367 research outputs found
A sensitivity analysis on tidal stream turbine loads caused by operational, geometric design and inflow parameters
This paper presents a sensitivity analysis on a numerical tidal stream turbine model where a multitude of input parameters' effect on the load output were determined. The statistical procedure used, known as the Morris method, provided insight into the interactions between the parameters as well as showing their comparative influence on the turbine loading. The investigation covered parameters from the operational, geometric design and inflow variable domains where the rotor radius, current shear, blade root pitch, surface velocity and wave height were identified as most influential. The blade pitch was regarded as a surprisingly prominent influence on the loads. The turbine's operating depth and the blade geometry were also found to be of limited influence in the ranges investigated. In terms of load transmission into the internal components of a turbine's drive train, the rotor out-of-plane bending moment, or eccentric bending moment, was found to be a considerable contribution to the off-axis loads on the shaft. Therefore, special attention was paid to the input parameters' relationship to the eccentric load component by performing a detailed study on the load variations caused by the identified primary input parameters. It is concluded that performing a sensitivity analysis on a tidal stream turbine in a specific operating climate can yield insight to the expected load range and that the eccentric loading transmitted to the shaft is significant for most input cases
Scaling in Late Stage Spinodal Decomposition with Quenched Disorder
We study the late stages of spinodal decomposition in a Ginzburg-Landau mean
field model with quenched disorder. Random spatial dependence in the coupling
constants is introduced to model the quenched disorder. The effect of the
disorder on the scaling of the structure factor and on the domain growth is
investigated in both the zero temperature limit and at finite temperature. In
particular, we find that at zero temperature the domain size, , scales
with the amplitude, , of the quenched disorder as with and in two
dimensions. We show that , where is the
Lifshitz-Slyosov exponent. At finite temperature, this simple scaling is not
observed and we suggest that the scaling also depends on temperature and .
We discuss these results in the context of Monte Carlo and cell dynamical
models for phase separation in systems with quenched disorder, and propose that
in a Monte Carlo simulation the concentration of impurities, , is related to
by .Comment: RevTex manuscript 5 pages and 5 figures (obtained upon request via
email [email protected]
The exclusive and decays in the general two Higgs doublet model
We study the differential branching ratio, branching ratio and the
forward-backward asymmetry for the exclusive and decays in the general two Higgs doublet model including
the neutral Higgs boson effects. We analyze the dependencies of these
quantities on the neutral Higgs boson contributions and the other model
parameters. We observe that two Higgs doublet model with the neutral Higgs
boson exchanges gives quite sizable contributions to these observables for both
channels we consider. Since the neutral Higgs boson exchanges are the only
source of the forward-backward asymmetry for decay,
which is at the order of magnitude , measurement of this observable is
promising to determine the neutral Higgs boson effects.Comment: 27 pages, 18 eps figures, requires JHEP3.cls (included), replaced
with the version to appear in JHE
Leading logarithmic QCD corrections to the B_s --> \gamma \gamma decays in the two Higgs doublet model
We calculate the leading logarithmic QCD corrections to the decay B_s -->
\gamma \gamma in the two Higgs doublet model (2HDM) including O_7 type long
distance effects and estimate the restrictions of the 2HDM parameters, tan\beta
and m_H, using the experimental data of B --> X_s \gamma decay provided by the
CLEO collaboration. A lower bound for the charged Higgs mass m_H as a function
of the renormalization scale \mu is given for 2HDM model II. We further present
the dependencies of the branching ratio Br(B_s --> \gamma \gamma) and the ratio
|A^{+}|^2/|A^{-}|^2 on m_H and tan\beta including leading logarithmic QCD
corrections. The dependence on the renormalization scale is found to be strong
for both ratios. An additional uncertainty arises from the variation of the
parameters of the bound state model, (m_b, \bar{\Lambda}_s). We see, that to
look for charged Higgs effects the measurement of the branching ratio Br(B_s
--> \gamma \gamma) is promising.Comment: 25 pages, 19 figures (required epsf.sty
Rare B -> K^* l^+ l^- decay, two Higgs doublet model, and light cone QCD sum rules
The decay width, forward-backward asymmetry and lepton longitudinal and
transversal polarization for the exclusive K^* -> l^+ l^- decay in a two Higgs
doublet model are computed. It is shown that all these quantities are very
effective tools for establishing new physics.Comment: 18 pages, 7 figures, LaTeX formatte
Early stage scaling in phase ordering kinetics
A global analysis of the scaling behaviour of a system with a scalar order
parameter quenched to zero temperature is obtained by numerical simulation of
the Ginzburg-Landau equation with conserved and non conserved order parameter.
