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Towards the fractional quantum Hall effect : a noncommutative geometry perspective (2005)

by M Marcolli, V Mathai
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A WALK IN THE NONCOMMUTATIVE GARDEN

by Alain Connes, Matilde Marcolli
"... 2. Handling noncommutative spaces in the wild: basic tools 2 3. Phase spaces of microscopic systems 6 4. Noncommutative quotients 9 ..."
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2. Handling noncommutative spaces in the wild: basic tools 2 3. Phase spaces of microscopic systems 6 4. Noncommutative quotients 9
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...ying geometry to account for an average effect of the multi-electron interactions. One can obtain this way a model of the fractional quantum Hall effect via noncommutative geometry (cf. [152], [153], =-=[154]-=-), where one uses hyperbolic geometry to simulate the interactions. The noncommutative geometry approach to the quantum Hall effect described above was extended to hyperbolic geometry in [37]. The ana...

Spin-Hall effect with quantum group symmetry

by Giovanni Landi - Lett. Math. Phys , 2006
"... We construct a model of spin-Hall effect on the noncommutative sphere S 4 θ with isospin degrees of freedom (coming from a noncommutative instanton) and invariance under a quantum group SOθ(5). The corresponding representation theory allows to explicitly diagonalize the Hamiltonian and construct the ..."
Abstract - Cited by 7 (3 self) - Add to MetaCart
We construct a model of spin-Hall effect on the noncommutative sphere S 4 θ with isospin degrees of freedom (coming from a noncommutative instanton) and invariance under a quantum group SOθ(5). The corresponding representation theory allows to explicitly diagonalize the Hamiltonian and construct the ground state; there are both integer and fractional excitations. Similar models exist on higher dimensional spheres S N Θ and projective spaces CPN Θ.
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...echniques from noncommutative geometry played a crucial role in the analysis of [2] of the integer quantum Hall effect. For a noncommutative approach to the fractional quantum Hall effect we refer to =-=[19]-=-. 2 Noncommutative spheres Toric noncommutative manifolds MΘ were constructed and studied in [9]. One starts with any (Riemannian spin) manifold M carrying a torus action and then deforms the torus to...

Solvmanifolds and Noncommutative Tori with Real Multiplication

by Matilde Marcolli
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On twisted Fourier analysis and convergence of Fourier series on discrete groups

by Erik Bédos, Roberto Conti , 2006
"... We study convergence and summation processes of Fourier series in reduced twisted group C ∗-algebras of discrete groups. ..."
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We study convergence and summation processes of Fourier series in reduced twisted group C ∗-algebras of discrete groups.
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...as seem often to require the development of new methods to deal with, but even unavoidable for instance when dealing with the study of electrons in solids when a magnetic field is turned on (see e.g. =-=[8, 9, 64]-=-). Twisted group algebras associated with discrete groups may also be viewed as twisted compact quantum groups, being the twisted dual objects to the discrete groups themselves. The basic examples in ...

Singularities, swallowtails and Dirac points. An analysis for families of Hamiltonians and applications to wire networks, especially the Gyroid

by Ralph M. Kaufmann, Sergei Khlebnikov, Birgit Wehefritz–kaufmann - Annals of Physics , 2012
"... Abstract. Motivated by the Double Gyroid nanowire network we develop methods to detect Dirac points and classify level crossings, aka. singularities in the spectrum of a family of Hamiltonians. The approach we use is singularity theory. Using this language, we obtain a characterization of Dirac poin ..."
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Abstract. Motivated by the Double Gyroid nanowire network we develop methods to detect Dirac points and classify level crossings, aka. singularities in the spectrum of a family of Hamiltonians. The approach we use is singularity theory. Using this language, we obtain a characterization of Dirac points and also show that the branching behavior of the level crossings is given by an unfolding of An type singularities. Which type of singularity occurs can be read off a characteristic region inside the miniversal unfolding of an Ak singularity. We then apply these methods in the setting of families of graph Hamiltonians, such as those for wire networks. In the particular case of the Double Gyroid we analytically classify its singularities and show that it has Dirac points. This indicates that nanowire systems of this type should have very special physical properties.
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...type of analysis explicit in the non–commutative geometry language. There should be some kind of characteristic classes and parings much like in the setting of the quantum Hall effect as presented in =-=[14,15]-=-. Acknowledgments RK thankfully acknowledges support from NSF DMS-0805881. BK thankfully acknowledges support from the NSF under the grant PHY0969689. Any opinions, findings and conclusions or recomme...

