Loading in 5 sec....

An introduction to Quantum OpticsPowerPoint Presentation

An introduction to Quantum Optics

- 137 Views
- Uploaded on
- Presentation posted in: General

An introduction to Quantum Optics

Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author.While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server.

- - - - - - - - - - - - - - - - - - - - - - - - - - E N D - - - - - - - - - - - - - - - - - - - - - - - - - -

An introduction to Quantum Optics

T. Coudreau

Laboratoire Kastler Brossel, UMR CNRS 8552 et Université Pierre et Marie Curie, PARIS, France

also withPôle Matériaux et Phénomènes Quantiques, Fédération de Recherche CNRS 2437 et Université Denis Diderot , PARIS, France

- Quantum optics are concerned with the statistics of the electromagnetic field (variance, correlation functions …)
- The statistics give an idea on the nature of the source : thermal, poissonian...
- The statistics may give an idea on the basic properties of astrophysical sources
- www.astro.lu.se/~dainis

- Historical approach
- Electromagnetism
- Planck and Einstein
- Quantum Mechanics
- Quantum Electrodynamics
- Conclusive experiments

- Statistical properties of light
- Quantum optics with OPOs

Does light consist in waves or particles ?

- 17th century : Newton particle
- 19th century : Fresnel, Maxwell... wave
- 1900s : Planck, Einsteinparticle
- 1920s : Quantum mechanics
- 1950s : Quantum Electrodynamics
- 1960s : Quantum Optics

- Young (~1800) : interferences, a light wave can be added or substracted
- Sinusoïdal wave

- Scalar wave

- Transverse vectorial wave

- wave withwith
Everything is understood but...

- The spectral behaviour of black body radiation is not understood :
- why the decrease at high frequency ?

- Photoelectric effect (Hertz and Hallwachs, 1887)
- UV light removes charges on the surface while a visible light does not
Planck : energy exchange occur with multiples of

Bohr : atomic energy levels

- UV light removes charges on the surface while a visible light does not

- Light is made of unbreakable “quanta” of energy (Einstein 1905)
This was later checked by Millikan

- The Compton effect (1923)
The particle (“photon”) possesses a given momentum

- Photomultiplier :
light can be seen as a photon current

pulses

Taylor (1909) : Young's slits with an attenuated source

("a candle burning at a distance slightly exceeding a mile”)

Photographic plate

Exposure time

"each photon then interferes only with itself”, Dirac

- Complete quantum theory of matter : energy levels, atomic collisions
- Atom-field interaction :
Classical electromagnetic waveQuantum atom

« Semi classical theory :

- Energy transfers only by units of
- Momentum transfers by units of

- Photoelectric, Compton effects can be understood with a classical wave
- Pulses recorded in the photomultiplier are due to quantum jumps inside the material and not to the granular structure of light
same for the photographic plate in Taylor ’s experiment

Light remains a classical electromagnetic wave

- Should Einstein be deprived of his (only) Nobel prize ?
- And Compton ?

- Quantum calculations are applied to light in the absence of matter
- In the case of a monochromatic light, the energy is quantified :
- contains n photons (quanta) : En
- contains 0 photons (quanta) : E0
(Vacuum, absence of radiation, fundamental state of the system)

- Existence of an Heisenberg inequality analogous to
(for a monochromatic wave)

Consequences

- There is no null field at all moments (see “there is no particle at rest”)
- The electromagnetic field in vacuum is not identically null
The field is null only on average : existence of vacuum fluctuations

- Excited levels of atoms are unstable

- Through a quadratic Stark effect, the vacuum fluctuations displace the excited levels ("Lamb shift").

- Reasons
1) Problem of interpretation

2) Problem of formalism : many diverging quantities

e.g. Vacuum energy :

3) Problem of "concurrence" : the more simple semiclassical theory gives (generally) the same results

- 2) was solved in 1947 (Feynman, Schwinger & Tomonaga) :
QED serves as a base and model for all modern theoretical physics (elementary particles…)

- Large success of quantum electrodynamics to predict properties of matter “in the presence of vacuum”.
- Agreement between theory and experiment 10-9

- Progress in optical techniques
- lasers
- better detectors
- non linear optics

Wave

Continuous

Unlocalised, breakable

Photons

Discontinuous

Localised, unbreakable

A crucial experiment : the semitransparent plate

50% reflected

(1)

(2)

50%

transmitted

The plate does not cut the photon in two !

