3,264 research outputs found

    A Fermi Fluid Description of the Half-Filled Landau Level

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    We present a many-body approach to calculate the ground state properties of a system of electrons in a half-filled Landau level. Our starting point is a simplified version of the recently proposed trial wave function where one includes the antisymmetrization operator to the bosonic Laughlin state. Using the classical plasma analogy, we calculate the pair-correlation function, the static structure function and the ground state energy in the thermodynamic limit. These results are in good agreement with the expected behavior at ν=12\nu=\frac12.Comment: 4 pages, REVTEX, and 4 .ps file

    Effective mass of composite fermion: a phenomenological fit in with anomalous propagation of surface acoustic wave

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    We calculate the conductivity associated with the anomalous propagation of a surface acoustic wave above a two-dimensional electron gas at ν=1/2\nu=1/2. Murthy-Shankar's middle representation is adopted and a contribution to the response functions beyond the random phase approximation has been taken into account. We give a phenomenological fit for the effective mass of composite fermion in with the experimental data of the anomalous propagation of surface acoustic wave at ν=1/2\nu=1/2 and find the phenomenological value of the effective mass is several times larger than the theoretical value mth∗=6ϵ/e2l1/2m_{th}^*=6\epsilon/e^2l_{1/2} derived from the Hartree-Fock approximation. We compare our phenomenologically fitting composite fermion effective mass with those appeared in the measurements of the activation energy and the Shubnikov-de Haas effect and find that our result is fairly reasonable.Comment: 8 pages, 5 figures, the longer version of cond-mat/9801131 with crucial corrections, accepted for publication by PR

    The role of the chemokine receptor CXCR4 in infection with feline immunodeficiency virus

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    Infection with feline immunodeficiency virus (FIV) leads to the development of a disease state similar to AIDS in man. Recent studies have identified the chemokine receptor CXCR4 as the major receptor for cell culture-adapted strains of FIV, suggesting that FIV and human immunodeficiency virus (HIV) share a common mechanism of infection involving an interaction between the virus and a member of the seven transmembrane domain superfamily of molecules. This article reviews the evidence for the involvement of chemokine receptors in FIV infection and contrasts these findings with similar studies on the primate lentiviruses HIV and SIV (simian immunodeficiency virus)

    Diffusion Thermopower at Even Denominator Fractions

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    We compute the electron diffusion thermopower at compressible Quantum Hall states corresponding to even denominator fractions in the framework of the composite fermion approach. It is shown that the deviation from the linear low temperature behavior of the termopower is dominated by the logarithmic temperature corrections to the conductivity and not to the thermoelectric coefficient, although such terms are present in both quantities. The enhanced magnitude of this effect compared to the zero field case may allow its observation with the existing experimental techniques.Comment: Latex, 12 pages, Nordita repor

    Weiss Oscillations in Surface Acoustic Wave Propagation

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    The interaction of a surface acoustic wave (SAW) with a a two-dimensional electron gas in a periodic electric potential and a classical magnetic field is considered. We calculate the attenuation of the SAW and its velocity change and show that these quantities exhibit Weiss oscillations.Comment: 4 pages REVTEX, 2 figures included as eps file

    Transition from an electron solid to the sequence of fractional quantum Hall states at very low Landau level filling factor

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    At low Landau level filling of a two-dimensional electron system, typically associated with the formation of an electron crystal, we observe local minima in Rxx at filling factors nu=2/11, 3/17, 3/19, 2/13, 1/7, 2/15, 2/17, and 1/9. Each of these developing fractional quantum Hall (FQHE) states appears only above a filling factor-specific temperature. This can be interpreted as the melting of an electron crystal and subsequent FQHE liquid formation. The observed sequence of FQHE states follow the series of composite fermion states emanating from nu=1/6 and nu=1/8

