{"id":378649,"date":"2021-12-09T16:26:16","date_gmt":"2021-12-09T13:26:16","guid":{"rendered":"https:\/\/en.buradabiliyorum.com\/toward-achieving-megatesla-magnetic-fields-in-the-laboratory\/"},"modified":"2021-12-09T16:26:16","modified_gmt":"2021-12-09T13:26:16","slug":"toward-achieving-megatesla-magnetic-fields-in-the-laboratory","status":"publish","type":"post","link":"https:\/\/buradabiliyorum.com\/en\/toward-achieving-megatesla-magnetic-fields-in-the-laboratory\/","title":{"rendered":"#Toward achieving megatesla magnetic fields in the laboratory"},"content":{"rendered":"<p>&#8220;<strong>#Toward achieving megatesla magnetic fields in the laboratory<\/strong>&#8221;<\/p>\n<div>\n<div class=\"article-gallery lightGallery\">\n<div data-thumb=\"https:\/\/scx1.b-cdn.net\/csz\/news\/tmb\/2021\/toward-the-achievement.jpg\" data-src=\"https:\/\/scx2.b-cdn.net\/gfx\/news\/2021\/toward-the-achievement.jpg\" data-sub-html=\"Figure 1. Illustration of a microtube implosion. Due to the laser-produced hot electrons with megaelectron volt energies, cold ions in the inner wall surface implode toward the central axis. By pre-seeding uniform magnetic fields of the kilotesla order, the Lorentz force induces a Larmor gyromotion of the imploding ions and electrons. Due to the resultant collective motion of relativistic charged particles around the central axis, strong spin currents of approximately peta-ampere\/cm2 are produced with a few tens of nm size, generating megatesla-order magnetic fields. Credit: Masakatsu Murakami\">\n<figure class=\"article-img\">\n            <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/scx1.b-cdn.net\/csz\/news\/800a\/2021\/toward-the-achievement.jpg\" alt=\"Toward the achievement of megatesla magnetic fields in the laboratory\" title=\"Figure 1. Illustration of a microtube implosion. Due to the laser-produced hot electrons with megaelectron volt energies, cold ions in the inner wall surface implode toward the central axis. By pre-seeding uniform magnetic fields of the kilotesla order, the Lorentz force induces a Larmor gyromotion of the imploding ions and electrons. Due to the resultant collective motion of relativistic charged particles around the central axis, strong spin currents of approximately peta-ampere\/cm2 are produced with a few tens of nm size, generating megatesla-order magnetic fields. Credit: Masakatsu Murakami\" width=\"596\" height=\"458\"\/><figcaption class=\"text-darken text-low-up text-truncate-js text-truncate mt-3\">\n                Figure 1. Illustration of a microtube implosion. Due to the laser-produced hot electrons with megaelectron volt energies, cold ions in the inner wall surface implode toward the central axis. By pre-seeding uniform magnetic fields of the kilotesla order, the Lorentz force induces a Larmor gyromotion of the imploding ions and electrons. Due to the resultant collective motion of relativistic charged particles around the central axis, strong spin currents of <a href=\"https:\/\/buradabiliyorum.com\/en\/category\/download-scripts-themes-apps\/\" data-internallinksmanager029f6b8e52c=\"9\" title=\"Download Scripts &amp; Themes &amp; Apps\" target=\"_blank\" rel=\"noopener\">app<\/a>roximately peta-ampere\/cm2 are produced with a few tens of nm size, generating megatesla-order magnetic fields. Credit: Masakatsu Murakami<br \/>\n            <\/figcaption><\/figure>\n<\/p><\/div>\n<\/div>\n<p>Recently, a research team at Osaka University has successfully demonstrated the generation of megatesla (MT)-order magnetic fields via three-dimensional particle simulations on laser-matter interaction. The strength of MT magnetic fields is 1\u201310 billion times stronger than geomagnetism (0.3\u20130.5 G), and these fields are expected to be observed only in the close vicinity of celestial bodies such as neutron stars or black holes. This result should facilitate an ambitious experiment to achieve MT-order magnetic fields in the laboratory, which is now in progress.