Physics of Semiconductor Nanostructures 鄭舜仁 (http://www.cc.nctu.edu.tw/~sjcheng/Frameset05.htm) Department of Electrophysics, National Chiao Tung University 2006 Spring Semester Reference Books & Articles: [1] "The physics of low-dimensional semiconductors: an introduction", by John H. Davies, Cambridge university press (1998). URL: http://userweb.elec.gla.ac.uk/j/jdavies/ldsbook (Chapter 1,3,4,6,9,10) [2] Thesis “Correlations in semiconductor quantum dots” , Marek Korkusinski, June 2004, University of Ottawa (Chapter1,2,3 ) [3] Thesis “Collective Excitations and Coulomb Drag in Two-Dimensional Semiconductor Systems” , Shun-Jen Cheng, September 2001, Universität Würzburg (Chapter2 ) [4] “ A Guide to Feyman Diagrams in the Many-Body Problem, R.F. Mattuck (Dover Books) (1992) [5] “Electronic structure of quantum dots”, S. M. Reimann and M. Manninen, Reviews of Modern Physics, 74, 1283 (2002) [6] “Magnetism in condensed matter”, Stephen Blundell, Oxford University Press (2001) (Chapter 1 &2) [7] “Quantum theory of the optical and electronic properties of semiconductors”, H. Haug and S. W. Koch, World Scientific (Chapter 1) [8] “Excitonic artificial atoms: engineering optical properties of quantum dots”, Pawel Hawrylak, Phys. Rev. B 60, 5597 (1999). Evaluation: 1. Exercises: 50% 2. Oral presentation: 50% Semiconductor nanostructures Gate-defined dot Mesa-etched dot 1m~100nm - - - -- - - - - 1µm~100nm Self-Assembled Quantum Dots +~20nm ~20nm Quantum ring Three-dimensional STM image of an uncovered InAs quantum dot grown on GaAs(001). J. Marquez, et al, Appl. Phys. Lett. 78 (2001) 2309. Semiconductor nanostructures Colloidal nanocrystals ~ few nm Carbon nanotubes: One dimensional system (Courtesy Cees Dekker, Delft Institute of Technology, the Netherlands.) This research was reported in the 7 May 1998 issue of Nature. Here are some real-world nanotube materials, produced by laser ablation of a graphite target containing metal catalyst additives. On top is an atomic force microscopy image of a chiral tube with a diameter of 1.3 nanometers (Technical University, Delft: www.pa.msu.edu/cmp/csc/nanotube.html). Outline Outline: 6. Transport properties[5,6] (2w) 1. Introduction to semiconductor nanostructures [1,2](1w) Coulomb Blockade spectroscopy(1w) 2. Formation of semiconductor nanostructures [1,2](0.5w) Hund’s rule(1w) gate-defined quantum dots (QDs) Quantum Hall droplets in QDs* self-assembled QDs 7. Optical properties[1,7,8](2w) synthesized nanocrystals (NCs) Dipole approximation & Fermi’s golden rules quantum wires, quantum rings… emission and absorption spectrum 3. Single-particle properties [1,2,3](2w) Fine structure of the optical spectrum of QDs band theory in solids 8. Magnetic properties[6](2w) k.p theory Magnetism of QDs envelope function approximation Semi-magnetic QDs quantum disk Spintronics parabolic model spherical quantum dots (QDs) quantum rings* strain effects * asymmetric nanostructures 4. Electric and magnetic fields [1] (1w) nanostructures in magnetic fields nanostructures in magnetic fields :Stark effects Fermi’s golden rule The Aharonov-Bohm effect* Quantum Hall effects in 2D and 0D systems* 5. Many-particle problems [1,4] (3w) Hartree & Hartree-Fock approximation(0.5w) Second quantization(2.5w) [#]: reference#; *: optional; (nw): n weeks Configuration interaction method Technique of exact diagonalization* Many electrons in QDs 總授課時間約14週 Oral presentation: 2週 Home work: 4~6次 Outline Outline: 6. Transport properties[5,6] (2w) 1. Introduction to semiconductor nanostructures [1,2](1w) Coulomb Blockade spectroscopy(1w) 2. Formation of semiconductor nanostructures [1,2](0.5w) Hund’s rule(1w) gate-defined quantum dots (QDs) Quantum Hall droplets in QDs* self-assembled QDs 7. Optical properties[1,7,8](2w) synthesized nanocrystals (NCs) Dipole approximation & Fermi’s golden rules quantum wires, quantum rings… emission and absorption spectrum 3. Single-particle properties [1,2,3](2w) Fine structure of the optical spectrum of QDs band theory in solids 8. Magnetic properties[6](2w) k.p theory Magnetism of QDs envelope function approximation Semi-magnetic QDs quantum disk Spintronics parabolic model spherical quantum dots (QDs) quantum rings* strain effects * asymmetric nanostructures 4. Electric and magnetic fields [1] (1w) Electrostatic potential Stark effects Fermi’s golden rule The Aharonov-Bohm effect* Quantum Hall effects in 2D and 0D systems* 5. Many-particle problems [1,4] (3w) Hartree & Hartree-Fock approximation(0.5w) Second quantization(2.5w) [#]: reference#; *: optional; (nw): n weeks Configuration interaction method Technique of exact diagonalization* Many electrons in QDs 總授課時間約14週 Oral presentation: 2週 Home work: 4~6次 Introduction to semiconductor nanostructures • • • • • • Semiconductor (SC). Fabrication Scale of nanometer. Interesting Physics in SC nanostructures: - transport measurement - optical spectroscopy - magnetic (& spin) properties Observations & Measurements Possible Applications Physics of Semiconductor Nanostructures Why study the physics? What’s interesting physics? How to study the physics? Understand better the physics, then… What’s SC? Why SC? What’s “structure”? What’s “nano-scale”? Why nanostructures? Metal, Insulator, and Semiconductor Conductor (Cu, Ag..) Resistivity (Ohm.cm) 10 6 ~ 102 Semiconductor Insulator (Si, GaAs..) (SiO2,..) 10 2 ~ 109 metal SC ins 1014 ~ 10 22 Band Diagram of Solids Single atom Solid 3s conduction band 2p Valence band 2s N 6N Energy 2N 2N 1s position Metal, Insulator, and Semiconductor Rmetal RSC Rins metal insulator semiconductor Conduction Band (CB) Energy gap (Eg) Valence Band (VB) T>0 doping ++++++ Semiconductor Heterostructures* * 2000 Nobel prize in physics A B Confinement potential Is Nanometer small or large? 1nm 10 9 m 10 A Length scales in semiconductors (SC’s) (see “Electronic transport in mesoscopic systems”, S. Datta, Cambridge Univ. Press) 100m mesoscopic 10m 1m Mean free path: Coherent length: E 100nm lF of bulk: 101 ~ 10 2 nm 10nm Effective Bohr Radius: ~ 101 nm a 1nm 0.1nm E F k F2 Lattice constant: 10 1 ~ 100 nm 1 l2F Low-Dimensional Systems Quantum Well (quasi-2D) Quantum Wire (quasi-1D) Quantum Dot (quasi-0D) <<100nm, in usual. Formation of Quantum Dots Gate-defined dot Pillar dot 1m~100nm 1m~100nm + ----- ----- Self-assembled dots ~10nm etching Aspects of Nanostructures bulk Room temp. kT~25meV Nano-Technology dN/dE (density of states) ~100meV (for GaAs) 10nm Nano-scale Semiconductor nano-technology, Material engineering, etc… E Fundamental Interest Atom physics, Many-body physics, Quantum optics etc….. Advanced Applications Quantum-dot lasers, Photodetectors, Single electron devices, Single photon devices, Quantum computing, etc…. Current transport through a classical resistance I I w + V _ V Conductance (G) Ohm' s law I GV G W L W Quantum Point Contact B.J. van Wees, PRL 60, 848(1988). (see also J.H. Davies Fig.5.22/p186) Quantum Point Contact _ ~250nm Vg Vg G ( 2e 2 / h ) 5 4 3 I V + 2 1 : metal (gate) : two-dimensional electron gas h: Planck’s constant von Klitzing' s resistance h RK 2 25812.807 e W Vg *see also quantum Hall effect (Nobel prizes in ’85,’98) p228 in textbook. Quantum Point Contact (metal) Quantized conductance through individual rows of suspended gold atoms H. OHNISHI, et al., Nature 395, p780 (‘98) lF of metal:100 ~ 101 nm (lF , M lF ,SC ) ~0.9nm Coulomb Blockade in Quantum Dot (Q.D.) Quantum dot J. Weis, et al. Phys. Rev. Lett. 71, 4019-4022 (1993) Vg Vg G I “single” electron transister (SET) S D S D G G (a review article about Q.D.: S.M. Reimann and M. Manninen, Review of Modern Physics, 74,1283 (2000)) Vg Quantum Hall