  In the non-Markovian regime, the bath has the memory about the past behavior
of the open quantum system. This memory has slowly-decaying power-law tails.
Such a long-range character of the memory complicates the description of the
resulting real-time dynamics on large time scales. In a numerical simulation,
this problem manifests itself in a `revival', a spurious reflected signal which
appears after a finite time thus invalidating the simulation. In the present
work, we approach this problem and develop a numerical discretization of the
bath without revivals. We find that a crucial role is played by the
singularities of the bath spectral density (e.g. edges of bands): the memory
about the (spectral) behaviour of the open system in the remote past is
completely averaged out (forgotten), except an increasingly small vicinity of
these singular frequencies. Therefore, we introduce the concept of memory
channel, to denote such an irreversible information loss process around a
particular singular frequency. On a technical side, we begin the treatment by
noting that with respect to the memory loss, the quantum field of the bath
should be divided into the following two different parts: the observable and
the virtual quanta. Information about the former is never lost: they contribute
to the trace over the bath degrees of freedom. The only way to avoid the
revival from the observable quanta is to calculate their dynamics exactly. We
do this by employing a stochastic sampling of the Husimi function of the bath.
The other part, the virtual quanta, are always annihilated after a certain
delay time. We construct a dedicated quantum representation for the virtual
states by assigning amplitudes to the delay times before annihilation. It is in
this representation we rigorously define the concept of memory channels.
