Related resources
Full-text held externally
- DOI: 10.1038/nature04233
Search for item elsewhere
University researcher(s)
Academic department(s)
Two Dimensional Gas of Massless Dirac Fermions in Graphene
K.S. Novoselov, A.K. Geim, S.M. Morozov, M.I. Katsnelson, I.V. Grigorieva, S.V. Dubonos, A.A. Firsov.
Nature. 2005;438(7065):197-200.
Access to files
Full-text and supplementary files are not available from Manchester eScholar. Full-text is available externally using the following links:
Full-text held externally
- DOI: 10.1038/nature04233
Abstract
Quantum electrodynamics (resulting from the merger of quantum mechanics and relativity theory) has provided a clear understanding of phenomena ranging from particle physics to cosmology and from astrophysics to quantum chemistry1, 2, 3. The ideas underlying quantum electrodynamics also influence the theory of condensed matter4, 5, but quantum relativistic effects are usually minute in the known experimental systems that can be described accurately by the non-relativistic Schrödinger equation. Here we report an experimental study of a condensed-matter system (graphene, a single atomic layer of carbon6, 7) in which electron transport is essentially governed by Dirac's (relativistic) equation. The charge carriers in graphene mimic relativistic particles with zero rest mass and have an effective 'speed of light' c* approximately 106 m s-1. Our study reveals a variety of unusual phenomena that are characteristic of two-dimensional Dirac fermions. In particular we have observed the following: first, graphene's conductivity never falls below a minimum value corresponding to the quantum unit of conductance, even when concentrations of charge carriers tend to zero; second, the integer quantum Hall effect in graphene is anomalous in that it occurs at half-integer filling factors; and third, the cyclotron mass mc of massless carriers in graphene is described by E = mcc*2. This two-dimensional system is not only interesting in itself but also allows access to the subtle and rich physics of quantum electrodynamics in a bench-top experiment.