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SNO+

SNO+ detector. The inner vessel is filled with 780T of liquid scintillator and surrounded by a geodesic sphere of photomultiplier tubes immersed in ultra-pure water. The detector is located 2.1km underground at Canada's SNOLAB, outside of Sudbury, Western Ontario.

Credit: SNOLAB

Jeff Tseng

Professor of Physics

Research theme

  • Particle astrophysics & cosmology
  • Fundamental particles and interactions

Sub department

  • Particle Physics

Research groups

  • Rubin-LSST
  • SNO+
Jeff.Tseng@physics.ox.ac.uk
Telephone: 01865 (2)73398
Denys Wilkinson Building, room 674
Home page
  • About
  • Publications

Measurement of Reactor Antineutrino Oscillations with 1.46 Kilotonne-Years of Data at SNO+

Physical Review Letters American Physical Society (APS) 137:10 (2026) 101807

Authors:

M Abreu, A Allega, MR Anderson, S Andringa, DM Asner, DJ Auty, A Bacon, T Baltazar, F Barão, N Barros, R Bayes, EW Beier, A Bialek, SD Biller, E Caden, M Chen, S Cheng, B Cleveland, D Cookman, J Corning, S DeGraw, R Dehghani, J Deloye, MM Depatie, C Dima, J Dittmer, KH Dixon, MS Esmaeilian, E Falk, N Fatemighomi, R Ford, S Gadamsetty, A Gaur, D Gooding, C Grant, J Grove, S Hall, AL Hallin, D Hallman, MR Hebert, WJ Heintzelman, RL Helmer, C Hewitt, B Hreljac, P Huang, R Hunt-Stokes, AS Inácio, CJ Jillings, S Kaluzienski, T Kaptanoglu, J Kladnik, JR Klein, LL Kormos, B Krar, C Kraus, T Kroupová, C Lake, L Lebanowski, C Lefebvre, V Lozza, M Luo, S Maguire, A Maio, S Manecki, J Maneira, RD Martin, N McCauley, AB McDonald, C Mills, G Milton, D Morris, I Morton-Blake, M Mubasher, S Naugle, LJ Nolan, HM O’Keeffe, GD Orebi Gann, S Ouyang, J Page, S Pal, K Paleshi, W Parker, LJ Pickard, RC Pitelka, B Quenallata, P Ravi, A Reichold, S Riccetto, J Rose, R Rosero, J Shen, J Simms, P Skensved, M Smiley, R Tafirout, B Tam, J Tseng, E Vázquez-Jáuregui, CJ Virtue, F Wang, M Ward, JD Wilson, JR Wilson, A Wright, S Yang, Z Ye, M Yeh, S Yu, Y Zhang, K Zuber, A Zummo

Abstract:

The SNO+ Collaboration reports new results on reactor antineutrino oscillations using data acquired from May 2022 through July 2025. The spectral analysis of a flux dominated by nuclear reactors at 240, 340, and 350 km yields the mass-squared difference Δ m 21 2 = ( 7.9 1 − 0.25 + 0.22 ) × 10 − 5 eV 2 . This result is compatible with and approaches the precision of the only other long-baseline reactor antineutrino measurement, by KamLAND. Combining these measurements, along with those from solar neutrino experiments, the global values of the neutrino mixing parameters become Δ m 21 2 = ( 7.59 ± 0.17 ) × 10 − 5 eV 2 and sin 2 θ 12 = 0.310 ± 0.012 . The analysis of geoneutrinos at SNO + is also improved, with a measured signal of 48 − 12 + 14 TNU.
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The Effect of Mass Loss and Convective Overshooting on the Pre-Collapse Structure, Composition, and Neutrino Emission of Red Supergiants

ArXiv 2604.22605 (2026)

Authors:

McKenzie A Myers, Claire B Campbell, Kelly M Patton, Segev BenZvi, Marta Colomer Molla, Alec Habig, James P Kneller, Dan Milisavljevic, Jeffrey Tseng
Details from ArXiV

Data-driven core-collapse supernova multilateration with first neutrino events

Physical Review D American Physical Society (APS) 113:6 (2026) 063005

Authors:

Farrukh Azfar, Jeff Tseng, Marta Colomer Molla, Kate Scholberg, Alec Habig, Segev BenZvi, Melih Kara, James Kneller, Jost Migenda, Dan Milisavljevic, Evan O’Connor

Abstract:

A Galactic core-collapse supernova (CCSN) is likely to be observed in neutrino detectors around the world minutes to hours before the electromagnetic radiation arrives. The SuperNova Early Warning System (SNEWS2.0) network of neutrino and dark matter detectors aims to use the relative arrival times of the neutrinos at the different experiments to point back to the supernova so as to facilitate follow-up observation. One of the simplest methods to estimate the CCSN direction is to use the first neutrino events detected through the inverse β decay (IBD) process, ν ¯ e p → e + n . We will consider neutrino detectors sensitive to IBD interactions with low backgrounds. The difference in signal arrival times between a large and a small detector will be biased, however, with the first event at the smaller detector, on average, arriving later than that at the larger detector. This bias can be mitigated by using these first events in a data-driven approach without recourse to simulations or models. The resulting method requires, at minimum, only the times of the first events at most detectors, along with a longer time series of events from one larger detector to act as a reference lightcurve. In this article, we demonstrate this method and its uncertainty estimate using pairs of detectors of different sizes and with different supernova distances. Finally, we use this method to calculate probability skymaps using four detectors currently in operation, Super-Kamiokande, Jiangmen Underground Neutrino Observatory (JUNO), Large Volume Detector (LVD), and SNO + , and show that the calculated probabilities yield appropriate confidence intervals for all supernova directions. The area of the 68% confidence interval varies by distance and direction, but is expected to be a few thousand square degrees. The resulting skymaps should be useful for the multimessenger community as a rapid, initial pointing to follow up on the SNEWS2.0 Galactic CCSN neutrino alert.
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Data-driven core collapse supernova multilateration with first neutrino events