A rich structure emerges, characterized by early and asymptotic scaling
regimes, separated by a crossover. The interplay among different dynamical
behaviours is investigated by varying the parameters of the quench and can be
interpreted as due to the competition of different dynamical fixed points.Comment: 21 pages, latex, 7 figures available upon request from
[email protected]
Quantum Oscillations In Eufe2 As2 Single Crystals
Quantum oscillation measurements provide relevant information about the Fermi surface (FS) properties of strongly correlated metals. Here, we report on the Shubnikov-de Haas effect via high-field resistivity measurements of EuFe2As2 (Eu122) and BaFe2As2 (Ba122) single crystals. Although both pnictide compounds are isovalent with similar effective masses and density of states, at the Fermi level, our results reveal subtle changes in their fermiology. Remarkably, although the spin-density-wave (SDW) ordering temperature is higher in the Eu-rich end, Eu122 displays a much more isotropic and three-dimensional-like FS when compared with Ba122, in agreement with band structure calculations. Our experimental results suggest an anisotropic contribution of the Fe 3d orbitals to the FS in Ba122. We speculate that this orbital differentiation may be responsible for the suppression of the SDW phase in the FeAs-based compounds.9019Kamihara, Y., Watanabe, T., Hirano, M., Hosono, H., (2008) J. Am. Chem. Soc., 130, p. 3296. , JACSAT 0002-7863Rotter, M., Tegel, M., Johrendt, D., Schellenberg, I., Hermes, W., Pöttgen, R., (2008) Phys. Rev. B, 78, p. 020503. , (R). PRBMDO 1098-0121Rotter, M., Tegel, M., Johrendt, D., (2008) Phys. Rev. Lett., 101, p. 107006. , PRLTAO 0031-9007Wang, C., Li, L., Chi, S., Zhu, Z., Ren, Z., Li, Y., Wang, Y., Xu, Z., (2008) Europhys. Lett., 83, p. 67006. , EULEEJ 0295-5075Ishida, K., Nakai, Y., Hosono, H., (2009) J. Phys. Soc. Japan, 78, p. 062001. , JUPSAU 0031-9015Johnston, D.C., (2010) Adv. Phys., 59, p. 803. , ADPHAH 0001-8732Paglione, J., Greene, R.L., (2010) Nat. Phys., 6, p. 645. , 1745-2473Canfield, P.C., Bud'Ko, S.L., (2010) Annu. Rev. Cond. Mat. Phys., 1, p. 27. , 1947-5454Wen, H.H., Li, S., (2011) Annu. Rev. Cond. Mat. Phys., 2, p. 121. , 1947-5454Stewart, G.R., (2011) Rev. Mod. Phys., 83, p. 1589. , RMPHAT 0034-6861Urbano, R.R., Green, E.L., Moulton, W.G., Reyes, A.P., Kuhns, P.L., Bittar, E.M., Adriano, C., Pagliuso, P.G., (2010) Phys. Rev. Lett., 105, p. 107001. , PRLTAO 0031-9007Zhou, B., Zhang, Y., Yang, L.-X., Xu, M., He, C., Chen, F., Zhao, J.-F., Feng, D.L., (2010) Phys. Rev. B, 81, p. 155124. , PRBMDO 1098-0121De Jong, S., Van Heumen, E., Thirupathaiah, S., Huisman, R., Massee, F., Goedkoop, J.B., Ovsyannikov, R., Golden, M.S., (2010) Europhys. Lett., 89, p. 27007. , EULEEJ 0295-5075Ding, H., Nakayama, K., Richard, P., Souma, S., Sato, T., Takahashi, T., Neupane, M., Wang, N.L., (2011) J. Phys. Condens. Matt., 23, p. 135701. , JCOMEL 0953-8984Hin, Z.P., Haule, K., Kotliar, G., (2011) Nat. Mater., 10, p. 932. , 1476-1122Thirupathaiah, S., (2011), Ph.D. thesis, Helmholtz-Zentrum