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一条控制激光尾波场加速电子纵向相空间的光束线,将其传输到一个波荡器。

A beamline to control longitudinal phase space whilst transporting laser wakefield accelerated electrons to an undulator.

机构信息

Department of Physics and Astronomy, The University of Manchester, Manchester, M13 9PL, UK.

The Cockcroft Institute, Warrington, WA4 4AD, UK.

出版信息

Sci Rep. 2023 May 31;13(1):8831. doi: 10.1038/s41598-023-35435-7.

DOI:10.1038/s41598-023-35435-7
PMID:37258601
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC10232591/
Abstract

Laser wakefield accelerators (LWFAs) can produce high-energy electron bunches in short distances. Successfully coupling these sources with undulators has the potential to form an LWFA-driven free-electron laser (FEL), providing high-intensity short-wavelength radiation. Electron bunches produced from LWFAs have a correlated distribution in longitudinal phase space: a chirp. However, both LWFAs and FELs have strict parameter requirements. The bunch chirp created using ideal LWFA parameters may not suit the FEL; for example, a chirp can reduce the high peak current required for free-electron lasing. We, therefore, design a flexible beamline that can accept either positively or negatively chirped LWFA bunches and adjust the chirp during transport to an undulator. We have used the accelerator design program MAD8 to design a beamline in stages, and to track particle bunches. The final beamline design can produce ambidirectional values of longitudinal dispersion ([Formula: see text]): we demonstrate values of + 0.20 mm, 0.00  mm and - 0.22 mm. Positive or negative values of [Formula: see text] apply a shear forward or backward in the longitudinal phase space of the electron bunch, which provides control of the bunch chirp. This chirp control during the bunch transport gives an additional free parameter and marks a new approach to matching future LWFA-driven FELs.

摘要

激光尾场加速器(LWFAs)可以在短距离内产生高能电子束。成功地将这些光源与波动器耦合在一起,有可能形成一个 LWFA 驱动的自由电子激光(FEL),提供高强度的短波长辐射。LWFAs 产生的电子束在纵向相位空间中具有相关分布:啁啾。然而,LWFAs 和 FELs 都有严格的参数要求。使用理想的 LWFA 参数产生的脉冲啁啾可能不适合 FEL;例如,啁啾可以降低自由电子激光所需的高峰值电流。因此,我们设计了一个灵活的光束线,可以接受正啁啾或负啁啾的 LWFA 束,并在传输过程中调整到波动器的啁啾。我们使用加速器设计程序 MAD8 分阶段设计了一条光束线,并对粒子束进行了跟踪。最终的光束线设计可以产生双向的纵向色散值([Formula: see text]):我们演示了+0.20mm、0.00mm 和-0.22mm 的值。[Formula: see text]的正值或负值在电子束的纵向相位空间中向前或向后施加剪切,从而提供对脉冲啁啾的控制。在束流传输过程中进行的这种啁啾控制提供了一个额外的自由参数,并标志着一种新的方法来匹配未来的 LWFA 驱动的 FEL。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2905/10232591/e841986ce35b/41598_2023_35435_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2905/10232591/58fe7273570b/41598_2023_35435_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2905/10232591/8eae66e6a3f9/41598_2023_35435_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2905/10232591/9068cd10a864/41598_2023_35435_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2905/10232591/23f79a103ffc/41598_2023_35435_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2905/10232591/446d83c1d539/41598_2023_35435_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2905/10232591/abb2f11928ac/41598_2023_35435_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2905/10232591/48eace6c6f19/41598_2023_35435_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2905/10232591/e841986ce35b/41598_2023_35435_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2905/10232591/58fe7273570b/41598_2023_35435_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2905/10232591/8eae66e6a3f9/41598_2023_35435_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2905/10232591/9068cd10a864/41598_2023_35435_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2905/10232591/23f79a103ffc/41598_2023_35435_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2905/10232591/446d83c1d539/41598_2023_35435_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2905/10232591/abb2f11928ac/41598_2023_35435_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2905/10232591/48eace6c6f19/41598_2023_35435_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2905/10232591/e841986ce35b/41598_2023_35435_Fig8_HTML.jpg

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本文引用的文献

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