Physical Review D: Particles, Fields, Gravitation and Cosmology American Physical Society 113 (2026) 063005

Authors:

farrukh Azfar, Jeff Tseng

Abstract:

A Galactic core-collapse supernova (CCSN) is likely to be observed in neutrino detectors around the world minutes to hours before the electromagnetic radiation arrives. The SNEWS2.0 network of neutrino and dark matter detectors aims to use the relative arrival times of the neutrinos at the different experiments to point back to the supernova so as to facilitate follow-up observation. One of the simplest methods to estimate the CCSN direction is to use the first neutrino events detected through the inverse beta decay (IBD) process, v̄ep → e+n. We will consider neutrino detectors sensitive to IBD interactions with low backgrounds. The difference in signal arrival times between a large and a small detector will be biased, however, with the first event at the smaller detector, on average, arriving later than that at the larger detector. This bias can be mitigated by using these first events in a data-driven approach without recourse to simulations or models. The resulting method requires, at minimum, only the times of the first events at most detectors, along with a longer time series of events from one larger detector to act as a reference lightcurve. In this article, we demonstrate this method and its uncertainty estimate using pairs of detectors of different sizes and with different supernova distances. Finally, we use this method to calculate probability skymaps using four detectors currently in operation (Super-Kamiokande, JUNO, LVD, and SNO+) and show that the calculated probabilities yield appropriate confidence intervals for all supernova directions. The area of the 68\% confidence interval varies by distance and direction, but is expected to be a few thousand square degrees. The resulting skymaps should be useful for the multi-messenger community as a rapid, initial pointing to follow up on the SNEWS2.0 Galactic CCSN neutrino alert.

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Details from ORA

Cosmogenic neutron production in water at SNO+

Physical Review D American Physical Society (APS) 113:5 (2026) 052014

Authors:

M Abreu, A Allega, MR Anderson, S Andringa, DM Asner, DJ Auty, A Bacon, T Baltazar, F Barão, N Barros, R Bayes, EW Beier, A Bialek, SD Biller, E Caden, EJ Callaghan, M Chen, S Cheng, B Cleveland, D Cookman, J Corning, S DeGraw, R Dehghani, J Deloye, MM Depatie, C Dima, J Dittmer, KH Dixon, MS Esmaeilian, E Falk, N Fatemighomi, R Ford, S Gadamsetty, A Gaur, D Gooding, C Grant, J Grove, S Hall, AL Hallin, D Hallman, MR Hebert, WJ Heintzelman, RL Helmer, C Hewitt, B Hreljac, P Huang, R Hunt-Stokes, AS Inácio, CJ Jillings, S Kaluzienski, T Kaptanoglu, J Kladnik, JR Klein, LL Kormos, B Krar, C Kraus, T Kroupová, C Lake, L Lebanowski, C Lefebvre, B Liggins, V Lozza, M Luo, S Maguire, A Maio, S Manecki, J Maneira, RD Martin, N McCauley, AB McDonald, G Milton, D Morris, M Mubasher, S Naugle, LJ Nolan, HM O’Keeffe, GD Orebi Gann, S Ouyang, J Page, S Pal, K Paleshi, W Parker, LJ Pickard, RC Pitelka, B Quenallata, P Ravi, A Reichold, S Riccetto, J Rose, R Rosero, J Shen, J Simms, P Skensved, M Smiley, MI Stringer, R Tafirout, B Tam, J Tseng, E Vázquez-Jáuregui, CJ Virtue, F Wang, M Ward, JR Wilson, JD Wilson, A Wright, S Yang, Z Ye, M Yeh, S Yu, Y Zhang, K Zuber

Abstract:

Accurate measurement of the cosmogenic muon-induced neutron yield is crucial for constraining a significant background in a wide range of low-energy physics searches. Although previous underground experiments have measured this yield across various cosmogenic muon energies, SNO + is uniquely positioned due to its exposure to one of the highest average cosmogenic muon energies at 364 GeV. Using ultrapure water, we have determined a neutron yield of Y n = ( 3.3 8 − 0.30 + 0.23 ) × 10 − 4 cm 2 g − 1 μ − 1 at SNO + . Comparison with simulations demonstrates clear agreement with the neutron production model, highlighting discrepancies with the widely used 4 model. Furthermore, this measurement reveals a lower cosmogenic neutron yield than that observed by the SNO experiment, which used heavy water under identical muon flux conditions. This result provides new evidence that nuclear structure and target material composition significantly influence neutron production by cosmogenic muons, offering fresh insight with important implications for the design and background modeling of future underground experiments.
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