Berlin, Albert-Einstein-StrasseSchoenberg, D., (1984) Magnetic Oscillations in Metals, , (Cambridge University Press, Cambridge)Sebastian, S.E., (2012) Magnetism and Superconductivity: From Cuprates to Iron-Pnictides, p. 4. , in (Pan Stanford, Singapore), Chap.Sebastian, S.E., Gillett, J., Harrison, N., Lau, P.H.C., Singh, D.J., Mielke, C.H., Lonzarich, G.G., (2008) J. Phys.: Cond. Matt., 20, p. 422203. , JCOMEL 0953-8984Analytis, J.G., McDonald, R.D., Chu, J.-H., Riggs, S.C., Bangura, A.F., Kucharczyk, C., Johannes, M., Fisher, I.R., (2009) Phys. Rev. B, 80, p. 064507. , PRBMDO 1098-0121Terashima, T., Kurita, N., Tomita, M., Kihou, K., Lee, C.-H., Tomioka, Y., Ito, T., Nakajima, M., (2011) Phys. Rev. Lett., 107, p. 176402. , S. Uji,. PRLTAO 0031-9007Harrison, N., McDonald, R.D., Mielke, C.H., Bauer, E.D., Ronning, F., Thompson, J.D., (2009) J. Phys. Condens. Matter, 21, p. 322202. , JCOMEL 0953-8984Kurita, N., Kimata, M., Kodama, K., Harada, A., Tomita, M., Suzuki, H.S., Matsumoto, T., Terashima, T., (2011) J. Phys.: Conf. Ser., 273, p. 012098. , 1742-6596Jeevan, H.S., Hossain, Z., Kasinathan, D., Rosner, H., Geibel, C., Gegenwart, P., (2008) Phys. Rev. B, 78, p. 052502. , PRBMDO 1098-0121Jiang, S., Luo, Y., Ren, Z., Zhu, Z., Wang, C., Xu, X., Tao, Q., Xu, Z., (2009) New J. Phys., 11, p. 025007. , NJOPFM 1367-2630Garitezi, T.M., Adriano, C., Rosa, P.F.S., Bittar, E.M., Bufaical, L., De Almeida, R.L., Granado, E., Pagliuso, P.G., (2013) Brazilian J. Phys., 43, p. 223. , BJPHE6 0103-9733Blaha, P., Schwarz, K., Madsen, G.K.H., Kvasnick, D., Luitz, J., (2001) WIEN2K, , (Karlheinz Schwarz, Techn. Universitat Wien, Vienna, Austria)Perdew, J.P., Wang, Y., (1992) Phys. Rev. B, 45, p. 13244. , PRBMDO 0163-1829Anisimov, V.I., Zaanen, J., Andersen, O.K., (1991) Phys. Rev. B, 44, p. 943. , PRBMDO 0163-1829Xiao, Y., Su, Y., Meven, M., Mittal, R., Kumar, C.M.N., Chatterji, T., Price, S., Brueckel Th., (2009) Phys. Rev. B, 80, p. 174424. , PRBMDO 1098-0121Huang, Q., Qiu, Y., Bao, W., Green, M.A., Lynn, J.W., Gasparovic, Y.C., Wu, T., Chen, X.H., (2008) Phys. Rev. Lett., 101, p. 257003. , PRLTAO 0031-9007Xiao, Y., (2010) Phys. Rev. B, 81, p. 220406. , (R). PRBMDO 1098-0121Graf, D., Stillwell, R., Murphy, T.P., Park, J.-H., Palm, E.C., Schlottmann, P., McDonald, R.D., Tozer, S.W., (2012) Phys. Rev. B, 85, p. 134503. , PRBMDO 1098-0121Rosa, P.F.S., Adriano, C., Iwamoto, W., Garitezi, T.M., Grant, T., Fisk, Z., Pagliuso, P.G., (2012) Phys. Rev. B, 86, p. 165131. , PRBMDO 1098-0121Rosa, P.F.S., Adriano, C., Garitezi, T.M., Grant, T., Fisk, Z., Urbano, R.R., Pagliuso, P.G., (2014) Sci. Rep., 4, p. 6543. , 2045-2322Granado, E., Mendonça-Ferreira, L., Garcia, F., De M. Azevedo, G., Fabbris, G., Bittar, E.M., Adriano, C., Pagliuso, P.G., (2011) Phys. Rev. B, 83, p. 184508. , PRBMDO 1098-0121Raffius, H., Morsen, E., Mosel, B.D., Muller, W., Warmuth, W., Jeitschko, W., Terbuchte, L., Vomhof, T.J., (1993) J. Phys. Chem. Solids, 54, p. 135. , JPCSAW 0022-369
