Open main menu
Home
Random
Recent changes
Special pages
Community portal
Preferences
About Wikipedia
Disclaimers
Incubator escapee wiki
Search
User menu
Talk
Dark mode
Contributions
Create account
Log in
Editing
Hartree
Warning:
You are not logged in. Your IP address will be publicly visible if you make any edits. If you
log in
or
create an account
, your edits will be attributed to your username, along with other benefits.
Anti-spam check. Do
not
fill this in!
{{for|other articles and the surname|Hartree (disambiguation)}} {{Short description|Unit of energy in the atomic units system}} The '''hartree''' (symbol: ''E''<sub>h</sub>), also known as the '''Hartree energy''', is the [[measurement unit|unit]] of [[energy]] in the [[atomic units]] system, named after the British physicist [[Douglas Hartree]]. Its [[CODATA]] recommended value is {{physconst|Eh|symbol=yes}} = {{physconst|Eh_eV|after=.}} The hartree is approximately the negative [[electric potential energy]] of the electron in a [[hydrogen]] [[atom]] in its [[ground state]] and, by the [[virial theorem]], approximately twice its [[ionization energy]]; the relationships are not exact because of the finite [[mass]] of the [[Atomic nucleus|nucleus]] of the hydrogen atom and [[Quantum electrodynamics|relativistic corrections]]. The hartree is usually used as a unit of energy in [[atomic physics]] and [[computational chemistry]]: for experimental measurements at the atomic scale, the [[electronvolt]] (eV) or the [[reciprocal centimetre]] (cm<sup>β1</sup>) are much more widely used. == Other relationships == : <math>E_\mathrm{h} = {\hbar^2 \over {m_\mathrm{e} a^2_0}} = m_\mathrm{e}\left(\frac{e^2}{4\pi\varepsilon_0\hbar}\right)^2 = m_\mathrm{e} c^2 \alpha^2 = {\hbar c \alpha \over {a_0}} </math> :: = 2 [[Rydberg constant#Rydberg unit of energy|Ry]] = 2 [[Rydberg constant|''R''<sub>β</sub>]]''hc'' :: = {{physconst|Eh_eV|unit={{val|ul=eV}}}} :: = {{physconst|Eh|unit={{val|ul=J}}}} :: = {{val|4.3597447222060|(48)|e=-11|ul=erg}} :: β {{val|2625.4996394799|(50)|ul=kJ/mol}} <!-- to be recalculated or {{physconst}} used --> :: β {{val|627.5094740631|(12)|ul=kcal/mol}} <!-- to be recalculated or {{physconst}} used --> :: β {{val|219474.63136320|(43)|ul=cm-1}} <!-- to be recalculated or {{physconst}} used --> :: β {{val|6579.683920502|(13)|ul=THz}} <!-- to be recalculated or {{physconst}} used --> where: * ''Δ§'' is the [[reduced Planck constant]], * ''m''<sub>e</sub> is the [[electron mass]], * ''e'' is the [[elementary charge]], * ''a''<sub>0</sub> is the [[Bohr radius]], * ''Ξ΅''<sub>0</sub> is the [[electric constant]], * ''c'' is the [[speed of light]] in vacuum, and * ''Ξ±'' is the [[fine-structure constant]]. Effective hartree units are used in semiconductor physics where <math>e^2</math> is replaced by <math>e^2/\varepsilon</math> and <math>\varepsilon </math> is the static dielectric constant. Also, the electron mass is replaced by the effective band mass <math>m^*</math>. The effective hartree in semiconductors becomes small enough to be measured in [[millielectronvolt]]s (meV).<ref> Tsuneya Ando, Alan B. Fowler, and Frank Stern Rev. Mod. Phys. '''54''', 437 (1982) </ref> == References == {{reflist}} [[Category:Units of energy]] [[Category:Physical constants]]
Edit summary
(Briefly describe your changes)
By publishing changes, you agree to the
Terms of Use
, and you irrevocably agree to release your contribution under the
CC BY-SA 4.0 License
and the
GFDL
. You agree that a hyperlink or URL is sufficient attribution under the Creative Commons license.
Cancel
Editing help
(opens in new window)
Pages transcluded onto the current version of this page
(
help
)
:
Template:For
(
edit
)
Template:Physconst
(
edit
)
Template:Reflist
(
edit
)
Template:Short description
(
edit
)
Template:Val
(
edit
)