Cascaded generation of isolated sub-10 attosecond half-cycle pulses
Sub-10 attosecond pulses (APs) with half-cycle electric fields provide exceptional options to detect and manipulate electrons in the atomic timescale. However, the availability of such pulses is still challenging. Here, we propose a method to generate isolated sub-10 attosecond half-cycle pulses bas...
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Veröffentlicht in: | New journal of physics 2021-05, Vol.23 (5), p.53003 |
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creator | Shou, Yinren Hu, Ronghao Gong, Zheng Yu, Jinqing Chen, Jia erh Mourou, Gerard Yan, Xueqing Ma, Wenjun |
description | Sub-10 attosecond pulses (APs) with half-cycle electric fields provide exceptional options to detect and manipulate electrons in the atomic timescale. However, the availability of such pulses is still challenging. Here, we propose a method to generate isolated sub-10 attosecond half-cycle pulses based on a cascade process naturally happening in plasma. A backward AP is first generated by shooting a moderate overdense plasma with a one-cycle femtosecond pulse. After that, an electron sheet with the thickness of several nanometers is formed and accelerated forward by the electrostatic field. Then this electron sheet goes through unipolar perturbations driven by the tail of the first-stage AP instead of the initial laser pulse. As a result, a half-cycle sub-10 AP is cascadedly produced in the transmission direction. Two-dimensional particle-in-cell simulations indicate that an isolated half-cycle pulse with the duration of 7.3 attoseconds can be generated from the cascaded scheme. Apart from a one-cycle driving pulse, such a scheme also can be realized with a commercial 100 TW 25 fs driving laser by shaping the pulse with a relativistic plasma lens in advance. |
doi_str_mv | 10.1088/1367-2630/abf612 |
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However, the availability of such pulses is still challenging. Here, we propose a method to generate isolated sub-10 attosecond half-cycle pulses based on a cascade process naturally happening in plasma. A backward AP is first generated by shooting a moderate overdense plasma with a one-cycle femtosecond pulse. After that, an electron sheet with the thickness of several nanometers is formed and accelerated forward by the electrostatic field. Then this electron sheet goes through unipolar perturbations driven by the tail of the first-stage AP instead of the initial laser pulse. As a result, a half-cycle sub-10 AP is cascadedly produced in the transmission direction. Two-dimensional particle-in-cell simulations indicate that an isolated half-cycle pulse with the duration of 7.3 attoseconds can be generated from the cascaded scheme. Apart from a one-cycle driving pulse, such a scheme also can be realized with a commercial 100 TW 25 fs driving laser by shaping the pulse with a relativistic plasma lens in advance.</description><identifier>ISSN: 1367-2630</identifier><identifier>EISSN: 1367-2630</identifier><identifier>DOI: 10.1088/1367-2630/abf612</identifier><identifier>CODEN: NJOPFM</identifier><language>eng</language><publisher>Bristol: IOP Publishing</publisher><subject>Attosecond pulses ; Electric fields ; Femtosecond pulses ; isolated attosecond pulses ; near-critical density plasmas ; Particle in cell technique ; particle-in-cell simulations ; Perturbation ; Physics ; Relativistic plasmas ; relativistically intense laser pulses ; Thickness</subject><ispartof>New journal of physics, 2021-05, Vol.23 (5), p.53003</ispartof><rights>2021 The Author(s). Published by IOP Publishing Ltd on behalf of the Institute of Physics and Deutsche Physikalische Gesellschaft</rights><rights>2021. 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Phys</addtitle><description>Sub-10 attosecond pulses (APs) with half-cycle electric fields provide exceptional options to detect and manipulate electrons in the atomic timescale. However, the availability of such pulses is still challenging. Here, we propose a method to generate isolated sub-10 attosecond half-cycle pulses based on a cascade process naturally happening in plasma. A backward AP is first generated by shooting a moderate overdense plasma with a one-cycle femtosecond pulse. After that, an electron sheet with the thickness of several nanometers is formed and accelerated forward by the electrostatic field. Then this electron sheet goes through unipolar perturbations driven by the tail of the first-stage AP instead of the initial laser pulse. As a result, a half-cycle sub-10 AP is cascadedly produced in the transmission direction. Two-dimensional particle-in-cell simulations indicate that an isolated half-cycle pulse with the duration of 7.3 attoseconds can be generated from the cascaded scheme. Apart from a one-cycle driving pulse, such a scheme also can be realized with a commercial 100 TW 25 fs driving laser by shaping the pulse with a relativistic plasma lens in advance.