Possible Unconventional Superconductivity In Substituted Bafe 2 As 2 Revealed By Magnetic Pair-breaking Studies
The possible existence of a sign-changing gap symmetry in BaFe 2 As 2 -derived superconductors (SC) has been an exciting topic of research in the last few years. To further investigate this subject we combine Electron Spin Resonance (ESR) and pressure-dependent transport measurements to investigate magnetic pair-breaking effects on BaFe 1.9 M 0.1 As 2 (M = Mn, Co, Cu, and Ni) single crystals. An ESR signal, indicative of the presence of localized magnetic moments, is observed only for M = Cu and Mn compounds, which display very low SC transition temperature (T c) and no SC, respectively. From the ESR analysis assuming the absence of bottleneck effects, the microscopic parameters are extracted to show that this reduction of T c cannot be accounted by the Abrikosov-Gorkov pair-breaking expression for a sign-preserving gap function. Our results reveal an unconventional spin- and pressure-dependent pair-breaking effect and impose strong constraints on the pairing symmetry of these materials.4Kamihara, Y., Watanabe, T., Hirano, M., Hosono, H., Iron-based layered superconductor La[O12xFx]FeAs (x 5 0. 05-0. 12) with Tc 5 26 K (2008) J. Am. Chem. Soc., 130, p. 3296Rotter, M., Spin density wave anomaly at 140 K in the ternary iron arsenide BaFe2As2 (2008) Phys. Rev. B, 78, pp. 020503RIshida, K., Nakai, Y., Hosono, H., To what extent iron-pnictide new superconductors have been clarified: A progress report (2009) J. Phys. Soc. Japan, 78, p. 062001Hirschfeld, P.J., Korshunov, M.M., Mazin, I.I., Gap symmetry and structure of Fe-based superconductors (2011) Rep. Prog. Phys., 74, p. 124508Chubukov, A.V., Pairing mechanism in fe-based superconductors (2012) Annu. Rev. Cond. Mat. Phys., 3, p. 57Bittar, E.M., Co-substitution effects on the fe valence in the BaFe2As2 superconducting compound: A study of hard x-ray absorption spectroscopy (2011) Phys. Rev. Lett., 107, p. 267402Granado, E., Pressure and chemical substitution effects in the local atomic structure of BaFe2As2 (2011) Phys. Rev. B, 83, p. 184508Wadati, H., Elfimov, I., Sawatzky, G.A., Where are the extra d electrons in transition-metal-substituted iron pnictides? (2010) Phys. Rev. Lett., 105, p. 157004Ideta, S., Dependence of carrier doping on the impurity potential in transition-metal-substituted feas-based superconductors (2013) Phys. Rev. Lett., 110, p. 107007Berlijn, T., Lin, C.-H., Garber, W., Ku, W., Do transition-metal substitutions dope carriers in iron-based superconductors? (2012) Phys. Rev. Lett., 108, p. 207003Hin, Z.P., Haule, K., Kotliar, G., Kinetic frustration and the nature of the magnetic and paramagnetic states in iron pnictides and iron chalcogenides (2011) Nature Materials, 10, pp. 932a-935aRosa, P.F.S., Evolution of Eu21 spin dynamics in Ba12xEuxFe2As2 (2012) Phys. Rev. B, 86, p. 165131Rosa, P.F.S., (2014) Site Specific Spin Dynamics in BaFe2As2: Tuning the Ground State by Orbital Differentiation, , arxiv:1402. 