phases and phase transitions of quantum materials
TRANSCRIPT
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Subir SachdevYale University
Phases and phase transitions of quantum materials
Talk online:http://pantheon.yale.edu/~subir
or Search for Sachdev on
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Phase changes in natureJames BayWinter Summer
Ice Water
At low temperatures,minimize energy
At high temperatures,maximize entropy
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Classical physics: In equilibrium, at the absolute zero of temperature ( T = 0 ), all particles will reside at rest at positions which minimize their total interaction energy. This defines a (usually) unique phase of matter e.g. ice.
Quantum physics: By Heisenberg’s uncertainty principle, the precise specification of the particle positions implies that their velocities are uncertain, with a magnitudedetermined by Planck’s constant . The kinetic energy of this -induced motion adds to the energy cost of the classically predicted phase of matter.
Tune : If we are able to vary the “effective” value of , then we can change the balance between the interaction and
kinetic energies, and so change the preferred phase:matter undergoes a quantum phase transition
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Outline
1. The quantum superposition principle – a qubit
2. Interacting qubits in the laboratory - LiHoF4
3. Breaking up the Bose-Einstein condensateBose-Einstein condensates and superfluidsThe Mott insulator
4. The cuprate superconductors
5. Conclusions
Varying “Planck’s constant” in the laboratory
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1. The Quantum Superposition Principle
The simplest quantum degree of freedom –
a qubitqubit
Ho ions in a crystal of LiHoF4
Two quantum states:
and ↑ ↓
These states represent e.g. the orientation of the electron spin on a
Ho ion in LiHoF4
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An electron with its “up-down” spin orientation uncertain has a definite
“left-right” spin
( )
( )
12
12
→ = ↑ + ↓
← = ↑ − ↓
A spin is a quantum superposition of and spins
→
↑ ↓
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2. Interacting qubits in the laboratory
In its natural state, the potential energy of the qubits in LiHoF4 is
minimized by
........↑↑↑↑↑↑↑↑↑↑↑
........↓↓↓↓↓↓↓↓↓↓↓
or
A Ferromagnet
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Enhance quantum effects by applying an external “transverse” magnetic field which prefers that each
qubit point “right”
For a large enough field, each qubit will be in the state
( )12
→ = ↑ + ↓
The qubits are collectively in the state
→→→ = ↑↑↑ + ↓↑↑ + ↑↓↑
+ ↑↑↓ + ↓↓↑ + ↑↓↓
+ ↓↑↓ + ↓↓↓
≠ ↑↑↑ + ↓↓↓
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Phase diagram
g = strength of transverse magnetic field
Quantum phase transition
........↑↑↑↑↑↑↑↑ →→→→→
Absolute zero of temperature
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Phase diagram
g = strength of transverse magnetic field
Quantum phase transition
Spin relaxation rate ~ /T
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3. Breaking up the Bose-Einstein condensate
A. Einstein and S.N. Bose (1925)
Certain atoms, called bosons (each such atom has an even
total number of electrons+protons+neutrons), condense at low temperatures
into the same single atom state. This state of matter is a
Bose-Einstein condensate.
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The Bose-Einstein condensate in a periodic potential“Eggs in an egg carton”
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The Bose-Einstein condensate in a periodic potential“Eggs in an egg carton”
○
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The Bose-Einstein condensate in a periodic potential“Eggs in an egg carton”
○
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The Bose-Einstein condensate in a periodic potential“Eggs in an egg carton”
○
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The Bose-Einstein condensate in a periodic potential“Eggs in an egg carton”
= + G + ○ ○ ○
Lowest energy state of a single particle minimizes kinetic energy by maximizing
the position uncertainty of the particle
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The Bose-Einstein condensate in a periodic potential
=
= + + +
+ + + + ....27 terms
BEC GGG
○ ○○○
○ ○○
○
○
○ ○
○○ ○ ○
○○
○○
○○
Lowest energy state for many atoms
Large fluctuations in number of atoms in each potential well – superfluidity (atoms can “flow” without dissipation)
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The Bose-Einstein condensate in a periodic potential
=
= + + +
+ + + + ....27 terms
BEC GGG
○ ○○○
○ ○○
○
○
○ ○
○○ ○ ○
○○
○○
○○
Lowest energy state for many atoms
