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Surface laser

Lykke K R and Kay B D 1990 State-to-state inelastic and reactive molecular beam scattering from surfaces Laser Photoionization and Desorption Surface Analysis Techniquesvo 1208, ed N S Nogar (Bellingham, WA SPIE) p 1218... [Pg.919]

MOLECULAR DESORPTION FROM SOLID SURFACES LASER DIAGNOSTICS AND CHEMICAL DYNAMICS... [Pg.45]

Molecular Desorption from Solid Surfaces Laser Diagncbtics AND Chemical Dynamics 45... [Pg.393]

Activation by high temperature hot filament/hot surfaces, laser heating, arc discharge and arc plasma jets, chemically induced hot gas flames, etc. [Pg.334]

Interfacial Viscosity. In a clean system in which two pure liquids produce an interface, the viscosity of the interface should be the same as the bulk solution viscosity. However, surfactant or impurity adsorption at an interface can cause a resistance to fiow to occur that can be measured as the interfacial shear viscosity. This viscosity is defined as the ratio between the shear stress and the shear rate in the plane of the interface (12), Methods used to make these measurements include a viscous traction surface viscometer (J2), droplet-droplet coalescence (J3), the rotating ring viscometer (14), and surface laser light scattering (9). [Pg.269]

Fig. 14. Growing-in profiles of pyrene excimer fluorescence on various silica surfaces. Laser pulse is also presented. (Reprinted with permission from Langmuir, 2 (1986) 616, our ref. (40), Copyright (1986) American Chemical Society). Fig. 14. Growing-in profiles of pyrene excimer fluorescence on various silica surfaces. Laser pulse is also presented. (Reprinted with permission from Langmuir, 2 (1986) 616, our ref. (40), Copyright (1986) American Chemical Society).
Fig. 1. Raman spectra of four waters, HjO, H2 0, D2O, and Di left) as ice at 77 K with a liquid N2 cell (see Fig. 6), 135° backscattering directly off the ice surface, laser power 250 mW, spectral slit width 6 cm and right) as neat liquid at room temperature with a capillary tube, 90° scattering, laser power 250 mW, spectral slit width 10 cm". Exciting radiation (488.0 nm) for all RR spectra was provided by a Coherent Innova 90-6 Ar ion laser. The scattered light was dispersed by a SPEX 1403 double monochromator equipped with 1800 grooves/mm holographic gratings and detected by a cooled Hamamatsu 928 photomultiplier tube under the control of a SPEX DM3000 data station as described elsewhere. ... Fig. 1. Raman spectra of four waters, HjO, H2 0, D2O, and Di left) as ice at 77 K with a liquid N2 cell (see Fig. 6), 135° backscattering directly off the ice surface, laser power 250 mW, spectral slit width 6 cm and right) as neat liquid at room temperature with a capillary tube, 90° scattering, laser power 250 mW, spectral slit width 10 cm". Exciting radiation (488.0 nm) for all RR spectra was provided by a Coherent Innova 90-6 Ar ion laser. The scattered light was dispersed by a SPEX 1403 double monochromator equipped with 1800 grooves/mm holographic gratings and detected by a cooled Hamamatsu 928 photomultiplier tube under the control of a SPEX DM3000 data station as described elsewhere. ...
Laser surface treatment can be used either below or beyond the ablation threshold of the surface. Laser treatment is more often used below the ablation threshold of the material, thus inducing efficient modification of the surface composition [12, 18]. Various laser parameters, such as the wavelength, the fluence (laser intensity), the nature of the environmental gas, or the pulse number, may be changed in order to modify the characteristics of the treated surface as the treatment induces the formation of polar chemical species (hydroxyls, carboxyls, peroxides, etc.). Therefore, the use of laser treatment below the ablation threshold induces adhesion improvement mainly through thermodynamic and chemical parameters. [Pg.310]

Fig. 10.28 SERS for benzenethiol at roughened Au and Pt surfaces. Laser power at the sample 0.5 mW. Fig. 10.28 SERS for benzenethiol at roughened Au and Pt surfaces. Laser power at the sample 0.5 mW.
The process time depends on the complexity of the 3D microstructures therefore, it is commonly used for prototyping. An extensive review on stereolithography can be found in Reference 119. The latter method is a subtractive manufacturing process that uses a focused high-intensity laser beam to evaporate the material from the surface. Laser ablation is mostly used to fabricate microchannels in thermosetting polymers such as polyimide due to its physical properties. Microstructures of nanometer scale have been danonstrated, but the surface roughness and properties using laser... [Pg.373]

Rapid Tooling, Fig. 10 Repair of a textured surface, laser generating with powder nozzle (Source Trumpf)... [Pg.1033]

