Download presentation
Presentation is loading. Please wait.
Published byEvan Gray Modified over 9 years ago
1
Optical Lattices 1 Greiner Lab Winter School 2010 Florian Huber 02/01/2010
2
Outline Solid State Physics How to make optical lattices How to diagnose optical lattices
3
Solid State Physics Phonons Lattice vibrations Thermal properties (isolators) Mediating electron-electron interaction in type 1 (=BCS) superconductors Acoustic and optical phonons Electrons Electrical and thermal properties Semiconductors Magnetism Quantum Simulation
4
Lattice Atoms in solids arranged in regular pattern In general: 3D = 14 Bravais lattices… … but we usually only have to deal with simple cubic (s.c.) lattices x y
5
Free Electrons High School Physics: Metal Reduction of energy by delocalizing outer electrons (more or less) free electron gas
6
Bloch’s Theorem Delocalized electrons “feel” periodic potential, thus their wave function has to inherit periodicity a Free ElectronsElectrons in Per. Pot. Wave function Dispersion
7
Band Gap 1 st Brillouin Zone Restrict to 1 st BZ x Standing wave 2 has higher probability near the ion cores higher energy than 1 band gap
8
From free to tightly bound Lattice Depth Harmonic oscillator energies (Solid state systems: Atomic energy levels)
9
Bloch VS. Wannier Bloch waves: – Delocalized – Plane-wave-like Deeper lattices better described by Wannier functions: – Localized on each lattice site – Closer to QHO Eigenstates – Intuitive picture for J in Bose-Hubbard
10
Bloch Oscillations
11
Optical Dipole Force
12
One Dimension Intensity Here: red detuned
13
More dimensions 1D2D3D “Pancakes” “Tubes” D>1: Typically orthogonal beams are not interfering. different frequency or orthogonal polarizations Otherwise: Relative phase matters! Simple-cubic
14
Harmonic Confinement In D>1 configuration: – Additional (anti-) confinement due to Gaussian profile of orthogonal laser beams. Red detuned: Blue detuned: Potential
15
Realization
16
Recycling Recycle a beam to make lattice along another axis – Beams are interfering! Different lattice pattern
17
Adiabatic loading of superfluid (slower than what? Tunneling?) Sudden release and TOF: Matter wave point sources on each lattice site BEC in Lattice 1/ext. confinement 1/lattice spacing 1/f(Tunneling)
18
Lattice Pulsing Depth measurement Cycle: – BEC (superfluid) – Lattice suddenly pulsed on – Lattice suddenly switched of again – Image diffraction pattern in TOF – Repeat and vary intensity
19
Lattice Pulsing: Grating Picture Position dependent AC Stark shift of lattice imprints a phase pattern into BEC depending of the intensity/duration of the pulse (thin-grating)
20
Lattice Pulsing: Band Picture Projection Time evolution TOF Lattice On Lattice Off
21
Lattice Pulsing: Raman Picture S P
22
Bragg Scattering
23
Lattice Pulsing: Math Bessel Proportional to lattice depth
24
Lattice Pulsing: Pictures
25
Parametric Heating
26
Band Mapping Adiabatic Ramp Down of Lattice Depth preserves the quasi-momentum 1 st BZ
27
Band Mapping Increase lattice depth
28
Band Mapping: Higher Bands Why only every other band?
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.