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Biomedical subjects

J E Sipe

Publications and source records attributed to J E Sipe.

18 recordsLinked to original sources

Minimizing finite-size effects in artificial resonance tunneling structures.

We consider finite-size effects in coupled cavity structures. Starting with microring resonator structures well described by transfer matrices, we obtain conditions that lead to the minimization of finite-size effects. Our approach does not require numerical optimization and requires only slight modification of design parameters guided by closed-form analytical expressions. Using a Breit-Wigner scattering formalism, we demonstrate that the scheme can be used to minimize finite-size effects in a general class of coupled cavity structures. The strength of the present technique lies in its simplicity and its applicability to a wide variety of structures described by tight-binding formalisms.

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Generation of spin currents via Raman scattering.

We show theoretically that stimulated spin-flip Raman scattering can be used to inject spin currents in doped semiconductors with spin-split bands. A pure spin current, where oppositely oriented spins move in opposite directions, can be injected in zinc blende crystals and structures. The calculated spin current should be detectable by pump-probe optical spectroscopy and anomalous Hall effect measurement.

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Extrinsic optical scattering loss in photonic crystal waveguides: role of fabrication disorder and photon group velocity.

Formulas are presented that provide clear physical insight into the phenomenon of extrinsic optical scattering loss in photonic crystal waveguides due to random fabrication imperfections such as surface roughness and disorder. Using a photon Green-function-tensor formalism, we derive explicit expressions for the backscattered and total transmission losses. Detailed calculations for planar photonic crystals yield extrinsic loss values in overall agreement with experimental measurements, including the full dispersion characteristics. We also report that loss in photonic crystal waveguides scales inversely with group velocity, at least, thereby raising serious questions about future low-loss applications based on operating frequencies that approach the photonic band edge.

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Nonlinear optical interactions of wave packets in photonic crystals: Hamiltonian dynamics of effective fields.

We develop an effective-field formalism that is suitable for describing nonlinear interactions of multiple wave packets in photonic crystals of arbitrary dimensionality. The theory is valid for "high-contrast" variations of the refractive index in the photonic crystal, provided dispersion and absorption effects can be neglected; it is based on a Hamiltonian formulation of the underlying Maxwell equations. We show that the dynamical equations for the effective fields are similar to those commonly used in nonlinear optics of homogeneous media, but with coefficients determined from the photonic band structure. We can introduce an effective energy density and an effective Poynting vector, expressed in terms of the effective fields, that satisfy a continuity equation. We illustrate our approach with a solution of the problem of degenerate optical parametric amplification in the undepleted pump approximation, and by considering the linear electro-optic effect as a quadratic nonlinear optical process.

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Carrier-envelope phase-controlled quantum interference of injected photocurrents in semiconductors.

We demonstrate quantum interference control of injected photocurrents in a semiconductor using the phase stabilized pulse train from a mode-locked Ti:sapphire laser. Measurement of the comb offset frequency via this technique results in a signal-to-noise ratio of 40 dB (10 Hz resolution bandwidth), enabling solid-state detection of carrier-envelope phase shifts of a Ti:sapphire oscillator.

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Effective field theory for the nonlinear optical properties of photonic crystals.

We introduce an effective field theory for the nonlinear optics of photonic crystals of arbitrary dimensionality. Based on a canonical Hamiltonian formulation of Maxwell's equations, canonical effective fields are introduced to describe the electromagnetic field. Conserved quantities are easily constructed and their physical significance identified; the formalism can be easily quantized. We illustrate the approach by considering a periodic Kerr medium, and show how the nonlinear coupled mode and nonlinear Schrödinger equations emerge. We extend the latter to treat optical shock effects, and compare our canonical formulation with earlier treatments.

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Depositing light in a photonic stop gap by use of Kerr nonlinear microresonators.

