Lukas Novotny

Facts and artifacts in near-field optical microscopy

Near-field optical (NFO) microscopes with an auxiliary gap width regulation (shear force, tunneling) may produce images that represent the path of the probe rather than optical properties of the sample. Experimental and theoretical evidence leads us to the conclusion that many NFO results reported in the past might have been affected or even dominated by the resulting artifact. The specifications derived from such results for the different types of NFO microscopes used therefore warrant reexamination. We show that the resolving power of aperture NFO microscopes, 30–50 nm, is of genuine NFO origin but can be heavily obscured by the artifact.

Spectral dependence of single molecule fluorescence enhancement.

The fluorescence from a single molecule can be strongly enhanced near a metal nanoparticle acting as an optical antenna. We demonstrate the spectral tunability of this antenna effect and show that maximum enhancement is achieved when the emission frequency is red-shifted from the surface plasmon resonance of the particle. Our experimental results, using individual gold and silver particles excited at different laser-frequencies, are in good agreement with an analytical theory which predicts a different spectral dependence of the radiative and non-radiative decay rates.

Demonstration of Zero Optical Backscattering from Single Nanoparticles

We present the first experimental demonstration of zero backscattering from nanoparticles at optical frequencies as originally discussed by Kerker et al. [ Kerker , M. ; Wang , D. ; Giles , C. J. Opt. Soc. A 1983 , 73 , 765 ]. GaAs pillars were fabricated on a fused silica substrate and the spectrum of the backscattered radiation was measured in the wavelength range 600-1000 nm. Suppression of backscattering occurred at ~725 nm, agreeing with calculations based on the discrete dipole approximation. Particles with zero backscattering provide new functionality for metamaterials and optical antennas.

Scanning near-field optical probe with ultrasmall spot size

A novel light-emitting probe for scanning near-field optical microscopy is investigated theoretically. The three-dimensional vectorial Helmholtz equation is solved for the new probe geometry by using the multiple multipole method. The novel probe consists of a dielectric tip that is entirely metal coated. It provides a single near-field spot that can be smaller than 20 nm (FWHM). The dependence on tip radius, taper angle, and metal thickness in front of the tip is investigated for the power transmission through the probe as well as for the spot size.

Near-field optical imaging using metal tips illuminated by higher-order Hermite-Gaussian beams

Abstract We propose a new scheme for high-resolution near-field optical imaging. The method relies on the highly enhanced fields at sharp metal tips under laser illumination. These fields are laterally confined to the tip size and can be used to locally excite the sample surface. Illumination along the tip axis with a higher-order beam mode (Hermite–Gaussian (1,0) mode) and detection of nonlinear responses (two-photon fluorescence, generation of second/third harmonics) ensure sufficient background discrimination. We outline the theory of laser beams beyond the paraxial approximation and investigate the electromagnetic fields for the proposed scheme.

LIGHT PROPAGATION THROUGH NANOMETER-SIZED STRUCTURES : THE TWO-DIMENSIONAL-APERTURE SCANNING NEAR-FIELD OPTICAL MICROSCOPE

The propagation of light through nanometer-sized structures is studied computationally by use of multiple-multipole method. A two-dimensional scanning near-field optical microscope structure is chosen as an example. The relevant near and far fields as well as some imaging properties are determined for the two principal polarizations. Strikingly different results are obtained for the two principal polarizations: for s polarization, strong field confinement in the gap region, high sensitivity of the radiation pattern to the presence of an object, and high contrast; for p polarization, higher signal level with low contrast. At small gap widths a substantial amount of radiation is coupled into the substrate at angles larger than the critical angle. Line scan simulations for λ = 488 nm indicate a resolution of approximately two times the optical slit width. Resolution and contrast can be optimized by the appropriate choice of detector orientation and angle of acceptance. Coherent superposition of the radiation emitted into different directions permits further improvements.

Electron and phonon renormalization near charged defects in carbon nanotubes

Owing to their influence on electrons and phonons, defects can significantly alter electrical conductance, and optical, mechanical and thermal properties of a material. Thus, understanding and control of defects, including dopants in low-dimensional systems, hold great promise for engineered materials and nanoscale devices. Here, we characterize experimentally the effects of a single defect on electrons and phonons in single-wall carbon nanotubes. The effects demonstrated here are unusual in that they are not caused by defect-induced symmetry breaking. Electrons and phonons are strongly coupled in sp(2) carbon systems, and a defect causes renormalization of electron and phonon energies. We find that near a negatively charged defect, the electron velocity is increased, which in turn influences lattice vibrations locally. Combining measurements on nanotube ensembles and on single nanotubes, we capture the relation between atomic response and the readily accessible macroscopic behaviour.

Raman characterization of defects and dopants in graphene

In this article we review Raman studies of defects and dopants in graphene as well as the importance of both for device applications. First a brief overview of Raman spectroscopy of graphene is presented. In the following section we discuss the Raman characterization of three defect types: point defects, edges, and grain boundaries. The next section reviews the dependence of the Raman spectrum on dopants and highlights several common doping techniques. In the final section, several device applications are discussed which exploit doping and defects in graphene. Generally defects degrade the figures of merit for devices, such as carrier mobility and conductivity, whereas doping provides a means to tune the carrier concentration in graphene thereby enabling the engineering of novel material systems. Accurately measuring both the defect density and doping is critical and Raman spectroscopy provides a powerful tool to accomplish this task.

Subkelvin Parametric Feedback Cooling of a Laser-Trapped Nanoparticle

We optically trap a single nanoparticle in high vacuum and cool its three spatial degrees of freedom by means of active parametric feedback. Using a single laser beam for both trapping and cooling we demonstrate a temperature compression ratio of four orders of magnitude. The absence of a clamping mechanism provides robust decoupling from the heat bath and eliminates the requirement of cryogenic precooling. The small size and mass of the nanoparticle yield high resonance frequencies and high quality factors along with low recoil heating, which are essential conditions for ground state cooling and for low decoherence. The trapping and cooling scheme presented here opens new routes for testing quantum mechanics with mesoscopic objects and for ultrasensitive metrology and sensing.

Plasmon‐coupled tip‐enhanced near‐field optical microscopy

Near the cut‐off radius of a guided waveguide mode of a metal‐coated glass fibre tip it is possible to couple radiation to surface plasmons propagating on the outside surface of the metal coating. These surface plasmons converge toward the apex of the tip and interfere constructively for particular polarization states of the initial waveguide mode. Calculations show that a radially polarized waveguide mode can create a strong field enhancement localized at the apex of the tip. The highly localized enhanced field forms a nanoscale optical near‐field source.