How can condensed-matter problems interact with field ... - IPMU

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Panel discussion (Wed morning) David Hilbert 1900 Mathematische Probleme (@ Int Cong Mathematicians, Paris) Weyl 1951 CMP meets HEP 2010 LHC (http://press.web.cern.ch/)
Jan 2010, News & Analysis
Page 1 and 2: IPMU Focus Week Feb 2010 "Condensed
Page 3: Hideo Aoki & Hiroshi Ooguri: CMP an
Page 7 and 8: Many worlds understandable --- look
Page 9 and 10: Various phenomena even within gauge
Page 11 and 12: SC Exotic SC: ・ T-rev broken (p+i
Page 13 and 14: Topological phases (as opposed to b
Page 15 and 16: Quantum criticality / strong coupli
Page 17 and 18: Boundary states * Bulk states dicta
Page 19 and 20: SC F FQHE
Page 21 and 22: Y SSB (u k v k = |D(k)|/2E k , s wa
Page 23 and 24: isotropic pairing * phonon mechanis
Page 25 and 26: Hubbard model (a generic model) U /
Page 27 and 28: Cu, Ru compounds Co compound Hf com
Page 29 and 30: Tc in SC from repulsion (if duality
Page 31 and 32: Disconnected Fermi surfaces + + - +
Page 33 and 34: dxz dx2-y2 dyz
Page 35 and 36: First phase-sensitive measurement C
Page 37 and 38: Phase diagram High-Tc Organics (BED
Page 39 and 40: Colour SC in hadron physics μ B ~
Page 41 and 42: electron-phonon Coexisting el-el an
Page 43 and 44: E Ferromagnetism very difficult to
Page 45 and 46: Flat-band ferromagnetism Ferromagne
Page 47 and 48: SC F QHE
Page 49 and 50: FQH liquid Coulomb repulsion + qua
Page 51 and 52: Composite fermion picture N S A ver
Page 53 and 54: Composite-fermion picuture for the
Page 55 and 56:
Various phases in the quantum Hall
Page 57 and 58:
Integer QHE --- Hall conductivity a
Page 59 and 60:
Integer QHE in 3D periodic systems
Page 61 and 62:
Graphene - massless Dirac Weyl neut
Page 63 and 64:
Chirality in graphene H = S c k+ g
Page 65 and 66:
s xy bulk s xy edge Ordinary QHE:
Page 67 and 68:
Dirac particles with randomness ran
Page 69 and 70:
“Massless Dirac” sequence t’
Page 71 and 72:
“Dirac cones” in 3D crystals Bi
Page 73 and 74:
1.QHE (Geim; Kim) Wider Hall effect
Page 75 and 76:
Wave propagation in a circularly po
Page 77 and 78:
Splitting of graphene Landau levels
Page 79 and 80:
Mechanisms for split Landau levels
Page 81 and 82:
FQHE in graphene (Suspended graphen
Page 83 and 84:
Dielectric breakdown Mott`s gap Non
Page 85 and 86:
(Horiguchi et al, 2008)
Page 87:
Summary interaction +0 SC, M, QHE,
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How can condensed-matter problems interact with field ... - IPMU

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