首页> 外文会议>IEEE Nuclear Science Symposium >A low-temperature proton detector for a neutron lifetime experiment
【24h】

A low-temperature proton detector for a neutron lifetime experiment

机译:用于中子寿命实验的低温质子探测器

获取原文

摘要

The measurement of the neutron lifetime has always been an active area in fundamental physics. The experimental value, together with one correlation between the products of the neutron β decay, protons, electrons and antineutrinos, allows to address one of the main problems in the standard model of particle physics, the unitarity of the Cabibbo-Kobayashi-Maskawa matrix. The most promising experimental method is the storage of ultra-cold neutrons (UCN) (kinetic energies below 250 neV!). These very slow neutrons have the pleasant property to be reflected when hitting walls from suitable materials. Hence they may be stored in bottles and the lifetime may be determined by varying the storage time and observing the number of surviving neutrons. The value adopted in 2006 by the Particle Data Group (PDG), τ{sub}n = 885.7 ± 0.8s, is mainly determined by one measurement with UCN stored in such a material bottle. A new experiment [1], however, using the same method, but cooling the walls, arrived at τ{sub}n = 878.5 ± 0.8 s, a value 6σ off the PDG value. Therefore it seems mandatory to scrutinize the results again by conducting a new and complementary measurement. The possibility to perform such an experiment comes from the interaction of the neutron magnetic moment with a strong magnetic field. Neutrons with the right orientation of this magnetic moment are repelled by an increasing field. B = 2T is sufficient to trap UCN with kinetic energies below 110 neV. This allows loss-less storage without wall contacts.
机译:中子寿命的测量始终是基本物理学的有源区。实验值与中子β衰变,质子,电子和抗内芽孢杆菌的产物之间的一个相关性,允许解决粒子物理标准模型中的主要问题,Cabibbo-Kobayashi-maskawa基质的统一性。最有希望的实验方法是储存超冷中子(UCN)(高于250 Nev的动力学!)。这些非常缓慢的中子具有令人愉快的财产,以击中来自合适材料的墙壁。因此,它们可以存储在瓶子中,并且可以通过改变存储时间并观察幸存中子的数量来确定寿命。通过粒子数据组(PDG),τ{sub} n = 885.7±0.8s采用的2006年的值主要由储存在这种材料瓶中的UCN的一个测量来决定。然而,新的实验[1],使用相同的方法,但冷却壁,到达τ{sub} n = 878.5±0.8 s,值6σ关闭PDG值。因此,通过进行新的和互补的测量,似乎必须再次审查结果。执行这种实验的可能性来自中子磁矩与强磁场的相互作用。具有这种磁矩的正确取向的中子被越来越多的领域排斥。 B = 2T足以捕获UCN,具有低于110 NEV的动力学能量。这允许丢失损耗而无需墙壁触点。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号