{"id":8999,"date":"2020-06-22T18:00:00","date_gmt":"2020-06-22T09:00:00","guid":{"rendered":"https:\/\/www.icrr.u-tokyo.ac.jp\/?post_type=news&#038;p=8999"},"modified":"2020-06-22T16:45:12","modified_gmt":"2020-06-22T07:45:12","slug":"cta%e5%a4%a7%e5%8f%a3%e5%be%84%e6%9c%9b%e9%81%a0%e9%8f%a11%e5%8f%b7%e6%a9%9f%e3%80%80%e3%81%8b%e3%81%ab%e6%98%9f%e9%9b%b2%e3%83%91%e3%83%ab%e3%82%b5%e3%83%bc%e3%81%8b%e3%82%89%e3%81%ae%e4%bf%a1-2","status":"publish","type":"news","link":"https:\/\/www.icrr.u-tokyo.ac.jp\/en\/news\/8999\/","title":{"rendered":"CTA Prototype LST-\uff11 Detects Very High-Energy Emission from the Crab Pulsar"},"content":{"rendered":"\n<p><strong>La Palma, Canary Islands, Spain<\/strong> \u2013Between January and February 2020, the prototype Large-Sized Telescope (LST), the LST-\uff11, observed the Crab Pulsar, the neutron star at the centre of the Crab Nebula. The telescope, which is being commissioned on the CTA-North site on the island of La Palma in the Canary Islands, was conducting engineering runs to verify the telescope performance and adjust operating parameters.<\/p>\n\n\n\n<figure class=\"wp-block-image size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"775\" height=\"538\" src=\"https:\/\/www.icrr.u-tokyo.ac.jp\/prwps\/wp-content\/uploads\/8ca34bd4f89f3842a68395e14487592a.png\" alt=\"\" class=\"wp-image-9049\" srcset=\"https:\/\/www.icrr.u-tokyo.ac.jp\/prwps\/wp-content\/uploads\/8ca34bd4f89f3842a68395e14487592a.png 775w, https:\/\/www.icrr.u-tokyo.ac.jp\/prwps\/wp-content\/uploads\/8ca34bd4f89f3842a68395e14487592a-300x208.png 300w, https:\/\/www.icrr.u-tokyo.ac.jp\/prwps\/wp-content\/uploads\/8ca34bd4f89f3842a68395e14487592a-768x533.png 768w\" sizes=\"auto, (max-width: 775px) 100vw, 775px\" \/><figcaption>Figure 1. Multiwavelength view of the Crab Nebula and the Crab pulsar \u2013 the bright spot at the centre of the image. Credit: NASA, ESA, G. Dubner (IAFE, CONICET-University of Buenos Aires) et al.; A. Loll et al.; T. Temim et al.; F. Seward et al.; VLA\/NRAO\/AUI\/ NSF; Chandra\/ CXC; Spitzer\/JPL-Caltech; XMM-Newton\/ESA; Hubble\/STScI<\/figcaption><\/figure>\n\n\n\n<p>Pulsars are very rapid rotating and strongly magnetized neutron stars that emit light in the form of two beams, which can be observed from Earth only when passing our line of sight. While detecting the strong and steady emission or outbursts of gamma-ray sources with Imaging Atmospheric Cherenkov Telescopes (IACTs) has become routine, pulsars are much more challenging to detect due to their weak signals and the typical dominance of the foreground gamma-ray signal from the surrounding nebulae. Despite hundreds of observations hours by IACTs around the globe, only four pulsars emitting signals in the very high-energy gamma-ray regime have been discovered, so far. Now that the LST-\uff11 has shown that it can detect the Crab pulsar, it joins the field of telescopes capable of detecting gamma-ray pulsars, validating the timestamping\u00a0system and the low-energy performance of the telescope.<\/p>\n\n\n\n<p>&#8220;This milestone shows us that the LST-\uff11 is already performing at an extraordinary level, detecting a challenging source in record time,&#8221; says Masahiro Teshima, Director of Max-Planck-Institute for physics in Munich and Principal Investigator of LST. &#8220;Pulsars are one of the key scientific targets of the LSTs, and it&#8217;s exciting to imagine what we&#8217;ll be able to achieve when the telescope is fully commissioned and operational.\u201d<\/p>\n\n\n\n<p>The data set collected includes 11.4 hours from eight observation nights. Figure\uff12 shows the resulting phasogram, plotting the gamma-ray events as a function of the pulsar rotation phase. The flat background is a mixture of gamma-like isotropic cosmic rays and dominant irreducible steady emission from the Crab pulsar wind nebula. In the phase regions marked P1 and P2, one expects to see more gamma rays in these time intervals as gamma rays from the Crab pulsar are emitted towards the Earth. The signal detected with the LST-\uff11 is undeniably significant for phase P2, while the signal during P1 is still marginal. The animation in Figure\uff13 highlights the pulse behavior of the source during the different phases.