Bose–Einstein correlations

In physics, Bose–Einstein correlations^[1][2] are correlations between identical bosons. They have important applications in astronomy, optics, particle and nuclear physics.

From intensity interferometry to Bose–Einstein correlations

The interference between two (or more) waves establishes a correlation between these waves. In particle physics, in particular, where to each particle there is associated a wave, we encounter thus interference and correlations between two (or more) particles, described mathematically by second or higher order correlation functions.^[3] These correlations have quite specific properties for identical particles. We then distinguish Bose–Einstein correlations for bosons and Fermi–Dirac correlations for fermions. While in Fermi–Dirac second order correlations the particles are antibunched, in Bose–Einstein correlations (BEC)^[4] they are bunched. Another distinction between Bose–Einstein and Fermi–Dirac correlation is that only BEC can present quantum coherence (cf. below).

In optics two beams of light are said to interfere coherently, when the phase difference between their waves is constant; if this phase difference is random or changing the beams are incoherent.

The coherent superposition of wave amplitudes is called first order interference. In analogy to that we have intensity or second order Hanbury Brown and Twiss (HBT) interference, which generalizes the interference between amplitudes to that between squares of amplitudes, i.e. between intensities.

In optics amplitude interferometry is used for the determination of lengths, surface irregularities and indexes of refraction; intensity interferometry, besides presenting in certain cases technical advantages (like stability) as compared with amplitude interferometry, allows also the determination of quantum coherence of sources.

Bose–Einstein correlations and quantum coherence

The concept of higher order or quantum coherence of sources was introduced in quantum optics by Glauber.^[5] While initially it was used mainly to explain the functioning of masers and lasers, it was soon realized that it had important applications in other fields of physics, as well: under appropriate conditions quantum coherence leads to Bose–Einstein condensation. As the names suggest Bose–Einstein correlations and Bose–Einstein condensation are both consequences of Bose–Einstein statistics and thus applicable not only to photons but to any kind of bosons. Thus Bose–Einstein condensation is at the origin of such important condensed matter phenomena as superconductivity and superfluidity, and Bose–Einstein correlations manifest themselves also in hadron interferometry.

Almost in parallel to the invention by Hanbury-Brown and Twiss of intensity interferometry in optics Gerson Goldhaber, Sulamith Goldhaber, Wonyong Lee, and Abraham Pais (GGLP) discovered^[6] that identically charged pions produced in antiproton-proton annihilation processes were bunched, while pions of opposite charges were not. They interpreted this effect as due to Bose–Einstein statistics. Subsequently^[7] it was realized that the HBT effect is also a Bose–Einstein correlation effect, that of identical photons.^[8]

The most general theoretical formalism for Bose–Einstein correlations in subnuclear physics is the quantum statistical approach,^[9][10] based on the classical current^[11] and coherent state,^[12][13] formalism: it includes quantum coherence, correlation lengths and correlation times.

Starting with the 1980s BEC has become a subject of current interest in high-energy physics and at present meetings entirely dedicated to this subject take place.^[14] One reason for this interest is the fact that BEC are up to now the only method for the determination of sizes and lifetimes of sources of elementary particles. This is of particular interest for the ongoing search of quark matter in the laboratory: To reach this phase of matter a critical energy density is necessary. To measure this energy density one must determine the volume of the fireball in which this matter is supposed to have been generated and this means the determination of the size of the source; that can be achieved by the method of intensity interferometry. Furthermore, a phase of matter means a quasi-stable state, i.e. a state which lives longer than the duration of the collision that gave rise to this state. This means that we have to measure the lifetime of the new system, which can again be obtained by BEC only.

Quantum coherence in strong interactions

Bose–Einstein correlations of hadrons can also be used for the determination of quantum coherence in strong interactions.^[15][16] To detect and measure coherence in Bose–Einstein correlations in nuclear and particle physics has been quite a difficult task, because these correlations are rather insensitive to even large admixtures of coherence, because of other competing processes which could simulate this effect and also because often experimentalists did not use the appropriate formalism in the interpretation of their data.^[17]

The most clear evidence^[18] for coherence in BEC comes from the measurement of higher order correlations in antiproton-proton reactions at the CERN SPS collider by the UA1-Minium Bias collaboration.^[19] This experiment has also a particular significance because it tests in quite an unusual way the predictions of quantum statistics as applied to BEC: it represents an unsuccessful attempt of falsification of the theory ^[1]. Besides these practical applications of BEC in interferometry, the quantum statistical approach ^[10] has led to quite an unexpected heuristic application, related to the principle of identical particles, the fundamental starting point of BEC.

Bose-Einstein correlations and the principle of identical particles in particle physics

As long as the number of particles of a quantum system is fixed the system can be described by a wave function, which contains all the information about the state of that system. This is the first quantisation approach and historically Bose–Einstein and Fermi–Dirac correlations were derived through this wave function formalism. In high-energy physics, however, one is faced with processes where particles are produced and absorbed and this demands a more general field theoretical approach called second quantisation. This is the approach on which quantum optics is based and it is only through this more general approach that quantum statistical coherence, lasers and condensates could be interpreted or discovered. Another more recent phenomenon discovered via this approach is the Bose–Einstein correlation between particles and anti-particles.