Laser ablation, also referred to as laser machining or drilling, is a process in which a laser is used to remove materials from a substrate, thereby creating a patterned surface. Laser drilling is a rapid and accurate means to produce holes in materials. By using pulsed lasers, little heat is transferred to... [Pg.440]

Chemical vapor deposition Deposition of solid material when gaseous reactants encounter a hot surface. Laser assisted CVD employs a hot laser-focus rather than a hot surface. [Pg.335]

A schematic of a modem LIBS system is shown in Figure 7.51. The components required are a high-peak-power Q-switched laser, optics to focus the laser onto the sample surface, laser pulse... [Pg.575]

Bescos B, Orea JM, Urena AG (2000) Laser desorption dynamics of carbendazim on a glass surface. Laser Chem 18(4) 219-237... [Pg.35]

Key words recycling alloys, amorphous alloys, alloy coatings, laser surfacing, laser alloying. [Pg.234]

Light from three different lasers (A, B, and C), each with a different wavelength, was shined onto the same metal surface. Laser A produced no photoelectrons. Lasers B and C both produced photoelectrons, hut the photoelechons produced by laser B had a greater velocity than those produced by laser C. Arrange the lasers in order of increasing wavelength. [Pg.327]

The intense fluorescence of laser-dyes embodied in these thin-film glasses, the simplicity to cast these sol-gel glasses in a multilayered sequence of tailored indices of refraction and the waveguide properties observed in such assemblies imply that such multilayered films may be constructed into a surface-laser. Currently, we are examining these structures as the core of a two dimensional laser and other non-linear optical devices. [Pg.423]


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See also in sourсe #XX -- [ Pg.305 , Pg.541 ]




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Alloys laser surface alloying

Coating laser surface alloying

Comparing plasma and laser treatments of textile surfaces

Diffuse reflectance laser flash-photolysis surface studies

Effect of Laser Irradiation on the Surface

Example Vertical-cavity surface-emitting lasers

Excimer Laser Surface Treatment

Experimental methods to investigate laser-induced surface reactions

Imaging surface assisted laser desorption/ionization

Laser Irradiation on the Chemical Composition of Metal Surfaces

Laser ablation polymer surfaces

Laser dynamic surface

Laser induced periodic surface structures

Laser induced surface reaction

Laser surface alloying

Laser surface analysis

Laser surface chemistry

Laser surface melting

Laser surface melting schematic

Laser surface modification

Laser surface processing, definition

Laser surface profilometry

Laser surface reactions

Laser technologies textiles surfaces

Laser-chemical processes at surfaces nanoscale patterning

Mass spectrometry matrix-enhanced surface-assisted laser

Mass spectrometry surface-enhanced laser desorption ionization

Mass spectroscopy surface-enhanced laser

Mass surface-assisted laser-desorption ionization

Matrix-assisted laser desorption/ionization surface preparation

Matrix-enhanced surface-assisted laser

Matrix-enhanced surface-assisted laser desorption/ionization mass spectrometry

Novel surface treatments effect of LTP plasma and UV-laser

Potential energy surfaces infrared laser excitation

SALI (surface analysis by laser

SELDI surface-enhanced laser

Sample laser pulse striking surface

Structuring of Metal Surfaces by Ultra-Short Pulsed Laser Irradiation

Surface Analysis Using Laser Ablation with ICP-OES

Surface Analysis by Laser Ionization, SALI

Surface Enhanced Laser Desorption Ionization Time-of-Flight SELDI-TOF)

Surface Laser Irradiation

Surface analysis by laser ablation

Surface analysis by laser ionization

Surface chemistry, laser-induced

Surface emitting laser

Surface enhanced laser desorption ionisation

Surface enhanced laser desorption/ionization SELDI)

Surface-assisted laser desorption ionisation

Surface-assisted laser desorption ionization

Surface-assisted laser desorption/ionization SALDI)

Surface-enhanced laser

Surface-enhanced laser desorption

Surface-enhanced laser desorption assessment

Surface-enhanced laser desorption ionization , tissue protein

Surface-enhanced laser desorption ionization protein chips with

Surface-enhanced laser desorption ionization technology

Surface-enhanced laser desorption/ionization

Surface-enhanced laser desorption/ionization time-of-flight

Technologies for GaN Surface Emitting Lasers

Vertical cavity surface emitting laser VCSEL)

Vertical cavity surface emitting laser fabrication

Vertical cavity surface emitting laser structure

Vertical cavity surface emitting lasers VCSELs)

Vertical cavity surface-emitting laser

Vertical cavity surface-emitting laser VCSEL) diodes

Vertical cavity surface-emitting laser diode

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