C. Hooley

ORCID: 0000-0002-9976-2405
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About
Contact & Profiles
Research Areas
  • Analytic Number Theory Research
  • Mathematics and Applications
  • Physics of Superconductivity and Magnetism
  • History and Theory of Mathematics
  • Cold Atom Physics and Bose-Einstein Condensates
  • Advanced Condensed Matter Physics
  • Quantum many-body systems
  • Advanced Mathematical Theories
  • Algebraic Geometry and Number Theory
  • Advanced Mathematical Identities
  • Quantum and electron transport phenomena
  • Quantum, superfluid, helium dynamics
  • Black Holes and Theoretical Physics
  • Computability, Logic, AI Algorithms
  • Limits and Structures in Graph Theory
  • Theoretical and Computational Physics
  • Rare-earth and actinide compounds
  • Magnetic Properties and Applications
  • graph theory and CDMA systems
  • Opinion Dynamics and Social Influence
  • Magnetic properties of thin films
  • 2D Materials and Applications
  • Advanced Algebra and Geometry
  • Semiconductor Quantum Structures and Devices
  • Advanced Differential Equations and Dynamical Systems

Max Planck Institute for the Physics of Complex Systems
2023-2025

Coventry University
2025

Computational Physics (United States)
2025

University of St Andrews
2014-2024

Scottish Universities Physics Alliance
2007-2024

Cardiff University
2001-2018

Universidade Federal de São Carlos
2012

University of Birmingham
2001-2006

Rutgers, The State University of New Jersey
2001-2002

University of Wales
1977-2000

We consider spinless fermions on a finite one-dimensional lattice, interacting via nearest-neighbor repulsion and subject to strong electric field. In the non-interacting case, due Wannier-Stark localization, single-particle wave functions are exponentially localized even though model has no quenched disorder. show that this system remains in presence of interactions exhibits physics analogous models conventional many-body localization (MBL). particular, entanglement entropy grows...

10.1103/physrevlett.122.040606 article EN publisher-specific-oa Physical Review Letters 2019-01-30

Band inversions are key to stabilising a variety of novel electronic states in solids, from topological surface inverted bulk band gaps insulators the formation symmetry-protected three-dimensional Dirac and Weyl points nodal-line semimetals. Here, we create inversion not states, but rather between manifolds states. We realise this by aliovalent substitution Nb for Zr Sb S ZrSiS family nonsymmorphic Using angle-resolved photoemission density-functional theory, show how two pairs known ZrSiS,...

10.1038/s41467-019-13464-z article EN cc-by Nature Communications 2019-12-02

10.1007/bf02391856 article EN Acta Mathematica 1963-01-01

10.1112/plms/s3-7.1.396 article EN Proceedings of the London Mathematical Society 1957-01-01

10.1112/s002557930000797x article EN Mathematika 1967-06-01

In this paper, we describe animations and animated visualizations for introductory intermediate-level quantum mechanics instruction developed at the University of St Andrews. The aim to help students build mental representations concepts. They focus on known areas student difficulty misconceptions by including step-by-step explanations key points. are freely available, with additional resources available instructors. We have investigated their educational effectiveness both in terms attitude...

10.1088/0143-0807/31/6/010 article EN European Journal of Physics 2010-09-30

10.1515/crll.1967.225.209 article EN Journal für die reine und angewandte Mathematik (Crelles Journal) 1967-01-01

10.1112/plms/s3-38.1.115 article EN Proceedings of the London Mathematical Society 1979-01-01

Quantum matter is everywhere, from the interiors of neutron stars to electrons in everyday metals. Like ordinary, classical matter, it made up many interacting particles. In however, possible think each particle as an individual entity, whereas quantum Heisenberg's uncertainty principle prevents us telling particles apart: their behaviour can only be described collectively. spite this, types are well understood a theoretical point view. For example, "electron liquid" that responsible for...

