8
collaborators
2017–2024
years active
Contributions
QIP QCrypt TQC talk poster presenter award · △program ◇steering ○organizing · filled = chair
15 Posters
| Title | Conference | Co-authors |
|---|---|---|
| Randomness extraction analysis simplified by Pearson's criterion | QCRYPT 2024 | Andrei Gaidash, Anton Kozubov |
We investigate multi-pixel quantum random number generators as a Gaussian entropy source. The procedure of randomness extraction implies maximization of the conditional probability as a step of conditional min-entropy estimation, implying an eavesdropper may influence the signal. Usually, it requires to artificially limit the dynamic range of the variable that an eavesdropper may control. We propose the approach that may expel a necessity of this assumption by utilizing Pearson’s goodness-of-fit criterion, such that the histogram of measured outcomes fits well into the dynamical range and well approximated by a Gaussian. The latter greatly simplifies the min-entropy estimations and may be incorporated in security criterion estimation. |
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| Intermode-interaction-induced dynamics of continuous variable quantum key distribution observables | QCRYPT 2024 | Andrei Gaidash, Alexei Kiselev, Anton Kozubov |
We theoretically study dynamical regimes of the observables that govern the operating conditions of continuous variable (CV) quantum key distribution (QKD) systems, depending on quantum-channel-induced intermode interactions. In contrast to the widely used approach, where losses and thermal broadening are introduced through a beamsplitter transformation, our analysis uses the exactly solvable quantum channel model describing the Lindblad dynamics of multimode bosonic systems interacting with a heat bath and additionally takes into account imperfections of the homodyne detection scheme. The analytical results for the photon count difference and the quadrature probability distributions are used to derive the expression for the mutual information between legitimate parties, which explicitly links the information properties of CV QKD and the parameters of the channel. For the important special case of a two-mode photonic system propagating in a fiber channel, the latter can be conveniently parameterized using the frequency and the relaxation rate vectors that characterize the coherent (dynamical) intermode couplings and the incoherent (environment mediated) interaction between the bosonic modes, respectively. It turned out that these vectors determine four qualitatively different dynamical regimes of the mutual information and the phase difference between the signal and the local oscillator that may significantly affect the operation of CV QKD. |
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| Quantum network security dependent on connection density between trusted nodes | QCRYPT 2022 | Andrei Gaidash, Alexei Kiselev, Anton Kozubov |
| Algebraic approach for investigation of a multi-mode quantum system dynamics | QCRYPT 2022 | Andrei Gaidash, Anton Kozubov, Alexei Kiselev |
| Dissipative dynamics of quantum states in the fiber channel | QCRYPT 2020 | Andrei Gaidash, Anton Kozubov |
In this paper we consider the Liouville equation that describes the quantum non-unitary dynamics of quantum states in optical fiber.We consider particular case of thermalization aiming to applications related to various quantum information protocols; however the model can be generalized in various ways taking into account more features (external pump, nonlinear interactions, continuous spectra, free space propagation, etc.). In order to obtain the appropriate evolution models for states in the channel we use the SU(1,1) algebra formalism in the Liouville representation. Developed model is applied in cases of two different initial states as an example. The first is single- and multi-frequency-mode (e.g. wavelength-division-multiplexed) weak coherent states in quantum notation as rather simple but useful example. This particular example is of interest since weak coherent states are commonly used tool in various fields of optics, e.g. optical communication, quantum key distribution, etc. Results for coherent states are well agreed with classical theories however in order to highlight quantum features of developed theory we also consider the case of non-classical light, in particular Fock states. Considered implementation of model takes into account dichroism, retardance, thermalization, dispersion, decoherence in polarization domain. We derive expressions of evolved states, mean photon number and estimate the Stokes parameters as well as degree of polarization. Considered examples explicitly demonstrates all the features and effects of developed approach. Described approach allows to connect the information properties of quantum channels with its physical ones. In order to illustrate this statement we consider BB84 quantum key distribution protocol and investigate behavior of quantum bit error rate affected by considered physical phenomena in optical fiber. |
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| Complete Bell state analyser for photonic qubits using semi-demolition or entangled non-demolition measurements | QCRYPT 2020 | Anton Kozubov, Andrei Gaidash |
In this paper we present for the first time two possible techniques for deterministic two-step complete Bell state analyzer of optical (polarization) qubits using semi-demolition or entangled non-demolition measurements. Main difference to a prior studies in the field is that we do not use hyperentanglement or representation of the Bell states as concatenated Greenber–Horne–Zeilinger (C-GHZ) state to provide the discrimination. We demonstrate two different approaches for complete Bell state measurement based on different types of filtration. In entangled non-demolition measurement we allocate two pairs of the states from each other as the filtration process. The approach can be based on the utilization of cubic (Kerr) nonlinearity and auxiliary mode. In semi-demolition measurement two states are unambiguously discriminated and hence destroyed; however two other states passes the filter without modification. The measurement destroys the single photon subspace in every mode and preserves the superposition of zero and two photons. It can be realized with discrete photodetection based on microresonator with atoms. Such filtration can be considered as quadratic nonlinearity just as any measurement. The most significant about this approach is that we do not transform the initial states using any type of filtration based on different nonlinearities. |
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| Unambiguous state discrimination of phase-coded multi-mode weak coherent states | QCRYPT 2019 | Andrei Gaidash, Anton Kozubov |
| Quantum model of decoherence in polarization domain for the fiber channel | QCRYPT 2019 | Anton Kozubov, Andrei Gaidash |
| Quantum control attack on quantum key distribution systems | QCRYPT 2019 | Anton Kozubov, Andrei Gaidash |
| Quantum model of decoherence for coherent states in the fiber optical channels | QCRYPT 2019 | Andrei Gaidash, Anton Kozubov |
| Finite-key analysis for subcarrier wave quantum key distribution | QCRYPT 2018 | Anton Kozubov, Andrei Gaidash, Artur Gleim |
| Precise overestimation of quantum bit error rate to minimize failure probability of low density parity check error correction | QCRYPT 2018 | Vladimir Chistiakov, Andrei Gaidash, Anton Kozubov, Vladimir Egorov, Artur Gleim |
| Modulation index decoy states protocol for subcarrier wave quantum key distribution system | QCRYPT 2018 | Andrei Gaidash, Vladimir Chistyakov, Anton Kozubov, Artur Gleim |
| Practical security for subcarrier wave quantum key distribution against collective beam-splitting attack. | QCRYPT 2017 | Anton Kozubov, Andrei Gaidash, Dmitri Horoshko, Artur Gleim |
| Analysis of modulation parameters inequality in subcarrier wave quantum communication and its application to countering unambiguous state discrimination attack | QCRYPT 2017 | Andrei Gaidash, Anton Kozubov, Vladimir Egorov, Artur Gleim |
Collaborators
| Co-author | Joint talks |
|---|---|
| Andrei Gaidash | 15 |
| Anton Kozubov | 15 |
| Artur Gleim | 5 |
| Alexei Kiselev | 3 |
| Vladimir Egorov | 2 |
| Dmitri Horoshko | 1 |
| Vladimir Chistiakov | 1 |
| Vladimir Chistyakov | 1 |