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Bombarding conditions ions

ln+ at energies up to 40-60 keV (for small high-brightness ion probes 100 nm in diameter) for depth profiling the beam is usually of 10 to KKK) nm diameter, with ion current density of 1 to 10 pA-mm -. [Pg.284]


The properties of silicon dioxide films also depend upon all plasma deposition parameters. Temperature is the critical parameter (240), although the compressive stress level varies with rf frequency (237, 240). Film topography can be varied during deposition by altering ion bombardment conditions (242, 243). In particular, the incorporation of Ar in the deposition atmosphere enhances sputtering and thus promotes conformal step coverage during film formation (243). [Pg.438]

Ion Bombardment Conditions. A base pressure of 10 9 Torr is maintained in this chamber the noble gas pressure (He, Xe) rises to about 10"7 Torr during the ion bombardment. The ion beam is rastered on (1.5 x 1.5) mm2 areas at normal incidence 4He-2 keV ions are used for the ISS analysis when Xe-4 keV ions are used for SIMS. The incident ion current is measured with the aid of a moveable Faraday cup. Since the investigated samples are electrical insulators, charge neutralization is performed with low energy electrons ( 10 eV) emitted from a heated W filament. [Pg.211]

This paper is primarily concerned with the direct method of glow discharge polymerization. The bombardment of positive ions plays an important role in film formation by the direct method as mentioned above, but the bombarding ion itself and the reactive species in the gas phase may contribute to film formation. The relative importance of these factors depends on the discharge conditions. A theoretical equation for the growth rate of film will be presented from a phenomenological point of view and compared with experimental results. The theory takes into account bombardment by ions and transport of ions. [Pg.66]

It is of Interest at this point to add as a footnote to this work that we have found that for films formed under enhanced ion bombardment conditions (l.e., substrate biased... [Pg.207]

This method is already relatively old and has been used for the past several years in organic chemistry and biochemistry. High kinetic energy (several keV) primary ions, e.g., Ar, bombard a surface on which the sample has been deposited. Under these conditions, ions are extracted from the surface and can be analyzed, Benninghoven and co-workers [102] presented a number of examples carbohydrates, alkaloids, amino acids (and derivatives) and peptides. As with the other methods, both positive and negative ionization modes are possible (Fig. 14). More recently, the same author [103] demonstrated the possibility of studying non-volatile nucleic acids and compared the results obtained with the other desorption methods. Sensitivity limits are on the order of ng. [Pg.165]

The secondary ion signal will depend upon the element, sample, bombardment conditions, species... [Pg.48]

Table 3 Secondary Ion Count Rates Under Different Bombardment Conditions... Table 3 Secondary Ion Count Rates Under Different Bombardment Conditions...
Munster, H. Theobald, F. Budzikie-wicz, H. The Formation of a Matrix Plasma in the Gas Phase Under Fast Atom Bombardment Conditions. Int. J. Mass Spectrom. Ion Proc. 1987, 79, 73-79. [Pg.501]

The basis of SIMS can be traced back to the beginning of the twentieth century with the first experimental evidence of secondary ions reported by J.J. Thomson in 1910 (Thomson 1910). As quoted the secondary rays. ..which were on the most part neutral with a small fraction of positively charged particles, were recorded following bombardment of a metal sample by primary kanalstralen (Canal rays). These positive ions were noted within a Crookes tube when a metal specimen held under vacuum conditions was bombarded by ions. The resulting emissions were... [Pg.6]

If a sample solution is introduced into the center of the plasma, the constituent molecules are bombarded by the energetic atoms, ions, electrons, and even photons from the plasma itself. Under these vigorous conditions, sample molecules are both ionized and fragmented repeatedly until only their constituent elemental atoms or ions survive. The ions are drawn off into a mass analyzer for measurement of abundances and mJz values. Plasma torches provide a powerful method for introducing and ionizing a wide range of sample types into a mass spectrometer (inductively coupled plasma mass spectrometry, ICP/MS). [Pg.87]

Desorption ionization (DI). General term to encompass the various procedures (e.g., secondary ion mass spectrometry, fast-atom bombardment, californium fission fragment desorption, thermal desorption) in which ions are generated directly from a solid or liquid sample by energy input. Experimental conditions must be clearly stated. [Pg.438]

Physical Chemical Characterization. Thiamine, its derivatives, and its degradation products have been fully characterized by spectroscopic methods (9,10). The ultraviolet spectmm of thiamine shows pH-dependent maxima (11). H, and nuclear magnetic resonance spectra show protonation occurs at the 1-nitrogen, and not the 4-amino position (12—14). The H spectmm in D2O shows no resonance for the thiazole 2-hydrogen, as this is acidic and readily exchanged via formation of the thiazole yUd (13) an important intermediate in the biochemical functions of thiamine. Recent work has revised the piC values for the two ionization reactions to 4.8 and 18 respectively (9,10,15). The mass spectmm of thiamine hydrochloride shows no molecular ion under standard electron impact ionization conditions, but fast atom bombardment and chemical ionization allow observation of both an intense peak for the patent cation and its major fragmentation ion, the pyrimidinylmethyl cation (16). [Pg.85]

The chemical and electronic properties of elements at the interfaces between very thin films and bulk substrates are important in several technological areas, particularly microelectronics, sensors, catalysis, metal protection, and solar cells. To study conditions at an interface, depth profiling by ion bombardment is inadvisable, because both composition and chemical state can be altered by interaction with energetic positive ions. The normal procedure is, therefore, to start with a clean or other well-characterized substrate and deposit the thin film on to it slowly at a chosen temperature while XPS is used to monitor the composition and chemical state by recording selected characteristic spectra. The procedure continues until no further spectral changes occur, as a function of film thickness, of time elapsed since deposition, or of changes in substrate temperature. [Pg.30]


See other pages where Bombarding conditions ions is mentioned: [Pg.284]    [Pg.284]    [Pg.146]    [Pg.36]    [Pg.21]    [Pg.86]    [Pg.282]    [Pg.359]    [Pg.357]    [Pg.25]    [Pg.4678]    [Pg.901]    [Pg.990]    [Pg.133]    [Pg.426]    [Pg.432]    [Pg.475]    [Pg.166]    [Pg.262]    [Pg.306]    [Pg.307]    [Pg.321]    [Pg.366]    [Pg.373]    [Pg.464]    [Pg.2927]    [Pg.2930]    [Pg.20]    [Pg.37]    [Pg.113]    [Pg.437]    [Pg.130]    [Pg.396]    [Pg.522]    [Pg.525]    [Pg.143]    [Pg.700]   


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