Search results for "Ionization."

showing 10 items of 1229 documents

Spatial distribution of air kerma rate and impact of accelerating voltage on the quality of an ultra soft X-ray beam generated by a cold cathode tube…

2015

Abstract Ultrasoft X-ray characteristic aluminum K alpha line (Al Kα with energy of 1.5 keV) is used in radiobiological experiments to study the effect of radiation on biological matter. A simple method to generate a continuous beam of those X-ray radiations is to bombarding an aluminum target with accelerated electrons using high voltage (HV). In this work, by varying the HV we study the characteristics of a photon beam generated by means of a cold cathode transmission X-ray tube. The anode is a thin (16 μm) aluminum foil supported by a copper grid. The spatial distribution of air kerma is measured using gafchromic films of HD-810 calibrated with a parallel plate free-air ionization chambe…

PhysicsRadiationbusiness.industryX-ray tubeAcceleration voltageCathodelaw.inventionAnodeKermaOpticslawIonization chamberCold cathodeAtomic physicsbusinessInstrumentationBeam (structure)Radiation Measurements
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Development of the CRIS (Collinear Resonant Ionisation Spectroscopy) beam line

2012

The CRIS (Collinear Resonant Ionisation Spectroscopy) beam line is a new experimental set up at the ISOLDE facility at CERN. CRIS is being constructed for highresolution laser spectroscopy measurements on radioactive isotopes. These measurements can be used to extract nuclear properties of isotopes far from stability. The CRIS beam line has been under construction since 2009 and testing of its constituent parts have been performed using stable and radioactive ion beams, in preparation for its first on-line run. This paper will present the current status of the CRIS experiment and highlight results from the recent tests. ispartof: pages:012070-6 ispartof: Journal of Physics: Conference Serie…

PhysicsRadioactive ion beamsHistoryLarge Hadron ColliderNuclear structureCRIS beam line[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciences010305 fluids & plasmasComputer Science ApplicationsEducationNuclear physicsBeamlineIonization0103 physical sciencesPhysics::Accelerator PhysicsCollinear resonant ionisation spectroscopyAtomic physicsNuclear Experiment010306 general physicsSpectroscopyComputingMilieux_MISCELLANEOUS
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Excited atomic energy levels in protactinium by resonance ionization spectroscopy

2018

We present high-resolution data of the single-excitation spectrum of protactinium, reaching slightly beyond the first-ionization threshold. Within this work, more than 1500 energy levels are recorded in different excitation energy ranges below $50\phantom{\rule{0.16em}{0ex}}000\phantom{\rule{4pt}{0ex}}{\mathrm{cm}}^{\ensuremath{-}1}$. Our experimental results show that the tabulated data in the literature severely underestimate the density of states particularly regarding the highly excited spectral range.

PhysicsRange (particle radiation)010308 nuclear & particles physicsProtactiniumchemistry.chemical_element01 natural scienceschemistryExcited state0103 physical sciencesResonance ionizationDensity of statesAtomic physics010306 general physicsSpectroscopyEnergy (signal processing)ExcitationPhysical Review A
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Ionization dynamics of a model molecular ion

2005

We study the ionization dynamics of a model one-dimensional molecular ion as a function of the internuclear distance R, for different values of the laser intensity. The electron–nucleus potential is assumed to be a Poschl–Teller potential, whose parameters are chosen to have only two bare bound molecular states in the range of R considered. We describe three different theoretical approaches to study the dynamics of the system: an exact numerical, a semiperturbative and a phenomenological approach. All these approaches indicate the presence of a sharp ionization peak for a critical value of the internuclear distance, for which the energy difference between the two bound levels coincides with…

PhysicsRange (particle radiation)Field (physics)Polyatomic ionPhotoionizationCondensed Matter PhysicsLaserCritical valueDiatomic moleculeAtomic and Molecular Physics and Opticslaw.inventionIonization dinamics of moleculeslawIonizationPhysics::Atomic PhysicsAtomic physics
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Evolution of the electron distribution function in intense laser-plasma interactions

1994

We report a numerical investigation of the time evolution of the electron distribution function (EDF) in a laser-embedded, fully ionized plasma. A distinctive feature of the calculations is removal of the frequently adopted assumption of small anisotropy of the EDF in velocity space. This requires solving a two-dimensional partial differential equation for the EDF. Within the adopted range of parameters, the EDF undergoes significant changes. An initially isotropic EDF transforms rapidly into an anisotropic one characterized by a longitudinal velocity scale larger than the perpendicular one. This longitudinal stretching persists for several cycles of the radiation field, implying the establ…

PhysicsRange (particle radiation)Partial differential equationIonizationIsotropyTime evolutionPerpendicularPlasmaAtomic physicsAnisotropyComputer Science::Operating SystemsPhysical Review E
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Radiation controlled energy of photoelectrons produced by two-color short pulses.

