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IP telephony network components such as IP phones are usually assumed to be intelligent, in the sense of being a fully-qualified Internet host, as defined in [Bra89]. Additionally, the entities are aware of their call state. Several IP telephony components are found typical set-ups.

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As the interaction with matter is dealt with only in 5, we will not describe here the way of generating squeezed states mentioned above. Instead, we will describe a less practical but more dramatic and theoretically interesting alternative way that will also help illustrate some of the points discussed earlier. As a single-cavity mode is equivalent to a harmonic oscillator, let us start this discussion by considering a harmonic oscillator of unit mass whose Hamiltonian is given by (4.84) 2 2' where pis the particle's momentum operator and qits position operator. The oscillator energy quanta annihilation operator is defined by (see Section 2.4.1)





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IP phones are the most common end systems in IP telephony systems. They are network elements that offer a direct interface for users. These equivalents to traditional telephone are available as a variety of hardware devices, often with graphical output capabilities for call-related information, or as software clients such as Windows XP Messenger or kphone.

A fwA . P =V2h q + z v'2wn:

(12.14)

(4.85)

IP telephony servers are intermediate network entities that handle application-level routing control. The servers are placed within the IP telephony network and fulfill supplementary services similar to the PSTN. Both H.323 and Session Initiation Protocol (SIP) use a conceptual server that provides functionality for end-device registration, maintenance and administrative support. User custom services are a noticeable distinction from traditional telephony systems. These services are created by (ambitious) users to fulfill specific call-control

Now what happens if the frequency of this oscillator were to change quite suddenlyiO from w to w' As we are working in the SchOdinger picture, the particle's position and momentum operators remain unchanged, but the energy quanta annihilation operator will change to

Define an abstract process that intercepts all requests for resources and checks them for compliance with authorizations.

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where g/fi is a dimensionless weak coupling and q is the momentum carried by the weak boson (the factors 1/12 and t are inserted so that we have the conventional definition of g). In contrast to the photon, the weak boson must be massive, otherwise it would have been directly produced in weak decays. Indeed, it turns out that M w - 80 GeY (see 15). In (12.14), we have been cavalier about the spin sum in the boson propagator, see (6.87). However, at the moment, we are interested in situations where q2 Ma, (e.g., /3-decay and p.-decay). Then, (12.14) reverts to (12.11) with

(4.86)

makesRequestTo Subject * *

From (4.85) and (4.86) we find that the energy quanta annihilation operator after the sudden frequency change is related to the annihilation and creation operators before by [319]

8Ma,

~ {(WI +w)b + (w' -w)b t }.

Reference monitor *

(4.87)

exists *

(12.15)

As during a sudden change of Hamiltonian, the quantum state remains unchanged [441], (4.87) is entirely equivalent to (4.79). Thus, the sudden change in the oscillator's frequency leads to squeezing [246, 319]. But how can we suddenly change the frequency of an oscillator Janszky and Yushin [319] suggested using a Franck- Condon transition. This is a molecular transition between two vibrational states belonging to different electronic states (see Secs. 14.1 and 16.4 of [262]). Now we will look into a way to achieve this frequency jump in cavity QED. In a cavity, the frequency of the oscillator corresponding to a mode can be changed by changing the size of the cavity. As the size that matters is the effective optical size, it can be changed by actually moving the cavity walls or by changing the dielectric permittivity inside the cavity [656]. But either way, the analogy between a single cavity-mode and a harmonic oscillator will no longer hold, as the change in cavity size

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