3,685 research outputs found

    Entropy Change through Rayleigh-B\'enard Convective Transition with Rigid Boundaries

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    The previous investigation on Rayleigh-B\'enard convection of a dilute classical gas [T. Kita: J. Phys. Soc. Jpn. {\bf 75} (2006) 124005] is extended to calculate entropy change of the convective transition with the rigid boundaries. We obtain results qualitatively similar to those of the stress-free boundaries. Above the critical Rayleigh number, the roll convection is realized among possible steady states with periodic structures, carrying the highest entropy as a function of macroscopic mechanical variables.Comment: 5 pages, 4 figure

    A theory of new type of heavy-electron superconductivity in PrOs_4Sb_12: quadrupolar-fluctuation mediated odd-parity pairings

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    It is shown that unconventional nature of superconducting state of PrOs_4Sb_12, a Pr-based heavy electron compound with the filled-Skutterudite structure, can be explained in a unified way by taking into account the structure of the crystalline-electric-field (CEF) level, the shape of the Fermi surface determined by the band structure calculation, and a picture of the quasiparticles in f2^{2}-configuration with magnetically singlet CEF ground state. Possible types of pairing are narrowed down by consulting recent experimental results. In particular, the chiral "p"-wave states such as p_x+ip_y is favoured under the magnetic field due to the orbital Zeeman effect, while the "p"-wave states with two-fold symmetery such as p_x can be stabilized by a feedback effect without the magnetic field. It is also discussed that the double superconducting transition without the magnetic field is possible due to the spin-orbit coupling of the "triplet" Cooper pairs in the chiral state.Comment: 12 pages, 2 figures, submitted to J. Phys.: Condens. Matter Lette

    Theory of Flux-Flow Resistivity near Hc2H_{c2} for s-wave Type-II Superconductors

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    This paper presents a microscopic calculation of the flux-flow resistivity ρf\rho_{f} for s-wave type-II superconductors with arbitrary impurity concentrations near the upper critical field Hc2H_{c2}. It is found that, as the mean free path ll becomes longer, ρf\rho_{f} increases gradually from the dirty-limit result of Thompson [Phys. Rev. B{\bf 1}, 327 (1970)] and Takayama and Ebisawa [Prog. Theor. Phys. {\bf 44}, 1450 (1970)]. The limiting behaviors suggest that ρf(H)\rho_{f}(H) at low temperatures may change from convex downward to upward as ll increases, thus deviating substantially from the linear dependence ρfH/Hc2\rho_{f}\propto H/H_{c2} predicted by the Bardeen-Stephen theory [Phys. Rev. {\bf 140}, A1197 (1965)]

    Ozone-enhanced layers in the troposphere over the equatorial Pacific Ocean and the influence of transport of midlatitude UT/LS air

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    International audienceOccurrence of ozone (O3)-enhanced layers in the troposphere over the equatorial Pacific Ocean and their seasonal variation were investigated based on ozonesonde data obtained at three Southern Hemisphere ADditional OZonesondes (SHADOZ) sites, Watukosek, American Samoa and San Cristobal, for 6 years between 1998 and 2003. O3-enhanced layers were found in about 50% of observed O3 profiles at the three sites on yearly average. The formation processes of O3-enhanced layers were investigated by meteorological analyses including backward trajectories. On numerous occasions, O3-enhanced layers resulted from the transport of air masses affected by biomass burning. The contribution of this process was about 30% at San Cristobal during the periods from February to March and from August to September, while it was relatively low, about 10%, at Watukosek and Samoa. A significant number of the O3-enhanced layers were attributed to the transport of midlatitude upper-troposphere and lower-stratosphere (UT/LS) air. Meteorological analyses indicated that these layers originated from equatorward and downward transport of the midlatitude UT/LS air masses through a narrow region between high- and low-pressure systems around the subtropical jet stream. This process accounted for more than 40% at Watukosek between May and December, about 60% or more at Samoa all year around, and about 40% at San Cristobal between November and March, indicating that it was important for O3 budget over the equatorial Pacific Ocean

    Ensiling Characteristics of Sudangrass Silage Treated with Green Tea Leaf Waste or Green Tea Polyphenols

