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Steven H. Simon

Publications and source records attributed to Steven H. Simon.

161 records · Page 9Linked to original sources
arXiv1999

The half-filled Landau level - composite fermions and dipoles

The composite-fermion approach as formulated in the fermion Chern-Simons theory has been very successful in describing the physics of the lowest Landau level near Landau level filling factor 1/2. Recent work has emphasized the fact that the true quasiparticles at these filling factors are electrically neutral and carry an electric dipole moment. In a previous work, we discussed at length two formulations in terms of dipolar quasiparticles. Here we briefly review one approach - termed electron-centered quasiparticles - and show how it can be extended from 1/2 to nearby filling factors where the quasiparticles carry both an electric dipole moment and an overall charge.

cond-mat.mes-hall↗
arXiv1999

Comment on ``Evidence for Anisotropic State of Two-Dimensional Electrons in High Landau Levels''

In a recent letter M. Lilly et al [PRL 82, 394 (1999)] have shown that a highly anisotropic state can arise in certain two dimensional electron systems. In the large square samples studied, resistances measured in the two perpendicular directions are found to have a ratio that may be 60 or larger at low temperature and at certain magnetic fields. In Hall bar measurements, the anisotropy ratio is found to be much smaller (roughly 5). In this comment we resolve this discrepancy by noting that the anisotropy of the underlying sheet resistivities is correctly represented by Hall bar resistance measurements but shows up exponentially enhanced in resistance measurements on square samples due to simple geometric effects. We note, however, that the origin of this underlying resistivity anisotropy remains unknown, and is not addressed here.

cond-mat.mes-hall↗
arXiv1998

The Chern-Simons Fermi Liquid Description of Fractional Quantum Hall States

The composite fermion picture has had a remarkable number of recent successes both in the description of the fractional quantized Hall states and in the description on the even denominator Fermi liquid like states. In this review we give an introductory account of the Chern-Simons fermion theory, focusing on the description of the even denominator states as unusual Fermi liquids. Contents include: 1. Introduction 2. Introduction to Chern-Simons Fermions 3. RPA 4. Landau Fermi Liquid Theory and MRPA 5. Magnetization and M2RPA 6. Perturbative Approaches and Trouble in the Infrared 7. Wavefunction Picture of Composite Fermions and Dipole Approach 8. Selected Experiments 9. Last Words

cond-mat.mes-hall↗
arXiv1998

Hall effect in the perovskite manganites

We compute the zero temperature phase diagram and the Hall response of the doped perovskite manganites within the model of double exchange and Jahn-Teller coupling, employing the large dimensionality approximation proposed by Millis et al. We find that in this scenario a ``hole - like'' $R_H$ for the hole doped manganites, as observed at low temperature by Matl et al., can be obtained only when lattice distortions persist in the metallic state at zero temperature. The calculated temperature dependence of $R_H$ seems to be consistent with the measured ``normal'' Hall coefficient in thin films.

cond-mat.str-el↗
arXiv1997

Derivative relation for thermopower in the quantum Hall regime

Recently, Tieke et al (to be published in PRL) have observed the relation S_{yx} = alpha B dS_{xx}/dB for the components of the thermopower tensor in the quantum Hall regime, where alpha is a constant and B is the magnetic field. Simon and Halperin (PRL 73, 3278 (1994)) have suggested that an analogous relation observed for the resistivity tensor R_{xx} = αB dR_{xy}/dB can be explained with a model of classical transport in an inhomogeneous medium where the local Hall resistivity is a function of position and the local dissipative resistivity is a small constant. In the present paper, we show that this new thermopower relation can be explained with a similar model.

cond-mat.mes-hall↗
arXiv1997

Reply to Comment on ``Scaling of the quasiparticle spectrum for d-wave superconductors''

Volovik and Kopnin make two seperate points regarding our recent paper (S. H. Simon and P. A. Lee, PRL 78, 1548 (1997); cond-mat/9611133). First they note that the scaling regime we address in our paper is limited by the curvature of the Fermi surface, and secondly they note that the crossover scale derived in our paper is incorrect. These points are valid and are discussed in this reply. With the exception of the incorrectly predicted crossover scale, the results of our paper remain unchanged.

cond-mat.supr-con↗
arXiv1996

Scaling of the quasiparticle spectrum for d-wave superconductors

In finite magnetic field H, the excitation spectrum of the low energy quasiparticles in a 2 dimensional d-wave superconductor exhibits a scaling with respect to $H^{1/2}$. This property can be used to calculate scaling relations for various physical quantities at low temperature T. As examples, we make predictions for the scaling behavior of the finite magnetic field specific heat, quasiparticle magnetic susceptibility, optical conductivity tensor, and thermal conductivity tensor. These predictions are compatible with existing experimental data. Most notably, the thermal Hall coefficient $κ_{xy}$ measured by Krishana et al. in YBCO is found to scale as $κ_{xy} \sim T^2 F(αT/H^{1/2})$ for $T \lesssim 30 K$ in agreement with our predictions, where $α$ is a constant and F is a scaling function.

cond-mat.supr-con↗
arXiv1996

Towards a Fermi Liquid Theory of the $ν$=1/2 State : Magnetized Composite Fermions

The Fermionic Chern-Simons approach has had remarkable success in the description of quantum Hall states at even denominator filling fractions $ν=\frac{1}{2m}$. In this paper we review a number of recent works concerned with modeling this state as a Landau-Silin Fermi liquid. We will then focus on one particular problem with constructing such a Landau theory that becomes apparent in the limit of high magnetic field, or equivalently the limit of small electron band mass $m_b$. In this limit, the static response of electrons to a spatially varying magnetic field is largely determined by kinetic energy considerations. We then remedy this problem by attaching an orbital magnetization to each fermion to separate the current into magnetization and transport contributions, associated with the cyclotron and guiding center motions respectively. This leads us to a description of the $ν=\frac{1}{2m}$ state as a Fermi liquid of magnetized composite fermions which correctly predicts the $m_b$ dependence of the static and dynamic response in the limit $m_b \rightarrow 0$. As an aside, we derive a sum rule for the Fermi liquid coefficients for the Chern-Simons Fermi liquid. This paper is intended to be readable by people who may not be completely familiar with this field.

