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A Longitudinal Density Monitor for the LHC

机译:大型强子对撞机的纵向密度监测仪

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摘要

At the Large Hadron Collider (LHC), the world’s largest and highest energy particle accelerator, ion bunches circulate in two counter-rotating beams and are brought into collision. Each bunch is confined within a bucket by the longitudinal focusing effect of the radio frequency (RF) cavities. The RF period is 2.5 ns, while the minimum bunch spacing is 25 ns. Thus, 9 out of every 10 buckets should be empty, as well as additional gaps to allow for the rise-time of injection and dump kickers. In practice, however, small numbers of particles can occupy these supposedly empty buckets, causing problems for machine protection and for the absolute calibration of the LHC’s luminosity. The Longitudinal Density Monitor (LDM) is a new monitor, designed to measure the longitudinal distribution of particles in the LHC with a sufficiently high dynamic range to quantify the relative particle population in the supposedly empty buckets. A non-interceptive measurement is made possible by the use of synchrotron radiation (SR). Single photon counting with an avalanche photo-diode operating in Geiger mode allows a very high dynamic range to be achieved despite the low levels of light available. The imperfect response of the avalanche photo-diode is compensated using a specially designed correction algorithm which reduces noise and distortion to a minimum. This work presents the design, implementation and operation of the LDM. Signal correction methods are discussed with reference to the deadtime and afterpulsing of the avalanche photodiode, and the analysis of the LDM data for use in LHC luminosity calibration is explained. Experimental results with both proton and heavy ion beams are shown illustrating the LDM‘s exceptional performance, combining a high dynamic range of 105 with a 90 ps time resolution. Finally, a novel scheme to extend the dynamic range by several more orders of magnitude is presented.
机译:在世界上最大,最高能量的粒子加速器大型强子对撞机(LHC)中,离子束在两个反向旋转的光束中循环并发生碰撞。每个束通过射频(RF)腔的纵向聚焦作用而被限制在一个桶中。 RF周期为2.5 ns,最小束间距为25 ns。因此,每10个铲斗中应有9个是空的,并应留有额外的间隙以留出注入和卸料踢的时间。然而,实际上,少量颗粒会占据这些所谓的空桶,从而给机器保护和LHC发光度的绝对校准带来麻烦。纵向密度监测器(LDM)是一种新型监测器,旨在以足够高的动态范围测量LHC中颗粒的纵向分布,以量化假定空桶中的相对颗粒数量。通过使用同步辐射(SR),可以进行非拦截式测量。尽管可用光水平很低,但使用在盖革模式下运行的雪崩光电二极管进行单光子计数仍可实现很高的动态范围。雪崩光电二极管的不完美响应使用专门设计的校正算法进行了补偿,该算法可将噪声和失真降至最低。这项工作介绍了LDM的设计,实现和操作。讨论了雪崩光电二极管的死区时间和后脉冲信号校正方法,并解释了用于LHC发光度校准的LDM数据分析。显示了质子和重离子束的实验结果,说明了LDM的出色性能,结合了105的高动态范围和90 ps的时间分辨率。最后,提出了一种将动态范围扩展几个数量级的新颖方案。

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