@InHenriPoincare@univ_paris13 Bruno Laburthe-Tolra: works with quantum gases, with density 10¹²–10¹⁵ at/cm³, at nK or µK, with de Broglie wavelengths and inter-atomic distance > 100nm.
These systems (boson or fermions) are “clean” analogues of condensed matter systems. #QuPa#LTQI
@InHenriPoincare@univ_paris13 Bruno Laburthe-Tolra: Optical lattices are periodic (spin indeendent) potentials induced by stationary optical waves. This allows to make 1D, 2D and 3D potential, making 2D, 1D and strongly correlated spin gases. #LTQI#QuPa
@InHenriPoincare@univ_paris13 Bruno Laburthe-Tolra:Effective spin–spin (Heisenberg like) interaction can arise through Coulomb (condensed matter)/ van der Waals (optical lattice) interaction.
This allows to revisit the Hubbard model from solid-state physics experimentally with cold atoms #QuPa#LTQI
@InHenriPoincare@univ_paris13 Bruno Laburthe-Tolra: The Hubbard model is only an approximate Hamiltonian (dipolar interactions, density assisted tunneling), and the “corrections” can change qualitatively the behaviour
@InHenriPoincare@univ_paris13 Bruno Laburthe-Trola: With cold atoms in periodic potentials, we can directly dive into regime which are intractable by classical computers.
E.g. Interacting spin-less bosons, spin ½ interactiong bosons and fermions, super-exchange interaction #LTQI#QuPa
@InHenriPoincare@univ_paris13 Bruno LAburthe-Tolra: With trapped ions, one can investigate long-range spin-spin interaction.
Bruno LAurthe-Tolra’s main interest is simulation with dipolar particles #LTQI#QuPa
@InHenriPoincare@univ_paris13 Bruno Laburthe-Tolra: Some optical systems allow to change the lattice topology, moving e.g. between decorated triangular, 1D and KAgomé lattices. #LTQI#QuPa
@InHenriPoincare@univ_paris13 Bruno Laburthe-Tolra: Some settings (but not his) have site-resolved imaging. But it needs spaced site ⇒ slow tunneling.
It allows to see the SF–Mott transition atom bu atom (Greiner group) #LTQI#QuPa
@InHenriPoincare@univ_paris13 Bruno Laburthe-Tolra: Greiner‘s group observed the checkerboard pattern with anti-ferromagnetic correlations (s=½ fermions).
Adding doping (away to ½full lattice) is easy experimentally (add holes) but very hard theoretically. Allows to explore a strange metal phase #LTQI#QuPa
@InHenriPoincare@univ_paris13 Brun Laburthe-Tolra: The hard thing experimentally is low temperature, because of spin entropy (close to log(2): ∄ direct way to cool the spins.
The usual strategy relies on super-exchange, but it is VERY long #LTQI#QuPa
Bruno Laburthe-Tolra: It is actually impossible, because the potential is spin insensitive, and conservation laws. The initial spin is ∝√N, because of statistical fluctuations, and we want a regime of total spin close to 0 #QuPa#LTQI
Bruno Laburthe-Tolra: It is possible to play with local density, on order to have low spin-entropy regions.
Another way (more promising) is to use spin-dependent hamiltonian. E.g. arxiv:1803.10663 arxiv.org/abs/1803.10663 but other strategies are possible #QuPa#LTQI
Bruno Laburthe-Tolra: Has experimental data showing his system is not described by mean-field theory arXiv:1803.02628 arxiv.org/abs/1803.02628 : Helps from theoreticians is needed now to describe current systems! #LTQI#QuPa
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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