Improved measurement of electron antineutrino disappearance at Daya Bay

An, Fengpeng; An, Q.; Bai, J. Z.; Balantekin, A. B.; Band, H. R.; Beriguete, W.; Bishai, M.; Blyth, S.; Brown, Richard; Cao, G. F.; Cao, Jun; Carr, R.; Chan, W. T.; Chang, J. F.; Chang, Yun Hsuan; Chasman, C.; Chen, H. S.; Chen, H. Y.; Chen, S. J.; Chen, S. M.; Chen, X. C.; Chen, X. H.; Chen, X. S.; Chen, Y.; Chen, Y. X.; Cherwinka, J. J.; Chu, M. C.; Cummings, J. P.; Deng, Z. Y.; Ding, Yayun; Diwan, M. V.; Draeger, E.; Du, X. F.; Dwyer, D. A.; Edwards, W. R.; Ely, S.; Fang, S. D.; Fu, J.; Fu, Z.; Ge, Liangquan; Gill, R. L.; Gonchar, M.; Gong, Guanghua; Gong, H.; Gornushkin, Y.; Gu, W.; Guan, Mengyun; Guo, Xin-Heng; Hackenburg, R.; Hahn, R. L.; Hans, S.; Huang, Hao; He, M.; He, Q.; Heeger, K. M.; Heng, Y. K.; Hinrichs, P.; Hor, Y. K.; Hsiung, Y.; Hu, Bei-Zhen; Hu, T.; Huang, Hanxiong; Huang, H. Z.; Huang, X. T.; Huber, Patrick; Issakov, Vadim; Isvan, Z.; Jaffe, D. E.; Jetter, S.; Ji, X. L.; Ji, X.; Jiang, Hao; Jiao, J. B.; Johnson, R. A.; Li, Kang; Kettell, S. H.; Krämer, M.; Kwan, K. K.; Kwok, M. W.; Kwok, T.; Lai, C. Y.; Lai, Wanchang; Lai, W.; Lau, K.; Lebanowski, L.; Lee, J.; Lei, Ruiting; Leitner, R.; Leung, J. K. C.; Leung, Kwong-Sak; Lewis, C. A.; Li, F.; Li, G. S.; Li, Q. J.; Li, W. D.; Li, X. B.; Li, X. N.; Li, X. Q.; Li, Y.; Li, Z. B.; Liang, H.; Lin, C. J.; Lin, Guey-Lin; Lin, S.; Lin, Y. C.; Ling, Jiajie; Link, J. M.; Littenberg, L.; Littlejohn, B. R.; Liu, D. W.; Liu, J. C.; Liu, J. L.; Liu, Y. B.; Lü, C.; Lu, Haoqi; Luk, A.; Luk, K. B.; M., Q.; B., X.; Y., X.; Q., Y.; McDonald, Kirk T.; McFarlane, M. C.; McKeown, R. D.; Meng, Y.; Mohapatra, D.; Nakajima, Yasuhiro; Napolitano, J.; Naumov, D.; Nemchenok, I.; Ngai, H. Y.; Ngai, W. K.; Nie, Yao; Ning, Z.; Ochoa-Ricoux, J. P.; Olshevski, A. G.; Patton, S.; Pec, V.; Peng, J. C.; Piilonen, L. E.; Pinsky, L.; Pun, C. S. J.; Qi, F. Z.; Qi, M.; Qian, X.; Raper, N.; Ren, Jie; Rosero, R.; Roskovec, B.; Ruan, X. C.; Shao, B.; Shih, Kendrick Co; Steiner, H.; Sun, G. X.; Sun, Jian; Tagg, N.; Tam, Y. H.; Tanaka, Hiroyuki; Tang, Xiao; Themann, H.; Torun, Y.; Trentalange, S.; Tsai, O. D.; Tsang, K. V.; Tsang, R.; Tull, C. E.; Tung, Y. C.; Viren, B.; Vorobel, V.; Wang, C. H.; Wang, L. S.; Wang, L. Y.; Wang, L. Z.; Wang, M.; Wang, N. Y.; Wang, R. G.; Wang, W.; Wang, X.; Wang, Y. F.; Wang, Z.; Wang, Z. M.; Webber, D.M.; Wei, H.; Wei, Yadong; Wen, L.; Whisnant, K.; White, C.; Whitehead, L.; Williamson, Y.; Wise, T.; Wong, H. L. H.; Worcester, E.; Wu, Fenfang; Wu, Q.; Jin, Xi; Xia, Dongmei; Xing, Z. Z.; Xu, Jing; Xu, Y.; Xue, T.; Yang, Changgen; Yang, Lei; Ye, M.; Yeh, M.; Yeh, Y. S.; Young, Ben; Yu, Z. Y.; Zhan, Liang; Zhang, C.; Zhang, F. H.; Zhang, J. W.; Zhang, Q. M.; Zhang, S. H.; Zhang, Y. C.; Zhang, Y. H.; Zhang, Y. X.; Zhang, Z. J.; Zhang, Z. P.; Zhang, Z. Y.; Zhao, J.; Zhao, Q.; Zhao, Yue; Zheng, Lei; Zhong, Weili; Li, Zhou; Zhou, Z. Y.; Zhuang, H. L.; Zou, J. H.

doi:10.1088/1674-1137/37/1/011001

Cited by 308 publications

(284 citation statements)

References 52 publications

Supporting

Mentioning

280

Contrasting

Order By: Relevance

“…The reason is that the corresponding generalized CP transformation matrix is not symmetric. 2 Therefore we shall concentrate on the case of δ = 2γ mod n in the following. The neutrino mass matrix is given by…”

