Majorana fermion

From Wikipedia, the free encyclopedia
Jump to: navigation, search

A Majorana fermion, also referred to as a Majorana particle, is a fermion that is its own antiparticle. They were hypothesised by Ettore Majorana in 1937. The term is sometimes used in opposition to a Dirac fermion, which describes fermions that are not their own antiparticles.

All of the Standard Model fermions except the neutrino behave as Dirac fermions at low energy (after electroweak symmetry breaking), but the nature of the neutrino is not settled and it may be either Dirac or Majorana. In condensed matter physics, Majorana fermions exist as quasiparticle excitations in superconductors and can be used to form Majorana bound states possessing non-abelian statistics.

Theory[edit]

The concept goes back to Majorana's 1937 suggestion[1] that neutral spin-1/2 particles can be described by a real wave equation (the Majorana equation), and would therefore be identical to their antiparticle (since the wave function of particle and antiparticle are related by complex conjugation).

The difference between Majorana fermions and Dirac fermions can be expressed mathematically in terms of the creation and annihilation operators of second quantization. The creation operator \gamma^{\dagger}_j creates a fermion in quantum state j (described by a real wave function), while the annihilation operator \gamma_j annihilates it (or, equivalently, creates the corresponding antiparticle). For a Dirac fermion the operators \gamma^{\dagger}_j and \gamma_j are distinct, while for a Majorana fermion they are identical.

Elementary particle[edit]

Since particles and antiparticles have opposite conserved charges, only an uncharged particle can have a Majorana mass[clarification needed]. All of the elementary fermions of the Standard Model have gauge charges, so they cannot have fundamental Majorana masses. However, the right-handed sterile neutrinos introduced to explain neutrino oscillation could have Majorana masses. If they do, then at low energy (after electroweak symmetry breaking), by the seesaw mechanism, the neutrino fields would naturally behave as six Majorana fields, with three expected to have very high masses (comparable to the GUT scale) and the other three expected to have very low masses (comparable to 1 eV). If right-handed neutrinos exist but do not have a Majorana mass, the neutrinos would instead behave as three Dirac fermions and their antiparticles with masses coming directly from the Higgs interaction, like the other Standard Model fermions.

The seesaw mechanism is appealing because it would naturally explain why the observed neutrino masses are so small. However, if the neutrinos are Majorana then they violate the conservation of lepton number and even B − L.

Neutrinoless double beta decay, which can be viewed as two beta decay events with the produced antineutrinos immediately annihilating with one another, is only possible if neutrinos are their own antiparticles.[2] Experiments are underway to search for this type of decay.[3]

The high energy analog of the neutrinoless double beta decay process is the production of same sign charged lepton pairs at hadron colliders;[4] it is being searched for by both the ATLAS and CMS experiments at the Large Hadron Collider. In theories based on left–right symmetry, there is a deep connection between these processes.[5] In the most accepted explanation of the smallness of neutrino mass, the seesaw mechanism, the neutrino is naturally a Majorana fermion.

Majorana fermions cannot possess intrinsic electric or magnetic moments, only toroidal moments.[6][7][8] Such minimal interaction with electromagnetic fields makes them potential candidates for cold dark matter.[9][10] The hypothetical neutralino of supersymmetric models is a Majorana fermion.

Majorana bound states[edit]

In superconducting materials, Majorana fermions can emerge as (non-fundamental) quasiparticles. This becomes possible because a quasiparticle in a superconductor is its own antiparticle. Mathematically, the superconductor imposes electron hole "symmetry" on the quasiparticle excitations, relating the creation operator \gamma(E) at energy E to the annihilation operator {\gamma^{\dagger}(-E)} at energy -E. Majorana fermions can be bound to a defect at zero energy, and then the combined objects are called Majorana bound states or Majorana zero modes.[11] This name is more appropriate than Majorana fermion (although the distinction is not always made in the literature), since the statistics of these objects is no longer fermionic. Instead, the Majorana bound states are an example of non-abelian anyons: interchanging them changes the state of the system in a way which depends only on the order in which exchange was performed. The non-abelian statistics that Majorana bound states possess allows to use them as a building block for a topological quantum computer.[12]

A quantum vortex in certain superconductors or superfluids can trap midgap states, so this is one source of Majorana bound states.[13][14][15] Shockley states at the end points of superconducting wires or line defects are an alternative, purely electrical, source.[16] An altogether different source uses the fractional quantum Hall effect as a substitute for the superconductor.[17]

