We study the three-quark light-cone amplitudes of the proton including quarks’ transverse momenta. We classify these amplitudes using a newly-developed method in which light-cone wave functions are constructed from a class of light-cone matrix elements. We derive the constraints on the amplitudes from parity and time-reversal symmetries. We use the amplitudes to calculate the physical observables which vanish when the quark orbital angular momentum is absent. These include transverse-momentum dependent parton distributions , , $\delta q(x, k_\perp)\delta q_L(x,k_\perp)g_T(x)h_L(x)E(x, \xi=0, Q^2)F_2(Q^2)$.

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