By Roy J. Glauber
A precis of the pioneering paintings of Glauber within the box of optical coherence phenomena and photon information, this booklet describes the elemental principles of recent quantum optics and photonics in an instructional sort. it truly is therefore not just meant as a reference for researchers within the box, but additionally to provide graduate scholars an perception into the elemental theories of the field.
Written by means of the Nobel Laureate himself, the options defined during this booklet have shaped the root for 3 additional Nobel Prizes in Physics in the final decade.Content:
Chapter 1 The Quantum idea of Optical Coherence (pages 1–21):
Chapter 2 Optical Coherence and Photon records (pages 23–182):
Chapter three Correlation services for Coherent Fields (pages 183–195):
Chapter four Density Operators for Coherent Fields (pages 197–216):
Chapter five Classical habit of structures of Quantum Oscillators (pages 217–220):
Chapter 6 Quantum idea of Parametric Amplification I (pages 221–262):
Chapter 7 Quantum conception of Parametric Amplification II (pages 263–286):
Chapter eight Photon information (pages 287–329):
Chapter nine Ordered Expansions in Boson Amplitude Operators (pages 331–381):
Chapter 10 Density Operators and Quasiprobability Distributions (pages 383–423):
Chapter eleven Coherence and Quantum Detection (pages 425–462):
Chapter 12 Quantum thought of Coherence (pages 463–530):
Chapter thirteen The Initiation of Superfluorescence (pages 531–536):
Chapter 14 Amplifiers, Attenuators and Schrodingers Cat (pages 537–576):
Chapter 15 The Quantum Mechanics of Trapped Wavepackets (pages 577–594):
Chapter sixteen Density Operators for Fermions (pages 595–631):
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Additional resources for Quantum Theory of Optical Coherence: Selected Papers and Lectures
Sample text
We therefore turn once again to a definition of coherence as a factorization property of the correlation functions. µ2n (x1 . . xn , xn+1 . . 59) where it is understood that the vector field Eµ (x) is independent of n. It is immediately clear, from the transformation properties of the definition, that a field coherent in one coordinate frame is equally coherent in any rotated frame. 58). 59) imply that the field is fully polarized in the direction of the vector E (x) at each point x. The formal way of seeing this is to note that (1) the intensity matrix Gµν (x, x), which we discussed earlier in general terms, reduces for a coherent field to, (1) (x, x) = Eµ∗ (x) Eν (x) .
As we shall later see, an ideal photon counter (one which has zero size and is equally sensitive to all frequencies) measures the product 2 E (−) (r ,t )E (+) (r ,t ) = E (+) (r ,t ) . That, at least, is what the detector would measure if we were capable of preparing fields with precisely fixed field strengths. But of course we are never capable of controlling the motions of the charges in our sources with very great precision. In practice all fields are radiated by sources whose behavior is subject to considerable statistical uncertainty.
A. Rebka, R. V. Pound, Nature 180, 1035 (1957). 3 E. M. Purcell, Nature 178, 1449 (1956). References 4 See, for example, P. A. M. , pp. 239–242; Oxford University Press, New York 1947. 5 M. Born, E. Wolf, Principles of Optics, Chap. X; Pergamon Press, London, 1959. An extensive bibliography is given there. 6 R. J. Glauber, Phys. Rev. Lett. 10, 84 (1963). The particular field referred to as incoherent in that note may have first-order coherence if it is monochromatic, but not second- or higher order coherence.