Section: Neutrino Sectormentioning

confidence: 99%

“…The effective mass of neutrinoless double-beta decay is [68] |m ee | = (m 1 For normal hierarchy, the masses are 2) and for inverted hierarchy…”

Section: Neutrinoless Double-beta Decaymentioning

confidence: 99%

“…Following the pioneering measurements of the reactor mixing angle θ 13 by the Daya Bay [1,2], RENO [3], and Double Chooz [4,5] reactor neutrino experiments, the three lepton mixing angles θ 12 , θ 23 , θ 13 and both mass-squared differences ∆m 2 sol and ∆m 2 atm have by now been measured to quite good accuracy, as recently summarised, for example, at the Neutrino Oscillation Workshop 2014 [6].…”

Section: Introductionmentioning

confidence: 99%

See 2 more Smart Citations

Generalised CP and Δ(6n 2) family symmetry in semi-direct models of leptons

Ding

King

Neder

2014

J. High Energ. Phys.

View full text Add to dashboard Cite

Abstract:We perform a detailed analysis of ∆(6n 2 ) family symmetry combined with a generalised CP symmetry in the lepton sector, breaking to different remnant symmetries G ν in the neutrino and G l in the charged lepton sector, together with different remnant CP symmetries in each sector. We discuss the resulting mass and mixing predictions for G ν = Z 2 with G l = K 4 , Z p , p > 2 and G ν = K 4 with G l = Z 2 . All cases correspond to the preserved symmetry smaller than the full Klein symmetry, as in the semi-direct approach, leading to predictions which depend on a single undetermined real parameter, which mainly determines the reactor angle. We focus on five phenomenologically allowed cases for which we present the resulting predictions for the PMNS parameters as a function of n, as well as the predictions for neutrinoless double beta decay.

show abstract

Section: Neutrino Sectormentioning

confidence: 99%

“…The effective mass of neutrinoless double-beta decay is [68] |m ee | = (m 1 For normal hierarchy, the masses are 2) and for inverted hierarchy…”

Section: Neutrinoless Double-beta Decaymentioning

confidence: 99%

Section: Introductionmentioning

confidence: 99%

See 1 more Smart Citation

Generalised CP and Δ(6n 2) family symmetry in semi-direct models of leptons

Ding

King

Neder

2014

J. High Energ. Phys.

View full text Add to dashboard Cite

show abstract

“…As long as tan β is rather small, the deviation would be tiny but the large tan β scenario may be also fascinating because of the discrepancy of (g − 2) µ . Furthermore, nonzero θ 13 is confirmed at the experiments [17][18][19][20][21][22], so it is important to discuss the contribution of the T -breaking terms to the PMNS matrix. In the next section, we investigate the mass mixing from the one-loop correction, and discuss the contribution to θ 13 and the flavor changing processes.…”

Section: Setting (δMmentioning

confidence: 97%

“…Especially, we could find so many models motivated by the large mixing in neutrino sector, because the experimental result may imply so-called Tri-Bi maximal mixing [5][6][7], which can be easily accommodated by the BSMs with non-Abelian discrete flavor symmetry such as A 4 [8][9][10][11][12], S 4 [13][14][15], and ∆ (27) [16] etc.. Recent result on the nonzero θ 13 [17][18][19][20][21][22] may require some small modifications in those models, but we could expect that so many kinds of flavor symmetric models can be still consistent with the experimental results [4,. Then, the next question in this approach to the flavor structure would be how to test the flavor symmetry in experiments.…”

Section: Jhep10(2015)042mentioning

confidence: 99%

Study of lepton flavor violation in flavor symmetric models for lepton sector

Kobayashi

Omura

Takayama

et al. 2015

J. High Energ. Phys.

View full text Add to dashboard Cite

Flavor symmetric model is one of the attractive Beyond Standard Models (BSMs) to reveal the flavor structure of the Standard Model (SM). A lot of efforts have been put into the model building and we find many kinds of flavor symmetries and setups are able to explain the observed fermion mass matrices. In this paper, we look for common predictions of physical observables among the ones in flavor symmetric models, and try to understand how to test flavor symmetry in experiments. Especially, we focus on the BSMs for leptons with extra Higgs SU(2) L doublets charged under flavor symmetry. In many flavor models for leptons, remnant symmetry is partially respected after the flavor symmetry breaking, and it controls well the Flavor Changing Neutral Currents (FCNCs) and suggests some crucial predictions against the flavor changing process, although the remnant symmetry is not respected in the full lagrangian. In fact, we see that τ − → e + µ − µ − (µ + e − e − ) and e + e − → τ + τ − (µ − µ + ) processes are the most important in the flavor models that the extra Higgs doublets belong to triplet representation of flavor symmetry. For instance, the stringent constraint from the µ → eγ process could be evaded according to the partial remnant symmetry. We also investigate the breaking effect of the remnant symmetry mediated by the Higgs scalars, and investigate the constraints from the flavor physics: the flavor violating τ and µ decays, the electric dipole moments, and the muon anomalous magnetic moment. We also discuss the correlation between FCNCs and nonzero θ 13 , and point out the physical observables in the charged lepton sector to test the BSMs for the neutrino mixing.

show abstract

First Measurement of the Muon Anti-Neutrino Charged Current Quasielastic Double-Differential Cross Section

Grange

2015

Springer Theses

View full text Add to dashboard Cite

Improved measurement of electron antineutrino disappearance at Daya Bay

Cited by 308 publications

References 52 publications

Generalised CP and Δ(6n 2) family symmetry in semi-direct models of leptons

Generalised CP and Δ(6n 2) family symmetry in semi-direct models of leptons

Study of lepton flavor violation in flavor symmetric models for lepton sector

First Measurement of the Muon Anti-Neutrino Charged Current Quasielastic Double-Differential Cross Section

Contact Info

Product

Resources

About