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Employee List: This list makes it easy for you to keep track of employee contact information, plus information about employees salaries, taxes, and bene ts ( 21 is devoted to setting up and managing employee data) Other Names List: If you need to keep a list of names that do not fall neatly into one of the other people categories (Employees, Vendors, or Customers), you can keep it here For example, perhaps you maintain a list of technical experts you call for quotes to include in articles you write Customer & Vendor Pro le Lists: These lists allow you to maintain databases of sales representatives, customer types, vendor types, job types, messages to send to customers, sales terms you offer customers, shipping information, payment methods, and information about any vehicles used or owned by your company.

Radio transmitters generate electromagnetic radiation that, to a good approximation, can be regarded as coherent waves. This coherence allows us to modulate the wave's amplitude (AM) or its frequency (FM) to carry sound to far-away radio receivers. Before the invention of the laser, there was no such coherent source for electromagnetic radiation in the optical region of the spectrum. The laser is often regarded as a direct by-product of the modem ideas of the "quantum revolution." But it is also the natural generalization of the idea of radio transmitters to optical frequencies. This chapter starts by showing the similarities between lasers and radio transmitters. Then we move on to discuss how the nonnegligible quantum nature of lasers brings about a number of phenomena that have no

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counterparts in classical radio transmitters. This departure from well-known classical behavior becomes even more dramatic as we go from traditional lasers and masers to their cavity QED cousins: the micromaser and the micro laser. In the next section we introduce the basic idea behind the maser and the laser: amplification by stimulated emission of radiation (ASER).1 Unlike in radio transmitters, noise is usually very important in lasers. So in Section 8.2 we have an interlude where we learn how to add noise to the usual deterministic differential equations of motion encountered in classical physics. In Section 8.3 we show the effect of spontaneous emission noise and introduce the idea of laser threshold. In Section 8.4 we begin our quantum description of ASERs by examining another simple model of a laser that allows us to calculate the quantum state of light generated in a laser. Then we go directly to the other extreme, the quantum regime, and examine a truly microscopic device: the micromaser. The micromaser is the closest experimental realization of the fundamental interaction between a two-level atom and a single mode of the quantized radiation field described by the celebrated Jaynes-Cummings model presented in 6. In Section 8.6 we sketch the connection between this simple microscopic device and complicated macroscopic lasers and masers, showing how dissipation can transform an optical micro maser into an ordinary laser. On the way we see how strong coupling can lead to the disappearance of the laser threshold. Then in the final section of the chapter we discuss briefly a recent breakthrough in cavity QED: the realization of the one-and-the-same atom laser in the strong-coupling regime.

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In the 1950s there was a lot of excitement about radar and, on the basic research side, about spectroscopy. Radar was crucial for the allied war effort. Some say that it was radar which in fact won the war for the allies. Spectroscopy helped to bring us quantum mechanics and important advances in chemistry. Developments in both radar and spectroscopy called for an oscillator for microwaves and beyond. Radar uses radio waves to locate distant objects, as a bat uses sound to find its way through the night. The resolution with which it can locate things depends on the wavelength of these waves. The shorter the wavelength, the higher the resolution, allowing it to locate smaller objects. 2 In spectroscopy, the resolution with which one can resolve an atomic absorption line, say, depends on the bandwidth of the radiation used to probe the line. For atomic resonances in the visible region, one had to use a light bulb or some other thermal source of light. To get as close to a monochromatic signal as possible, the light was fed through a series offrequency filters. The problem

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