</description><subject>Attosecond pulses</subject><subject>Electric fields</subject><subject>Femtosecond pulses</subject><subject>isolated attosecond pulses</subject><subject>near-critical density plasmas</subject><subject>Particle in cell technique</subject><subject>particle-in-cell simulations</subject><subject>Perturbation</subject><subject>Physics</subject><subject>Relativistic plasmas</subject><subject>relativistically intense laser pulses</subject><subject>Thickness</subject><issn>1367-2630</issn><issn>1367-2630</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><sourceid>O3W</sourceid><sourceid>BENPR</sourceid><sourceid>DOA</sourceid><recordid>eNp9UD1PwzAQjRBIlMLOGImBhdDzR1x7RBUflZBYYLYuzrmkKnGw04F_T0pQYUBM9_T07t27l2XnDK4ZaD1jQs0LrgTMsPKK8YNssqcOf-Hj7CSlNQBjmvNJtlhgclhTna-opYh9E9o8-LxJYYP9QKdtVTDIse9DIhfaOn_FjS_ch9tQ3m03idJpduRxAGffc5q93N0-Lx6Kx6f75eLmsXBS6r6oBKtFVQGQ1NqXZBB0aZgnY6gWSnDHjEM0hIpKrlAxEMQBqdZGOpRimi1H3zrg2naxecP4YQM29osIcWUx9s0QzFbIRSlgLuYAkhFDUl5j6Vxp5lIwNXhdjF5dDO9bSr1dh21sh_iWl1waqZnaqWBUuRhSiuT3VxnYXe1216vd9WrH2oeVq3GlCd2P5z_yyz_k7bqzXNjSwvAECNvVXnwCaMWOrA</recordid><startdate>20210501</startdate><enddate>20210501</enddate><creator>Shou, Yinren</creator><creator>Hu, Ronghao</creator><creator>Gong, Zheng</creator><creator>Yu, Jinqing</creator><creator>Chen, Jia erh</creator><creator>Mourou, Gerard</creator><creator>Yan, Xueqing</creator><creator>Ma, Wenjun</creator><general>IOP Publishing</general><scope>O3W</scope><scope>TSCCA</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>H8D</scope><scope>L7M</scope><scope>PHGZM</scope><scope>PHGZT</scope><scope>PIMPY</scope><scope>PKEHL</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>DOA</scope><orcidid>https://orcid.org/0000-0002-6272-1853</orcidid><orcidid>https://orcid.org/0000-0001-8217-8301</orcidid><orcidid>https://orcid.org/0000-0003-0843-1334</orcidid></search><sort><creationdate>20210501</creationdate><title>Cascaded generation of isolated sub-10 attosecond half-cycle pulses</title><author>Shou, Yinren ; 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Phys</addtitle><date>2021-05-01</date><risdate>2021</risdate><volume>23</volume><issue>5</issue><spage>53003</spage><pages>53003-</pages><issn>1367-2630</issn><eissn>1367-2630</eissn><coden>NJOPFM</coden><abstract>Sub-10 attosecond pulses (APs) with half-cycle electric fields provide exceptional options to detect and manipulate electrons in the atomic timescale. However, the availability of such pulses is still challenging. Here, we propose a method to generate isolated sub-10 attosecond half-cycle pulses based on a cascade process naturally happening in plasma. A backward AP is first generated by shooting a moderate overdense plasma with a one-cycle femtosecond pulse. After that, an electron sheet with the thickness of several nanometers is formed and accelerated forward by the electrostatic field. Then this electron sheet goes through unipolar perturbations driven by the tail of the first-stage AP instead of the initial laser pulse. As a result, a half-cycle sub-10 AP is cascadedly produced in the transmission direction. Two-dimensional particle-in-cell simulations indicate that an isolated half-cycle pulse with the duration of 7.3 attoseconds can be generated from the cascaded scheme. Apart from a one-cycle driving pulse, such a scheme also can be realized with a commercial 100 TW 25 fs driving laser by shaping the pulse with a relativistic plasma lens in advance.</abstract><cop>Bristol</cop><pub>IOP Publishing</pub><doi>10.1088/1367-2630/abf612</doi><tpages>9</tpages><orcidid>https://orcid.org/0000-0002-6272-1853</orcidid><orcidid>https://orcid.org/0000-0001-8217-8301</orcidid><orcidid>https://orcid.org/0000-0003-0843-1334</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Attosecond pulses Electric fields Femtosecond pulses isolated attosecond pulses near-critical density plasmas Particle in cell technique particle-in-cell simulations Perturbation Physics Relativistic plasmas relativistically intense laser pulses Thickness |
title | Cascaded generation of isolated sub-10 attosecond half-cycle pulses |
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