Classical particles are described at classical level by the coordinates q&p and the all important classical obervable called "Hamiltonian".Quantizing these 3 basic classical observables according to the second postulate of QM basically realizes the "quantization" of the system and therefore this theory is called Quantum MECHANICS.It's a quantized version of classical Hamilton mechanics,so it deals with the quantum observable called HAMILTONIAN (a densly defined self-adjoint linear operator) and with the concepts of operators for momentum,position,kinetic and potential energy,aso.
Classical fields (such as the electromagnetic field) are described by generally complex functions defined on the flat Minkowski space taking values in the algebra of either the real functions (the em field,the gluon field,the scalar boson field,the nonphysical Goldstone boson,the Higgs boson,...),complex functions (the complex scalar field) or in an exotic algebra called the Grassmann algebra (the (seminteger)spinor fields).All these fields are representations of the restricted Poincaré group,that is the group of space-time proper roto-translations.Each of these classical fields,when quantized accordingly to the second postulate,describes at quantum level a free relativistic particle with positive integer/seminteger spin.This is QFT.Then all u have to do is find appropriate interaction hamiltonians and build interactions between these particles...