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    Green tea waste (GTW), emitted from beverage companies manufacturing tea drinks, contains high crude protein (CP) and polyphenols. Kondo et al. (2004) showed that GTW addition to forage ensiling enhanced lactic acid fermentation and decreased pH value. Ishihara et al. (2001) showed that high counts of Lactobacillus species were maintained and the counts of clostridia were decreased in the intestinal microflora of animals fed the diet containing green tea polyphenols (GTP). It is hypothesised that GTP might activate lactic acid bacteria and enhance silage fermentation. This study was conducted to evaluate the potential of GTW and GTP as silage additives and explored the mechanisms of enhanced lactic acid fermentation by GTW

    Fermentation Characteristics of Maize/Sesbania Bi-Crop Silage

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    Maize is one of the main forages for dairy production and is a suitable material for silage making because of high fermentable carbohydrates, high counts of lactic acid bacteria (LAB) and low buffering capacity (BC) (Nishino et al. 2003; McDonald et al. 1991). Whole crop maize silage is high in energy but low in crude protein (CP). On the other hand, legumes are high in CP but difficult to conserve because of their low water soluble carbohydrates (WSC) and high BC. It might be possible that maize/legume bi-crop silage compensate for their negative points. Sesbania is a legume originated in tropical area and might be suitable for inter-crops with maize. Therefore, we investigated the fermentation characteristics of bi-crop silage from maize and sesbania

    Quasiparticles of d-wave superconductors in finite magnetic fields

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    We study quasiparticles of d-wave superconductors in the vortex lattice by self-consistently solving the Bogoliubov-de Gennes equations. It is found for a pure dx2y2d_{x^2-y^2} state that: (i) low-energy quasiparticle bands in the magnetic Brillouin zone have rather large dispersion even in low magnetic fields, indicating absense of bound states for an isolated vortex; (ii) in finite fields with kFξ0k_F \xi_0 small, the calculated tunneling conductance at the vortex core shows a double-peak structure near zero bias, as qualitatively consistent with the STM experiment by Maggio-Aprile et al. [Phys. Rev. Lett. {\bf 75} (1995) 2754]. We also find that mixing of a dxyd_{xy}- or an s-wave component, if any, develops gradually without transitions as the field is increased, having little effect on the tunneling spectra.Comment: 4 pages, 4 figures, LaTe

    Entropy and Spin Susceptibility of s-wave Type-II Superconductors near Hc2H_{c2}

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    A theoretical study is performed on the entropy SsS_{\rm s} and the spin susceptibility χs\chi_{\rm s} near the upper critical field Hc2H_{c2} of s-wave type-II superconductors with arbitrary impurity concentrations. The changes of these quantities through Hc2H_{c2} may be expressed as [Ss(T,B)Ss(T,0)]/[Sn(T)Ss(T,0)]=1αS(1B/Hc2)(B/Hc2)αS[S_{\rm s}(T,B)-S_{\rm s}(T,0)]/[S_{\rm n}(T)-S_{\rm s}(T,0)]=1-\alpha_{S}(1-B/H_{c2})\approx (B/H_{c2})^{\alpha_{S}}, for example, where BB is the average flux density and SnS_{\rm n} denotes entropy in the normal state. It is found that the slopes αS\alpha_{S} and αχ\alpha_{\chi} at T=0 are identical, connected directly with the zero-energy density of states, and vary from 1.72 in the dirty limit to 0.50.60.5\sim 0.6 in the clean limit. This mean-free-path dependence of αS\alpha_{S} and αχ\alpha_{\chi} at T=0 is quantitatively the same as that of the slope αρ(T=0)\alpha_{\rho}(T=0) for the flux-flow resistivity studied previously. The result suggests that Ss(B)S_{\rm s}(B) and χs(B)\chi_{\rm s}(B) near T=0 are convex downward (upward) in the dirty (clean) limit, deviating substantially from the linear behavior B/Hc2\propto B/H_{c2}. The specific-heat jump at Hc2H_{c2} also shows fairly large mean-free-path dependence.Comment: 8 pages, 5 figure
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