{"id":4887,"date":"2025-10-20T15:06:34","date_gmt":"2025-10-20T06:06:34","guid":{"rendered":"https:\/\/jteccorp.wdkb.jp\/?page_id=4887"},"modified":"2026-06-03T17:26:00","modified_gmt":"2026-06-03T08:26:00","slug":"high-precision-x-ray-mirror","status":"publish","type":"page","link":"https:\/\/www.j-tec.co.jp\/english\/optical\/high-precision-x-ray-mirror\/","title":{"rendered":"JTEC CORPORATION high-precision X-ray mirror"},"content":{"rendered":"<h1 class=\"c-title content-head -bd\">Introduction of High-precision X-ray Mirrors<\/h1>\n<section class=\"c-section\">\n<h2 class=\"c-title l2\">JTEC CORPORATION&#8217;s High-precision X-ray Mirrors<\/h2>\n<div class=\"c-text\">\n<p>Synchrotron radiation is artificial electromagnetic waves (light) generated when high-energy electrons traveling in a straight line inside a circular accelerator (synchrotron) have their trajectory bent by deflecting electromagnets. It includes wavelengths ranging from long infrared rays to short X-rays. A synchrotron radiation facility is an experimental facility where this synchrotron radiation can be utilized. Here, synchrotron radiation is used by extracting light of the required wavelength according to measurement and analysis purposes (this is called &#8220;spectroscopy&#8221;), but high-brightness (very bright) X-rays are used to illuminate the world of atoms and molecules at the nanometer level.<\/p>\n<p>SPring-8, a large synchrotron radiation facility in Hyogo Prefecture that began operation in 1997, is called one of the world&#8217;s three major synchrotron radiation facilities, along with APS (Advanced Photon Source) in the United States and ESRF (European Synchrotron Radiation Facility) in Europe. It is equipped with a circular accelerator with a total circumference of 1,436m and 62 experimental locations called beamlines, and has achieved many excellent results from basic research to industrial applications through the world&#8217;s highest level of high-brightness synchrotron radiation provided there.<\/p>\n<div class=\"c-image u-mt40\"><img src=\"\/assets\/img\/business\/optical.webp\" \/><\/p>\n<p class=\"u-text-center u-mt10\">Various high-precision X-ray mirrors<\/p>\n<\/div>\n<\/div>\n<h2 class=\"c-title l2\">Features of X-ray mirrors<\/h2>\n<div class=\"c-text u-mt40\">\n<p>(1) The surface has a shape error of several nanometers or less compared to the ideal shape obtained by geometric calculation<\/p>\n<p>(2) It is a crystal plane with well-ordered atomic arrangement without crystalline defects or distortion<\/p>\n<p>(3) A multilayer film surface is formed with a thickness of several to 10 nanometers per layer, generating X-ray diffraction phenomena with high reflectivity<\/p>\n<\/div>\n<div class=\"c-image u-mt40 u-text-center\"><img src=\"\/assets\/img\/optical\/high-precision-x-ray-mirror\/fig-en.webp\" alt=\"Surface shape and shape error graph of high-precision X-ray mirror\" width=\"800\" \/><\/p>\n<p class=\"u-text-center u-mt10\">Example of shape and surface roughness of high-precision X-ray mirror reflection surface<\/p>\n<\/div>\n<\/section>\n<section class=\"c-section\">\n<h2 class=\"c-title l2\">Nano Fabrication Technology and Nano Measurement Technology<\/h2>\n<div class=\"c-text\">\n<p>The reflection surface of our high-precision X-ray mirrors is realized by Elastic Emission Machining (EEM), which enables atomic-level (0.1nm level) removal processing based on fundamental research at The University of Osaka, and Micro Stitching Interferometry (MSI) and Relative Angle Determinable Stitching Interferometry (RADSI), which enable shape measurement at the nanometer level over a wide range in the meter region.