In a multi-particle system, multiple orthonormal forms of this quantity are multiplied to compute the Hartree product. For a particle described by the Klein-Gordon equation, this quantity's d'Alembertian is equal to negative m squared c squared divided by h-bar squared times, this quantity. This quantity is antisymmetric under fermion interchange. The Hamiltonian operator on this function is proportional to this function's time derivative. Non-square-integrable examples of this function are non-normalizable and thus non-physical. The square of 
In a multi-particle system, multiple orthonormal forms of this quantity are multiplied to compute the Hartree product. For a particle described by the Klein-Gordon equation, this quantity's d'Alembertian is equal to negative m squared c squared divided by h-bar squared times, this quantity. This quantity is antisymmetric under fermion interchange. The Hamiltonian operator on this function is proportional to this function's time derivative. Non-square-integrable examples of this function are non-normalizable and thus non-physical. The square of the magnitude of this function represents a probability density for the location of the particles it describes. For 10 points, name this function which is the solution of the Schrodinger equation and which describes the state of a quantum particle.
In a multi-particle system, multiple orthonormal forms of this quantity are multiplied to compute the Hartree product.
wavefunction