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Photoionization beam

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]

Figure B2.3.7. Schematic apparatus of crossed molecular beam apparatus with synclirotron photoionization mass spectrometric detection of the products [12], To vary the scattering angle, the beam source assembly is rotated in the plane of the detector. (By pemrission from AIP.)... Figure B2.3.7. Schematic apparatus of crossed molecular beam apparatus with synclirotron photoionization mass spectrometric detection of the products [12], To vary the scattering angle, the beam source assembly is rotated in the plane of the detector. (By pemrission from AIP.)...
Yang X, Lin J, Lee Y T, Blank D A, Suits A G and Wodtke A M 1997 Universal crossed molecular beams apparatus with synchrotron photoionization mass spectrometric product detection Rev. Sc/. Instrum 68 3317-26... [Pg.2086]

In Surface Analysis by Laser Ionization (SALI), a probe beam such as an ion beam, electron beam, or laser is directed onto a surfiice to remove a sample of material. An untuned, high-intensity laser beam passes parallel and close to but above the sur-fiice. The laser has sufficient intensity to induce a high degree of nonresonant, and hence nonselective, photoionization of the vaporized sample of material within the laser beam. The nonselectively ionized sample is then subjected to mass spectral analysis to determine the nature of the unknown species. SALI spectra accurately reflect the surface composition, and the use of time-of-flight mass spectrometers provides fast, efficient and extremely sensitive analysis. [Pg.42]

Dithiiranethione is an isomer of CS3 and its preparation and structure have been drawing much attention [75JCS(P2)559]. In the chemiionization process of CS + CS2 using the molecular beam photoionrzation method, the photoionization efficiency curve of CS3 was observed (80JCP4242). [Pg.234]

An excellent agreement with the X-ray photoionization spectra of ethylene, butadiene and hexatriene (7) is obtained (12) (Figure 3) when including in our calculations the Gelius (36) photoionization cross sections for an Alka photon beam, by means of Eqs. (4) and (5). Such a direct comparison is impossible for octatetraene, a compound for which there is no available XPS data. [Pg.86]

Figure 1. Photoelectron circular dichroism angular distribution [/icp(0) - /rcp(6)] for the hv = 10.3-eV photoionization of (/ )-camphor, as imaged with the photon beam propagating along the X axis. The x,y axis scales are the physical pixel coordinates of the detector. Figure 1. Photoelectron circular dichroism angular distribution [/icp(0) - /rcp(6)] for the hv = 10.3-eV photoionization of (/ )-camphor, as imaged with the photon beam propagating along the X axis. The x,y axis scales are the physical pixel coordinates of the detector.
The cluster reactor is attached to the pulsed cluster source s condensation channel, as shown in Figure 6. (16) To it is attached a high-pressure nozzle from which a helium/hydrocarbon mixture is pulsed into the reactor at a time selected with respect to the production and arrival of the clusters. The effect of turbulent mixing with the reactant pulse perturbs the beam, but clusters and reaction products which survive the travel from the source to the photoionization regime ( 600y sec) and the photoionization process are easily detected. [Pg.120]

Figure 13. Phase lag between the photoionization and photodissociation of vinyl chloride resulting from the Gouy phase of the focused laser beam. The dashed curve shows the results of the analytical model discussed in the text, and the solid curve is a numerical calculation of the phase lag without adjustable parameters. Figure 13. Phase lag between the photoionization and photodissociation of vinyl chloride resulting from the Gouy phase of the focused laser beam. The dashed curve shows the results of the analytical model discussed in the text, and the solid curve is a numerical calculation of the phase lag without adjustable parameters.
In this chapter we have discussed the successful implementation in our laboratory, for the first time, of the soft (i.e. low energy) electron-impact ionization method for product detection in crossed molecular beams reactive scattering experiments with mass spectrometric detection. Analogous to the approach of soft photoionization by tunable VUV synchrotron radiation,... [Pg.373]

B. Molecular Beam-Photoionization-Time-of-Flight Mass Spectrometry. . 189... [Pg.185]

By employing a laser for the photoionization (not to be confused with laser desorption/ ionization, where a laser is irradiating a surface, see Section 2.1.21) both sensitivity and selectivity are considerably enhanced. In 1970 the first mass spectrometric analysis of laser photoionized molecular species, namely H2, was performed [54]. Two years later selective two-step photoionization was used to ionize mbidium [55]. Multiphoton ionization mass spectrometry (MPI-MS) was demonstrated in the late 1970s [56—58]. The combination of tunable lasers and MS into a multidimensional analysis tool proved to be a very useful way to investigate excitation and dissociation processes, as well as to obtain mass spectrometric data [59-62]. Because of the pulsed nature of most MPI sources TOF analyzers are preferred, but in combination with continuous wave lasers quadrupole analyzers have been utilized [63]. MPI is performed on species already in the gas phase. The analyte delivery system depends on the application and can be, for example, a GC interface, thermal evaporation from a surface, secondary neutrals from a particle impact event (see Section 2.1.18), or molecular beams that are introduced through a spray interface. There is a multitude of different source geometries. [Pg.25]

If reliable thermochemical data [28,82] is required, the above influences have to be substantially reduced. [46] One way is to use an electron monochromator (accuracy up to 0.1 eV). [83,84] An electron monochromator is a device for selecting nearly monoenergetic electrons from an electron beam. [85] Alternatively, one can employ photoionization (PI) instead of El ... [Pg.45]

Figure 2 The photoabsorption (c), photoionization (o-,-), and photodissociation (cr Figure 2 The photoabsorption (c), photoionization (o-,-), and photodissociation (cr<j) cross sections of CH4 as a function of the incident photon energy measured via the double ionization chamber and synchrotron radiation as mentioned in Section 2.1. The values of cr in the range below the first ionization potential were measured by the photon-beam attenuation method, using the ionization chamber as a conventional gas cell. The bandpass was 0.1 nm, which corresponds to the energy width of 32 meV at the incident photon energy of 20 eV. The vertical ionization potentials of the ionic states involved are also indicated by the vertical bars [11]. (From Ref [7]. Reprinted with permission from Flsevier Science.)...
The real-photon method is essentially more direct and easier compared to the dipole-simulation method in obtaining absolute values of photoabsorption cross sections (o ), photoionization cross sections and photoionization quantum yields (t],). In the real-photon method, however, there is a practical need to use the big and dedicated facilities of synchrotron radiation where, in many cases, one should change the beam lines equipped with different types of monochromators depending on used photon-wavelengths—and to develop some specific new experimental techniques in the range from the vacuum ultraviolet radiation to soft X-ray. [Pg.114]


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See also in sourсe #XX -- [ Pg.318 , Pg.319 , Pg.342 ]




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