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such as Tl ions in a NaI(Tl) crystal, pass through the transparent uor substance and out through a clear window to impinge on an adjacent photocathode The typical photocathode is composed of a thin, photosensitive layer (commonly a cesium antimony alloy) on the inner surface of the end of the photomultiplier tube Here impinging photons, particularly those having wave lengths between 3000 and 6000 A, are absorbed, with a consequent emission of photoelectrons The number of photoelectrons ejected is slightly less than, but directly proportional to, the number of incident photons Such a burst of photoelectrons resulting from a single g-ray interaction in the crystal is still far too weak to be registered directly Ampli cation occurs by means of a series of electrodes, called dynodes, spaced along the length of the photomultiplier tube (see Fig 1820).

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= PI cI cH + 2 I I (11.3)

p Fq ( 1 , 2 , . . . , p ;

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Each dynode is maintained at a higher potential (usually about 50 V higher) than the preceding one The photoelectrons emitted from the photocathode are focused by an electric eld to hit the rst dynode Striking the dynode surface, they cause the secondary emission of a larger number of electrons This new burst of electrons is guided by the potential gradient to the second dynode in the series, where a still larger number of electrons are dislodged This electron-multiplying process continues at each dynode until at last the collecting anode is struck by 105 106 electrons for each original photoelectron ejected from the photocathode Thus, the size of the output pulse from the photomultiplier is directly related to the quantity of energy dissipated by the incident g-ray photon in the uor.

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simple container for the name, phone, and email strings. If the element name in startElement() is a name, person, or email element, a flag is set to indicate that any incoming data was found inside that particular element type. The next method to be called, under normal circumstances, will be the characters() method with the actual content of the element. The type of data is determined in the characters() method by checking the flags, and the string is added to the current Person object. Next, the endElement() method is called, which allows the content handler to clear the flag that indicates the type of the current element; or if it is a person element, the current Person object has been filled with all the information available so that it is stored in the Vector object named personVec for future retrieval. All of this flag setting and clearing is necessary because the SAX parser has no context; it does not keep track of anything, so the program must do it. The Person class in Listing 5.6 is capable of containing the three strings and returning them on request, or returning the string none if the requested string is not present. A collection of Person objects is stored in a Vector object. The endDocument() method of MyTextHandler uses a simple swap sort to alphabetize the names.

To present a quantitative example of the energy conversions involved in scintillation detection, we trace the results of the interaction of a single 117-MeV g ray from 60Co with a thallium-activated sodium iodide crystal [Nal(TI)]: 1 If 20% of the energy of the g ray results in exciton production in a uor crystal, and if it is assumed that 7 eV is needed to produce an exciton, then approximately 33,000 excitons could result from this g-ray photon 2 Assuming that only 10% of the excitation events result in the production of photons of visible light seen by the adjacent photocathode, this would mean that about 3300 photons would reach the photocathode 3 This number of photons striking a photocathode with a conversion ef ciency of 10% would eject approximately 330 photoelectrons 4.

i(L 1)

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