2008

We report on numerical results of energy spectra of photoelectrons emitted by irradiating a hydrogen atom with the superposition of two pulses. The spectra have been obtained by numerical integration of the time dependent Schr¨odinger equation. The highest frequency component of the pulse has been assumed to have low intensity and such a frequency that a single photon may ionize the atom. Its duration has been assumed to lie in the range of subfemtoseconds. The lowest frequency component that redistribute the energy of the ionized electrons has an higher intensity and duration of few femtoseconds. We find that when the field are aligned, the electron energy spectra strongly depend on the ti…

PhysicsRange (particle radiation)PhotonField (physics)General Physics and AstronomyElectronRadiationPhotoelectric effectPulse (physics)energy spectra photoelectrons Schr¨odinger equationIonizationGeneral Materials SciencePhysical and Theoretical ChemistryAtomic physics
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Determination of ion-induced K-shell ionization cross sections by comparison with nuclear Coulomb excitation

1979

Abstract A new method for the determination of cross sections for K-shell ionization of heavy atoms by charged particles is proposed. The method is based on a comparison of photon lines due to K X-rays and low-energy γ-rays, the latter ones being produced in nuclear Coulomb excitation with accurately known cross sections. This procedure applies within a limited energy range to the study of targets comprising deformed even nuclei, but can also be extended to other targets having Z≳30. A test of the new technique has been carried out for Gd, W, Th and U natural targets irradiated by 4.75 MeV protons. For Th, also energies of 6.80–10.10 MeV were used. The results are briefly discussed with ref…

PhysicsRange (particle radiation)PhotonIonizationElectron shellNuclear cross sectionGeneral MedicineCoulomb excitationAtomic physicsCharged particleIonNuclear Instruments and Methods
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Perturber's charge effect on Stark broadened hydrogen lines in helium plasmas

2002

Abstract The Stark line profiles for hydrogen Ly α , Ly β , Hα, and Hβ are calculated using the computer simulation method for helium plasmas in the range of electron concentration from 1018 to 10 19 cm −3 at increasing temperature values kT from 7 to 10 eV , according to the experimental measurements in dense plasmas (Bochum experiment). The calculation was carried out at two limiting assumptions about the perturbers: (a) in the helium plasma only singly ionized helium ions occur, and (b) in the plasma the doubly ionized ions exclusively exist. In the paper the ratio of the calculated full half-widths, FWHM(b)/FWHM(a), for these lines are presented. The ratio equals about to 1.1 for Lyβ an…

PhysicsRange (particle radiation)RadiationHydrogenchemistry.chemical_elementPlasmaAtomic and Molecular Physics and OpticsIonFull width at half maximumchemistryIonizationAtomic physicsSpectroscopyHeliumLine (formation)Journal of Quantitative Spectroscopy and Radiative Transfer
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SU-E-T-218: Octavius 4D: Commissioning and Clinical Implementation of a New Device for VMAT Verifications

2013

Purpose: To commission a new device for pre‐treatment patient specific verification of VMAT plans, which is capable of reconstructing 3D dose with high resolution. Methods: Octavius 4D system (PTW) consists of an ion chamber array embedded in a cylindrical phantom which, assisted by an inclinometer, rotates synchronously with the gantry. For VMAT plans, it measures planar dose distributions as a function of gantry angle in order to compute the resulting 3D dose distribution. There are two options for the ion chamber array: Octavius 729 (general purpose) and Octavius 1000 SRS (small field size, high resolution). We have used three linacs: two Varian Clinac iX and one TrueBeam with MLC HD 120…

PhysicsReproducibilitybusiness.industrymedicine.medical_treatmentTruebeamGeneral MedicineGantry angleRadiosurgeryLinear particle acceleratorSmall fieldIonization chambermedicineNew deviceNuclear medicinebusinessMedical Physics
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High-precision ab initio calculations of the spectrum of Lr$^+$

2019

The planned measurement of optical resonances in singly-ionised lawrencium (Z = 103) requires accurate theoretical predictions to narrow the search window. We present high-precision, ab initio calculations of the electronic spectra of Lr$^+$ and its lighter homologue lutetium (Z = 71). We have employed the state-of-the-art relativistic Fock space coupled cluster approach and the AMBiT CI+MBPT code to calculate atomic energy levels, g-factors, and transition amplitudes and branching-ratios. Our calculations are in close agreement with experimentally measured energy levels and transition strengths for the homologue Lu$^+$ , and are well-converged for Lr$^+$ , where we expect a similar level o…

PhysicsSPECTROSCOPYSETSAtomic Physics (physics.atom-ph)ENERGIESFOS: Physical scienceschemistry.chemical_elementConfiguration interaction01 natural sciencesSpectral lineLutetiumPhysics - Atomic Physics010305 fluids & plasmasFock spaceATOMSCoupled clusterchemistryAb initio quantum chemistry methodsIonization0103 physical sciencesPROGRAMddc:530Atomic physics010306 general physicsLawrencium
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