100 research outputs found

    Quantum entropy of the Kerr black hole arising from gravitational perturbation

    Get PDF
    The quantum entropy of the Kerr black hole arising from gravitational perturbation is investigated by using Null tetrad and \'t Hooft\'s brick-wall model. It is shown that effect of the graviton\'s spins on the subleading correction is dependent of the square of the spins and the angular momentum per unit mass of the black hole, and contribution of the logarithmic term to the entropy will be positive, zero, and negative for different value of a/r+a/r_+.Comment: 8 pages, 1 figure, Latex. to appear in Phys. Rev.

    Development of a posture detector using a flex sensor

    Get PDF
    In this digital age, many people spend hours every day looking at their cell phones and computers. Overuse of these devices can result in users\u27 posture deterioration. Poor postures not only detract from a person\u27s appearance but can also lead to chronic back discomfort and inflammation. Even though everyone knows the detrimental effects of poor postures, it is difficult for them to correct their bad habits. This is because poor postures are gradually developed, and they are usually related to a person\u27s lifestyle. The purpose of this project was to embed a poor posture detector (a posture coach) into clothing so that users could wear it unobtrusively and comfortably. Its functions were to detect and alert users of poor postures, to help the users maintain proper postures continuously, and to help users correct their habits related to bad postures

    Detrital heavy minerals constraints on the Triassic tectonic evolution of the West Qinling terrane, NW China: implications for understanding subduction of the Paleotethyan Ocean

    Get PDF
    We have examined the Triassic sediments in the west Qinling terrane, northeastern Tibet. These sediments consist mainly of flysch and shallow-sea and fluvial deposits with abundant lithic and heavy mineral detritus, sandwiched between and overlying Late Paleozoic and Early-Middle Triassic ophiolitic mélanges. Volcanic and metamorphic detritus dominates the lithic component of Lower Triassic sandstones accompanied by high Cr-spinel, pyroxene, and magnetite contents, indicating a mixed ophiolite and metamorphic source. Detrital mineral geochemistry further suggests that ophiolitic, high-grade metamorphic, basic, and intermediate-acidic igneous rocks must have been exposed and deeply eroded in their source area. Abundances of zircon, rutile, garnet, tourmaline, and epidote are greater in the Middle Triassic samples, and granitic and volcanic sources are the major contributors of detrital clasts. Considering these new observations on sedimentary petrography and detrital heavy mineral geochemistry, along with published data on paleocurrents, detrital zircon U-Pb ages, sedimentary facies, and regional magmatism, we suggest that these Triassic sediments represent the sedimentary fill of a forearc basin that overlies a late Paleozoic ophiolitic complex. A south-facing Andean-type convergent continental margin system developed along the southern margin of the North China block during the Triassic, in response to northward subduction of the Paleotethyan Ocean

    Statistical Entropy of a Stationary Dilaton Black Hole from Cardy Formula

    Get PDF
    With Carlip's boundary conditions, a standard Virasoro subalgebra with corresponding central charge for stationary dilaton black hole obtained in the low-energy effective field theory describing string is constructed at a Killing horizon. The statistical entropy of stationary dilaton black hole yielded by standard Cardy formula agree with its Bekenstein-Hawking entropy only if we take period T T of function vv as the periodicity of the Euclidean black hole. On the other hand, if we consider first-order quantum correction then the entropy contains a logarithmic term with a factor −1/2-{1/2}, which is different from Kaul and Majumdar's one, −3/2-{3/2}. We also show that the discrepancy is not just for the dilaton black hole, but for any one whose corresponding central change takes the form c12=AH8πG2πκT\frac{c}{12}= \frac{A_H}{8\pi G}\frac{2\pi}{\kappa T}.Comment: 11 pages, no figure, RevTex. Accepted for publication in Phys. Rev.
    • …
    corecore