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Series in optics and optoelectronics

Single-photon wave packet correlations

Published May 13, 2014• 0 citations
Publisher
DOI
10.1201/b16917-21

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In Sec. 15.4 we introduced polychromatic single-photon states in Hilbert space [Eq. (15.80)], |Φ〉 = L− 32 ∑ i φi|Pi〉, i = (q, s), (16.1) by linear superposition of monochromatic plane (P) one-photon states |Pi〉 ≡ |1i〉 = aˆ†i |0〉. (16.2) In the one-photon subspace the |Pi〉 states satisfy the orthonormality, 〈Pj |Pi〉 = δij , (16.3) and completeness ∑ i |Pi〉〈Pi| = 1 (16.4) relations. Instead of taking the |Pi〉’s as a basis set for the expansion of |Φ〉, one may use different sets of one-photon wave-packet states, as we now shall see. The generalization to wave-packet expansion is of importance from a fundamental point of view, and in this chapter we shall realize the usefulness of such an expansion for single-photon correlation studies.

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In Sec. 15.4 we introduced polychromatic single-photon states in Hilbert space [Eq. (15.80)], |Φ〉 = L− 32 ∑ i φi|Pi〉, i = (q, s), (16.1) by linear superposition of monochromatic plane (P) one-photon states |Pi〉 ≡ |1i〉 = aˆ†i |0〉. (16.2) In the one-photon subspace the |Pi〉 states satisfy the orthonormality, 〈Pj |Pi〉 = δij , (16.3) and completeness ∑ i |Pi〉〈Pi| = 1 (16.4) relations. Instead of taking the |Pi〉’s as a basis set for the expansion of |Φ〉, one may use different sets of one-photon wave-packet states, as we now shall see. The generalization to wave-packet expansion is of importance from a fundamental point of view, and in this chapter we shall realize the usefulness of such an expansion for single-photon correlation studies.