Experiments in superconductivity[edit]

In 2008 Fu and Kane provided a groundbreaking development by theoretically predicting that Majorana bound states can appear at the interface between topological insulators and superconductors.[18][19] Many proposals of a similar spirit soon followed, where it was shown that Majorana bound states can appear even without topological insulator. An intense search to provide experimental evidence of Majorana bound states in superconductors[20][21] first produced some positive results in 2012.[22][23] A team from the Kavli Institute of Nanoscience at Delft University of Technology in the Netherlands reported an experiment involving indium antimonide nanowires connected to a circuit with a gold contact at one end and a slice of superconductor at the other. When exposed to a moderately strong magnetic field the apparatus showed a peak electrical conductance at zero voltage that is consistent with the formation of a pair of Majorana bound states, one at either end of the region of the nanowire in contact with the superconductor.[24]

This experiment from Delft marks a possible verification of independent theoretical proposals from two groups[25][26] predicting the solid state manifestation of Majorana bound states in semiconducting wires.

References[edit]

  1. ^ E. Majorana (1937). "Teoria simmetrica dell’elettrone e del positrone". Nuovo Cimento (in Italian) 14: 171. doi:10.1007/bf02961314. English translation. 
  2. ^ J. Schechter, J.W.F. Valle. (1982). "Neutrinoless Double beta Decay in SU(2) x U(1) Theories". Physical Review D25: 2951. Bibcode:1982PhRvD..25.2951S. doi:10.1103/PhysRevD.25.2951. 
  3. ^ W. Rodejohann (2011). "Neutrino-less Double Beta Decay and Particle Physics". International Journal of Modern Physics E20: 1833. arXiv:1106.1334. Bibcode:2011IJMPE..20.1833R. doi:10.1142/S0218301311020186. 
  4. ^ W.-Y. Keung and G. Senjanovic (1983). "Majorana Neutrinos and the Production of the Right-Handed Charged Gauge Boson". Physical Review Letters 50: 1427. Bibcode:1983PhRvL..50.1427K. doi:10.1103/PhysRevLett.50.1427. 
  5. ^ V. Tello, M. Nemevsek, F. Nesti and G. Senjanovic (2011). "Left-Right Symmetry: from LHC to Neutrinoless Double Beta Decay". Physical Review Letters 106: 151801. arXiv:1011.3522. Bibcode:2011PhRvL.106o1801T. doi:10.1103/PhysRevLett.106.151801. 
  6. ^ Kayser, Boris; Goldhaber, Alfred S. (1983), "CPT and CP properties of Majorana particles, and the consequences", Phys. Rev. D 28: 2341–2344, Bibcode:1983PhRvD..28.2341K, doi:10.1103/PhysRevD.28.2341 
  7. ^ Radescu, E. E. (1985), "On the electromagnetic properties of Majorana fermions", Phys. Rev. D 32: 1266–1268, Bibcode:1985PhRvD..32.1266R, doi:10.1103/PhysRevD.32.1266 
  8. ^ Boudjema, F.; Hamzaoui, C.; Rahal, V.; Ren, H. C. (1989), "Electromagnetic Properties of Generalized Majorana Particles", Phys. Rev. Lett. 62 (8): 852–854, Bibcode:1989PhRvL..62..852B, doi:10.1103/PhysRevLett.62.852 
  9. ^ Pospelov, Maxim; ter Veldhuis, Tonnis (2000), "Direct and indirect limits on the electro-magnetic form factors of WIMPs", Phys. Lett. B 480: 181–186, arXiv:hep-ph/0003010, Bibcode:2000PhLB..480..181P, doi:10.1016/S0370-2693(00)00358-0 
  10. ^ Ho, C. M.; Scherrer, R. J. (2013), "Anapole Dark Matter", Phys. Lett. B 722 (8): 341–346, arXiv:1211.0503, Bibcode:1989PhRvL..62..852B, doi:10.1103/PhysRevLett.62.852 
