Abstract

Conventional absorption spectroscopy is not nearly sensitive enough for quantitative overtone measurements on submonolayer coatings. While cavity-enhanced absorption detection methods using microresonators have the potential to provide quantitative absorption cross sections of even weakly absorbing submonolayer films, this potential has not yet been fully realized. To determine the absorption cross section of a submonolayer film of ethylene diamine (EDA) on a silica microsphere resonator, we use phase-shift cavity ringdown spectroscopy simultaneously on near-IR radiation that is Rayleigh backscattered from the microsphere and transmitted through the coupling fiber taper. We then independently determine both the coupling coefficient and the optical loss within the resonator. Together with a coincident measurement of the wavelength frequency shift, an absolute overtone absorption cross section of adsorbed EDA, at submonolayer coverage, was obtained and was compared to the bulk value. The smallest quantifiable absorption cross section is σmin=2.7×10−12 cm2. This absorption cross section is comparable to the extinction coefficients of, e.g., single gold nanoparticles or aerosol particles. We therefore propose that the present method is also a viable route to absolute extinction measurements of single particles.

Highlights

  • Single-molecule detection and single-atom detection rely largely on the measurement of excited-state fluorescence [1,2]

  • The maximum dosage level indicated by the quartz crystal microbalance (QCM) is a factor of 4 greater than that based on the whispering gallery” cavity modes (WGMs) wavelength shift

  • We use the more reliable coverages obtained from Eq (1) instead of the values given by the QCM

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Summary

Introduction

Single-molecule detection and single-atom detection rely largely on the measurement of excited-state fluorescence [1,2]. The resonance frequencies of the “whispering gallery” cavity modes (WGMs) are sensitive to the surface coverage and the refractive index of the adsorbed chemical species [11,19], while the optical absorption of the surface layer leads to a decrease of the quality (Q) factor [20] and can be retrieved either from the reduction of power that is transferred to the resonator mode [21], from the decrease of the cavity ringdown time, or from the broadening of the resonance line These cavity-enhanced absorption detection methods have, the potential to provide quantitative absorption cross sections of single particles. A measurement of the total optical loss in the microresonator obtained from resonance lifetime or linewidth measurements does not permit us to distinguish losses due to molecular absorption from changes in the cavity coupling coefficient

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