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Hidden order in URu2Si2 originates from Fermi surface gapping induced by dynamic symmetry breaking

Elgazzar, S (author)
Uppsala universitet,Institutionen för fysik och materialvetenskap
Rusz, Jan (author)
Uppsala universitet,Institutionen för fysik och materialvetenskap
Amft, Martin (author)
Uppsala universitet,Institutionen för fysik och materialvetenskap
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Oppeneer, Peter M. (author)
Uppsala universitet,Institutionen för fysik och materialvetenskap
Mydosh, J. A. (author)
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 (creator_code:org_t)
2009
2009
English.
In: Nature Materials. - 1476-1122 .- 1476-4660. ; 8:4, s. 337-341
  • Journal article (peer-reviewed)
Abstract Subject headings
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  • Spontaneous, collective ordering of electronic degrees of freedom leads to second-order phase transitions that are characterized by an order parameter driving the transition. The notion of a 'hidden order' has recently been used for a variety of materials where a clear phase transition occurs without a known order parameter. The prototype example is the heavy-fermion compound URu2Si2, where a mysterious hidden-order transition occurs at 17.5 K. For more than twenty years this system has been studied theoretically and experimentally without a firm grasp of the underlying physics. Here, we provide a microscopic explanation of the hidden order using density-functional theory calculations. We identify the Fermi surface 'hot spots' where degeneracy induces a Fermi surface instability and quantify how symmetry breaking lifts the degeneracy, causing a surprisingly large Fermi surface gapping. As the mechanism for the hidden order, we deduce spontaneous symmetry breaking through a dynamic mode of antiferromagnetic moment excitations.

Subject headings

NATURVETENSKAP  -- Fysik (hsv//swe)
NATURAL SCIENCES  -- Physical Sciences (hsv//eng)

Keyword

Physics
Fysik

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Elgazzar, S
Rusz, Jan
Amft, Martin
Oppeneer, Peter ...
Mydosh, J. A.
About the subject
NATURAL SCIENCES
NATURAL SCIENCES
and Physical Science ...
Articles in the publication
Nature Materials
By the university
Uppsala University

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