10 research outputs found

    Example of a VMI image

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    <p><strong>Figure 3.</strong> Example of a VMI image. Photon energy 23.95 eV, circular polarization. Sample: He. (a) Raw data. The arrow indicates the direction of propagation of the light. (b) pBasex [<a href="http://iopscience.iop.org/0953-4075/46/16/164007/article#jpb466820bib20" target="_blank">20</a>] reconstructed image (central part of image set to zero). (c) Photoelectron spectrum generated by angular averaging. (d) A polar plot of the angular distribution of the electrons in the outermost ring of the image where the polar angle is the angle between the direction of propagation of the light and the direction of emission of the elections and the distance from the origin of the plot is proportional to the intensity of electron emission in that direction.</p> <p><strong>Abstract</strong></p> <p>The low density matter end-station at the new seeded free electron laser FERMI@Elettra is a versatile instrument for the study of atoms, molecules and clusters by means of electron and ion spectroscopies. Beams of atoms, molecules and helium droplets as well as clusters of atoms, molecules and metals can be produced by three different pulsed valves. The atomic and molecular beams may be seeded, and the clusters and droplets may be pure, or doped with other atoms and molecules. The electrons and ions produced by the ionization and fragmentation of the samples by the intense light of FERMI can be analysed by the available spectrometers, to give mass spectra and energy as well as angular distributions of charged particles. The design of the detector allows simultaneous detection of electrons and ions using velocity map imaging and time-of-flight techniques respectively. The instruments have a high energy/mass resolution and large solid-angle collection efficiency. We describe the current status of the apparatus and illustrate the potential for future experiments.</p

    (a) Cut-away view of the main chamber, showing the VMI and the TOF mass spectrometer

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    <p><strong>Figure 2.</strong> (a) Cut-away view of the main chamber, showing the VMI and the TOF mass spectrometer. (b) Photograph of the detectors: (1) VMI MCP, (2) extractor, (3) interaction region, (4) repeller, (5) flight tube. The repeller–extractor gap is 18 mm. The photograph is inverted with respect to the drawing and its orientation when mounted.</p> <p><strong>Abstract</strong></p> <p>The low density matter end-station at the new seeded free electron laser FERMI@Elettra is a versatile instrument for the study of atoms, molecules and clusters by means of electron and ion spectroscopies. Beams of atoms, molecules and helium droplets as well as clusters of atoms, molecules and metals can be produced by three different pulsed valves. The atomic and molecular beams may be seeded, and the clusters and droplets may be pure, or doped with other atoms and molecules. The electrons and ions produced by the ionization and fragmentation of the samples by the intense light of FERMI can be analysed by the available spectrometers, to give mass spectra and energy as well as angular distributions of charged particles. The design of the detector allows simultaneous detection of electrons and ions using velocity map imaging and time-of-flight techniques respectively. The instruments have a high energy/mass resolution and large solid-angle collection efficiency. We describe the current status of the apparatus and illustrate the potential for future experiments.</p

    Schematic layout of the system

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    <p><strong>Figure 1.</strong> Schematic layout of the system. (a) Schematic view of the section from the last valve of PADReS to the experimental station, the main chamber with the sources on one side and the diagnostics on the other, and the beam dump. (b) Overview with 3D rendition, rear view. The FEL light enters chamber 4 from the far side. (1) Source chamber. (2) Doping chamber. (3) Differential pumping chamber. (4) Detector chamber. (5) Quadrupole mass spectrometer chamber. (6) Surface ionization detector chamber.</p> <p><strong>Abstract</strong></p> <p>The low density matter end-station at the new seeded free electron laser FERMI@Elettra is a versatile instrument for the study of atoms, molecules and clusters by means of electron and ion spectroscopies. Beams of atoms, molecules and helium droplets as well as clusters of atoms, molecules and metals can be produced by three different pulsed valves. The atomic and molecular beams may be seeded, and the clusters and droplets may be pure, or doped with other atoms and molecules. The electrons and ions produced by the ionization and fragmentation of the samples by the intense light of FERMI can be analysed by the available spectrometers, to give mass spectra and energy as well as angular distributions of charged particles. The design of the detector allows simultaneous detection of electrons and ions using velocity map imaging and time-of-flight techniques respectively. The instruments have a high energy/mass resolution and large solid-angle collection efficiency. We describe the current status of the apparatus and illustrate the potential for future experiments.</p

    TOF mass spectrum of singly and doubly ionized Xe and residual gas

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    <p><strong>Figure 4.</strong> TOF mass spectrum of singly and doubly ionized Xe and residual gas. Photon energy: 21.7 eV.</p> <p><strong>Abstract</strong></p> <p>The low density matter end-station at the new seeded free electron laser FERMI@Elettra is a versatile instrument for the study of atoms, molecules and clusters by means of electron and ion spectroscopies. Beams of atoms, molecules and helium droplets as well as clusters of atoms, molecules and metals can be produced by three different pulsed valves. The atomic and molecular beams may be seeded, and the clusters and droplets may be pure, or doped with other atoms and molecules. The electrons and ions produced by the ionization and fragmentation of the samples by the intense light of FERMI can be analysed by the available spectrometers, to give mass spectra and energy as well as angular distributions of charged particles. The design of the detector allows simultaneous detection of electrons and ions using velocity map imaging and time-of-flight techniques respectively. The instruments have a high energy/mass resolution and large solid-angle collection efficiency. We describe the current status of the apparatus and illustrate the potential for future experiments.</p

    A modular end-station for atomic, molecular, and cluster science at the low density matter beamline of FERMI@Elettra

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    The low density matter end-station at the new seeded free electron laser FERMI@Elettra is a versatile instrument for the study of atoms, molecules and clusters by means of electron and ion spectroscopies. Beams of atoms, molecules and helium droplets as well as clusters of atoms, molecules and metals can be produced by three different pulsed valves. The atomic and molecular beams may be seeded, and the clusters and droplets may be pure, or doped with other atoms and molecules. The electrons and ions produced by the ionization and fragmentation of the samples by the intense light of FERMI can be analysed by the available spectrometers, to give mass spectra and energy as well as angular distributions of charged particles. The design of the detector allows simultaneous detection of electrons and ions using velocity map imaging and time-of-flight techniques respectively. The instruments have a high energy / mass resolution and large solid-angle collection efficiency. We describe the current status of the apparatus and illustrate the potential for future experiments

    Clusters and Nanocrystals

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    Clusters and nanocrystals constitute intermediates between molecules and condensed matter. Due to their finite size, clusters have a wide spectrum of applications ranging from building blocks for novel materials to model systems for fundamental investigations about light-matter interactions. Short-wavelength radiation from synchrotron radiation sources and free-electron lasers allows the detailed investigation of their geometric, electronic, and magnetic structure as well as dynamical processes. Conversely, clusters can serve as idealized sample systems for the development of new experimental techniques and pioneering experiments with novel x-ray sources. The chapter starts with a brief introduction to cluster physics, followed by a comprehensive overview of research performed at synchrotron light sources on van der Waals, metal, and semiconductor clusters. With the advent of short-wavelength free-electron lasers, a new research field in the x-ray peak intensity regime has opened. Experiments on single clusters, such as x-ray imaging and tracing ultrafast dynamics, now become possible
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