<\/p>\n<\/div>\n<div><a class=\"c-button u-mb20 u-mt20 u-mr20\" href=\"\/english\/optical\/nano-processing-technology\/#eem\"> EEM processing technology <\/a> <a class=\"c-button\" href=\"\/english\/optical\/nano-measurement-technology\/#msi-radsi\"> MSI and RADSI <\/a><\/div>\n<\/section>\n<section class=\"c-section\">\n<h2 class=\"c-title l2\">Synchrotron Radiation Facility<\/h2>\n<div class=\"c-text\">\n<p>A large synchrotron radiation facility can be compared to a &#8220;giant microscope.&#8221; To observe the world of atoms and molecules, we need strong light (X-ray) that illuminates the microscopic world inside the material. This can be realized using strong, high-luminance X-rays from a large accelerator with a special bending electromagnet.<\/p>\n<p>The synchrotron radiation facility is a research facility where microstructures can be examined by applying synchrotron radiation to the sample material. Electrons emitted from the electron gun are accelerated to values close to the speed of light, and powerful radiation can be obtained by using a deflecting electromagnet and an insertion light source device. The synchrotron radiation travels from the storage ring to the experimental line (beam line) allocated radially and is used for diverse research and analysis.<\/p>\n<p>SPring-8 is a large-scale synchrotron radiation facility that can produce the world&#8217;s highest performance synchrotron radiation. The ring has a total circumference of 1.5 km and 62 beamlines (of which 56 are in operation). SPring-8 is among the world&#8217;s highest level synchrotron radiation facilities, with Advanced Photon Source (APS) in the US and the European Synchrotron Radiation Facility (ESRF) in Europe, and has achieved excellent results from basic research to industrial use. Usually 4 to 10 X-ray mirrors are used in a beamline. We have delivered a number of mirrors to SPring-8 and the adjacent X-ray free electron laser facility SACLA.<\/p>\n<\/div>\n<ul class=\"c-col2 u-mt40 -half\">\n<li>\n<div class=\"c-image u-text-center u-text-center\"><img class=\"\" src=\"\/assets\/img\/optical\/high-precision-x-ray-mirror\/img_xray10-en.webp\" alt=\"\" \/><\/p>\n<p class=\"u-text-center u-mt10\">Example of synchrotron radiation facility configuration<\/p>\n<\/div>\n<\/li>\n<li>\n<div class=\"c-image     u-text-center\"><img class=\"\" src=\"\/assets\/img\/optical\/high-precision-x-ray-mirror\/img_xray3-en.webp\" alt=\"\" \/><\/p>\n<p class=\"u-text-center u-mt10\">Principle of synchrotron radiation generation<\/p>\n<\/div>\n<\/li>\n<\/ul>\n<ul class=\"u-flex2 u-mt50\">\n<li>\n<div class=\"u-text-center\"><img class=\"\" src=\"\/assets\/img\/optical\/high-precision-x-ray-mirror\/high-precision-x-ray-mirror03-en.webp\" alt=\"\" \/><\/p>\n<p class=\"u-text-center u-mt10\">Configuration