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| Main Authors: | , , , , , , , , , , , , , , , , |
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| Format: | Preprint |
| Published: |
2025
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| Subjects: | |
| Online Access: | https://arxiv.org/abs/2504.11479 |
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| _version_ | 1866908320914210816 |
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| author | Pengfei, Li Wanqi, Liu Shuai, Ha Yuzhou, Pan Xuhong, Fan Zhanhui, Du Chengliang, Wan Ying, Cui Ke, Yao Yue, Ma Zhihu, Yang Caojie, Shao Schuch, Reinhold Di, Lu Yushou, Song Hongqiang, Zhang Ximeng, Chen |
| author_facet | Pengfei, Li Wanqi, Liu Shuai, Ha Yuzhou, Pan Xuhong, Fan Zhanhui, Du Chengliang, Wan Ying, Cui Ke, Yao Yue, Ma Zhihu, Yang Caojie, Shao Schuch, Reinhold Di, Lu Yushou, Song Hongqiang, Zhang Ximeng, Chen |
| contents | The transmission of 2-keV electrons through a polyethylene terephthalate (PET) nanocapillary with a diameter of 800 nm and a length of 10 μm is studied. The transmitted electrons are detected using a microchannel plate (MCP) with a phosphor screen. It is found that the transmission rate for the transmitted electrons at the incident energy can reach up to 10% for an aligned capillary in the beam direction, but drops to less than 1% when the tilt angle exceeds the geometrically allowable angle. The transmitted electrons with the incident energy do not move with changes in the tilt angle, so the incident electrons are not guided in the insulating capillary, which is different from the behavior of positive ions. In the final stage of transmission, the angular distribution of the transmitted electrons within the geometrically allowable angle splits into two peaks along the observation angle perpendicular to the tilt angle. The time evolution of the transmitted complete angular distribution shows that when the beam is turned on, the transmission profile forms a single peak. As the incident charge and time accumulate, the transmission profile begins to stretch in the plane perpendicular to the tilt angle and gradually splits into two peaks. When the tilt angle of the nanocapillary exceeds the geometrically allowable angle, this splitting tends to disappear. Simulation of charge deposition in the capillary directly exposed to the beam indicates the formation of positive charge patches, which are not conducive to guiding, unlike positive ions. Based on the simulation results, we can explain our data and discuss the possible reasons for the splitting of the transmission angular profiles. |
| format | Preprint |
| id |
arxiv_https___arxiv_org_abs_2504_11479 |
| institution | arXiv |
| publishDate | 2025 |
| record_format | arxiv |
| spellingShingle | Transmission of low energy electrons through a polyethylene terephthalate 800-nm diameter nanocapillary Pengfei, Li Wanqi, Liu Shuai, Ha Yuzhou, Pan Xuhong, Fan Zhanhui, Du Chengliang, Wan Ying, Cui Ke, Yao Yue, Ma Zhihu, Yang Caojie, Shao Schuch, Reinhold Di, Lu Yushou, Song Hongqiang, Zhang Ximeng, Chen Materials Science Mesoscale and Nanoscale Physics The transmission of 2-keV electrons through a polyethylene terephthalate (PET) nanocapillary with a diameter of 800 nm and a length of 10 μm is studied. The transmitted electrons are detected using a microchannel plate (MCP) with a phosphor screen. It is found that the transmission rate for the transmitted electrons at the incident energy can reach up to 10% for an aligned capillary in the beam direction, but drops to less than 1% when the tilt angle exceeds the geometrically allowable angle. The transmitted electrons with the incident energy do not move with changes in the tilt angle, so the incident electrons are not guided in the insulating capillary, which is different from the behavior of positive ions. In the final stage of transmission, the angular distribution of the transmitted electrons within the geometrically allowable angle splits into two peaks along the observation angle perpendicular to the tilt angle. The time evolution of the transmitted complete angular distribution shows that when the beam is turned on, the transmission profile forms a single peak. As the incident charge and time accumulate, the transmission profile begins to stretch in the plane perpendicular to the tilt angle and gradually splits into two peaks. When the tilt angle of the nanocapillary exceeds the geometrically allowable angle, this splitting tends to disappear. Simulation of charge deposition in the capillary directly exposed to the beam indicates the formation of positive charge patches, which are not conducive to guiding, unlike positive ions. Based on the simulation results, we can explain our data and discuss the possible reasons for the splitting of the transmission angular profiles. |
| title | Transmission of low energy electrons through a polyethylene terephthalate 800-nm diameter nanocapillary |
| topic | Materials Science Mesoscale and Nanoscale Physics |
| url | https://arxiv.org/abs/2504.11479 |