Stieltjes integral at }0,\nonumber \\ \end{aligned}$$
(A.8)
$$\begin{aligned}{} & {} \lim _{v \downarrow 0} f(v) g(v) = 0, \end{aligned}$$
(A.9)
$$\begin{aligned}{} & {} \lim _{v \downarrow 0} \frac{1}{f(v)g(v)}\! \int _{0}^{v}\! g(s)\hspace{0.83328pt}df(s) = \frac{\alpha }{1+\alpha }. \end{aligned}$$
(A.10)

Proof

Let \(u, v \in (0,b]\) such that \(u < v\). As in the preceding theorem we notice that since f is of bounded variation on [uv] the integration by parts ( [96, Theorem 2.21]) yields

$$\begin{aligned} \int _{u}^{v} g(s)\hspace{0.83328pt}df(s) = f(v)g(v) - f(u)g(u) - \int _{u}^{v} f(s)\hspace{0.83328pt}dg(s). \end{aligned}$$
(A.11)

In this proof we will also use that, since g is a continuous increasing bijection, we have that \(u \downarrow 0\) if and only if \(g(u)\downarrow 0\).

Assume (A.8), (A.9) and (A.10). Letting \(u\downarrow 0\) and using (A.8) and (A.9) in (A.11) yields

$$\begin{aligned} \int _{0}^{v} g(s)\hspace{0.83328pt}df(s) = f(v)g(v) - \int _{0}^{v} f(s)\hspace{0.83328pt}dg(s) \end{aligned}$$
(A.12)

for all \(v \in (0,b]\). Therefore, for all \(v \in (0,b]\) we have

$$\begin{aligned} \begin{aligned} \frac{1}{f(v)g(v)} \int _{0}^{v} g(s)\hspace{0.83328pt}df(s)&= 1 - \frac{1}{f(v)g(v)}\int _{0}^{v} f(s) dg(s) \\&= 1 - \frac{1}{f(v)g(v)}\int _{0}^{g(v)} f\bigl (g^{-1}(t)\bigr ) dt, \end{aligned} \end{aligned}$$
(A.13)

where, for the second equality, we used the change of variables formula in Riemann-Stieltjes integral, [79, Theorem 12.11]. Now (A.10) implies

$$\begin{aligned} \frac{1}{1+\alpha } = \lim _{v \downarrow 0} \frac{1}{f(v)g(v)}\int _{0}^{g(v)} f\bigl (g^{-1}(t)\bigr ) dt = \lim _{u \downarrow 0} \frac{1}{u f\bigl (g^{-1}(u)\bigr )}\int _{0}^{u} f\bigl (g^{-1}(t)\bigr ) dt. \end{aligned}$$

Since we assume \(1+\alpha > 0\), Theorem A.5 yields that is regularly varying at \(0_+\) with index \(\alpha \).

To prove the converse assume that is regularly varying at \(0_+\) with index \(\alpha > -1\). Then the function \(x\mapsto xf\bigl (g^{-1}(x)\bigr )\) is regularly varying at \(0_+\) with index \(\alpha + 1 > 0\) and (A.9) follows from Corollary A.4 after a change of variables in the limit. By the change of variables formula for all \(u \in (0,a]\) we have

$$\begin{aligned} \int _{u}^{a} s\hspace{0.83328pt}d f\bigl (g^{-1}(s)\bigr ) = \int _{g^{-1}(u)}^{b} g(t)\hspace{0.83328pt}df(t). \end{aligned}$$

Consequently, (A.8) follows from (A.3) in Theorem A.6 applied to with \(\gamma = 1\). Therefore, (A.12) and consequently (A.13) both hold. Now (A.10) follows from (A.2) in Theorem A.5 with \(\gamma =1\). \(\square \)

1.3 Asymptotic Equivalence of Functions on a Sequence

In the next definition we extend the notation \(\sim \) of asymptotic equivalence of functions to hold only on a sequence.

Definition A.8

Let \(a \in {\mathbb {R}}_+\). For functions \(f,g:[a,+\infty ) \rightarrow {\mathbb {R}}_+\) we write

if and only if there exists an increasing sequence \((x_n)\) in \([a,+\infty )\) such that

$$\begin{aligned} \lim _{n\rightarrow +\infty } x_n = +\infty \quad \text {and} \quad \lim _{n\rightarrow +\infty } \frac{f(x_n)}{g(x_n)} = 1. \end{aligned}$$

For functions \(f,g:(0,a] \rightarrow {\mathbb {R}}_+\) we write

if and only if there exists a decreasing sequence \((x_n)\) in (0, a] such that

$$\begin{aligned} \lim _{n\rightarrow +\infty } x_n = 0 \quad \text {and} \quad \lim _{n\rightarrow +\infty } \frac{f(x_n)}{g(x_n)} = 1. \end{aligned}$$

Recall, see [7, 91, 5.10.11], that for a function \(\phi :[a,+\infty )\) a real number L is a cluster value of \(\phi \) at \(+\infty \) if for every \(\epsilon > 0\) and for every \(X \in {\mathbb {R}}\) there exists \(x > X\) such that \(|\phi (x) - L| < \epsilon \). Similarly, for a function \(\phi :(0, a]\) a real number L is a cluster value of \(\phi \) at \(0_+\) if for every \(\epsilon > 0\) and for every \(\delta > 0\) there exists \(x \in (0,\delta )\) such that \(|\phi (x) - L| < \epsilon \). Notice that at \(+\infty \) (at \(0_+\)) if and only if 1 is a cluster value of the function f/g at \(+\infty \) (at \(0_+\)).