Large fluctuations in number of atoms in each potential well – superfluidity (atoms can “flow” without dissipation)
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The Bose-Einstein condensate in a periodic potential
=
= + + +
+ + + + ....27 terms
BEC GGG
○ ○○○
○ ○○
○
○
○ ○
○○ ○ ○
○○
○○
○○
Lowest energy state for many atoms
Large fluctuations in number of atoms in each potential well – superfluidity (atoms can “flow” without dissipation)
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The Bose-Einstein condensate in a periodic potential
=
= + + +
+ + + + ....27 terms
BEC GGG
○ ○○○
○ ○○
○
○
○ ○
○○ ○ ○
○○
○○
○○
Lowest energy state for many atoms
Large fluctuations in number of atoms in each potential well – superfluidity (atoms can “flow” without dissipation)
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The Bose-Einstein condensate in a periodic potential
=
= + + +
+ + + + ....27 terms
BEC GGG
○ ○○○
○ ○○
○
○
○ ○
○○ ○ ○
○○
○○
○○
Lowest energy state for many atoms
Large fluctuations in number of atoms in each potential well – superfluidity (atoms can “flow” without dissipation)
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The Bose-Einstein condensate in a periodic potential
=
= + + +
+ + + + ....27 terms
BEC GGG
○ ○○○
○ ○○
○
○
○ ○
○○ ○ ○
○○
○○
○○
Lowest energy state for many atoms
Large fluctuations in number of atoms in each potential well – superfluidity (atoms can “flow” without dissipation)
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The Bose-Einstein condensate in a periodic potential
=
= + + +
+ + + + ....27 terms
BEC GGG
○ ○○○
○ ○○
○
○
○ ○
○○ ○ ○
○○
○○
○○
Lowest energy state for many atoms
Large fluctuations in number of atoms in each potential well – superfluidity (atoms can “flow” without dissipation)
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3. Breaking up the Bose-Einstein condensate
= + +
+ + +
MI ○ ○ ○
○ ○
○ ○ ○○ ○
○○
○
○ ○ ○ ○ ○
By tuning repulsive interactions between the atoms, states with multiple atoms in a potential well can be suppressed. The lowest energy state is then a Mott insulator – it has
negligible number fluctuations, and atoms cannot “flow”
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3. Breaking up the Bose-Einstein condensate
= + +
+ + +
MI ○ ○ ○
○ ○
○ ○ ○○ ○
○○
○
○ ○ ○ ○ ○
By tuning repulsive interactions between the atoms, states with multiple atoms in a potential well can be suppressed. The lowest energy state is then a Mott insulator – it has
negligible number fluctuations, and atoms cannot “flow”
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3. Breaking up the Bose-Einstein condensate
= + +
+ + +
MI ○ ○ ○
○ ○
○ ○ ○○ ○
○○
○
○ ○ ○ ○ ○
By tuning repulsive interactions between the atoms, states with multiple atoms in a potential well can be suppressed. The lowest energy state is then a Mott insulator – it has
negligible number fluctuations, and atoms cannot “flow”
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3. Breaking up the Bose-Einstein condensate
= + +
+ + +
MI ○ ○ ○
○ ○
○ ○ ○○ ○
○○
○
○ ○ ○ ○ ○
By tuning repulsive interactions between the atoms, states with multiple atoms in a potential well can be suppressed. The lowest energy state is then a Mott insulator – it has
negligible number fluctuations, and atoms cannot “flow”
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Phase diagram
Quantum phase transition
Bose-EinsteinCondensate
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4. The cuprate superconductors
A superconductor conducts electricity without resistance
below a critical temperature Tc
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La,Sr
O
Cu
La2CuO4 ---- insulator
La2-xSrxCuO4 ----superconductor for
0.05 < x < 0.25
Quantum phase transitions as a function of Sr concentration x
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La2CuO4 --- an insulating antiferromagnet
with a spin density wave
La2-xSrxCuO4 ----a superconductor
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Zero temperature phases of the cupratesuperconductors as a function of hole density
x
Insulator with a spin density wave
Superconductor with a spin density wave
Superconductor
~0.05 ~0.12
Applied magnetic field
Theory for a system with strong interactions: describe superconductor and superconductor+spin density
wave phases by expanding in the deviation from the quantum critical point between them.
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Accessing quantum phases and phase transitions by varying “Planck’s constant” in the laboratory
• Immanuel Bloch: Superfluid-to-insulator transition in trapped atomic gases
• Gabriel Aeppli: Seeing the spins (‘qubits’) in quantum materials by neutron scattering
• Aharon Kapitulnik: Superconductor and insulators in artificially grown materials
• Matthew Fisher: Exotic phases of quantum matter