(1)

But a very faint source does not produce a true one photon state :

the beam is a superposition of different states, e.g.

A faint source does not give a clear result

(2)

A single dipole (atom, ion…) emits a single photon at a time

Kimble, Dagenais and Mandel, Phys. Rev. Lett. 39 691 (1977)

First experimental proof of the particle nature of light

To MZ2

To MZ1

Ca beam

Grangier et al., Europhys. Lett 1 173(1986)

- With a pump at frequency 0, the crystal generates twin photons at frequencies 1 and 2.
There is a perfect correlation between the two channels

- Furthermore, the system behaves as an efficient source of single photon states :
the resulting light cannot be described by two classical waves emitted by a crystal described quantically

Hong, Ou and Mandel,

Phys. Rev. Lett. 59 2044 (1987)

No interference fringes : the crystal does not produce classical beams but

Value predicted by

classical theory

Perfect anticorrelations at zero phase shift

(2) and (4) give which is not verified experimentally

the crystal does not produce classical particles

(1) (2) (3) (4)

- Light can behave like a classical wave
- Classical interferences

- One photon interferences

- Two photon interferences

Time

B

A

Space

magnet B

source

magnet A

- 1935 (A. Einstein, B. Podolsky, and N. Rosen, Phys. Rev. 47, 777 (1935) ) : Einstein, Podolski and Rosen worry about the non-local character of quantum mechanics.

A and B measure the spin of particles 1 and 2 along a given axis.

If the two observers choose the same axis, they get an opposite result but if they choose different axis, can they measure simultaneously orthogonal directions ?

is there a “supertheory” (hidden variables) ?

1965 (J. S. Bell, Physics 1, 195 (1965). ) : J.S Bell proposes a way to discriminate between a local hidden variables theory and quantum theory.

One assumes that the experimental result depends on a “hidden variable” and on the magnets orientations but not on the other measurement :

The classical probability to obtain a given result is given by

While the quantum theory prediction is written

a

a

source

c

b

c

b

B

A

Classical, hidden variable theory predicts

P(SaSb)+P(Sb Sc)+P(ScSa) = 1 + 2(P1+P8) 1

while Quantum Mechanics predicts :

P(SiSj) = cos2(60°) = 1/4 so that

P(SaSb)+P(Sb Sc)+P(ScSa) = 3/4 < 1!

“Bell inequalities” enable us to discriminate

Among the first experiments :

A. Aspect, P. Grangier, and G. Roger, Phys. Rev. Lett. 49, 91 (1982).

Weihs et al. performed an experiment using parametric down conversion and detectors 400 m apart

Weihs et al., Phys. Rev. Lett 81, 5039(1998)

A

B

Experimental result :

Non local correlations exist !

They do not allow superluminous transfer of information

- All measurement results (up to now) are in agreement with the predictions of quantum electrodynamics
- (including experiments of measurement and control of quantum fluctuations)
- No more mysteries
- the actual theory explains without ambiguity all phenomena
- but still "strange" behaviours
- Physical images
- several may workwave and particle
- only one workswave or particle
- none worksneither wave nor particle
- Vacuum fluctuations
- Path interferences

- Different sources, single atoms, nonlinear crystals, … are able to generate different types of fields.
- What should we study ?
- The statistical properties of the field
- The properties of statistical variables are described by
- Photon number probability distributions
- 2nd order moment : 2nd order coherence
- (1st order = interference)

- Spontaneous emission by a single dipole (atom, ion, …)
- variance and photon number distribution : depend on pumping
- antibunching

- Spontaneous emission by an incoherent ensemble of dipoles
- (Thermal / chaotic light)
- bunching
- (Hanbury Brown & Twiss)

- Laser field (stimulated emission inside an optical cavity)
- Poissonian distribution

- N photon state

At the output of an OPO, the signal and idler beams have quantum

intensity correlations.

Heidmann et al., Phys. Rev. Lett. 59, 2555 (1987)

Result : 30 % noise reduction

(now : over 85 %)

- No more mysteries
QED explains without ambiguity all phenomena

but still "strange" behaviours

- The results depend on the quantum state of the field
- Vacuum
- n photons
- statistical mixture

- Statistical properties of light give an insight on the properties of the emitting object
- OPOs provide an efficient source of non classical light