W. G. Unruh
Template:Short description Template:Infobox scientist William George Unruh (Template:IPAc-en;Template:Citation needed born August 28, 1945) is a Canadian physicist at the University of British Columbia, Vancouver who described the hypothetical Unruh effect in 1976.
Early life and educationEdit
Unruh was born into a Mennonite family in Winnipeg, Manitoba. His parents were Benjamin Unruh, a refugee from Russia, and Anna Janzen, who was born in Canada. He obtained his B.Sc. from the University of Manitoba in 1967, followed by an M.A. (1969) and Ph.D. (1971) from Princeton University, New Jersey, under the direction of John Archibald Wheeler.
Areas of researchEdit
Unruh has made seminal contributions to our understanding of gravity,<ref name="Choptuik1986"> Template:Cite journal</ref><ref name="Unruh1989a"> Template:Cite journal</ref> black holes,<ref name="Unruh1976"> Template:Cite journal</ref> cosmology, and quantum fields in curved spaces, including the discovery of what is now known as the Unruh effect. Unruh has contributed to the foundations of quantum mechanics in areas such as decoherence<ref name="Unruh1989b"> Template:Cite journal</ref> and the question of time in quantum mechanics. He has helped to clarify the meaning of nonlocality in a quantum context, in particular that quantum nonlocality does not follow from Bell's theorem and that ultimately quantum mechanics is a local theory.<ref name="Unruh2005"> {{#invoke:citation/CS1|citation |CitationClass=web }}</ref> Unruh is also one of the main critics of the Afshar experiment.<ref name="Unruh2004"> {{#invoke:citation/CS1|citation |CitationClass=web }}</ref>
Unruh is also interested in music and teaches the Physics of Music.
Unruh effectEdit
{{#invoke:Labelled list hatnote|labelledList|Main article|Main articles|Main page|Main pages}} The Unruh effect, described by Unruh in 1976, is the prediction that an accelerating observer will observe black-body radiation where an inertial observer would observe none.<ref name="Unruh1976"/> In other words, the accelerating observer will find itself in a warm background, the temperature of which is proportional to the acceleration. The same quantum state of a field, which is taken to be the ground state for observers in inertial systems, is seen as a thermal state for the uniformly accelerated observer. The Unruh effect therefore means that the very notion of the quantum vacuum depends on the path of the observer through spacetime.
The Unruh effect can be expressed in a simple equation giving the equivalent energy kT of a uniformly accelerating particle (with a being the constant acceleration), as:
- <math> kT = \frac{\hbar a}{2\pi c}</math>