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Recent advances in cooling and in optical mirror coating technologies have allowed the realization of a long-dreamed goal in cavity QED: to build a laser with a gain medium consisting of a single atom trapped inside a high-Q cavity, where it interacts with the single-mode radiation field in the strong-coupling regime [436] In ordinary lasers, masers, and even in the micromaser, the field is built up in the cavity by the contributions of many individual atoms In lasers, these atoms are usually all inside the cavity at the same time But the distances between atoms are large enough for them to interact with the field independently rather than cooperatively as in superradiance [255] This lack of cooperativity leads to the same sort of field buildup that is achieved in the micromaser, where atoms go through the cavity one at a time [214, 417].

The differences between the highly quantum fields produced in the micro maser and the quasiclassical fields generated in ordinary lasers are due primarily to the strong coupling achieved in the micromaser rather than to there being one atom at a time in the cavity The one-and-the-same atom laser had been studied extensively [234, 299, 328, 355, 412, 443, 444, 459, 487, 488] before its realization in Jeff Kimble's quantum optics group at Caltech [436] There was even a detailed experimental proposal of an ion-trap laser in 1997 by Meyer, Briegel, and Walther from the Max-Planck Institute for Quantum Optics [444] In the long ran, however, neutral atom trapping using a FORT (far-off resonance trap) [442] proved to be a more workable technology for intracavity trapping.

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You can build your test project from the menu using the Unit Test Wizard This process builds the tests for existing code similar to the preceding process, but with the steps in a slightly different order To build a test project based on existing code using the Unit Test Wizard: 1 Select Test | New Test from the main menu bar The Add New Test dialog is displayed, as shown in Figure 614

As the atom is held inside the cavity for a long time compared to the lifetime of its energy levels and of a photon in the cavity mode, the incoherent decay dynamics cannot be neglected during its interaction with the field So unlike that of the micromaser, the theory of the one-and-the-same atom laser must be solved numerically The usual approach is to write down the master equation and then solve it.

in a truncated Fock space In the theoretical analysis of their experiment [65,437], McKeever, Boca, Boozer, Buck, and Kimble used the MATLAB 30 quantum-optics toolbox developed by Sze M Tan [589], and in some cases the truncation of Fock space was done at two photons For more details on the numerics, see [534, 535, 589] The experiment [436] showed that such a cavity QED laser has indeed no ordinary laser threshold There is, however, a second threshold, due to the Stark shifting of the upper lasing level out of resonance with the cavity as the pump strength increases beyond a certain value Both the photon number and the Fano parameter, as functions of the pump intensity, exhibit a second threshold It is interesting to compare this with the result of the ion-trap laser simulations, as the latter showed both the ordinary laser threshold and the second threshold [444].

Figure 614 Use the Add New Test dialog to select the type of test to be created This chapter describes only unit tests 2 Select the Unit Test Wizard template and click OK If you select the Create a new Visual Basic test project option from the Add to Test Project drop-down list, the New Test Project dialog is displayed (see Figure 613) If you previously created a unit test project, you can add to it by selecting the project from the Add to Test Project drop-down list You are not asked for the name of the test project Instead, the

We can understand why this happens by looking at how the time scales compare in the two cases In the ion-trap laser proposal [444], the best realistic values given the constraint of finding a suitable ion for trapping, were g ~ 148 MHz, t-;a~ ~ 1 MHz, and 'I'll ~ 106 MHz Notice how the atomic decay rate 'I'll is dangerously close to the Rabi frequency In the one-and-the-same atom laser experiment [436], however, g ~ 16 MHz, t-;a~ ~ 42 MHz, and 'I'll ~ 26 MHz So whereas in the ion-trap laser proposal the saturation photon number was no ~ 02 and the critical atom number No ~ 009, in the Caltech experiment no ~ 001 and No ~ 008 Another important experimental result is the demonstration of sub-Poissonian photon statistics.

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