33,387 research outputs found

    The Rationalities of Emotion

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    I argue that emotions are not only rational in-themselves, strictly speaking, but they are also instrumentally rational, epistemically rational, and evaluatively rational. I begin with a discussion of what it means for emotions to be rational or irrational in-themselves, which includes the derivation of a criterion for the ontological rationality of emotions (CORe): For emotion or an emotion there exists some normative standard that is given by what emotion or an emotion is against which our emotional responses can be judged or evaluated in virtue of the fact that our emotions manifest our rationality. I conclude with a brief discussion of the implications of this account

    Strong Coupling of a Cavity QED Architecture for a Current-biased Flux Qubit

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    We propose a scheme for a cavity quantum electrodynamics (QED) architecture for a current-biased superconducting flux qubit with three Josephson junctions. The qubit operation is performed by using a bias current coming from the current mode of the circuit resonator. If the phase differences of junctions are to be coupled with the bias current, the Josephson junctions should be arranged in an asymmetric way in the qubit loop. Our QED scheme provides a strong coupling between the flux qubit and the transmission line resonator of the circuit.Comment: 5 pages, 3 figure

    Synthesis of several bisabolane sesquiterpenoids from xanthorrhizol isolated from C. Xanthorrhiza

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    Xanthorrhizol was isolated from the essential oil of fresh rhizomes of C. xanthorrhiza in 20.2% yield by fractionation using vacuum liquid chromatography. Several bisabolane-type sesquiterpenoids have been synthesised from this xanthorrhizol. Both diastereomers of 10,11-dihydro-10,11-dihydroxyxanthorrhizols, sesquiterpenoids isolated from the Mexican medicinal plant, Iostephane heterophylla, have been prepared in three steps from xanthorrhizol via Sharpless asymmetric dihydroxylation as the key steps. Fremy’s salt oxidation of xanthorrhizol gave curcuhydroquinone in 60% yield, which was successfully reduced with sodium dithionite to curcuhydroquinone in 100% yield. Sequential acetylation and Sharpless asymmetric dihydroxylation on curcuhydroquinone led to the diacetate derivative of helibisabonol A. Cleavage of the diacetate esters by reduction with lithium borohydride furnished helibisabonol A, an allelopathic agent isolated from Helianthus annuus (sunflowers). The unexpected difficulty in deprotection of helibisabonol A diacetate was due to acidic, basic and air-sensitive natures of helibisabonol A. An allylic alcohol derivative of O-methylxanthorrhizol, (3S,6R)-(3- methoxy-4-methylphenyl)-2-methylhept-1-en-3-ol, has been synthesised from xanthorrhizol in five steps via Sharpless asymmetric dihydroxylation as the key steps. Sharpless asymmetric dihydroxylation in all syntheses gave excellent enantioselectivity (ee > 98%). The enantiomeric excess and the absolute configuration of the diol was determined by the modified Mosher’s method

    Macroscopic Many-Qubit Interactions in Superconducting Flux Qubits

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    Superconducting flux qubits are considered to investigate macroscopic many-qubit interactions. Many-qubit states based on current states can be manipulated through the current-phase relation in each superconducting loop. For flux qubit systems comprised of NN qubit loops, a general expression of low energy Hamiltonian is presented in terms of low energy levels of qubits and macroscopic quantum tunnelings between the many-qubit states. Many-qubit interactions classified by {\em Ising type- or tunnel-}exchange interactions can be observable experimentally. Flux qubit systems can provide various artificial-spin systems to study many-body systems that cannot be found naturally.Comment: 5 pages, 1 figur

    Controllable Coupling in Phase-Coupled Flux Qubits

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    We propose a scheme for tunable coupling of phase-coupled flux qubits. The phase-coupling scheme can provide a strong coupling strength of the order of Josephson coupling energy of Josephson junctions in the connecting loop, while the previously studied inductive coupling scheme cannot provide due to small mutual inductance and induced currents. We show that, in order to control the coupling, we need {\it two} dc-SQUID's in the connecting loop and the control fluxes threading the dc-SQUID's must be in {\it opposite} directions. The coupling strength is analytically calculated as a function of the control flux at the co-resonance point.Comment: version to appear in Phys. Rev.
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