arXiv subjects

Jeremy Tillay

Publications and source records attributed to Jeremy Tillay.

3 recordsLinked to original sources

arXiv2024

Noisy intermediate-scale quantum simulation of the one-dimensional wave equation

We design and implement quantum circuits for the simulation of the one-dimensional wave equation on the Quantinuum H1-1 quantum computer. The circuit depth of our approach scales as $O(n^{2})$ for $n$ qubits representing the solution on $2^{n}$ grid points, and leads to infidelities of $O(2^{-4n} t^{2})$ for simulation time $t$ assuming smooth initial conditions. By varying the qubit count we study the interplay between the algorithmic and physical gate errors to identify the optimal working point of minimum total error. Our approach to simulating the wave equation can be used with appropriate state preparation algorithms across different quantum processors and serve as an application-oriented benchmark.

quant-ph↗

arXiv2016

Spectra of semi-infinite quantum graph tubes

The spectrum of a semi-infinite quantum graph tube with square period cells is analyzed. The structure is obtained by rolling up a doubly periodic quantum graph into a tube along a period vector and then retaining only a semi-infinite half of the tube. The eigenfunctions associated to the spectrum of the half-tube involve all Floquet modes of the full tube. This requires solving the complex dispersion relation $D(λ,k_1,k_2)=0$ with $(k_1,k_2)\in(\mathbb{C}/2π\mathbb{Z})^2$ subject to the constraint $αk_1 + βk_2 \equiv 0$ (mod $2π$), where $α$ and $β$ are integers. The number of Floquet modes for a given $λ\in\mathbb{R}$ is $2\max\left\{ α, β\right\}$. Rightward and leftward modes are determined according to an indefinite energy flux form. The spectrum may contain eigenvalues that depend on the boundary conditions, and some eigenvalues may be embedded in the continuous spectrum.

math-ph↗

arXiv2016

Spectra of Half-Infinite Quantum Graph Tubes

Carbon nanotubes are a feverishly-studied topic in the scientific community as of late. Mathematically, they can be modeled with a quantum graph. Here we consider a structure somewhat similar to carbon nanotubes, another quantum graph that is formed by rolling a square lattice instead of a graphene structure. This symmetry imposes properties that make certain motions easier to study by creating convenient pairs of incoming and outgoing motions.

math-ph↗