Abstract

We demonstrate theoretically and experimentally that the three-dimensional orientation of a single fluorescent nanoemitter can be determined by polarization analysis of the emitted light (while excitation polarization analysis provides only the in-plane orientation). The determination of the emitter orientation by polarimetry requires a theoretical description, including the objective numerical aperture, the 1D or 2D nature of the emitting dipole, and the environment close to the dipole. We develop a model covering most experimentally relevant microscopy configurations and provide analytical relations that are useful for orientation measurements. We perform polarimetric measurements on high-quality core-shell CdSe/CdS nanocrystals and demonstrate that they can be approximated by two orthogonal degenerated dipoles. Finally, we show that the orientation of a dipole can be inferred by polarimetric measurement, even for a dipole in the vicinity of a gold film, while in this case, the well-established defocused microscopy is not appropriate.

Highlights

  • The determination of the orientation of a single photoluminescent emitter has been a major issue since early single-molecule studies [1,2,3,4,5]

  • We demonstrate theoretically and experimentally that the three-dimensional orientation of a single fluorescent nanoemitter can be determined by polarization analysis of the emitted light

  • We show that the three-dimensional orientation ðΘ; ΦÞ of a nanoemitter can be obtained by analyzing its emission polarization on avalanche photodiodes, even in the case of a fluctuating emission

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Summary

INTRODUCTION

The determination of the orientation of a single photoluminescent emitter has been a major issue since early single-molecule studies [1,2,3,4,5]. In order to measure Θ, various sophisticated schemes have been proposed to increase the out-of-plane component of the electric field [4,19,20,21,22,23] Most of these works intrinsically probe the orientation of the absorbing dipole, which for nonresonant photoluminescence can be extremely different from the emitting dipole. We provide an analytical model that can be used to interpret the data and extract ðΘ; ΦÞ in a wide range of realistic experimental conditions We demonstrate this experimentally by measuring the orientation of highquality thick-shell CdSe/CdS nanocrystals with 2D-dipolar emission, including the case when the emitter lies in proximity to a gold film, a situation for which the more standard defocused imaging is not sufficiently sensitive to provide reliable information. VI, we consider the case of a nanocrystal near a metallic film and show that the orientation can be obtained from polarization analysis but not from defocused imaging

THEORETICAL FRAMEWORK
CA sin θ1 cos φ
DETERMINATION OF THE EMITTING DIPOLE DIMENSION
THEORETICAL RESULTS
EXPERIMENTAL ORIENTATION MEASUREMENT
VICINITY OF A GOLD SURFACE
CONCLUSION
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