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Analytical Chemistry Chemical Cytometry Quantitates Superoxide

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Figure 2. Intensity chromatograms for the n-alkanes mixture<br />

obtained in the SIM mode: (a) at m/z ) 71 operating the setup in the<br />

qualitative configuration; (b) at m/z 44 and 45 operating the setup in<br />

the quantitative configuration.<br />

and the filling of the reservoir, traces of this compound possibly<br />

present in the Helium gas used to dilute de 13 CO2 and traces<br />

of air still present in the EI source. The high enrichment<br />

obtained provides a very wide range of optimum analyte/spike<br />

ratios and then a sample containing compounds in a large range<br />

of concentrations could be quantified in the same analysis<br />

without affecting the accuracy of the results. 3<br />

The short-term (30 min) and long-term (9 h) stability of the<br />

12 C/ 13 C isotope ratio is given in the Supporting Information<br />

(Figures SI-3 and SI-4). In both cases the measured isotope ratios,<br />

0.0339 ± 0.0002 and 0.034 ± 0.001 (n ) 8), respectively, were<br />

remarkably stable. Similar results were obtained in different days<br />

indicating that the setup was robust enough for routine analysis.<br />

Evaluation of the GC-Combustion-IDMS System. The<br />

overall performance of the developed instrumentation was evaluated<br />

here by analyzing a standard solution of a mixture of<br />

n-alkanes (C9-C20). To study peak broadening, 1 µL of a<br />

solution containing approximately 5 µg/g of these compounds<br />

in n-hexane was injected in the chromatograph both in the<br />

qualitative (combustion oven bypassed) and quantitative (through<br />

the oven) modes. The Selected Ion Monitoring chromatogram<br />

obtained at m/z ) 71 (fragment characteristic of n-alkanes) is<br />

shown in Figure 2a, whereas the chromatogram obtained at<br />

masses 44 and 45 after combustion and postcolumn isotope<br />

dilution analysis is shown in Figure 2b. As can be observed, no<br />

significant peak broadening due to the combustion unit or to the<br />

different connections was observed, being the peak width measured<br />

at the half height equal to that found when operating the<br />

6866 <strong>Analytical</strong> <strong>Chemistry</strong>, Vol. 82, No. 16, August 15, 2010<br />

Figure 3. Mass flow chromatograms obtained for the n-akanes<br />

mixture.<br />

GC-MS in the conventional way (0.02 min, Figure 2a). Only a small<br />

increase in retention times was observed (∼20 s) because of the<br />

combustion furnace. The mass flow chromatogram obtained after<br />

the application of the online isotope dilution equation (eq 1) is<br />

shown in Figure 3. As can be observed, the sensitivity is roughly<br />

constant for all compounds which is in clear contrast with the<br />

results shown in Figure 2a for mass 71 without combustion (SIM<br />

detection). The peak areas in the mass flow chromatogram were<br />

linear with the amount of carbon injected over 2 orders of<br />

magnitude (the maximum range assayed). The detection limit<br />

obtained for tetradecane was 9 ppb (ng/g) based on three times<br />

the standard deviation of the baseline. Taking into account that<br />

the injection volume was 0.5 µL, this value corresponds to an<br />

absolute limit of detection of 3 pg of tetradecane injected. If we<br />

take into account the peak width at the baseline (4s approximately<br />

in this particular case), then we can make our detection limit<br />

independent of the column employed and the carrier gas flowrate.<br />

The value found was 0.8 pg C s -1 , being in the same order<br />

that those provided by a mass spectrometer in full scan mode<br />

(1 pg C s -1 ) and clearly better than those of a flame ionization<br />

detector (10 pg C s -1 ). This detection limit is mainly limited<br />

by the background level observed at m/z ) 44, and explains<br />

the difference in comparison with the detection limit achievable<br />

using the mass spectrometer in SIM mode bypassing the oven<br />

(typically 0.1 pg C s -1 ) in spite of the fact that both sensitivities<br />

were very similar. In contrast, it should be mentioned that the<br />

EI detection limit observed is 3 orders of magnitude lower than<br />

that obtained for carbon using 13 C postcolumn isotope dilution<br />

and ICP-MS detection (0.7 ng C s -1 ). 12<br />

For the quantitative analysis of the standard mixture of<br />

n-alkanes (C9-C20) we needed first to quantify the mass flow<br />

of postcolumn 13 CO2. Out of the two possibilities of using<br />

internal standard (IS) or external standard, we selected an IS<br />

because it provided the advantage of compensation for small<br />

variations in the sample volume injected (we were using manual<br />

injection). Moreover, as recently pointed out by Heilmann and<br />

Heumann, 11 an additional advantage of using an internal<br />

standard is that the mass flow of enriched carbon dioxide does<br />

not need to be determined. The peak areas of both the analyte<br />

and the internal standard in the mass flow chromatogram are<br />

related to the unknown mass flow of spike (eq 1). However,<br />

the ratio of peak areas analyte/IS will be equal to the actual ratio<br />

of concentrations in the injected sample and independent of the<br />

mass flow of spike used in the calculations. Thus, quantification

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