Title: Quantum Electronics Seminar presentation Tobias Kippenberg
1Quantum Electronics Seminarpresentation Tobias
Kippenberg
2Outline
- Historical overview
- A quantum mechanical derivation of the Casimir
force on two parallel conducting plates - The Casimir force in the age of nanotechnology
MEMS - Effects of the casimir force on MEMS
- Dynamical effects of the casimir force
3The Casimir force
Hendrik Casimir (1909-2000)
Koninkl. Ned. Akad. Wetenschap. Proc. 51, 793
(1948).
Source physicsweb.org
4Family of Casimir forces
- Several attractive forces are termed Casimir
forces - Attraction between an atom and a dielectric
- Attraction between an atom and a metalic surface
- Attraction between two dielectrics
- Attraction between two metallic surfaces.
Casimir-Polder forces
Casimir-forces
5Zero point energy
- Zero point energy First introduced by Planck
second theory of black body radiation (ca. 1930)
Zero point energy was needed to reconcile
thermodynamics with radiation spectrum, when
considering a harmonic oscillator in equilibrium
with temperature.
Initially thought that the zero point Energy was
of no physical consequence.
The total zero point energy of all modes is
infinite!
e.g. P.W. Milonni, Contemporary Physics 1992, V
33, No. 5, 313
6Derivation of the Casimir forceby zero-point
energy consideration
Casimirs idea was to look at situations where
the zero point Energy might change. He considered
two parallel conducting plates.
The allowed frequencies obey
The vacuum energy is the sum of the now discrete
set of modes
He considered the differences of the vacuum energy
Closely spaced
Infinite separation
e.g. P.W. Milonni, Contemporary Physics 1992, V
33, No. 5, 313
7Derivation of the casimir forceby zero-point
energy consideration
- The sum of these two infinite sums can be
calculated (Euler-Maclaurin series). This change
in energy give rise to a attractive force between
the plat
- This gives rise to an attractive force, varying
as the fourth power between two metallic plates
separates a distance z
- First successful experiments were reported by
Derjaguin et al. in 1951. good quantitative
agreement due to the lack of absorption spectra
e.g. P.W. Milonni, Contemporary Physics 1992, V
33, No. 5, 313
8Casimir-type effect in fluid dynamics
Source Buks, Roukes, newsviews, Nature 2002
9Alternative interpretation Linear momentum of
photons
- The casimir force can also be interpreted by
considering the radiation pressure due to the
photon momentum.
10Casimir force for different geometries
- Casimir force for two conducting plates
- 1cm x 1cm conducting plates separated by 1
micron. Casimir Force F 130 nN - Force is identical to the gravitational
attraction of two blocks of mass m 1lb 0.5 inch
apart
- Casimir force between a plate and a conductor
11Resurgence of Casimir force
- Driving force MEMS micro-electro-mechanical
systems
Stiction
Source www.sandia.gov
12Casimir force experiment
Source physicsweb.org
13Casimir force measurement
Heavily doped poly-silicon top plate
Torsional rod (rotation axis)
Electrical contacts
archor for torsional rod
Source Capasso et al. Science
14Casimir force measurements setup
- Capacitance measurements to measure torque angle
- Application of DC voltage to cause a torque
- Use a AC voltage to sense the change in
capacitance
?C1 part 2x105 Equivalent angle 8x10-8 rad
Source Capasso et al. Science
15Calibration using electrostatic attraction
To measure a force, the mechanical system need to
be characterized in terms of the torsional spring
constant.
Small amplitude approximation
Electrostatic attraction (V290mV)
?6x10-5 N rad-1 z0 67 nm V0 30 mV (work
function difference of two Gold surfaces)
Source Capasso, Science, Vol. 291 (2001)
16Casimir force measurements
By turning of the electrostatic attraction by
proper biasing the Casimir force can be
observed!!!
- Maximum force is ca. 700 pN
- forces become observable at ca. 300 nm
- Short range 1/r3
- Surface roughness increases Casimir force
- transmission of gold at 500 nm weakens the
Casimir force
Electrostatic attraction
Source Capasso, Science, Vol. 291 (2001)
17Pertubation of a harmonic oscillator by the
Casimir force
Source Capasso et al. Phys. Rev. Lett. (2001)
18Casimir oscillator
2V
- The torsional rod is driven
- by an AC voltage
- Mechanical resonance frequency at 2.7KHz
- Oscillator is harmonic
V
Source Capasso et al. Phys. Rev. Lett. (2001)
19Anharmonic oscillator due to Casimir force
Shifted resonance
- Driving force (torque)
- Natural oscillation frequency
- Damping coefficient
- Casimir force
- Anharmonic contributions due to the Casimir
force - 2nd order
- 3rd order
20Casimir oscillator in the small oscillation regime
IN the small pertubation regime the anharmonic
terms which are cubic and quadratic in order can
be neglected.
Casimir force
Electrostatic attraction
Source Capasso et al. Phys. Rev. Lett. (2001)
21Nonlinear Casimir oscillator
3300 nm
141 nm
116.5 nm
98 nm
Source Capasso et al. Phys. Rev. Lett. (2001)
22Outlook
- - Casimir force is a non-intuitive force which
exemplifies the profound influence of quantum
vacuum - - The force is likely to receive revived interest
in the future due to the drive in miniaturization
and high sensitivity measurems.
23Historical overview of the Casimir force
- Prediction Hendrik Casimir of Philips Research
Laboratories in the Netherlands - "colloidal solutions". These are viscous
materials, such as paint and mayonnaise, that
contain micron-sized particles in a liquid
matrix. The properties of such solutions are
determined by van der Waals forces - long-range,
attractive forces that exist between neutral
atoms and molecules. - 1932 Theo Overbeek, realized that the theory
that was used at the time to explain van der
Waals forces, which had been developed by Fritz
London in 1932, did not properly explain the
experimental measurements on colloids. Overbeek
therefore asked Casimir to investigate the
problem. Working with Dirk Polder, Casimir
discovered that the interaction between two
neutral molecules could be correctly described
only if the fact that light travels at a finite
speed was taken into account - Soon afterwards, Casimir noticed that this result
could be interpreted in terms of vacuum
fluctuations. He then asked himself what would
happen if there were two mirrors - rather than
two molecules - facing each other in a vacuum. It
was this work that led to his famous prediction
of an attractive force between reflecting plates.