14,406,106 research outputs found

    Thermoelectric figure of merit of tau-type conductors of several donors

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    Dimensionless thermoelectric figure of merit ZTZT is investigated for two-dimensional organic conductors τ−(EDO−S,S−DMEDT−TTF)2(AuI2)1+y\tau-(EDO-S,S-DMEDT-TTF)_2(AuI_2)_{1+y}, τ\tau-(EDT-S,S-DMEDT-TTF)_2(AuI_2)_{1+y}and and \tau−(P−S,S−DMEDT−TTF)2(AuI2)1+y-(P-S,S-DMEDT-TTF)_2(AuI_2)_{1+y} (y≤0.875y \le 0.875), respectively. The ZTZT values were estimated by measuring electrical resistivity, thermopower and thermal conductivity simultaneously. The largest ZTZT is 2.7 ×\times 10−2^{-2} at 155 K for τ−(EDT−S,S−DMEDT−TTF)2(AuI2)1+y\tau-(EDT-S,S-DMEDT-TTF)_2(AuI_2)_{1+y}, 1.5 ×\times 10−2^{-2} at 180 K for τ−(EDO−S,S−DMEDT−TTF)2(AuI2)1+y\tau-(EDO-S,S-DMEDT-TTF)_2(AuI_2)_{1+y} and 5.4 ×\times 10−3^{-3} at 78 K for τ−(P−S,S−DMEDT−TTF)2(AuI2)1+y\tau-(P-S,S-DMEDT-TTF)_2(AuI_2)_{1+y}, respectively. Substitution of the donor molecules fixing the counter anion revealed EDT-S,S-DMEDT-TTF is the best of the three donors to obtain larger ZTZT.Comment: proceedings of ISCOM 2009 (to be published in Physica B

    Inferring an Indeterminate String from a Prefix Graph

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    An \itbf{indeterminate string} (or, more simply, just a \itbf{string}) \s{x} = \s{x}[1..n] on an alphabet Σ\Sigma is a sequence of nonempty subsets of Σ\Sigma. We say that \s{x}[i_1] and \s{x}[i_2] \itbf{match} (written \s{x}[i_1] \match \s{x}[i_2]) if and only if \s{x}[i_1] \cap \s{x}[i_2] \ne \emptyset. A \itbf{feasible array} is an array \s{y} = \s{y}[1..n] of integers such that \s{y}[1] = n and for every i∈2..ni \in 2..n, \s{y}[i] \in 0..n\- i\+ 1. A \itbf{prefix table} of a string \s{x} is an array \s{\pi} = \s{\pi}[1..n] of integers such that, for every i∈1..ni \in 1..n, \s{\pi}[i] = j if and only if \s{x}[i..i\+ j\- 1] is the longest substring at position ii of \s{x} that matches a prefix of \s{x}. It is known from \cite{CRSW13} that every feasible array is a prefix table of some indetermintate string. A \itbf{prefix graph} \mathcal{P} = \mathcal{P}_{\s{y}} is a labelled simple graph whose structure is determined by a feasible array \s{y}. In this paper we show, given a feasible array \s{y}, how to use \mathcal{P}_{\s{y}} to construct a lexicographically least indeterminate string on a minimum alphabet whose prefix table \s{\pi} = \s{y}.Comment: 13 pages, 1 figur

    Can Y(4140) be a ccˉssˉc \bar c s \bar s tetraquark ?

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    In this exploratory study the spectrum of tetraquarks of type ccˉssˉc \bar c s \bar s is calculated within a simple quark model with chromomagnetic interaction and effective quark masses extracted from meson and baryon spectra. It is tempting to see if this spectrum can accommodate the resonance Y(4140), observed by the CDF collaboration, but not yet confirmed. The results seem to favour the JPC^{PC} = 1++^{++} sector where the coupling to the VV channel is nearly as small as that of X(3872), when described as a ccˉqqˉc \bar c q \bar q tetraquark. This suggests that Y(4140) could possibly be the strange partner of X(3872), in a tetraquark interpretation. However the sector JPC^{PC} = 0++^{++} cannot entirely be excluded. This work questions the practice of extracting effective quark masses containing spin independent contributions, from mesons and baryons, to be used in multiquark systems as well.Comment: new additional parts, published versio

    ORION S-band data acquisition for S-Y calibration

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    Error sources in the Operational Radio Interferometry Observing Network (ORION) are addressed. Specifically, the performance of the S-band receiver and the optimum allocation of data volume between S- and X-band observations is studied. It is found that the requirements on the S-band receiver are not very stringent. The system temperature of the ORION S-band receiver has a very small effect on baseline determination accuracy. It is unwise to pay a high cost for an S-band receiver with a low system temperature; a system temperature as high as 240 K is tolerable. Only 20 to 40 percent of data volume is to be allocated to S-band observations for minimum baseline error. The error remains low over a rather wide range of data volume ratio. Hence precise allocation of the 14 pairs of the Mark 3 very long base interferometer data channels between S- and X-band observations is not critical
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