<\/p>\n<section class=\"article-banner first-banner ads-336x280\">\n         <!-- \/4988204\/Phys_Story_InText_Box --><\/p>\n<\/section>\n<p>Since the 19th century, scientists have strived to achieve the highest magnetic fields in the laboratory. To date, the highest magnetic field observed in the laboratory is in the kilotesla (kT)-order. In 2020, Masakatsu Murakami at Osaka University proposed a novel scheme called microtube implosions (MTI) to generate ultrahigh magnetic fields on the MT-order. Irradiating a micron-sized hollow cylinder with ultraintense and ultrashort laser pulses generates hot electrons with velocities close to the speed of light. Those hot electrons launch a cylindrically symmetric implosion of the inner wall ions towards the central axis. An applied pre-seeded magnetic field of the kilotesla-order, parallel to the central axis, bends the trajectories of ions and electrons in opposite directions because of the Lorentz force. Near the target axis, those bent trajectories of ions and electrons collectively form a strong spin current that generates MT-order magnetic fields.<\/p>\n<p>In this study, one of the team members, Didar Shokov, has extensively conducted three-dimensional simulations using the supercomputer OCTOPUS at Osaka University&#8217;s Cyber<a href=\"https:\/\/buradabiliyorum.com\/en\/category\/social-mediaa\/\" data-internallinksmanager029f6b8e52c=\"1\" title=\"Social Media\" target=\"_blank\" rel=\"noopener\">media<\/a> Center. As a result, a distinct scaling law has been found relating the performance of the generation of the magnetic fields by MTI and such external parameters as applied laser intensity, laser energy, and target size.<\/p>\n<div class=\"article-gallery lightGallery\">\n<div data-thumb=\"https:\/\/scx1.b-cdn.net\/csz\/news\/tmb\/2021\/toward-the-achievement-1.jpg\" data-src=\"https:\/\/scx2.b-cdn.net\/gfx\/news\/2021\/toward-the-achievement-1.jpg\" data-sub-html=\"Figure2. Perspective views of the normalized ion density ni\/ni0 and the z-component of the magnetic field Bz, respectively, observed at t\u223c200 fs, which is obtained by a 3D EPOCH simulation. A cubic aluminum target with a size of 14 \u03bcm \u00d7 14 \u03bcm \u00d7 14 \u03bcm is set at the center, which has a cylindrical cavity with a radius of R0 = 5 \u03bcm and an axis overlapping the z-axis. The seed magnetic field B0 = 6 kT parallel to the z-axis is uniformly set over the entire domain. The four faces of the target parallel to the z-axis are normally irradiated by uniform laser pulses simultaneously, which are characterized by \u03bbL = 0.8 \u03bcm, IL =3\u00d71021 Wcm\u22122 and \u03c4L =50fs. Credit: Masakatsu Murakami et al., High Power Laser Science and Engineering\">\n<figure class=\"article-img text-center\">\n            <img decoding=\"async\" src=\"https:\/\/scx1.b-cdn.net\/csz\/news\/800a\/2021\/toward-the-achievement-1.jpg\" alt=\"Toward the achievement of megatesla magnetic fields in the laboratory\" title=\"Figure2. Perspective views of the normalized ion density ni\/ni0 and the z-component of the magnetic field Bz, respectively, observed at t\u223c200 fs, which is obtained by a 3D EPOCH simulation. A cubic aluminum target with a size of 14 \u03bcm \u00d7 14 \u03bcm \u00d7 14 \u03bcm is set at the center, which has a cylindrical cavity with a radius of R0 = 5 \u03bcm and an axis overlapping the z-axis. The seed magnetic field B0 = 6 kT parallel to the z-axis is uniformly set over the entire domain. The four faces of the target parallel to the z-axis are normally irradiated by uniform laser pulses simultaneously, which are characterized by \u03bbL = 0.8 \u03bcm, IL =3\u00d71021 Wcm\u22122 and \u03c4L =50fs. Credit: Masakatsu Murakami et al., High Power