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Gauge invariance and topological order in quantum many-particle systems
오시가와 마사기(Masaki Oshikawa)
동경공대(Tokyo Institute of Technology)
2005 년 10 월 28 일 @ 한국고등과학원
Commensurability and Luttinger’s theorem implications of (fractional) particle density (“old” stuffs)
Ground-state degeneracy and topological order what is the topological order and when do we find it? (more recent developments)
Quantum phases and transitions (at T=0)ga
p Phase I
Phase II
critical point (gapless)
Typical example: Ising model with a transverse field in d-dim. (equivalent to classical Ising in (d+1)-dim.)
ordered phase disordered phase
Renormalization Group
Critical point = gapless
RG fixed point
There is always a relevant perturbation!
We have to fine-tune the coupling to achieve the criticality
However ……. there are many gapless systems in cond-mat physics, without any apparent fine-tuning! solids, metals, etc. ……
Why is the gapless phase “protected”?
Nambu-Goldstone theorem: gapless excitations exist if a continuous symmetry is spontaneously broken explains gapless phonons in solids but what about metals?? Let’s seek a new mechanism……
Magnetization process of an antiferromagnet
(at T=0 )
classical picture
H
magnetization curve
H
msaturation
Magnetization process in quantum antiferromagnets
Long history of study
Exact magnetization curve for S=1/2 Heisenberg antiferromagnetic chain (Bethe Ansatz exact solution)
Quantitave difference from classical case
No qualitative difference??
New feature in the quantum case
Shiramuraet al. (1998)[H. Tanaka group,Tokyo Inst. Tech.]
H
mmagnetizationplateau
difficult to understand in classical picture!
Quantization condition for a plateau:
n : # of spins per unit cell of the groundstateS : spin quantum number
(M.O.-Yamanaka-Affleck ’97)
T=0
10
Understanding the quantum magnetization process
At T=0, the system should be in the ground state
magnetization curve = magnetization of the ground state for the Hamiltonian (which depends on the magnetic field)
Hamiltonian:
Magnetic field(Zeeman term)
Exchange interaction (typical example)
Let us assume that the interaction is invariant under the rotation about z-axis (direction of the applied field)
We can choose simultaneous eigenstates of
and
They are also always eigenstates of
no change in the eigenstates even if the magnetic field is changed!
how does the ground-state magnetization increase by the magnetic field?
E
H
lowest energystate with
lowest energy state with
g.s. magnetization = M M+1
plateau of width
gap
For any (finite size) quantum magnet (with the axial symmetry)the magnetization curve at T=0 consistsof plateaus and steps!
In the thermodynamic limit (infinite system size)
“gapless” ( ! 0 above the ground state) : smooth magnetization curve
“gapful” ( remains finite above the g.s.): plateau
H
T=0
gapful!
gaplessm
when can the quantum magnet be gapful?
gapful phases are rather “special”!
Quantum magnet as a many-particle system
e.g. consider S=1/2
“down”
“up” empty site
occupied by a particle
particle hopping
interaction
particle creation op.annihilation op.
When can the quantum many-particle system on a lattice be gapful?
usually, particles can move around, giving gapless (arbitrary low-energy) excitations
A finite excitation gap may appear if the particles are “locked” by the lattice to form a stable ground state. (particles are then mobilized only by giving an energy
larger than the gap.)
To have the particles “locked”, the density of the particles must be commensurate with the lattice.
1 particle/ unit cell (= 2 sites)
add extra particles (“doping”)
mobile carriers
commensurate density
particle density (# of particle/site)# of sites/ unit cell of the g.s.
# of particles/unit cell of the g.s.
particles may be “locked” to forman insulator, with a finite gap
incommensurate densityparticles are mobile,forming a conductor withgapless excitations
20
(possibly with SSB of translation symmetry ---- will come back on this later)
Finite-temperature transition near the plateau
magnetization//H vs. T
MFT
T
m
Magnon BEC picture Tsuneto-Murao 1971 ...........Nikuni et al. 2000
singlet on dimer
(lowest) triplet on dimer
vacuum
magnon (boson)
magnetic field chemical potential
ordering transition magnon BEC
Dispersion: (near the bottom)
Consequences of the BEC picturecondensed magnons
Quantum spin system in a field = “particles” with a tunable chemical potential
Nikuni, MO, Oosawa, Tanaka 2000
Back to the quantization…..
e.g. consider S=1/2
“down”
“up” empty site
occupied by a particle
commensurability condition
Is it really true?physical properties of the system (such as magnetization curve): generally depends on Hamiltonian
ground state in strongly interacting system: very complicated!
why would the commensurability condition be valid in strongly interacting systems??
d=1A generalization of Lieb-Schultz-Mattis argument (1961) shows
There are q degenerate groundstates if = p/q and if the system has a gap
(M.O.-Yamanaka-Affleck, 1997)d ¸ 2
Topological argument (with assumptions)
Relation to Drude/Kohn argument
Rigorous proofs
(M.O. 2000)
(M.O. 2003)
(Hastings 2004, 2005)
Insulator vs. conductorLinear response theory
Drude weight
D=0 : insulatorD>0 : conductor
(Kohn, 1963)
Real-time formulation of Dinitial condition: ground state at t=0
taking t! 1, T ! 1
(as long as the linear response theory is valid)
circumference:
E
uniform electric field
cf. Laughlin (1981)
energy gain
30
(unit flux quantum)choose
and take the limit
Hamiltonian at t=T with the unit flux quantum is equivalent to that at t=0 with =0
Does the groundstate go back to the groundstate?
