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Phys. Rev. Lett. 80, 1800–1803 (1998)

Quantum-Mechanical Position Operator in Extended Systems

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Raffaele Resta
INFM-Dipartimento di Fisica Teorica, Università di Trieste, Strada Costiera 11, 34014 Trieste, Italy
and Department of Physics, The Catholic University of America, Washington, D.C. 20064

Received 15 September 1997; published in the issue dated 2 March 1998

The position operator (defined within the Schrödinger representation in the standard way) becomes meaningless when periodic boundary conditions are adopted for the wave function, as usual in condensed matter physics. I show how to define the position expectation value by means of a simple many-body operator acting on the wave function of the extended system. The relationships of the present findings to the Berry-phase theory of polarization are discussed.

© 1998 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevLett.80.1800
DOI:
10.1103/PhysRevLett.80.1800
PACS:
03.65.Ca, 03.65.Bz, 71.10.-w, 77.84.-s

See Also

Comment: J. Zak, Comment on “Quantum-Mechanical Position Operator in Extended Systems”, Phys. Rev. Lett. 85, 1138 (2000).