Laser Science and Engineering\"\/><figcaption class=\"text-left text-darken text-truncate text-low-up mt-3\">\n                Figure2. Perspective views of the normalized ion density ni\/ni0 and the z-component of the magnetic field Bz, respectively, observed at t\u223c200 fs, which is obtained by a 3D EPOCH simulation. A cubic aluminum target with a size of 14 \u03bcm \u00d7 14 \u03bcm \u00d7 14 \u03bcm is set at the center, which has a cylindrical cavity with a radius of R0 = 5 \u03bcm and an axis overlapping the z-axis. The seed magnetic field B0 = 6 kT parallel to the z-axis is uniformly set over the entire domain. The four faces of the target parallel to the z-axis are normally irradiated by uniform laser pulses simultaneously, which are characterized by \u03bbL = 0.8 \u03bcm, IL =3\u00d71021 Wcm\u22122 and \u03c4L =50fs. Credit: Masakatsu Murakami et al., High Power Laser <a href=\"https:\/\/buradabiliyorum.com\/en\/category\/sciencee\/\" data-internallinksmanager029f6b8e52c=\"5\" title=\"Science\" target=\"_blank\" rel=\"noopener\">Science<\/a> and Engineering<br \/>\n            <\/figcaption><\/figure>\n<\/p><\/div>\n<\/div>\n<p>&#8220;Our simulation showed that ultrahigh megatesla magnetic fields, which were thought to be impossible to realize on earth, can be achieved using today&#8217;s laser <a href=\"https:\/\/buradabiliyorum.com\/en\/category\/technology\/\" data-internallinksmanager029f6b8e52c=\"4\" title=\"Technology\" target=\"_blank\" rel=\"noopener\">technology<\/a>. The scaling law and detailed temporal behavior of the magnetic fields in the target are expected to facilitate laboratory experiments using the Peta-watt laser system &#8216;LFEX&#8217; at Osaka University&#8217;s Institute of Laser Engineering, which are now in progress,&#8221; Murakami says.<\/p>\n<hr\/>\n<div class=\"article-main__explore my-4 d-print-none\">\n<p>                                            Could megatesla magnetic fields be realized on Earth?\n                                        <\/p><\/div>\n<hr class=\"mb-4\"\/>\n<div class=\"article-main__more p-4\">\n                                                                                                <strong>More information:<\/strong><br \/>\n                                                D. Shokov et al, Laser scaling for generation of megatesla magnetic fields by microtube implosions, <i>High Power Laser Science and Engineering<\/i> (2021).  <a rel=\"nofollow noopener\" target=\"_blank\" data-doi=\"1\" href=\"http:\/\/dx.doi.org\/10.1017\/hpl.2021.46\">DOI: 10.1017\/hpl.2021.46<\/a><\/p><\/div>\n<div class=\"d-inline-block text-medium my-4\">\n                                                Provided by<br \/>\n                                                                                                    Osaka University<br \/>\n                                                                                                        <a rel=\"nofollow noopener\" target=\"_blank\" class=\"icon_open\" href=\"http:\/\/www.osaka-u.ac.jp\/en\"><br \/>\n                                                        <svg>\n                                                            <use href=\"https:\/\/phys.b-cdn.net\/tmpl\/v6\/img\/svg\/sprite.svg#icon_open\" x=\"0\" y=\"0\"\/>\n                                                        <\/svg><br \/>\n                                                    <\/a><\/p><\/div>\n<p>                                        <!