Chapter 3
Propagators and Second Quantization
The Schrödinger equation for an electron or for N noninteracting electrons is
with units such that Planck’s constant is 2π and the electron mass is 1, and with ξ = (, ζ) being a combined space-spin variable. The wave function or Schrödinger amplitude (ξ, t) can be expressed in an orthonormal basis {us(ξ)} as
giving the Schrödinger equation in discrete form
The notation
has been employed.
Let x be a unitary transformation to energy eigenstates: x†x = xx† = 1, x†hx = ∊ (diagonal). A formal solution to Eq. (3.3) may be written as
The system may be prepared such that |ar(t′)|2 = 1, and |as(t′)|2 = 0 for s ≠ r. Then the quantity
is the probability ...
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