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
Color confinement
(section)
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!
{{Short description|Phenomenon in quantum chromodynamics}} [[Image:Quark confinement.svg|right|thumb|350px|The color force favors confinement because at a certain range it is more energetically favorable to create a quark–antiquark pair than to continue to elongate the color flux tube. This is analogous to the behavior of an elongated rubber-band.]] [[File:Gluon tube-color confinement animation.gif|thumb|300px|An animation of color confinement. If energy is supplied to the quarks as shown, the gluon tube elongates until it reaches a point where it "snaps" and forms a quark–antiquark pair. Thus single quarks are never seen in isolation.]] In [[quantum chromodynamics]] (QCD), '''color confinement''', often simply called '''confinement''', is the phenomenon that [[color charge|color-charged]] particles (such as [[quark]]s and [[gluon]]s) cannot be isolated, and therefore cannot be directly observed in normal conditions below the [[Hagedorn temperature]] of approximately 2 [[tera-|tera]][[kelvin]] (corresponding to energies of approximately 130–140 M[[electron volt|eV]] per particle).<ref>{{cite book |last1=Barger |first1=V. |last2=Phillips |first2=R. |year=1997 |title=Collider Physics |publisher=[[Addison–Wesley]] |isbn=978-0-201-14945-6 }}</ref><ref>{{Cite book<!--Deny Citation Bot--> |last=Greensite |first=J. |year=2011 |title=An introduction to the confinement problem |series=Lecture Notes in Physics |volume=821 |publisher=[[Springer Science+Business Media|Springer]] |isbn=978-3-642-14381-6 |bibcode=2011LNP...821.....G |doi=10.1007/978-3-642-14382-3 }}</ref> Quarks and gluons must clump together to form [[hadron]]s. The two main types of hadron are the [[meson]]s (one quark, one antiquark) and the [[baryon]]s (three quarks). In addition, colorless [[glueball]]s formed only of gluons are also consistent with confinement, though difficult to identify experimentally. Quarks and gluons cannot be separated from their parent hadron without producing new hadrons.<ref> {{cite book |last1=Wu |first1=T.-Y. |author2-link=Woei-Yann Pauchy Hwang |last2=Hwang |first2=Pauchy W.-Y. |year=1991 |title=Relativistic quantum mechanics and quantum fields |pages=321 |publisher=[[World Scientific]] |isbn=978-981-02-0608-6 }}</ref>
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)