Search results for "waves"

showing 10 items of 1766 documents

Ultracompact and Low-Power Plasmonic MZI Switch Using Cyclomer Loading

2015

We present a $2\times 2$ hybrid silicon-plasmonic thermooptic (TO) asymmetric Mach–Zehnder interferometric (MZI) switch having only 40- $\mu \text{m}$ long active cyclomer-loaded plasmonic phase arms. It requires less than 12 mW of power and has 2/5- $\mu \text{s}$ ON/OFF-times, respectively, a modulation depth higher than 90% and a 13.2-dB extinction ratio. Data traffic evaluation has been carried out using 10-Gb/s nonreturn-to-zero streams, yielding error-free operation at both switching states with power penalties ranging between 1 to 4.8 dB. The use of the cyclomer loading having a higher TO coefficient than polymethyl methacrylate has resulted to the smallest footprint among plasmonic …

PhysicsExtinction ratiobusiness.industryPhase (waves)Optical switchAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic MaterialsPower (physics)Amplitude modulationInterferometryOpticsElectrical and Electronic EngineeringAdaptive opticsbusinessPlasmonIEEE Photonics Technology Letters
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Nonlinear pulse shaping and polarization dynamics in mode-locked fiber lasers

2014

International audience; We review our recent progress on the study of new nonlinear mechanisms of pulse shaping in passively mode-locked fiber lasers. These include a mode-locking regime featuring pulses with a triangular distribution of the intensity, and spectral compression arising from nonlinear pulse propagation. We also report on our recent experimental studies unveiling new types of vector solitons with processing states of polarization for multi-pulse and tightly bound-state soliton (soliton molecule) operations in a carbon nanotube (CNT) mode-locked fiber laser with anomalous dispersion cavity.

PhysicsFemtosecond pulse shaping[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics][ PHYS.PHYS.PHYS-OPTICS ] Physics [physics]/Physics [physics]/Optics [physics.optics]business.industryStatistical and Nonlinear PhysicsCondensed Matter PhysicsPolarization (waves)Pulse shapingNonlinear systemOpticsFiber laserOptoelectronicsSolitonbusinessUltrashort pulseBandwidth-limited pulse
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SANS polarization analysis at V4 SANS instrument of HMI Berlin

2008

The V4 instrument has recently been upgraded with a 3He spin filter cell, placed directly in the homogeneous field B of the sample magnet, to enhance the SANSPOL option for polarization analysis. The prototype setup was still affected by: (a) a quick relaxation of the 3He nuclear polarization in the cell with a time constant of only ?130 min which significantly changes the spin filter transmissions T+ and T? for neutrons polarized parallel I+ and anti-parallel I? to B, and (b) the absence of a flipping aid behind the sample. The usual polarization analysis procedure, expecting virtually time-independent transmissions and a second flipping device, is therefore not applicable. We present an a…

PhysicsFerrofluidScatteringbusiness.industryApplied MathematicsTime constantPolarization (waves)Small-angle neutron scatteringOpticsMagnetNeutronAtomic physicsbusinessInstrumentationEngineering (miscellaneous)SuperparamagnetismMeasurement Science and Technology
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The Møller Polarimeter for MAMI

1991

The polarization of high-energy electrons can conveniently be measured by means of Moller scattering from polarized electrons in a magnetized ferromagnetic target. This process exhibits in the limit of high energies (E ≥ 100 MeV) still relatively large, energy independent and well known analysator strengths. Furthermore, the laboratory cross section in the kinematical range suitable for polarimeter applications is large $$ \frac{{d\sigma }}{{d\Omega }}({\Theta _{cm}} = 90^\circ ) = Z \cdot 0.18{\text{ }}barn/sr$$ and energy-independent.

PhysicsFerromagnetismPolarimeterElectronMøller scatteringAtomic physicsPolarization (waves)Omega
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Risken–Nummedal–Graham–Haken instability in class-B lasers

1999

We determine analytical expressions for the Risken-Nummedal-Graham-Haken multimode laser instability outside the uniform field limit in the case of very fast polarization decay (class-B laser). A new condition for the observability of that instability, concerning the value of the cavity mirrors reflectivity, is predicted.

