Optical Properties of Solids: Lecture 10 Stefan Zollner Properties Lecture 10 Zollner.pdfStefan...
Transcript of Optical Properties of Solids: Lecture 10 Stefan Zollner Properties Lecture 10 Zollner.pdfStefan...
Optical Properties of Solids: Lecture 10
Stefan ZollnerNew Mexico State University, Las Cruces, NM, USA
and Institute of Physics, CAS, Prague, CZR (Room 335)[email protected] or [email protected]
NSF: DMR-1505172http://ellipsometry.nmsu.edu
These lectures were supported by β’ European Union, European Structural and Investment Funds (ESIF) β’ Czech Ministry of Education, Youth, and Sports (MEYS), Project IOP
Researchers Mobility β CZ.02.2.69/0.0/0.0/0008215
Thanks to Dr. Dejneka and his department at FZU.
Optical Properties of Solids: Lecture 10
Excitons (Wannier-Mott, Frenkel)Ionization of excitonsExcitons in low dimensions
New Mexico State University
References: Band Structure and Optical Properties
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 3
Solid-State Theory and Semiconductor Band Structures:β’ Mark Fox, Optical Properties of Solids (Chapter 4)β’ Ashcroft and Mermin, Solid-State Physics β’ Yu and Cardona, Fundamentals of Semiconductorsβ’ Dresselhaus/Dresselhaus/Cronin/Gomes, Solid State Propertiesβ’ Cohen and Chelikowsky, Electronic Structure and Optical Propertiesβ’ Klingshirn, Semiconductor Opticsβ’ Grundmann, Physics of Semiconductorsβ’ Ioffe Institute web site: NSM Archive
http://www.ioffe.ru/SVA/NSM/Semicond/index.html
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 4
Outline
Wannier-Mott and Frenkel ExcitonsBohr model for excitons (Elliott/Tanguy theory)Examples: GaAs, ZnO, LiF, solid rare gasesIonization of excitons (thermal, high field, high density)Excitons in low-dimensional semiconductors
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 5
Uncorrelated single-electron energy
GaAs
Ξk=0Direct transition:Initial and final electron state have same wave vector.
β’ A photon is absorbed.β’ A negatively charged electron is
removed from the VB, leaving a positively charged hole.
β’ The negatively charged electronis placed in the CB.
β’ Energy conservation:Δ§Ο=Ef-Ei
This IGNORES the Coulomb force between the electron and hole.
Use BOHR model.
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 6
Exciton concept
Valence Band
Conduction BandEnergy
Ef
Ei
Eg
hΟ
e
Exciton: bound electron β hole pairExcitons in semiconductors
Conduction band
Valence band
e
Semiconductor Picture
Ground State Exciton
Large radius
Radius is larger than atomic spacing
Weakly bound
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 7
Bohr model for free excitons
πΈπΈ ππ = βππππ0
1ππππ2π π π»π»ππ2
1. Reduced electron/hole mass (optical mass)
2. Screening with static dielectric constant Ξ΅r.
3. Exciton radius:
aH=0.53 Γ 4. Excitons stable if EX>>kT.5. Exciton momentum is zero.
1ππ
=1ππππ
+1ππβ
Electron and hole form a bound state with binding energy.
RH=13.6 eV Rydberg energy.QM mechanical treatment easy.
ππππ =ππ0
ππππππππ2πππ»π»
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 8
Wannier-Mott and Frenkel excitonsHow does the (excitonic) Bohr radius compare with the lattice constant?
Fox, Chapter 4Yu & Cardona
Wannier-Mott exciton(semiconductors)
~1-10 meV
Frenkel exciton(insulators)
100-1000 meV
localized
Free exciton examples
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 9
β’ Effective mass increases like the band gap.β’ Narrow-gap semiconductors have weak excitons.β’ Insulators (GaN, ZnO, SiC) have strongly bound
excitons.
β’ Discrete series of exciton states β’ (unbound) exciton continuum
Sommerfeld enhancement.
Fox, Chapter 4Yu & Cardona
Free exciton examples
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 10
Fox, Chapter 4Jellison, PRB 58, 3586 (1998).
