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Advanced Methods of Linear ODEs

A linear ODE can be solved locally without revealing how its solutions fit together globally. This book begins where local existence theory leaves off: with the connection matrices, monodromy, Stokes data, and boundary functions that turn local solutions into spectra and physical response.

For canonically normalized fundamental solutions Φα\Phi_\alpha and Φβ\Phi_\beta in two regions, the organizing equation is

Φβ(z)=Φα(z)Cαβ.\Phi_\beta(z)=\Phi_\alpha(z)\,C_{\alpha\beta}.

The matrix CαβC_{\alpha\beta} is simple to write and often difficult to compute. Its entries can be obtained directly from Wronskians, analytic continuation, recurrences, or numerical matching. In suitable families, selected parts of the same global data can instead be encoded by isomonodromic tau functions, conformal blocks, quantum periods, Seiberg–Witten/Nekrasov–Shatashvili quantities, spectral determinants, ODE/IM functional relations, or TBA equations.

The book develops that problem for second-order complex linear ODEs and their locally equivalent traceless rank-two systems. Globally, three constructions are kept separate: a single-valued trace-zero gauge of a given GL(2)GL(2) system uses a horizontal determinant trivialization; an SL(2)SL(2) lift of its projectivization is a lifting or twisting problem; and a scalar oper realization uses a theta characteristic. Higher-order equations enter only where they are intrinsic to ODE/IM.

Write a fundamental matrix with columns formed from two independent scalar solutions,

Φα(z)=(yα,1(z)yα,2(z)yα,1(z)yα,2(z)).\Phi_\alpha(z)= \begin{pmatrix} y_{\alpha,1}(z) & y_{\alpha,2}(z)\\ y'_{\alpha,1}(z) & y'_{\alpha,2}(z) \end{pmatrix}.

A connection matrix is meaningful only together with its normalization ledger. If the two bases are changed by constant invertible matrices,

Φ~α=ΦαGα,Φ~β=ΦβGβ,\widetilde{\Phi}_\alpha=\Phi_\alpha G_\alpha, \qquad \widetilde{\Phi}_\beta=\Phi_\beta G_\beta,

then the same continuation problem is represented by

C~αβ=Gα1CαβGβ.\widetilde C_{\alpha\beta} =G_\alpha^{-1}C_{\alpha\beta}G_\beta.

Thus a bare gamma-function formula, continued fraction, tau function, or period is not yet a connection formula. One must also specify the equation, bases, leading normalizations, branches, continuation path, resonant exceptions, and—at an irregular singularity—the sectors and lateral summation prescription.

A map from canonical local bases through global connection data to monodromy, exact-WKB, gauge-theory, and integrability methods, ending in spectral and physical consequences.

The book is organized around global connection data. Solid arrows are direct ODE constructions or checks; dashed arrows require a model-specific dictionary and stated analytic hypotheses.

Three layers recur throughout the book:

LayerTypical objectsQuestion being answered
LocalFrobenius bases, formal normal forms, canonical sectorial solutionsWhat are the independent solutions near this point or in this sector?
GlobalConnection matrices, monodromy and Stokes matrices, Wronskians, boundary functionsHow do normalized solutions compare after continuation?
Spectral or physicalEigenvalues, resonances, quasinormal modes, Green functions, correlatorsWhich global coefficient vanishes, has a pole, or gives a response ratio?

The middle layer is indispensable. A boundary condition becomes a spectral condition only after it has been translated into a statement about a normalized connection coefficient or boundary Wronskian.

No single equation naturally illustrates every method. The book therefore uses two families in parallel.

LaboratoryProgressionWhat it teaches
Connection problemsHypergeometric \to HeunG \to confluent Heun equationsFrobenius bases, Wronskians, recurrences, monodromy, isomonodromy, conformal blocks, AGT, black-hole boundary data
Quantum curvesAiry and Weber \to Mathieu and modified Mathieu \to anharmonic and Razavy systemsTurning points, exact WKB, resurgence, quantum periods, Seiberg–Witten/NS theory, ODE/IM, TBA, tunnelling spectra

Each recurring example receives a persistent data sheet: equation and normal form, singularities and ranks, local and formal exponents, preferred bases, branch cuts and cycles, boundary conditions, known global data, and independent numerical checks.

