Bose–Einstein condensation of quasiparticles explained

Bose–Einstein condensation can occur in quasiparticles, particles that are effective descriptions of collective excitations in materials. Some have integer spins and can be expected to obey Bose–Einstein statistics like traditional particles. Conditions for condensation of various quasiparticles have been predicted and observed. The topic continues to be an active field of study.

Properties

BECs form when low temperatures cause nearly all particles to occupy the lowest quantum state. Condensation of quasiparticles occurs in ultracold gases and materials. The lower masses of material quasiparticles relative to atoms lead to higher BEC temperatures. An ideal Bose gas has a phase transitions when inter-particle spacing approaches the thermal De-Broglie wavelength:

k _{B} T = ~ \hbar ^{2} n ^{2/3} /M . The critical concentration is then N \propto (T/ 2 \pi) ^{3} u ^{1/2} P / v \hbar ^{3} , leading to a critical temperature: T _{c} < 32 \pi ^{3} \hbar ^{6} V ^{2} _{0 P} . The particles obey the Bose–Einstein distribution and all occupy the ground state:

The Bose gas can be considered in a harmonic trap,

V(r) = M \omega ^{2} / 2 , with the ground state occupancy fraction as a function of temperature:f( 0 ) = (N _{0(t)})/(N) = 1 - \left( (T)/(T _{c}) \right) ^{3}

This can be achieved by cooling and magnetic or optical control of the system. Spectroscopy can detect shifts in peaks indicating thermodynamic phases with condensation. Quasiparticle BEC can be superfluids. Signs of such states include spatial and temporal coherence and polarization changes. Observation for excitons in solids was seen in 2005 and for magnons in materials and polaritons in microcavities in 2006. Graphene is another important solid state system for studies of condensed matter including quasi particles; It's a 2D electron gas, similar to other thin films.^{[1] [2]}

Excitons

Excitons are electron-hole pairs. Similar to helium-4 superfluidity^[3] at the

λ -point (2.17K);^{[4] [5]} a condensate was proposed by Böer et al. in 1961.^[6] Experimental phenomenon were predicted leading to various pulsed laser searches that failed to produce evidence. Signs were first seen by Fuzukawa et al. in 1990, but definite detection was published later in the 2000s. Condensed excitons are a superfluid and will not interact with phonons. While the normal exciton absorption is broadened by phonons, in the superfluid absorption degenerates to a line.

Theory

Excitons results from photons exciting electrons creating holes, which are then attracted and can form bound states. The 1s paraexciton and orthoexciton are possible. The 1s triplet spin state, 12.1meV below the degenerate orthoexciton states(lifetime ~ns), is decoupled and has a long lifetime to an optical decay. Dilute gas densities (n~10¹⁴cm⁻³) are possible, but paraexciton generation scales poorly, so significant heating occurs in creating high densities(10¹⁷cm⁻³) preventing BECs. Assuming a thermodynamic phase occurs when separation reaches the de Broglie wavelength(

λ _{dB} ) gives:

Where,

n is the exciton density, effective mass(of electron mass order) m _{eff} , and \hbar ,k are the Planck and Boltzmann constants. Density depends on the optical generation g and lifetime as: n = g\tau . Tuned lasers create excitons which efficiently self-annihilate at a rate: dn/dt = - an ^{2} , preventing a high density paraexciton BEC.^[7] A potential well limits diffusion, damps exciton decay, and lowers the critical number, yielding an improved critical temperature versus the T^3/2 scaling of free particles:N _{c} = \zeta( 3 ) \left( (kT)/(\hbar \omega) \right) ^{3}

Experiments

In an ultrapure Cu₂O crystal:

\tau = 10s. For an achievable T = 0.01K, a manageable optical pumping rate of 10⁵/s should produce a condensate.^[8] More detailed calculations by J. Keldysh^[9] and later by D. Snoke et al.^[10] started a large number of experimental searches into the 1990s that failed to detect signs.^{[11] [12] [13]} Pulse methods led to overheating, preventing condensate states. Helium cooling allows mili-kelvin setups and continuous wave optics improves on pulsed searches. Relaxation explosion of a condensate at lattice temperature 354 mK was seen by Yoshioka et al. in 2011.^[14] Recent experiments by Stolz et al. using a potential trap have given more evidence at ultralow temperature 37 mK.^[7] In a parabolic trap with exciton temperature 200 mK and lifetime broadened to 650ns, the dependence of luminescence on laser intensity has a kink which indicates condensation. The theory of a Bose gas is extended to a mean field interacting gas by a Bogoliubov approach to predict the exciton spectrum; The kink is considered a sign of transition to BEC. Signs were seen for a dense gas BEC in a GaAs quantum well.^[15]

Magnons

Magnons, electron spin waves, can be controlled by a magnetic field. Densities from the limit of a dilute gas to a strongly interacting Bose liquid are possible. Magnetic ordering is the analog of superfluidity. The condensate appears as the emission of monochromatic microwaves, which are tunable with the applied magnetic field.