Several discrete states can be seen in pure GaAs at very low T.
ZnO has a very strong exciton.II/VI material, very polar.Uniaxial (solid-dashed lines).Strong exciton-phonon coupling.Exciton-phonon complex.
Giant Rydberg excitons in Cu2O
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 11
Kazimierczuk, Nature 514, 343 (2014)
n=25
Band-band optical dipole transition forbidden by parity
n=1 forbiddenπΈπΈ ππ = β
π π ππππ2
Excitonic effects are weak if band gap is small
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 12
0.10 0.15 0.20 0.25 0.30 0.35 0.400.0
0.2
0.4
0.6
0.8
1.0
1.2
1.4
1.6
1.8
Ξ΅ 2
Energy (eV)
77 K 100 K 125 K 150 K 175 K 200 K 225 K 250 K 275 K 300 K 325 K 350 K
InSb0.6 0.7 0.8 0.9 1.0 1.1 1.2
0.0
0.2
0.4
0.6
0.8
1.0
1.2
Ξ΅ 2
Photon energy (eV)
718 K
10 K
Ge
InSb:Eg=0.2 eVEX=0.4 meVaX=100 nm
Ge:Eg=0.9 eVEX=1.7 meVaX=24 nm
Emminger, Zamarripa, ICSE 2019
Sommerfeld enhancement
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 13
Excitonic Rydberg energyDiscrete states
Discrete absorption
Continuum absorption
π π ππ =ππ
ππ0ππππ2π π π»π»
πΈπΈππ = πΈπΈππ β1ππ2π π ππ
R. J. Elliott, Phys. Rev. 108, 1384 (1957)Yu & Cardona
ππ2 πΈπΈ =8ππ ππ 2ππ3
ππ2 4ππππ0 3ππππ3οΏ½ππ=1
β1ππ3πΏπΏ πΈπΈ β πΈπΈππ
ππ2 πΈπΈ =2 ππ 2 2ππ β3 2 πΈπΈ β πΈπΈ0
ππ2ππππππ
sinh ππππ = ππ οΏ½π π ππ
πΈπΈ β πΈπΈ0Use Bohr wave functions to calculate Ξ΅2.Toyozawa discusses broadening.
Tanguy: Kramers-Kronig transform of Elliott formula
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 14
R. J. Elliott, Phys. Rev. 108, 1384 (1957)C. Tanguy, Phys. Rev. Lett. 75, 4090 (1995)
Electron-holeabsorption
Sommerfeld enhancement
(excitonic effects)
Digamma function
Amplitude pre-factor
ππ ππ = 2ln(ππ) β 2ππcot(ππππ) β 2ππ(ππ) β1ππ
π΄π΄ =β2ππ2
2ππππ0ππ02
2ππβ2
β3 2
ππ 2
exciton bound states and continuum:
ππ π§π§ = οΏ½π π πππΈπΈ0 β π§π§
ππ πΈπΈ =π΄π΄ π π πππΈπΈ + ππΞ 2 ππ ππ πΈπΈ + ππΞ + ππ ππ βπΈπΈ β ππΞ β 2ππ ππ 0
ππ π§π§ =ππlnΞ π§π§πππ§π§
Tanguy: Kramers-Kronig transform of Elliott formula
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 15
R. J. Elliott, Phys. Rev. 108, 1384 (1957)C. Tanguy, Phys. Rev. Lett. 75, 4090 (1995)
Exciton bound states have disappeared due to broadening.
Significant Sommerfeld enhancement of the excitonic continuum.
Ξ΅1 peaks below Eg due to excitonic effects.
Eg=1.42 eV, RX=4 meV, Ξ=6 meV
Tanguy model applied to Ge
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 16
Ξ΅ 1Ξ΅ 2
β’ Fixed parameters:
β Electron and hole masses
β Excitonic binding energy Ri
β’ Adjustable parameters:
β Linear background A1 and B1(contribution from E1)
β Broadening Ξ: 2.3 meV
β Band gap E0
β Amplitude A (similar to P)
Carola Emminger, ICSE 2019
Thermal ionization of excitons
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 17
0.6 0.7 0.8 0.9 1.0 1.1 1.20.0
0.2
0.4
0.6
0.8
1.0
1.2
Ξ΅ 2
Photon energy (eV)
E0
E0+Ξ0
10 K
718 K
Strong excitonic peak at 10 K, disappears at high T.
