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Indefinite causal order has shown improvements for quantum communication where the channels used along the process are very noisy, thus being able to obtain improved transmission rates. Following such trend, it has also been studied the improvements obtained in teleportation as a genuine communication channel when the entangled resource is imperfect. It induces naturally a Pauli channel well characterized as function of the characteristic parameters of the entangled resource. We show that with more than two channels in superposition of causal order, the fidelity of teleportation improves, despite the probability of stochastic process due to the involvement of post-measurement shows a progressive decrease. In this work, we tackle the problem when two or more channels are applied under indefinite causal order, then analyzing the fidelity thus observing that the probability of successful transmission becomes compromised with the grown of channels. Then, a novel approach with the assistance of a weak measurement is analyzed in order to correct such loss. The weak measurement is aimed to select the best configuration for the channel in order to improve such probability with loss for the fidelity of transmission.

Quantum 2020

Improving imperfect quantum teleportation with indefinite causal order assisted by post-measurement and weak measurement

weak measurement

post-measurement

indefinite causal order

teleportation

The Institute of Physics and IOP Publishing, in partnership with the Chinese Physical Society (CPS) and the University of Science and Technology of China (USTC) are proud to have brought together the international quantum science community online for this inaugural conference.


Early career and leading researchers from universities, industry and government worldwide came together to share, learn and collaborate on the latest research and emerging areas of high interest across quantum science and technology. The broad themes covered by Quantum 2020 included:

Quantum communication;
Quantum computing and quantum simulation;
Quantum sensing, metrology and imaging;
Quantum information theory, software and algorithms;
Quantum foundations;
Quantum technology in industry.
The four-day event featured talks from world-renowned scientists, interactive poster sessions and two exciting panel discussions on the themes of Quantum Technology in Industry and Quantum Technology Programmes Around the World.


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CAP Virtual Congress 2021

poster

Heralded single photons emitted from spontaneous four-wave mixing process in a cold atomic cloud have extremely long coherence time up to microseconds, due to slow light effect of electromagnetically induced transparency (EIT). The temporal state of these single photons is typically characterized by the photon counting approach. For the first time, we utilize balanced homodyne tomography (BHT) to fully characterize the temporal state. From reconstructing its density matrix, and further verify that the temporal state shaped through EIT window is pure. To further improve the mode matching between the optical field of Anti-Stokes and the local field in BHT, the driving beam of EIT is split from the local field, and frequency shifted using an electric-optic modulator. The characterization of the pure temporal-spectral state of the single photons paves the way for exploiting the temporal-spectral degree of freedom to develop photonic-quantum information processing.

Tomography of the pure temporal state of single photons from a cold atomic ensemble

We study the classical analog of the quantum metric tensor for two well known models in atomic and nuclear physics. First, we analyze the geometry of the parameter space for the Dicke model with the aid of the classical and quantum metrics in the thermodynamic limit and compute their scalar curvatures, finding that they are continuous across the phase transition when there is no resonance, and that they diverge in the same way under resonance. Second, we compute the classical and quantum metrics for the Lipkin-Meshkov-Glick model in the thermodynamic limit and find a perfect agreement between them. Finally, we complement the analytic results with a finite-size numerical analysis.

Classical and quantum perspectives of the parameter space geometry in the Dicke and Lipkin models

This paper argues that the “Measurement Problem” is foundationally moot, using the abstraction of “Color Guessing Game”. It has been reasoned that the preferred question to ask is, once taken the measurement, what is the certainty that the measured physical state of quantum system is the original intended state governed by absolute laws of nature. The certainty of the measured state |ϕ_k〉 of the physical system with wave function |ψ〉=∑_i〖c_i |ϕ_i〉〗 being the original intended state is given by P(|ϕ_k〉)_certainty=[|c_k |^2/(∑_i|c_i |^2 )]∙[|c_k |^2/(∑_j|c_j |^2 ) ]_measurement, given that the measurement probe’s wave function interaction with |ψ〉 is unknown. It has been argued that measured state’s interactions with other quantum system corresponds to classical reality, which can be changed by the act of measurement.

The Problem with 'The Measurement Problem'

Designing band structures through the application of coherent time-periodic drives applied to quantum systems of reduced dimensions is a powerful experimental tool for inducing novel out-of-equilibrium quantum phases. In our work, we study an effect of the high-order harmonics generation in currents flowing through a quantum ring, being under the influence of an external microwave field and coupled to one or two reservoirs biased with a voltage periodic in time. The proposed technique that can be tunable by the joint action of a sine-wave voltage bias and microwave pumping permits to implement a simple detection system of microwaves as well as novel practically useful nanoscale setups with a discrete structure in the frequency domain. Fundamental quantum laws governing the system guarantee existence, identification and more stability under change of its states. We discuss possible realizations of the proposed device and analyze from this viewpoint results of recent experiments on equilibrium charge transport in AlxGa1-xAs/GaAs based quantum rings.

Tailoring high-harmonic generation from a phase-coherent quantum ring

Quantum catalysis is a fascinating concept which demonstrates that certain transformations can only become possible when given access to a specific resource that has to be returned unaffected. It was first discovered in the context of entanglement theory and since then applied in a number of resource-theoretic frameworks, including quantum thermodynamics. Although in that case the necessary (and sometimes also sufficient) conditions on the existence of a catalyst are known, almost nothing is known about the precise form of the catalyst state required by the transformation. In particular, it is not clear whether it has to have some special properties or be finely tuned to the desired transformation. In this work we describe a surprising property of multi-copy states: we show that in resource theories governed by majorization all resourceful states are catalysts for all allowed transformations. In quantum thermodynamics this means that the so-called "second laws of thermodynamics" do not require a fine-tuned catalyst but rather any state, given sufficiently many copies, can serve as a useful catalyst.

