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1.
Phys Rev Lett ; 118(23): 233602, 2017 Jun 09.
Artigo em Inglês | MEDLINE | ID: mdl-28644642

RESUMO

We investigate the temperature dependence of photon coherence properties through two-photon interference (TPI) measurements from a single quantum dot (QD) under resonant excitation. We show that the loss of indistinguishability is related only to the electron-phonon coupling and is not affected by spectral diffusion. Through these measurements and a complementary microscopic theory, we identify two independent separate decoherence processes, both of which are associated with phonons. Below 10 K, we find that the relaxation of the vibrational lattice is the dominant contribution to the loss of TPI visibility. This process is non-Markovian in nature and corresponds to real phonon transitions resulting in a broad phonon sideband in the QD emission spectra. Above 10 K, virtual phonon transitions to higher lying excited states in the QD become the dominant dephasing mechanism, this leads to a broadening of the zero phonon line, and a corresponding rapid decay in the visibility. The microscopic theory we develop provides analytic expressions for the dephasing rates for both virtual phonon scattering and non-Markovian lattice relaxation.

2.
Phys Rev Lett ; 111(2): 026403, 2013 Jul 12.
Artigo em Inglês | MEDLINE | ID: mdl-23889424

RESUMO

We report on coherent emission of the neutral exciton state in a single semiconductor self-assembled InAs/GaAs quantum dot embedded in a one-dimensional waveguide, under resonant picosecond pulsed excitation. Direct measurements of the radiative lifetime and coherence time are performed as a function of excitation power and temperature. The characteristic damping of Rabi oscillations observed is attributed to an excitation-induced dephasing due to a resonant coupling between the emitter and the acoustic phonon bath of the matrix. Other sources responsible for the decrease of the coherence time have been evidenced, in particular an enhancement of the radiative recombination rate due to the resonant strong coupling between the dot and the one-dimensional optical mode. As a consequence, the emission couples very efficiently into the waveguide mode, leading to an additional relaxation term of the excited-state population.

3.
Opt Express ; 20(16): 18085-90, 2012 Jul 30.
Artigo em Inglês | MEDLINE | ID: mdl-23038356

RESUMO

Fluorescence spectroscopy is widely used to probe the electromagnetic intensity amplification on optical antennas, yet measuring the excitation intensity amplification is a challenge, as the detected fluorescence signal is an intricate combination of excitation and emission. Here, we describe a novel approach to quantify the electromagnetic amplification in aperture antennas by taking advantage of the intrinsic non linear properties of the fluorescence process. Experimental measurements of the fundamental f and second harmonic 2f amplitudes of the fluorescence signal upon excitation modulation are used to quantify the electromagnetic intensity amplification with plasmonic aperture antennas.

4.
Opt Lett ; 36(17): 3317-9, 2011 Sep 01.
Artigo em Inglês | MEDLINE | ID: mdl-21886196

RESUMO

Conventional fluorescence detection is sensitive to an intricate product of the number of fluorescent emitters times the local excitation intensity. Here, we describe a method to locally quantify the excitation intensity and the number of emitters separately, enabling a clear distinction between the phenomena responsible for a given fluorescence signal. Our technique is based on harmonic excitation modulation and higher-order fluorescence demodulation. It is compatible with a wide range of observations, opening new characterization routes for fluorescence detection or imaging on complex systems, such as plasmonic substrates or scattering media.


Assuntos
Microscopia de Fluorescência/métodos , Fenômenos Ópticos
5.
Opt Express ; 19(13): 12562-8, 2011 Jun 20.
Artigo em Inglês | MEDLINE | ID: mdl-21716497

RESUMO

Performing label free coherent anti-Stokes Raman scattering (CARS) and stimulated Raman scattering (SRS) in endoscope imaging is a challenge, with huge potential clinical benefit. To date, this goal has remained inaccessible because of the inherent coherent Raman noise that is generated in the fiber itself. By developing double-clad hollow core photonic crystal fiber, we demonstrate coherent anti-Stokes Raman scattering and stimulated Raman scattering in an 'endoscope-like' scheme. Both the excitation beams and the collected CARS and SRS signals travel through the same fiber. No CARS and SRS signals are generated within the hollow core fiber even for temporally overlapping pump and Stokes beams, leading to excellent image quality. The CARS and SRS signals generated in the sample are coupled back into a high numerical aperture multimode cladding surrounding the central photonic crystal cladding. We demonstrate this scheme by imaging molecular vibrational bonds of organic crystal deposited on a glass surface.


Assuntos
Cristalização/métodos , Endoscópios , Microscopia/métodos , Fibras Ópticas , Análise Espectral Raman/métodos , Artefatos , Biologia Celular/instrumentação , Desenho de Equipamento , Microscopia Eletrônica de Varredura , Dinâmica não Linear , Polissacarídeo-Liases/química , Vibração
6.
Opt Express ; 17(5): 3165-72, 2009 Mar 02.
Artigo em Inglês | MEDLINE | ID: mdl-19259153

RESUMO

Band-edge photonic crystal lasers were fabricated and their temporal characteristics were minutely analyzed using a high resolution up-conversion system. The InGaAs/InP photonic crystal laser operates at room temperature at 1.55 microm with turn on time ranging from 17ps to 30ps.

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