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The Glauber-Sudarshan quasiprobability distribution seen in Section 4.1 is not the only one used in quantum optics. Another example of quasiprobability distribution is the Wigner function [644], which is associated with symmetrical ordering rather than normal ordering. It introduces the idea of phase-space in quantum mechanics (for a phase space approach to quantum optics, see Schleich's book [537]). Some of the advantages of the Wigner function are that unlike P, it is not singular for coherent states and for physical quantum states, and that it makes important features such as quantum interference easy to identify visually.

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Implied contracts are contracts that, as their name suggests, are implied from the conduct of the parties and other circumstances surrounding the transaction. For example, suppose there is a milkman that always delivers milk to your house. You have never actually met him, but you take the milk in the house and drink it every week. If the court were to look for evidence of an offer and an acceptance, it might not nd any. But based on the conduct of the parties, it is likely that an implied contract exists. Implied contracts are based on the legal doctrines of promissory estoppel or unjust enrichment. Under these doctrines, a party may be disallowed (that is, estopped) from denying the existence of a contract. This happens when it is

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Biotechnology Strategy Council (BT Strategy Council). This council, launched in 2002, is composed of the Prime Minister, seven cabinet mem bers, and a dozen representatives from academia and industry. The BT Strategy Council is tasked with formulating a national strategy for biotech that cuts across all ministries and makes the best use of academia in bring ing biotech products to the international market.

In the 1990s, the Wigner function of a light beam was determined experimentally for the first time using the technique of quantum tomography. For an excellent account of this as well as a list of some of the key references in that period, see [399]. Unfortunately, this technique does not apply to quantum fields in high-Q microwave cavities, as those fields cannot be taken out of the cavity and as there are no photon detectors for those frequencies. For this typical cavity QED scenario, a different technique was proposed in which atoms are used to probe the field: atomic homodyne detection [168, 170, 652].

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Outside the former Iron Curtain, interest in moving mirrors and time-dependent boundary conditions was sparked by the possibility of particle generation due to the expansion of the universe [57, 475]. The first known paper on the problem of the quantum radiation field in a cavity with moving walls was published by Gerald T. Moore in 1970 [457]. There are, however, older papers on the classical theory of time-dependent boundary conditions that were published in the former Soviet Union. For a comprehensive review of the moving mirrors problem (also known as the dynamic Casimir effect), see [161]. More recently, Law found an effective Hamiltonian that explicitly describes the physical processes that happen during a change of cavity size [394, 395]. Also of interest are a recent calculation of the decoherence produced by moving boundaries [141] and the proposal by Schwinger [546-550] to explain the phenomenon

simply unfair, in the court s view, to allow a party to wiggle out of any obligations based on its overall conduct in inducing the other party to perform.

of sonoluminescence l6 in terms of the dynamic Casimir effect, but there are alternative theories, such as [292] . For more on the use of squeezed states for optical communications, see [558, 657, 661. 662]. Although they only became popular in the 1960s with the work of Roy Glauber. coherent states were actually introduced in 1926 by SchrOdinger [540]. Squeezed states were first introduced by Kennard in 1927 [351], long before Horace Yuen's seminal paper on two-photon coherent states of the radiation field [660]. For a historical account of these discoveries. see [465].

4.1 Show that acannot have any left eigenstate. Hint: Find a recursive relation for the Fock state components of such a hyp('thetical eigenstate. Then show that the vacuum component must vanish so that all the other components will also vanish. 4.2 Derive the explicit expression (4.20) for the normalized coherent state In} directly from (4.5). Hint: Multiply (4.5) by a Fock state (nl from the left and work out a recursive relation for {nla}. 4.3 Show that R( 0) = exp (iOa t a). Hint: Start with an infinitesimal rotation 69. 4.4 Show that if f)t f) =

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