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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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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
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
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
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
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
ˆ
qx //
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
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
Constants of motion
Enlarged (2+1) – Galilei Group
anyons
Central Charges: , ,
‘ =‘ = ‘ =
6D-Orbits:
Local Coord.:
4D-Orbits: Extremum of
Local Coord.:
0*m
eBcrit
1
dYdXeBcrit 2' criteBYX /1,
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,
,ˆ
E
E
txBeqqx jijcycli ,,, 21
( , const unif.)
( , generic)
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
P. Horvathy, L. M., P. Stichel, Mod. Phys. Lett. A 20 (2005), 1177-1185
(in w.f.l.)
3D-Minkowski sp.
d
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
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
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
Future outlook
3r
rbB
B. Basu, S. Ghosh, hep-th/0503263
3k
kg
C. Zang et al , cond-mat/0507125