cond-mat↗
arXiv1996

Coupling of Surface Acoustic Waves to a Two Dimensional Electron Gas

When a surface acoustic wave (SAW) is coupled piezoelectrically to a two dimensional electron gas (2DEG), a velocity shift and attenuation of the SAW are induced that reflect the conductivity of the 2DEG. This paper considers the case of a AlGaAs heterostructure with a 2DEG a distance $d$ from a (100) surface of the crystal where the SAWs are propagated in the [011] direction at wavevector $q$. It is found that the velocity shift $Δv_s$ and the attenuation coefficient $κ$ satisfy the well known equation $(Δv_s/v_s) - (i κ/q) = (α^2/2)/\left(1 + \frac{i σ_{xx}(q,ω)} {σ_m}\right)$ where $σ_{xx}(q,ω)$ is the complex conductivity at wavevector $q$ and frequency $ω= v_s q$ with $v_s$ the velocity of the SAW. The coefficients $α$ and $σ_m$ are calculated and it is found that $α$ has a nontrivial dependence on the product $qd$.

cond-mat↗
arXiv1996

Composite Fermions with Orbital Magnetization

For quantum Hall systems, in the limit of large magnetic field (or equivalently small electron band mass $m_b$), the static response of electrons to a spatially varying magnetic field is largely determined by kinetic energy considerations. This response is not correctly given in existing approximations based on the Fermion Chern-Simons theory of the partially filled Landau level. We remedy this problem by attaching an orbital magnetization to each fermion to separate the current into magnetization and transport contributions, associated with the cyclotron and guiding center motions respectively. This leads to a Chern-Simons Fermi liquid description of the $ν=\frac{1}{2m}$ state which correctly predicts the $m_b$ dependence of the static and dynamic response in the limit $m_b \rightarrow 0$.

cond-mat↗
arXiv1995

Problems With the Vortex-Boson Mapping in 1+1 Dimensions

Using the well known boson mapping, we relate the transverse magnetic susceptibility of a system of flux vortices in 1+1 dimensions to an appropriately defined conductivity of a one-dimensional boson system. The tilt response for a system free of disorder is calculated directly, and it is found that a subtle order of limits is required to avoid deceptive results.

cond-mat↗
arXiv1995

Commensurability Effects in Large Josephson Junctions

Two types of commensurability effects are possible in a large Josephson junction patterned with columnar defects. The first occurs for a periodic array of pins when the mean fluxon spacing (tuned by the magnitude of the applied in--plane magnetic field) is a rational fraction of the defect spacing. We show that this effect leads, under fairly general conditions, to a mapping of the behavior of the Josephson junction near the commensurate field values to that of a zero field junction with an effective Josephson penetration depth. The second occurs for more general arrangements of pinning sites, when the orientation of the Josephson vortex lattice (tuned by the direction of the applied field) nearly matches the orientation of the defects. We investigate this tilt response in the limit of a single Josephson vortex. The results are compared, where possible, to recent experiments. As an aside from our main analysis, we prove that, contrary to recent claims in the literature, the critical current density vanishes in the thermodynamic limit, even in the presence of (non--pathologically distributed) pinning disorder

cond-mat↗
arXiv1994

Explanation for the Resistivity Law in Quantum Hall System

We consider a 2D electron system in a strong magnetic field, where the local Hall resistivity $ρ_{xy}(\vec r)$ is a function of position and $ρ_{xx}(\vec r)$ is small compared to $ρ_{xy}$. Particularly if the correlations fall off slowly with distance, or if fluctuations exist on several length scales, one finds that the macroscopic longitudinal resistivity $R_{xx}$ is only weakly dependent on $ρ_{xx}$ and is approximately proportional to the magnitude of fluctuations in $ρ_{xy}$. This may provide an explanation of the empirical law $R_{xx} \propto B \frac{dR_{xy}}{dB}$ where $R_{xy}$ is the Hall resistance, and $B$ is the magnetic field.

cond-mat↗
arXiv1994

Response Function of the Fractional Quantized Hall State on a Sphere I: Fermion Chern-Simons Theory

Using a well known singular gauge transformation, certain fractional quantized Hall states can be modeled as integer quantized Hall states of transformed fermions interacting with a Chern-Simons field. In previous work we have calculated the electromagnetic response function of these states at arbitrary frequency and wavevector by using the Random Phase Approximation (RPA) in combination with a Landau Fermi Liquid approach. We now adopt these calculations to a spherical geometry in order to facilitate comparison with exact diagonalizations performed on finite size systems.

cond-mat↗
arXiv1993

Finite-Wavevector Electromagnetic Response of Fractional Quantized Hall States

A fractional quantized Hall state with filling fraction $ν= p/(2mp+1)$ can be modeled as an integer quantized Hall state of transformed fermions, interacting with a Chern-Simons field. The electromagnetic response function for these states at arbitrary frequency and wavevector can be calculated using a semiclassical approximation or the Random Phase Approximation (RPA). However, such calculations do not properly take into account the large effective mass renormalization which is present in the Chern-Simons theory. We show how the mass renormalization can be incorporated in a calculation of the response function within a Landau Fermi liquid theory approach such that Kohn's theorem and the $f$-sum rules are properly satisfied. We present results of such calculations.

cond-mat↗