Geometric quantum mechanics

The manifold of pure quantum states can be regarded as a complex projective space endowed with the unitary-invariant Fubini-Study metric. According to the principles of geometric quantum mechanics, the physical characteristic s of a given quantum system can be represented by geometrical features that are preferentially identified in this complex manifold. Here we construct a number of examples of such features as they arise in the state spaces for spin 1/2, spin 1, spin 3/2 and spin 2 systems, and for pairs of spin 1/2 s ystems. A study is then undertaken on the geometry of entangled states. A l ocally invariant measure is assigned to the degree of entanglement of a giv en state for a general multi-particle system, and the properties of this me asure are analysed for the entangled states of a pair of spin 1/2 particles . With the specification of a quantum Hamiltonian, the resulting Schrodinge r trajectories induce an isometry of the Fubini-Study manifold, and hence a lso an isometry of each of the energy surfaces generated by level values of the expectation of the Hamiltonian. For a generic quantum evolution, the c orresponding Killing trajectory is quasiergodic on a toroidal subspace of t he energy surface through the initial state. When a dynamical trajectory is lifted orthogonally to Hilbert space, it induces a geometric phase shift o n the wave function. The uncertainty of an observable in a given state is t he length of the gradient vector of the level surface of the expectation of the observable in that state, a fact that allows us to calculate higher or der corrections to the Heisenberg relations. A general mixed state is deter mined by a probability density function on the state space, for which the a ssociated first moment is the density matrix. The advantage of a general st ate is in its applicability in various attempts to go beyond the standard q uantum theory, some of which admit a natural phase-space characterisation. (C) 2001 Elsevier Science B.V. All rights reserved.