  An eigenvalue equation representing symmetric (dual) quantum equation is
introduced. The particle is described by two scalar wavefunctions, and two
vector wavefunctions. The eigenfunction is found to satisfy the quantum
Telegraph equation keeping the form of the particle fixed but decaying its
amplitude. An analogy with Maxwellian equations is presented. Massive
electromagnetic field will satisfy a quantum Telegraph equation instead of a
pure wave equation. This equation resembles the motion of the electromagnetic
field in a conducting medium. With a particular setting of the scalar and
vector wavefunctions, the dual quantum equations are found to yield the
quantized Maxwell's equations. The total energy of the particle is related to
the phase velocity ($v_p$) of the wave representing it by $E=p\,|v_p|$\,, where
$p$ is the matter wave momentum. A particular solution which describes the
process under which the particle undergoes a creation and annihilation is
derived. The force acting on the moving particle is expressed in a dual
Lorentz-like form. If the particle moves like a fluid, a dissipative (drag)
quantum force will arise.
