on the foundations of fluctuation forces€¦ · on the foundations of fluctuation forces carsten...
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On the Foundations of Fluctuation Forces
Carsten Henkel1 and Vanik E. Mkrtchian2
1Universitat Potsdam, Germany 2Academy of Sciences, Armenia
Progress in Electromagnetic Research Symposium (Stockholm Aug 2013)
thanks to:
G. Pieplow, H. Haakh, J. Schiefele, network ‘Casimir’ (ESF), DFG
arXiv:1307.0682, New J Phys 15 (2013) 023027
Institute of Physics and Astronomy, Universitat Potsdam, Germany
www.quantum.physik.uni-potsdam.de
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(1831–79) (1872–1946) (1879–1955) (1908–96)
Paul Langevin Sergei Michailovich Rytov
Stockholm, Aug 2013
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Outline
Why?
Fluctuation interactions
How?
Langevin dialect of Maxwellian = Rytov theory
Basic observables
Local thermodynamic equilibrium
For example?
Non-equilibrium field theory (& Mkrtchian)
Quantum friction (& Pieplow, Haakh, Schiefele)
As time goes by . . .
Potential conversations
Forgotten references
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Maxwell & Langevin
Macroscopic electrodynamics
∂tB +∇×E = 0 ∇ ·B = 0
∂tD−∇×H = −j ∇ ·D = ρ
(inhomogeneous) material
approximation: linear response . . . always matter that provides nonlinearity
D = ε0ε(x, ω)E ε(ω), µ(ω) must be complex
H = µ−10 µ−1(x, ω)B ε(x), µ(x) cannot be local
[Wed 3P3b,Wed 3P5,
Thu 4P4
]Rytov: losses come with fluctuating sources (Langevin forces)
50mm[r]Principles Stat Radiophys (Springer 1989)
Stockholm, Aug 2013
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Maxwell & Langevin
Macroscopic electrodynamics
−iω
c2ε(x, ω)E = ∇× µ−1(x, ω)B− µ0j(x, ω) −iωB = ∇×E
Rytov: losses come with fluctuating sources (Langevin forces)
j = jfree − iωP(x, ω) +∇×M(x, ω) ‘noise polarization’ P
ρ = ρfree −∇ ·P(x, ω) ‘noise magnetization’ M
Maxwell-Langevin equation: ‘stochastic differential equation’
0 = 〈P(x, t)〉
0 6= 〈P(x, t)P(x′, t′)〉 =
∫dω
2πSP (x,x′, ω) eiω(t−t
′)spectral density
50mm[r]Principles Stat Radiophys (Springer 1989)
Stockholm, Aug 2013
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Maxwell & Langevin
Macroscopic electrodynamics
−iω
c2ε(x, ω)E = ∇× µ−1(x, ω)B− µ0j(x, ω) −iωB = ∇×E
Rytov: losses come with fluctuating sources (Langevin forces)
j = jfree − iωP(x, ω) +∇×M(x, ω) ‘noise polarization’ P
ρ = ρfree −∇ ·P(x, ω) ‘noise magnetization’ M
Maxwell-Langevin equation: ‘stochastic differential equation’
0 = 〈P(x, t)〉
0 6= 〈P(x, t)P(x′, t′)〉 =
∫dω
2πSP (x,x′, ω) eiω(t−t
′)spectral density
Rytov: SP,ij(x,x′, ω) ≈ 2hN(ω)ε0 Im εij(x, ω)δ(x− x′) . . . fluctuation-dissipation relation
Bose-Einstein distribution N(ω), local equilibrium T 7−→ T (x)
50mm[r]Principles Stat Radiophys (Springer 1989)
Stockholm, Aug 2013
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Fluctuation forces
Field energy (density, in vacuum)
u(x) =ε02〈E(x) ·E(x)〉+
µ−10
2〈B(x) ·B(x)〉 =
+∞∫−∞
dω u(x, ω)
• thermal sources 7−→ blackbody radiation (Planck 1900)
• near objects: non-universal spectrum, distance dependence (Planck, Purcell)
Dorofeyev & Vinogradov (Phys Rep 2011)
Force on rigid body in vacuum
d
dt(total momentum)i =
∮surf
dAj〈Tij〉 〈Maxwell stress tensor〉
〈Tij〉 = ε0〈EiEj −δij2E ·E〉+ µ−10 〈BiBj −
δij2B ·B〉
• quantum fluctuations 7−→ Casimir force (cosmological constant?)
