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Michael Shaevitz Professor of
Physics
Columbia University Department of Physics and Nevis Laboratories Office: 722 Pupin Mailing Address: Columbia University Department of Physics 538 West 120th St. New York, NY 10027 Office Phone Numbers: 914-591-2806 Email: shaevitz at nevis.columbia.edu |
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Current Experiments |
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SBND - Near Detector for the Short-Baseline Neutrino (SBN) Program at Fermilab
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Future Experiments Being Developed |
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IceCube - Gen2
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IsoDAR (Isotope
Decay-at-Rest) is an experiment to search for electron antineutrino disappearance
using an extremely high intensity source
of neutrinos from the decay of 8Li isotopes. The
large number of 8Li isotopes are produced using a 10 ma, 60 MeV proton
cyclotron that is being developed in collaboration with industrial
partners. The source can be placed near a large scintillator
detector such as KAMLAND to detect the antineutrino interaction rate
versus distance using the inverse beta-decay process, νe + p → e+ + n.
Neutrino oscillations would be detected by seeing an anomalous change
in rate versus distance divided by energy, L/E. IsoDAR can also
investigate
non-standard νe interactions
by making precision measurements of the rate for antineutrino-electron
elastic scattering, νe + e− → νe + e− . IsoDAR at KamLAND Conceptual Design Report (CDR) IsoDAR at KamLAND and JUNO Precision Antineutrino-Electron Scattering with IsoDAR |
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DAEδALUS
(Decay-At-rest Experiment for δCP studies At the
Laboratory for Underground Science) is a phased program for
CP-violation studies associated with νμ → νeneutrino
oscillations. Such CP violation could be connected to
the matter-antimatter asymmetry in the universe. The experiment
measures the oscillation wave using three high-intensity, pion
decay-at-rest neutrino sources located at 1.5 km, 8 km, and 20 km from
an underground, ultra-large water or oil based neutrino detector.
The three neutrino sources use 800 MeV proton beams from 10 ma
cyclotrons that pulse sequentially to identify the source to detector
distance. The DAEδALUS data set combined
with a νμ → νe data set from an experiment such as Hyper-K will have
extcellent sensitivity for detecting if CP violation effects are
present.
Cyclotrons as Drivers for Precision Neutrino Measurements |
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DUNE - Long Baseline
Neutrino Facility and DUNE Experimental Collaboration
This long-baseline neutrino program is composed
of a new neutrino source (LBNF) combined with a new set of detectors
(DUNE) optimized for a broad physics program. The program is
conceived around three central components: (1) the new, high intensity
neutrino source generated from a megawatt-class proton accelerator at
Fermi NationalAccelerator Laboratory, (2) a fine-grained near neutrino
detector installed just downstream of the source, and (3) a massive
liquid argon time-projection chamber deployed as a far detector deep
underground at the Sanford Underground Research Facility. This
facility, located at the site of the former Homestake Mine in Lead,
South Dakota, is ~1300 m from the neutrino source at Fermilab — a
distance (baseline) that delivers optimal sensitivity to neutrino
charge-parity (CP) symmetry violation and mass ordering effects. |
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Past Experiments still Analyzing: |
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Double ChoozDouble Chooz is an experiment located in northern France. It searches for the oscillations of electron antineutrinos produced by nuclear power reactors. Neutrinos (and also antineutrinos), of which there are three types, have been found to oscillate from one type to another. These oscillations are governed by several parameters of which one, the mixing angle θ13, was first shown to be fairly large by the Double Chooz experiment. Currently, the Double Chooz experiment has measured this mixing angle to be 8.7 ± 1.5 degrees. The value of θ13 is very important for future neutrino oscillation experiments since its value is not only crucial for interpreting these measurements but its size also determines how big CP violating effects will be.Improved measurements of the neutrino mixing angle θ13 with the Double Chooz detector Reactor electron antineutrino disappearance in the Double Chooz experiment |
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MiniBooNEMiniBooNE was designed to address the LSND νμ → νe oscillation anomaly. The MiniBooNE experiment ran for ten years, from 2002 until 2012, switching between neutrino and antineutrino mode running. MiniBooNE searched for νμ → νe and νμ → νe and oscillations by measuring the rate of observed νe events and testing whether the measured rate was consistent with the estimated background rate.The Events/MeV figure shows the reconstructed neutrino and antineutrino events compared to the MC simulation. For the neutrino data, the magnitude of the observed versus predicted excess is similar to expectations from the LSND antineutrino signal, but the shape is different and mainly below 500 MeV. In contrast, the antineutrino excess shows a similar magnitude and shape with respect to the LSND predictions and is fully consistent with the LSND signal. This behavior leads to the allowed regions shown in the Δm2 vs sin22θ figure where the MiniBooNE allowed region is somewhat below the LSND region for neutrinos. The LSND and MiniBooNE Oscillation Searches at High Δm2 Significant Excess of ElectronLike Events in the MiniBooNE Short-Baseline Neutrino Experiment |
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