
Andreas Mielke
Institut für Theoretische Physik
RuprechtKarls Universität
Philosophenweg 19
D69120 Heidelberg
Germany
Tel.: ++49 6221 549431 (Sekretariat)
Fax: ++49 6221 549331
email:
mielke@tphys.uniheidelberg.de
Korrelierte Fermionen und Bosonen, Hubbardmodell
Ferromagnetismus ist eine der
am längsten untersuchten Eigenschaften des Hubbardmodell.
Man kann nur für sehr wenige Fälle exakte Resultate
herleiten. Eine große Klasse von Modellen, die
Ferromagnetismus zeigen, sind Modelle mit mehreren Bändern,
von denen eines dispersionslos ist. Diesen sogenannten
flat band Ferromagnetismus haben wir seit 1991
ausführlich untersucht.
In den letzten Jahren konnten diese Resultate auf
Modelle mit einem teilweise flachen Band verallgemeinert werden.
Dies eröffnet einen möglichen Weg zu metallischem Ferromagnetismus
im Hubbardmodell.
Wechselwirkende Bosonen in Strukturen mit flachen Bändern zeigen eine Reihe
von interessanten Phänomenen, u.a. die Bildung eines Wignerkristalls und Paarbildung.
Ausgewählte Publikationen aus diesem Gebiet
Moritz Drescher, Andreas Mielke: Hardcore bosons in flat band systems above the critical density
Eur. Phys. J. B90,
217
(2017)
.
Abstract:We investigate the behaviour of hardcore bosons in one and twodimensional flat band systems, the chequerboard and the kagom\'e lattice and onedimensional analogues thereof. The one dimensional systems have an exact local reflection symmetry which allows for exact results. We show that above the critical density an additional particle forms a pair with one of the other bosons and that the pair is localised. In the twodimensional systems exact results are not available but variational results indicate a similar physical behaviour.
Andreas Mielke: Pair formation of hard core bosons in flat band systems
preprint arXiv:1708.02508,
(2017)
.
Abstract:Hard core bosons in one or two dimensional flat band systems have an upper critical density, below which the ground states can be described completely. At the critical density, the ground states are Wigner crystals. If one adds a particle to the system at the critical density, the ground state and the low lying multi particle states of the system can be described as a Wigner crystal with an additional pair of particles. The energy band for the pair is separated from the rest of the spectrum. The proofs use a Gerschgorin type of argument for block diagonally dominant matrices. In certain onedimensional structures one can show that the pair is localised and that the energy band is flat except at the boundaries of the system.
Petra Pudleiner, Andreas Mielke: Interacting bosons in twodimensional flat band systems
Eur. Phys. J. B88,
207
(2015)
.
Abstract:The Hubbard model of bosons on two dimensional lattices with a lowest flat band is discussed. In these systems there is a critical density, where the ground state is known exactly and can be represented as a charge density wave. Above this critical filling, depending on the lattice structure and the interaction strength, the additional particles are either delocalised and condensate in the ground state, or they form pairs. Pairs occur at strong interactions, e.g., on the chequerboard lattice. The general mechanism behind this phenomenon is discussed.
Andreas Mielke: Properties of Hubbard models with degenerate localised single particle eigenstates
Eur. Phys. J. B85,
(2012)
.
Abstract:We consider the repulsive Hubbard model on a class of lattices or graphs for which there is a large degeneracy of the single particle ground states and where the projector onto the space of single particle ground states is highly reducible. This means that one can find a basis in the space of the single particle ground states such that the support of each single particle ground state belongs to some small cluster and these clusters do not overlap. We show how such lattices can be constructed in arbitrary dimensions. We construct all multiparticle ground states of these models for electron numbers not larger than the number of localised single particle eigenstates. We derive some of the ground state properties, esp. the residual entropy, i.e. the finite entropy density at zero temperature.
Johannes Motruk, Andreas Mielke: BoseHubbard model on twodimensional line graphs
J. Phys. A: Math. Gen45,
225206
(2012)
.
Abstract:We construct a basis for the manyparticle ground states of the positive hopping BoseHubbard model on line graphs of finite 2connected planar bipartite graphs at sufficiently low filling factors. The particles in these states are localized on nonintersecting vertexdisjoint cycles of the line graph which correspond to nonintersecting edgedisjoint cycles of the original graph. The construction works up to a critical filling factor at which the cycles are closepacked.
Andreas Mielke: Ferromagnetism in single band Hubbard models with a partially flat band
Phys. Rev. Lett.82,
43124315
(1999)
.
Abstract:A Hubbard model with a single, partially flat band has ferromagnetic ground states. It is shown that local stability of ferromagnetism implies its global stability in such a model: The model has only ferromagnetic ground states if there are no single spinflip ground states. Since a singleband Hubbard model away from half filling describes a metal, this result may open a route to metallic ferromagnetism in single band Hubbard models.
