Gibbs–Thomson equation: Difference between revisions

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{{redirect|RENO|other uses|Reno (disambiguation)}}
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'''RENO''' (Reactor Experiment for Neutrino Oscillations) is a short baseline reactor [[neutrino oscillation]] experiment in [[South Korea]]. The experiment was designed to either measure or set a limit on θ<sub>13</sub>, a neutrino oscillation parameter responsible for changing [[electron neutrino]]s into other neutrinos.
 
On 2012 April 3, with some corrections on April 8, the RENO collaboration announced  a [[Statistical significance#In terms of σ (sigma)|4.9σ]] observation of ''θ''<sub>13</sub> ≠ 0, with
:<math> \sin^2 2 \theta_{13} = 0.113 \pm 0.013({\rm stat.}) \pm 0.019({\rm syst.}) </math><ref>{{cite journal|author=RENO Collaboration|journal=Physical Review Letters|volume=108|issue=18|pages=191802|doi=10.1103/PhysRevLett.108.191802|arxiv=1204.0626|title=Observation of electron-antineutrino disappearance at RENO|date=2012-04-03|bibcode = 2012PhRvL.108s1802A }}</ref><ref>{{cite web|author=RENO Collaboration|url=http://www.interactions.org/cms/?pid=1031612|title=Announcement of the First Results from RENO: Observation of the Weakest Neutrino Transformation|publisher=Interactions NewsWire|date=2012-04-04}}</ref>
 
This measurement confirmed a similar result announced by the [[Daya Bay Reactor Neutrino Experiment|Daya Bay Experiment]] three weeks before and is consistent with earlier, but less significant results by [[T2K]], [[MINOS]] and [[Double Chooz]].  
 
==References==
<references />
 
==See also==
* [[Yeong duk Kim]]
 
{{neutrino detectors}}
 
[[Category:Neutrino experiments]]
 
{{physics-stub}}
{{Korea-stub}}

Latest revision as of 11:17, 16 December 2014

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