International audienceWe 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

Plasmonic near fields, wherein light is magnified and focused within nanoscale volumes, are utilized in a broad array of technologies including optoelectronics, catalysis, and sensing. Within these nanoscale cavities, increases in temperature are expected and indeed have been demonstrated. Heat generation can be beneficial or detrimental for a given system or technique, but in either case it is useful to have knowledge of local temperatures. Surface-enhanced Raman spectroscopy (SERS), potentially down to the limit of single-molecule (SM) detection, has been suggested as a viable route for measuring nanoscale temperatures through simultaneous collection of Stokes and anti-Stokes SER scattering, as the ratio of their intensities is related to the Boltzmann distribution. We have rigorously verified SM detection in anti-Stokes SERS of rhodamine 6G on aggregated Ag nanoparticles using the isotopologue method. We observe a broad distribution in the ratio of anti-Stokes and Stokes signal intensities among SM events. An equivalent distribution in high-coverage, single-aggregate SERS suggests that the observed variance is not a SM phenomenon. We find that the variance is instead caused by a combination of local heating differences among hot spots as well as variations in the near-field strength as a function of frequency, effectively causing nonequivalent enhancement factors (EFs) for anti-Stokes and Stokes scattering. Additionally, we demonstrate that dark-field scattering cannot account for the frequency dependence of the optical near field. Finite-difference time-domain simulations for nanoparticle aggregates predict a significant wavelength dependence to the ratio of anti-Stokes/Stokes EFs, confirming that the observed variation in this ratio has strong nonthermal contributions. Finally, we outline the considerations that must be addressed in order to accurately evaluate local temperatures using SERS.

Ultrafast optical pump, X-ray diffraction probe experiments were performed on CdSe nanocrystal (NC) colloidal dispersions as functions of particle size, polytype, and pump fluence. Bragg peak shifts related to heating and peak amplitude reduction associated with lattice disordering are observed. For smaller NCs, melting initiates upon absorption of as few as ∼15 electron-hole pair excitations per NC on average (0.89 excitations/nm for a 1.5 nm radius) with roughly the same excitation density inducing melting for all examined NCs. Diffraction intensity recovery kinetics, attributable to recrystallization, occur over hundreds of picoseconds with slower recoveries for larger particles. Zincblende and wurtzite NCs revert to initial structures following intense photoexcitation suggesting melting occurs primarily at the surface, as supported by simulations. Electronic structure calculations relate significant band gap narrowing with decreased crystallinity. These findings reflect the need to consider the physical stability of nanomaterials and related electronic impacts in high intensity excitation applications such as lasing and solid-state lighting.