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Prospects of warm dense matter research at HiRadMat facility at CERN using 440 MeV SPS proton beam

机译:使用440 MeV SPS质子束在CERN HiRadMat设施进行热致密物质研究的前景

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In this paper we present numerical simulations of heating of a solid copper cylinder by the 440 GeV proton beam delivered by the Super Proton Synchrotron (SPS) at CERN. The beam is made of 288 proton bunches while each bunch comprises of 1.15·10~(11) so that the total number of protons in the beam is about 1.3·10~(13). The bunch length is 0.5 ns while two neighboring bunches are separated by 25 ns so that the beam duration is 7.2 μs. Particle intensity distribution in the transverse direction is a Gaussian and the beam can be focused to a spot size with σ = 0.1 mm-1.0 mm. In this paper we present results using two values of σ, namely 0.2 mm and 0.5 mm, respectively. The target length is 1.5 m with a radius = 5 cm and is facially irradiated by the beam. The energy deposition code FLUKA and the two-dimensional hydrodynamic code BIG2 are employed using a suitable iteration time to simulate the hydrodynamic and the thermodynamic response of the target. The primary purpose of this work was to design fixed target experiments for the machine protection studies at the HiRadMat (High Radiation Materials) facility at CERN. However this work has shown that large samples of High Energy Density (HED) matter will be generated in such experiments which suggests an additional application of this facility. In the present paper we emphasize the possibility of doing HED physics experiments at the HiRadMat in the future.
机译:在本文中,我们提供了由CERN的超级质子同步加速器(SPS)输送的440 GeV质子束加热固体铜圆柱体的数值模拟。束由288个质子束组成,每个束由1.15·10〜(11)组成,因此束中的质子总数约为1.3·10〜(13)。束长度为0.5 ns,而两个相邻束之间的间隔为25 ns,因此束持续​​时间为7.2μs。横向上的粒子强度分布是高斯分布,并且光束可以聚焦到σ= 0.1 mm-1.0 mm的光斑尺寸。在本文中,我们使用两个σ值分别表示0.2 mm和0.5 mm的结果。目标长度为1.5 m,半径= 5 cm,并且通过光束在面部进行照射。能量沉积代码FLUKA和二维流体动力代码BIG2使用适当的迭代时间来模拟目标的流体动力和热力学响应。这项工作的主要目的是在CERN的HiRadMat(高辐射材料)工厂设计固定目标实验,以进行机器保护研究。但是,这项工作表明,在此类实验中将生成大量的高能量密度(HED)物质样品,这提示了该设备的另一种应用。在本文中,我们强调将来在HiRadMat上进行HED物理实验的可能性。

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