Abstract We investigate prospects of building a future accelerator-based neutrino oscillation experiment in China, including site selection, beam optimization and tau neutrino physics aspects. CP violation, non-unitary mixing and non-standard neutrino interactions are discussed. We simulate neutrino beam setups based on muon and beta decay techniques and compare Chinese laboratory sites by their expected sensitivities. A case study on the Super Proton–Proton Collider and the China JinPing Laboratory is also presented. It is shown that the muon-decay-based beam setup can measure the Dirac CP phase by about 14.2° precision at 1 σ CL, whereas non-unitarity can be probed down to ∣ α ij ∣ ≲ 0.37 ( i ≠ j = 1, 2, 3) and non-standard interactions to <?CDATA $| {\epsilon }_{{\ell }{\ell }^{\prime} }^{m}| \lesssim $?> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mo stretchy="false">∣</mml:mo> <mml:msubsup> <mml:mrow> <mml:mi>ϵ</mml:mi> </mml:mrow> <mml:mrow> <mml:mi mathvariant="italic">ℓ</mml:mi> <mml:mi mathvariant="italic">ℓ</mml:mi> <mml:mo accent="false">′</mml:mo> </mml:mrow> <mml:mrow> <mml:mi>m</mml:mi> </mml:mrow> </mml:msubsup> <mml:mo stretchy="false">∣</mml:mo> <mml:mo>≲</mml:mo> </mml:math> 0.11 ( <?CDATA ${\ell }\ne {\ell }^{\prime} =e$?> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi mathvariant="italic">ℓ</mml:mi> <mml:mo>≠</mml:mo> <mml:mi mathvariant="italic">ℓ</mml:mi> <mml:mo accent="false">′</mml:mo> <mml:mo>=</mml:mo> <mml:mi>e</mml:mi> </mml:math> , μ , τ ) at 90% CL, respectively. 

/pdf/precision-measurements-and-tau-neutrino-physics-in-a-future-1yndlp2a.pdf

Precision measurements and tau neutrino physics in a future accelerator neutrino experiment

The baseline target system for a Neutrino Factory or Muon Collider is a free liquid-metal (mercury) jet inside a 20-Tcapturesolenoidmagnet.A peaksolenoidfieldof 15T at themercurytarget locationis beingconsideredasanalternative to simply the target system. The tapering field profile, from Bi = 15 −20-T down to Bf = 1.5 −2-T over distance zf −zi, is optimized to maximize the muon yield at 50 m downstream of the mercury target within a defined energy window. The axial magnetic field is specified analytically using a inverse-cubic form, and the off-axis field is computed from a series expansionbasedon axial derivation of the axialfield. Thesimulation is performed using the MARS15 code,and results of the dependenceof the muon yield on the field profile are discussed.

/pdf/progress-on-the-neutrino-factory-target-system-design-2v387kmcjz.pdf

Progress on the Neutrino Factory Target System Design

International design study for the neutrino factory : first progress report

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International design study for the neutrino factory : first progress report