All states are universal catalysts in quantum thermodynamics

Binning a continuous degree of freedom of one particle creates an effective, finite-dimensional qudit. Photonic time-bin qubits and qudits are popular [1,2,3], though efficiently processing high-dimensional time-bins remains challenging. In this theoretical work, we devise a scheme using a single, binned degree of freedom of one particle as a system of multiple, effective qubits. Distinct qubits correspond to scales of the original, continuous variable. While general bin processing overhead scales polynomially with dimension [4,5], efficient quantum algorithms implemented on multi-qubit time-bins may use polynomial-size circuits optimized for conventional, multi-qubit quantum computing. Considering scales below accessible precision, we find intriguing analogies to infinite-dimensional von Neumann algebras. Finally, scale-separated qubits present an experimentally accessible medium to probe the quantum-classical transition of chaos.

[1] Bussieres et al. 2006. arXiv:quant-ph/0608183

[2] Islam et al. 2017 Sci. Adv. doi:10.1126/sciadv.1701491

[3] Victora et al. 2019. Quantum Photonics: Pioneering Advances and Emerging Applications, pp 179-206. doi:10.1007/978-3-319-98402-5_5

[4] Reck et al. 1994. Phys. Rev. Lett. doi:10.1103/PhysRevLett.73.58

[5] Kumar & Dhand. 2020. arXiv:2001.02012

Scale-Separated Qubits from Binned Continuous Variables

Introducing quantum entanglement into game theory led to a major milestone in the studies of quantum games. Such a breakthrough is achieved through the application of two-qubit operators which are uniquely represented by the geometrical points (c 1 , c 2 , c 3 ). While the quantization scheme proposed by Eisert et al involves controlled unitary operators, modification of the scheme includes a much wider class of two-qubit operators. It is known that altering the entangling operator in the quantization scheme has a direct effect on the average payoffs of the players involved in the game. However, we show in the present work that two different class of two-qubit entangling operators can produce the same average payoffs of the players. Such an analysis is carried out in the light of conversion of symmetric to potential games. While entangling operators play an inevitable role in quantum computing, we find its significance in game theory through this work.

Entangling operators and their interplay with average payoffs in quantum games

In many current experimental setups and quantum information technologies, protocols that maximize a case-specific figure of merit are highly desirable. In this talk we focus on the preparation of cat states, i.e., quantum superposition of two opposite-phase coherent states, in a nonlinear optical Kerr resonator. To solve this quantum state control problem, we implement the dynamics of the system as part of a fully differentiable program [1]. This framework ultimately combines machine learning and the knowledge of the differential equations governing the dynamics of the physical system. We employ a neural network that maps the state of the system at a given time to a control pulse. Finally, we verify the robustness of the method against noise in the initial states.

[1] F. Schäfer, M. Kloc, C. Bruder, N. Lörch, Mach. Learn.: Sci Technol. 1 035009

A differentiable programming method for optimal preparation of cat states

In High Energy Physics (HEP), calorimeter outputs play an essential role in understanding low distance processes occurring during particle collisions. Due to the complexity of underlying physics, the traditional Monte-Carlo simulation is computationally expensive, and thus, the HEP community has suggested Generative Adversarial Networks (GAN) for fast simulation. Meanwhile, it has also been proposed that, in certain circumstances, simulation using GANs can itself be sped-up by using quantum GANs (qGANs).
Our work presents an advanced prototype of qGAN, that we call the dual-Parameterized Quantum Circuit (PQC) GAN, with a classical discriminator and two quantum generators which take the form of PQCs. The first PQC learns the probability distribution over the images of N pixels, while the second generates normalized pixel intensities of an individual image for each PQC input. The dual-PQC architecture exhibits an apparent quantum advantage, by using only O(log(N)) qubits, unlike the classical GAN with O(N) neurons. Its performance has been evaluated through the application in HEP to imitate calorimeter outputs, translated into pixelated images. The results demonstrate that the model can reproduce a fixed number of images with a reduced size as well as their probability distribution and allows us to scale up to real calorimeter outputs. 


Dual-Parameterized Quantum Circuit GAN Model in High Energy Physics

In oblivious transfer, a sender Alice sends two bits to a receiver Bob, who only receives one of them. Alice does not know which bit Bob received. Oblivious transfer is a useful cryptographic primitive. It is universal for multiparty computation, where two or more parties want to compute something together, while not revealing more than necessary about their input data to the other party. Perfect quantum oblivious transfer is impossible, but imperfect variants remain possible. We show that it is possible to “reverse” a quantum oblivious transfer protocol by Amiri et al., arXiv:2007.04712, so that one can achieve quantum oblivious transfer “both ways” even if one of the parties can only send quantum states, and the other one can only measure quantum states. This can be useful for applications.


Improving imperfect quantum teleportation with indefinite causal order assisted by post-measurement and weak measurement

Next from Quantum 2020

Tomography of the pure temporal state of single photons from a cold atomic ensemble

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