The complex projective space (ℂn) can be interpreted as the space of all quantum pure states of size n. A distance on this space, interesting from the perspective of quantum physics, can be induced from a classical di...
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Every graph with maximum degree Δ can be colored with (Δ + 1) colors using a simple greedy algorithm. Remarkably, recent work has shown that one can find such a coloring even in the semi-streaming model: there exist...
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In this paper we introduce and investigate the concept of a perfect quantum protractor, a pure quantum state |ψ〉 ∈ H that generates three different orthogonal bases of H under rotations around each of the three perp...
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We review application of level dynamics to spectra of quantally chaotic systems. We show that statistical mechanics approach gives us predictions about level statistics intermediate between integrable and chaotic dyna...
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We discuss a new classical action that enables efficient computation of the gluonic tree amplitudes but does not contain any triple point vertices. This new formulation is obtained via a canonical transformation of th...
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K Nearest Neighbors (KNN) algorithm is a straight-forward yet powerful Machine Learning (ML) tool widely used in classification, clustering, and regression applications. In this work, KNN is applied, with three distan...
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We analyze the real-space paired state with the k-dependent superconducting gap in the presence of Rashba-type spin-orbit coupling and external magnetic field. We show that the extended s-wave pairing symmetry is the ...
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We analyze the real-space paired state with the k-dependent superconducting gap in the presence of Rashba-type spin-orbit coupling and external magnetic field. We show that the extended s-wave pairing symmetry is the most probable scenario to appear in the low electron concentration regime. According to our study, the van Hove singularity induced by the spin-orbit coupling may lead to a significant enhancement of the superconducting gap, critical temperature, and critical magnetic field. Moreover, the combined effect of the spin-orbit coupling and the external magnetic field results in a nonzero total momentum of the Cooper pairs, which is a characteristic feature of the so-called helical state. In such a situation, due to the C4 symmetry breaking, a small d-wave and p-wave contributions to the pairing appear, which significantly change the character of the helical state. The obtained results are discussed in the context of the experimental data related with the unconventional superconducting features of the transition metal oxide interfaces as well as the recently reported supercurrent diode effect.
We introduce a tensor network designed to faithfully simulate the AdS/CFT correspondence, akin to the multiscale entanglement renormalization ansatz (MERA), following hyperinvariant tensor network. The proposed constr...
We introduce a tensor network designed to faithfully simulate the AdS/CFT correspondence, akin to the multiscale entanglement renormalization ansatz (MERA), following hyperinvariant tensor network. The proposed construction integrates bulk indices within the network architecture to uphold the key features of the HAPPY code, including complementary recovery. This framework accurately reproduces the boundary conformal field theory’s (CFT) two- and three-point correlation functions, while considering the image of any bulk operator. Furthermore, we provide an explicit methodology for calculating the correlation functions in an efficient manner. Our findings highlight the physical aspects of the relation between bulk and boundary within the tensor network models, contributing to the understanding and simulation of holographic principles in quantum information.
We present a numerical macrospin model for harmonic voltage detection in multilayer spintronic devices. The core of the computational backend is based on the Landau-Lifshitz-Gilbert-Slonczewski equation, which combine...
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We present a numerical macrospin model for harmonic voltage detection in multilayer spintronic devices. The core of the computational backend is based on the Landau-Lifshitz-Gilbert-Slonczewski equation, which combines high performance and satisfactory agreement with the experimental results in large-scale applications. We compare the simulations with the experimental findings in a Ta/CoFeB bilayer system for angular- and magnetic-field-dependent resistance measurements, electrically detected magnetization dynamics, and harmonic Hall voltage detection. Using simulated scans of the selected system parameters such as the polar angle θ, magnetization saturation (μ0Ms), or uniaxial magnetic anisotropy (Ku), we show the resultant changes in the harmonic Hall voltage, demonstrating the dominating influence of the μ0Ms on the first and second harmonics. In the spin-diode ferromagnetic resonance method, the (μ0Ms, Ku) parameter space may be optimized numerically to obtain a set of viable curves that fit the experimental data.
We investigate the energy spectrum of a single- and two-electron quantum dot (QD) embedded in two-dimensional electron gas at the interface between SrTiO3 and LaAlO3, in the presence of the external magnetic field. Fo...
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We investigate the energy spectrum of a single- and two-electron quantum dot (QD) embedded in two-dimensional electron gas at the interface between SrTiO3 and LaAlO3, in the presence of the external magnetic field. For this purpose, the three-band model of 3d electrons defined on the square lattice of Ti ions was utilized. We demonstrate that, for the weak parabolic confinement potential, the low-energy spectrum is sufficiently well described by the effective Hamiltonian reduced to the one dxy orbital with the spin-orbit interaction originating from the coupling to the dxz and dyz bands. This is not the case for stronger confinement where contribution of the states related to the dxz/yz orbital is relevant. Based on the time-dependent calculations, we discuss in detail the manipulation of the electron spin in a QD by external AC voltages, in the context of the electric dipole spin resonance. The allowed and forbidden transitions are discussed in detail with respect to the parity selection rule. Our calculations show that, for a single-electron QD, the spin flip in the ground state has the character of a Rabi resonance, while for two electrons, the singlet-triplet transition is forbidden by the parity symmetry. For the two-electron QD, we demonstrate that the spin-flip transition can still be accomplished via a second-order, two-photon process that has a two-state Rabi character for low AC field amplitude. The violation of the parity symmetry on the spin-flip transitions is also analyzed.
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