Homogeneous polynomial - Revision history

en>Omnipaedista: standardized capitalization

2014-12-26T11:07:27Z

standardized capitalization

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en>Myasuda: sp

2014-03-02T04:21:24Z

← Older revision		Revision as of 06:21, 2 March 2014
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	~~In [[high energy physics]],~~ a '~~''vector meson'''~~ is a [~~[meson]] with [[total angular momentum quantum number\|total spin]] 1 and odd [[parity (physics)\|parity]~~] ~~(usually noted as {{nowrap\|~~''~~J<sup>P<~~/~~sup>'' {{=}} 1~~<~~sup~~>~~−~~<~~/sup~~>~~}}). Compare to a [[pseudovector meson]], which has a [[total angular momentum quantum number\|total spin]] 1 and even [[parity (physics)\|parity]].~~

	Vector mesons have been seen in experiments since the 1960s, and are well known for their spectroscopic pattern of masses. Since the development of the [[quark model]] by [[Murray Gell-Mann]] (and independently by [[George Zweig]] as well), the vector mesons have demonstrated the spectroscopy of pure states. The fact that the {{nowrap\|''[[Isospin\|I]]'' {{=}} 1}} [[rho meson]] (ρ~~) and {{nowrap\|''I'' {{=}} 0}}~~ [~~[omega meson]] (ω) have nearly equal mass centered around 770–{{val\|780\|ul=MeV~~/~~c2}}, while the [[phi meson]] (φ) has a higher mass around {{val\|1020\|u=MeV~~/~~c2}}, indicates that the light-quark vector mesons appear in nearly pure states with the φ meson having a nearly 100 percent amplitude of hidden [[strangeness]].~~		Have a lօok at my web blog; [http://www.fizzlive.com/member/1218403/blog/view/3605865 Linne 5 Nätcasino]

	This characteristic of the vector mesons is not at all evident in the [[pseudoscalar meson]] or [[scalar meson]] multiplets, and may be only slightly realized among the [[tensor meson]] and [[pseudovector meson]] multiplets. This fact makes the vector mesons an excellent probe of the quark [[flavour (physics)\|flavor]] content of other types of mesons, measured through the respective [[decay rate]]s of non-vector mesons into the different types of vector mesons. Such experiments are very revealing for theorists who seek to determine the flavor content of mixed state mesons.

	~~At higher masses, the vector mesons include [[charm quark\|charm]] and [[bottom quark]]s in their structure~~. ~~In this realm, the [[radiative process]]es tend to stand out, with heavy tensor and scalar mesons decaying dominantly into vector mesons by [[photon emission]]~~. Pseudovector mesons transition by a similar process into pseudoscalar mesons. Because much of the spectrum of heavy mesons is tied by radiative processes to the vector mesons, one may think of vector mesons as forming a sort of backbone to the spectroscopy of mesons in general.

	~~Some vector mesons can, compared to other mesons, be measured to a very high precision. This stems from the fact that they have the same quantum numbers as the photon, {{nowrap\|''J<sup>PC<~~/~~sup>'' {{=}} 1<sup>−0<~~/~~sup>}}. Therefore they appear in electron-positron collisions in the process <math>e^- e^+ \to \gamma \to q\bar q<~~/~~math>, which provides experimentally a clear signal compared to other measurement, which have to use hadronic processes.~~

	~~==Examples==~~

	* [[rho meson\|ρ meson]]
	* [[omega meson\|ω meson]]
	* [[phi meson\|φ meson]]
	* [[Kaon\|K*(892) meson]]
	* [[D meson\|D* meson]]
	* [[J/~~Psi meson\|{{SubatomicParticle\|J~~/~~Psi}} meson]]~~
	* [[Upsilon meson\|{{SubatomicParticle\|Upsilon}} meson]]

	~~==See also==~~
	* [[List of mesons]]
	* [[Vector meson dominance]]


	~~{{particle-stub}}~~
	~~{{particles}}~~

	~~[[Category:Mesons]~~]

en>SamuelRiv: quick ref note on homogenous polynomials in physics via dimensional analysis

2014-01-17T17:00:08Z

quick ref note on homogenous polynomials in physics via dimensional analysis

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en>D.Lazard: /* Basic properties */ Typos

2012-03-25T12:40:51Z

Basic properties: Typos

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