I · Analytic foundations and direct methods

Chapters 1–4 build the common trunk: complex singularities, monodromy and connection matrices, the Heun laboratories, Wronskians, recurrences, and verified numerical computation.

II · Isomonodromy and conformal blocks

Chapters 5–7 develop monodromy-preserving deformation, Painlevé systems, BPZ equations, and the distinct roles of analytic c=1c=1 blocks and classical large-cc blocks.

III · Exact WKB and resurgence

Chapters 8–9 pass from formal WKB geometry to Borel summation, Stokes graphs, Voros symbols, wall crossing, transseries, and chamber-correct quantization.

IV · Seiberg–Witten theory and AGT

Chapters 10–11 establish the cycle, normalization, mass, momentum, and accessory-parameter dictionaries needed to compare ODE, CFT, and gauge descriptions.

V · ODE/IM and TBA

Chapters 12–13 derive spectral-determinant functional relations and show when analyticity data turn them into nonlinear integral equations.

VI · Integrating applications

Chapters 14–15 compare the methods on quantum-mechanical potentials, black-hole perturbations, quasinormal modes, and holographic response.

Chapters 1–4 are the common prerequisite trunk. Later branches can be read selectively, but the AGT dictionary assumes both the CFT and Seiberg–Witten/NS branches, while the TBA chapter assumes exact WKB and the ODE/IM functional-relation language.

The correspondences in this book are complementary tools, not interchangeable names for one universal object.

MethodPrimary outputWhat it does not provide automatically
Wronskian matchingExact ratios of connection coefficients or a boundary spectral conditionA stable computation when the chosen bases cannot be evaluated in a common domain
Recurrences and continued fractionsMinimal-solution conditions, connection amplitudes, spectraConvergence and conditioning without asymptotic analysis
IsomonodromyMonodromy-preserving flow, tau function, accessory dataA deformation family for an arbitrary isolated ODE
Analytic c=1c=1 blocksFourier/structure-constant expansions of isomonodromic tau functionsThe classical large-cc BPZ connection problem
Classical large-cc blocksAccessory parameters and, with extra data, connection coefficientsFusion, braiding, normalization, and analytic continuation factors by themselves
Formal WKBAsymptotic solutions and formal quantum periodsA unique exact value for a divergent series
Exact WKB and resurgenceDirectional Borel sums, Stokes jumps, chamber-dependent quantizationA chamber-independent formula without summability and boundary hypotheses
Seiberg–Witten/NS theoryQuantum periods and twisted-superpotential dataA model-independent nonperturbative completion
ODE/IMSpectral determinants and functional relations for suitable ODE familiesA construction for every linear ODE
TBA or Riemann–Hilbert integral equationsNonlinear integral equations and high-precision resummed dataEquivalence between ODE/IM TBA and exact-WKB/GMN equations in general

This distinction is a practical safeguard. For example, a zero of an isomonodromic tau function becomes a quantization condition only after the relevant monodromy and boundary constraints are imposed. Likewise, a classical conformal block principally fixes accessory data; a full connection coefficient also needs basis normalization and degenerate fusion or braiding data.

The book labels advanced statements by status:

  • Theorem — proved under the hypotheses stated on the page.
  • Proposition or derivation — established directly in the text.
  • Formal identity — an equality of formal series, with no convergence claim.
  • Conditional exact statement — exact after the listed summability, topology, analyticity, or boundary assumptions.
  • Conjectural correspondence — supported analytically or numerically but not proved in the stated generality.
  • Numerical observation — accompanied by method, precision, branch and contour choices, convergence criterion, and an independent check.

Substantial formulas include a normalization ledger. Computational claims aim for two independent checks chosen from an exactly solvable limit, a Wronskian identity, direct integration, a recurrence, an independent period calculation, spectral comparison, or a controlled confluence or symmetry limit.

The main audience is graduate students and researchers in mathematical physics, special functions, spectral theory, gravity, quantum field theory, and integrable systems. The common trunk assumes:

  • undergraduate ODEs and linear algebra;
  • complex differentiation, residues, and analytic continuation;
  • elementary asymptotic expansions;
  • basic quantum mechanics for the spectral examples.

The just-in-time toolkit supplies the required fundamental groups, local systems, Riemann surfaces, absolute and relative homology, intersection pairings, and minimal operator theory. CFT, supersymmetric gauge theory, and integrability are introduced only to the depth needed for the ODE problem.