randomness and chaos in qubit models · randomness and chaos in qubit models pak hang chris lau...
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![Page 1: Randomness and chaos in qubit models · Randomness and chaos in qubit models Pak Hang Chris Lau (NCTS) ... Transverse Ising model • 𝐿𝐿= 4. Comparison • Same behaviour as](https://reader035.vdocuments.us/reader035/viewer/2022071409/61027fcaed248961f928e671/html5/thumbnails/1.jpg)
Randomness and chaos in qubit models
Pak Hang Chris Lau (NCTS) with Chen-Te Ma (SCNU), Jeff Murugan (Cape Town U.) and Masaki Tezuka (Kyoto U)
Phys. Lett. B795 (2019) 230-235
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Classical chaos
• Non-linear system • Double rod pendulum
• Weather
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Definition
• Sensitivity to initial condition 𝛿𝛿𝛿𝛿 𝑡𝑡𝛿𝛿𝛿𝛿 0 = 𝑒𝑒𝜆𝜆𝜆𝜆
• Topologically transitive
𝑓𝑓:𝑋𝑋 → 𝑋𝑋 𝑓𝑓𝑛𝑛 𝐴𝐴 ∩ 𝐵𝐵 ≠ ∅ 𝐴𝐴,𝐵𝐵 ⊂ 𝑋𝑋
• Dense periodic orbits
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Quantum chaos
• Quantum mechanics
• Schrodinger equation • Linear
• Classical definition of chaos ↔ Quantum ?
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Quantum chaos
• Quantum ?→ Classical chaos
• Early time • Out of time-ordered correlator (OTOC)
• Late time • Spectral form factor
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Diagnostic 1
• Out of time ordered correlator (OTOC)
• Quantum mechanics • Operators 𝛿𝛿�, �̂�𝑝
• 𝛿𝛿� 𝑡𝑡 , �̂�𝑝(0) = 𝑖𝑖 𝛿𝛿𝛿𝛿 𝜆𝜆𝛿𝛿𝛿𝛿 0
𝐶𝐶𝑇𝑇 = − 𝑊𝑊 𝑡𝑡 ,𝑈𝑈 0 2𝛽𝛽~𝑒𝑒2𝜆𝜆𝜆𝜆
![Page 7: Randomness and chaos in qubit models · Randomness and chaos in qubit models Pak Hang Chris Lau (NCTS) ... Transverse Ising model • 𝐿𝐿= 4. Comparison • Same behaviour as](https://reader035.vdocuments.us/reader035/viewer/2022071409/61027fcaed248961f928e671/html5/thumbnails/7.jpg)
OTOC
• Holography • Maximum bound
• Jackiw–Teitelboim gravity • 1+1d dilaton gravity
• Sachedev-Ye-Kitaev model • 0+1 Fermionic quantum mechanics with all to all couplings
𝜆𝜆 ≤2𝜋𝜋𝑘𝑘𝐵𝐵𝛽𝛽𝛽
J. Maldacena, S.H. Shenker, D. Stanford JHEP (2016) 08 106
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Diagnostic 2
• Quantum → Probabilistic • Statistic properties of the system
• Random matrix theory (RMT) • Spectra of heavy nuclei
• Wigner 1955
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Classical chaos & RMT
• Sinai billiard • Chaotic
• Quantum Sinai billiard • Spectrum
• RMT
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Quantum spectrum
• Level spacing distribution 𝑃𝑃 𝑠𝑠 • Correlation of neighbour states
• Uncorrelated • Poisson distribution 𝑃𝑃 𝑠𝑠 = 𝑒𝑒−𝑠𝑠
• Correlated (RMT)
• Wigner-Surmise 𝑃𝑃 𝑠𝑠 ~𝑠𝑠𝛽𝛽𝑒𝑒−𝑘𝑘𝑠𝑠2
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Diagnostic 2 - RMT
• Spectral form factor (SFF) • Correlation between eigenvalues
𝑔𝑔 𝑡𝑡 =
Z 𝛽𝛽, 𝑡𝑡 2
Z 𝛽𝛽, 0 2
Z 𝛽𝛽, 𝑡𝑡 = Tr 𝑒𝑒 −𝛽𝛽+𝑖𝑖𝜆𝜆 𝐻𝐻
J.S. Cotler et.al JHEP (2017) 1705: 118.
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Ensemble averaged
• Annealed spectral form factor
• Quenched spectral form factor
𝑔𝑔𝑎𝑎𝑛𝑛𝑛𝑛 𝑡𝑡 =Z 𝛽𝛽, 𝑡𝑡 2
Z 𝛽𝛽, 0 2
𝑔𝑔𝑞𝑞𝑞𝑞𝑞𝑞 𝑡𝑡 =Z 𝛽𝛽, 𝑡𝑡 2
Z 𝛽𝛽, 0 2
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Sachedev-Ye-Kitaev model
• Hamiltonian
• Majorana fermions 𝜓𝜓𝑖𝑖 ,𝜓𝜓𝑗𝑗 = 𝛿𝛿𝑖𝑖𝑗𝑗
• Random coupling
• Gaussian variance 𝑞𝑞 − 1 ! 𝐽𝐽2
𝑁𝑁𝑞𝑞−1
• Most studied case • 𝑞𝑞 = 4 large N (chaotic)
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Model
• 𝑞𝑞 = 2 Sachdev-Ye-Kitaev model (SYK) • Majorona fermions
• Random coupling • Gaussian
• Integrable
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Numerical calculation
• Jordan-Wigner transformation • Fermions → Spin (Pauli matrices)
• Hamiltonian
• 2𝑁𝑁2 × 2
𝑁𝑁2 matrix
• 2𝑁𝑁2 eigenvalues
• Order 1010 ensembles
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SYK2 - Spectral form factor
J.S. Cotler et.al JHEP (2017) 2017: 118.
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Spectral form factor
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Small N SFF
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Small N SFF
• Only 𝑁𝑁 = 2 • No dip-ramp-plateau
• 𝑁𝑁 = 2 solvable analytically
• Eigenvectors • Independent of coupling
• Origin of dip-ramp-plateau?
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Transverse Ising model
• Spin system with 𝐿𝐿 sites
• Random coupling 𝐾𝐾𝑖𝑖
• Magnetic field 𝑀𝑀
• Analytically integrable
R B Stinchcombe (1973) Journal of Physics C 6(15) 2459
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Transverse Ising model
• 𝐿𝐿 = 2
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Transverse Ising model
• 𝐿𝐿 = 4
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Comparison
• Same behaviour as the SYK4 model (chaotic) for 𝑁𝑁 > 2 • Transverse Ising model consistent
• General integrable spin system?
• Dip-ramp-plateau • Generate from large set of eigenstates
• 𝑁𝑁 = 2 eigenvectors independent of couplings
• Not sufficient condition to diagnose chaos
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Connection to thermalisation
• Closed random quantum system • Pure state → Thermal state
• Decoherence
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Set-up
• A general quantum state
• Random couplings
• Expectation value of operators • Ensemble averaged
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Decoherence
• A particular weight
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One qubit model
• Most general Hamiltonian
• Random couplings • Gaussian
• Operators
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One qubit model
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Summary
• Randomness can generate dip-ramp-plateau behaviour • Chaos like?
• Randomness leads to decoherence • Thermalisation of expectation values
• Relation to Chaos → Thermalisation?