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MINOS

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and energy spectrum. Because they are weakly interacting and therefore usually pass through matter, the vast majority of the neutrinos travel through the near detector and the 734 km of rock, then through the far detector and off into space. On the way toward Soudan, about 20% of the muon
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The MINOS experiment started detecting neutrinos from the NuMI beam in February 2005. On 30 March 2006, the MINOS collaboration announced that the analysis of the initial data, collected in 2005, is consistent with neutrino oscillations, with the oscillation parameters which are consistent with
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After the detectors for the project were upgraded in 2012, MINOS corrected their initial result and found agreement with the speed of light, with the difference in the arrival times of −0.0006% (±0.0012%) between neutrinos and light. Further measurements are going to be conducted.
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MINOS measures the difference in neutrino beam composition and energy distribution in the near and far detectors with the aim of producing precision measurements of the neutrino squared mass difference and
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In 2010 and 2011, MINOS reported results according to which there is a difference in the disappearance and consequently the masses between antineutrinos and neutrinos, which would violate
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which started taking data in 2013. The experiment was shut down on June 29, 2016, and the far detector has been dismantled and removed. It was moved to Puerto Vallarta, Jalisco in Mexico.
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In 2008, MINOS released a further result using over twice the previous data (3.36×10 protons-on-target; this includes the first data set). This is the most precise measurement of Δ
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In 2011, the above results were updated again, using a more than double data sample (exposure of 7.25×10 protons on target) and improved analysis methodology. The results are:
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On 29 July 2006, the MINOS collaboration published a paper giving their initial measurements of oscillation parameters as judged from muon neutrino disappearance. These are:
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interact with, and approximately 100 meters underground. The commissioning of the near detector was completed in December 2004, and it is now fully operational.
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to bend, making it possible to distinguish interactions with neutrinos from those with antineutrinos. This feature of the MINOS detectors allows MINOS to search for
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results from the MINOS far detector have shown that there is a strong correlation between high energy cosmic rays measured and the temperature of the
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in Northern Minnesota at a depth of 716 meters. The far detector has been fully operational since summer 2003, and has been taking
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P. Adamson et al. (MINOS Collaboration) (2007). "Measurement of neutrino velocity with the MINOS detectors and NuMI neutrino beam".
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D.G. Michael; et al. (2006). "Observation of muon neutrino disappearance with the MINOS detectors in the NuMI neutrino beam".
405:. However, after additional data were evaluated in 2012, MINOS reported that this gap has closed and no excess is there any more. 2127: 2056: 1771: 1510: 1453: 93:
Super-K measurements. MINOS received the last neutrinos from the NUMI beam line at midnight on 30 April 2012. It was upgraded to
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Adamson, P.; et al. (2011). "Observation in the MINOS far detector of the shadowing of cosmic rays by the sun and moon".
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Adamson, P.; et al. (1 January 2010). "Observation of muon intensity variations by season with the MINOS far detector".
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as well as the change in seasons. The MINOS far detector is also able to observe a reduction in cosmic rays caused by the
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P. Adamson; et al. (2008). "Study of muon neutrino disappearance using the Fermilab Main Injector neutrino beam".
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P. Adamson; et al. (2008). "Measurement of neutrino oscillations with the MINOS detectors in the NuMI beam".
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That group found, although with less precision, that the neutrino speeds were consistent with the speed of light.
