Hamiltonians -- A Tid Bit About These

When one is referring to the operational-based Hamiltonian, one is here talking about the momentum of a superstring.  Such a Hamiltonian operation here specifically refers to the permittivity of a given arbitrary superstring.  The discrete impedance of a substringular unit is physically localized at the directly corresponding Fadeev-Popov-Trace that corelates to the said given superstring that may be arbitrarily conisdered in an individual case.  Substringular permittivity may be viewed of as being "into the board" in the general direction of the Lagrangian-based directoral-basis that is being considered here in any individual arbitrary case that may be extrapolated by a format relating to a Sterling approximation.  However, the substringular impedance may be viewed of as being "out of the board" in the general direction that is in the reverse of the Lagrangian-based directoral-basis that is being considered here in any individual arbitrary case that may be extrapolated by a format relating to a Sterling approximation.  So, if a superstring is moving through a unitary Lagrangian over a metrical-based time-wise format, then, the permittivity of the superstring -- that here acts as the Hamiltonian operation of the said given arbitrary superstring -- is directorally in the path of the motion of the said superstring when taken through the trajectory of the projection of the directly corresponding said unitary Lagrangian.  So, the inverse of the directly related Hamiltonian operation -- the equal and opposite response of the corelative Hamiltonian operation -- is the impedance of the given arbitrary superstring.  Such impedance acts in the opposite directoral path of the direclty corresponding permittivity, and thus, discrete substringular impedance may be mapped in the opposite holomorphicity of the path of the direclty correponding substringular permittivity.