@InHenriPoincare@CompSciOxford Carlo MAria Scandolo’s use the tools of resource theories, were some resources are free and others are costly.
Free resources induce a preorder: A more valuable then B if A –free→ B.
It describes allowed thermodynamics transitions #LTQI#QuPa
@InHenriPoincare@CompSciOxford Carlo Maria Scandolo: A test is a collection of porcesses {C_i} with input A and B. A—[{C_i}]—B
Channel=deterministic test. Some are reversible.
State=test with no input
Observation test: test with no outputs #LTQI#QuPa
Carlo Maria Scandolo then use this to construct circuits #LTQI#QuPa
Carlo MAria Scandolo: This general frameworks of operational-probabilistic theories (OPTs) is more generic than quantum mechanics. It contains stranger theories. #LTQI#QuPa
Carlo Maria Scandolo: Look at the microcanonical states, where all allowed microstates are equally probable.
Microstate=deterministic pure state.
Ideally χ=∫ψ dψ. χ should be unique and invariant under reversible dynamic. #LTQI#QuPa
Carlo Maria Scandolo: χ exists in finite dimensions (from Haar Measure)
Theorem: χ is unique iff the action of reversible channels on deterministic pure states is transitive.
∀pair ψ, ψ', ∃reversible channel U s.t. ψ'=Uψ. #QuPa#LTQI
Carlo MAria Scandolo: Reversible transformations are symmetries of the state space. E.g. ∄χ on the half disk, but it exists on the square (it’s at the centre) #LTQI#QuPa
Carlo Maria Scandolo: It’s natural to set the χ of a composite system to be the compositionof microcanonical systems χAB=χA⊗χB #LTQI#QuPa
Carlo Maria Scandolo: Noisy operations are generated by 1. prepare χ 2. apply reversible evolution 3. discard channels #LTQI#QuPa
Carlo MAria Scandolo: There is also RaRe (Random reversible channels),
and the more generic unital channels mapping χA to χB
Noisy⊆Unital and RaRe⊆Unital #LTQI#QuPa
Carlo Maria Scandolo look at sharp theories with purifications, where every pure state can be obtained (¿) via reversible operations (?) #LTQI#QuPa
Carlo Maria Scandolo: These theories have following axioms:
causality,
purity preservation (composition of pure transformations is pure)
Pure Sharpness (∀system, ∃pure effect occuring with prob 1 on some state ρ)
... #LTQI#QuPa
Carlo MAria Scandolo:
LAst axiom:
Purification (all state can be purified, aull purifcation ar equivialet upto reversible operation on purifying system) #LTQI#QuPa
Carlo Maria Scandolo: Sharp theories with purification have a well defined microcanoncal state. All states are diagonalizable.
We have the following inclusion:
RaRe ⊆ Noisy ⊆ Unital
⇒RaRe convertibility is the harder to satisfy #LTQI#QuPa
Carlo Maria Scandolo: Do eigenvalue of state tell anything about state convertibility? In classical & quantum theory, majorization plays an important role: ρ→σ if Sp(ρ)≻Sp(σ).
Almost the case, but majorization is not sufficient for RaRe channels (∃ counterexample) #LTQI#QuPa
Carlo Maria Scandolo: An additional axiom (unrestricted reversibility) is necessary and sufficient to link majorization with eigenvalues.
But this leads to theories very close to quantum mechanics #LTQI#QuPa
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