We show theoretically that it is possible to trap light in a microresonator structure by use of four-wave mixing. The efficiency of the parametric process is substantially increased by the high group delay of light inside the structure. The energy that is trapped has a half-life of approximately 500 ps in the presence of both linear and nonlinear loss in the channel waveguides and resonators. We also demonstrate that the energy can be extracted from the cavity with a similar process.

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Direct observation of optically injected spin-polarized currents in semiconductors.

Quantum interference of one- and two-photon excitation of unbiased semiconductors yields ballistic currents of carriers. The magnitudes and directions of the currents and the spin orientations of the carriers are controlled by the polarization and relative phase of the exciting femtosecond laser fields. We provide direct experimental evidence for the spin polarization of the optically injected spin currents by detecting a phase-dependent spatial shift of the circularly polarized photoluminescence in cubic ZnSe.

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Quantum interference control of ballistic pure spin currents in semiconductors.

We demonstrate all-optical quantum interference injection and control of a ballistic pure spin current (without an accompanying charge current) in GaAs/AlGaAs quantum wells, consisting of spin-up electrons traveling in one direction and spin-down electrons traveling in the opposite direction. This current is generated through quantum interference of one- and two-photon absorption of approximately 100 fs phase-locked pulses that have orthogonal linear polarizations. We use a spatially resolved pump-probe technique to measure carrier movement of approximately 10 nm. Results agree with recent theoretical predictions.

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Hamiltonian formulation of the nonlinear coupled mode equations.

We derive a canonical Hamiltonian formulation of the nonlinear coupled mode equations (CME) that govern the dynamics of pulse propagation in a one-dimensional, periodic Kerr medium when the frequency content of the pulse is in the vicinity of a photonic band gap, and sufficiently narrow relative to a carrier frequency. The Hamiltonian is equal to the energy in the electromagnetic field. We show that even for large photonic band gaps (25% of the Bragg frequency), the CME give an excellent approximation to the dispersion relation of the linear, periodic medium. This suggests that two- and three-dimensional photonic band-gap materials, which necessarily have large index contrasts, might be effectively described by a set of generalized CME.

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Canonical Hamiltonian formulation of the nonlinear Schrödinger equation in a one-dimensional, periodic Kerr medium.

A canonical Hamiltonian formulation of the nonlinear Schrödinger equation has been derived in this paper. This formulation governs the dynamics of pulse propagation in a one-dimensional, periodic Kerr medium when the frequency content of the pulse is sufficiently narrow relative to a carrier frequency, and sufficiently far removed from a photonic band gap of the medium. Our Hamiltonian is numerically equal to the energy, and our fields obey canonical commutation relations, so the theory can easily be quantized. We clarify the nature of the conserved quantities associated with simple symmetries.

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Optical pulse propagation in nonlinear photonic crystals.

We present a formalism for optical pulse propagation in nonlinear photonic crystals of arbitrary dimensionality. Using a multiple-scale analysis, we derive the dynamical nonlinear Schrödinger equation obeyed by the envelope function modulating an underlying Bloch function. Effective coefficients appear in that equation characterizing the effects of Kerr nonlinearity, linear gain or loss, and material dispersion. They depend on how the underlying Bloch function "samples" these effects in the photonic crystal, and require for their calculation a specification of these effects throughout the photonic crystal, and the calculated bandstructure of the photonic crystals in the linear, nondispersive limit. We show that wave packets from different bands can experience significantly modified effective material properties.

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Optically injected spin currents in semiconductors.

We show that quantum interference of one and two photon absorption from a two color field allows one to optically inject ballistic spin currents in unbiased semiconductors. The spin currents can be generated with or without an accompanying electrical current and can be controlled using the relative phase of the two colors. We characterize the injected spin currents using symmetry arguments and an eight-band Kane model.

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Generation of soliton oscillations in nonlinear quadratic materials.