Andreas Mielke: Stability of ferromagnetism in Hubbard models with degenerate singleparticle ground states
J. Phys. A, Math. Gen.32,
84118418
(1999)
.
Abstract:A Hubbard model with a \( N_{d} \)fold degenerate singleparticle ground state has ferromagnetic ground states if the number of electrons is less or equal to \( N_{d} \). It is shown rigorously that the local stability of ferromagnetism in such a model implies global stability: The model has only ferromagnetic ground states, if there are no single spinflip ground states. If the number of electrons is equal to \( N_{d} \), it is well known that the ferromagnetic ground state is unique if and only if the singleparticle density matrix is irreducible. We present a simplified proof for this result.
Andreas Mielke: Ferromagnetism in the Hubbard model and Hund's rule
Phys. Lett. A174,
443448
(1993)
.
Abstract:We investigate the Hubbard model with a $N_{\rm d}$fold degenerate single particle ground state. If the number of electrons satisfies $N_{\rm e}<N_{\rm d}$, the model has ferromagnetic multiparticle ground states. We give a necessary and sufficient condition for the ground state to be unique $N_{\rm e}=N_{\rm d}$. It is ferromagnetic with spin $S=\frac12N_{\rm e}$. As a corollary, we obtain Hund's rule for the general Hubbard model with degenerate single particle eigenstates on translationally invariant lattices in the special case, where each of the degenerate single particle states if filled with one electron.
Andreas Mielke, Hal Tasaki: Ferromagnetism in the Hubbard model  Examples from Models with Degenerate SingleElectron Ground States
Commun. Math. Phys.158,
341371
(1993)
.
Abstract:Whether spinindependent Coulomb interaction can be the origin of a realistic ferromagnetism in an itinerant electron system has been an open problem for a long time. Here we study a class of Hubbard models on decorated lattices, which have a special property that the corresponding singleelectron Schrödinger equation has $N_{\rm d}$fold degenerate ground states. The degeneracy $N_{\rm d}$ is proportional to the total number of sites $\abs{\Lambda}$. We prove that the ground states of the models exhibit ferromagnetism when the electron filling factor is not more than and sufficiently close to $\rho_0=N_{\rm d}/(2\abs{\Lambda})$, and paramagnetism when the filling factor is sufficiently small. An important feature of the present work is that it provides examples of three dimensional itinerant electron systems which are proved to exhibit ferromagnetism in a finite range of the electron filling factor.
Abstract:The author gives a complete and rigorous description of the ground states of the Hubbard model on the Kagome lattice for electron densities n>or=5/3 and U>0. If 11/6>n>or=5/3 the system shows a ferromagnetic behaviour at zero temperature. If n is above 11/6 the system is paramagnetic. The proof of these results uses some graphtheoretic methods. The results are applicable to all line graphs of planar lattices, of which the Kagome lattice is an example.
Abstract:The author investigates the U= infinity Hubbard model on a large class of lattices which are line graphs. The most interesting lattices in this class are line graphs of regular bipartite lattices with Ns sites and coordination number k>or=4. The ground state energy and some ground states are given. If the number of electrons N satisfies Ns>or=N>or=2Ns/k2, the ground state energy is 4 mod t mod (NsN). The ground states have no magnetic ordering, they are projections of the ground states at U=0 onto the subspace of states without doubly occupied sites.
Andreas Mielke: Ferromagnetic ground states for the Hubbard model on line graphs
J. Phys. A: Math. Gen.24,
L73L77
(1991)
.
Abstract:The author discusses some of the properties of the Hubbard model on a line graph with n vertices. It is shown that the model has ferromagnetic ground states if the interaction is repulsive (U)0) and if the number of electrons N satisfies 2n>or=N>or=M. M is a natural number that depends on the line graph. For example, the Kagome lattice is a line graph, it has M=5n/31.
Andreas Mielke: Ferromagnetism in the Hubbard model on line graphs and further considerations
J. Phys. A: Math. Gen.24,
33113321
(1991)
.
Abstract:Let L(G) be the line graph of a graph G=(V,E). The Hubbard model on L(G) has ferromagnetic ground states with a saturated spin if the interaction is repulsive (U>0) and if the number of electrons N satisfies N>or=M. M= mod E mod + mod V mod 1 if G is bipartite and M= mod E mod + mod V mod otherwise. The author shows that the ferromagnetic ground state is unique if N=M. Further he gives a sufficient condition for the existence of other ground states if N>M. The results are valid also for a multiband Hubbard model on a bipartite graph. In the case of a periodic lattice, the results are related to the existence of a flat energy band.
Letzte Änderung: 16.3.2018.
mielke@tphys.uniheidelberg.de