PhysicsFiber diameterAnalytical expressionsbusiness.industryPhysics::OpticsPolarization (waves)LaserInstabilityReflectivityAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic Materialslaw.inventionOpticslawUniform fieldObservabilityElectrical and Electronic EngineeringPhysical and Theoretical ChemistrybusinessOptics Communications
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Notice of Removal: Stochastic generation of the phononic band structure of lossy and infinite crystals

2017

The concept of the band structure is central to the field of phononic crystals. Indeed, capturing the dispersion of Bloch waves — the eigenmodes of propagation in periodic media — gives invaluable information on allowed propagation modes, their phase and group velocities, local resonances, and band gaps. Band structures are usually obtained by solving an eigenvalue problem defined on a closed and bounded domain, which results in a discrete spectrum. There are at least two cases, however, that cannot be reduced to a simple eigenvalue problem: first, when materials showing dispersive loss are present and second, when the unit-cell extends beyond any bound, as in the case of phononic crystal o…

PhysicsField (physics)Band gapBounded functionQuantum mechanicsPhase (waves)Electronic band structureDispersion (water waves)Eigenvalues and eigenvectorsBloch wave2017 IEEE International Ultrasonics Symposium (IUS)
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Narrow-band tunable terahertz detector in antiferromagnets via staggered-field and antidamping torques

2018

We study dynamics of antiferromagnets induced by simultaneous application of dc spin current and ac charge current, motivated by the requirement of all-electrically controlled devices in the terahertz (THz) gap (0.1--30 THz). We show that ac electric current, via N\'eel spin-orbit torques, can lock the phase of a steady rotating N\'eel vector whose precession is controlled by a dc spin current. In the phase-locking regime the frequency of the incoming ac signal coincides with the frequency of auto-oscillations, which for typical antiferromagnets falls into the THz range. The frequency of auto-oscillations is proportional to the precession-induced tilting of the magnetic sublattices related …

PhysicsField (physics)Condensed matter physicsTerahertz radiationDetectorPhase (waves)02 engineering and technology021001 nanoscience & nanotechnology01 natural sciences7. Clean energySignalMagnetization0103 physical sciencesPrecessionCondensed Matter::Strongly Correlated ElectronsElectric current010306 general physics0210 nano-technologyPhysical Review B
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Constant-adiabaticity ultralow magnetic field manipulations of parahydrogen-induced polarization: application to an AA'X spin system

2021

The field of magnetic resonance imaging with hyperpolarized contrast agents is rapidly expanding, and parahydrogen-induced polarization (PHIP) is emerging as an inexpensive and easy-to-implement method for generating the required hyperpolarized biomolecules. Hydrogenative PHIP delivers hyperpolarized proton spin order to a substrate via chemical addition of H2 in the spin-singlet state, but it is typically necessary to transfer the proton polarization to a heteronucleus (usually 13C) which has a longer spin lifetime. Adiabatic ultralow magnetic field manipulations can be used to induce the polarization transfer, but this is necessarily a slow process, which is undesirable since the spins co…

PhysicsField (physics)General Physics and Astronomy02 engineering and technology010402 general chemistry021001 nanoscience & nanotechnologySpin isomers of hydrogenPolarization (waves)01 natural sciencesInduced polarization0104 chemical sciencesMagnetic fieldPhysics - Chemical PhysicsChemical additionProton spin crisisPhysical and Theoretical ChemistryAtomic physics0210 nano-technologySpin-½Physical Chemistry Chemical Physics
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Spin-orbit interaction in bremsstrahlung and its effect on the electron motion in a strong Coulomb field

2015

Linear polarization of bremsstrahlung x rays produced in collisions of longitudinally polarized 2.1-MeV electrons with gold atoms was studied using the Compton scattering technique. We observed that the angle of x-ray polarization is strongly correlated with the incoming electron polarization. This correlation reveals the dominance of the spin-orbit interaction in bremsstrahlung and indicates a striking effect of the electron spin on the electron motion in a strong Coulomb field. The results confirm the validity of the theoretical predictions in a computationally challenging energy regime.

PhysicsField (physics)Linear polarizationAstrophysics::High Energy Astrophysical PhenomenaCompton scatteringBremsstrahlungCoulombElectronSpin–orbit interactionAtomic physicsPolarization (waves)Atomic and Molecular Physics and OpticsPhysical Review A
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Possible gyrotron operation in the “no start current” zone caused by the axial dependence of the phase of the resonator field

2018

It is known that gyrotrons (as well as other electron beam driven microwave and millimeter-wave oscillators) can operate in the regime of either soft or hard self-excitation. In the regime of soft self-excitation, the beam current exceeds its starting value; thus, the oscillations can start to grow from the noise produced by electrons. In the regime of hard self-excitation, the beam current is less than its starting value. Therefore, for exciting the oscillations, a certain start-up scenario is required, which may include the variation of the mod-anode and/or beam voltage or the guiding magnetic field. It was found recently [O. Dumbrajs and G. S. Nusinovich, Phys. Plasmas 25, 013121 (2018)]…

PhysicsField (physics)Phase (waves)ElectronCondensed Matter Physics01 natural sciences010305 fluids & plasmaslaw.inventionComputational physicsMagnetic fieldResonatorlawGyrotron0103 physical sciences010306 general physicsBeam (structure)Noise (radio)Physics of Plasmas
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