Generalized Schrödinger Representation

The orthogonality condition for the eigenkets [i.e., the generalization of Equation (2.26)] is

(2.59) |

The completeness condition [i.e., the generalization of Equation (2.27)] is

(2.60) |

The standard ket is defined such that

The standard bra is the dual of the standard ket. A general state ket is written

(2.62) |

The associated wavefunction is

(2.63) |

Likewise, a general state bra is written

(2.64) |

where

(2.65) |

The probability of an observation of the system simultaneously finding the first coordinate in the range to , the second coordinate in the range to , et cetera, is

(2.66) |

Finally, the normalization condition for a physical wavefunction is

(2.67) |

The linear operators (where runs from 1 to ) are defined

These linear operators can also act on bras (provided the associated wavefunctions are square integrable) in accordance with

(2.69) |

[See Equation (2.42).] Corresponding to Equation (2.46), we can derive the commutation relations

(2.70) |

It is also clear that

(2.71) |

showing that

(2.72) |

It can be seen, by comparison with Equations (2.23)-(2.25), that the linear operators satisfy the same commutation relations with the 's and with each other that the 's do. The most general conclusion that we can draw from this coincidence of commutation relations is

(2.73) |

However, the function can be transformed away via a suitable readjustment of the phases of the basis eigenkets [32]. (See Section 2.4.) Thus, we can always construct a set of simultaneous eigenkets of for which

This is the generalized Schrödinger representation.

It follows from Equations (2.61), (2.68), and (2.74) that

(2.75) |

Thus, the standard ket in the Schrödinger representation is a simultaneous eigenket of all the momentum operators belonging to the eigenvalue zero. Note that

(2.76) |

Hence,

(2.77) |

so that

The dual of the previous equation gives