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Ionisation signal

Figures 1.4(a) and (b) show examples of the ionisation signals that are... Figures 1.4(a) and (b) show examples of the ionisation signals that are...
Figure 1.4. Experimental and theoretical femtosecond spectroscopy of IBr dissociation. Experimental ionisation signals as a function of pump-probe time delay for different pump wavelengths given in (a) and (b) show how the time required for decay of the initally excited molecule varies dramatically according to the initial vibrational energy that is deposited in the molecule by the pump laser. The calculated ionisation trace shown in (c) mimics the experimental result shown in (b). Figure 1.4. Experimental and theoretical femtosecond spectroscopy of IBr dissociation. Experimental ionisation signals as a function of pump-probe time delay for different pump wavelengths given in (a) and (b) show how the time required for decay of the initally excited molecule varies dramatically according to the initial vibrational energy that is deposited in the molecule by the pump laser. The calculated ionisation trace shown in (c) mimics the experimental result shown in (b).
Thermoelectric flame failure detection Analog burner control systems Safety temperature cut-out Mechanical pressure switch Mechanic/pneumatic gas-air-ration control Thermoelectric flame supervision Thermal combustion products, discharge safety devices Electronic safety pilot Electronic burner control systems Electronic cut-out with NTC Electronic pressure sensor/transmitter Electronic gas-air-ration control with ionisation signal or 02 sensor Ionisation flame supervision Electronic combustions product discharge safety device... [Pg.221]

With the use of a resonant cavity the threshold for collective emission is lower by the magnitude of the cavity finesse. Using a cavity finesse of a 100 or so Rydberg maser action on sodium has been observed. In this case the field ionisation signal was used to monitor the population as a function of time for the states 27S, 26P and 25P corresponding to transitions An = 1 at X = 1 470 mm and An = 2... [Pg.215]

The combustion of mixtures of hydrogen and air produces very few ions so that with only the carrier gas and hydrogen burning an essentially constant signal is obtained. When, however, carbon-containing compounds are present ionisation occurs and there is a large increase in the electrical conductivity of the flame. Because the sample is destroyed in the flame a stream-splitting device is employed when further examination of the eluate is necessary this device is inserted between the column and detector and allows the bulk of the sample to by-pass the detector. [Pg.242]

Recent attention has focused on MS for the direct analysis of polymer extracts, using soft ionisation sources to provide enhanced molecular ion signals and less fragment ions, thereby facilitating spectral interpretation. The direct MS analysis of polymer extracts has been accomplished using fast atom bombardment (FAB) [97,98], laser desorption (LD) [97,99], field desorption (FD) [100] and chemical ionisation (Cl) [100]. [Pg.46]

The mass spectrometer is a mass-flow sensitive device, which means that the signal is proportional to the mass flow dm/dl of the analyte, i.e. the concentration times the flow-rate. It is only now possible to realise the high (theoretically unlimited) mass range and the high-sensitivity multichannel recording capabilities that were anticipated many years ago. Of considerable interest to the problem of polymer/additive deformulation are some of the latest developments in mass spectrometry, namely atmospheric pressure ionisation (API), and the revival of time-of-flight spectrometers (allowing GC-ToFMS, MALDI-ToFMS, etc.). [Pg.351]

With the introduction of FAB in 1981, interest in the development of both DCI and FD sharply decreased. Indeed, on highly polar substances FAB provides more valuable results than DCI or FD and a more stable signal. On the other hand, nonpolar substances with high molecular weight are not amenable to FAB, since they are poorly ionised and also they cannot be easily dissolved in the most common FAB matrices. Thus, alternative ionisation methods have to be employed with such compounds. DCI-MS of nonvolatile compounds has been reviewed [40]. [Pg.365]

Quantitative analysis using FAB is not straightforward, as with all ionisation techniques that use a direct insertion probe. While the goal of the exercise is to determine the bulk concentration of the analyte in the FAB matrix, FAB is instead measuring the concentration of the analyte in the surface of the matrix. The analyte surface concentration is not only a function of bulk analyte concentration, but is also affected by such factors as temperature, pressure, ionic strength, pH, FAB matrix, and sample matrix. With FAB and FTB/LSIMS the sample signal often dies away when the matrix, rather than the sample, is consumed therefore, one cannot be sure that the ion signal obtained represents the entire sample. External standard FAB quantitation methods are of questionable accuracy, and even simple internal standard methods can be trusted only where the analyte is found in a well-controlled sample matrix or is separated from its sample matrix prior to FAB analysis. Therefore, labelled internal standards and isotope dilution methods have become the norm for FAB quantitation. [Pg.369]

Desorption/ionisation techniques such as LSIMS are quite practical, as they give abundant molecular ion signals and fragmentation for structural information. In the conditions of Jackson et al. [96], all the molecular ion and/or protonated molecule ion species were observed in the LSIMS spectrum when only 1 pmol of each additive was placed on the probe tip. However, as mentioned above, in LSIMS/MS experiments the choice of the matrix (e.g. NBA, m-nitrobenzylalcohol) is very important. Matrix effects can lead to suppression of the generation of molecular ions for some additives. LSIMS is not ideal for the quantitative detection of polymer additives, as matrix effects are very important [96]. [Pg.372]

After passing through the column, the separated solutes are sensed by an in-line detector. The output of the detector is an electrical signal, the variation of which is displayed on a potentiometric recorder, a computing integrator or a vdu screen. Most of the popular detectors in hplc are selective devices, which means that they may not respond to all of the solutes that are present in a mixture. At present there is no universal detector for hplc that can compare with the sensitivity and performance of the flame ionisation detector used in gas chromatography. Some solutes are not easy to detect in hplc, and have to be converted into a detectable form after they emerge from the column. This approach is called post-column derivatisation. [Pg.19]

The selectivity of negative or positive ionisation for most of the anionic or non-ionic surfactants, respectively. So, positive ionisation of this environmental extract made compounds recognisable, which were assumed to be AE surfactants because of their equally spaced signals of ions (cf. Fig. 2.5.1(a)). Negative ionisation of the same extract, however, proved the presence of the anionic linear alkylben-... [Pg.158]


See other pages where Ionisation signal is mentioned: [Pg.11]    [Pg.185]    [Pg.368]    [Pg.3136]    [Pg.11]    [Pg.185]    [Pg.368]    [Pg.3136]    [Pg.546]    [Pg.309]    [Pg.242]    [Pg.337]    [Pg.309]    [Pg.274]    [Pg.321]    [Pg.361]    [Pg.362]    [Pg.368]    [Pg.369]    [Pg.372]    [Pg.384]    [Pg.394]    [Pg.395]    [Pg.396]    [Pg.405]    [Pg.412]    [Pg.498]    [Pg.510]    [Pg.541]    [Pg.60]    [Pg.247]    [Pg.132]    [Pg.405]    [Pg.231]    [Pg.388]    [Pg.253]    [Pg.206]    [Pg.154]    [Pg.155]    [Pg.163]    [Pg.166]    [Pg.176]   
See also in sourсe #XX -- [ Pg.47 ]




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