- Nano Express
- Open Access
Single-photon emission from single InGaAs/GaAs quantum dots grown by droplet epitaxy at high substrate temperature
© Benyoucef et al.; licensee Springer. 2012
- Received: 18 July 2012
- Accepted: 21 August 2012
- Published: 31 August 2012
The authors report single-photon emission from InGaAs quantum dots grown by droplet epitaxy on (100) GaAs substrates using a solid-source molecular beam epitaxy system at elevated substrate temperatures above 400°C without post-growth annealing. High-resolution micro-photoluminescence spectroscopy exhibits sharp excitonic emissions with lifetimes ranging from 0.7 to 1.1 ns. The coherence properties of the emitted photons are investigated by measuring the first-order field correlation function.
- III-V semiconductors
- Quantum dots
- Droplet epitaxy
- Single-photon emission
- Radiative lifetime
Various quantum emitters have been used to demonstrate single-photon emission, with single atoms or ions being the prototypical examples [1, 2]. Other systems capable of single-photon generation are single molecules and single nanocrystals [3–5]. Their main drawback is their time stability, which is restricted by photo-bleaching and blinking .
Self-assembled semiconductor quantum dots (QDs) are the most promising zero-dimensional material system for the production of triggered single photons with high repetition rate [5, 7, 8], indistinguishable photons , and entangled photon pairs . These are essential for quantum information and in novel photonic devices such as lasers, solar cells, detectors, and light-emitting diodes due to their ability to control their optical properties and the growth process. The Stranski-Krastanov (SK) method is the most used growth method on lattice-mismatched substrates.
Droplet epitaxy (DE) growth method was proposed  as an effective way of fabricating QDs without a wetting layer (WL) for both lattice-matched and lattice-mismatched epitaxial systems. Due to the lack of a WL, the DE QDs might have improved carrier confinement with high optical quality. DE offers advantages over the conventional SK method and thus a unique route to the fabrication of unpredicted nanostructures. Typically, DE uses low temperature for QD growth to prevent material redistribution [12, 13]. However, the low-temperature growth hinders the good optical quality of the grown QD structures. Post-growth annealing processes were used for the restoration of the crystalline quality [14, 15]. Post-growth annealing at 680°C for 1 h  improved the photoluminescence (PL) intensity, indicating efficient passivation of defects. It should be noted that some trap defects formed during the low-temperature growth cannot be recovered even by rapid thermal annealing at very high temperature. This problem could be avoided by growing the QDs at high substrate temperatures .
In this work, we report on the observation of triggered single-photon emission from a single InGaAs QD grown by DE mode on (100) GaAs substrates using a solid-source molecular beam epitaxy system at elevated substrate temperatures above 400°C. The morphological and structural properties are investigated. Their optical properties are characterized by single-dot spectroscopy and time-resolved spectroscopy. The excitonic states of a single QD are identified using power-dependent measurements on mesa-patterned samples.
The investigated samples were grown on GaAs substrates by DE mode in a GEN II molecular beam epitaxy (MBE) system (Veeco Instruments Inc., Plainview, NY, USA) using an arsenic valved cracker cell for precise control of the As4 flux. The temperatures were measured using an optical pyrometer, and the QD formation was observed by reflection high-energy electron diffraction (RHEED). After removal of the native oxide at 600°C under As4 flux, a 200-nm GaAs buffer layer was grown at 590°C with a growth rate of 1 monolayer (ML)/s. Then, the InGaAs QDs have been grown under constant growth conditions. The substrate temperature was decreased to desired temperatures of 410°C and 500°C, and the arsenic valve was completely closed to reach a background pressure in the order of 1 × 10−9 Torr. A nominal amount of gallium equivalent to 1.75 MLs of GaAs was deposited on the GaAs buffer layer. Then, indium droplets equivalent to an amount of 4 MLs of InAs were deposited on the Ga-stabilized surface and supplied with an As4 molecular beam flux of 10−5-Torr beam equivalent pressure for a relatively short time to crystallize the indium droplets into InGaAs QDs. The time for QD formation was determined by RHEED. The QDs were capped with a 50-nm GaAs barrier layer with a growth rate of 1 ML/s without growth interruption. A second QD layer was grown on the top of the sample at the same growth conditions as the first QD layer for morphology investigations. Then, the samples were rapidly cooled down without arsenic pressure and taken out from the MBE chamber. For this study, we investigate two samples: Sample (A) and sample (B) consist of InGaAs QDs grown on a (100) GaAs substrate at 410°C and 500°C, respectively. It should be noted that no post-growth and rapid thermal annealing processes were applied in this study.
