Search results for "Axis"

showing 10 items of 751 documents

Experimental evidence for chirality in the odd-A 105Rh

2004

Abstract High-spin states in 105 Rh were populated by the 96 Zr( 13 C, p3n) reaction at beam energies of 51 and 58 MeV, and studied using the EUROBALL IV γ -ray spectrometer and the DIAMANT charged particle array. A pair of nearly degenerate Δ I = 1 three-quasiparticle bands with the same spins and parity have been observed. Comparison of the experimental results with tilted axis cranking calculations confirms the chiral character of the two bands, while arguments based on the excitation of particles within the π g 9 / 2 ν ( h 11 / 2 ) 2 configuration of the yrast band and comparison with the previously observed γ band exclude the other possible interpretations. This is the first experiment…

PhysicsNuclear and High Energy PhysicsSpins010308 nuclear & particles physics[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]Chiral partner bandsYrastDegenerate energy levelsParity (physics)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Tilted axis cranking01 natural sciences21.10.Re; 21.60.-n; 23.20.Lv; 27.60.+jCore-quasiparticle coupling calculationsCharged particleThree-quasiparticle configuration0103 physical sciencesQuasiparticleAtomic physics010306 general physicsChirality (chemistry)ExcitationPhysics Letters B
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The distribution of the rotational transition strength in warm nuclei studied through γ-ray correlations

1995

Abstract The study of damping of rotational motion applying te rotational plane mapping (RPM) method is presented and discussed. The aim of this technique is to extract the distribution of the rotational transition strength from an analysis of the shape of the “central valley” of two- and three-dimensional γ-ray spectra. The method is applied to a triple γ-coincidence data set of 162,163Tm nuclei formed in 37Cl+130Te reactions. The rotational transition strength is obtained as a function of rotational frequency for selected regions of entry states, and the width is found to be rather constant and approximately equal to 80 keV. This value is significantly smaller than the value predicted the…

PhysicsNuclear reactionNuclear and High Energy PhysicsRotation around a fixed axisRotational transitionRotational temperatureRotational–vibrational spectroscopyAtomic physicsResidualRotational partition functionSpectral lineNuclear Physics A
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Continuously Variable Periodic Test Target

1987

CONTINUOUSLY VARIABLE PERIODIC TEST TARGETP. ANDRES*, J. OJEDA- CASTANEDAt, and J.C. BARREIRO*tINAOE, Apartado Postal 216, 72000 Puebla, Pue., Mexico*Departamento de Optica, Universidad de Valencia, 46100 Burjasot, Spain1. INTRODUCTIONThe modulus of the optical transfer function (MTF) of the eye or any other optical system is usuallyevaluated by imaging either several gratings each with different spatial frequency, or a single test tar-get having patterns with different frequencies (USAF resolution chart). In any of these two usual proce-dures, the measurement of the MTF is made at discrete values of the spatial frequency.Here we describe a method based on the self -imaging phenomenon for p…

PhysicsOptical axisOpticsbusiness.industryOptical transfer functionTalbot effectImage processingSpatial frequencyMonochromatic colorGratingbusinessImage resolutionSPIE Proceedings
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Impact of anisotropy on the noncritical squeezing properties of two-transverse-mode optical parametric oscillators

2013

In a series of articles we studied the quantum properties of a degenerate optical parametric oscillator tuned to the first family of transverse modes at the subharmonic. We found that, for a cavity having rotational symmetry respect to the optical axis, a TEM$_{10}$ mode with an arbitrary orientation in the transverse plane is emitted above threshold. We proved then that quantum noise induces a random rotation of this bright TEM$_{10}$ mode in the transverse plane, while the mode orthogonal to it, the so-called dark mode, has perfect quadrature squeezing irrespective of the distance to threshold (noncritical squeezing). This result was linked to the spontaneous rotational symmetry breaking …

PhysicsQuantum PhysicsDegenerate energy levelsQuantum noiseRotational symmetryFOS: Physical sciences01 natural sciencesAtomic and Molecular Physics and OpticsÒptica quànticaTransverse mode010309 opticsOptical axisTransverse planeQuantum mechanics0103 physical sciencesOptical parametric oscillator010306 general physicsAnisotropyQuantum Physics (quant-ph)
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BeppoSAX serendipitous discovery of the X-ray pulsar SAX J1802.7-2017

2003

We report on the serendipitous discovery of a new X-ray source, SAX J1802.7-2017, ~22' away from the bright X-ray source GX 9+1, during a BeppoSAX observation of the latter source on 2001 September 16-20. SAX J1802.7-2017 remained undetected in the first 50 ks of observation; the source count rate in the following ~300 ks ranged between 0.04 c/s and 0.28 c/s, corresponding to an averaged 0.1-10 keV flux of 3.6 10^{-11} ergs cm^{-2} s^{-1}. We performed a timing analysis and found that SAX J1802.7-2017 has a pulse period of 139.612 s, a projected semimajor axis of a_x sin i ~ 70 lt-s, an orbital period of ~4.6 days, and a mass function f(M) ~ 17 Msun. The new source is thus an accreting X-ra…