We show analytically and numerically that the generation of long-lasting soliton oscillations in resonant chi(2) optical materials possesses a threshold for the amplitude of a fundamental wave. The persistent oscillations of solitary waves reported by Etrich et al. [Phys. Rev. E 54, 4321 (1996)] are found to appear for finite values of the wave amplitude.

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Ribosomal ribonucleic acid-adenine (N 6 -) methylase of Escherichia coli strain B: ionic and substrate site requirements.

These investigations are concerned with the ionic and substrate-site requirements of ribosomal ribonucleic acid (rRNA)-adenine (N(6)-) methylase of Escherichia coli B. The methylase was essentially inactive in solutions of low ionic strength. The addition of MgCl(2) (optimal at 5 mM) or; to a lesser degree, KCl (optimal at 45 mM) stimulated the rate of methylation; the combination of MgCl(2) and KCl stimulated methylation to an extent equivalent to the sum of the stimulation of each acting alone. The extent of nonspecific binding of the methylase to rRNA decreased as the ionic strength of the solution increased. In the absence of ions, dimethylsulfoxide (DMSO), a nucleic acid denaturing agent, had little influence on the rate of methylation; however, DMSO plus KCl synergistically increased both the rate and the extent of methylation to a greater degree than the combination of Mg(2+) plus K(+). NH(4) (+) was less effective than K(+), and the divalent Mg(2+) offered little stimulation. Monovalent anions (acetate, nitrate, and chloride) were equally effective, whereas divalent SO(4) (2-) was decidedly inhibitory. The appropriate ionic milieu of mono- and divalent cations was required to provide the appropriate conformation of the rRNA and to facilitate specific interactions of the methylase and its recognition sites in the rRNA, while decreasing nonspecific ionic binding of the methylase to rRNA. DMSO may facilitate methylation by increasing the number of substrate sites exposed in single-stranded regions of the rRNA. Nonmethylatable rRNA species served as competitive inhibitors, whereas the polyanions deoxyribonucleic acid, transfer RNA, and polyadenylic acid were inactive. Micrococcus lysodeikticus and Bacillus subtilis rRNA, methylated by the methylase, each contained two distinct heptanucleotides containing newly synthesized 6-methyladenine moieties. The data are consistent with the view that E. coli strain B possesses two species of rRNA-adenine (N(6)-) methylases, each of which recognizes a specific adenine moiety in a unique pentapurine nucleotide sequence in a single-stranded region of rRNA.

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Characterization of S-adenosylmethionine: ribosomal ribonucleic acid-adenine (N 6 -) methyltransferase of Escherichia coli strain B.

This study is concerned with the isolation and characterization of the enzyme, S-adenosylmethionine:ribosomal ribonucleic acid-adenine (N(6-)) methyl-transferase [rRNA-adenine (N(6)-) methylase] of Escherichia coli strain B, which is responsible for the formation of N(6)-methyladenine moieties in ribosomal ribonucleic acids (rRNA). A 1,500-fold purified preparation of the species-specific methyltransferase methylates a limited number of adenine moieties in heterologous rRNA (Micrococcus lysodeikticus and Bacillus subtilis) and methyl-deficient homologous rRNA. The site recognition mechanism does not require intact 16 or 23S rRNA. The enzyme does not utilize transfer ribonucleic acid as a methyl acceptor nor does it synthesize 2-methyladenine or N(6)-dimethyladenine moieties. Mg(2+), spermine, K(+), and Na(+) increase the reaction rate but not the extent of methylation; elevated concentrations of the cations inhibit markedly. The purified preparations utilize 9-beta-ribosyl-2,6-diaminopurine (DAPR) as a methyl acceptor with the synthesis of 9-beta-ribosyl-6-amino-2-methylaminopurine. A comparison of the two activities demonstrated that one methyltransferase is responsible for the methylation of both DAPR and rRNA. This property provides a sensitive assay procedure unaffected by ribonucleases and independent of any specificity exhibited by rRNA methyl acceptors.

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