The geometry of the double gyroid wire network: quantum and classical

by Ralph M. Kaufmann, Sergei Khlebnikov, Birgit Wehefritz–kaufmann - Journal of Noncommutative Geometry , 2012
"... Abstract. Quantum wire networks have recently become of great interest. Here we deal with a novel nano material structure of a Double Gyroid wire network. We use methods of commutative and non-commutative geometry to describe this wire network. Its non–commutative geometry is closely related to non- ..."
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Abstract. Quantum wire networks have recently become of great interest. Here we deal with a novel nano material structure of a Double Gyroid wire network. We use methods of commutative and non-commutative geometry to describe this wire network. Its non–commutative geometry is closely related to non-commutative 3-tori as we discuss in detail.
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...utative geometric properties. The underlying geometry in that situation is the quantum 2-torus. Recently there have been further analyses on the fractional effect using hyperbolic geometry as a model =-=[15]-=-. The conceptual approach as outlined in [2] is to replace the Brillouin zone by a non–commutative Brillouin zone which is given by a C∗–algebra that contains the translational symmetry operators and ...

The algebraic geometry of Harper operators

by Dan Li
"... ar ..."
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NONCOMMUTATIVE GEOMETRY AND ARITHMETIC

by Matilde Marcolli
"... This is an overview of recent results aimed at developing a geometry of noncommutative tori with real multiplication, with the purpose of providing a parallel, for real quadratic fields, of the classical theory of elliptic curves with complex multiplication for imaginary quadratic fields. This talk ..."
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This is an overview of recent results aimed at developing a geometry of noncommutative tori with real multiplication, with the purpose of providing a parallel, for real quadratic fields, of the classical theory of elliptic curves with complex multiplication for imaginary quadratic fields. This talk concentrates on two main aspects: the relation of Stark numbers to the geometry of noncommutative tori with real multiplication, and the shadows of modular forms on the noncommutative boundary of modular curves, that is, the moduli space of noncommutative tori.
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...s especially useful in the noncommutative geometry models of the integer quantum Hall effect, where this noncommutative space replaces the Brillouin zone in the presence of a magnetic field, see [3], =-=[43]-=-. 3. L-functions, solvmanifolds, and noncommutative tori I give an overview here of recent progress in understanding the geometry of a special class of noncommutative tori, which have real multiplicat...

8. Shimizu L-function and Lorentzian geometry 28

by unknown authors
"... 6. Twisted index theorem, K-theory, and the range of the trace 16 ..."
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6. Twisted index theorem, K-theory, and the range of the trace 16
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...]). We recall briefly the definition and properties of twisted group C ∗ -algebras, as this will be useful in the following. For a similar overview and applications to the case of Fuchsian groups see =-=[20]-=-.SOLVMANIFOLDS AND NC TORI 9 4.1. Twisted group algebras. Let Γ be a finitely generated discrete group, and let σ : Γ × Γ → U(1) be a multiplier, that is, a 2-cocycle satisfying the cocycle property ...

TWISTED INDEX THEORY ON ORBIFOLD SYMMETRIC PRODUCTS AND THE FRACTIONAL QUANTUM HALL EFFECT

by Matilde Marcolli, Kyle Seipp
"... Abstract. We extend the noncommutative geometry model of the fractional quantum Hall effect, previously developed by Mathai and the first author, to orbifold symmetric products. It retains the same properties of quantization of the Hall conductance at integer multiples of the fractional Satake orbif ..."
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Abstract. We extend the noncommutative geometry model of the fractional quantum Hall effect, previously developed by Mathai and the first author, to orbifold symmetric products. It retains the same properties of quantization of the Hall conductance at integer multiples of the fractional Satake orbifold Euler characteristics. We show that it also allows for interesting composite fermions and anyon representations, and possibly for Laughlin type wave functions. 1.
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...sponding to cn ∈ H2(Γ)⊕n ⊂ H2(Γn), and n!(#G) n = #Gn. The case (6.2), without the cyclic cocycle c, computes the range of the trace on K-theory, which is useful for gap labelling purposes, see [49], =-=[51]-=-. Here we focus on the higher version with the cyclic cocycle, as that will provide the quantization of the Hall conductance as in [51]. Lemma 6.2. Let E be an orbifold vector bundle over the good 2-d...

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