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Semiclassical dynamics of wave - packets in generalized mechanics ine iclassical Approximations in Condensed Matter Physics ry Phase in Cond. Matt. amical Systems for Wave Packets: Hamiltonian and Lagrangian formulat metries Papers: P. Horvathy, L. M., P. Stichel, Phys. Lett B 615 (2005), 87-92 P. Horvathy, L. M., P. Stichel, Mod. Phys. Lett. A 20 (2005), 1177-1185 C. Duval, Z. Horvath, P. A. Horvathy, L. M., P.Stichel, Mod. Phys. Lett. B. 20 No. 7 (2006) 373-378 L. Martina, Fundam. Appl. Math. 12 (2006), 109-118

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Semiclassical dynamics of wave - packets in generalized mechanics. Outline Semiclassical Approximations in Condensed Matter Physics Berry Phase in Cond. Matt. Dynamical Systems for Wave Packets: Hamiltonian and Lagrangian formulations Symmetries. Papers: - PowerPoint PPT Presentation

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Page 1: Semiclassical dynamics of wave - packets in generalized mechanics

Semiclassical dynamics of wave - packets in generalized mechanics

Outline

•Semiclassical Approximations in Condensed Matter Physics•Berry Phase in Cond. Matt.•Dynamical Systems for Wave Packets: Hamiltonian and Lagrangian formulations•Symmetries

Papers: P. Horvathy, L. M., P. Stichel, Phys. Lett B 615 (2005), 87-92P. Horvathy, L. M., P. Stichel, Mod. Phys. Lett. A 20 (2005), 1177-1185C. Duval, Z. Horvath, P. A. Horvathy, L. M., P.Stichel, Mod. Phys. Lett. B. 20 No. 7 (2006) 373-378L. Martina, Fundam. Appl. Math. 12 (2006), 109-118

Page 2: Semiclassical dynamics of wave - packets in generalized mechanics

Lattice constant

Wave – length of the modulations

x

xc

“Periodic” Hamiltonian Op.(xc)

Bloch Theory

txuex qnxqi

qn ,

xulxu qnqn

txtxpxH r ,ˆ,,,ˆ,ˆ,ˆ 1

2..,ˆˆ2

1ˆc

icixccc xxOchtxHxxHH

c

txtxpxHtxH crccc ,,,,,ˆ,ˆ,ˆ1

qnccnqncc tqxEtxH ,,,ˆ tqxE ccn ,,

Sundaram,Niu, Phys.Rev. B (1999)

xxc

,0,,,,1 tqxEtqxEE ccnccngapn

,gapn

pert E

hT

Dispersion of the w-p

gappert q

hL

Im

Page 3: Semiclassical dynamics of wave - packets in generalized mechanics

IBZ

cqn txtqaqd ,,

1

2, tqaqqdtqc

c

c qcellqnqqnqqc xuxutqatx

,arg

cell

qnqqnnnqqnqn txuitxuqqqqix ,,''ˆ'''

lattlq

1

cccc

ccjiji

qqccqxccc

qxqyqzqzqyijccyz

uHEutqxEE

uuuuitqx

~ˆIm,,

,,,

n fixed

txcxqcxxxc

tqcqqcqxqc

tqtxEtq

tqtxEtx

c

c

U(1) - Berry connection

Berry – curvature

Page 4: Semiclassical dynamics of wave - packets in generalized mechanics

Modulation by EM f.

txeAtxAepxHH ,ˆ,ˆˆ,ˆˆ0

txtqxMtxtxBtxetq

tqxqtxtqxMtqxEtx

cccxcccc

cccccccccqc

c

c

,,,,,

,,,,,,,

BE

B

cqqqcellcqqcc

cccccijqqijkcci

uHEuetqxM

txAeqEtqxEtqx

ˆIm,,

,,,,2

1,, 00

Anomalous Hall Effect (Karplus-Luttinger, Phys. Rev. (1954)