If so, the energy gain =0 thus the system is an insulator
(no Aharonov-Bohm effect)
No change in the momentum?!As long as we choose constant-A gauge, Hamiltonian is translational invariant.
Momentum is gauge-dependent!!
large gauge transf.
To compare the momentum, we compare
and
lattice translation operator
cross section
Total momentum change (after large gauge tr.)
and has same momentum
(Lieb-Schultz-Mattis, 1961)
Momentum Px is defined modulo 2
The final state must be different from the initial state (g.s.) if Z (for appropriate C)
In order to have an insulator for an incommensurate particle density Z, one must have low-energy state with the extra momentum
1 dim. 2dim.:
3 dim. and higher: no constraint from D=0
(M.O. 2003)
Application to gapless system
non-interacting electrons = free Fermi gas
Fermi sea
Consider a system of electrons (fermions)
Landau’s Fermi liquid theory
Interacting electrons: what happens??
elementary excitation: “quasiparticles” collective excitation in terms of electrons but behaves like free fermions
“Fermi sea” of quasiparticles
What is the volue of the “Fermi sea”?
Luttinger’s theorem: VF is not renormalized by interactions
In some cases, the original proof by Luttinger does not apply, or is questionable….
eg. one dimensional systems systems involving localized spins (Kondo lattice) non-Fermi liquids
Alternative approach?
E
cf. Laughlin (1981)
adiabatically insert unit flux quantum (again!)
calculate the momentum change due to the flux insertion
(i) by Fermi liquid theory (or any effective theory)
(ii) using the large gauge transformation
Applicationselectrons coupled to localized spins (Kondo lattice)
localized spins do contribute to Fermi seavolume! (if low-energy excitations are exhausted by Fermi liquid)
“Fractionalized Fermi liquid” a phase that has similar low-energy excitations as the Fermi liquid but violates Luttinger’s theorem (with fractionalized spin exc.)
(Senthil-Sachdev-Vojta, 2003)
1
Adiabatic process commutes with the translation operator , so
momentum is conserved.
2ˆ However exp ;
so shift in momentum between states ' and
x
x
x x Tx
x
T
P
iU T U T n
L
P U
rr
0
is
2 mod 1 .
Alternatively, we can compute by assuming it is absorbed by
quasiparticles of a Fermi liquid. Each quasip
yx T
x
x
LP n
v a
P
2
article has its momentum
shifted by 2 , and so
Volume enclosed by Fermi surface2 2 mod 2 .
2
From 1 and 2 , same argument in direction, using coprime , :
x
xx xx y
x x y y
L
PL aL L
y L a L a
0
2 2 Volume enclosed by Fermi surface mod 22
T
vn
M. Oshikawa, Phys. Rev. Lett. 84, 3370 (2000).
[From http://sachdev.physics.harvard.edu/]
Effect of flux-piercing on a topologically ordered quantum paramagnetN. E. Bonesteel, Phys. Rev. B 40, 8954 (1989). G. Misguich, C. Lhuillier, M. Mambrini, and P. Sindzingre, Eur. Phys. J. B 26, 167 (2002).
DD
a D D
1 2 3Lx-1Lx-2 Lx
Number of bonds cutting dashed line
After flux insertion
1 ;
D
D
vison
0
Equivalent to inserting a inside hole of the torus.
carries momentum yL v
vison
Vison
Ly
[From http://sachdev.physics.harvard.edu/]
Flux piercing argument in Kondo lattice
Shift in momentum is carried by nT electrons, where
nT = nf+ nc
In topologically ordered, state, momentum associated with nf=1 electron is absorbed by creation of vison. The remaining momentum is absorbed by Fermi surface quasiparticles, which enclose a volu
me associated with nc electrons.
A Fractionalized Fermi liquid.
cond-mat/0209144
[From http://sachdev.physics.harvard.edu/]
“Bose volume”
The present argument actually appliesto system of boson as well.
The momentum change due toapplied electric field is “quantized”!
The corresponding “Luttinger’s theorem” gives a quantization of magnus force in lattice bose systems at T=0
(Vishwanath and Paramekanti, 2004)
Summary Quantum many-particle systems on a periodic lattice
: # of particles / unit cell
Topological restrictions:
If the system is gapless the “Fermi(Bose) volume” is quantized -- “Luttinger’s theorem”
If the system is gapful for Z there must be q-fold groundstate degeneracy
conductor or insulator?
