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Perl read, write and other functions (along with a large number of functions for manipulating directory entries e.g. changing a file s access permissions). Perl programs work with encapsulated versions of stdio FILE* file streams. In Perl, these are referenced by filehandles . Conventionally, Perl filehandles are given names composed entirely of capital letters; these names are in their own namespace, separate from the namespaces used for scalars, lists and hashes. (Filehandles do not have a type identifier symbol comparable to the $ of scalars, @ of lists, or % of hashes.) An input stream can be opened from a file as follows:

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Many different combinations of interferometers and gratings can be used to design a single mode laser cavity. A rigorous analysis of these cavities involves a complicated coupled element approach [6, 7] that usually can only be solved numerically. However, in most situations a reasonable approximation can be found simply by multiplying the filtering effect of all the different elements together and assuming it to be the net transmission function of the laser cavity. This can then be compared with the gain available to determine the spectral mode structure of the laser. For example, consider the combination Fabry Perot resonator with gain and diffraction grating laser in Figure 8.15. The grating has a filter function given by Equation (8.17).

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Typically, if the power in a single mode is more than 30 dB or, in other words, 1000 times greater than the optical power at other frequencies, the laser is considered to be single mode [7]. Suppression of side modes in diode lasers can be achieved by frequency filtering the feedback that the resonator provides to the gain medium. Put simply, unwanted frequencies are prohibited from lasing by increasing their cavity loss. However, this loss must be frequency selective as it is undesirable to increase the loss for the preferred single mode. Since unwanted side modes may be less than 1 GHz from the lasing mode, this is not a simple exercise. Mechanisms for frequency filtering the feedback in diode lasers can be categorized into two main classes that will be addressed here; interferometric feedback and grating feedback [6-9]. Specific examples from both classes will be discussed, even though today, it is only diffraction grating-based schemes that have any significant commercial application. Alternatively, a diode laser can also be forced into a single mode by reducing the length of the Fabry Perot cavity so that the mode spacing is greater than the width of the gain curve (see Equation (8.5)). But there are technical difficulties in fabricating these high gain-low loss devices [7] because of the very small cavity lengths ( 10 m) required to achieve mode spacings of the order of THz.

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Semiconductor lasers with phase-conjugate feedback (PCF) from a phase conjugating mirror (PCM) have received considerable attention because they have a number of positive properties Due to the reversal of the light front in the PCM, the reflected wave travels back along the same path as the incident wave, meaning that alignment of the mirror is less of an issue Furthermore, perturbations on the way to the PCM are undone on the way back, resulting in potentially more stable operation The main technical difficulty is realizing a PCM Phase conjugation can be achieved by a number of nonlinear optical processes, including stimulated Brillouin scattering, backward stimulated Raman scattering and three-wave down conversion [17] Probably the most common process is degenerate four-wave mixing in which three input waves mix to produce a fourth output wave.

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Two of the input waves are counter-propagating pump waves of a given frequency, for example, from additional semiconductor lasers The incident wave is the third wave, that enters the medium at any angle to the pump waves and is coupled to the pump waves through a third-order susceptibility 3 This results in a fourth wave, which is phase-conjugated to the incident wave, see 3 for more introductory information Phase conjugate feedback may produce a highly focused beam [17], which is of considerable advantage when stable output is desired The main application is mode locking [20] and phase locking, where PCF has been shown to reduce the laser noise considerably [1, 21, 61] However, many other dynamical regimes have been identified, including periodic and quasiperiodic output, as well as chaotic dynamics, see, for example, [1, 17, 21, 39].

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