Where and are solenoidal and irrotational projection operators satisfying 1 } } and and are the non-conservative and conservative parts of the body force.
22.
The basic idea was already published by John Cramer in his transactional interpretation except the beables that exist between the von Neumann strong projection operator measurements.
23.
The above projection operator, when applied to any spinor, will give that part of the spinor that corresponds to the electron state we seek.
24.
Another important part of the theorem is that measurement is performed by applying a generalized projection operator " P " to the state ?.
25.
The coupling of the charged weak interaction to fermions is proportional to the first projection operator, which is responsible for this interaction's parity symmetry violation.
26.
The projection operator formalism later found wide application and is now known as the Zwanzig-Mori formalism ( also named after Hazime Mori, who published similar results in 1965 ).
27.
By means of a projection operator the dynamics is split into a slow, collective part ( " relevant part " ) and a rapidly fluctuating " irrelevant " part.
28.
He developed the projection operator formalism, which made it possible to derive irreversible transport equations ( such as the Boltzmann equation and other master equations ) from reversible microscopic quantum mechanical dynamic equations.
29.
Consequently, we can make a projection operator from it that projects out the sub-algebra of the Dirac algebra that has spin oriented in the ( a, b, c ) direction:
30.
A physical proposition \, P about the system at a fixed time can be represented by a projection operator \ hat { P } on \ mathcal { H } ( See quantum logic ).
