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photons

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Image
Published: 01 January 1986
Fig. 1 Absorption of a photon. (a) Ground state. (b) Transition. (c) Excited state More
Image
Published: 31 October 2011
Fig. 1 Fiber optic cable connector. Courtesy of IPG Photonics More
Image
Published: 01 August 2018
Fig. 17 Calculated mass absorption coefficient for uranium as a function of photon energy (solid line) and contributions of various atomic processes (dashed lines). Rayleigh scattering is the difference between total scattering and Compton scattering. More
Image
Published: 15 December 2019
Fig. 6 XPS emission process for a model atom. An incoming photon causes the ejection of a photoelectron (a). The relaxation process results in an emission process of an Auger electron (b) KL 23 L 23 . The final arrangement results in a two-electron vacancy at the L 2,3 or 2p level ( Ref 8 ). More
Image
Published: 15 December 2019
Fig. 9 XPS machine (Kratos AXIS Ultra) with a fracture stage, ultraviolet photon source, Auger attachment, and reaction cell (at the back, not shown). Courtesy of Marshall Space Flight Center More
Image
Published: 15 June 2020
Fig. 5 (a) Stimulated absorption of a photon. (b) Spontaneous emission or the nonradiative transition of energy in a two-level system. (c) Stimulated emission of a photon. Transitions are shown to occur between lower ( E 1 ) and upper ( E 2 ) energy levels, where each filled-in circle More
Image
Published: 15 June 2020
Fig. 14 Photonic Doppler velocimetry (PDV). (a) Experimental setup for the PDV technique used. (b) Relative velocity vs. time for an unsuccessful bond. (c) Relative velocity vs. time for a successful bond. Source: Ref 82 More
Image
Published: 15 December 2019
Fig. 7 (a) MIKROGAP detector with sample output. (b) Hybrid photon detector with example output (reprinted from Ref 13 with permission of Wiley. Copyright © International Union of Crystallography). (c) Micro x-ray diffraction Rigaku image plate system with simulated diffraction reflections More
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Published: 15 December 2019
Fig. 26 Generation of Auger electron and x-ray photon by inner shell ionization of an atom and subsequent electron transitions More
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Published: 15 December 2019
Fig. 1 Schematic of energy-level diagrams showing (a) x-ray photon emission and (b) Auger electron emission. Courtesy of Physical Electronics, USA More
Series: ASM Handbook
Volume: 6A
Publisher: ASM International
Published: 31 October 2011
DOI: 10.31399/asm.hb.v06a.a0005630
EISBN: 978-1-62708-174-0
.... Courtesy of IPG Photonics An optical fiber propagates light down its length through the principle of total internal reflection. The numerical aperture (NA) is the solid angle over which the fiber optic can accept light. A fiber optic input NA will be the same as its output NA, provided...
Series: ASM Handbook
Volume: 6A
Publisher: ASM International
Published: 31 October 2011
DOI: 10.31399/asm.hb.v06a.a0005641
EISBN: 978-1-62708-174-0
... than that observed in electron beam welding, because the kinetic energy of electrons with rest mass (inertia) is greater than that of the photons (with zero rest mass) in the laser beam. For example, the maximum thickness of type 304 stainless steel plate that can be welded using a 77 kW CO 2 laser...
Series: ASM Handbook
Volume: 6A
Publisher: ASM International
Published: 31 October 2011
DOI: 10.31399/asm.hb.v06a.a0005631
EISBN: 978-1-62708-174-0
Image
Published: 01 December 1998
Fig. 5 Schematic of energy dispersive x-ray detector. Detector measures the energy of each incoming x-ray photon by counting the number of electron-hole pairs it produces. A histogram is then developed and plotted of the x-ray energies of the many (typically tens to hundreds of thousands More
Image
Published: 15 December 2019
Fig. 1 The energy gap (Δ E ) between the ground state ( g ) and excited state ( g *) of a species changes during a spot test reaction. The value of Δ E is equal to the energy of a photon ( E photon ) that the molecule can absorb, which depends on Planck’s constant ( h ), the speed of light More
Series: ASM Desk Editions
Publisher: ASM International
Published: 01 December 1998
DOI: 10.31399/asm.hb.mhde2.a0003250
EISBN: 978-1-62708-199-3
... are excited to higher quantum states (energy levels) or removed from the atom (ionization). These “excited” atoms quickly “relax” by electrons from higher energy levels filling the vacated levels. When this happens, photons are emitted whose energies are equal to the differences between the two energy levels...
Book Chapter

By S. Lampman
Series: ASM Handbook
Volume: 10
Publisher: ASM International
Published: 15 December 2019
DOI: 10.31399/asm.hb.v10.a0006645
EISBN: 978-1-62708-213-6
... can easily provide detection limits for lead in soil of less than 100 ppm, well below typical regulatory levels of 300 to 1500 ppm. Operating Principles X-rays, discovered by Roentgen in 1895, are high-energy photons that occur from nuclear decay or when electrons in a disturbed or excited atom...
Series: ASM Handbook
Volume: 17
Publisher: ASM International
Published: 01 August 2018
DOI: 10.31399/asm.hb.v17.a0006459
EISBN: 978-1-62708-190-0
... Abstract Digital radiography is a technique that uses digital detector arrays (linear or area) to capture an X-ray photonic signal and convert it to an electronic signal for display on a computer. This article begins with an overview of real-time radiography and provides a schematic...
Series: ASM Handbook
Volume: 17
Publisher: ASM International
Published: 01 August 2018
DOI: 10.31399/asm.hb.v17.a0006448
EISBN: 978-1-62708-190-0
... light, and infrared radiation showing their relationship with wavelength and photon energy X-rays and γ-rays are physically indistinguishable; they differ only in the manner in which they are produced. X-rays result from the interaction between a rapidly moving stream of electrons and atoms...
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Published: 31 October 2011
Fig. 3 Output profiles for (a) single-mode fiber optic and (b) stepped-index fiber optic. Courtesy of IPG Photonics and Primes More