Proposition A.9

Let f and g be regularly varying functions at \(+\infty \) with indices \(\alpha \) and \(\beta \), respectively. If at \(+\infty \), then \(\alpha = \beta \).

Proof

We will prove the contrapositive. Assume that \(\alpha < \beta \). Since the function f(x)/g(x) is regularly varying with index \(\alpha -\beta <0\) it follows from Corollary A.4 that \(\lim _{x\rightarrow +\infty }f(x)/g(x)=0\). Thus, at \(+\infty \) is not true. If \(\alpha > \beta \) the preceding limit is \(+\infty \), so at \(+\infty \) is not true in this case either. \(\square \)

The converse of the preceding proposition is not true. For example, let f be a slowly varying function at \(+\infty \) and \(g=2f\). Then \(\alpha = \beta =0\), but at \(+\infty \) is clearly not true.

The following theorem extends [84, Proposition 0.8(vi)] to the concept introduced in the previous definition. This theorem can be deduced from [15, Corollary 7.66]. A direct proof is presented in [19, Theorem A.11, Corollary A.12].

Theorem A.10

Let f and g be strictly monotonic positive functions defined in a neighbourhood of \(0_+\) and let f be regularly varying at \(0_+\) with a nonzero index.

  1. (a)

    If f and g are increasing with 0 limit at \(0_+\), then the inverses \(f^{-1}\) and \(g^{-1}\) are also increasing, defined in a neighbourhood of \(0_+\) and the following equivalence holds

  2. (b)

    If f and g are decreasing and unbounded, then the inverses \(f^{-1}\) and \(g^{-1}\) are decreasing, defined in a neighbourhood of \(+\infty \) and the following equivalence holds

The following corollary is a consequence of the fact that the negation of at \(0_+\) is the statement

$$\begin{aligned} \left( \frac{f(x)}{g(x)} - 1 \right) ^{-1} = O(1) \quad \text {as} \quad x \downarrow 0. \end{aligned}$$

Each of the two statements in Theorem A.10 can be expressed using one of these negations. We state only the analogue of the last statement in Theorem A.10 since that is what is used in Theorem 4.16.

Corollary A.11

Let f and g be strictly monotonic positive functions defined in a neighbourhood of \(0_+\) and let f be regularly varying at \(0_+\) with a nonzero index. If f and g are decreasing and unbounded, then the inverses \(f^{-1}\) and \(g^{-1}\) are decreasing, defined in a neighbourhood of \(+\infty \) and the following equivalence holds

$$\begin{aligned} \left( \frac{f(x)}{g(x)} - 1 \right) ^{\!\!-1} = O(1) \ \text {as} \ x \downarrow 0 \quad \Leftrightarrow \quad \left( \frac{f^{-1}(y)}{g^{-1}(y)} - 1 \right) ^{\!\!-1} = O(1) \ \text {as} \ y \rightarrow +\infty . \end{aligned}$$

Clearly \(f\sim g\) at \(+\infty \) implies at \(+\infty \). In the next example we will demonstrate that at \(+\infty \) does not imply \(f\sim g\) at \(+\infty \) even for smooth normalized slowly varying increasing functions f and g for which f/g is normalized slowly varying function.

1.4 Positively Increasing Functions

The following class of functions was introduced as a generalization of regularly varying functions with positive index, see [15, Section 3.1 and Definition 3.26].

Definition A.12

Let \(a \in {\mathbb {R}}_+\). A nondecreasing function \(f: (0,a] \rightarrow {\mathbb {R}}_+\) is called positively increasing at 0 from the right if there exists \(\lambda \in (0,1)\) such that

$$\begin{aligned} \limsup _{x\downarrow 0}\frac{f(\lambda x)}{f(x)} < 1. \end{aligned}$$

A function \(g:[-a,0) \rightarrow {\mathbb {R}}_-\) is called positively increasing at 0 from the left if the function \(f(x) = -g(-x), x \in [-a,0)\), is positively increasing at 0 from the right.

A function \(g:[a,+\infty ) \rightarrow {\mathbb {R}}_+\) is called positively increasing at \(+\infty \) if the function \(f(x) = 1/g(1/x), x \in (0,1/a]\), is positively increasing at 0 from the right. A function \(g:(-\infty ,-a] \rightarrow {\mathbb {R}}_-\) is called positively increasing at \(-\infty \) if the function \(f(x) = -1/g(-1/x), x \in (0,1/a]\), is positively increasing at 0 from the right.

The relationship between regularly varying and positively increasing functions at \(+\infty \), and analogously at \(-\infty \), \(0_+\) and \(0_-\), is as follows. Each regularly varying function with positive index is positively increasing, while a regularly varying function with a nonpositive index is not positively increasing. In particular, a slowly varying function is not positively increasing. The exponential function \(\exp \) is positively increasing at \(+\infty \) but not regularly varying at \(+\infty \). As was shown in [19, Example A.17], there exists a nondecreasing function \(f:[1,+\infty )\rightarrow {\mathbb {R}}_+\) which is neither positively increasing nor slowly varying at \(+\infty \).

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Ćurgus, B., Derkach, V. & Trunk, C. Indefinite Sturm–Liouville Operators in Polar Form. Integr. Equ. Oper. Theory 96, 2 (2024). https://doi.org/10.1007/s00020-023-02746-3

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