2001v01Garitezi, T.M., Transport critical current measurements on a Cu-substituted BaFe2As2 superconductor (2014) J. Appl. Phys., 115, pp. 17D704Rosa, P.F.S., Pressure effects on magnetic pair-breaking in Mn- and Eusubstituted BaFe2As2 (2014) J. Appl. Phys., 115, pp. 17D702Thaler, A., Physical and magnetic properties of Ba(Fe12xMnx) 2As2 single crystals (2011) Phys. Rev. B, 84, p. 144528Et Al., A., Pressure effects on the electron-doped high Tc superconductor BaFe22xCoxAs2 (2008) J Phys. Cond. Mat., 20, p. 472201Et Al., D., Pressure versus concentration tuning of the superconductivity in Ba(Fe12xCox) 2As2 (2010) J. Phys. Soc. Japan, 79, p. 124705Yamaichi, S., Katagiri, T., Sasagawa, T., Uniaxial pressure effects on the transport properties in Ba(Fe12xCox) 2As2 single crystals (2013) Physica C, 494, pp. 62-64Canfield, P.C., Budko, S.L., Ni, N., Yan, J.Q., Kracher, A., Decoupling of the superconducting and magnetic/structural phase transitions in electron-doped BaFe2As2 (2009) Phys. Rev. B, 80, pp. 060501RKirshenbaum, K., Saha, S.R., Ziemak, S., Drye, T., Paglione, J., Universal pairbreaking in transition metal-substituted iron-pnictide superconductors (2012) Phys. Rev. B, 86, pp. 140505ROnari, S., Kontani, H., Violation of Andersonaŝ Theorem for the Sign-Reversing s-Wave State of Iron-Pnictide Superconductors (2009) Phys. Rev. Lett., 103, p. 177001Li, J., Superconductivity suppression of Ba0. 5K0. 5Fe222xMn2xAs2 single crystals by substitution of transition metal (M 5 Mn, Ru, Co, Ni, Cu, and Zn) (2012) Phys. Rev. B, 85, p. 214509Bang, Y., Choi, H.-Y., Won, H., Impurity effects on the s6-wave state of the ironbased superconductors (2009) Phys. Rev. B, 79, p. 054529Wang, Y., Kreisel, A., Hirschfeld, P.J., Mishra, V., Using controlled disorder to distinguish s6 and s11 gap structure in Fe-based superconductors (2013) Phys. Rev. B, 87, p. 094504Fernandes, R.M., Vavilov, M.G., Chubukov, A.V., Enhancement of Tc by disorder in underdoped iron pnictide superconductors (2012) Phys. Rev. B, 85, pp. 140512RNi, N., Temperature versus doping phase diagrams for Ba(Fe12xTMx) 2As2 (TM 5 Ni,Cu,Cu/Co) single crystals (2010) Phys. Rev. B, 82, p. 024519Patz, A., Ultrafast observation of critical nematic fluctuations and giant magnetoelastic coupling in iron pnictides (2014) Nature Comm., 5, p. 3229Abrikosov, A.A., Gorkov, L.P., Contribution to the theory of superconducting alloys with paramagnetic impurities (1961) Sov. Phys. JETP, 12, p. 1243Skalski, S., Betbeder-Matibet, O., Weiss, P.R., Properties of superconducting alloys containing paramagnetic impurities (1964) Phys. Rev., 136, pp. A1500-A1518Pagliuso, P.G., Electron spin resonance of Gd31 in the normal state of RNi2B2C (R 5 Y, Lu) (1998) Phys. Rev. B, 57, p. 3668Korringa, J., Nuclear magnetic relaxation and resonance line shift in metals (1950) Physica, 16, p. 601Rettori, C., Dynamic behavior of paramagnetic ions and conduction electrons in intermetallic compounds: GdxLu12xAl2 (1974) Phys. Rev. B, 10, p. 1826Davidov, D., Electron spin resonance of Gd in the intermetallic compounds YCu, YAg, and LaAg:Wave vector dependence of the exchange