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LIFS

Gilman [124] and Westwood and Hitch [135] have applied the cleavage technique to a variety of crystals. The salts studied (with cleavage plane and best surface tension value in parentheses) were LiF (100, 340), MgO (100, 1200), CaFa (111, 450), BaFj (111, 280), CaCOa (001, 230), Si (111, 1240), Zn (0001, 105), Fe (3% Si) (100, about 1360), and NaCl (100, 110). Both authors note that their values are in much better agreement with a very simple estimate of surface energy by Bom and Stem in 1919, which used only Coulomb terms and a hard-sphere repulsion. In more recent work, however, Becher and Freiman [126] have reported distinctly higher values of y, the critical fracture energy. ... [Pg.279]

LIF Laser-induced fluorescence Incident laser beam excites Excited-state processes ... [Pg.317]

LISC Laser-induced surface Similar to LIF chemical Pbotochemistry, desorption... [Pg.317]

Figure Al.3.24. Band structure of LiF from ab initio pseudopotentials [39],... Figure Al.3.24. Band structure of LiF from ab initio pseudopotentials [39],...
The reflectivity of LiF is illustrated in figure Al.3.26. The first large peak corresponds to an excitonic transition. [Pg.127]

LIF has been used to study state-selected ion-atom and ion-molecule collisions in gas cells. Ar reactions with N2 and CO were investigated by Leone and colleagnes in the 1980s [13, 14] and that group has... [Pg.799]

LIF is also used witii liquid and solid samples. For example, LIF is used to detect lJO ions in minerals the uranyl ion is responsible for the bright green fluorescence given off by minerals such as autunite and opal upon exposure to UV light [23],... [Pg.800]

However, with the advent of lasers, the teclmique of laser-induced fluorescence (LIF) has probably become the single most popular means of detennining product-state distributions an early example is the work by Zare and co-workers on Ba + FLT (X= F, Cl, Br, I) reactions [25]. Here, a tunable laser excites an electronic transition of one of the products (the BaX product in this example), and the total fluorescence is detected as a... [Pg.873]

Figure B2.3.8. Energy-level sehemes deseribing various optieal methods for state-seleetively deteeting ehemieal reaetion produets left-hand side, laser-indueed fluoreseenee (LIF) eentre, resonanee-enlianeed multiphoton ionization (REMPI) and right-hand side, eoherent anti-Stokes Raman speetroseopy (CARS). The ionization oontinuiim is denoted by a shaded area. The dashed lines indieate virtual eleetronie states. Straight arrows indieate eoherent radiation, while a wavy arrow denotes spontaneous emission. Figure B2.3.8. Energy-level sehemes deseribing various optieal methods for state-seleetively deteeting ehemieal reaetion produets left-hand side, laser-indueed fluoreseenee (LIF) eentre, resonanee-enlianeed multiphoton ionization (REMPI) and right-hand side, eoherent anti-Stokes Raman speetroseopy (CARS). The ionization oontinuiim is denoted by a shaded area. The dashed lines indieate virtual eleetronie states. Straight arrows indieate eoherent radiation, while a wavy arrow denotes spontaneous emission.
Figure B2.5.10. LIF signal of free Na atoms produced in the photodissociation of Nal. t - q is the delay between the photolysis pulse (at L) and the probe pulse. Adapted from [111]. Figure B2.5.10. LIF signal of free Na atoms produced in the photodissociation of Nal. t - q is the delay between the photolysis pulse (at L) and the probe pulse. Adapted from [111].
A recent study of the vibrational-to-vibrational (V-V) energy transfer between highly-excited oxygen molecules and ozone combines laser-flash photolysis and chemical activation with detection by time-resolved LIF [ ]. Partial laser-flash photolysis at 532 mn of pure ozone in the Chappuis band produces translationally-... [Pg.2139]

The chemical-activation step is between one and two orders of magnitude faster than the subsequent collisional deactivation of vibrationally excited O2. Finally, the population of individual vibrational levels v" of O2 is probed tluough LIF in the Schiunann-Runge band Oi X E") after exciting the oxygen... [Pg.2139]

Baer M, Loesch H J, Werner H J and Last I 1994 Integral and differential cross sections for the Li + HF to LiF + H process. A comparison between quantum mechanical and experimental results Chem. Phys. Lett. 219 372... [Pg.2328]

Tunable visible and ultraviolet lasers were available well before tunable infrared and far-infrared lasers. There are many complexes that contain monomers with visible and near-UV spectra. The earliest experiments to give detailed dynamical infonnation on complexes were in fact those of Smalley et al [22], who observed laser-induced fluorescence (LIF) spectra of He-l2 complexes. They excited the complex in the I2 B <—A band, and were able to produce excited-state complexes containing 5-state I2 in a wide range of vibrational states. From line w idths and dispersed fluorescence spectra, they were able to study the rates and pathways of dissociation. Such work was subsequently extended to many other systems, including the rare gas-Cl2 systems, and has given quite detailed infonnation on potential energy surfaces [231. [Pg.2447]

