Notes
Outline
Micromechanical Systems
in the Quantum Regime
Angus MacKinnon
Cavendish Lab, Cambridge
Blackett Lab., Imperial College, London
Acknowledgements
Miles P Blencowe
Dartmouth College, USA
Andrew D Armour
University of Nottingham
Web Sites
Caltech – Roukes
http://www.its.caltech.edu/~nano/
Cornell – Craighead
http://www.hgc.cornell.edu/index.html
UCSB – Cleland
http://www.qi.ucsb.edu/cleland/
Munich – Blick
http://www.nano.physik.uni-muenchen.de/Blick/Blick.html
Buzz Words
Nanomechanics
Yoctocalorimetry
Spin Physics
Quantum Computing
Nanotubes
Peapods
Computational Molecular Biology
Single Phonons
Squeezed Phonons
Quantum Shuttle
Which-Path devices
MEMS
NEMS
Entanglement
Universal limits
Slide 5
2 Groups of Devices
Mechanical Systems
Free standing quantum wires
Heat & phonon flow
Machines
Electromechanical Devices
Which-way devices
Quantum shuttle
Entanglement
Free Standing Wires
Musical Instruments
Thermal Landauer Formula
Universal Limits
Yoctocalorimetry
Measuring single phonons
Typical phonon energy – 10-24J = 1 Yoctojoule
2 Measurements
Thermal Conductivity
Thermal Decay
Slide 12
Quantum Gears
Gears locked together.
Incompatible angular momentum quantisation.
Is this compatible with macroscopic behaviour?
Planetary Gear
Hamiltonian
2 Gears:
Simplified – 1 Driven Gear
Single Gear
Simple Hamiltonian
Rotating Frame
Nearly Free Gear
Try
Only coupled for
Compare with
No. of states in BZ = No. of teeth
Angular Group Velocity
Nearly Free Electrons/Gears
Unexpected Result
Finite V – Finite Angular Group Velocity
Except at
 But this condition is almost certainly not fulfilled.
Why should               be an integer?
2 Gears
Let
Selection Rules
But
1st Brillouin Zone:
Tunnelling except:
Identical Gears
Different Gears
Summary - Gears
Quantisation of angular momentum not generally consistent with
Driving frequency
Other gears
>2 Gears
No solutions except for special cases.
Finite Temperature
Need
Quantum Shuttle
3 Dot Model
Crossings and Anti-crossings
Steady State Current
Landauer Model
Elastic Transmission
Inelastic Transmission
Electron-Phonon Energy Transfer
Current – Voltage Characteristic
Summary - Shuttle
Shuttle is self-driving
If potential difference big enough
Sensitive to dissipation mechanism
I-V Characteristic quickly washed out at finite T.
How to calculate transit time?
How to avoid negative delay times?
Current standard?
Which Path Device
Which Path Device – Why?
Quantum Measurement
Complementarity
Interference
Entanglement
Schrödinger’s cat
Electromechnical
Which-Path Device
Electromechanical Device
Simple Ideas
No change in the state of the cantilever
Aharonov-Bohm interference fringes
Cantilever state changes
Fringes destroyed
No non-destructive measurements
But
What about coherent coupling to the cantilever?
Resonant Coupling
Dwell time on dot » resonant frequency
Destroyed by coupling of cantilever to the environment
Need a high Q cantilever
Dissipation not well understood
Reflectivity
Slide 41
Summary
Simple nanomechanical devices
 now being made.
Nature got there first
lots of biological examples
Science fiction?
Micro machines to go around the bloodstream fixing the body
Lots of interesting new physics.