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Page 1: From: Solid State Theory, Harrisonlamp.tu-graz.ac.at/~hadley/ss2/lectures16/jun13.pdf · Transverse optical plasma waves The dispersion relation for light 2 22 00 2 k c For a free

From: Solid State Theory, Harrison

Page 2: From: Solid State Theory, Harrisonlamp.tu-graz.ac.at/~hadley/ss2/lectures16/jun13.pdf · Transverse optical plasma waves The dispersion relation for light 2 22 00 2 k c For a free

2

2

d ynm neEdt

0

neyE

2 2 2

20

d y n e ynmdt

22

2 0pd y ydt

2

0p

nem

Plasma frequencyKittel

Plasma waves can be quantized like any other wave

Longitudinal plasma waves

There is no magnetic component of the wave.

Page 3: From: Solid State Theory, Harrisonlamp.tu-graz.ac.at/~hadley/ss2/lectures16/jun13.pdf · Transverse optical plasma waves The dispersion relation for light 2 22 00 2 k c For a free

Electron energy loss spectroscopy

pE n

EELS is often used to measure phonons

Page 4: From: Solid State Theory, Harrisonlamp.tu-graz.ac.at/~hadley/ss2/lectures16/jun13.pdf · Transverse optical plasma waves The dispersion relation for light 2 22 00 2 k c For a free

Aluminum

Plasmons 15.3 eV

Surface plasmons 10.3 eV

Magnesium

Plasmons 10.6 eV

Surface plasmons 7.1 eV

Electron energy loss spectroscopy

Page 5: From: Solid State Theory, Harrisonlamp.tu-graz.ac.at/~hadley/ss2/lectures16/jun13.pdf · Transverse optical plasma waves The dispersion relation for light 2 22 00 2 k c For a free

Transverse optical plasma waves

The dispersion relation for light 2

2 20 0 2 k

c

For a free electron gas2

21 p

22 2 2

21 p c k

2 2 2 2p c k

Kittel

Plasmons

Page 6: From: Solid State Theory, Harrisonlamp.tu-graz.ac.at/~hadley/ss2/lectures16/jun13.pdf · Transverse optical plasma waves The dispersion relation for light 2 22 00 2 k c For a free

Surface Plasmons

Waves in the electron density at the boundary of two materials.

Surface plasmons have a lower frequency that bulk plasmons. This confines them to the interface.

Page 7: From: Solid State Theory, Harrisonlamp.tu-graz.ac.at/~hadley/ss2/lectures16/jun13.pdf · Transverse optical plasma waves The dispersion relation for light 2 22 00 2 k c For a free

Surface Plasmons

High-resolution surface plasmon imaging of gold nanoparticles by energy-filtered transmission electron microscopy

PHYSICAL REVIEW B 79, 041401 R 2009

Surface plasmons on nanoparticles are efficient at scattering light.

Green and blue require different sized particles.

Page 8: From: Solid State Theory, Harrisonlamp.tu-graz.ac.at/~hadley/ss2/lectures16/jun13.pdf · Transverse optical plasma waves The dispersion relation for light 2 22 00 2 k c For a free

Surface plasmons are used for biosensors.

Nature Photonics

Page 9: From: Solid State Theory, Harrisonlamp.tu-graz.ac.at/~hadley/ss2/lectures16/jun13.pdf · Transverse optical plasma waves The dispersion relation for light 2 22 00 2 k c For a free

Polaritons

Transverse optical phonons will couple to photons with the same and k.

photon dispersionavoided crossing

Light Bragg reflects off the sound wave; sound Bragg reflects off the light wave.

Page 10: From: Solid State Theory, Harrisonlamp.tu-graz.ac.at/~hadley/ss2/lectures16/jun13.pdf · Transverse optical plasma waves The dispersion relation for light 2 22 00 2 k c For a free

Polaritons

22Tm PmP eE

Ne Ne

22 2

TNe EP P

m

2 20 0k E E P

2 2 20 0 0

2 2 2 0/ T

kNe m

Newton: 2

2

d xm eE Cxdt

TCm

P Nex polarization:

Optical phonons are modelled by a 1-D mass-spring system.

Component of E-field parallel to mass-spring motion.

Page 11: From: Solid State Theory, Harrisonlamp.tu-graz.ac.at/~hadley/ss2/lectures16/jun13.pdf · Transverse optical plasma waves The dispersion relation for light 2 22 00 2 k c For a free

Polaritons

2 2 20 0 0

2 2 2 0/ T

kNe m

There are two solutions for every k, one for the upper branch and one for the lower branch.

A gap exists in frequency.

22 2

TNe EP P

m

2 20 0k E E P

Polaritons are the normal modes near the avoided crossing.

Page 12: From: Solid State Theory, Harrisonlamp.tu-graz.ac.at/~hadley/ss2/lectures16/jun13.pdf · Transverse optical plasma waves The dispersion relation for light 2 22 00 2 k c For a free

Polaritons allow us to study the properties of phonons using optical measurements

Kittel= 4.7E13 = 3.1E13

By looking at the reflectance in different crystal directions, you can determine the frequencies of the transverse optical phonons.

Page 13: From: Solid State Theory, Harrisonlamp.tu-graz.ac.at/~hadley/ss2/lectures16/jun13.pdf · Transverse optical plasma waves The dispersion relation for light 2 22 00 2 k c For a free

Polaritons and optical properties

Page 14: From: Solid State Theory, Harrisonlamp.tu-graz.ac.at/~hadley/ss2/lectures16/jun13.pdf · Transverse optical plasma waves The dispersion relation for light 2 22 00 2 k c For a free

Polarons

Electronic charge is partially screened by lattice ions. This is a charge -phonon coupling.

A polaron is a quasiparticle consisting of an electron and an ionic polarization field. The electron density is low so the screening by electrons can be neglected.

Page 15: From: Solid State Theory, Harrisonlamp.tu-graz.ac.at/~hadley/ss2/lectures16/jun13.pdf · Transverse optical plasma waves The dispersion relation for light 2 22 00 2 k c For a free

Large polaron (Fröhlich polaron)

Electrons move in bands with a large effective mass (432 me for NaCl)

The spatial extent of the polaron is much larger than the lattice constant.

Large polarons typically form bands.

Page 16: From: Solid State Theory, Harrisonlamp.tu-graz.ac.at/~hadley/ss2/lectures16/jun13.pdf · Transverse optical plasma waves The dispersion relation for light 2 22 00 2 k c For a free

Small polaron (Holstein polaron)

Small polaron - Holstein Hamiltonian - electrons are localized and hop (thermally activated or tunneling). Small polarons often form in organic material. In soft materials the energy for making a distortion is smaller.

For a small polaron, the polarization is about the size of the lattice contant.

Page 17: From: Solid State Theory, Harrisonlamp.tu-graz.ac.at/~hadley/ss2/lectures16/jun13.pdf · Transverse optical plasma waves The dispersion relation for light 2 22 00 2 k c For a free
Page 18: From: Solid State Theory, Harrisonlamp.tu-graz.ac.at/~hadley/ss2/lectures16/jun13.pdf · Transverse optical plasma waves The dispersion relation for light 2 22 00 2 k c For a free