-- print only --><\/p>\n<div class=\"d-none d-print-block\">\n<p>                                                 <strong>Citation<\/strong>:<br \/>\n                                                 Toward achieving megatesla magnetic fields in the laboratory (2021, December  9)<br \/>\n                                                 retrieved  9 December 2021<br \/>\n                                                 from https:\/\/phys.org\/<a href=\"https:\/\/buradabiliyorum.com\/en\/category\/news\/\" data-internallinksmanager029f6b8e52c=\"2\" title=\"News\" target=\"_blank\" rel=\"noopener\">news<\/a>\/2021-12-megatesla-magnetic-fields-laboratory.html<\/p>\n<p>                                            This document is subject to copyright. Apart from any fair dealing for the purpose of private study or research, no<br \/>\n                                            part may be reproduced without the written permission. The content is provided for information purposes only.<\/p><\/div>\n<\/p><\/div>\n<p><script id=\"facebook-jssdk\" async=\"\" src=\"https:\/\/connect.facebook.net\/en_US\/sdk.js\"><\/script><\/p>\n<blockquote><p><strong><span style=\"color: #ff6600;\">If you liked the article, do not forget to share it with your friends. Follow us on\u00a0<span style=\"color: #ff0000;\"><a style=\"color: #ff0000;\" href=\"https:\/\/news.google.com\/publications\/CAAqBwgKMLG0nwswvr63Aw\" target=\"_blank\" rel=\"nofollow noopener noreferrer\">Google News<\/a><\/span>\u00a0too, click on the star and choose us from your favorites.<\/span><\/strong><\/p><\/blockquote>\n<blockquote>\n<p style=\"text-align: center;\">For forums sites go to <span style=\"color: #ff9900;\"><a style=\"color: #ff9900;\" href=\"https:\/\/forum.buradabiliyorum.com\/\" target=\"_blank\" rel=\"noopener\">Forum.BuradaBiliyorum.Com<\/a><\/span><\/strong>\n<\/p><\/blockquote>\n<blockquote>\n<p style=\"text-align: center;\"><strong>If you want to read more Like this articles, you can visit our <span style=\"color: #ff9900;\"><a style=\"color: #ff9900;\" href=\"https:\/\/en.buradabiliyorum.com\/science\/\" target=\"_blank\" rel=\"noopener\">Science category.<\/a><\/span><\/strong><\/p>\n<\/blockquote>\n<p><span style=\"color: black;\"><a style=\"color: #ff9900;\" href=\"https:\/\/phys.org\/news\/2021-12-megatesla-magnetic-fields-laboratory.html\" target=\"_blank\" rel=\"noopener\">Source<\/a><\/span><\/p>\n","protected":false},"excerpt":{"rendered":"<p>&#8220;#Toward achieving megatesla magnetic fields in the laboratory&#8221; Figure 1. Illustration of a microtube implosion. Due to the laser-produced hot electrons with megaelectron volt energies, cold ions in the inner wall surface implode toward the central axis. By pre-seeding uniform magnetic fields of the kilotesla order, the Lorentz force induces a Larmor gyromotion of the&#8230;<\/p>\n","protected":false},"author":1,"featured_media":378650,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"fifu_image_url":"https:\/\/scx2.b-cdn.net\/gfx\/news\/2021\/toward-the-achievement.jpg","fifu_image_alt":"","footnotes":""},"categories":[16],"tags":[],"class_list":["post-378649","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-sciencee"],"_links":{"self":[{"href":"https:\/\/buradabiliyorum.com\/en\/wp-json\/wp\/v2\/posts\/378649","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/buradabiliyorum.com\/en\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/buradabiliyorum.com\/en\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/buradabiliyorum.com\/en\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/buradabiliyorum.com\/en\/wp-json\/wp\/v2\/comments?post=378649"}],"version-history":[{"count":0,"href":"https:\/\/buradabiliyorum.com\/en\/wp-json\/wp\/v2\/posts\/378649\/revisions"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/buradabiliyorum.com\/en\/wp-json\/wp\/v2\/media\/378650"}],"wp:attachment":[{"href":"https:\/\/buradabiliyorum.com\/en\/wp-json\/wp\/v2\/media?parent=378649"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/buradabiliyorum.com\/en\/wp-json\/wp\/v2\/categories?post=378649"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/buradabiliyorum.com\/en\/wp-json\/wp\/v2\/tags?post=378649"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}