The PL measurements are performed at 5 K. The sample is mounted in a helium flow cryostat which can be moved using computer-controlled xy-linear stages with a spatial resolution of 100 nm. A microscope objective (NA = 0.7) is used to focus continuous wave (cw) laser with an excitation wavelength of 532 nm for micro-photoluminescence (μPL) measurements and a Ti:sapphire laser operating at 845 nm for photon correlation and time-resolved measurements. The same microscope objective was used to collect the QD emission. The collected luminescence was then spectrally filtered using a 0.75-m focal length monochromator equipped with a liquid nitrogen-cooled charge-coupled device for PL measurements. For photon statistics measurements, the PL light is directly sent to a modified Hanbury Brown and Twiss (HBT) correlation setup. The HBT consisted of a 50/50 non-polarizing beam splitter, two bandpass filters used to select a specific emission line, and two single-photon counting avalanche photodiodes (APDs), each providing a time resolution of approximately 700 ps. The lifetime measurements are performed using time-correlated single-photon counting technique. The signal is detected using a fast APD with a temporal resolution of about 50 ps.
From atomic force microscope studies (data not shown here), the QD density decreases from approximately 1011 to approximately 5 × 109 cm−2 with increasing substrate temperature from 410°C to 500°C, respectively, due to the larger diffusion length of the indium atoms at higher substrate temperature which shows a behavior similar to SK growth mode. The optical properties of the QD ensemble characterized by macro-photoluminescence (not shown here) show that the emission wavelength of QDs formed at 410°C is blueshifted in comparison to that of QDs formed at 500°C due to the smaller size of dots. The energy peak and the full width at half maximum of a QD ensemble grown at 500°C are similar to those of QDs grown by SK which is an indication for the good optical quality of the QDs formed by DE. For the following, we focus on single-QD investigations.
To confirm the improvement in optical quality, we have also performed time-resolved μPL measurements on single QDs in sample B. Figure 3b shows typical time-resolved PL of the X line of single QD. While the excitonic lifetimes of QDs in sample A are less than 0.8 ns, those of sample B are larger than 1.1 ns. These results confirm the improved optical quality of QDs grown at 500°C. This could be due to the removal of excess arsenic atoms which act as effective nonradiative recombination centers. The increased radiative lifetime for QDs grown at 500°C compared to QDs grown at 410°C could also be due to the increasing QD size, which has been predicted theoretically  and also reported experimentally . This could likely be due to variation of the e-h overlap induced by different QD morphologies and by piezoelectric effects . However, further investigations are necessary to classify the nature of the defects related to the excess arsenic incorporation by using low-density QD samples.
In conclusion, we have demonstrated single-photon emission from single InGaAs QDs grown by droplet epitaxy at elevated substrate temperatures. Excitation power-dependent and time-resolved micro-photoluminescence (TRμPL) measurements were performed at low temperature to characterize the optical properties of the excitonic states. TRμPL measurements showed an increase in lifetime from 0.70 to 1.16 ns with the increasing substrate temperature, which could be related to the removal of excess arsenic atoms that act as nonradiative recombination centers and the increased QD sizes. The lifetime characteristics were attributed to good quantum confinement of carriers in DE-grown QDs.
We acknowledge F. Schnabel, A. Dirk, and K. Fuchs for the technical support. This work was supported by the BMBF (QuaHL-Rep).
- Kuhn A, Hennrich M, Rempe G: Deterministic single-photon source for distributed quantum networking. Phys Rev Lett 2002, 89: 067901.View ArticleGoogle Scholar
- Keller M, Lange B, Hayasaka K, Lange W, Walther H: Continuous generation of single photons with controlled waveform in an ion-trap cavity system. Nature (London) 2004, 431: 1075–1078. 2004. 2004. 10.1038/nature02961View ArticleGoogle Scholar
