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Optical Vortices and Electric Quadrupole transitions Optical Vortices and Electric Quadrupole transitions

Optical Vortices and Electric Quadrupole transitions - PowerPoint Presentation

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Optical Vortices and Electric Quadrupole transitions - PPT Presentation

James Bounds Organization Dipole and Quadrupole transitions Special Laser beam types Using special laser beams to induce Quadrupole transitions Experimental Realization Possible extensions EM Fields ID: 555632

gaussian quadrupole beam modes quadrupole gaussian modes beam transition orbital angular beams state transitions equation laser momentum selection rules

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Slide1

Optical Vortices and Electric Quadrupole transitions

James BoundsSlide2

Organization

Dipole and Quadrupole transitions

Special Laser beam types

Using special laser beams to induce Quadrupole transitions

Experimental Realization

Possible extensionsSlide3

E-M FieldsSlide4

Gauge FreedomSlide5

Perturbing Term in Length GaugeSlide6

Classical correspondance of perturbing termSlide7

Time-Dependent Perturbation TheorySlide8

Problem is reduced to finding expansion coefficientsSlide9

Separation of emission and absorption termsSlide10

Dipole Matrix ElementSlide11

Probability of being in state bSlide12

Relation to Einstein CoefficientsSlide13

Classical Dipole RadiationSlide14

Higher Order terms

By including higher order terms, the field gradients become more important.Slide15

Selection RulesSlide16

Quadrupole selection Rules

Selection rules are then for hydrogen like systems:Slide17

Fundamental Laser Modes

Hermite

-Gaussian Beam

Mode usually found in lasers

Laguerre-Gaussian

Beam

Contains a sharp amount of orbital angular momentum

Bessel Beam

Diffraction Free

Not possible with finite apertureSlide18

Huygen's principleSlide19

Approximated Fresnel IntegralSlide20

Helmholtz EquationSlide21

Relation to Schrodinger equationSlide22

Substitution into Helmholtz equationSlide23
Slide24

Hermite-Gaussian Modes

Solution of the paraxial wave equation in cartesian coordinatesSlide25

Hermite-Gaussian ModesSlide26

Laguerre-Gaussian Modes

Arise when there is cylindrical symmetry

Usually not favored due to astigmatism

Carry sharply defined amount of orbital angular momentum (OAM)Slide27

Leguerre-Gaussian ModesSlide28

Ince-Gaussian Modes

Solution of paraxial wave equation in elliptic coordinates

Provides smooth connection between HG and LG beams

OAM not as sharply definedSlide29

The non-zero Leguerre-Gaussian modes form optical vorticesSlide30

Orbital Angular momentum

The

Laguerre-Gaussian

Beams are special in that they carry a very sharp amount of orbital angular momentum

The

Poyting

vector

reperesents

a helical spiralSlide31

Orbital Angular Momentum (OAM)

Property of individual photons and not just beam

Can be coupled to external systems

Rotation of Ion crystals

Forbidden transitions

Communication Systems

OAM MultiplexingSlide32

Generation of LG beams

Computer Generated Hologram

Diffracts plane wavefronts into helical wavefronts

Spatial light modulator

Laser etched gratingsSlide33

Holographic PlatesSlide34

Construction of Laser etched gratingsSlide35

Phase-Amplitude modulation from phase only gratingSlide36

Difficulty for pulsed operation

Pulsed operation not favored for holographic plates

Angular chirp

Pulse front tilt

2f-2f setupSlide37

Spatial Light modulator

LCD Crystals respond to computer generated image

Can be used to not only generate, but characterize LG beams

Work done by

James Strohaber

Holographic Knife

edge techniqueSlide38

Holographic Knife Edge

Similar to a mechanical knife edge technique, we can use the SLM to diffract part of the beam awaySlide39

Knife Edge for LG BeamsSlide40

Knife Edge for LG BeamsSlide41

Simultaneous Generation and characterization of LG beamsSlide42

Experimental Realization of quadrupole transitions

Schmiegelow, “Excitation of an Atomic Transition with a Vortex Laser Beam”Slide43

State is easily probed

3

2

D State is metastable

Transition wavelengths accessible

Calcium Quadrupole TransitionSlide44

3

2

D state depopulated

854nm transition

3

2

D state is metastable

Population vs. 729 nm LG pulse length gives Rabi frequency

State PreparationSlide45

Population Detection

4

2

S poulation determined by 866nm fluorescenceSlide46

Zeeman Splitting of Ca+ Quadrupole Transition at 729nm

Quadrupole TransitionSlide47

Relative strengths of transitionsSlide48

Large Gradient and zero field = electric quadrupole transitionSlide49

Conclusions

We have demonstrated the origin of the quadrupole transition

Selection rules

Investigated fundamental beam modes

Generation and characterization

Orbital Angular momentum

Experimental realization of coupling of OAM to

atoms