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Near-field radiative heat transfer and Casimir Force Measurement J. Chevrier Institut Néel, CNRS and Université Joseph Fourier, Grenoble, France ESRF, Grenoble, France mercredi 7 octobre 2009

Near-field radiative heat transfer and Casimir Force ...cnls.lanl.gov/casimir/PresentationsSF/Joel_Santa_Fe_reduit.pdf · 3 Probing near-field thermal radiation New insights into

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Page 1: Near-field radiative heat transfer and Casimir Force ...cnls.lanl.gov/casimir/PresentationsSF/Joel_Santa_Fe_reduit.pdf · 3 Probing near-field thermal radiation New insights into

Near-field radiative heat transfer

and Casimir Force Measurement

J. Chevrier

Institut Néel,

CNRS and Université Joseph Fourier,

Grenoble, France

ESRF, Grenoble, France

mercredi 7 octobre 2009

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Probing near-field thermal radiation

New insights into the behaviour of radiative heat transfer at the nanoscale have now been made, thanks to highly

precise measurements made using scanning probe microscopy.

Achim Kittel

News and views Nature Photonics

In 1900, Max Planck used quantum theory to explain the puzzling nature of the

spectral density of thermal far-field radiation.

However, Planck realized that the situation becomes more complex in the near-field

regime, where the distance between two bodies is comparable to the characteristic

wavelength of thermal radiation (that is, the sub-micrometre range).

!1 µm

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Polder, D. & Van Hove, M. Theory of radiative heat transfer between closely spaced

bodies. Phys. Rev. B 4, 3303–3314 (1971).

Rytov, S. M., Kratsov, Yu. A. & Tatarskii, V. I.

Principles of Statistical Radiophysics 3, Ch. 3 (1987).

Hargreaves, C. M.

Anomalous radiative transfer between closely-spaced bodies.

Phys. Lett. A 30, 491–492 (1969).

Domoto, G. A., Boehm, R. F. & Tien, C. L.

Experimental investigation of radiative transfer between metallic surfaces at cryogenic

temperatures.

J. Heat Transfer 92, 412 (1970).

E. G. Cravalho, C. L. Tien, and R. P. Caren, J. Heat Transfer 89, 351 (1967).

R.P. Caren and C.-K. Liu, in Progr. Aeronautics and Astronautics 21, edited by T.J.

Bevans (1969), p509 (1968)

E.G. Cravalho, G.A. Domoto and C.L. Tien, in Progr. Aeronautics and Astronautics

21, edited by T.J. Bevans (Academic, New-York, 1969), p531 (1968)

S. Shen, A. Narayanaswamy, and G. Chen, Surface phonon polariton mediated energy transfer between nanoscale gaps, Nano Letters, 2009

mercredi 7 octobre 2009

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T1

T2

T1 > T2

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Casimir force and radiative heat transfer:two phenomena with the same origin

Casimir force at short distances:

10 nm SiC/SiC plane/plane geometry

T1T1S

FF

[N

/(m

2H

z)]

Casimir force power spectrum

SiC silicon carbide

IRclose to 300K

UV>>300K

d=10nm

C. Henkel et al 2004 PRA

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Casimir force and radiative heat transfer:two phenomena with the same origin

SF

F [N

/(m

2H

z)]

Casimir force power spectrum

SiC silicon carbide

IRclose to 300K

UV>>300K

electron/ion resonancehw >> kT

plasmon polariton

ion/ion resonancehw ! kT

phonon polariton

m/M

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Casimir force and radiative heat transfer:two phenomena with the same origin

Near-field radiative heat

transfer:

energy transfer

non equilibrium situation

Thermal energy density in near field regime at 300K

300K

SiC

d=10nm

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Dielectric materials: surface Phonon-Polariton enchantement e!ect

Density of energy near a SiC-vacuum interface

PRL, 85 p 1548 (2000)

Far field: the energy density well

reproduces the Planck black body theory

propagating waves

Near field: the energy density exceeds

the Planck black body theory

evanescent waves

orders of magnitude

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Dielectric materials: surface Phonon-Polariton enhancement e!ect

Surface waves: described by dielectric constant !(")

Infra-red resonance

(SiC, silica= glass)