Ge
Carola Emminger, ICSE 2019
EX(hh)=1.7 meV
kB=0.086 meV/K
TC=20 K
Excitons in electric fields
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 18
Excitons are unstable at high temperature, if kT>>EX.They are also unstable in a high electric field.
Fox, Chapter 4
Energy of dipole in electric field
Critical field
GaAs:RX=1.5 meVaX=13 nmEc=60 kV/m
ππ = οΏ½βοΏ½π οΏ½ πΈπΈ = 2πππ₯π₯πππΈπΈ = π π ππ
πΈπΈππ =π π ππ
2ππππππ
Field ionization
Condensation of excitons at high density
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 19Fox, Chapter 4
Exciton gas
Electron-hole liquid
Mott transition (insulator-metal) when electron separation equals exciton radius.
Electron separation d for density N
Mott transition occurs at rs near 1.GaAs: n=1017 cmβ3.
Biexciton, triexciton molecule formation.Electron-hole droplets.Bose-Einstein condensation.
πππ π =ππππππ
ππ =3 3
4ππππdimensionless
Excitons in doped or excited semiconductors
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 20
C. Tanguy, Phys. Rev. 60, 10660 (1999)Banyai & Koch, Z. Phys. B 63, 283 (1986).
Need to include exciton screening due to doping.Yukawa potential: SchrΓΆdinger equation not solvable.Use Hulthen potential as an approximation
Coulomb
Yukawa
Hulthen
ππ ππ = βππ1ππ
ππ ππ = βππexp β βππ ππD
ππ
Hulthen exciton
ππ ππ = βππβ2 ππππππ
exp 2ππππππππ
β 1
ππ =ππ2
4ππππ0ππππ
πππ·π· =ππππππ0πππ΅π΅ππππππ2
ππ =πππ·π·ππππ
Unscreened: g=βFully screened: g=0Mott criterion: g=1
Tanguy: Dielectric function of screened excitons
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 21
C. Tanguy, Phys. Rev. B 60, 10660 (1999)
ππ2 ππ =2πππ΄π΄ π π ππ
πΈπΈ2οΏ½ππ=1
ππ2<ππ
2π π ππ1ππ
1ππ2
βππ2
ππ2πΏπΏ πΈπΈ β πΈπΈππ +
π π ππ2
1 βππ2
ππ
2
π΄π΄ =β2ππ2
2ππππ0ππ02
2ππβ2
β3 2
ππ 2Bound exciton states:
exciton continuum:
ππ2 ππ =2πππ΄π΄ π π ππ
πΈπΈ2sinhππππππ
cosh ππππππ β cosh ππππ ππ2 β 4ππ
ππ πΈπΈ β πΈπΈππ
ππ = ππ οΏ½πΈπΈ β πΈπΈ0π π ππ
Need to introduce Lorentzian broadening and perform KK transform.
