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Quantum-Dot Lasers Nanoelectronics term project R91543013 徐維良 指導教授 : 劉致為.

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Presentation on theme: "Quantum-Dot Lasers Nanoelectronics term project R91543013 徐維良 指導教授 : 劉致為."— Presentation transcript:

1 Quantum-Dot Lasers Nanoelectronics term project R91543013 徐維良 指導教授 : 劉致為

2 Outline  半導體雷射與 Quantum dot laser  Quantum dot laser 的製造  Quantum dot laser 的特色  高能的 Quantum dot laser  1.3 µ m Quantum Dot Lasers  結論

3 半導體雷射 LASER:Light Amplification by Stimulated Emission of Radiation 必要的元件 : --Gain medium --Optical feedback 利用 Quantum dot transition 的放射結合來放大. Pumping over p-n junction by current injection 利用水晶面來反射以共振

4 增益與尺寸

5 Quantum Dot 的好處 Discrete energy level : high density of states no temperature dependence

6 Quantum Dot 的好處 reduced diffusion → no diffusion to surfaces reduced active volume → low absorption, low inversion densities refractive index decoupled from carrier density → no chirp

7 Quantum dot laser 的製造 MBE-Growth Integration of Quantum dot layer into the active zone of a semiconductor laser Dot density>10^10cm^-2

8 改良 Carrier Confinement SSLs as 布拉格反射體 改良 Carrier Confinement Quantum dot laser 的 active region 對於 thermal losses 較 敏感

9 改良 Carrier Confinement 不同區域的 short period superlattices 之結合  mini bandgap 的部分重合導致 effective barrier height 的增加

10 溫度與 Quantum dot laser Operation temperature > 210 °C Reduced wavelength shift: QW: 0.33 nm/K QDots: 0.17 - 0.19 nm/K

11 Quantum dot laser 之增益 About 3 times broader gain spectrum due to dot size distribution Much larger tuning range for wavelength tuning of DFB lasers

12 Single mode Emitting Quantum dot lasers 使用 E-Beam 製造 Wavelength selection by grating periode (SMSR = 52 dB) Ith < 20 mA for all periods (.λ = 33 nm)

13 溫度穩定性 Stable single mode emission No mode hopping Single mode operation over 194K temperature range 三倍大的頻寬 溫度飄移少一倍

14 Quantum Dot 與 Quantum Well Reduced threshold current density for L > 2.5 mm (cross over) Lower optical confinement for QDots, but inversion condition is relaxed

15 Material Gain of Q-Dot and QW- Laser

16 波長對溫度敏感度 Quantum dot laser 有較 低的溫度敏感度 △ λ/ △ T = 0.35 nm/K for QWLs = 0.23 nm/K for QDLs

17 高能的 Quantum dot laser 2 mm × 100 µ m broad area laser Record value of 4 W cw output power Wall plug efficiency > 50 % at 1 W

18 高能的 Quantum dot laser Emission by fundamental mode High temperature stability Low wavelength shift (for QWs 50% higher)

19 高能的 Quantum dot laser 在 20°C 與 80°C 的區域中,每增 加一瓦的能量,只有多百分之二十 的電流 高的 characteristic temperature T= 110 K up to 110 °C

20 1.3 µ m Quantum Dot Lasers  替代昂貴的 InP-based material system  Growth on GaAs substrates, -- 便宜、 大的 WAFER 面積 (6", 8")  special dot 優點 --low threshold density --broad gain function --low temperature sensitivity

21 InAs/GaInAs Quantum Dots InAs embedded in GaInAs buffer layers – Room temperature emission at 1.3 µ m – High quantum dot density Growth rate: r(GaAs) = 1 µ m/h r(InAs) = 140 to 260 nm/h Growth temperature: T = 510 °C

22 1.3 µ m Quantum Dots

23 High dot densities for InAs on GaInAs 35 - 40 meV line width 60 meV level distance Longer wavelength at higher In content

24 1.3 µ m Quantum Dot Laser 6 InAs/GaInAs Q-Dot layers with 50 nm GaAs spacers 650 nm cavity width GRINSCH with SSL structure 1,6 µ m Al0.4Ga0.6As cladding layers

25 1.3 µ m Quantum Dot Laser Laser emission by fundamental mode 800 µ m resonator length possible without mirror coating