Sensitivity levels more typical of kinetic studies are of the order of lO molecules cm . A schematic diagram of an apparatus for kinetic LIF measurements is shown in figure C3.I.8. A limitation of this approach is that only relative concentrations are easily measured, in contrast to absorjDtion measurements, which yield absolute concentrations. Another important limitation is that not all molecules have measurable fluorescence, as radiationless transitions can be the dominant decay route for electronic excitation in polyatomic molecules. However, the latter situation can also be an advantage in complex molecules, such as proteins, where a lack of background fluorescence allow s the selective introduction of fluorescent chromophores as probes for kinetic studies. (Tryptophan is the only strongly fluorescent amino acid naturally present in proteins, for instance.)... [Pg.2958]

Figure C3.1.8. Schematic diagram of a transient kinetic apparatus using iaser-induced fluorescence (LIF) as a probe and a CO2 iaser as a pump source. (From Steinfeid J I, Francisco J S and Fiase W L i989 Chemical Kinetics and. Dynamics (Engiewood Ciiffs, NJ Prentice-Fiaii).)... Figure C3.1.8. Schematic diagram of a transient kinetic apparatus using iaser-induced fluorescence (LIF) as a probe and a CO2 iaser as a pump source. (From Steinfeid J I, Francisco J S and Fiase W L i989 Chemical Kinetics and. Dynamics (Engiewood Ciiffs, NJ Prentice-Fiaii).)...
The UIIF wnive fimction can also apply to singlet molecules. F sn-ally, the results are the same as for the faster RHF method. That is, electron s prefer to pair, with an alpha electron sh arin g a m olecu lar space orbital with a beta electron. L se the L lIF method for singlet states only to avoid potential energy discontinuities when a covalent bond Is broken and electron s can impair (see Bond Breaking on page 46). [Pg.37]

In peptide syntheses, where partial racemization of the chiral a-carbon centers is a serious problem, the application of 1-hydroxy-1 H-benzotriazole ( HBT") and DCC has been very successful in increasing yields and decreasing racemization (W. Kdnig, 1970 G.C. Windridge, 1971 H.R. Bosshard, 1973), l-(Acyloxy)-lif-benzotriazoles or l-acyl-17f-benzo-triazole 3-oxides are formed as reactive intermediates. If carboxylic or phosphoric esters are to be formed from the acids and alcohols using DCC, 4-(pyrrolidin-l -yl)pyridine ( PPY A. Hassner, 1978 K.M. Patel, 1979) and HBT are efficient catalysts even with tert-alkyl, choles-teryl, aryl, and other unreactive alcohols as well as with highly bulky or labile acids. [Pg.145]

Far-ultraviolet Microwave discharge in noble gases Lyman discharge LiF (or no windows) Grating Photomultiplier photodiode photographic plate... [Pg.60]


See other pages where LIFS is mentioned: [Pg.241]    [Pg.241]    [Pg.506]    [Pg.520]    [Pg.268]    [Pg.124]    [Pg.124]    [Pg.579]    [Pg.799]    [Pg.799]    [Pg.799]    [Pg.874]    [Pg.874]    [Pg.1448]    [Pg.2126]    [Pg.2958]    [Pg.128]    [Pg.141]    [Pg.234]    [Pg.113]    [Pg.642]    [Pg.103]    [Pg.248]    [Pg.393]    [Pg.630]    [Pg.663]    [Pg.838]    [Pg.1130]    [Pg.432]   


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Applications of LIF

BaF2-LiF

BaF2-LiF system

Covalent and ionic curve crossings in LiF

Detectability interferences, LIFS

Determination of Population Distributions by LIF

Diethylamino LIF spectra of complexes with acetonitrile

Experimental Aspects of LIF

Fluoride LiF

LIF

LIF

LIF Sensing Instrumentation

LIF detection

LIF detectors

LIF excitation spectroscopy

LIF instrumentation

LIF of Polyatomic Molecules

LIF photometric instrument specification

LIF receptor

LIF sensing classification

LIF spectroscopy

LIF system

LIF technique

LIF test

Laser Induced Fluorescence (LIF) and Scattering Method (Lorenz-Mie, Rayleigh, Raman)

Laser-induced fluorescence, LIF

LiF Catalysts for Super-Rate Burning

LiF LITHIUM FLUORIDE

LiF catalyzed double-base propellant

LiF crystals

LiF dosimeter

LiF elimination

LiF formation

LiF layer

LiF negative catalyst

LiF-BeFj

LiF-ThF

LiF-catalyzed AP composite propellant

LiF-catalyzed propellant

LiF/Al electrode

LiF/Au electrode

Measurement of Inelastic Collisions by LIF

Population LIFS, measuring

Product State Analysis by Laser-induced Fluorescence (LIF)

Thermodynamic Investigation of the BaF2-LiF-NdF3 System

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