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MINOS Collaboration (2011). "Search for the disappearance of muon antineutrinos in the NuMI neutrino beam".
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MINOS service building at Fermilab, the entrance to the underground MINOS hall that hosts the near detector.
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P. Adamson; et al. (2011). "Measurement of the neutrino mass splitting and flavor mixing by MINOS".
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NuMI Target Hall (left), the starting point of the NuMI tunnel with the Main Injector in the background.
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Front face of the MINOS far detector. On the left is the control room and on the right is a mural by
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contamination. Neutrino interactions in the near detector are used to measure the initial neutrino
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MINOS Collaboration (2012). "An improved measurement of muon antineutrino disappearance in MINOS".
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The near detector is similar to the far detector in design, but smaller in size with a mass of
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MINOS Collaboration (2011). "First Direct Observation of Muon Antineutrino Disappearance".
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are observed at two detectors, one very close to where the beam is produced (the
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target. The resulting interactions of protons with the target material produce
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Osprey, S.; Barnett, J.; Smith, J.; the MINOS Collaboration (7 March 2009).
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at 68% confidence level, and at 99% confidence level a range between
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In 2007, an experiment with the MINOS detectors found the speed of
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made out of alternating planes of magnetized steel and
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June 5, 2012 549:de Jong, Jeffrey (12 September 2012). 154:data since early in its construction. 7: 1268:10.1016/j.astropartphys.2010.10.010 232:, which are focused by a system of 574:Tzanankos, G; et al. (2011). 14: 2194:Long Baseline Neutrino Experiment 220:proton pulses hit a water-cooled 2271:Accelerator neutrino experiments 1344:D. Overbye (22 September 2011). 600:. Fermi National Accelerator Lab 249:neutrinos oscillate into other 135:The far detector has a mass of 65:("Neutrinos at Main Injector") 1371:. Fermilab today. June 8, 2012 1104:10.1103/PhysRevLett.108.191801 968:10.1103/PhysRevLett.107.021801 885:10.1103/PhysRevLett.106.181801 822:10.1103/PhysRevLett.101.131802 619:Basu, Paroma (30 March 2006). 596:Olmstead, Molly (2016-08-01). 437:Measurements of neutrino speed 57:(Super-K) experiment in 1998. 1: 1511:Lederman–Schwartz–Steinberger 704:10.1103/PhysRevLett.97.191801 2250:List of neutrino experiments 1142:Geophysical Research Letters 417:sudden stratospheric warming 431:Time of flight of neutrinos 16:Particle physics experiment 2302: 1323:10.1103/PhysRevD.76.072005 1215:10.1103/PhysRevD.81.012001 1029:10.1103/PhysRevD.84.071103 767:10.1103/PhysRevD.77.072002 434: 18: 257:Physics goals and results 158:Both MINOS detectors are 646:"Site map of NuMI/MINOS" 398:(90% confidence limit). 53:, first discovered by a 1074:Physical Review Letters 938:Physical Review Letters 854:Physical Review Letters 791:Physical Review Letters 673:Physical Review Letters 551:"'Final' MINOS Results" 142:. It is located in the 583:Fermilab-Proposal-1016 206: 110: 35: 21:Minos (disambiguation) 1404:47.82000°N 92.24167°W 1238:Astroparticle Physics 204: 178:causes the path of a 108: 51:neutrino oscillations 29: 2286:Particle experiments 2281:Fermilab experiments 1565:Neutrino oscillation 1162:10.1029/2008GL036359 510:on 19 September 2007 356:90% confidence limit 308:68% confidence limit 19:For other uses, see 2235:Kamioka Observatory 1409:47.82000; -92.24167 1400: /  1315:2007PhRvD..76g2005A 1260:2011APh....34..457A 1207:2010PhRvD..81a2001A 1154:2009GeoRL..36.5809O 1096:2012PhRvL.108s1801A 1021:2011PhRvD..84g1103A 960:2011PhRvL.107b1801A 877:2011PhRvL.106r1801A 814:2008PhRvL.101m1802A 759:2008PhRvD..77g2002A 696:2006PhRvL..97s1801M 317:. The results are: 174:scintillators. 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Index

Minos (disambiguation)

Joseph Giannetti
particle physics
neutrino oscillations
Super-Kamiokande
Neutrinos
NuMI
beamline
Fermilab
Chicago
Minnesota
MINOS+

tons
graphite
protons
kt
Soudan mine
cosmic ray
neutrino
steel
scintillator
calorimeters
plastic
magnetic field
muon
muon neutrino
interaction
CPT-violation

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