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通过微喷嘴加速产生千兆电子伏特质子束。

Generation of giga-electron-volt proton beams by micronozzle acceleration.

作者信息

Murakami M, Balusu D, Maruyama S, Murakami Y, Ramakrishna B

机构信息

Institute of Laser Engineering, Osaka University, 2-6 Yamadaoka, 565-0871, Suita, Osaka, Japan.

Department of Physics, Indian Institute Technology Hyderabad, Sangareddy, Telangana, 502285, India.

出版信息

Sci Rep. 2025 May 31;15(1):19112. doi: 10.1038/s41598-025-03385-x.

DOI:10.1038/s41598-025-03385-x
PMID:40450035
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC12126492/
Abstract

Our proposed ion acceleration scheme, micronozzle acceleration (MNA), generates proton beams with extremely high kinetic energies on the giga-electron-volt (GeV) order. The underlying physics and performance of MNA are studied with two-dimensional particle-in-cell simulations. In MNA targets, a micron-sized hydrogen rod is embedded inside a hollow micronozzle. Subsequent illumination of the target along the symmetric axis by an ultraintense ultrashort laser pulse forms a strong electrostatic field with a long lifetime and an extensive space around the downstream tail of the nozzle. The electric field significantly amplifies the kinetic energies of the accelerated protons, and ≳ GeV protons are generated at an applied laser intensity of [Formula: see text] W/[Formula: see text].

摘要

我们提出的离子加速方案——微喷嘴加速(MNA),能产生动能极高、达到吉电子伏特(GeV)量级的质子束。利用二维粒子模拟研究了MNA的基本物理原理和性能。在MNA靶中,一根微米级的氢棒嵌入一个中空的微喷嘴内。随后,用超强超短激光脉冲沿对称轴照射靶,在喷嘴下游尾部周围形成一个寿命长且空间广阔的强静电场。该电场显著放大了加速质子的动能,在激光强度为[公式:见原文]W/[公式:见原文]时可产生≳GeV的质子。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/bbc9/12126492/64becfdbe7f0/41598_2025_3385_Fig11_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/bbc9/12126492/bd42d47843dc/41598_2025_3385_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/bbc9/12126492/13e2db854774/41598_2025_3385_Fig2_HTML.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/bbc9/12126492/d59060fe1db3/41598_2025_3385_Fig5_HTML.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/bbc9/12126492/f535d7f65f57/41598_2025_3385_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/bbc9/12126492/a289396920c8/41598_2025_3385_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/bbc9/12126492/64becfdbe7f0/41598_2025_3385_Fig11_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/bbc9/12126492/bd42d47843dc/41598_2025_3385_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/bbc9/12126492/13e2db854774/41598_2025_3385_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/bbc9/12126492/de5e5d91a42e/41598_2025_3385_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/bbc9/12126492/05d205308c5d/41598_2025_3385_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/bbc9/12126492/d59060fe1db3/41598_2025_3385_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/bbc9/12126492/1cdb55fd90b9/41598_2025_3385_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/bbc9/12126492/8e59998c58c5/41598_2025_3385_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/bbc9/12126492/6cd7f9c89535/41598_2025_3385_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/bbc9/12126492/f535d7f65f57/41598_2025_3385_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/bbc9/12126492/a289396920c8/41598_2025_3385_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/bbc9/12126492/64becfdbe7f0/41598_2025_3385_Fig11_HTML.jpg

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