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Non-equilibrium dynamic critical scaling of the quantum Ising chain. Michael Kolodrubetz Princeton University In collaboration with: Bryan Clark, David Huse David Pekker Krishnendu Sengupta. Quantum state of transverse-field Ising model during slow ramp is…. Universal
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Non-equilibrium dynamic critical scaling of the quantum Ising chain Michael Kolodrubetz Princeton University In collaboration with: Bryan Clark, David Huse David Pekker KrishnenduSengupta
Quantum state of transverse-field Ising model during slow ramp is… • Universal • Non-equilibrium • Experimentally viable • Non-thermal • Dephasing resistant
Classical Phase Transitions “Magnetization” Landau-Ginzburg functional
Classical Phase Transitions “Magnetization”
Classical Phase Transitions “Magnetization” Thermal fluctuations
Quantum Phase Transitions One-dimensional transverse-field Ising chain
Quantum Phase Transitions One-dimensional transverse-field Ising chain Paramagnet (PM) Ferromagnet (FM)
Quantum Phase Transitions One-dimensional transverse-field Ising chain Paramagnet (PM) Ferromagnet (FM) Quantum fluctuations
Critical Scaling [Smirnov, php.math.unifi.it/users/paf/LaPietra/files/Chelkak01.ppt]
Critical Scaling [Smirnov, php.math.unifi.it/users/paf/LaPietra/files/Chelkak01.ppt]
Critical Scaling , Dynamiccritical exponent Correlation lengthcritical exponent [Smirnov, php.math.unifi.it/users/paf/LaPietra/files/Chelkak01.ppt]
Critical Scaling Ising: , Dynamiccritical exponent Correlation lengthcritical exponent
Critical Scaling Ising: Order parametercritical exponent , Dynamiccritical exponent Correlation lengthcritical exponent
Critical Scaling Ising: Order parametercritical exponent , Dynamiccritical exponent Correlation lengthcritical exponent
Kibble-Zurek ramps Ramp rate
Kibble-Zurek ramps Ramp rate
Kibble-Zurek ramps Ramp rate Adiabatic
Kibble-Zurek ramps Ramp rate Impulse Adiabatic
Kibble-Zurek ramps Ramp rate Impulse Adiabatic
Kibble-Zurek ramps Ramp rate Impulse Adiabatic
Kibble-Zurek ramps Ramp rate Impulse Adiabatic
Kibble-Zurek ramps Ramp rate Impulse Adiabatic
Kibble-Zurek ramps Ramp rate Impulse Adiabatic
Kibble-Zurek ramps Ramp rate Impulse Adiabatic
Kibble-Zurek ramps Ramp rate Impulse Adiabatic
Kibble-Zurek ramps Ramp rate Impulse Adiabatic
Transverse-field Ising chain Sachdev: “Quantum Phase Transitions”
Transverse-field Ising chain Wigner fermionize Sachdev: “Quantum Phase Transitions” phase
Transverse-field Ising chain Wigner fermionize Sachdev: “Quantum Phase Transitions” phase
Transverse-field Ising chain Wigner fermionize • Quadratic Integrable Sachdev: “Quantum Phase Transitions” phase
Transverse-field Ising chain Wigner fermionize • Quadratic Integrable • Hamiltonian conserves parity for each mode k Sachdev: “Quantum Phase Transitions” phase
Transverse-field Ising chain Wigner fermionize • Quadratic Integrable • Hamiltonian conserves parity for each mode k • Work in subspace where parity is even Sachdev: “Quantum Phase Transitions” phase
Transverse-field Ising chain Wigner fermionize • Quadratic Integrable • Hamiltonian conserves parity for each mode k • Work in subspace where parity is even Sachdev: “Quantum Phase Transitions” phase
Transverse-field Ising chain Low energy, long wavelength theory
Kibble-Zurek ramps Low energy, long wavelength theory? Ramp rate Impulse Adiabatic
Kibble-Zurek ramps Low energy, long wavelength theory Ramp rate Impulse Adiabatic
Kibble-Zurek ramps Low energy, long wavelength theory Ramp rate Impulse Adiabatic
Kibble-Zurek scaling limit Schrödinger Equation OR Observable Fixed