Abstract

AbstractCoherent control is an ingenious tactic to steer a system to a desired optimal state by tailoring the phase of an incident ultrashort laser pulse. A relevant process is the two-photon–induced photoluminescence (TPPL) of nanoantennas, as it constitutes a convenient route to map plasmonic fields, and has important applications in biological imaging and sensing. Unfortunately, coherent control of metallic nanoantennas is impeded by their ultrafast femtosecond dephasing times so far limiting control to polarization and spectral optimization. Here, we report that phase control of the TPPL in resonant gold nanoantennas is possible. We show that, by compressing pulses shorter than the localized surface plasmon dephasing time (<20 fs), a very fast coherent regime develops, in which the two-photon excitation is sensitive to the phase of the electric field and can therefore be controlled. Instead, any phase control is gone when using longer pulses. Finally, we demonstrate pure phase control by resorting to a highly sensitive closed-loop strategy, which exploits the phase differences in the ultrafast coherent response of different nanoantennas, to selectively excite a chosen antenna. These results underline the direct and intimate relation between TPPL and coherence in gold nanoantennas, which makes them interesting systems for nanoscale nonlinear coherent control.

Highlights

  • In the field of optics, coherent control refers to the capability of precisely tailored laser fields to actively manipulate the outcome of certain light–matter interactions by exploiting the coherent properties of the system under study

  • In order to unveil the coherent response of gold nanoantennas, we first investigated the ultrafast dynamics of the two-photon excitation (TPE) by varying the excitation pulse duration in the range of 15 fs–1 ps and detecting the two-photon–induced photoluminescence (TPPL) with a high-resolution confocal microscope

  • We have presented a detailed and comprehensive study of the TPE process and its dependence on the phase of an ultrashort laser pulse in gold nanoantennas

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Summary

Introduction

In the field of optics, coherent control refers to the capability of precisely tailored laser fields to actively manipulate the outcome of certain light–matter interactions by exploiting the coherent properties of the system under study. Stockman et al [23] and Stockman [24] first linked the field of coherent control to the study of optical nanoantennas with the objective of simultaneously achieving nanometre and femtosecond control of optical fields Experimental demonstrations of such control principle include: the phase and polarization manipulation of nanooptical fields in the incoherent regime [25, 26]; the simultaneous high space and time resolution imaging of surface plasmon dynamics in the coherent and incoherent regimes [27,28,29,30,31,32,33]; and the phase-dependent control of the propagation of LSPRs through nanoparticle arrays caused by different amounts of dispersion acquired in different propagation directions [34, 35]. We show that the intrinsic nature of the TPE in gold nanoantennas, in which an intermediate state (the LSPR) mediates the process, leads to a very fast initial coherent regime This regime is only accessible by ultrashort laser pulses, shorter than the coherence time T2 (

The initial coherent regime
Closed-loop coherent control of pairs of nanoantennas
Conclusions
Methods
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