(Kohn, 1963)
magnetization plateau
Luttinger’s theorem (1960)
topological quantization
gauge invariance and QHE
(Laughlin, 1981)
Lieb-Schultz-Mattis theorem (1961)
Haldane conjecture (1983)
Topological restrictions:
If the system is gapless the “Fermi(Bose) volume” is quantized -- “Luttinger’s theorem”
If the system is gapful there must be groundstate degeneracy
what does this mean?
“Usually” it is a consequence of Spontaneous Symmetry Breaking characterized by a local order parameter
e.g. Neel order
Topological degeneracy
There is also an “unusual” possibility that the groundstate degeneracy is due to a “topological order”
Characteristics of the topological degeneracy
(i) Degeneracy (# of g.s.) depending on the topology of the system (sphere, torus….) well known for Fractional Quantum Hall Liquids
[ cannot be understood with the ordinary SSB]
(ii) Absence of the local order parameter
Topological degeneracy
degenerate g.s.: indistinguishable by any local operator
ground-state degeneracy N depends on topology of the system
g=0 g=1 g=2
not a consequence of a ordinary SSB….. a signature of a topological order!
Quantum many-particle systems on a periodic lattice
: # of particles / unit cell
Topological restrictions:
If the system is gapful for Z there must be some kind of order, either the standard SSB with a local order parameter or a topological order
Systematic determination of order parameter
S. Furukawa, G. Misguich and M.O., cond-mat/0508469
How to find the order parameter without a prior knowledge?
measure all the correlation functions?
is there a better way?
In a quantum system, ground-state (GS) degeneracysignals some kind of order!
can be found without knowing the order parameter!
Suppose there aretwo-fold (quasi-) degenerate GSs below the gap, in a system of finite size L (sufficiently large)
Ene
rgy
gap
and
usually the degeneracy isa consequence of SSB
Symmetry-Breaking GSs
and(linear combinations of
and )
Order parameter: an observable which can distinguish these GSs
: observable defined on area is an
order parameter, if
“Difference” of the two GSs w.r.t.
for any normalized
Information on the expectation value of arbitrary observable on is encoded in the reduced density matrices
where are eigenvalues of
if “diff” is non-zero on an area there is an order parameter defined on
Properties of “diff”
Maximum is achieved with the “optimal order parameter”
If µ
Simple examplesNeel ordered state
diff = 2 already for = 1 spin
Spontaneously dimerized state
diff = 0 for single spin (no order parameter)
diff = 3/2 for two spins
S=1/2 ladder with 4-spin exchange
studied by many people
gap
[schematic phase diagram]
0.07 0.1476 0.39
2-fold degenerate GSs in the both phases --- what are the order parameters for them?
Phase I
Phase II
Symmetry-breaking GSs: two possibilities
Finite-size (quasi-) GSs
and : real (“time-reversal” invariant)
: real in Sz-basis (“time-reversal” invariant)
“time-reversal” invariant
“time-reversal” breaking
so calculate both “diff1” and “diff2” separately
We can’t know a priori which is the case;
Phase I Phase II
Numerical result on 14x2 system (with periodic BC) 0* : exactly zero due to symmetries, even in a finite system
Optimal order parameters on minimal area
Phase I
(leg) dimer order
Phase II
scalar chiral order(broken “time reversal”)
reproduced known results!
crossing point of diff1 and diff 2: agrees very well with the exact
Quantum Dimer Model on KagomeSolvable Hamiltonian
h: hexagon in the Kagome loop involving only one hexagon h
Misguich-Serban-Pasquier 2002
Zheng-Elser
dimer shiftalong the loop
Exact solutionGS(s): “Rokhsar-Kivelson” type RVB state
Finite gap above the GS(s)
GS degeneracy depends on the topology of the system cylinder: 2-fold, torus: 4-fold ………
Exact realization of “Z2 spin liquid”
What is the order parameter?
“topological degeneracy”
(uniform superposition of “short-ranged” valence bond states)
Order parameter of Kagome QDM
We can show that
between any (linear combinations of ) and for any local area
absence of local order parameter!
stability of qubit against decoherence
Expected property for the topological degeneracy, but is here shown explicitly and rigorously (cf. Ioffe-Feigel’man 2002)
system
Non-local order parameter
For the “diff” to be non-zero, must extend over the system
non-local order parameter necessary to detect the “topological order”
QDM on triangular lattice
consider Rokhsar-Kivelson wavefunctions (in topologically distinct sectors)
Is there a local order parameter? – apparently NO
(not exactly solvable!)
Possible developmentscan we identify a “new” order parameter?
combination with QMC/DMRG etc.
relation to DMRG, (quantum) information theory
degeneracy > 2 : optimization also on
systematic evaluation of the stability of many-body “topological” qubits
How to detect the topological order
Vishwanath-Paramekanti 2004
Even*Odd system: Momenta of the GSs: (0, 0) & (,0) whether the system has the SSB of translation symmetry or the topological order
Even*Even system:
Gauge argument
Momenta of the GSs: (0,0) & (,0) SSB(0,0) & (0,0) topological
Flux insertion = vison insertion
What is “order”?
What is “phase”?
We are just beginning to understand….
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