Now at #MCQS, Andrea Rocchetto, from @UCL@UniofOxford on «Machine learning in quantum information theory, a selection of results» #LTQI
@ucl@UniofOxford Andrea Rocchetto defines the PAC (porbabilistically aproximate correct) models, and defines the concept of PAC-learnable: a concept is PAC-learnable iff one can guess a good model for arbitrary input distributions #LTQI#MCQS
@ucl@UniofOxford Andrea Rocchetto: PAC learning on quantum states. The goal is to guess σ havig the same probability ditribution under a binary POVM than the training set ρ. Aaronson proved in 2007 that the problem is really different from tomography. #LTQI#MCQS
@ucl@UniofOxford Andrea Rocchetto: σ is PAC learnable, but at an exponential complexity cost. “The information is there, but we cannot get it”.
In contrast, Stabiliser states are efficiently PAC-learnable #LTQI#MCQS
@ucl@UniofOxford Andrea Rocchetto: it works by predicting the output of measurement without generating the states and/or the full stabilizer group. Only the commutation relations with the generators are checked #LTQI#MCQS
@ucl@UniofOxford Andrea Rocchetto looks at learning boolean function in disjunctive normal form (DNF)
Best classical algorithm is 2^Õ(n^⅓), learnung under product is quasipolynomial n^O(log(n))
and poly(n) under membership queries. #LTQI#MCQS
@ucl@UniofOxford Andrea Rocchetto: A key tool in these classical results is the approximation of DNF with heavy Fourier coefficients.
Using the quantum Fourier transform (QFT) allows to accelerate this in the quantum setting. #LTQI#MCQS
@ucl@UniofOxford Andrea Rocchetto: These result actually use µ-biased Fourier transform, which can be quantized and used in a quantum version of the Kushilevitz–Mansour algorithm #LTQI#MCQS
Andrea Rocchetto moves on to approximating Hamiltonian dynamics using Nyström method (arXiv:1804.02484 arxiv.org/abs/1804.02484 ). The goal here is a different classical simulation technique for quantum systems #LTQI#MCQS
Andrea Rocchetto: Random linear transformation can be used for dimensionality reduction. The Nyström method use random projection to construct a low rank approximate version of a matrix #LTQI#MCQI
Andrea Rocchetto: H can be efficiently simulted if it is row-computable, row-searchable and has a bounded Froebenius norm.
Output: an efficient representation of exp(-iHt)[ψ⟩ #LTQI#MCQI
Andrea Rocchetto: an open question is to find physical Hamiltonians which respect the conditions of the theorem. #LTQI#MQCS
Andrea Rocchetto moves on to learnign hard quantum states (
(arXiv:1710.00725 arxiv.org/abs/1710.00725 )
where he suses neural netwroks (Restricted/deep Boltzmann machines (RBMs /DBMs) to encode quantum states #LTQI#MCQI
Andrea Rocchetto induced a deep generative models (variational autoencoders) for quantum states. Depth is useful, and allows a constant compression factor for hard states #LTQI#MCQS
@ucl@UniofOxford Andrea Rocchetto’s talk on «Machine learning in quantum information theory, a selection of results» is available on
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Now at #JapanEUWorkshop, Shuntaro Takeda on A strategy for large-scale optical quantum computing #LTQI
Shuntaro Takeda: use a deterministic approach, a loop to increase scalability. Determinism is brought by continuous variable (CV) system, which need 5 gates to be universal: 3 linear, squeezing and cubic gate (the hard one) #LTQI#JapanEUWorkshop
Shuntaro Takeda: both discrete CNOT and CV cubit gates need χ⁽³⁾ and are therefore difficult, but the latter is at least deterministic. #LTQI#JapanEUWorkshop
Now at #JapanEUWorkshop , Anthony Laing on Photonic simulations of molecular quantum dynamics #LTQI
Anthony Laing essentially looks a photnic simulation of vibrational modes of molecules
Anthony Lang looks at selective dissociation with a single quantum of vibration NH₃→NH₂+H. These molecular transition can be manipulated through control of the wavepacket. #LTQI
Now Erika Kawakami on Capacitive read-out of the Rydberg states towards the realization of a quantum computer
using electrons on helium #LTQI#JapanEUWorkshop
Erika Kawakami: Why use electrons on helium? The system is clean: electrons float in vacuum, far prom nuclear spin and other charges. Electron qubits are 1µm away, which will be useful for surface codes #LTQI#JapanEUWorkshop
Erika Kawakami: The spin-state is used a qubit state, the rydberg states are auxiliary states. T₂=100 s for spin states. 1 qubit gates through ESR; 2-qubit gate using Coulomb interacton #LTQI#JapanEUWorkshop
Now, Eleni Diamanti on Practical Secure Quantum Communications #JapanEUWorkshop#LTQI
Eleni Diamanti: The current solution to secure network links: Symmetric + Asymmetric cryptography. Recent development to fight the threat of quantum computers: postquantum cryptography. Quantum cryptography offers the advantage to be future proof #LTQI
Now, Yoshiro Takahashi from @KyotoU_News on Advanced quantum simulator with novel
spin and orbital degrees of freedom #LTQI
@KyotoU_News Yoshihiro Takahashi: With ¹⁷³Yb nuclear spins, we have a SU(6) Fermi-Hubbard model. They observe formation of SU(6) Mott insulator. #LTQI#JapanEUWorkshop
@KyotoU_News Yoshihiro Takahashi ’s next traget: SU(6) quantum magnetism. A difficulty is measuring spin correlation, which is achieved through singlet-triplet oscillation compined with photo association #LTQI#JapanEUWorkshop
Now, Christian Groß, on quantum simulation of the Hubbard model, from hidden correlations to magnetic polarons. #LTQI
Christian Groß simulates Hubbard model with cold atoms in optical lattices. Li atoms hop with amplitude t. Currently, they only have global control, no local control. #LTQI
Christian Groß observes the atoms with quantum gas microscopy. He observes a single plane desctructively through a high NA objective every 30s. #LTQI