interaction (1973) Solid State Comm., 12, p. 621Narath, A., Weaver, H.T., Effects of electron-electron interactions on nuclear spin-lattice relaxation rates and knight shifts in alkali and noble metals (1968) Phys. Rev., 175, p. 373Shaw, R.W., Warren, W.W., Enhancement of the korringa constant in alkali metals by electron-electron interactions (1971) Phys. Rev. B, 3, p. 1562Bittar, E.M., Electron spin resonance study of the LaIn32xSnx superconducting system (2011) J. of Phys.: Cond. Matt., 23, p. 455701Maple, M.B., Dependence of s 2 f exchange on atomic number in rare earth dialuminides (1970) Solid State Comm., 8 (22), pp. 1915-1917Garitezi, T.M., Synthesis and characterization of BaFe2As2 single crystals grown by in-flux technique (2013) Brazilian Journal of Physics, 43, p. 223Alireza, P.L., Superconductivity up to 29 K in SrFe2As2 and BaFe2As2 at high pressures (2009) J. Phys. Condens. Matter, 21, p. 012208Rotter, M., Tegel, M., Johrendt, D., Superconductivity at 38 K in the Iron Arsenide Ba12xKxFe2As2 (2008) Phys. Rev. Lett., 101, p. 107006Wang, C., Thorium-dopingaînduced superconductivity up to 56âK in Gd12xThxFeAsO (2008) EPL, 83, p. 67006Shibata, A., Thorium-dopingaînduced superconductivity up to 56âK in Gd12xThxFeAsO (1986) J. Phys. Soc. Jpn., 55, p. 6Cooley, J.C., Aronson, M.C., Canfield, P.C., High pressures and the Kondo gap in Ce3Bi4Pt3 (1997) Phys. Rev. B, 55, p. 7533Oomi, G., Kagayama, T., Effect of pressure and magnetic field on the electrical resistivity of cerium kondo compounds (1996) J. Phys. Soc. Jpn., 65 (SUPPL. B), pp. 42-48Ramos, S.M., Superconducting quantum critical point in CeCoIn52xSnx (2010) Phys. Rev. Lett., 105, p. 126401Hering, E.N., Pressureâtemperatureâcomposition phase diagram of Ce2MIn8 (2006) Physica B: Cond. Matt., 378Dyson, F.J., Electron spin resonance absorption in metals. Ii. Theory of electron diffusion and the skin effect (1955) Phys. Rev., 98, p. 349Texier, Y., Mn local moments prevent superconductivity in iron pnictides Ba(Fe12xMnx) 2As2 (2012) EPL, 99, p. 17002Leboeuf, D., (2013) NMR Study of Electronic Correlations in Mn-doped Ba(Fe12xCox) 2As2 and BaFe(As12xPx) 2, p. 4969. , arXiv1310Suzuki, H., Absence of superconductivity in the hole-doped Fe pnictide Ba(Fe12xMnx) 2As2: Photoemission and x-ray absorption spectroscopy studies (2013) Phys. Rev. B, 88, pp. 100501RKim, M.G., Effects of transition metal substitutions on the incommensurability and spin fluctuations in BaFe2As2 by elastic and inelastic neutron scattering (2012) Phys. Rev. Lett., 109, p. 167003Et Al., F., Short-range magnetic order and effective suppression of superconductivity by manganese doping in LaFe12xMnxAsO12yFy (2013) Phys. Rev. B, 87, p. 174515Golubov, A.A., Mazin, I.I., Effect of magnetic and nonmagnetic impurities on highly anisotropic superconductivity (1997) Phys. Rev. B, 55, p. 15146Openov, L.A., Combined effect of nonmagnetic and magnetic scatterers on the critical temperatures of superconductors with different anisotropies of the gap (1997) JETP Lett., 66, p. 661Efremov, D.V., Disorder-induced