| Display title | Physics:Heavy quark effective theory |
| Default sort key | Heavy quark effective theory |
| Page length (in bytes) | 4,838 |
| Namespace ID | 3020 |
| Namespace | Physics |
| Page ID | 415438 |
| Page content language | en - English |
| Page content model | wikitext |
| Indexing by robots | Allowed |
| Number of redirects to this page | 0 |
| Counted as a content page | Yes |
| HandWiki item ID | None |
| Edit | Allow all users (infinite) |
| Move | Allow all users (infinite) |
| Page creator | imported>QCDvac |
| Date of page creation | 03:50, 23 October 2022 |
| Latest editor | imported>QCDvac |
| Date of latest edit | 03:50, 23 October 2022 |
| Total number of edits | 1 |
| Recent number of edits (within past 90 days) | 0 |
| Recent number of distinct authors | 0 |
Description | Content |
Article description: (description)
This attribute controls the content of the description and og:description elements. | In quantum chromodynamics, heavy quark effective theory (HQET) is an effective field theory describing the physics of heavy (that is, of mass far greater than the QCD scale) quarks. It is used in studying the properties of hadrons containing a single charm or bottom quark. The effective theory was formalised... |
