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Quantum physics
Quantum physics

... • Thereby Intensity ∝ Rate of incidence of photons, N/t {for a given λ} • Photocurrent I = (n/t)e, where (n/t) = rate of emission of electrons • Why rate of emission of electrons << rate of incidence of photons {for f>f0}: • Not every photon would collide with an electron; most are reflected by the ...
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Chapter 10 - Lecture 3
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Atomic Emission Spectra, Electron Configuration, Periodicity

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... electromagnetic spectrum is this emission found? 4B. Determine the final value of n associated with this emission? (Hint: Consider E = h and the Rydberg equation, use this to find the value of nf.) 4C. Determine the initial value of n associated with this emission. (Hint: Will this value be higher o ...
Structure of atoms and solids
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Physics 280/Jones Week 02 In-Class Problems Fall 2014 1
Physics 280/Jones Week 02 In-Class Problems Fall 2014 1

... turned back down to zero, how fast will the fastest electrons travel? Given, the mass of an electron: me = 9.11 × 10−31 kg. Solution: Recall that when the current has come to a full stop, all electrons including the ones with maximum kinetic energy are held onto the plate: ...
CHAPTER 7 READING GUIDE – IONIC COMPOUNDS AND METALS
CHAPTER 7 READING GUIDE – IONIC COMPOUNDS AND METALS

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The Photoelectric Effect
The Photoelectric Effect

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Auger electron spectroscopy



Auger electron spectroscopy (AES; pronounced [oʒe] in French) is a common analytical technique used specifically in the study of surfaces and, more generally, in the area of materials science. Underlying the spectroscopic technique is the Auger effect, as it has come to be called, which is based on the analysis of energetic electrons emitted from an excited atom after a series of internal relaxation events. The Auger effect was discovered independently by both Lise Meitner and Pierre Auger in the 1920s. Though the discovery was made by Meitner and initially reported in the journal Zeitschrift für Physik in 1922, Auger is credited with the discovery in most of the scientific community. Until the early 1950s Auger transitions were considered nuisance effects by spectroscopists, not containing much relevant material information, but studied so as to explain anomalies in x-ray spectroscopy data. Since 1953 however, AES has become a practical and straightforward characterization technique for probing chemical and compositional surface environments and has found applications in metallurgy, gas-phase chemistry, and throughout the microelectronics industry.
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