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1

International Commission on Radiation Units and Measurements., ed. Secondary electron spectra from charged particle interactions. Bethesda, Md: International Commission on Radiation Units and Measurements, 1996.

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2

M, Asnin Vladimir, Petukhov Andre G e NASA Glenn Research Center, eds. Secondary electron emission spectroscopy of diamond surfaces. [Cleveland, Ohio]: National Aeronautics and Space Administration, Glenn Research Center, 1999.

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3

A, Jensen Kenneth, Roman Robert F e United States. National Aeronautics and Space Administration. Scientific and Technical Information Division., eds. Secondary electron emission characteristics of molybdenum-masked, ion-textured OFHC copper. [Washington, D.C.]: National Aeronautics and Space Administration, Office of Management, Scientific and Technical Information Division, 1990.

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4

United States. National Aeronautics and Space Administration. Scientific and Technical Information Branch., ed. Calculation of secondary electron trajectories in multistage depressed collectors for microwave amplifiers. [Washington, DC]: National Aeronautics and Space Administration, Scientific and Technical Information Branch, 1986.

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5

United States. National Aeronautics and Space Administration. Scientific and Technical Information Branch., ed. Calculation of secondary electron trajectories in multistage depressed collectors for microwave amplifiers. [Washington, DC]: National Aeronautics and Space Administration, Scientific and Technical Information Branch, 1986.

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6

T, Mearini G., e United States. National Aeronautics and Space Administration., eds. Effects of surface treatments on secondary electron emission from CVD diamond films. [Washington, D.C: National Aeronautics and Space Administration, 1995.

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7

Nauchnyĭ sovet po probleme "Fizicheskai͡a ėlektronika" (Akademii͡a nauk SSSR) e Tashkentskiĭ politekhnicheskiĭ institut im. Abu Raĭkhana Beruni, eds. VII Simpozium po vtorichnoĭ ėlektronnoĭ, fotoėlektronnoĭ ėmissii͡am i spektroskopii poverkhnosti tverdogo tela, Tashkent, 7-9 ii͡uni͡a 1990 goda: Tezisy dokladov. Tashkent: Tashkentskiĭ politekhnicheskiĭ in-t im. Beruni, 1990.

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8

A, Jensen Kenneth, e United States. National Aeronautics and Space Administration. Scientific and Technical Information Branch., eds. Textured carbon on copper: A novel surface with extremely low secondary electron emission characteristics. [Washington, D.C.]: National Aeronautics and Space Administration, Scientific and Technical Information Branch, 1985.

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9

Novikov, I︠U︡ A. Mekhanizmy vtorichnoĭ ėlektronnoĭ ėmissii relʹefnoĭ poverkhnosti tverdogo tela. Moskva: Nauka, Fizmatlit, 1998.

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10

Kovalev, V. P. Vtorichnye ėlektrony. Moskva: Ėnergoatomizdat, 1987.

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11

Komolov, S. A. Total current spectroscopy of surfaces. Philadelphia: Gordon and Breach Science Publishers, 1992.

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12

Komolov, S. A. Integralʹnai͡a︡ vtorichno-ėlektronnai͡a︡ spektroskopii͡a︡ poverkhnosti. Leningrad: Izd-vo Leningradskogo universiteta, 1986.

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13

S, Vasilʹev I͡U︡, ed. Fizika prot͡s︡essov u granit͡s︡ razdela: Sbornik nauchnykh trudov. Leningrad: Leningradskiĭ politekhn. in-t im. M.I. Kalinina, 1985.

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14

Akkerman, A. F. Vtorichnoe ėlektronnoe izluchenie iz tverdykh tel pod deĭstviem gamma-kvantov. Moskva: Ėnergoatomizdat, 1986.

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15

A, Dadayan K., e United States. National Aeronautics and Space Administration., eds. Question on the measurement of the metal work function in an electron spectrometer by the secondary-electron emission threshold method. Washington D.C: National Aeronautics and Space Administration, 1988.

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16

Espahangizi, Kijan Malte. Experimentalsysteme, Erinnerungskulturen und die transatlantische Quantenrevolution: Die "Entdeckung der Materiewellen" und die Bell Telephone Laboratories (1925-27). Münster: LIT, 2005.

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17

Wright, A. G. Secondary emission and gain. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780199565092.003.0005.

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Resumo:
Secondary-electron emission generates gain in conventional vacuum photomultipliers with discrete dynodes. This is a cascade process involving between 6 and 20 elements. Generally, the higher the number of stages, the higher is the gain and similarly for applied voltage. Gain is dependent on the composition of the dynodes, with SbCs and activated BeO being the most common materials. There are ten different dynode types, each of which serves a particular purpose: for example, operation in high magnetic fields and high temperature. The continuous channel dynode is available as a single unit and as a multichannel structure, the microchannel plate. The quality of a dynode system is described by its single-electron response. Discrete dynodes produce a spread in output size whereas the channel devices are generally operated in saturation. Gain may be quoted as DC, G, and pulsed ‹g› and methods for measuring these parameters are given.
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18

Taglauer, E., e W. Heiland. Inelastic Particle-Surface Collisions: Proceedings of the Third International Workshop on Inelastic Ion-Surface Collisions Feldkirchen-Westerham, Fed. Rep. of Germany September 17-19 1980. Springer, 2012.

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19

Taglauer, E., e W. Heiland. Inelastic Particle-Surface Collisions: Proceedings of the Third International Workshop on Inelastic Ion-Surface Collisions Feldkirchen-Westerham, Fed. Rep. of Germany September 17-19, 1980. Springer, 2012.

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20

Pami︠a︡ti professora K.K. Aglint︠s︡eva: Sbornik trudov. Sankt-Peterburg: Agenstvo INFO OL, 2006.

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21

(Harwell), D. W. Fry, e H. Bruining. Physics and Applications of Secondary Electron Emission : Pergamon Science Series: Electronics and Waves--A Series of Monographs. Elsevier Science & Technology Books, 2016.

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22

Physics and Applications of Secondary Electron Emission : Pergamon Science Series: Electronics and Waves-a Series of Monographs. Pergamon, 2013.

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