Cavity ringdown spectra of theà 2 A −X 2 A electronic transition in the IR are reported for the methyl and ethyl peroxy radicals. Analysis of partially resolved rotational structure for the origin band of the transition provides information about both theà andX states of CH3O2·. An estimate for the absorption cross-section is determined from the CRDS absorption and the rate of radical-radical recombination.Low temperature oxidation of hydrocarbons is a pervasive process in both nature and technology. It is critically important for the environmental quality of our atmosphere. [1][2][3][4][5] Similarly it is critical to the efficiency and fuel economy of internal combustion engines. 6-8 Arguably the most important reaction 7 for low temperature oxidation is the production of peroxy radicals (RO 2 ·) from alkyl radicals (R·), i.e.,There are a number of important alkyl peroxy radicals defined by the nature of the R group, ranging 1 from the simplest species, methyl (R=CH 3 ) peroxy to complex species with R containing at least 8-10 carbon atoms with correspondingly many structural isomers. Because of their significance, much effort 1 has been expended studying the mechanisms and kinetics of peroxy radical production and their subsequent reactions. This work has largely been based upon monitoring of the peroxy radicals via theirB 2 A −X 2 A UV absorption. This is a strong transition, common to all the peroxies, that is centered around 240nm.Unfortunately this transition is broad and unstructured with a half-width of ≈40nm. The quasi-continuum nature of this transition has at least two clear disadvantages. It is unsuitable for obtaining rotational or vibrational information about the radical. Additionally the overlapping of the UV spectra of different RO 2 · radicals makes the identification of a specific alkyl peroxy radical, particularly from a mixture, a significant challenge.Experiments involving the peroxyà 2 A −X 2 A transition in the IR are sparse. There was an early report, 9 using low resolution modulated absorption spectroscopy, of the observation of theÃ−X IR transition of several RO 2 · radicals and more recently a report 10 of the observation of fragmentary spectra of ethyl peroxy using a cw absorption technique. There was also a report 11 of the detection of theÃ−X transition of CH 3 O 2 · by intracavity laser absorption spectroscopy, but few spectroscopic details were given. Based upon the recent observation 12 and analysis 13 of a well resolved spectrum of the hydroperoxy radical, HO 2 ·, we expect thẽ A −X IR transitions of the alkyl peroxy radicals to be well structured and observable using cavity ringdown spectroscopy (CRDS).Historically this IR transition has been viewed as difficult to study because of its small oscillator strength (the cross-section σ is ≈ 2 × 10 −21 cm −2 for the corresponding transition 13 in HO 2 ·) and the near IR spectral region (≈ 7000 − 8000 cm −1 ) in which the transition is located. However CRDS is a powerful technique 14-16 for dealing with these difficulties. T...