  11. ^ F. Wilczek (2009). "Majorana returns". Nature Physics 5 (9): 614. Bibcode:2009NatPh...5..614W. doi:10.1038/nphys1380. 
  12. ^ C. Nayak, S. Simon, A. Stern, M. Freedman, and S. Das Sarma (2008). "Non-Abelian anyons and topological quantum computation". Reviews of Modern Physics 80: 1083. arXiv:0707.1889. Bibcode:2008RvMP...80.1083N. doi:10.1103/RevModPhys.80.1083. 
  13. ^ N.B. Kopnin; M.M. Salomaa (1991). "Mutual friction in superfluid 3He: Effects of bound states in the vortex core". Physical Review B 44 (17): 9667. Bibcode:1991PhRvB..44.9667K. doi:10.1103/PhysRevB.44.9667. 
  14. ^ G.E. Volovik (1999). "Fermion zero modes on vortices in chiral superconductors". JETP Letters 70 (9): 609. arXiv:cond-mat/9909426. Bibcode:1999JETPL..70..609V. doi:10.1134/1.568223. 
  15. ^ N. Read; D. Green (2000). "Paired states of fermions in two dimensions with breaking of parity and time-reversal symmetries and the fractional quantum Hall effect". Physical Review B 61 (15): 10267. arXiv:cond-mat/9906453. Bibcode:2000PhRvB..6110267R. doi:10.1103/PhysRevB.61.10267. 
  16. ^ A. Yu. Kitaev (2001). "Unpaired Majorana fermions in quantum wires". Physics-Uspekhi (supplement) 44 (131): 131. arXiv:cond-mat/0010440. Bibcode:2001PhyU...44..131K. doi:10.1070/1063-7869/44/10S/S29. 
  17. ^ G. Moore; N. Read (1991). "Nonabelions in the fractional quantum Hall effect". Nuclear Physics B 360 (2–3): 362. Bibcode:1991NuPhB.360..362M. doi:10.1016/0550-3213(91)90407-O. 
  18. ^ L. Fu; C. L. Kane (2008). "Superconducting Proximity Effect and Majorana Fermions at the Surface of a Topological Insulator". Physical Review Letters 10 (9): 096407. arXiv:0707.1692. Bibcode:2008PhRvL.100i6407F. doi:10.1103/PhysRevLett.100.096407. 
  19. ^ L. Fu; C. L. Kane (2009). "Josephson current and noise at a superconductor/quantum-spin-Hall-insulator/superconductor junction". Physical Review B 79 (16): 161408. arXiv:0804.4469. Bibcode:2009PhRvB..79p1408F. doi:10.1103/PhysRevB.79.161408. 
  20. ^ J. Alicea. New directions in the pursuit of Majorana fermions in solid state systems. arXiv:1202.1293. Bibcode:2012RPPh...75g6501A. doi:10.1088/0034-4885/75/7/076501. 
  21. ^ C. W. J. Beenakker. "Search for Majorana fermions in superconductors". arXiv:1112.1950.
  22. ^ E. S. Reich (28 February 2012). "Quest for quirky quantum particles may have struck gold". Nature News. doi:10.1038/nature.2012.10124. 
  23. ^ Jonathan Amos (13 April 2012). "Majorana particle glimpsed in lab". BBC News. Retrieved 15 April 2012. 
  24. ^ V. Mourik; K. Zuo; S.M. Frolov; S.R. Plissard; E.P.A.M. Bakkers; L.P. Kouwenhoven (12 April 2012). "Signatures of Majorana fermions in hybrid superconductor-semiconductor nanowire devices". Science. arXiv:1204.2792. Bibcode:2012Sci...336.1003M. doi:10.1126/science.1222360. 
  25. ^ R. Lutchyn; J. Sau; S. Das Sarma (2010). "Majorana Fermions and a Topological Phase Transition in Semiconductor-Superconductor Heterostructures". Physical Review Letters 105 (7): 077001. arXiv:1002.4033. Bibcode:2010PhRvL.105g7001L. doi:10.1103/PhysRevLett.105.077001. 
  26. ^ Y. Oreg; G. Refael; F. von Oppen (2010). "Helical Liquids and Majorana Bound States in Quantum Wires". Physical Review Letters 105 (17): 177002. arXiv:1003.1145. Bibcode:2010PhRvL.105q7002O. doi:10.1103/PhysRevLett.105.177002. 

Further reading[edit]

  • Palash B. Pal: Dirac, Majorana and Weyl fermions, arXiv:1006.1718, 24 June / 17 July 2009 (introductory article)