Nanophotonics class 4. Density of states

Слайд 2

Outline Spontaneous emission: an exited atom/molecule/.. decays to the ground state

Outline

Spontaneous emission: an exited atom/molecule/.. decays to the ground state and

emits a photon

Emission rates are set by Fermi’s Golden Rule
Fermi’s Golden Rule & the number of available photon states (LDOS)
Experiments demonstrating emission rate control via LDOS
Conclusion

Слайд 3

Fermi’s Golden Rule Consider an atom, molecule or quantum dot with

Fermi’s Golden Rule

Consider an atom, molecule or quantum dot with

eigenstates ψ.
Suppose the system is perturbed, e.g. by incident light.
Perturbing term in hamiltonian:

The coupling can take the atom in initial state ψi to another state ψf
Fermi’s Golden Rule: rate of decay of the initial state ψi

light

Dipole operator

Слайд 4

Understanding Fermi’s Golden Rule Energy conservation Matrix elements: Transition strength Selection

Understanding Fermi’s Golden Rule

Energy conservation

Matrix elements:
Transition strength
Selection rules

Spontaneous emission of a

two-level atom:
Initial state: excited atom + 0 photons.
Final state: ground state atom + 1 photon in some photon state
Question: how many states are there for the photon ???
(constraint: photon energy = atomic energy level difference)
Слайд 5

How many photon states are there in a box of vacuum

How many photon states are there in a box of vacuum

?

States in an LxLxL box:

l,m,n positive integers

Number of states with |k|between k and k+dk:

l,m,n > 0
fill one octant

fudge 2 for
polarization

As a function of frequency ω (=ck):

Picture from
http://britneyspears.ac

k

dk

Слайд 6

Density of states in vacuum Example: ~50000 photon states per m3

Density of states in vacuum

Example: ~50000 photon states per m3 of

vacuum per 1 Hz @ λ=500 nm
Слайд 7

Controlling the DOS Photonic band gap material Example: fcc close-packed air

Controlling the DOS

Photonic band gap material

Example:
fcc close-packed
air spheres in

n=3.5
Lattice spacing 400 nm

Photonic band gap: no states = no spontaneous emission
Enhanced DOS: faster spontaneous emission according to Fermi G. Rule

Слайд 8

Local DOS An emitter doesn’t just count modes (as in DOS)

Local DOS

An emitter doesn’t just count modes (as in DOS)
It also

feels local mode strength |E|2.
It can only emit into a mode if the mode is not zero at the emitter

DOS: just count states

Local DOS

A

B

Atom at position A can not emit into
cavity mode.

Atom at position B can emit into
cavity mode.

Слайд 9

LDOS: emission in front of a mirror Drexhage (1966): fluorescence lifetime

LDOS: emission in front of a mirror

Drexhage (1966): fluorescence lifetime

of Europium ions depends
on source position relative to a silver mirror
(λ=612 nm)

Silver mirror

Spacer thickness d

Europium ions

Слайд 10

Example II: dielectric nano-sphere Eu ions in 100 nm – 1

Example II: dielectric nano-sphere

Eu ions in 100 nm – 1 μm

polystyrene spheres [1]
Er ions in 340 nm SiO2 spheres [2]

[1] Schniepp & Sandoghdar, Phys. Rev. Lett 89 (2002)
[2] de Dood, Slooff, Polman, Moroz & van Blaaderen, Phys. Rev. A 64 (2001)

LDOS
normalized to
LDOS in SiO2

Слайд 11

Dielectric nanosphere AFM Confocal AFM to check individual particle diameters Confocal

Dielectric nanosphere

AFM

Confocal

AFM to check individual particle diameters
Confocal microscopy to collect luminescence

n=1.52

n=1.33

n=1

Index

matching of sphere
with fluid droplets:
Emitter stays the same
Lifetime change disappears

[1] Schniepp & Sandoghdar, Phys. Rev. Lett 89 (2002)

Слайд 12

LDOS & measuring nonradiative decay A real emitter often also decays

LDOS & measuring nonradiative decay

A real emitter often also decays nonradiatively

(no photons but heat)

Measured in experiment

Unknown loss
local chemistry
at source

Fermi’s Golden Rule
LDOS

Measurement technique: vary the nanophotonic configuration
vary LDOS and not the chemistry
Example
Emitter in sphere: index match sphere to vary
Assignment: you can find by varying LDOS