A photoelectron is an electron emitted from a material when it absorbs energy from light, typically ultraviolet or X-ray radiation. This process is known as the photoelectric effect and is used in various scientific techniques such as photoelectron spectroscopy to analyze the electronic structure of materials.
An ejected electron is called a photoelectron.
In the photoelectric effect, the kinetic energy of a photoelectron is directly proportional to the frequency of the incident light. This means that higher frequency light will result in photoelectrons with greater kinetic energy.
To calculate the kinetic energy of a photoelectron emitted from a surface, you can use the equation: ( KE = hf - \phi ), where ( KE ) is the kinetic energy of the photoelectron, ( h ) is the Planck constant, ( f ) is the frequency of the incident photon, and ( \phi ) is the work function of the material.
The maximum photoelectron kinetic energy is given by the equation: Energy of incident light - Work function. If the energy of the incident light is three times the work function, then the maximum kinetic energy of the photoelectrons will be three times the work function. Therefore, the ratio of the maximum photoelectron kinetic energy to the work function is 3:1.
The time lag between the arrival of light at a metal surface and the emission of a photoelectron is extremely short, typically on the order of a few femtoseconds (10^-15 seconds) to tens of femtoseconds. This process is known as the photoelectric effect, where electrons are emitted from a material when it absorbs photons with sufficient energy to overcome the material's work function.
William Charles Price has written: 'A discussion on photoelectron spectroscopy' -- subject(s): Photoelectron spectroscopy
J. H. D. Eland has written: 'Photoelectron spectroscopy' -- subject(s): Photoelectron spectroscopy
The utilization of photo-ionization and kinetic energy distribution analysis of emitted photoelectrons to study the electronic state and composition of the surface region of a sample is known as photoelectron spectroscopy. This technique can be subdivided into two areas: X-ray photoelectron Spectroscopy and Ultraviolet Photoelectron Spectroscopy.
An ejected electron is called a photoelectron.
Stefan Hfner has written: 'Photoelectron spectroscopy'
In the photoelectric effect, the kinetic energy of a photoelectron is directly proportional to the frequency of the incident light. This means that higher frequency light will result in photoelectrons with greater kinetic energy.
To calculate the kinetic energy of a photoelectron emitted from a surface, you can use the equation: ( KE = hf - \phi ), where ( KE ) is the kinetic energy of the photoelectron, ( h ) is the Planck constant, ( f ) is the frequency of the incident photon, and ( \phi ) is the work function of the material.
W. C. Neely has written: 'X-ray photoelectron spectroscopy (XPS), Rutherford back scattering (RBS) studies ..' -- subject(s): Aluminun alloys, Auger spectroscopy, Backscattering, Electron transitions, Photoelectron spectroscopy, X ray spectroscopy
The maximum photoelectron kinetic energy is given by the equation: Energy of incident light - Work function. If the energy of the incident light is three times the work function, then the maximum kinetic energy of the photoelectrons will be three times the work function. Therefore, the ratio of the maximum photoelectron kinetic energy to the work function is 3:1.
The time lag between the arrival of light at a metal surface and the emission of a photoelectron is extremely short, typically on the order of a few femtoseconds (10^-15 seconds) to tens of femtoseconds. This process is known as the photoelectric effect, where electrons are emitted from a material when it absorbs photons with sufficient energy to overcome the material's work function.
Steven Allen Holmes has written: 'X-ray photoelectron spectroscopy of trifluoromethylbenzenes and chlorofluoromethanes' -- subject(s): X-ray spectroscopy
Melvin Walter Siegel has written: 'The electron affinity of nitric oxide and the molecular constants of its negative ion, determined by laser photoelectron spectroscopy'