Tanguy: Dielectric function of screened excitons
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 22
C. Tanguy, Phys. Rev. B 60, 10660 (1999)
ππ πΈπΈ =π΄π΄ π π πππΈπΈ + ππΞ 2 ππ ππ πΈπΈ + ππΞ + ππ ππ βπΈπΈ β ππΞ β 2ππ ππ 0
ππ ππ = β2ππππππ
βΞΎππβ 2ππ 1 β ππ β
1ππ
ππ π§π§ =2
πΈπΈππ β π§π§π π ππ
+πΈπΈππ β π§π§π π ππ
+ 4ππ
g=β
g=0g=0
g=βg=1.5
g=0
g=β
Tanguy: Dielectric function of screened excitons
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 23C. Tanguy, Phys. Rev. B 60, 10660 (1999)
Small broadening Large broadening
Excitons in laser-excited GaAs
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 24
Haug and Koch, Quantum Theory of Optical and Electronic Properties of SemiconductorsY. H. Lee, Phys. Rev. Lett 57, 2446 (1986)
Hulthen exciton
GaAs300 K
High laser excitation
g=β
g small
Excitons in doped or excited semiconductors
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 25
High laser excitation High doping
Non-linear effect.Fox, Chapter 4 Fujiwara, Phys. Rev. B 71, 075109 (2005)
Frenkel excitons in alkali halides
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 26
Also in rare gas crystals (Ne, Ar, Kr, Xe: 1β4 eV)
Fox, Chapter 4
New Mexico State UniversityStefan Zollner, February 2019, Optical Properties of Solids Lecture 9 27
0 1 2 3 4 5 6-20
-10
0
10
20
3035
Photon energy (eV)
<Ξ΅1>
E0
E0+β0
E1 E1+β1
E0'
E210K
-5
0
5
10
15
20
25
30
<Ξ΅2οΏ½>
Critical Points in Germanium
C. Emminger, ICSE-2019
β’ Structures in the dielectric function due to interband transitions
β’ Joint density of states
β’ Van Hove singularities
π·π·ππ πΈπΈπΆπΆπΆπΆ =1
4ππ3οΏ½
πππππππ»π»ππ πΈπΈπΆπΆπΆπΆ
E1β
New Mexico State UniversityStefan Zollner, February 2019, Optical Properties of Solids Lecture 9 28
Critical Points
Yu&CardonaDresselhaus, Chapter 17
E0
E1
πΈπΈππππ ππ = πΈπΈππππ ππ0 +
οΏ½ππ=1
3
ππππ ππππ β ππ0ππ 2
Some ai small or zero: 1D, 2D, 3D
Some ai positive, some negative
M-subscript: Number of negative mass parameters
Two-dimensional Bohr problem
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 29
Assume that Β΅|| is infinite (separate term).Use cylindrical coordinates.Separate radial and polar variables.Similar Laguerre solution as 3D Bohr problem.
M. Shinada and S. Sugano, J. Phys. Soc. Jpn. 21, 1936 (1966).
π»π» = ββ2
2ππβ₯ππ2
πππ₯π₯2+
ππ2
πππ¦π¦2ββ2
2ππβ₯ππ2
πππ§π§2βππ2
ππππππ
ππππ =4ππππ0ππππβ2ππ0
ππππ2π π ππ =
ππππ4
2β2ππ0 4ππππ0ππππ 2
πΈπΈππ = βπ π ππ
ππ β 122 , ππ = 1,2, β¦ Half-integral quantum numbers
Two-dimensional saddle-point excitons
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 30
B. Velicky and J. Sak, phys. status solidi 16, 147 (1966)C. Tanguy, Solid State Commun. 98, 65 (1996)W. Hanke and L.J. Sham, Phys. Rev. B 21, 4656 (1980)
ππ ππ = 2ln(ππ) β 2ππ(12β ππ)
π΄π΄ =ππππ2
ππππ0ππ02 ππ 2
ππ π§π§ = οΏ½π π πππΈπΈ0 β π§π§
ππ πΈπΈ =π΄π΄
πΈπΈ + ππΞ 2 ππ ππ πΈπΈ + ππΞ + ππ ππ βπΈπΈ β ππΞ β 2ππ ππ 0
ππ π§π§ =ππlnΞ π§π§πππ§π§
Excitons in Quantum Structures
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 31
R. Zimmermann, Jpn. J. Appl. Phys. 34, 228 (1995)
Electron-hole overlap is enhanced in quantum structures.Excitonic effects (shift and enhancement) are stronger.
πΈπΈππ = βπ π ππ
ππ β ππ 2q=0.5 2Dq=0 3D
Lz=0.4aX d=0.4aX
Summary
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 32
β’ Exciton: electron-hole pair bound by the Coulomb force.β’ Excitonic effects enhance band gap absorption.β’ Excitons can be ionized by electric fields, high
temperature, or high carrier density.β’ Excitonic effects stronger in low-dimensional materials.
Whatβs next ???
Stefan Zollner, February 2019, Optical Properties of Solids Lecture 10 33
11: Applications IWhat would you like to see ?Please send email to [email protected]
Quantum structures (2D, 1D, 0D)Defects
12: Applications IIProperties of thin films, stress/strain, deformation potentials