Description: Define the bra of a
vector used by Dirac notation. Based on definition
of bra in [Prugovecki] p. 186 (p.
180 in 1971 edition). In Dirac
bra-ket notation,   is a complex number equal to the inner
product   . But
physicists like to talk about the
individual components 
and  , called bra and ket
respectively. In order for their properties to make sense formally, we
define the ket
 as the vector itself, and the bra
 as a functional from to . We represent the
Dirac notation   by  bra     ; see
bravalval 10148. The reversal of the inner product arguments
not only makes
the bra-ket behavior consistent with physics literature (see comments
under ax-his3 9227) but is also required in order for the
associative law
kbass2 10330 to work.
Our definition of bra and the associated outer product df-kb 10057 differs
from, but is equivalent to, a common approach in the literature that
makes use of mappings to a dual space. Our approach eliminates the need
to have a parallel development of this dual space and instead keeps
everything in Hilbert space.
For an extensive discussion about how our notation maps to the
bra-ket
notation in physics textbooks, see
http://us.metamath.org/mpegif/mmnotes.txt,
under the
17-May-2006 entry. |