TA > TB or ∇T : Heat current (Poynting vector) (this session Mon 1P3)
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Potential Conversations
— ‘Dynamical fluctuations’ and ‘static’ zero-point energy
— Stress tensor in a medium (in/homogeneous) T Philbin, Ch Raabe & D-G Welsch, M v Laue
— EM Fields: (retarded) link between charges R Feynman & J A Wheeler
— Linear macroscopic response: ‘filter theory’ signal engineers
— Local equilibrium assumption: ‘incoherent summation’
coherence from propagation (diffraction) Ch Huyghens, T Young
FD relation valid for both bosonic and fermionic matter
H. B. Callen & T. A. Welton, F. Garcia de Abajo
— Beyond local equilibrium: ‘thermodynamic cut’ L Boltzmann, M Lax, U Weiss
— Quantum limit (TA, TB 7−→ 0):
establishing correlations (entanglement) between bodies J S Høye & I Brevik, I Klich, R Behunin
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Example 1: Non-equilibrium field theory
Goal: calculate field correlations with Schwinger-Keldysh technique
diagrammatic formulation of density operator dynamics
path integral evaluation of effective action
Symmetrized correlations of vector potential (‘Keldysh Green function’)
DK(x, x′) = −i〈A(x), A(x′)〉
= . . . =
∫da da′G(x, a)SJ(a, a′)G∗(a′, x′)
(retarded) Green function G(x, x′), surface current correlations SJ (a, a′)
Assumption: un-correlated surfaces (bodies)
−→ single-interface SJ(a, a′) reproduces Rytov theory
+ arbitrary reflection matrices, + Lorentz transformation of surface currents
– planar surfaces (translation symmetry), – stationary situation (spectra)
Mkrtchian & Henkel
arXiv:1307.0682
Janowicz & Holthaus
Phys Rev A 2003
Sherkunov
Phys Rev A 2007/09
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Example 2: Quantum friction near graphene08/08/13 14:26
Page 1 sur 2file:///Users/carstenh/Work/Voyages/Piers_Stockholm_Aug13/Pics/surface.svg
metallic nanoparticle at speed v ∼ c
graphene sheet (dielectric substrate)
• friction (‘Coulomb drag’)
↑ creation of excitations
photons in substrate (“Cherenkov”)
graphene plasmons
Mon 1A1, . . . Tue 2AK, Wed 3AKMotivation
giant anomalous Doppler shift: ω′ = γ(ω − k · v) < 0
bridge gap between metallic (UV) and graphene (IR) plasmons
controversy on quantum friction (T → 0 limit)
. . . 40 years of discordant results (Teodorovich 1978 ... session Tue 2P4)
Stockholm, Aug 2013
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2 Radiation forces and friction
Force on neutral, polarizable particle
F (x,v) = 〈di∇Ei〉︸ ︷︷ ︸dominates
+ 〈µi∇Bi〉 fluctuating particle dipole
fluctuating field & substrate excitations
Expansion in 4th order correlations:
— polarizability α(ω′) in co-moving frame: Doppler shift ω′ = γ(ω − k · v)
— dipole fluctuation spectrum Sd(xA, ω′) in local equilibrium
— field response = Green function . . .
Quantum friction force (substrate & field TF → 0, particle TA → 0)
Fx =h
2γ
∫dω
2π
d2k
(2π)2kx (sgnω − sgnω′)
× Im α(ω′)∑σ= s,p
φσ(k, ω) Im( e−2κzA rσ(k, ω)
κ
)Dedkov & Kyasov, Phys Solid St ≥ 2001; Pieplow & Henkel, New J Phys 2013
Stockholm, Aug 2013
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2 Resonant emission of graphene plasmons
force density Fx dω dkx
freq
uen
cyhω/E
F
0.00 0.05 0.10 0.15 0.20 0.25 0.30 0.350.0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
wave vector kx/kF (vx = 0.22 c)fr
equ
ency
hω/E
F
0.00 0.02 0.04 0.06 0.08 0.10 0.12 0.140.0
0.1
0.2
0.3
0.4
0.5
0.6
kx/kF (vx = 0.42 c)
plasmon dispersion
ω ∼√k ck
shifted particle resonance
−Ω = ω′ = γ(ω − k · v)
free-standing graphene film
EF = 0.5 eV, c ∼ 300 vF
distance 100 nm
gold particle plasmon hΩ ≈ 5.2 eV
G. Pieplow, H. Haakh, J. Schiefele, work in progress
giant anomalous Doppler shift: ω′ < 0
emission of 1st plasmon excites the particle: ω′ + Ω = 0
Frank & Tamm explain Cherenkov radiation (1937) review: Ginzburg (Phys Uspekhi 1996)
Stockholm, Aug 2013
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Appendix – forgotten references
von Laue: Thermal radiation in absorbing bodies (Ann. Phys. (Leipzig) 1910)
Bakker & Heller: ‘Quantum’ Brownian motion in electric resistances (Physica 1939)
Jauch & Watson: Phenomenological Quantum-Electrodynamics (Phys Rev 1948)
Callen & Welton: Irreversibility and generalized noise (Phys Rev 1951)
De Groot & al: Series on relativistic thermodynamics (Physica ≥ 1953)
V. L. Ginzburg: Electrical fluctuations (Fortschr Phys 1953)
Linder: Thermal Van der Waals interactions (J Chem Phys ≥ 1960)
van Kampen: FD relation in non-linear systems? (Physica 1960) vs Polevoi & Rytov (Theor Math Phys 1975)
Morris & Furth: Spatial field correlations near conducting surfaces (Physica 1960)
see also Fuchs (Radiophys Quant Electr 1965)
Jaynes & Cummings: Quantum vs semiclassical radiation theories (Proc. IEEE 1963)
Agarwal: FD theorems and series on field quantization (Z Phys 1972; Phys Rev A 1975)
Boyer: Connection between Rytov and quantum electrodynamics (Phys Rev D 1975)
Ginzburg & Ugarov: Macroscopic stress tensor (Sov Phys Usp 1976)
Polevoi: Tangential forces/friction in non-equilibrium fields (JETP 1985/90)
Eckhart: Problems with FD relations for heat transfer (Opt Commun ≥ 1982)
Henry & Kazarinov: Quantum noise in photonics (Rev Mod Phys 1996)
Stockholm, Aug 2013
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Summary – Status of Learning Curve
Rytov fluctuation electrodynamics
‘Robust working horse’ – as long as matter responds linearly
Universal framework to recover: thermal radiation, heat transfer,
Casimir-Lifshitz forces, quantum friction
. . . beyond local equilibrium: non-local response
Statistics (thermodynamics) vs quantum
Intuitive picture for vacuum fluctuations ‘semiclassical’, ‘dynamical’
Radiative infinities regularized by temperature and coupling to matter
. . . non-equilibrium interactions entropy production
entanglement production
www.quantum.physik.uni-potsdam.de → download slides (end of week)