    Specific Heat Study on a Novel Spin-Gapped System : (CH_3)_2NH_2CuCl_3

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    Specific heat measurements down to 120mK have been performed on a quasi-one-dimensional S=1/2S=1/2 spin-gapped system (CH3_3)2_2NH2_2CuCl3_3 in a magnetic field up to 8 T. This compound has a characteristic magnetization curve which shows a gapless ground state and a plateau at 1/2 of the saturation value. We have observed a spontaneous antiferromagnetic ordering and a field-induced one below and above the 1/2 plateau field range, respectively. The field versus temperature phase diagram is quite unusual and completely different from those of the other quantum spin systems investigated so far. In the plateau field range, a double-structure in the specific heat is observed, reflecting the coexistence of ferromagnetic and antiferromagnetic excitations. These behaviors are discussed on the basis of a recently proposed novel quantum spin chain model consisting of weakly coupled ferromagnetic and antiferromagnetic dimers.Comment: 4 pages, 3 figures, submitted to J. Phys. Soc. Jp

    Relation between variations in the intensity of the zonal circulation of the atmosphere and the displacements of the permanent centers of action atmosphere and the displacements of the permanent centers of action

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    This paper attempts to interpret, from a single point of view, several at first sight independent phenomena brought into focus through the synoptic investigations carried on at the Massachusetts Institute of Technology during the last few years…

    Composite fermions close to the one-half filling of the lowest Landau level revisited

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    By strictly adhering to the microscopic theory of composite fermions for the Landau-level filling fractions nu_e = p/(2 p + 1), we reproduce, with remarkable accuracy, the surface-acoustic-wave (SAW)-based experimental results by Willett and co-workers concerning two-dimensional electron systems with nu_e close to 1/2. Our results imply that the electron band mass m_b, as distinct from the composite fermion mass m_*, must undergo a substantial increase under the conditions corresponding to nu_e approximately equal to 1/2. In view of the relatively low aerial electronic densities n_e to which the underlying SAW experiments correspond, our finding conforms with the experimental results by Shashkin et al. [Phys. Rev. B 66, 073303 (2002)], concerning two-dimensional electrons in silicon, that signal sharp increase in m_b for n_e decreasing below approximately 2 x 10^{11} cm^{-2}. We further establish that a finite mean-free path l_0 is essential for the observed linearity of the longitudinal conductivity sigma_{xx}(q) as deduced from the SAW velocity shifts.Comment: 5 pages, 2 postscript figure

    Effective Mass of the Four Flux Composite Fermion at ν=1/4\nu = 1/4

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    We have measured the effective mass (m∗m^*) of the four flux composite fermion at Landau level filling factor ν=1/4\nu = 1/4 (4^4CF), using the activation energy gaps at the fractional quantum Hall effect (FQHE) states ν\nu = 2/7, 3/11, and 4/15 and the temperature dependence of the Shubnikov-de Haas (SdH) oscillations around ν=1/4\nu = 1/4. We find that the energy gaps show a linear dependence on the effective magnetic field BeffB_{eff} (≡B−Bν=1/4\equiv B-B_{\nu=1/4}), and from this linear dependence we obtain m∗=1.0mem^* = 1.0 m_e and a disorder broadening Γ∼\Gamma \sim 1 K for a sample of density n=0.87×1011n = 0.87 \times 10^{11} /cm2^2. The m∗m^* deduced from the temperature dependence of the SdH effect shows large differences for ν>1/4\nu > 1/4 and ν<1/4\nu < 1/4. For ν>1/4\nu > 1/4, m∗∼1.0mem^* \sim 1.0 m_e. It scales as Bν\sqrt{B_{\nu}} with the mass derived from the data around ν=1/2\nu =1/2 and shows an increase in m∗m^* as ν→1/4\nu \to 1/4, resembling the findings around ν=1/2\nu =1/2. For ν<1/4\nu < 1/4, m∗m^* increases rapidly with increasing BeffB_{eff} and can be described by m∗/me=−3.3+5.7×Beffm^*/m_e = -3.3 + 5.7 \times B_{eff}. This anomalous dependence on BeffB_{eff} is precursory to the formation of the insulating phase at still lower filling.Comment: 5 pages, 3 figure
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