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Plasma shield

Rocuronium bromide Verapamil (i.s.) Column Symmetry Human plasma Shield RP18 cartridge (50 x 2.1 mm) Detector ESI-MS Mobile phase linear gradient from 10% to 90% of ACN in water containing 0.1% TFA/ applied in 15 min. Column was then washed for 3 min at final gradient condition and set back to initial condition in 1 min and equilibrated for 5 min Single ion recording Rocuronium bromide m/z 265 and m/z 529 Verapamil m/z 455... [Pg.296]

The most popular lasers for ablation have nanosecond pulse lengths. Sufficiently high intensities for explosion-like ablation can be used and there is additional heating of the plasma gas. The intensities, the wavelength, the kind of gas and its pressure, must, however, also be chosen carefully in order to avoid plasma shielding of the sample. [Pg.440]

The heat conductance through the sample and in the plasma is responsible for the fact that with the Nd YAG lasers available today, the crater diameters are still much wider than the values determined by the diffraction limitations. When using conventional lasers with pulses in the ns and ps range the plasma shields the radiation, whereas with the femtosecond lasers that are now available a free expanding plasma is obtained, where the heating of the plasma appears to be less supplemented by the laser radiation. This leads to less fractionated volatilization of the solid sample and differences in crater shape, which need to be investigated further [229]. [Pg.135]

Laser ablation with laser pulses in the femtosecond (fs) range yields unique advantages, that is, negligible heat affected zone, lower ablation threshold fluence, plasma shielding is not an issue, and the possibility to structure materials that are transparent at the irradiation wavelength. [Pg.553]

Kinoshita, H., Kume, I., Sakai, H., Tagawa, M.and Ohmae, N., High growth rate of vertically aligned carbon nanotubes using a plasma shield in microwave plasma-enhanced chemical vapor deposition. Carbon, 42, 2004, XTii-llll. [Pg.13]

Pulse repetition rates vary widely with the lasing medium. This parameter shows great influence on the ablation process, because plasma shielding can take place at high pulse frequency which alters the ablation rate of the sample. Plasma shielding could be described as absorption or reflection of the incident laser beam by a plasma formed close to the sample surface as a result of the previous laser shot. [Pg.234]

An important characteristic of plasma is that the free charges move in response to an electric field or charge, so as to neutralize or decrease its effect. Reduced to its smaUest components, the plasma electrons shield positive ionic charges from the rest of the plasma. The Debye length, given by the foUowing ... [Pg.107]

Schematic of a fusion reactor, assuming a generally toroidal shape of the plasma and magnetic fusion. The principles emphasized are central hot core (red) at 100 million degrees, blanket and heat exchanger, shield, energy conversion, and the handling of D, T, and the "ash" He. Schematic of a fusion reactor, assuming a generally toroidal shape of the plasma and magnetic fusion. The principles emphasized are central hot core (red) at 100 million degrees, blanket and heat exchanger, shield, energy conversion, and the handling of D, T, and the "ash" He.
Shielded polyplexes with improved blood circulating properties are interesting tools for systemic cancer therapy (see Sect. 4.2). Nanoparticles can take advantage of the enhanced permeability and retention (EPR effect) [89] for passive tumor targeting. The EPR effect is based on the leakiness of tumor vasculature, due to neovascularization in growing tumors, combined with an inadequate lymphatic drainage. Nanoparticles with an elongated plasma circulation time can extravasate and passively accumulate at the tumor site. [Pg.5]

Isobaric interferences (especially those arising from the plasma itself, e.g., ArO+ on Fe) can be eliminated using cool-plasma conditions, sometimes in combination with a shield torch. This option is not suitable for seawater samples because a cool plasma, in the presence of a heavy matrix, cannot fully ionize elements with high first ionization potentials, notably Zn, Cd, and Hg. Protocols have thus been established for analysis of 10-fold diluted seawater on instalments with sufficiently high resolution to separate most of the affected isotopes from their isobaric interferences [1], To circumvent the issue entirely, others have used online chemical extraction to separate analytes of interest... [Pg.237]


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See also in sourсe #XX -- [ Pg.208 ]




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