Exotic atom

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An exotic atom is an otherwise normal atom in which one or more sub-atomic particles have been replaced by other particles of the same charge. For example, electrons may be replaced by other negatively charged particles such as muons (muonic atoms) or pions (pionic atoms).[1][2] Because these substitute particles are usually unstable, exotic atoms typically have very short lifetimes.

Muonic atoms[edit]

In a muonic atom (also called a mu-mesic atom),[3] an electron is replaced by a muon, which, like the electron, is a lepton. Since leptons are only sensitive to weak, electromagnetic and gravitational forces, muonic atoms are governed to very high precision by the electromagnetic interaction. The description of these atoms is not complicated by strong forces between the lepton and the nucleus.

Since a muon is more massive than an electron, the Bohr orbits are closer to the nucleus in a muonic atom than in an ordinary atom, and corrections due to quantum electrodynamics are more important. Study of muonic atoms' energy levels as well as transition rates from excited states to the ground state therefore provide experimental tests of quantum electrodynamics.

Muon-catalyzed fusion is a technical application of muonic atoms.

Hadronic atoms[edit]

A hadronic atom is an atom in which one or more of the orbital electrons is replaced by a charged hadron.[4] Possible hadrons include mesons such as the pion or kaon, yielding a mesonic atom; antiprotons, yielding an antiprotonic atom; and the Σ particle, yielding a Σ or sigmaonic atom.[5][6][7]

Unlike leptons, hadrons can interact via the strong force, so the energy levels of hadronic atoms are influenced by nuclear forces between the nucleus and the hadron. Since the strong force is a short-range interaction, these effects are strongest if the atomic orbital involved is close to the nucleus, when the energy levels involved may broaden or disappear because of the absorption of the hadron by the nucleus.[2][6] Hadronic atoms, such as pionic hydrogen and kaonic hydrogen, thus provide experimental probes of the theory of strong interactions, quantum chromodynamics.[8]

Onium[edit]

An onium (plural: onia[citation needed]) is the bound state of a particle and its antiparticle. The classic onium is positronium, which consists of an electron and a positron bound together as a long-lived metastable state. Positronium has been studied since the 1950s to understand bound states in quantum field theory. A recent development called non-relativistic quantum electrodynamics (NRQED) used this system as a proving ground.

Pionium, a bound state of two oppositely-charged pions, is useful for exploring the strong interaction. This should also be true of protonium. The true analogs of positronium in the theory of strong interactions, however, are not exotic atoms but certain mesons, the quarkonium states, which are made of a heavy quark such as the charm or bottom quark and its antiquark. (Top quarks are so heavy that they decay through the weak force before they can form bound states.) Exploration of these states through non-relativistic quantum chromodynamics (NRQCD) and lattice QCD are increasingly important tests of quantum chromodynamics.

Muonium, despite its name, is not an onium containing a muon and an antimuon, because IUPAC assigned that name to the system of an antimuon bound with an electron. However, the production of a muon/antimuon bound state, which is an onium, has been theorized.[9]

Understanding bound states of hadrons such as pionium and protonium is also important in order to clarify notions related to exotic hadrons such as mesonic molecules and pentaquark states.

Hypernuclear atoms[edit]

Atoms may be composed of electrons orbiting a hypernucleus that includes strange particles called hyperons. Such hypernuclear atoms are generally studied for their nuclear behaviour, falling into the realm of nuclear physics rather than atomic physics.

Quasiparticle atoms[edit]

In condensed matter systems, specifically in some semiconductors, there are states called excitons which are bound states of an electron and an electron hole.

See also[edit]

References[edit]

  1. ^ §1.8, Constituents of Matter: Atoms, Molecules, Nuclei and Particles, Ludwig Bergmann, Clemens Schaefer, and Wilhelm Raith, Berlin: Walter de Gruyter, 1997, ISBN 3-11-013990-1.
  2. ^ a b Exotic atoms, AccessScience, McGraw-Hill. Accessed on line September 26, 2007.
  3. ^ Dr. Richard Feynman's Douglas Robb Memorial Lectures
  4. ^ p. 3, Fundamentals in Hadronic Atom Theory, A. Deloff, River Edge, New Jersey: World Scientific, 2003. ISBN 981-238-371-9.
  5. ^ p. 8, §16.4, §16.5, Deloff.
  6. ^ a b The strange world of the exotic atom, Roger Barrett, Daphne Jackson and Habatwa Mweene, New Scientist, August 4, 1990. Accessed on line September 26, 2007.
  7. ^ p. 180, Quantum Mechanics, B. K. Agarwal and Hari Prakash, New Delhi: Prentice-Hall of India Private Ltd., 1997. ISBN 81-203-1007-1.
  8. ^ Exotic atoms cast light on fundamental questions, CERN Courier, November 1, 2006. Accessed on line September 26, 2007.
  9. ^ [1] DOE/SLAC National Accelerator Laboratory (2009, June 4). Theorists Reveal Path To True Muonium – Never-seen Atom. ScienceDaily. Retrieved June 7, 2009.