Recent progresses in Josephson-junction-based superconducting circuits have propelled quantum information processing forward. However, the lack of a metastable state in most superconducting artificial atoms hinders th...
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Recent progresses in Josephson-junction-based superconducting circuits have propelled quantum information processing forward. However, the lack of a metastable state in most superconducting artificial atoms hinders the development of photonic quantum memory in this platform. Here we use a single superconducting qubit-resonator system to realize a desired Λ-type artificial atom, and to demonstrate slow light with a group velocity of 3.6 km/s and the microwave storage with a memory time extending to several hundred nanoseconds via electromagnetically induced transparency. Our results highlight the potential of achieving microwave quantum memory, promising substantial advancements in quantum information processing within superconducting circuits.
Boro-tellurite glasses composed of 57B2O3– (4-y)Na2O-–15Bi2O3-20TeO2–3TiO2–1Tm2O3-yHo2O3 (y = 0, 0.5, 1.0, 1.5, 2.0, and 2.5 mol%) were succesfully synthesised and the change in their absorption spectra in wavelen...
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The delineation of Lymph Nodes (LNs) is pivotal in pinpointing therapeutic targets for radiotherapy in head and neck malignancies. Nevertheless, this endeavor poses a formidable challenge, primarily stemming from the ...
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Fictitious magnetic fields can be introduced in quantum magnets by strain engineering and the Aharonov-Casher effect. Here, we study impacts of a uniform fictitious magnetic field and corresponding Landau quantization...
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Fictitious magnetic fields can be introduced in quantum magnets by strain engineering and the Aharonov-Casher effect. Here, we study impacts of a uniform fictitious magnetic field and corresponding Landau quantization on the Néel order in the S=12 Heisenberg model on the square lattice as a prototypical system of quantum magnets. We first analyze the system by using the spin-wave approximation. It is found that the staggered magnetization is enhanced by the fictitious magnetic field and it shows a simple scaling behavior with respect to the magnetic length, in contrast with a naive expectation based on the Dzyaloshinskii-Moriya interaction. We also perform density-matrix-renormalization-group calculations to fully consider quantum effects and obtain quantitatively more accurate results. The enhancement is found to be anomalously strong, and it shows a nontrivial scaling behavior or a fluctuation induced discontinuity. These results are beyond the well-known understanding of correlated systems under magnetic fields called the magnetic catalysis.
We investigate competition and cooperation of magnetic frustration and the Kondo effect in the J1−J2 Kondo lattice model on the square lattice at zero temperature. In this model, the frustrated interactions J1,J2 betw...
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We investigate competition and cooperation of magnetic frustration and the Kondo effect in the J1−J2 Kondo lattice model on the square lattice at zero temperature. In this model, the frustrated interactions J1,J2 between the localized spins stabilize spin nematic orders, while the Kondo coupling favors local spin singlets. Using the slave boson mean field approximation, we find that the spin nematic order remains stable against small Kondo coupling, and the localized spins and the conduction electrons are effectively decoupled. On the other hand, a standard Fermi liquid state is formed for sufficiently strong Kondo interactions. Furthermore, in an intermediate region with moderate Kondo coupling, the spin nematic order and the Kondo effect coexist, and superconducting pairing of the conduction electrons is induced by the spinon pairing. We discuss the ground state phase diagram and nature of the quantum phase transitions between the different superconducting states.
We study the topological order that arises from chiral states with SU(N) or SO(N) edge-state symmetry. This extends our previous study of topological orders that descend from the bosonic E8 quantum Hall state. We use ...
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We study the topological order that arises from chiral states with SU(N) or SO(N) edge-state symmetry. This extends our previous study of topological orders that descend from the bosonic E8 quantum Hall state. We use exactly solvable models of coupled electron wires to construct states with SU(m)n, SO(m)n, or Sp(m)n topological order for various levels n. We use our constructions to write down string operators for various non-Abelian anyons. We thereby provide a systematic, model derivation of quantum Hall states, topological superconductors, and spin liquids with emergent non-Abelian quasiparticle excitations, including those of Ising, metaplectic, and Fibonacci type.
We confirm by using the Skyrme Hartree-Fock-Bogoliubov calculation that Pb164 is a possible heaviest N=Z doubly magic nucleus whose lifetime is long enough to be measured on accelerator experiments. We estimate the pr...
We confirm by using the Skyrme Hartree-Fock-Bogoliubov calculation that Pb164 is a possible heaviest N=Z doubly magic nucleus whose lifetime is long enough to be measured on accelerator experiments. We estimate the proton-emission and alpha-decay half-lives of Pb164. The estimated proton-emission half-life ranges from 0.1ps to 10ns, while the alpha decay can be safely neglected.
NaNbO3 doped with Zn (0.00, 0.02, and 0.05 mmol) was synthesized by the microwave-assisted hydrothermal method. Photocatalytic and antibacterial activities were investigated. X-ray diffraction revealed the coexistence...
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We investigate competition and cooperation of magnetic frustration and the Kondo effect in the J1-J2 Kondo lattice model on the square lattice at zero temperature. In this model, the frustrated interactions J1,J2 betw...
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We study creation of quasi-particles in fractional Chern insulators (FCI) under magnetic fields. We consider two representative models, the Kapit-Mueller model and the checkerboard model, which have distinct band prop...
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