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Theorem

Weinberg-Witten Theorem

Mathematical Physics

The Weinberg-Witten Theorem, proved by Steven Weinberg and Edward Witten, is a result of relativistic quantum field theory stating that massless particles of spin greater than one half cannot carry a Lorentz-covariant current, and massless particles of spin greater than one cannot carry a Lorentz-covariant stress-energy tensor, whether the particle is elementary or composite. Because the graviton has spin two, the theorem is usually interpreted as ruling out any composite graviton arising within an ordinary relativistic quantum field theory.

Facts
Statement
Massless particles, whether composite or elementary, with spin greater than one half cannot carry a Lorentz-covariant current, and massless particles with spin greater than one cannot carry a Lorentz-covariant stress-energy tensor. 1
Proof Year
1980 1
Classification
Statement Form
Inequality 1
Sources
1. Weinberg-Witten theorem, Wikipedia
  • Lead section
    massless particles (either composite or elementary) with spin j > 1/2 cannot carry a Lorentz-covariant current, while massless particles with spin j > 1 cannot carry a Lorentz-covariant stress-energy
  • References section
    Weinberg, Steven; Witten, Edward (1980). Limits on massless particles. Physics Letters B.
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