In this paper, we construct Yang-Mills theory in the -space-time, valid up to first order in the deformation parameter , using the generalisation of Feynman’s approach. Using the -deformed Wong’s equation derived, in the Jacobi identity involving velocities and coordinates of -deformed space-time, the -deformed homogeneous Yang-Mills equations are derived. We show the compatibility between the -deformed field strength derived using the Jacobi identity and the commutators of the gauge covariant derivative, up to first order in . The -deformed field strength is covariant under gauge transformations. We then construct the Lagrangian for Yang-Mills theory in -deformed space-time and show that it is invariant under transformation and not under U(N) transformation. We also derive the expression for the force experienced by an isospin-carrying particle in the presence of Yang-Mills field in the -space-time.

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