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B. Spivak, UW with S. Kivelson, Stanford

B. Spivak, UW with S. Kivelson, Stanford

2D electronic phases intermediate between the Fermi liquid and the Wigner crystal (electronic micro-emulsions). B. Spivak, UW with S. Kivelson, Stanford. Electron interaction can be characterized by a parameter r s =E pot /E kin.

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786 views • 61 slides
B. Spivak, UW with S. Kivelson, Stanford

B. Spivak, UW with S. Kivelson, Stanford

2D electronic phases intermediate between the Fermi liquid and the Wigner crystal (electronic micro-emulsions). B. Spivak, UW with S. Kivelson, Stanford. Electron interaction can be characterized by a parameter r s =E pot /E kin.

★ ★ ★ ★ ★

621 views • 61 slides
B. Spivak, UW S. Kivelson, Stanford

B. Spivak, UW S. Kivelson, Stanford

2D electronic phases intermediate between the Fermi liquid and the Wigner crystal (electronic micro-emulsions). B. Spivak, UW S. Kivelson, Stanford. Conclusion :. There are pure 2D electron phases which are intermediate between the Fermi liquid

★ ★ ★ ★ ★

696 views • 57 slides
B. Spivak, UW S. Kivelson, Stanford

B. Spivak, UW S. Kivelson, Stanford

2D electronic phases intermediate between the Fermi liquid and the Wigner crystal (electronic micro-emulsions). B. Spivak, UW S. Kivelson, Stanford. Conclusion :. There are pure 2D electron phases which are intermediate between the Fermi liquid

★ ★ ★ ★ ★

584 views • 57 slides
B. Spivak, UW S. Kivelson, Stanford, S. Sondhi, D. Huse, C. Lamman, Princeton

B. Spivak, UW S. Kivelson, Stanford, S. Sondhi, D. Huse, C. Lamman, Princeton

2D microemulsion phases in Bose and Fermi systems with dipolar interaction . B. Spivak, UW S. Kivelson, Stanford, S. Sondhi, D. Huse, C. Lamman, Princeton. interaction energy can be characterized by a parameter

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389 views • 29 slides

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