- Brunel C, Lounis B, Tamarat P, Orrit M: Triggered source of single photons based on controlled single molecule fluorescence. Phys Rev Lett 1999, 83: 2722–2725. 10.1103/PhysRevLett.83.2722View ArticleGoogle Scholar
- Lounis B, Moerner WE: Single photons on demand from a single molecule at room temperature. Nature (London) 2000, 407: 491–493. 10.1038/35035032View ArticleGoogle Scholar
- Michler P, Kiraz A, Becher C, Schoenfeld WV, Petroff PM, Zhang L, Hu E, Imamoglu A: A quantum dot single-photon turnstile device. Science 2000, 290: 2282–2285. 10.1126/science.290.5500.2282View ArticleGoogle Scholar
- Nirmal M, Dabbousi BO, Bawendi MG, Macklin JJ, Trautman JK, Harris TD, Brus LE: Fluorescence intermittency in single cadmium selenide nanocrystals. Nature (London) 1996, 383: 802–804. 10.1038/383802a0View ArticleGoogle Scholar
- Gérard JM, Gayral B: Strong purcell effect for InAs quantum boxes in three-dimensional solid-state microcavities. J Lightwave Technol 1999, 17: 2089–2095. 10.1109/50.802999View ArticleGoogle Scholar
- Benyoucef M, Ulrich SM, Michler P, Wiersig J, Jahnke F, Forchel A: Correlated photon pairs from single (In, Ga)As/GaAs quantum dots in pillar microcavities. J Appl Phys 2005, 97: 023101. 10.1063/1.1809251View ArticleGoogle Scholar
- Santori C, Fattal D, Vučković J, Solomon GS, Yamamoto Y: Indistinguishable photons from a single-photon device. Nature (London) 2002, 419: 594–597. 10.1038/nature01086View ArticleGoogle Scholar
- Stevenson RM, Young RJ, Atkinson P, Cooper K, Ritchie DA, Shields AJ: A semiconductor source of triggered entangled photon pairs. Nature (London) 2006, 439: 179–182. 10.1038/nature04446View ArticleGoogle Scholar
- Koguchi N, Takahashi S, Chikyow T: New MBE growth method for InSb quantum well boxes. J Crystal Growth 1991, 111: 688–692. 10.1016/0022-0248(91)91064-HView ArticleGoogle Scholar
- Koguchi N: Toward the fabrication of site-controlled III-V compound semiconductor quantum dots by droplet epitaxy. J Korean Physical Society 2004, 45: 650–655.Google Scholar
- Wang ZM, Holmes K, Mazur YI, Ramsey KA, Salamo GJ: Self-organization of quantum-dot pairs by high-temperature droplet epitaxy. Nanoscale Res Lett 2006, 1: 57–61. 10.1007/s11671-006-9002-zView ArticleGoogle Scholar
- Watanabe K, Tsukamoto S, Gotoh Y, Koguchi N: Photoluminescence studies of GaAs quantum dots grown by droplet epitaxy. J Cryst Growth 2001, 227: 1073–1077.View ArticleGoogle Scholar
- Sanguinetti S, Mano T, Gerosa A, Somaschini C, Bietti S, Koguchi N, Grilli E, Guzzi M, Gurioli M, Abbarchi M: Rapid thermal annealing effects on self-assembled quantum dot and quantum ring structures. J Appl Phys 2008, 104: 113519. 10.1063/1.3039802View ArticleGoogle Scholar
- Zürbig V, Bugaew N, Reithmaier JP, Kozub M, Musiał A, Sęk G, Misiewicz J: Growth temperature dependence of wetting layer formation in high density InGaAs/GaAs quantum dot structures grown by droplet epitaxy. Jpn J Appl Phys 2012, 51: 085501.View ArticleGoogle Scholar
- Abbarchi M, Troiani F, Mastrandrea C, Goldoni G, Kuroda T, Mano T, Sakoda K, Koguchi N, Sanguinetti S, Vinattieri A, Gurioli M: Spectral diffusion and line broadening in single self-assembled GaAs/AlGaAs quantum dot photoluminescence. Appl Phys Lett 2008, 93: 162101. 10.1063/1.3003578View ArticleGoogle Scholar
- Stier O, Grundmann M, Bimberg D: Electronic and optical properties of strained quantum dots modeled by 8-band k·p theory. Phys Rev B 1999, 59: 5688–5701. 10.1103/PhysRevB.59.5688View ArticleGoogle Scholar
- Boggess TF, Zhang L, Deppe DG, Huffaker DL, Cao C: Spectral engineering of carrier dynamics in In(Ga)As self-assembled quantum dots. Appl Phys Lett 2001, 78: 276–278. 10.1063/1.1337638View ArticleGoogle Scholar
- Heitz R, Veit M, Ledentsov NN, Hoffmann A, Bimberg D, Ustinov VM, Kop’ev PS, Alferov ZI: Energy relaxation by multiphonon process in InAs/GaAs quantum dots. Phys Rev B 1997, 56: 10435–10445. 10.1103/PhysRevB.56.10435View ArticleGoogle Scholar
- Kammerer C, Cassabois G, Voisin C, Perrin M, Delalande C, Roussignol P, Gérard JM: Interferometric correlation spectroscopy in single quantum dots. Appl Phys Lett 2002, 81: 2737–2739. 10.1063/1.1510158View ArticleGoogle Scholar
- Benyoucef M, Wang L, Rastelli A, Schmidt OG: Toward quantum interference of photons from independent quantum dots. Appl Phys Lett 2009, 95: 261908. 10.1063/1.3275702View ArticleGoogle Scholar
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