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Page ID (page_id) | 2667106 |
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Page title without namespace (page_title) | 'QCD string' |
Full page title (page_prefixedtitle) | 'QCD string' |
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New content model (new_content_model) | 'wikitext' |
Old page wikitext, before the edit (old_wikitext) | '{{Unreferenced|date=December 2009}}
In [[quantum chromodynamics]], (or in the more general case of [[Quantum gauge theory|quantum gauge theories]]), if a [[connection form|connection]] which is [[color confinement|color confining]] occurs, it is possible for stringlike degrees of freedom called '''QCD strings''' or '''QCD flux tubes''' to form. These stringlike excitations are responsible for the confinement of color charges since they are always attached to at least one string which exhibits [[Tension (mechanics)|tension]]. Their existence can be predicted from the [[Dual resonance model|dual]] [[spin network]]/[[spin foam]] models (this duality is exact over a [[Lattice model (physics)|lattice]]). To a surprisingly good approximation, these strings are described [[phenomenological model|phenomenologically]] by the [[Polyakov action]], making them [[noncritical string]]s.
==See also==
*[[Dual superconducting model]]
*[[Lattice gauge theory]]
{{DEFAULTSORT:Qcd String}}
[[Category:Quantum chromodynamics]]
[[Category:Gluons]]
{{Quantum-stub}}' |
New page wikitext, after the edit (new_wikitext) | '{{Unreferenced|date=December 2009}}
In [[quantum chromodynamics]] (or in the more general case of [[Quantum gauge theory|quantum gauge theories]]), if a [[connection form|connection]] which is [[color confinement|color confining]] occurs, it is possible for stringlike degrees of freedom called '''QCD strings''' or '''QCD flux tubes''' to form. These stringlike excitations are responsible for the confinement of color charges since they are always attached to at least one string which exhibits [[Tension (mechanics)|tension]]. Their existence can be predicted from the [[Dual resonance model|dual]] [[spin network]]/[[spin foam]] models (this duality is exact over a [[Lattice model (physics)|lattice]]). To a surprisingly good approximation, these strings are described [[phenomenological model|phenomenologically]] by the [[Polyakov action]], making them [[noncritical string]]s.
==See also==
*[[Dual superconducting model]]
*[[Lattice gauge theory]]
{{DEFAULTSORT:Qcd String}}
[[Category:Quantum chromodynamics]]
[[Category:Gluons]]
{{Quantum-stub}}' |
Unified diff of changes made by edit (edit_diff) | '@@ -1,4 +1,4 @@
{{Unreferenced|date=December 2009}}
-In [[quantum chromodynamics]], (or in the more general case of [[Quantum gauge theory|quantum gauge theories]]), if a [[connection form|connection]] which is [[color confinement|color confining]] occurs, it is possible for stringlike degrees of freedom called '''QCD strings''' or '''QCD flux tubes''' to form. These stringlike excitations are responsible for the confinement of color charges since they are always attached to at least one string which exhibits [[Tension (mechanics)|tension]]. Their existence can be predicted from the [[Dual resonance model|dual]] [[spin network]]/[[spin foam]] models (this duality is exact over a [[Lattice model (physics)|lattice]]). To a surprisingly good approximation, these strings are described [[phenomenological model|phenomenologically]] by the [[Polyakov action]], making them [[noncritical string]]s.
+In [[quantum chromodynamics]] (or in the more general case of [[Quantum gauge theory|quantum gauge theories]]), if a [[connection form|connection]] which is [[color confinement|color confining]] occurs, it is possible for stringlike degrees of freedom called '''QCD strings''' or '''QCD flux tubes''' to form. These stringlike excitations are responsible for the confinement of color charges since they are always attached to at least one string which exhibits [[Tension (mechanics)|tension]]. Their existence can be predicted from the [[Dual resonance model|dual]] [[spin network]]/[[spin foam]] models (this duality is exact over a [[Lattice model (physics)|lattice]]). To a surprisingly good approximation, these strings are described [[phenomenological model|phenomenologically]] by the [[Polyakov action]], making them [[noncritical string]]s.
==See also==
' |
New page size (new_size) | 1059 |
Old page size (old_size) | 1060 |
Size change in edit (edit_delta) | -1 |
Lines added in edit (added_lines) | [
0 => 'In [[quantum chromodynamics]] (or in the more general case of [[Quantum gauge theory|quantum gauge theories]]), if a [[connection form|connection]] which is [[color confinement|color confining]] occurs, it is possible for stringlike degrees of freedom called '''QCD strings''' or '''QCD flux tubes''' to form. These stringlike excitations are responsible for the confinement of color charges since they are always attached to at least one string which exhibits [[Tension (mechanics)|tension]]. Their existence can be predicted from the [[Dual resonance model|dual]] [[spin network]]/[[spin foam]] models (this duality is exact over a [[Lattice model (physics)|lattice]]). To a surprisingly good approximation, these strings are described [[phenomenological model|phenomenologically]] by the [[Polyakov action]], making them [[noncritical string]]s.'
] |
Lines removed in edit (removed_lines) | [
0 => 'In [[quantum chromodynamics]], (or in the more general case of [[Quantum gauge theory|quantum gauge theories]]), if a [[connection form|connection]] which is [[color confinement|color confining]] occurs, it is possible for stringlike degrees of freedom called '''QCD strings''' or '''QCD flux tubes''' to form. These stringlike excitations are responsible for the confinement of color charges since they are always attached to at least one string which exhibits [[Tension (mechanics)|tension]]. Their existence can be predicted from the [[Dual resonance model|dual]] [[spin network]]/[[spin foam]] models (this duality is exact over a [[Lattice model (physics)|lattice]]). To a surprisingly good approximation, these strings are described [[phenomenological model|phenomenologically]] by the [[Polyakov action]], making them [[noncritical string]]s.'
] |
New page wikitext, pre-save transformed (new_pst) | '{{Unreferenced|date=December 2009}}
In [[quantum chromodynamics]] (or in the more general case of [[Quantum gauge theory|quantum gauge theories]]), if a [[connection form|connection]] which is [[color confinement|color confining]] occurs, it is possible for stringlike degrees of freedom called '''QCD strings''' or '''QCD flux tubes''' to form. These stringlike excitations are responsible for the confinement of color charges since they are always attached to at least one string which exhibits [[Tension (mechanics)|tension]]. Their existence can be predicted from the [[Dual resonance model|dual]] [[spin network]]/[[spin foam]] models (this duality is exact over a [[Lattice model (physics)|lattice]]). To a surprisingly good approximation, these strings are described [[phenomenological model|phenomenologically]] by the [[Polyakov action]], making them [[noncritical string]]s.
==See also==
*[[Dual superconducting model]]
*[[Lattice gauge theory]]
{{DEFAULTSORT:Qcd String}}
[[Category:Quantum chromodynamics]]
[[Category:Gluons]]
{{Quantum-stub}}' |
Whether or not the change was made through a Tor exit node (tor_exit_node) | 0 |
Unix timestamp of change (timestamp) | 1479348640 |