26 Threshold Current Density For 6 Q-Dot layers threshold doubles but 800 µ m device length possible For 3 Q-Dot layers low threshold current density (100 - 200 A/cm2)but limitation to about 2.5 mm resonator length

27 Modal Gain of Quantum dot Layers L = shortest resonator length at which laser operation is still possible on the ground state About 2 - 3 cm-1 modal gain per dot layer Best results with 6 dot layers achieved

28 Tuning Range of QDot-Lasers Linear correlation of grating period and emission avelength – Tuning range > 35 nm – Basic device properties are almost identical over the whole tuning range → A further extension of the tuning range to longer and shorter wavelengths should be possible

29 高頻特性 Large modulation bandwidth for 800 µ m long HR/HR coated device 3dB bandwidth thermally limited

30 結論 Quantum dot laser 的好處 – 低很多的 inversion carrier density ( 低 threshold current) – 對溫度較不敏感 – 有大的頻寬 – low chirp

31 結論 已實體化的 Quantum dot laser – 980 nm single mode emitting laser with extremely high temperature stability (Top = 15 °C - 210 °C) – 980 nm high power lasers (4 W cw output power, > 50% wall plug eff.) – 1.3 µ m laser with high device performance (Ith = 4.4 mA, Top. > 150°C)

32 Reference http://www.compoundsemiconductor.net/articles/news/6/3/21/1 http://fibers.org/articles/fs/6/12/3/1 http://fibers.org/articles/fs/6/11/3/1 http://www.ee.leeds.ac.uk/nanomsc/presentations/module2presen tation.htm http://www.indianpatents.org.in/ach/quant.htm http://newton.ex.ac.uk/aip/physnews.595.html http://www.aip.org/enews/physnews/2003/ http://www.elec.gla.ac.uk/groups/nanospec/dotlaser.html http://www.shef.ac.uk/uni/academic/N- Q/phys/research/semic/qdresgroup.html#Laser

33 Reference http://optics.org/articles/ole/7/8/2/1 http://feynman.stanford.edu/Html-CQED/sqdl.html http://www.hinduonnet.com/thehindu/2001/09/13/stories/081300 06.htm http://www.phy.ncu.edu.tw/so/Chinese/Quantum%20Dots/Search %20subject1.htm http://www.sciam.com.tw/read/readshow.asp?FDocNo=121&DocN o=191 L.A.Coldren and S.W.Corzine, Diode Lasers and Photonic Integrated Circuits (Wiley, New York 1995). M.Asada, Y.Miyamoto, and Y.Suematsu, IEEE J.Quantum Electron. QE-22, 1915(1986).

34 Reference R. P. Mirin, J. P. Ibbetson, K. Nishi, A. C. Gossard, and J. E. Bowers, Appl. Phys. Lett.67, 3795 (1995). K. Nishi, H. Saito, S. Sugou, and J.-S. Lee, Appl. Phys. Lett. 74, 1111 (1999). V. M. Ustinov, N. A. Maleev, A. E. Zhukov, A. R. Kovsh, A. Yu. Egorov, A. V.Lunev, B. V. Volovik, I. L. Krestnikov, Yu. G. Musikhin, N. A. Bert, P. S. Kop ’ ev, andZh. I. Alferov, N. N. Ledentsov, and D. Bimberg, Appl. Phys. Lett. 74, 2815 (1999). D. L. Huffaker, G. Park, Z. Zou, O. B. Shchekin, and D. G. Deppe, Appl. Phys. Lett.73, 2564 (1998). Y.M. Shernyakov, D.A. Bedarev, E.Y. Kondrateva, P.S. Kopev, A.R. Kovsh, N.A. Maleev, M.V. Maximov, S.S. Mikhrin, A.F. Tsatsulnikov, V.M. Ustinov, B.V. Volovik,A.E. Zhukov, Z.I. Alferov,N.N.Ledentsov, D. Bimberg, Electron. Lett, 35, 898, (1999) G. T. Liu, A. Stintz, H. Li, K. J. Malloy, and L. F. Lester, Electron. Lett. 35, 1163(1999). L. F. Lester, A. Stintz, H. Li, T. C. Newell, E. A. Pease, B. A. Fuchs, and K. J. Malloy,IEEE Photon. Technol. Lett. 11, 931 (1999).


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