## Abstract

We study a large N

_{c}limit of a two-dimensional Yang–Mills theory coupled to bosons and fermions in the fundamental representation. Extending an approach due to Rajeev we show that the limiting theory can be described as a classical Hamiltonian system whose phase space is an infinite-dimensional super-Grassmannian. The linear approximation to the equations of motion and the constraint yields the ’t Hooft equations for the mesonic spectrum. Two other approximation schemes to the exact equations are discussed.Original language | English |
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Pages (from-to) | 2988–3010 |

Number of pages | 23 |

Journal | Journal of Mathematical Physics |

Volume | 43 |

Issue number | 6 |

DOIs | |

Publication status | Published - 1 Jun 2002 |

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