of synchrotron radiation<\/p>\n<\/div>\n<\/li>\n<li>\n<div class=\"u-text-center \"><img class=\"\" src=\"\/assets\/img\/optical\/high-precision-x-ray-mirror\/high-precision-x-ray-mirror04.webp\" alt=\"\" \/><\/p>\n<p class=\"u-text-center u-mt10\">Aerial photograph of SPring-8<\/p>\n<\/div>\n<\/li>\n<\/ul>\n<\/section>\n<section class=\"c-section\">\n<h2 class=\"c-title l2\">High-precision X-ray Mirrors in Synchrotron Radiation Facilities<\/h2>\n<div class=\"c-text \">\n<p>Our high-precision X-ray mirrors are used in the beam line for the purpose of focusing, spectroscopy, and imaging. As an example of use, a high-precision KB mirror can be installed in front of a test sample, and X-rays can be focused at nano scale to achieve higher resolution.<\/p>\n<\/div>\n<ul class=\"c-col2 u-mt40 -half\">\n<li>\n<div class=\"c-image u-text-center \"><img class=\"\" src=\"\/assets\/img\/optical\/high-precision-x-ray-mirror\/img_xray12-en.webp\" alt=\"\" \/><\/p>\n<p class=\"u-text-center u-mt10\">Focused X-ray and test sample<\/p>\n<\/div>\n<\/li>\n<li>\n<div class=\"c-image   u-text-center  \"><img class=\"\" src=\"\/assets\/img\/optical\/high-precision-x-ray-mirror\/high-precision-x-ray-mirror06.webp\" alt=\"\" \/><\/p>\n<p class=\"u-text-center u-mt10\">KB mirror installed in vacuum chamber<\/p>\n<\/div>\n<\/li>\n<\/ul>\n<\/section>\n<section class=\"c-section\">\n<h2 class=\"c-title l2\">Research results using Synchrotron Radiation<\/h2>\n<div class=\"c-text\">\n<p>Recent research results using synchrotron radiation include basic and applied research such as protein structural analysis of atomic arrangements, 3D structures of particles recovered from the asteroid Itokawa, structural determination of the regular growth of nanocrystalline composite thin films. It is also widely used in industrial fields such as visualization of the chemical state of platinum catalysts in fuel cells and new material development technology for high-performance tires.<\/p>\n<\/div>\n<h3 class=\"c-title l3  u-mt40\">Examples of research results at synchrotron radiation facilities<\/h3>\n<div class=\"c-col4 u-mt40\">\n<div class=\"c-col4__item\">\n<h3 class=\"c-col4__title\">Life science<\/h3>\n<p><img class=\"u-rad10\" src=\" \/assets\/img\/optical\/high-precision-x-ray-mirror\/img_xray5.webp\" alt=\"\" \/><\/p>\n<ul class=\"c-col4__list\">\n<li>Development of x-ray microscopy for 3D cell imaging<\/li>\n<li>Structural Analysis of Protein Complexes<\/li>\n<\/ul>\n<\/div>\n<div class=\"c-col4__item\">\n<h3 class=\"c-col4__title\">Material science \/ Industry use<\/h3>\n<p><img class=\"u-rad10\" src=\" \/assets\/img\/optical\/high-precision-x-ray-mirror\/img_xray6.webp\" alt=\"\" \/><\/p>\n<ul class=\"c-col4__list\">\n<li>Development of high capacity nickel-metal hydride battery<\/li>\n<li>Analysis of the internal structure of hair for the development of hair care products<\/li>\n<li>New method of 3D measurement for development of fuel-efficient tire<\/li>\n<\/ul>\n<\/div>\n<div class=\"c-col4__item\">\n<h3 class=\"c-col4__title\">Environmental science \/ Geoscience<\/h3>\n<p><img class=\"u-rad10\" src=\" \/assets\/img\/optical\/high-precision-x-ray-mirror\/img_xray7.webp\" alt=\"\" \/><\/p>\n<ul class=\"c-col4__list\">\n<li>Reproduce the environment inside the earth, it suggests that the outer core may be convected in two layers.