The wave function of two identical particles is symmetric or antisymmetric with respect to the permutation of the two particles, depending whether one considers identical bosons or identical fermions. For non-identical particles there is no permutation symmetry and according to the wave function formalism there should be no Bose–Einstein or Fermi–Dirac correlation between these particles. This applies in particular for a pair of particles made of a positive and a negative pion. However this is true only in a first approximation: If one considers the possibility that a positive and a negative pion are virtually related in the sense that they can annihilate and transform into a pair of two neutral pions (or two photons), i.e. a pair of identical particles, we are faced with a more complex situation, which has to be handled within the second quantisation approach. This leads,^[20][21] to a new kind of Bose–Einstein correlations, namely between positive and negative pions, albeit much weaker than that between two positive or two negative pions. On the other hand, there is no such correlation between a charged and a neutral pion. Loosely speaking a positive and a negative pion are less unequal than a positive and a neutral pion. Similarly the BEC between two neutral pions are somewhat stronger than those between two identically charged ones: in other words two neutral pions are “more identical” than two negative (positive) pions.

The surprising nature of these special BEC effects made headlines in the literature.^[22] These effects illustrate the superiority of the field theoretical second quantisation approach as compared with the wave function formalism. They also illustrate the limitations of the analogy between optical and particle physics interferometry: They prove that Bose–Einstein correlations between two photons are different from those between two identically charged pions, an issue which had led to misunderstandings in the theoretical literature and which was elucidated in ^[23] (see also Ref. [1]).

References

1. Richard M. Weiner, Introduction to Bose–Einstein Correlations and Subatomic Interferometry, John Wiley, 2000.
2. Richard M. Weiner, Bose–Einstein Correlations in Particle and Nuclear Physics, A Collection of Reprints, John Wiley, 1997, ISBN 0-471-96979-6.
3. The correlation function of order n defines the transition amplitudes between states containing n particles.
4. In this article the abbreviation BEC is reserved exclusively for Bose–Einstein correlations, not to be confused with that sometimes used in the literature for Bose–Einstein condensates.
5. R. J. Glauber, Phys. Rev. 131 (1963) 2766.
6. G. Goldhaber, S. Goldhaber, W. Lee, and A. Pais, Phys. Rev. 120 (1960), 300, reprinted in Ref.2, p.3.
7. V.G. Grishin, G.I. Kopylov and M.I. Podgoretski¡i, Sov. J. Nucl. Phys. 13 (1971) 638, reprinted in Ref.2, p.16.
8. That it took quite a long time to establish this connection is due in part to the fact that in HBT interferometry one measures distance correlations while in GGLP momentum correlations.
9. I. V. Andreev and R. M. Weiner, Phys. Lett. 253(1991) 416, reprinted in Ref.2, p. 312.
10. I. V. Andreev, M. Plümer and R. M. Weiner, Int. J. Mod. Phys. 8A (1993) 4577, reprinted in Ref.2. p. 352.
11. G. I. Kopylov and M. I. Podgoretskiĭ, Sov. J. Nucl. Phys. 18 (1974) 336, reprinted in Ref.2, p. 336.
12. G. N. Fowler and R. M. Weiner, Phys. Rev. D 17 (1978) 3118, reprinted in Ref.2, p. 78.
13. M.Gyulassy, S. K. Kaufmann and L. W. Wilson, Phys. Rev. C20 (1979) 2267, reprinted in Ref.2, p. 86.
14. This trend was inaugurated by the meeting Correlations and Multiparticle Production-CAMP the Proceedings of which were edited by M. Plümer, S. Raha and R. M. Weiner, World Scientific 1990, ISBN 981-02-0331-4.
15. E. V. Shuryak, Sov. J. Nucl. Phys. 18 (1974) 667, reprinted in Ref.2, p. 32.
16. G. N. Fowler, R. M. Weiner, Physics Lett. 70 B (1977) 201.
17. M. Biyajima, Phys. Lett. B 92 (1980) 193, reprinted in Ref. 2, p. 115; R. M. Weiner, Phys. Lett. B232 (1989) 278 and B 218 (1990), reprinted in Ref.2, p. 284.
18. M. Plümer, L. V. Razumov and R. M. Weiner, Phys. Lett. B 286 (1992) 335, reprinted in Ref.2, p.344.
19. N. Neumeister et al., Phys. Lett. B 275 (1992) 186, reprinted in Ref.2, p. 332
20. I. V. Andreev, M. Plümer and R. M. Weiner, Phys. Rev. Lett. 67 (1991) 3475, reprinted in Ref.2, p. 326.
21. L. V. Razumov and R. M. Weiner, Phys. Lett. B 348 (1995) 133, reprinted in Ref.2, p. 452.
22. M. Bowler, Phys. Lett. B276 (1992) 237.
23. R. M. Weiner, Physics Reports 327 (2000) 249.