The work function is the minimum energy (usually measured in electron volts) needed to remove an electron from a solid to a point immediately outside the solid surface (or energy needed to move an electron from the Fermi energy level into vacuum). In Physics and other Sciences energy (from the Greek grc ἐνέργεια - Energeia, "activity operation" from grc ἐνεργός The electron is a fundamental Subatomic particle that was identified and assigned the negative charge in 1897 by J Here "immediately" means that the final electron position is far from the surface on the atomic scale but still close to the solid on the macroscopic scale. The work function is an important property of metals. The magnitude of the work function is usually about a half of the ionization energy of a free atom of the metal. The ionization potential, ionization energy or EI of an Atom or Molecule is the Energy required to remove an Electron
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Work function W of a metal is closely related to its Fermi energy level
yet the two quantities are not exactly the same. The Fermi energy is a concept in Quantum mechanics usually referring to the energy of the highest occupied Quantum state in a system of Fermions at This is due to the surface effect of a real-world solid: a real-world solid is not infinitely extended with electrons and ions repeatedly filling every primitive cell over all Bravais lattice sites. In Geometry, Solid state physics and Mineralogy, particularly in describing Crystal structure, a primitive cell, is a minimum cell corresponding In Geometry and Crystallography, a Bravais lattice, named after Auguste Bravais, is an infinite set of points generated by a set of discrete translation Neither can one simply take a set of Bravais lattice sites
inside the geometrical region V which the solid occupies and then fill undistorted charge distribution basis into all primitive cells of
. Indeed, the charge distribution in those cells near the surface will be distorted significantly from that in a cell of an ideal infinite solid, resulting in an effective surface dipole distribution, or, sometimes both a surface dipole distribution and a surface charge distribution.
It can be proven that if we define work function as the minimum energy needed to remove an electron to a point immediately out of the solid, the effect of the surface charge distribution can be neglected, leaving only the surface dipole distribution. Let the potential energy difference across the surface due to effective surface dipole be
. And let
be the Fermi energy calculated for the finite solid without considering surface distortion effect, when taking the convention that the potential at
is zero. The Fermi energy is a concept in Quantum mechanics usually referring to the energy of the highest occupied Quantum state in a system of Fermions at Then, the correct formula for work function is:

Where
is negative, which means that electrons are bound in the solid.
For example, caesium has ionization energy 3. Caesium or cesium (ˈsiːziəm is the Chemical element with the symbol Cs and Atomic number 55 9 eV and work function 1. 9 eV.
The work function is the minimum energy that must be given to an electron to liberate it from the surface of a particular metal. In the photoelectric effect if a photon with an energy greater than the work function is incident on a metal photoelectric emission occurs. Introduction When a Metallic surface is exposed to Electromagnetic radiation above a certain threshold Frequency, the light is absorbed and Electrons In Physics, the photon is the Elementary particle responsible for electromagnetic phenomena Introduction When a Metallic surface is exposed to Electromagnetic radiation above a certain threshold Frequency, the light is absorbed and Electrons Any excess energy is given to the electron as kinetic energy.
Photoelectric work function is
where h is the Planck's constant and f0 is the minimum (threshold) frequency of the photon required to produce photoelectric emission. The Planck constant (denoted h\ is a Physical constant used to describe the sizes of quanta. When an electron gains energy, it jumps from one energy level to another in "quantum leaps. " This process is called exciting an electron, and the higher energy levels are called "excited states" while the bottom level is called "ground state. "
The work function is also important in the theory of thermionic emission. Thermionic emission is the flow of Charge carriers from a surface or over some other kind of Electrical potential barrier caused by thermal vibrational energy Here the electron gains its energy from heat rather than photons. In this case, as for an electron escaping from the heated negatively-charged filament of a vacuum tube, the work function may be called the thermionic work function. This article is about the electronic device not an evacuated pipe used for experiments in Free-fall. Tungsten is a very common metal for vacuum tube elements, with a work function of approximately 4. Tungsten (ˈtʌŋstən also known as wolfram (/ˈwʊlfrəm/ is a Chemical element that has the symbol W and Atomic number 74 5 eV.
Thermionic emission requires a filament heating current (if), to maintain a temperature of 2000-2700 K. A saturation state of the filament current is reached, where a minor change in the filament current does not affect the beam current. The electron gun is then operated with the filament current very near the potential to overcome the work function (W)(Goldstein, 2003) The thermionic work function depends on the orientation of the crystal and will tend to be smaller for metals with an open lattice, larger for metals in which the atoms are closely packed. The range is about 1. 5–6 eV. The volt (symbol V) is the SI derived unit of electric Potential difference or Electromotive force. It is somewhat higher on dense crystal faces than open ones.
In electronics the work function is important for design of the metal-semiconductor junction in Schottky diodes and for design of vacuum tubes. Electronics refers to the flow of charge (moving Electrons through Nonmetal conductors (mainly Semiconductors, whereas electrical The M acro E xpansion T emplate A ttribute L anguage complements TAL, providing macros which allow the reuse of code across A semiconductor' is a Solid material that has Electrical conductivity in between a conductor and an insulator; it can vary over that The Schottky diode (named after German physicist Walter H Schottky; also known as hot carrier diode) is a Semiconductor Diode with This article is about the electronic device not an evacuated pipe used for experiments in Free-fall.
Many techniques have been developed based on different physical effects to measure the electronic work function of a sample. One may distinguish between two groups of experimental methods for work function measurements: absolute and relative.
