5,145 research outputs found

    Giant viscosity enhancement in a spin-polarized Fermi liquid

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    The viscosity is measured for a Fermi liquid, a dilute 3^3He-4^4He mixture, under extremely high magnetic field/temperature conditions (B14.8B \leq 14.8 T, T1.5T \geq 1.5 mK). The spin splitting energy μB\mu B is substantially greater than the Fermi energy kBTFk_B T_F; as a consequence the polarization tends to unity and s-wave quasiparticle scattering is suppressed for TTFT \ll T_F. Using a novel composite vibrating-wire viscometer an enhancement of the viscosity is observed by a factor of more than 500 over its low-field value. Good agreement is found between the measured viscosity and theoretical predictions based upon a tt-matrix formalism.Comment: 4 pages, 4 figure

    Generalized Arcsine Law and Stable Law in an Infinite Measure Dynamical System

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    Limit theorems for the time average of some observation functions in an infinite measure dynamical system are studied. It is known that intermittent phenomena, such as the Rayleigh-Benard convection and Belousov-Zhabotinsky reaction, are described by infinite measure dynamical systems.We show that the time average of the observation function which is not the L1(m)L^1(m) function, whose average with respect to the invariant measure mm is finite, converges to the generalized arcsine distribution. This result leads to the novel view that the correlation function is intrinsically random and does not decay. Moreover, it is also numerically shown that the time average of the observation function converges to the stable distribution when the observation function has the infinite mean.Comment: 8 pages, 8 figure

    Stable Spin Precession at one Half of Equilibrium Magnetization in Superfluid 3He-B

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    New stable modes of spin precession have been observed in superfluid 3He-B. These dynamical order parameter states include precession with a magnetization S=pS_{eq} which is different from the equilibrium value S_{eq}. We have identified modes with p=1, 1/2 and \approx 0. The p=1/2 mode is the second member of phase correlated states of a spin superfluid. The new states can be excited in the temperature range 1-T/T_c \lesssim 0.02 where the energy barriers between the different local minima of the spin-orbit energy are small. They are stable in CW NMR due to low dissipation close to T_c.Comment: submitted to Physical Review Letters, 4 pages, revtex, 4 Figures in ftp://boojum.hut.fi/pub/publications/lowtemp/LTL-96005.p

    Dark-bright magneto-exciton mixing induced by Coulomb interaction in strained quantum wells

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    Coupled magneto-exciton states between allowed (`bright') and forbidden (`dark') transitions are found in absorption spectra of strained In0.2_{0.2}Ga0.8_{0.8}As/GaAs quantum wells with increasing magnetic field up to 30 T. We found large (~ 10 meV) energy splittings in the mixed states. The observed anticrossing behavior is independent of polarization, and sensitive only to the parity of the quantum confined states. Detailed experimental and theoretical investigations indicate that the excitonic Coulomb interaction rather than valence band complexity is responsible for the splittings. In addition, we determine the spin composition of the mixed states.Comment: 4 pages, 4 figure

    Precise measurement of HFS of positronium

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    The ground state hyperfine splitting in positronium, ΔHFS\Delta _{\mathrm{HFS}}, is sensitive to high order corrections of QED. A new calculation up to O(α3)O(\alpha ^3) has revealed a 3.9σ3.9 \sigma discrepancy between the QED prediction and the experimental results. This discrepancy might either be due to systematic problems in the previous experiments or to contributions beyond the Standard Model. We propose an experiment to measure ΔHFS\Delta_{\mathrm{HFS}} employing new methods designed to remedy the systematic errors which may have affected the previous experiments. Our experiment will provide an independent check of the discrepancy. The measurement is in progress and a preliminary result of ΔHFS=203.399±0.029GHz(143ppm)\Delta_{\mathrm{HFS}} = 203.399 \pm 0.029 \mathrm{GHz} (143 \mathrm{ppm}) has been obtained. A measurement with a precision of O(1) ppm is expected within a few years.Comment: 5 pages, 6 figures, contributed to POSMOL 2009, will be published in J. Phys.: Conf. Serie

    Spin-wave scattering at low temperatures in manganite films

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    The temperature TT and magnetic field HH dependence of the resistivity ρ\rho has been measured for La0.8y_{0.8-y}Sr0.2_{0.2}MnO3_{3} (y=0 and 0.128) films grown on (100) SrTiO3_{3} substrates. The low-temperature ρ\rho in the ferromagnetic metallic region follows well ρ(H,T)=ρ0(H)+A(H)ωs/sinh(ωs/2kBT)+B(H)T7/2\rho (H,T)=\rho _{0}(H)+A(H)\omega_{s}/\sinh (\hbar \omega_{s}/2k_{B}T)+B(H)T^{7/2} with ρ0\rho _{0} being the residual resistivity. We attribute the second and third term to small-polaron and spin-wave scattering, respectively. Our analysis based on these scattering mechanisms also gives the observed difference between the metal-insulator transition temperatures of the films studied. Transport measurements in applied magnetic field further indicate that spin-wave scattering is a key transport mechanism at low temperatures.Comment: 5 pages, 4 figures. to appear in Phys. Rev.
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