Advances in Superconductivity V 1993
DOI: 10.1007/978-4-431-68305-6_240
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Numerical Analysis for the Transport Properties of the Oxide S-N-S Junction

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Cited by 4 publications
(6 citation statements)
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“…While UMa I is dominated by old metal-poor stars, it appears to be systematically younger than the other galaxies in our sample. UMa I may be distorted, and Okamoto et al (2008) argue that it appears to be undergoing disruption; elongation along our sightline could be broadening the CMD, producing an apparent age spread. Hercules is the brightest galaxy in our sample (M v = −6.6 mag; Martin et al 2008b); it may have retained more gas during the reionization era, leading to a non-negligible population of younger stars.…”
Section: Discussionmentioning
confidence: 90%
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“…While UMa I is dominated by old metal-poor stars, it appears to be systematically younger than the other galaxies in our sample. UMa I may be distorted, and Okamoto et al (2008) argue that it appears to be undergoing disruption; elongation along our sightline could be broadening the CMD, producing an apparent age spread. Hercules is the brightest galaxy in our sample (M v = −6.6 mag; Martin et al 2008b); it may have retained more gas during the reionization era, leading to a non-negligible population of younger stars.…”
Section: Discussionmentioning
confidence: 90%
“…An appropriate object is the Galactic globular cluster M92 -one of the most ancient and metal-poor stellar systems known. Of the globular clusters with little extinction, it is the most metal-poor (Harris 1996), and it has served as a reference population in previous studies of UFDs (e.g., Belokurov et al 2006Belokurov et al , 2007Belokurov et al , 2009Belokurov et al , 2010Okamoto et al 2008Okamoto et al , 2012Sand et al 2009Sand et al , 2010Sand et al , 2012. It was observed with the same camera and filters by Brown et al (2005), and its CMD is shown in Figure 4.…”
Section: Analysis 31 Comparison With M92mentioning
confidence: 94%
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“…The theoretical results of the Raman spectra from the orbital wave agree with the polarization dependence of the spectra and their relative intensities in experiment. 40 Since the characteristic energy of the orbital excitation is much higher than that of the lattice vibration, we introduce the adiabatic approximation for the lattice degree of freedom in the calculation of the orbital wave. Then, the energy of orbital wave is approximately given by ω orb = (3J 1 +…”
Section: Summary and Discussionmentioning
confidence: 99%
“…The mean field theory proposed by de Gennes 24 is applied to the present system with orbital degeneracy and electron correlation. 25 In this theory, the spin and pseudo-spin operators are treated as classical vectors: (S ix , S iy , S iz ) = 1 2 (sin θ s i cos φ s i , sin θ s i sin φ s i , cos θ s i ), (5) and…”
Section: Model and Formulationmentioning
confidence: 99%