Title: Measurements of Forces at the Nanoscale
1 Measurements of Forces at the Nanoscale some
ideas for measurements at LEPES in 2005 J.
Chevrier 18 November 2004
2we consider three different forces - Casimir
hc J.m - Electrostatic e2/4pe0
J.m -Gravity Gm2 J.m
3-electrostatic Charles A. Coulomb 1736-1806
- strong force - long range today Easily
measured -gravity Henry
Cavendish Nice 1731 - Londres 1810 - weaker
force (e2/4pe0) / Gm2 ? 1040 - long range a
bit more difficultbut still a student training
4 - Casimir/van der Waals versus
electrostatic
Sphere diameter 50 mm sphere/surface 10nm -1 mm
hc / (e2/4pe0) ? 137 fine structure constant
However unless at very short distances (lt
1nm) (if static charges present not
neutral) electrostatic gtgt Casimir
Casimir short range characteristic distance
at the nanoscale Nanosciences
5origin of van der waals/casimir interaction
between two neutral systems in their fundamental
state electron-photon coupling by dipolar
interaction -d.E
Fundamental state
Fundamental state
Electronic excitations e(q,w)
-d.E
-d.E
temps
-d.E
-d.E
Fundamental state
Fundamental state
6Characteristic length for two metallic
surfaces (jellium model) defined by
electronic excitations coupled to
photons surface plasmons characteristic
length
l p 2p c/ w p
Aluminium h w p 14eV
l p ? 100nm
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8Coupling of
Surface
plasmons
Surface
plasmons
dltlt l p
9Fgt0 attractif
Flt0 répulsif
Al
Plasmon polariton
SiC
Phonon polariton
d10nm
Plasmon polariton
dltlt l p
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11The way the plasmon-photon coupling is changed
w
q
k
1
e
ph
1
2
k
e
x
2
k
sp
a
w
1
k
x
p
/a
12Experiment Force measurement at distances
close to 10nm below the plasma length to be
sensitive to surface electronic excitations
Using a resonating oscillator perturbed by the
van der Waals/Casimir interaction.
k, w
Interaction F
sample
13sample
14Electrostatic calibration
Dispersion force in the non retarded régime
15Home made force machine built within the X tip
european project at the ESRF in 2004
Pour le LEPES en 2005 extension to measurement
at short distances dltlt l p under vacuum and at
low T (4K) ...
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20Very very large roughness...
hope we shall avoid such a hard collision next
time good point however parallel surfaces well
prepared.
21 Experimental objective Combination of sphere
on cantilever or on tuning fork measurement
of frequency shift with resolution close to 1mHz
22Gauthier Torricelli Thèse LEPES/ESRF
Mario Rodriguez stage de Master 2 ESRF
Guillaume Jourdan Thèse LEPES/Lab. Kastler
Brossel Direction J. Chevrier/ A. Lambrecht