frustrated antiferromagnets at high fields: bec in degenerate spectra

12
Frustrated Antiferromagnets at High Fields: BEC in Degenerate Spectra George Jackeli In collaboration with: Mike Zhitomirsky PRL 93, 017201 (2004) Institute for Theoretical Physics, EPFL, Lausanne Les Houches, June 2006

Upload: vondra

Post on 21-Jan-2016

27 views

Category:

Documents


0 download

DESCRIPTION

Frustrated Antiferromagnets at High Fields: BEC in Degenerate Spectra. George Jackeli. Institute for Theoretical Physics, EPFL, Lausanne. In collaboration with: Mike Zhitomirsky PRL 93, 017201 (2004). Les Houches, June 2006. √. Summary. Outline. √. - PowerPoint PPT Presentation

TRANSCRIPT

Page 1: Frustrated Antiferromagnets at High Fields:     BEC in Degenerate Spectra

Frustrated Antiferromagnets at High Fields:

BEC in Degenerate Spectra

George Jackeli

In collaboration with: Mike Zhitomirsky

PRL 93, 017201 (2004)

Institute for Theoretical Physics,EPFL, Lausanne

Les Houches, June 2006

Page 2: Frustrated Antiferromagnets at High Fields:     BEC in Degenerate Spectra

Outline

Heisenberg AFM near saturation field: Bose gas analogy

The case of frustration: how to lift the degeneracy

Frustrated Models with lines of minima:

I. J1-J2 AFM at its critical point

II. AFM on FCC lattice

Summary √

Page 3: Frustrated Antiferromagnets at High Fields:     BEC in Degenerate Spectra

AFM near the Saturation Field

H>Hc H<Hc

Mapping to a Bose gas

Page 4: Frustrated Antiferromagnets at High Fields:     BEC in Degenerate Spectra

The Dilute Bose Gas

Effective interaction:

Expansion in gas parameter

Results:

Page 5: Frustrated Antiferromagnets at High Fields:     BEC in Degenerate Spectra

Examples of Frustrated Magnets

Impossible to satisfy simultaneously every pairwise interactions

Geometrical frustration Competing interactions

Infinitely many classical ground states

Degeneracy is typically lifted by “order-out-of-disorder” mechanism: Ordering by fluctuations

By quantum fluctuations:Different zero point energy

By thermal fluctuations:Entropic lowering of free energy

Page 6: Frustrated Antiferromagnets at High Fields:     BEC in Degenerate Spectra

The Case of Frustration

Macroscopic degeneracy below Hc√√ Anomalous spectra above Hc:

Continuous set of minima

Possible way out: Lift the degeneracy dynamically

Locate the minimum of Interaction:

Magnons condense at wv Q at which they less interact

Where do magnons condense?

Page 7: Frustrated Antiferromagnets at High Fields:     BEC in Degenerate Spectra

The Models with Lines of Minima: I. J1-J2 AFM at its critical point

J1>2J2 : Q=(,) J1<2J2 Q=(,)/(,)

Page 8: Frustrated Antiferromagnets at High Fields:     BEC in Degenerate Spectra

J1=2J2Magnon spectrum for

Interaction vertex GS Energy: Nonanalytic

Magnetization Curve: Singular

Single gapless mode

Page 9: Frustrated Antiferromagnets at High Fields:     BEC in Degenerate Spectra

II. AFM on FCC Lattice

Lines of minima at

Magnon spectrum at saturation field

Interaction vertex

Page 10: Frustrated Antiferromagnets at High Fields:     BEC in Degenerate Spectra

GS Energy Magnetization Curve

Single-Q state 3-Q state

GS Energy functional

Page 11: Frustrated Antiferromagnets at High Fields:     BEC in Degenerate Spectra

Temperature vs Field Phase Diagram

Hartree term from Therm. Fluc. Self-consistent gap equation.

Magnetic analog ofWeak Crystallization

Thermal Fluctuations Induce 1st Order Transition

Page 12: Frustrated Antiferromagnets at High Fields:     BEC in Degenerate Spectra

Conclusions

The spectrum has unique Goldstone mode at ordering wv away from it the gap is generated

√ The degeneracy can be lifted dynamically by dressed magnon interaction

√ Singularity in magnetization curve

√ Rich H-T phase diagram