In 1999 condensation was demonstrated in antiferromagnetic TlCuCl₃,^[16] at temperatures as large as 14 K. The high transition temperature (relative to atomic gases) is due to the small mass (near an electron) and greater density. In 2006, condensation in a ferromagnetic Yttrium-iron-garnet thin film was seen even at room temperature^{[17] [18]} with optical pumping. Condensation was reported in gadolinium in 2011.^[19] Magnon BECs have been considered as qubits for quantum computing.^[20]

Polaritons

Polaritons, caused by light coupling to excitons, occur in optical cavities and condensation of exciton-polaritons in an optical microcavity was first published in Nature in 2006.^[21] Semiconductor cavity polariton gases transition to ground state occupation at 19K.^[21] Bogoliubov excitations were seen polariton BECs in 2008.^[22] The signatures of BEC were observed at room temperature for the first time in 2013, in a large exciton energy semiconductor device ^{[23] [24]} and in a polymer microcavity.^[25]

Other quasiparticles

Rotons, an elementary excitation in superfluid ⁴He introduced by Landau,^[26] were discussed by Feynman^[27] and others.^[28] Rotons condense at low temperature. Experiments have been proposed and the expected spectrum has been studied,^{[29] [30] [31]} but roton condensates have not been detected. Phonons were first observed in a condensate in 2004 by ultrashort pulses in a bismuth crystal at 7K.^[32]

See also

• Bose–Einstein condensate
• Bose-Einstein condensation of polaritons

Important publications

• Ando . Tsuneya . Fowler . Alan B. . Stern . Frank . Electronic properties of two-dimensional systems . Reviews of Modern Physics . American Physical Society (APS) . 54 . 2 . 1 March 1982 . 0034-6861 . 10.1103/revmodphys.54.437 . 437–672. 1982RvMP...54..437A .
• Dalfovo . Franco . Giorgini . Stefano . Pitaevskii . Lev P. . Stringari . Sandro . Theory of Bose-Einstein condensation in trapped gases . Reviews of Modern Physics . American Physical Society (APS) . 71 . 3 . 1 March 1999 . 0034-6861 . 10.1103/revmodphys.71.463 . 463–512. cond-mat/9806038 . 1999RvMP...71..463D . 55787701 .
• Bloch . Immanuel . Dalibard . Jean . Zwerger . Wilhelm . Many-body physics with ultracold gases . Reviews of Modern Physics . 80 . 3 . 18 July 2008 . 0034-6861 . 10.1103/revmodphys.80.885 . 885–964. 0704.3011 . 2008RvMP...80..885B . 119618473 .
• Bugrij . A. I. . Loktev . V. M. . On the theory of Bose–Einstein condensation of quasiparticles: On the possibility of condensation of ferromagnons at high temperatures . Low Temperature Physics . AIP Publishing . 33 . 1 . 2007 . 1063-777X . 10.1063/1.2409633 . 37–50. 2007LTP....33...37B . 119340633 .
• Butov . L. V. . Lai . C. W. . Ivanov . A. L. . Gossard . A. C. . Chemla . D. S. . Towards Bose–Einstein condensation of excitons in potential traps . Nature . Springer Nature . 417 . 6884 . 2002 . 0028-0836 . 10.1038/417047a . 47–52. 11986661 . 2002Natur.417...47B . 4373555 .