Droplet Spin polarization 2 2 E B B dot Source Drain N-1 T.H.Oosterkamp, PRL, 82, 2931 (1999) Vg B Photoluminescence (PL) from Quantum Wells Photoluminescence (PL) from (parabolic) Quantum Well R.C. Miller, et al. Phys. Rev. B 29, 3740 (’84) Also see sec. 4.3 in textbook 40meV PL from Ensemble of Quantum Dots Artificial atoms!!! ~20nm Sylvain Raymond and cowokers, NRC, Canada Magneto-PL from Ensemble of Quantum Dots B d+ d dp+ p- s Sylvain Raymond et al. PRL(2004) Single-Dot PL Spectrum - Fermi’s golden rule - intitial state: ground state. - final state: GS & “all” excited states The interband polarization operator A( , N ) | f , ( N 1) P i GS , N | ( Ei E f ) 2 P hi , ci , i f experiment M.Bayer et al, Nature 405, 923 (2000) B=0 X6 theory Gs-to-GS Hawrylak, Cheng PL from Single Quantum Dot 20meV ~20nm Robin Williams and cowokers, at NRC, Canada Coulomb Blockade spectrum of a Single Nanocrystal U. Banin, Y. Cao,D. Katz, and O. Millo, Nature vol.400, 542 (1999) InAs NC Calculation Experiment N=1 2 Chemical potential N EGS ( N ) EGS ( N 1) µ4 3 4 5 6 78 Semiconductor Nanocrystals B M SQUID B M 0 B Paramagnetism M 0 B Diamagnetism Paramagnetism of QDs: experimental results M magnetic susceptibility B 0: paramagnetism CdMnSe QD Cd0.996Mn0.004Se 10000 0: damagnetism 1 M 1/ (mol Gauss / emu) B 100 Gauss 1000 Gauss 10000 Gauss 8000 PbSe QD 0.0009 6000 4000 2000 0 0 50 100 150 200 0.0006 SQUID 0.0003 0.0010 0.0000 -0.0003 -0.0006 100 Gauss 1000 Gauss 10000 Gauss 0.0008 (emu / mol Gauss) -1 -1 (emu mol Oe ) Temperature (K) 0 10000 20000 30000 40000 50000 Magnetic Field (Oe) Low-field paramagnetism B Wen-Bing Jian et al, to be published 0.0006 0.0004 0.0002 0.0000 -0.0002 0 40 80 120 160 200 Temperature (K) T Wen-Bing Jian et al Observation of Nanostructures • Scanning Electron Microscope (SEM) Resolution>10nm * 10-40kV Electron beam * See, for instance, “University Physics”, by Harrison Benson, John Wiley & Sons, Inc. Observation of Nanostructures • Transmission Electron Microscope (TEM) Electron beam 50-100kV diffraction Resolution>0.5nm Observation of Nanostructures Scannning Tunneling Microscope (STM)* * Nobel prize in 1986 I=const Resolution: 0.001nm (vertical) 0.1nm (horizontal) Three-dimensional STM image of an uncovered InAs quantum dot grown on GaAs (001). J. Marquez, et al, Appl. Phys. Lett. 78 (2001) 2309. Possible Applications 。Quantum dot infrared photodetectors, QDIPs -- Aslan, B.,Liu, H.C., Korkusinski, M., Cheng, S.-J., and Hawrylak, P., Appl. Phys. Lett. 82, 630 (2003) 。Optical memories --Petroff, P.M., in:Single Quantum Dots: Fundamentals, Application, and New Concepts, Peter Michler (Ed.) (Spring,Berlin,2003); -- Lundstrom, T., Schoenfeld, W. Lee, H., and Petroff, P.M., Science 286,2312(1999) 。Single-Photon sources --Michler, P., Kiraz, A., Becher, C., Schoenfeld, W.V., Petroff, P.M., Zhang, L., Hu, E, and Imamoglu, A., Science 290, 2282 (2000) --Moreau, E., Robert, I., Manin, L., Thierry-Mieg, V., Gerard, J.M., and Abram, I., Phys. Rev Lett. 87,183601 (2001) --Santori, C., Pelton, M., Solomon, G., Dale, Y., and Yamamoto, Y., Phys. Rev. Lett. 86, 1502 (2001) --M.Pelton et al, Phys. Rev. Lett.89, 233602 (2002) •Intra-band photocurrent spectrum I P-polarization T=6 K sample A sample B sample C (a) 0.8 0.6 0.4 0.2 0.0 (a) 0.8 0.6 0.4 0.2 0.0 1.0 S-polarization T=6 K sample A sample B sample C (b) 0.8 0.6 0.4 0.2 0.0 30 40 50 60 Photon energy (meV) 70 80 z Scaled photoresponse 1.0 Normilized photoresponse P-polarization T=6 K sample A sample B sample C 1.0 Normilezed photoresponse Normilized photoresponse 1.0 0.8 S-polarization T=6 K sample A sample B sample C (b) 45o P 0.6 IR S 0.4 0.2 0.0 100 150 200 250 Photon energy (meV) 300 350 Possible Applications 。QD lasers --Arakawa, Y., and Sasaki, H., Apl. Phys. 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