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Pion-Production Target for Mu2e-II: Simulation Design and Prototype Mu2e-II型导子生产目标:仿真设计与原型
Pub Date : 1900-01-01 DOI: 10.2172/1877635
V. Pronskikh, Ingrid Fang, Kevin Lynch, Stefan Mueller, D. Neuffer, James Popp, David Pushka
The main goal of the Mu2e experiment at Fermilab is to search for indications of charged lepton flavor violation [1]. To achieve this goal, experimenters will be searching for the coherent neutrinoless conversion of a negative muon into an electron in the field of a nucleus by measuring 105-MeV electrons emitted in conversions of negative muons into electrons in the nuclear field of an Al target. This will allow Mu2e to probe effective new physics mass scales up to the 10 3 – 10 4 TeV range. One of the central elements of the Mu2e experimental facility is its target station, where negative pions are generated in interactions of the 8 GeV primary proton beam with a tungsten target, shaped similar to a rod, which will be capable of producing around 3 : 6 (cid:1) 10 20 stopped negative muons in three years of running [2]. The Mu2e experiment is planned to be extended to a next-generation experiment, Mu2e-II, with a single event sensitivity improved by a factor of 10 or more. Mu2e-II will probe new physics mass scales up to 10 5 TeV by utilizing an 800-MeV 100-kW proton beam. This greater sensitivity is within reach by using the PIP-II accelerator upgrade, a 250-meter-long LINAC capable of accelerating a 2-mA proton beam to a kinetic energy of 800 MeV corresponding to 1.6 MW (the power not used by Mu2e-II will be directed to a neutrino experiment). The higher beam intensity would require a substantially more advanced target design. We are studying a novel conveyor target with tungsten or carbon spherical target elements moved through the beam path. The motion of the elements can be ensured either just mechanically or both mechanically and via He-gas flow. In this talk, we will discuss our recent advances in conceptual design R&D for a Mu2e-II target station based on energy deposition and radiation damage simulations. Our study involves Monte-Carlo codes (MARS15 [3], G4beamline [4], and FLUKA [5]) and thermal and mechanical ANSYS analyses to estimate the stability of the system. The concurrent use of the aforemen-tioned simulation software is intended to allow us to determine and minimize the systematic uncertainty of the simulations. Our simulations allowed us to rule out some other designs (rotated and fixed granular tar-gets) as less practical and supported our assessment of the new target station’s required working parameters and constraints. The thermal and mechanical analyses we performed enabled us to determine the choice of cooling scheme and prospective materials for the conveyor’s spherical elements. We will discuss the first prototype of the Mu2e-II target and its mechanical tests performed at Fermilab that indicated the feasibility of the proposed design and its weaknesses, and we will suggest directions for its further improvement.
费米实验室Mu2e实验的主要目标是寻找带电轻子风味违背的迹象[1]。为了实现这一目标,实验人员将通过测量在Al靶核场中负μ子转化为电子时发射的105-MeV电子来寻找负μ子在核场中转化为电子的相干中微子。这将允许Mu2e探测有效的新物理质量尺度达到103 - 104tev范围。Mu2e实验设施的核心要素之一是它的靶站,在那里,8 GeV的主质子束与一个形状类似于棒的钨靶相互作用产生负介子,在三年的运行中,它将能够产生大约3:6 (cid:1) 10 20个停止的负介子[2]。Mu2e试验计划扩展到下一代试验Mu2e- ii,单事件灵敏度提高10倍或更多。Mu2e-II将利用800-MeV的100千瓦质子束探测高达10.5 TeV的新物理质量尺度。通过使用PIP-II加速器升级,更高的灵敏度是可以达到的,这是一个250米长的直线加速器,能够将2毫安的质子束加速到800兆电子伏特的动能,相当于1.6兆瓦(mu2b - ii未使用的能量将用于中微子实验)。更高的光束强度需要更先进的靶设计。我们正在研究一种由钨或碳球形靶元在光束路径中移动的新型输送靶。元件的运动既可以通过机械方式保证,也可以通过机械方式和氦气流保证。在这次演讲中,我们将讨论我们在基于能量沉积和辐射损伤模拟的Mu2e-II目标站概念设计研发方面的最新进展。我们的研究涉及蒙特卡罗代码(MARS15 [3], G4beamline[4]和FLUKA[5])和热力学ANSYS分析来估计系统的稳定性。同时使用上述仿真软件是为了使我们能够确定并最小化仿真的系统不确定性。我们的模拟使我们排除了其他一些不太实用的设计(旋转和固定颗粒目标),并支持我们对新目标站所需工作参数和约束的评估。我们进行的热学和力学分析使我们能够确定冷却方案的选择和输送机球形元件的预期材料。我们将讨论Mu2e-II目标的第一个原型及其在费米实验室进行的机械测试,这些测试表明了所提议设计的可行性及其弱点,我们将提出进一步改进的方向。
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Pion-Production Target for Mu2e-II: Simulation Design and Prototype
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