An Efficient Source of Single Photons: A Single Quantum Dot in a Micropost Microcavity Matthew Pelton Glenn Solomon, Charles Santori, Bingyang Zhang, Jelena.

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Presentation transcript:

An Efficient Source of Single Photons: A Single Quantum Dot in a Micropost Microcavity Matthew Pelton Glenn Solomon, Charles Santori, Bingyang Zhang, Jelena Vučković, Jocelyn Plant, Edo Waks, and Yoshihisa Yamamoto University of Illinois at Urbana-Champaign Quantum Information Science Seminar April 9, 2003

Quantum Dots Increasing number of confining dimensions leads to fully quantized density of states

Self-Assembled Quantum Dots Advantages for single-photon source: Confined electron and hole levels Large oscillator strength Long-term stability High radiative efficiency Narrow emission bandwidth Possibility of incorporation into devices

Single-Dot Spectroscopy Dots isolated by etching microscopic mesas Electron-hole pairs excited in GaAs by laser pulse Carriers trapped in dots and relax to the ground state, where they recombine Conduction Band n=2 n=1 >1.52 eV 1.04 - 1.45 eV n=1 n=2 Valence Band

Carrier Complexes Ground-state emission shows several narrow peaks Coulomb interaction among carriers: excitons (X), biexcitons (2X), charged excitons, etc. 2X X Emission from the exciton recombination comes after emission from the biexciton recomb. Intensity (arbitrary units) Wavelength (nm)

Single-Photon Generation Excite with pulsed laser For each pulse, the last photon will be emitted at a unique frequency Spectral filtering isolates regulated single photons Dot Filter 1X 2X 3X C. Santori, M. Pelton, G. S. Solomon, Y. Dale, and Y. Yamamoto, Phys. Rev. Lett. 86 (8), 1502 (2001).

Modified Spontaneous Emission Most photons are radiated into the substrate: Efficiency  10-3 Linear elements can only redirect emission Changing density of available electromagnetic modes can change the rate of emission into useful directions Done using microscopic optical cavity: enhanced emission into resonant cavity modes G. S. Solomon, M. Pelton, and Y. Yamamoto, Phys. Rev. Lett. 86 (17), 3903 (2001). M. Pelton, J. Vučković, G. S. Solomon, A. Scherer, and Y. Yamamoto, IEEE J. Quantum Electron. 38 (2), 170 (2002).

Micropost Microcavities Planar microcavities grown by MBE Stacks of alternating quarter-wavelength thick AlAs / GaAs layers Separated by wavelength-thick GaAs layer Etched post acts as a waveguide Light confined in three dimensions 5 mm 0.5 mm

Etched Posts 0.6 mm Mirror stack 4.2 mm Cavity Mirror stack

Experimental Setup II

Poissonian Light Scattered laser light: all peak areas equal Coincidences Delay (ns)

Antibunching Scattered laser light: all peak areas equal Light from dot: central peak area is small

Antibunching Fit uses measured quantum-dot lifetime and instrument response time

Antibunching Multi-photon probability increases with pump power Possibly due to excitation of other states

Efficiency Efficiency saturates as pump power increases: hmax = 37 ± 1% M. Pelton, et al., Phys. Rev. Lett. 89, 233602 (2002). Note: This is the efficiency to emit a photon, not for the photon to leave the cavity, nor to be collected into a single-mode fiber!

Achieved g(2) = 0.04