10.1088/2058-7058/22/06/38 article EN Physics World 2009-06-01

as x ~ , for which many other interesting results in the theory of numbers we are indebted to Chebyshev, has a t racted interest several mathematicians. Revealed posthumously little more than fragment one Chebyshev's manuscripts, theorem was first published and fully proved memoir by Markov 1895 [6], while later same year generalisation Ivanov [4] appeared polynomial n2§ 1 replaced n2+A any positive A (an account both Markov's ' s work is be found Paragraphs 147 149 Landau's Primzahlen [5])....

10.1007/bf02395047 article EN Acta Mathematica 1967-01-01

We describe a collection of interactive animations and visualizations for teaching quantum mechanics. The can be used at all levels the undergraduate curriculum. Each animation includes step-by-step exploration that explains key points. instructor resources are freely available. By using diagnostic survey, we report substantial learning gains students who have worked with animations.

10.1119/1.3657800 article EN American Journal of Physics 2012-01-20

We report the evolution of electronic structure at surface layered perovskite Sr_{2}RuO_{4} under large in-plane uniaxial compression, leading to anisotropic B_{1g} strains ϵ_{xx}-ϵ_{yy}=-0.9±0.1%. From angle-resolved photoemission, we show how this drives a sequence Lifshitz transitions, reshaping low-energy and rich spectrum van Hove singularities that layer hosts. comparison tight-binding modeling, find strain is accommodated predominantly by bond-length changes rather than modifications...

10.1103/physrevlett.130.096401 article EN Physical Review Letters 2023-02-27

10.1515/crll.1988.386.32 article EN Journal für die reine und angewandte Mathematik (Crelles Journal) 1988-05-01

10.1515/crll.1975.274-275.206 article EN Journal für die reine und angewandte Mathematik (Crelles Journal) 1975-05-01

We explore the physics of disordered XYZ spin chain using two complementary numerical techniques: exact diagonalization (ED) on chains up to 17 spins, and time-evolving block decimation (TEBD) 400 spins. Our principal findings are as follows. First, clean shows ballistic energy transport for all parameter values that we investigated. Second, weak disorder there is a stable diffusive region persists critical strength depends XY anisotropy. Third, strengths above this value becomes...

10.1103/physrevb.98.180201 article EN publisher-specific-oa Physical review. B./Physical review. B 2018-11-05

Polar distortions in solids give rise to the well-known functionality of switchable macroscopic polarisation ferroelectrics and, when combined with strong spin-orbit coupling, can mediate giant spin splittings electronic states. While typically found insulators, ferroelectric-like remain robust against increasing itineracy, giving so-called "polar metals". Here, we investigate temperature-dependent structure Ca$_3$Ru$_2$O$_7$, a correlated oxide metal which octahedral tilts and rotations...

10.1073/pnas.2003671117 article EN Proceedings of the National Academy of Sciences 2020-06-23

10.5486/pmd.1965.12.1-4.06 article EN Publicationes Mathematicae Debrecen 2022-07-01

Time evolution in several classes of quantum devices is generated through the application gates. Resetting a critical technological feature these systems allowing for mid-circuit measurement and complete or partial qubit reset. The possibility realizing discrete-time reset dynamics on computers makes it important to investigate steady-state properties such dynamics. Here, we explore behavior generic unitary interspersed by random events. For Poissonian resets, compute stationary state...

10.22331/q-2025-05-13-1742 article EN cc-by Quantum 2025-05-13

We consider a single atom in an optical lattice, subject to harmonic trapping potential. The problem is treated the tight-binding approximation, with extra parameter \kappa denoting strength of trap. It shown that \to 0 limit this singular, sense density states for very shallow trap (\kappa 0) {\it qualitatively different} from translationally invariant lattice = 0). physics difference discussed, and densities wave functions are exhibited explained.

10.1103/physrevlett.93.080404 article EN Physical Review Letters 2004-08-19
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