Notes and References

1. Bose–Einstein condensation of excitons in bilayer electron systems. 9 December 2004. Nature. 10.1038/nature03081. 15592403. 432 . 7018. 691–694. cond-mat/0404113 . 2004Natur.432..691E . Eisenstein . JP . Macdonald . AH. 1538354.
2. Bose–Einstein condensation and superfluidity of trapped polaritons in graphene and quantum wells embedded in a microcavity. 1 November 2010. Philosophical Transactions of the Royal Society A. 10.1098/rsta.2010.0208. 21041225 . 368 . 1932. 5459–82. 2010RSPTA.368.5459B . Berman . OL . Kezerashvili . RY . Lozovik . YE . Snoke . DW.
3. London . F . 1938 . The λ -Point of Liquid Helium and the Bose–Einstein Condensation . 10.1038/141643a0 . Nature . 141 . 3571 . 1938Natur.141..643L . 643–644. 4143290 .
4. Einstein, A. (1920) Proc. Berlin Acad. Science
5. Kapiza . P . 1938 . Viscosity of Liquid Helium below the λ-Point. 10.1038/141074a0 . Nature . 141 . 3558 . 74. 1938Natur.141...74K . free .
6. Blatt, J.M., K.W. Boer, and W. Brandt, (1962) Bose–Einstein Condensation of excitons, Phys. Rev. 126.5, 1691
7. Heinrich Stolz. 2012. etal. 10.1088/1367-2630/14/10/105007 . 14 . 10. 105007. 1206.7029 . 2012NJPh...14j5007S . Condensation of excitons in Cu2O at ultracold temperatures: Experiment and theory. New Journal of Physics. 118415141.
8. Aurora, C.P. (2001) Thermodynamics, McGraw-Hill
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10. Snoke . D.W. . David Snoke . Wolfe . J.P. . Mysyrovicz . A. . 1990 . Evidence for Bose-Einstein condensation of excitons inCu2O. 10.1103/physrevb.41.11171 . 9993538 . Phys. Rev. B . 41 . 16. 11171–11184 . 1990PhRvB..4111171S .
11. 10.1016/j.jlumin.2004.09.035. Bosonic stimulation of cold excitons in a harmonic potential trap in CuO. Journal of Luminescence. 112. 1–4. 11–16. 2005. Naka. N.. Nagasawa. N.. 2005JLum..112...11N.
12. Joshioka . K. . Ideguchi . T. . Mysyrovicz . A . Kuwata-Gonokami . M. . 2010 . Quantum inelastic collisions between paraexcitons inCu2O. 10.1103/physrevb.82.041201 . Phys. Rev. B . 82 . 4. 041201 . 2010PhRvB..82d1201Y .
13. Stolz . H. . Semkat . D. . 2010 . Unique signatures for Bose-Einstein condensation in the decay luminescence lineshape of weakly interacting excitons in a potential trap. 10.1103/physrevb.81.081302 . Phys. Rev. B . 81 . 8. 081302 . 0912.2010 . 2010PhRvB..81h1302S . 119242758 .
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18. [superfluidity|Magnon Bose Einstein Condensation]
19. Bose–Einstein condensation of magnons in polycrystalline gadolinium with nano-size grains. Jul 6, 2011. J Phys Condens Matter. 10.1088/0953-8984/23/26/266003. 21673396 . 23 . 26. 266003. 2011JPCM...23z6003M . Mathew . SP . Kaul . SN. 23487383 .
20. Magnon qubit and quantum computing on magnon Bose–Einstein condensates. 2 October 2014. Phys. Rev. A . 90 . 4. 042303 . 10.1103/PhysRevA.90.042303. 2014PhRvA..90d2303A . Andrianov. S. N. Moiseev. S. A.
21. Bose–Einstein condensation of exciton polaritons. 28 September 2006. Nature. 10.1038/nature05131. 17006506. 443 . 7110. 409–414. 2006Natur.443..409K . Kasprzak . J . Richard . M . Kundermann . S . Baas . A . Jeambrun . P . Keeling . JM . Marchetti . FM . Szymańska . MH . André . R . Staehli . JL . Savona . V . Littlewood . PB . Deveaud . B . Dang . 854066.
22. Observation of Bogoliubov excitations in exciton-polariton condensates. 2008. Nature Physics . 4 . 9. 700–705. 10.1038/nphys1034. 2008NatPh...4..673U . Utsunomiya. S. Tian. L. Roumpos. G. Lai. C. W. Kumada. N. Fujisawa. T. Kuwata-Gonokami. M. Löffler. A. Höfling. S. Forchel. A. Yamamoto. Y. free.
23. Polariton Bose–Einstein condensate at room temperature in an Al(Ga)N nanowire–dielectric microcavity with a spatial potential trap. February 19, 2013. Proceedings of the National Academy of Sciences. 10.1073/pnas.1210842110. 23382183. 110 . 8. 2735–2740. 1208.2723 . 2013PNAS..110.2735D . 3581885 . Das . A . Bhattacharya . P . Heo . J . Banerjee . A . Guo . W. free.
24. News: SCIENTIFIC METHOD / SCIENCE & EXPLORATION Bose–Einstein condensate created at room temperature. Francis. Matthew. Feb 6, 2013. Ars Technica.
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