Methods of the first group employ electron emission from the sample induced by photon absorption (photoemission), by high temperature (thermionic emission), due to an electric field (field emission), or using electron tunnelling. Field emission (FE is the emission of electrons from the surface of a condensed phase into another phase due to the presence of high electric fields In Quantum mechanics, quantum tunnelling is a nanoscopic phenomenon in which a particle violates the principles of Classical mechanics by penetrating a
All relative methods make use of the contact potential difference between the sample and a reference electrode. Experimentally, either an anode current of a diode is used or the displacement current between the sample and reference, created by an artificial change in the capacitance between the two, is measured (the Kelvin Probe method, Kelvin probe force microscope). Kelvin probe force microscopy ( KPFM) also known as surface potential microscopy is a noncontact variant of atomic force microscopy (AFM that was
Photoelectron emission spectroscopy (PES) is the general term for spectroscopic techniques based on the outer photoelectric effect. Spectroscopy was originally the study of the interaction between Radiation and Matter as a function of Wavelength (λ In the case of Ultraviolet Photoelectron Spectroscopy (UPS), the surface of a solid sample is irradiated with ultraviolet (UV) light and the kinetic energy of the emitted electrons is analysed. Ultraviolet ( UV) light is Electromagnetic radiation with a Wavelength shorter than that of Visible light, but longer than X-rays The kinetic energy of an object is the extra Energy which it possesses due to its motion As UV light is electromagnetic radiation with an energy hν lower than 100 eV it is able to extract mainly valence electrons. Electromagnetic radiation takes the form of self-propagating Waves in a Vacuum or in Matter. In chemistry valence electrons are the Electrons contained in the outermost or valence, Electron shell of an Atom. Due to limitations of the escape depth of electrons in solids UPS is very surface sensitive, as the information depth is in the range of 2 – 20 monolayers (1-10nm). The resulting spectrum reflects the electronic structure of the sample providing information on the density of states, the occupation of states, and the work function.
The retarding diode method is one of the simplest and oldest method of measuring work functions. Dioden2jpg|thumb|right|150px|Figure 2 Various semiconductor diodes It is based on the thermionic emission of electrons from an emitter. An emitter is a device used to emit any signal, Beacon, Light, Odor, Liquid, Fragrance, or any other type of The current density J of the electrons collected by the sample depends on the work function φ of the sample and is given by the Richardson–Dushman equation J = AT2e − φ / kT where A, the Richardson constant, is a specific material constant. Thermionic emission is the flow of Charge carriers from a surface or over some other kind of Electrical potential barrier caused by thermal vibrational energy The current density increases rapidly with temperature and decreases exponentially with the work function. Changes of the work function can be easily determined by applying a retarding potential V between the sample and the electron emitter; φ is replaced by e(Φ + V) in above equation. The difference in the retarding potential measured at constant current is equivalent to the work function change, assuming that the work function and the temperature of the emitter is constant.
One can use the Richardson–Dushman equation directly to determine the work function by temperature variation of the sample, as well. Rearranging the equation yields ln(J / T2) = ln(A) − φ / kT. The line produced by plotting ln(J / T2) vs. 1 / T will have a slope of − φ / k allowing to determine the work function of the sample.
Units: eV electron Volts
reference: CRC handbook on Chemistry and Physics.
Note: Work function can change for crystaline elements based upon the orientation. For example Ag:4. 26, Ag(110):4. 64, Ag(110):4. 52, Ag(111):4. 74
| Element | eV | Element | eV | Element | eV | Element | eV | Element | eV | Element | eV |
|---|---|---|---|---|---|---|---|---|---|---|---|
| Ag | 4. 26 | Al | 4. 28 | As | 3. 75 | Au | 5. 1 | B | 4. 45 | Ba | 2. 7 |
| Be | 4. 98 | Bi | 4. 22 | C | 5 | Ca | 2. 87 | Cd | 4. 22 | Ce | 2. 9 |
| Co | 5 | Cr | 4. 5 | Cs | 2. 14 | Cu | 4. 65 | Eu | 2. 5 | Fe | 4. 5 |
| Ga | 4. 2 | Gd | 3. 1 | Hf | 3. 9 | Hg | 4. 49 | In | 4. 12 | Ir | 5. 27 |
| K | 2. 3 | La | 3. 5 | Li | 2. 9 | Lu | 3. 3 | Mg | 3. 66 | Mn | 4. 1 |
| Mo | 4. 6 | Na | 2. 75 | Nb | 4. 3 | Nd | 3. 2 | Ni | 5. 15 | Os | 4. 83 |
| Pb | 4. 25 | Pt | 5. 65 | Rb | 2. 16 | Re | 4. 96 | Rh | 4. 98 | Ru | 4. 71 |
| Sb | 4. 55 | Sc | 3. 5 | Se | 5. 9 | Si | 4. 85 | Sm | 2. 7 | Sn | 4. 42 |
| Sr | 2. 59 | Ta | 4. 25 | Tb | 3 | Te | 4. 95 | Th | 3. 4 | Ti | 4. 33 |
| Tl | 3. 84 | U | 3. 63 | V | 4. 3 | W | 4. 55 | Y | 3. 1 | Zn | 4. 33 |
| Zr | 4. 05 |
As a book:
For a quick reference to values of work function of the elements:
*Some of the work functions listed on these sites do not agree!*