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Письма в журнал технической физики

Волноводные логические вентили для магнитооптических кубитов

Ш.В. Эгамов, Abduvali M. Khidirov, Kh O Urinov, Kh. A. Zhumanov

Published Jan 1, 2020• 0 citations
Publisher

Abstract

Results of magneto-optical waveguide logic gates properties investigation are presented. Simple logic operations can be realized using photon properties in modulated magnetic field. Changing the magnetic field amplitude and its orientation relating to light propagation direction, choosing polarizer and analyzer orientation and proper waveguide geometry, we can design logic gates avoiding small coherence time of regular optic qubits.

DOI
10.21883/pjtf.2020.19.50035.18058

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Results of magneto-optical waveguide logic gates properties investigation are presented. Simple logic operations can be realized using photon properties in modulated magnetic field. Changing the magnetic field amplitude and its orientation relating to light propagation direction, choosing polarizer and analyzer orientation and proper waveguide geometry, we can design logic gates avoiding small coherence time of regular optic qubits.
Abstract Results of studying properties of magnetooptical waveguide logic gates are presented. Simple logical operations can be implemented by changing photon states in a substance under the action of a modulating magnetic field. Varying the amplitude and orientation of the magnetic field relative to the light propagation direction, choosing the orientation of the polarizer and analyzer and appropriate configuration of the waveguide, one can design logic gates, including ones for qubit models. In doing this, the time barrier of low coherence peculiar to optical qubits is passed.
This paper presents a study of magneto-optical waveguide logic gates for optical communication systems. Simple logic operations are implemented by modulating photon states in a material through applied magnetic fields. By controlling the magnetic field's amplitude and orientation relative to light propagation, selecting polarizer/analyzer alignment, and configuring waveguides, we designed logic gates including qubit-compatible models that overcome the low coherence times typical of optical qubits. Optical qubits are promising candidates for quantum information processing and data transmission. For cryptographic applications using Vernam encryption, we developed an XOR logic gate simulator based on magneto-optical principles. Experimental validation employed ASCII encoding and text encryption/decryption algorithms, demonstrating successful cryptographic processing of confidential data over fiber-optic lines. The results show that magneto-optical qubit control mechanisms enable modeling diverse waveguide-based logic gates, including a half adder performing parallel XOR and AND operations. These devices facilitate novel information processing and transmission architectures.
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We propose the use of magneto-optic Kerr effect (MOKE) to realize single-qubit quantum gates. We consider longitudinal and polar MOKE in reflection geometry in which the magnetic field is parallel to both the plane of incidence and surface of the film. MOKE couples incident TE and TM polarized photons and the Hamiltonian that represents this interaction is isomorphic to that of a canonical two-level quantum system. By varying the phase and amplitude of the magnetic field, we can realize Hadamard, NOT, and arbitrary phase-shift single-qubit quantum gates. The principal advantage is operation with magnetically non-transparent materials.
Quantum logic gates are basic blocks to construct quantum computing and quantum information processing systems. Quantum logic gates based on coupled-resonator optical waveguide (CROW) are analyzed with the advantage of integration with other devices. Photonic crystal CROW (PhC CROW) structure with different dimension and background medium exhibits electromagnetically induced transparency (EIT), which is used as single quantum bit (qubit) phase gate. Quantum Hadamard gate can also be realized by coupling element. Two qubit conditional quantum phase gate is achieved by concatenating two Hadamard gates and a phase gate doped with dopant. The simplicity and dynamic tunability of the device…
We report on experimental and theoretical investigations of the polarization dependence of magnetic resonance generated by synchronous optical pumping. Magnetic resonances with narrow linewidth are generated experimentally using a rubidium vapor cell with octadecyltrichlorosilane antirelaxation coating on inner walls. We studied the effect of light ellipticity on the amplitudes and widths of magnetic resonances by matching the light modulation frequency with $2{\mathrm{\ensuremath{\Omega}}}_{L}$ (alignment) and ${\mathrm{\ensuremath{\Omega}}}_{L}$ (orientation) in a Bell-Bloom interaction geometry, where ${\mathrm{\ensuremath{\Omega}}}_{L}$ corresponds to the Larmor frequency. Both $2{\mathrm{\ensuremath{\Omega}}}_{L}$ and ${\mathrm{\ensuremath{\Omega}}}_{L}$ resonance amplitudes showed a strong dependence on the light ellipticity. In addition, we showed that the duty cycle of light modulation changes the slope of amplitude variations in $2{\mathrm{\ensuremath{\Omega}}}_{L}$ and ${\mathrm{\ensuremath{\Omega}}}_{L}$ resonances with light ellipticity. As a potential application, we showed that the difference between $2{\mathrm{\ensuremath{\Omega}}}_{L}$ and ${\mathrm{\ensuremath{\Omega}}}_{L}$ resonance amplitudes can be used for in situ measurement of light ellipticity. We also studied the dependence of $2{\mathrm{\ensuremath{\Omega}}}_{L}$ and ${\mathrm{\ensuremath{\Omega}}}_{L}$ resonance amplitudes on the polarization angle of linearly polarized light. These amplitudes oscillate periodically with the polarization angle. We found this oscillatory behavior to be sensitive to the tilt in magnetic field direction from the polarization plane. Such a property could be used to realize a vector magnetometer. A density matrix based theoretical model is developed to simulate the magnetic resonance spectrum for different light polarizations. Our theoretical model accurately reproduces the above-mentioned experimental observations.