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Page 1: Phase diffusion in a BEC of light - Universiteit Utrechtstoof101/Poster_Phase.pdf · Interference experiment condensate photons and external laser: 2) Thermal fluctuations 1) Quantum

E.C.I. van der Wurff*, A.-W. de Leeuw, R.A. Duine, and H.T.C. StoofInstitute for Theoretical Physics, Utrecht University, Leuvenlaan 4, 3584 CE Utrecht, The Netherlands

References

Fluctuations

*[email protected]

Conclusions

Phase diffusion in a BEC of light

Phase Diffusion [2,3]

[1] J. Klaers et al., Nature 468, 545 (2010).[2] E.C.I. van der Wurff et al., Phys. Rev. A 90, 043627 (2014).[3] M. Lewenstein and L. You, Phys. Rev. Lett. 77, 3489 (1996). [4] J. Schmitt et al., arXiv:1512.07148v1 [cond-mat.quant-gas]

Thermal fluctuations dominate quantum fluctuations

0

-1

1

0 5 10 15 2520t/tμ

cos(θ(

t))

0

6

θ0-

P(θ

;t)

3

Photons in a dye-filled microcavity [1]

Figures (modified) from Ref. [1]

before (L) and after (R) condensation

-200 -100 0 100 200

0

2

4

6

8

10

x (µm)

Signa

l (a.u.

)

-200 -100 0 100 200

0

2

4

6

8

10

x (µm)

Signa

l (a.u.

)

Thermalization photon gas due to coupling to dye

Photon gas equivalent to 2D trapped massive Bose gas

Conserved number of photons in cavity

Experiment at room temperature

Pumping increases number of photons condensation

Recent experiments [4]

Figures (modified) from Ref. [3]

Mirror

Dye

Laser Mirror

Camera

Pump Beam

Mode Filter

Proposal for phase diffusion experiment [2]

U(1) symmetry: conservation number of particles

Formally only in thermodynamic limit

Finite number of particles: phase non-trivial dynamics [3]

Condensation: spontaneous U(1) symmetry breaking

system in well-defined phase

Interference experiment condensate photons and external laser:

2) Thermal fluctuations

1) Quantum fluctuations (at T = 0)

Interference experiment has been carried out [3]

Many measurements should be averaged to verify predicted timescale

Solution to Langevin equations. Solid curve: one arbitary noise configuration; dashed: averaged over 500 noise configurations.

Schrödinger-like equation for phase wavefunction:

Solution displays difussion and collapse and revival

Condensate of photons in dye-filled microcavity: new experimental possibilities

Measurable timescale proposed to measure phase diffusion

Coupling to dye induces damping

Langevin field equations with Gaussian noise:

Intensity profile

Measurable time scale

Observation of phase flips

possibility to measure phase diffusion

frequency (THz)wavenumber (transversal)

Energy photon

q = 6 q = 7q = 8