xyqqxqqqqy eqΕuHuv

y E

0

24

2

0

2 eqdEf

e

IBZ

FDxyqqxy Thouless et al, Phys. Rev. Lett. 82

GaAs, ferro-, Antiferro- crystals

Chern numbers

Page 5: Semiclassical dynamics of wave - packets in generalized mechanics

2D - Model

xyqqijicell

qnqqn

c

qtxuitxu

MtxAem

qtqxE

j,

2,,

0,,2

,, 0

2

qqtxAxtxAem

qxqLDH

2

,,2 0

2

ijijtxBemm ˆ,0,1*

qdqdm

xdxdB

dtqxddteqdmDH

22

2 E

00 Bd tDH E

C. Duval,P. Horvathy Phys. Lett B479 (2000)284 DHKer

22

220 mm

L LSZ

txextxeBq

txemqxm

,ˆ,

,ˆ*

E

E

J. Lukierski, P.C. Stichel, W.J. Zakrzewski, Ann. Phys. (1997)

22

0

2

1QQQL DH

Qx

qQ

ˆ

qx //

Page 6: Semiclassical dynamics of wave - packets in generalized mechanics

Hamiltonian Structure

ijjiijjiijji txeBm

mqq

m

mqx

m

mxx ,

*,,

*,,

*,

txAem

qH ,

2 0

2

Canonical Variables

XeB

qm

mQq

m

m

eBxX

ˆ

2

*,ˆ

*1

1

B = const

eBm crit

10*

*1,,

2*221

0

2

m

mtQ

BXAe

m

XeBQH

jiijjiijjiB dxdxBe

dqdqdxdq 22

2

*det

m

m

Page 7: Semiclassical dynamics of wave - packets in generalized mechanics

J. Negro, MA del Olmo, J. Math. Phys. 31 (1990) 2811,P. Horvathy et al Phys. Lett B 615 (2005), 87-92

tkkrtrtrAem

krk

tLL DHB

Enl

EE

E

2,

2

2

ret

tereBktemkrm

,0

ˆ,ˆ*

E

EE

Page 8: Semiclassical dynamics of wave - packets in generalized mechanics

Constants of motion

Enlarged (2+1) – Galilei Group

anyons

Central Charges: , ,

Page 9: Semiclassical dynamics of wave - packets in generalized mechanics

‘ =‘ = ‘ =

Page 10: Semiclassical dynamics of wave - packets in generalized mechanics

6D-Orbits:

Local Coord.:

4D-Orbits: Extremum of

Local Coord.:

0*m

eBcrit

1

dYdXeBcrit 2' criteBYX /1,

Page 11: Semiclassical dynamics of wave - packets in generalized mechanics

Enlarged symmetry

Anomalous couplings

V.P. Nair, A.P. Policronakos, Phys. Lett B 505 (2001)

ijjiijjiijji eBqqqxxx ,,,,,

txAem

qH ,

2 0

2

txeqm

txeBq

txemqxm

,ˆ,

E

E

txBeqqx jijcycli ,,, 21

( , const unif.)

( , generic)

Page 12: Semiclassical dynamics of wave - packets in generalized mechanics

Coadjoint Orbits

The gyromagnetic problem

A free relativistic particle in the plane Unitary representations of the planar Lorentz algebra 1,2o

1,2SO

L. Feher, PhD Thesis (1987)J. Negro, A.M. del Olmo, J. Tosiek math-ph/0512007 2D analog Pauli-Lubanski 4-vec

mc

kpjmcs

R. Jackiw, V.P. Nair, Phys. Lett B 480 (2000)237 2200 , m

c

sB

C. Chou, V.P. Nair, A. Polychronakos, Phys. Lett B304 (1993)105

2g

D.K. Maude et al., Phys. Rev. Lett. 77 (1996) 4604D.R. Leadley et al., Phys. Rev. Lett. 79 (1997) Experimental evidence 0g

CNP

Page 13: Semiclassical dynamics of wave - packets in generalized mechanics

P. Horvathy, L. M., P. Stichel, Mod. Phys. Lett. A 20 (2005), 1177-1185

(in w.f.l.)

3D-Minkowski sp.

d

Page 14: Semiclassical dynamics of wave - packets in generalized mechanics

ijji

ijji

ijji

eBm

mkk

Bkemm

mkr

km

mrr

*,

1*,*

,

,*

,

General Model for Bloch electrons

2D

2k

D. Culcer et al. Phys. Rev. B 68 (2003) 045327, zincoblende

Restricted orbits

Page 15: Semiclassical dynamics of wave - packets in generalized mechanics

3D

0,0 Brk

dkm

mu

* dkm

mx

uv

*1

0 vuut fvvvu t

m

m*

0*m 0 uB

uX

critt

E B

vE

Page 16: Semiclassical dynamics of wave - packets in generalized mechanics

Conclusions•Semiclassical dynamics of electron in crystals involves Berry phase effects•They are Hamiltonian systems •Enlarged formulations allows to embody the presence of external fields•In 2D the Enlarged – two folded Galilei Group symmetry defines the “exotic”free model DH•The exotic charge has a physical realization (constant Berry curvature)•The group orbit method has been used to describe the phase space and its singular foliations•Anomalous gyromagnetic effects can be considered by simple generalizations•The exotic model (g=0) is not a relativistic limit of relativistic anyons.•The anomalous gyromagnetic problem can be addressed for relativistic anyons,by a non-standard S·F contribution to the mass. •Hamiltonian formulation, both in 2D and 3D, of semiclassical electron wave packetsis provided. •Symmetry analysis and restricted Hall motions are characterized. •Boltzmann equation for 1 “exotic” particle distribution f. and is written.•Fluid equations

Page 17: Semiclassical dynamics of wave - packets in generalized mechanics

Future outlook

3r

rbB

B. Basu, S. Ghosh, hep-th/0503263

3k

kg

C. Zang et al , cond-mat/0507125