PhysicsSemi-major axisAstrophysics (astro-ph)FluxFOS: Physical sciencesAstronomy and AstrophysicsAstrophysicsAstrophysicsOrbital periodPulse periodSettore FIS/05 - Astronomia E AstrofisicaPulsarSpace and Planetary ScienceHigh massStars: Pulsars: General Stars: Pulsars: Individual: Alphanumeric: SAX J1802.7-2017 Stars: Magnetic Fields Stars: Neutron X-Rays: BinariesX-ray pulsar
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Analytical characterization of spectral anomalies in polychromatic apertured beams

2006

Abstract The power spectrum of polychromatic apertured spherical waves changes strongly in the vicinity of phase singularities. A spectral shift effect is observed and, in some cases, a spectral switch occurs together with a broadening of the power spectrum. Low-order moments of the power spectrum are evaluated in points of the focal volume with spectral anomalies. First-order analytical expressions are proposed for the evaluation of the relative spectral shift and the relative spectral broadening in the transverse focal plane and along the optical axis. The influence of the fractional bandwidth and the selected singularity order is considered.

PhysicsSpectral fluxbusiness.industrySpectral densityAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic MaterialsOptical axisTransverse planeSingularityOpticsCardinal pointSpectral envelopeElectrical and Electronic EngineeringPhysical and Theoretical ChemistrybusinessDoppler broadeningOptics Communications
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Field-free permanent molecular planar alignment

2009

We show the existence of a permanent molecular planar alignment in field-free conditions. We present different control strategies using shaped laser pulses to reach this state. The strategies are robust with respect to the temperature and can be implemented with the state of the art technology. They can be applied not only to linear molecules but also to symmetric or asymmetric top molecules along the most polarizable molecular axis. We propose potential applications of this planar alignment such as the increase of the adsorption on a surface.

PhysicsSurface (mathematics)[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph]Field (physics)business.industryLinear molecular geometryMolecular axisLaser01 natural sciencesMolecular physicsAtomic and Molecular Physics and Optics010305 fluids & plasmaslaw.inventionPlanar[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]Polarizabilitylaw0103 physical sciencesMoleculeOptoelectronics010306 general physicsbusiness[PHYS.QPHY] Physics [physics]/Quantum Physics [quant-ph]ComputingMilieux_MISCELLANEOUSPhysical Review A
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Poincaré sphere analysis of a ferroelectric liquid crystal optical modulator: application to optimize the contrast ratio

2008

The Poincare sphere representation is used to analyze the polarization transformation achieved with a ferroelectric liquid crystal (FLC) optical modulator. This device acts as a switchable wave-plate, in which the orientation of the principal axes rotates under the action of an applied bipolar voltage. In the standard operational mode for intensity switching, the rotation angle of the principal axes is �θ = π/4 and the phase shift is φ = π (half-wave-plate). However, for wavelengths different from the design one, the FLC deviates from the half-wave-plate performance and the optical contrast is diminished. We use the Poincare sphere representation to perform a theoretical analysis of the int…

PhysicsWavelengthOpticsOptical modulatorbusiness.industryLiquid crystalContrast ratioElliptical polarizationbusinessPolarization (waves)FerroelectricityAtomic and Molecular Physics and OpticsPrincipal axis theoremJournal of Optics A: Pure and Applied Optics
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Rotation of Molecules and Nuclear Spin Relaxation

1978

Nuclear spin relaxation has been developed as a standard method for studying molecular motions in liquids, solids, polymers, and—to a lesser extent—gases, staring with the pioneering work of Bloembergen, Purcell, and Pound [1]. Of the great variety of molecular motions possible (e.g., translations, rotations, vibrations) rotations are particularly important for nuclear spin relaxation. Conversely, nuclear spin relaxation can be especially successful if information about rotational motions is desired. In this case nuclear spin relaxation can yield quantitative information over an extraordinary wide range of characteristic frequencies, from about 1 Hz to 1014Hz. It shoud be noted that, typica…

PhysicsWork (thermodynamics)Spin polarizationCondensed matter physicsScatteringRelaxation (NMR)Rotation around a fixed axisNeutron scatteringRotationMagnetic dipole–dipole interaction
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Geometric Origin of the Tennis Racket Effect

2020

The tennis racket effect is a geometric phenomenon which occurs in a free rotation of a three-dimensional rigid body. In a complex phase space, we show that this effect originates from a pole of a Riemann surface and can be viewed as a result of the Picard-Lefschetz formula. We prove that a perfect twist of the racket is achieved in the limit of an ideal asymmetric object. We give upper and lower bounds to the twist defect for any rigid body, which reveals the robustness of the effect. A similar approach describes the Dzhanibekov effect in which a wing nut, spinning around its central axis, suddenly makes a half-turn flip around a perpendicular axis and the Monster flip, an almost impossibl…

Physics[PHYS]Physics [physics]Riemann surfaceGeneral Physics and AstronomyClassical Physics (physics.class-ph)FOS: Physical sciencesMathematical Physics (math-ph)Physics - Classical PhysicsRigid body01 natural sciencesUpper and lower boundssymbols.namesakePerpendicular AxisClassical mechanics[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]Phase space0103 physical sciencesRacketsymbolsIdeal (ring theory)Twist010306 general physicscomputerMathematical Physicscomputer.programming_language
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