Radiative thermal transfer

dominated by the resonance effect

Sheng Shen et al. Nano Letters July 2009

E

p

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Far fieldPlanck-Stephan

Near field

evanescent wave contribution

phonon polariton

flat Glass

300 K

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Dielectric materials: surface Phonon-Polariton enhancement e!ect

T1

T2

Plane-Plane geometry

T1 > T2

Theoretical estimation

see method and results in:

J. Ph. Mulet PhD thesis

and papers from

JJ Greffet group

evanescent and propagative waves included

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Glass/Glass

SiC/SiC dTexte

see method and results in J. Ph. Mulet PhD thesisfrom JJ Greffet group

1/d2

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Plane-plane geometry:

experimental issue

Plane-Plane

Theory developed

BUT

Parallel planes: very hard

Plane-sphere

Experimentally possible

BUT

Theory not yet developed

d d

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Sphere-Plane geometry: theory

Proximity force approximation

d

d

Sphere-Plane geometry

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Page 16: Near-field radiative heat transfer and Casimir Force ...cnls.lanl.gov/casimir/PresentationsSF/Joel_Santa_Fe_reduit.pdf · 3 Probing near-field thermal radiation New insights into

Sphere-Plane geometry: theory

Vacuum thermal conductance at all distances in PFA (local)

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Page 17: Near-field radiative heat transfer and Casimir Force ...cnls.lanl.gov/casimir/PresentationsSF/Joel_Santa_Fe_reduit.pdf · 3 Probing near-field thermal radiation New insights into

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Sphere-Plane geometry: theory

Proximity force approximation

d

d

Far field Far field

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Page 18: Near-field radiative heat transfer and Casimir Force ...cnls.lanl.gov/casimir/PresentationsSF/Joel_Santa_Fe_reduit.pdf · 3 Probing near-field thermal radiation New insights into

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Switch to radiative heat transfer measurement…

What we want to measure

How we want to measure

mercredi 7 octobre 2009

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Experimental set-up

Optical fiber

Au

Si 3

N4

starting with our Casimir set up

from Guillaume Jourdan thesis

EPL 85 No 3 (February 2009) 31001

Phys. Rev. Lett. 101, 133904 (2008)Nanotechnology 19 No 44 (5 November 2008)Nanotechnology 18 No 47 (28 November 2007)

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07/08/07

www.neel.cnrs.fr

Room temperature Casimir Machine

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07/08/07

www.neel.cnrs.fr

mercredi 7 octobre 2009

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07/08/07

www.neel.cnrs.fr

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Experimental set-up

Optical fiber

Au

Si 3

N4

Optical fiber

Au

Si 3

N4

Gold sphereGold plane

Glass sphereGlass plane

Casimir set up Thermal transfer set up

Tc Th

Static measurement

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Experimental set-up

- Power exchanged = lever deflection : thermal switch effect on the lever

-- High vacuum P~10-6 mbar : conduction neglegible

- #T = 10-20 K.

-Closed feedback loop and thermal drift

Optical fiber

Au

Si3N4

Thermal switch

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Optical fiber

Au

Si3N4

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lever bending versus heat flux:

H nW/nm

calibration required

absolute distance between sphere/plane: b: due to surface roughness

measured in direct contact for each measurement

always close to 50nmconsistent with SEM images of the glass sphere

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lever bending versus heat flux:

H nW/nm

$ = H . cantilever bending

H=2.3nW/nm

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!T=10, 17, 21 K,

H=2.17, 2.16, 2.14 (same H )

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Comparison Experience-theory

Glass sphere – glass plane

Sphere diameter 40 µm

H and % adjusted

H = 2.162 nW/nm (2.2)% = 31.8 &µ

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Glass sphere – glass plane

Sphere diameter 40 µm

ZOOM ON NEAR-FIELD REGIME

Comparison Experience-theory

H and % adjusted

H = 2.162 nW/nm (2.2)% = 31.8 &µ

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Comparison Experience-theory

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Conclusions and perspectives

Development of experimental set-up for the radiativethermal transfer

Radiative thermal tranfer forsphere-plane geometry based on PFA

Precise measurement of thermal flux in 50nm-5µm

Conclusions:

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END...

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