measurement of the casimir force with a ferrule-top sensor paul zuurbier supervisors: sven de man...
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![Page 1: Measurement of the Casimir force with a ferrule-top sensor Paul Zuurbier Supervisors: Sven de Man Davide Iannuzzi Technical support: Kier Heeck Associated](https://reader034.vdocuments.us/reader034/viewer/2022051316/56649d3e5503460f94a1730b/html5/thumbnails/1.jpg)
Measurement of the Casimir force with a ferrule-top sensor
Paul Zuurbier
Supervisors:Sven de ManDavide Iannuzzi
Technical support:Kier Heeck
Associated group members:Grzegorz GrucaDhwajal Chavan
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A phenomenon described in 1836
P.C.CausséeL’Album du Marin
Two parallel ships are driven to each other by a mysterious attractive force
They are pushed one against the other by the waves outside “the gap”
A likely explanation:The two ships act like barriers
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The Casimir effect
H.B.G.Casimir(1909-2000)
d
1948: In the presence of two parallel plates (conductors)
e.m. wave = harmonic oscillator
in vacuum
0 2
1dE
The energyBetween thePlates is lower
CasimirF
Closely relatedto van der Waals force
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The need of ferrule-top Casimir measurement
Increasing interest in studying the Casimir force in various environments, for instance in liquids and with varying temperature.
Our group designed and manufactured the ferrule-top sensor, which is versatile, adaptive and cost effective:
Measuring Casimir force is difficult, so it is a good benchmark.
My job: Test the new sensor by performing the first ferrule-top Casimir force measurement.
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Sphere and plate Casimir force
solution
If too small → F too small
Radius ≈ 100 µm
d ≈ 40 – 200 nm
F < ~4000 pN
macroscopic objectsat microscopic distancediameter ≈ 5000·dmin
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Ferrule-top force sensor fabrication
Borosilicate ferrule2.5 x 2.5 x 7.0 mm
Laser ablation:200 x 200 µm ridge
100 µm gap
sphere is glued on
optical fiber is insertedand fixed with glue
hole in cantilever is closed
gold layer is sputteredon the sensor
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not inuse
Ferrule-top
Interferometer
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Temperature stabilized Al cylinder
Al cover (dust and convection)
Dampers
Table-top setup design
Left: Piezo translator with gold plate (varying d)
Right: Mechanical translator with sensor + sphere
Anechoic chamber
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We calibrate continuously by applying a well known electrostatic force.
We apply an AC voltage to the sphere
We measure the signal due to this force
at double the frequency
We calculate the sensitivity
problems and solutions: Calibration
How does one calibrate a ferrule-top force sensor?
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problems and solutions: Distance
How does one measure a distance< 100 nm with ~1 nm accuracy?
From the electrostatic Coulomb force
we get a signal S proportional to 1/d. From this we can fit d0.
With an second interferometer we measure Δx. At this stage we know d = Δx + d0,but d0 is unknown.
Δx
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nmd
pNF
d
F
7
500
problems and solutions: Noise and drift
Since k~7 N/m and F<4 nN the cantilever bends only half a nanometer!
In this situation the drift of the interferometer intensity is overwhelming.Therefore we vibrate the plate and measure ΔF:
Because we are modulating the Casimir force we can use alock-in amplifier with superior noise suppression (AM).
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problems and solutions: Hydrodynamics
Plate vibration airflow hydrodynamic force on sphere.
How does one distinguish between hydrodynamic and Casimir force?
The Casimir force depends on d ~ cos(ωt)
The hydrodynamic force depends on ~ -sin(ωt)
Both signals are 90° out of phase (orthogonal).
The signal is measured with a lock-in amplifier and we can getthe Casimir force from channel X (in phase) and the hydrodynamic forcefrom channel Y (quadrature).
t
d
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Hydrodynamic results
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Final results
40.000 points
no free parameters
close agreementwith theory and earlierexperiments
conclusion:the sensor is capableof measuring Casimirforce,article published NJP
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End