<\/li>\n<li>Particle analysis of asteroid Itokawa<\/li>\n<\/ul>\n<\/div>\n<div class=\"c-col4__item\">\n<h3 class=\"c-col4__title\">Archaeology science<\/h3>\n<p><img class=\"u-rad10\" src=\" \/assets\/img\/optical\/high-precision-x-ray-mirror\/img_xray8.webp\" alt=\"\" \/><\/p>\n<ul class=\"c-col4__list\">\n<li>Analysis and appraisal of criminal investigation<\/li>\n<li>Investigation of archeological materials by X-ray fluorescence analysis<\/li>\n<li>Identify raw materials based on debris peeled from old wooden surface<\/li>\n<\/ul>\n<\/div>\n<\/div>\n<\/section>\n<section class=\"c-section\"><a class=\"u-scroll-point\" name=\"facility\"><\/a><\/p>\n<h2 class=\"c-title l2\">Facilities with delivery records<\/h2>\n<div class=\"c-text u-mb30\">\n<p>Currently, more than 40 synchrotron radiation facilities are in operation around the world, mainly in Japan, the United States, and Europe. Our high-precision X-ray mirrors are used in these advanced synchrotron radiation facilities and X-ray free electron laser facilities as mirrors that realize diffraction-limited focusing. The manufacturing accuracy of these mirrors is highly rated.<\/p>\n<\/div>\n<div class=\"c-image u-text-center \"><img src=\"\/assets\/img\/optical\/high-precision-x-ray-mirror\/map-en.webp\" alt=\"\" \/><\/div>\n<ul>\n<li>\n<h3 class=\"c-title l2\" style=\"font-size: 20px; margin-top: 40px;\">Facilities with delivery records (in Japan)<\/h3>\n<div class=\"c-table\">\n<table>\n<tbody>\n<tr>\n<td>Location<\/td>\n<td>Facility name<\/td>\n<\/tr>\n<tr>\n<td>Hyogo Prefect.<\/td>\n<td>SPring-8 (Super Photon Ring-8 GeV\uff09<\/td>\n<\/tr>\n<tr>\n<td>Hyogo Prefect.<\/td>\n<td>SACLA (SPring-8 Angstrom Compact free Electron LAser\uff09<\/td>\n<\/tr>\n<tr>\n<td>Hyogo Prefect.<\/td>\n<td>NewSUBARU (NewSUBARU Synchrotron Radiation Facility\uff09<\/td>\n<\/tr>\n<tr>\n<td>Miyagi Prefect.<\/td>\n<td>NanoTerasu (NanoTerasu Synchrotron Light Source\uff09<\/td>\n<\/tr>\n<tr>\n<td>Ibaraki Prefect.<\/td>\n<td>PF (Photon Factory\uff09<\/td>\n<\/tr>\n<tr>\n<td>Shiga Prefect.<\/td>\n<td>AURORA (Compact Synchrotron Light Source AURORA\uff09<\/td>\n<\/tr>\n<tr>\n<td>Saga Prefect.<\/td>\n<td>SAGA-LS (Saga Light Source\uff09<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<\/div>\n<\/li>\n<li>\n<h3 class=\"c-title l2\" style=\"font-size: 20px; margin-top: 40px;\">Facilities with delivery records (Overseas)<\/h3>\n<div class=\"c-table\">\n<table>\n<tbody>\n<tr>\n<td>Country<\/td>\n<td>Facility name<\/td>\n<\/tr>\n<tr>\n<td>UK<\/td>\n<td>DLS (Diamond Light Source\uff09<\/td>\n<\/tr>\n<tr>\n<td>Italy<\/td>\n<td>Elettra (Elettra Sincrotrone Trieste\uff09<\/td>\n<\/tr>\n<tr>\n<td>Swiss<\/td>\n<td>SwissFEL (Swiss Free Electron Laser\uff09<\/td>\n<\/tr>\n<tr>\n<td>Swiss<\/td>\n<td>SLS (Swiss Light Source\uff09<\/td>\n<\/tr>\n<tr>\n<td>Sweden<\/td>\n<td>MAX-\u2163 (MAX IV Laboratory\uff09<\/td>\n<\/tr>\n<tr>\n<td>Spain<\/td>\n<td>ALBA (ALBA Synchrotron\uff09<\/td>\n<\/tr>\n<tr>\n<td>Germany<\/td>\n<td>PETRAIII (Positron-Electron Tandem Ring Accelerator III\uff09<\/td>\n<\/tr>\n<tr>\n<td>Germany<\/td>\n<td>EU-XFEL (European XFEL (X-ray Free Electron Laser)\uff09<\/td>\n<\/tr>\n<tr>\n<td>Germany<\/td>\n<td>BESSY\u2161 (Berlin Electron Storage Ring Society for Synchrotron Radiation II\uff09<\/td>\n<\/tr>\n<tr>\n<td>France<\/td>\n<td>ESRF (European Synchrotron Radiation Facility\uff09<\/td>\n<\/tr>\n<tr>\n<td>France<\/td>\n<td>SOLEIL (Synchrotron SOLEIL \uff09<\/td>\n<\/tr>\n<tr>\n<td>China<\/td>\n<td>HALF (Hefei Advanced Light Facility\uff09<\/td>\n<\/tr>\n<tr>\n<td>China<\/td>\n<td>BSRF (Beijing Synchrotron Radiation Facility\uff09<\/td>\n<\/tr>\n<tr>\n<td>China<\/td>\n<td>HEPS (High Energy Photon Source\uff09<\/td>\n<\/tr>\n<tr>\n<td>China<\/td>\n<td>SSRF (Shanghai Synchrotron Radiation Facility\uff09<\/td>\n<\/tr>\n<tr>\n<td>China<\/td>\n<td>SHINE (Shanghai HIgh repetitioN rate XFEL and Extreme light facility\uff09<\/td>\n<\/tr>\n<tr>\n<td>China<\/td>\n<td>SXFEL (Shanghai Soft X-ray Free Electron Laser facility\uff09<\/td>\n<\/tr>\n<tr>\n<td>China<\/td>\n<td>S\u00b3FEL (Shenzhen Superconducting Soft-X-Ray Free Electron Laser \uff09<\/td>\n<\/tr>\n<tr>\n<td>Korea<\/td>\n<td>PAL-XFEL (Pohang Accelerator Laboratory X-ray Free Electron Laser\uff09<\/td>\n<\/tr>\n<tr>\n<td>Korea<\/td>\n<td>PLS\u2161 (Pohang Light Source II\uff09<\/td>\n<\/tr>\n<tr>\n<td>Taiwan<\/td>\n<td>TPS (Taiwan Photon Source\uff09<\/td>\n<\/tr>\n<tr>\n<td>Australia<\/td>\n<td>AS (Australian Synchrotron\uff09<\/td>\n<\/tr>\n<tr>\n<td>USA<\/td>\n<td>ALS (Advanced Light Source\uff09<\/td>\n<\/tr>\n<tr>\n<td>USA<\/td>\n<td>LCLS (Linac Coherent Light Source\uff09<\/td>\n<\/tr>\n<tr>\n<td>USA<\/td>\n<td>APS (Advanced Photon Source\uff09<\/td>\n<\/tr>\n<tr>\n<td>USA<\/td>\n<td>NSLS-II (National Synchrotron Light Source II\uff09<\/td>\n<\/tr>\n<tr>\n<td>Canada<\/td>\n<td>CLS (Canadian Light Source\uff09<\/td>\n<\/tr>\n<tr>\n<td>Brazil<\/td>\n<td>SIRIUS (Sirius Brazilian Synchrotron Light Source\uff09<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<\/div>\n<\/li>\n<\/ul>\n<\/section>\n","protected":false},"excerpt":{"rendered":"<p>Introduction of High-precision X-ray Mirrors JTEC CORPORATION&#8217;s High-precision X-ray Mirrors Synchrotron [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":4833,"menu_order":13,"comment_status":"closed","ping_status":"closed","template":"page-optical-detail.php","meta":[],"acf":[],"aioseo_notices":[],"_links":{"self":[{"href":"https:\/\/www.j-tec.co.jp\/english\/wp-json\/wp\/v2\/pages\/4887"}],"collection":[{"href":"https:\/\/www.j-tec.co.jp\/english\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/www.j-tec.co.jp\/english\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/www.j-tec.co.jp\/english\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.j-tec.co.jp\/english\/wp-json\/wp\/v2\/comments?post=4887"}],"version-history":[{"count":5,"href":"https:\/\/www.j-tec.co.jp\/english\/wp-json\/wp\/v2\/pages\/4887\/revisions"}],"predecessor-version":[{"id":7932,"href":"https:\/\/www.j-tec.co.jp\/english\/wp-json\/wp\/v2\/pages\/4887\/revisions\/7932"}],"up":[{"embeddable":true,"href":"https:\/\/www.j-tec.co.jp\/english\/wp-json\/wp\/v2\/pages\/4833"}],"wp:attachment":[{"href":"https:\/\/www.j-tec.co.jp\/english\/wp-json\/wp\/v2\/media?parent=4887"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}