“…Accurate measurements of MPAN are particularly challenging, because TD-CIMS is relatively insensitive to MPAN, and because ions other than methacrylate (CH 2 = C(CH 3 )CO − 2 ), e.g., trifluoromethoxy anions (CF 3 O − , generated from CF 3 OH that outgasses from Teflon tubing) and crotonate (CH 3 CH = CHCO − 2 , generated from peroxycrotonyl nitrate, CPAN), interfere at m/z 85 (Zheng et al, 2011;Mielke and Osthoff, 2012). PANs have also been quantified by proton transfer mass spectrometry (Hansel and Wisthaler, 2000;Hastie et al, 2010) and by quantifying the NO 2 generated from their thermal dissociation (usually by the difference relative to background NO 2 ) using luminol chemiluminescence (CL) (Nikitas et al, 1997;Marley et al, 2004), laser-induced fluorescence (LIF) (Day et al, 2002;Wooldridge et al, 2010), or cavity ring-down spectroscopy (CRDS) (Paul and Osthoff, 2010;Paul et al, 2009). In spite of the development of these new PAN measurement techniques, PAN-GCs remain attractive because of their relative simplicity, compactness, robustness, good sensitivity, and lack of interferences, properties that are desirable for long-term and unattended operations (e.g., Mills et al, 2007;Zhang et al, 2009;Fischer et al, 2010;Zhang et al, 2012).…”