transition between s6 and s11 states in two-band superconductors (2011) Phys. Rev. B, 84, p. 180512Tucker, G.S., Competition between stripe and checkerboard magnetic instabilities in Mn-doped BaFe2As2 (2012) Phys. Rev. B, 86, p. 020503Fernandes, R.M., Millis, A.J., Suppression of Superconductivity by Neel-Type magnetic fluctuations in the iron pnictides (2013) Phys. Rev. Lett., 110, p. 117004Chi, S., (2013) Sign Inversion in the Superconducting Order Parameter of LiFeAs Inferred from Bogoliubov Quasiparticle Interference. ArXiv:1308. 4413v1Johnston, D.C., (2010) Adv. Phys., 59, p. 803Paglione, J., Greene, R.L., Hightemperature superconductivity in iron-based materials (2010) Nature Phys., 6, p. 645Wen, H.H., Li, S., Materials and novel superconductivity in iron pnictide superconductors (2011) Annu. Rev. Cond. Mat. Phys., 2, p. 121Stewart, G.R., Superconductivity in iron compounds (2011) Rev. Mod. Phys., 83, pp. 1589-165
Tradable Credits Scheme on Urban Travel Demand: A Linear Expenditure System Approach and Simulation in Beijing
Using a linear expenditure system (LES) approach, we investigate the influences of a new mobility management measure, a tradable credits scheme (TCS), on the pattern of daily trips measured in kilometres. Generally, we assume that an individuals’ travel consists of a car mode and a non-car mode. The effects of the TCS are discussed from a microeconomic perspective and using a scenario simulation study for the municipality of Beijing. Whilst other research has shown that travellers trade their credits and are generally inclined to non-car mode, the implementation of the tradable credits scheme demonstrated here is that travellers are likely to restrain their use of both car and non-car travel modes. Furthermore, both car and non-car mode trips are shown to be price inelastic, whilst the cross-price elasticity for different districts demonstrates a complementary relationship between car and bus modes
Prediction of Neutrino Fluxes in the NOMAD Experiment
The method developed for the calculation of the flux and composition of the
West Area Neutrino Beam used by NOMAD in its search for neutrino oscillations
is described. The calculation is based on particle production rates computed
using a recent version of FLUKA and modified to take into account the cross
sections measured by the SPY and NA20 experiments. These particles are
propagated through the beam line taking into account the material and magnetic
fields they traverse. The neutrinos produced through their decays are tracked
to the NOMAD detector. The fluxes of the four neutrino flavours at NOMAD are
predicted with an uncertainty of about 8% for nu(mu) and nu(e), 10% for
antinu(mu), and 12% for antinu(e). The energy-dependent uncertainty achieved on
the R(e, mu) prediction needed for a nu(mu)->nu(e) oscillation search ranges
from 4% to 7%, whereas the overall normalization uncertainty on this ratio is
4.2%.Comment: 43 pages, 20 figures. Submitted to Nucl. Phys.
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