<p>We investigate Caputo time–fractional quantum dynamics generated by a <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathcal{P}\mathcal{T}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">P</mi> <mi mathvariant="script">T</mi> </mrow> </math></EquationSource> </InlineEquation>–symmetric complex periodic Schrödinger operator on the real line. The spatial part is a one-dimensional Schrödinger operator with an extended complex trigonometric potential that is <i>L</i>–periodic and <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mathcal{P}\mathcal{T}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">P</mi> <mi mathvariant="script">T</mi> </mrow> </math></EquationSource> </InlineEquation>–symmetric, and the time evolution is governed by a Caputo time–fractional Schrödinger equation of order <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(0&lt;\alpha \le 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>α</mi> <mo>≤</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> with time-independent Hamiltonian <i>H</i>. Within a Bloch–Floquet framework we express the solution in terms of Mittag–Leffler functions of the Bloch band energies and obtain a band-resolved spectral expansion. For the finite-band Heun polynomial states of degree <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(N=2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>=</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation> we derive explicit evolution formulas and identify a finite-dimensional quasi-exactly solvable subspace. The analysis provides an analytic framework for Caputo time–fractional quantum dynamics in <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\mathcal{P}\mathcal{T}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">P</mi> <mi mathvariant="script">T</mi> </mrow> </math></EquationSource> </InlineEquation>–symmetric complex periodic lattices.</p>

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Caputo Time–Fractional Dynamics of a PT–Symmetric Complex Periodic Schrödinger Operator

  • Volkan ALA

摘要

We investigate Caputo time–fractional quantum dynamics generated by a \(\mathcal{P}\mathcal{T}\) P T –symmetric complex periodic Schrödinger operator on the real line. The spatial part is a one-dimensional Schrödinger operator with an extended complex trigonometric potential that is L–periodic and \(\mathcal{P}\mathcal{T}\) P T –symmetric, and the time evolution is governed by a Caputo time–fractional Schrödinger equation of order \(0<\alpha \le 1\) 0 < α 1 with time-independent Hamiltonian H. Within a Bloch–Floquet framework we express the solution in terms of Mittag–Leffler functions of the Bloch band energies and obtain a band-resolved spectral expansion. For the finite-band Heun polynomial states of degree \(N=2\) N = 2 we derive explicit evolution formulas and identify a finite-dimensional quasi-exactly solvable subspace. The analysis provides an analytic framework for Caputo time–fractional quantum dynamics in \(\mathcal{P}\mathcal{T}\) P T –symmetric complex periodic lattices.