• Sonuç bulunamadı

Electric field dependence of modulation in multilayer InAs quantum dot waveguides

N/A
N/A
Protected

Academic year: 2021

Share "Electric field dependence of modulation in multilayer InAs quantum dot waveguides"

Copied!
1
0
0

Yükleniyor.... (view fulltext now)

Tam metin

(1)

1

Electric Field Dependence of Modulation in Multilayer InAs

Quantum Dot Waveguides

Imran B. Akca1, Aykutlu Dana2, Atilla Aydinli2, Marco Rossetti3, Lianhe Li3, Andrea Fiore3, N. Dagli4 1. Material Science and Nanotechnology Program, Bilkent University, Ankara, Turkey

2. Material Science and Nanotechnology Program and Physics Department, Bilkent University, Ankara, Turkey

3. Institute of Quantum Electronics and Photonics, Ecole Polytechnique Fédérale de Lausanne EPFL, CH-1015 Lausanne, Switzerland 4. ECE Department, University of California at Santa Barbara, California, USA

Semiconductor quantum wells and quantum dots are known to be good candidates for switching and modulation devices in photonic integrated circuits [1]. In this regard, we characterized the electro-absorption and electro-optic properties of multilayer InAs quantum dot waveguides at 1309 and 1515nm.

We worked on three layers (3QDs) of quantum dots with the lengths of 1, 1.3, 1.6 mm. The samples are grown by molecular beam epitaxy. The active region is formed by three layers of self-assembled InAs QDs, which are covered by a 5-nm In0.15Ga0.85As QW and separated from each other by a 40-nm GaAs spacer layer. The areal dot density of our

lens-shaped QDs is 3x1010cm-2. For each sample lasing is peaked at nearly 1285nm [2].

Measurement of the electro-absorption and electro-optic coefficients at 1.3 µm was carried out by coupling light from a tunable laser (Santec TSL-320) onto one end of the waveguide with a lens shaped fiber. At 1.5 µm, Santec Tunable LD Light Source TSL-520 was used. A controlled DC voltage source was used to apply 0 to 20 Volts reverse bias to the samples.At each voltage level, the transmission through the device is recorded as a function of wavelength and voltage.

Figure 1 (a) Voltage dependency of FB resonances of 1.6mm long 3QDs sample. (b) Absorption versus energy graph of the 1 mm long

3QDs sample. The absorption spectra blue shifts under the applied voltages.

The average values for linear electro-optic coefficients (r41/ Γ) of 3QDs samples are given as 7.7x10-13m/V which

is an enhancement compared to the bulk GaAs [1]. As a matter of fact examination of Fig. 1a reveals that full on/off modulation is possible for 1.6 mm long 3 QD sample using 6 V. This corresponds to less than 1 V-cm modulation efficiency. In other words using this modulator as the arms of a push pull driven Mach-Zehnder modulator, less than 1 V drive voltage would result for 1 cm long arms. We have also observed that absorption spectra of the samples blue shift with the applied voltage. We obtained the largest blue shift at the largest applied voltage of 18 Volts. The absorption spectrum is shown in Fig.1b.

In conclusion, we have observed the low voltage modulation in InAs quantum dot waveguides. We have measured the electro-optic coefficient in multilayer quantum dot structures far away from resonance and obtained an enhancement compared to bulk GaAs. Electro-absorption measurement results suggest that these waveguides are good candidates for use in electro-absorption modulators such as Mach-Zehnder devices.

This project is supported by Turkish Scientific and Technical Research Council (TUBITAK); Grant No: 103T115.

References:

[1]. L. Davis, K. Ko, W. Li, H.Sun, Y. Lam, T. Brock, S. Pang, and P. Bhattacharya, "Photoluminescence and electro-optic properties (25-35 nm diameter) quantum boxes", Appl. Phys. Lett., vol. 62, No.22, May 1993

[2]. A. Markus, J. X. Chen, C. Paranthoen, and A. Fiore," Simultaneous two-state lasing in quantum-dot lasers," Applied Physics Letter, vol. 82, No. 12, March 2003. 1515,00 1515,15 1515,30 1515,45 0,2 0,4 0,6 0,8 1,0 1,2 N o rm a liz e d P o w e r O u t λ(nm) 0V 2V 6V 1.6mm long 3QDs sample 6V 2V 0V 0,92 0,93 0,94 0,95 0,96 0,2 0,3 0,4 0,5 0,6 0,7 0,8 0,9 A b s o rp ti o n (a .u .) Energy(eV) 18V 12V 0V 1mm long 3QDs sample Smoothed graph

Shift to towards the left

0V 18V

Şekil

Figure 1 (a) Voltage dependency of FB resonances of 1.6mm long 3QDs sample. (b) Absorption versus energy graph of the 1 mm long 3QDs sample

Referanslar

Benzer Belgeler

For the purpose of the web services composition problem, OWL-S constructs should be translated into compound events in the event calculus framework.. Example of a

Naturally, the source electrode and the substrate experience binding energy shifts equal to or less (due to charging) than the applied potential depending on its

To investigate positive selection on the dog lineage early in the domestication process and prior to the recent diversification of breeds, we re-examine patterns of polymorphism at

Spectral overlap between the donor emission and acceptor excitation used in the preparation of macrocrystals.. As the spectral gap between donor and acceptor

It is important to note in this context that the Sublime Porte, another locus of political power that had limited the royal authority in the seventeenth and eighteenth centuries,

Stability of free standing N-N DB + GaN monolayer phase is only checked for 3x3 unit cell, which gives a stable structure as shown in Fig.. Figure 5.7: a) Phonon dispersion curves

The energy shifts of vacancy-induced localized states relative to the “bare” and extended nitrogene having single vacancy can be retrieved by calculating the local density of

The CEA decoupling system designed in this work uses a unique real time feedback control between the analog cancellation circuit and the MR system to facilitate automated adjustment