The structure of the history phase space G of a covariant field system
and its history group (in the sense of Isham and Linden) is analyzed on an
example of a bosonic string. The history space G includes the time map
T from the spacetime manifold (the two-sheet) Y to a
one-dimensional time manifold T as one of its configuration variables. A
canonical history action is posited on G such that its restriction to
the configuration history space yields the familiar Polyakov action. The
standard Dirac-ADM action is shown to be identical with the canonical history
action, the only difference being that the underlying action is expressed in
two different coordinate charts on G. The canonical history action
encompasses all individual Dirac-ADM actions corresponding to different choices
T of foliating Y. The history Poisson brackets of spacetime fields
on G induce the ordinary Poisson brackets of spatial fields in the
instantaneous phase space G0 of the Dirac-ADM formalism. The
canonical history action is manifestly invariant both under spacetime
diffeomorphisms DiffY and temporal diffeomorphisms DiffT. Both of
these diffeomorphisms are explicitly represented by symplectomorphisms on the
history phase space G. The resulting classical history phase space
formalism is offered as a starting point for projection operator quantization
and consistent histories interpretation of the bosonic string model.Comment: 45 pages, no figure