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Dual resonance model
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A dual resonance model is a term used in theoretical physics which refers to the early investigation (1968-1974) on strong interactions of string theory.
It was based upon the observation that the amplitudes for the s-channel scatterings matched exactly with the amplitudes for the t-channel scatterings among mesons and also the Regge trajectory. It
began with the Euler B-function model of Gabriele Veneziano in 1968 for a 4-particle amplitude which has the property
that it is explicitly s-t crossing symmetric, exhibits duality between the description in terms of
Regge poles or of resonances, and provides a closed-form
solution to non-linear finite-energy sum rules relating s- and t- channels.
The Veneziano formula was quickly generalized to an equally consistent N-particle amplitude
for which, in chronological order Yoichiro Nambu (1968), Holger Bech Nielsen (1969), and Leonard Susskind (1969),
provided a physical interpretation in terms of an infinite number of
simple harmonic oscillators describing the motion of an extended one-dimensional string, whence
string theory.
The study of dual resonance models was very popular from 1968 to 1974.

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Encyclopedia
A dual resonance model is a term used in theoretical physics which refers to the early investigation (1968-1974) on strong interactions of string theory.
It was based upon the observation that the amplitudes for the s-channel scatterings matched exactly with the amplitudes for the t-channel scatterings among mesons and also the Regge trajectory. It
began with the Euler B-function model of Gabriele Veneziano in 1968 for a 4-particle amplitude which has the property
that it is explicitly s-t crossing symmetric, exhibits duality between the description in terms of
Regge poles or of resonances, and provides a closed-form
solution to non-linear finite-energy sum rules relating s- and t- channels.
The Veneziano formula was quickly generalized to an equally consistent N-particle amplitude
for which, in chronological order Yoichiro Nambu (1968), Holger Bech Nielsen (1969), and Leonard Susskind (1969),
provided a physical interpretation in terms of an infinite number of
simple harmonic oscillators describing the motion of an extended one-dimensional string, whence
string theory.
The study of dual resonance models was very popular from 1968 to 1974. It
fell rapidly out of favor around 1974 mainly because it was superseded
by quantum chromodynamics as the accepted theory of strong interactions.
See also
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