<\/p>\n\n\n\n<figure class=\"wp-block-image size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"670\" src=\"https:\/\/www.icrr.u-tokyo.ac.jp\/prwps\/wp-content\/uploads\/96fe7a4ca1f1267a833ac5036263f798-1024x670.png\" alt=\"\" class=\"wp-image-9052\" srcset=\"https:\/\/www.icrr.u-tokyo.ac.jp\/prwps\/wp-content\/uploads\/96fe7a4ca1f1267a833ac5036263f798-1024x670.png 1024w, https:\/\/www.icrr.u-tokyo.ac.jp\/prwps\/wp-content\/uploads\/96fe7a4ca1f1267a833ac5036263f798-300x196.png 300w, https:\/\/www.icrr.u-tokyo.ac.jp\/prwps\/wp-content\/uploads\/96fe7a4ca1f1267a833ac5036263f798-768x503.png 768w, https:\/\/www.icrr.u-tokyo.ac.jp\/prwps\/wp-content\/uploads\/96fe7a4ca1f1267a833ac5036263f798-1536x1006.png 1536w, https:\/\/www.icrr.u-tokyo.ac.jp\/prwps\/wp-content\/uploads\/96fe7a4ca1f1267a833ac5036263f798.png 1726w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><figcaption>Figure 2: Phasogram of Crab Pulsar as measured by the LST-\uff11. The pulsar is known to emit pulses of gamma rays during phases P1 and P2. The shown significance is calculated considering source emission from those phases (in red) and background events from phases (in grey). Credit: LST Collaboration<\/figcaption><\/figure>\n\n\n\n<figure class=\"wp-block-video\"><video controls src=\"https:\/\/www.icrr.u-tokyo.ac.jp\/prwps\/wp-content\/uploads\/Pulsar_movie.m4v\"><\/video><figcaption>Figure 3: Animation of Crab pulsar\u2019s emission as seen by the LST-\uff11 along its different phases, Credit: Rub\u00e9n L\u00f3pez-Coto.<\/figcaption><\/figure>\n\n\n\n<figure class=\"wp-block-gallery columns-2 is-cropped wp-block-gallery-1 is-layout-flex wp-block-gallery-is-layout-flex\"><ul class=\"blocks-gallery-grid\"><li class=\"blocks-gallery-item\"><figure><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"755\" src=\"https:\/\/www.icrr.u-tokyo.ac.jp\/prwps\/wp-content\/uploads\/f2-1-1024x755.png\" alt=\"\" data-id=\"9007\" data-link=\"https:\/\/www.icrr.u-tokyo.ac.jp\/en\/news\/8999\/f2-1\/\" class=\"wp-image-9007\" srcset=\"https:\/\/www.icrr.u-tokyo.ac.jp\/prwps\/wp-content\/uploads\/f2-1-1024x755.png 1024w, https:\/\/www.icrr.u-tokyo.ac.jp\/prwps\/wp-content\/uploads\/f2-1-300x221.png 300w, https:\/\/www.icrr.u-tokyo.ac.jp\/prwps\/wp-content\/uploads\/f2-1-768x566.png 768w, https:\/\/www.icrr.u-tokyo.ac.jp\/prwps\/wp-content\/uploads\/f2-1-1536x1132.png 1536w, https:\/\/www.icrr.u-tokyo.ac.jp\/prwps\/wp-content\/uploads\/f2-1.png 1666w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/figure><\/li><li class=\"blocks-gallery-item\"><figure><img loading=\"lazy\" decoding=\"async\" width=\"743\" height=\"494\" src=\"https:\/\/www.icrr.u-tokyo.ac.jp\/prwps\/wp-content\/uploads\/d8d582d74c77d59a7e38b2dfabbc25e5.png\" alt=\"\" data-id=\"9051\" data-full-url=\"https:\/\/www.icrr.u-tokyo.ac.jp\/prwps\/wp-content\/uploads\/d8d582d74c77d59a7e38b2dfabbc25e5.png\" data-link=\"https:\/\/www.icrr.u-tokyo.ac.jp\/en\/news\/8999\/d8d582d74c77d59a7e38b2dfabbc25e5\/\" class=\"wp-image-9051\" srcset=\"https:\/\/www.icrr.u-tokyo.ac.jp\/prwps\/wp-content\/uploads\/d8d582d74c77d59a7e38b2dfabbc25e5.png 743w, https:\/\/www.icrr.u-tokyo.ac.jp\/prwps\/wp-content\/uploads\/d8d582d74c77d59a7e38b2dfabbc25e5-300x199.png 300w\" sizes=\"auto, (max-width: 743px) 100vw, 743px\" \/><\/figure><\/li><\/ul><figcaption class=\"blocks-gallery-caption\">Figure 4: Pictures of LST members during online LST general meeting in June 2020. Right: The LST-\uff11 in La Palma, Credit: Tomohiro Inada<\/figcaption><\/figure>\n\n\n\n<p><strong>About the LST<\/strong><\/p>\n\n\n\n<p>The <a href=\"https:\/\/www.cta-observatory.org\/project\/technology\/lst\/\">Large-Sized Telescope<\/a> (LST) is one of three types of telescope to be built to cover CTA\u2019s full energy range (20 GeV to 300 TeV). LSTs arranged at the centre of both the northern and southern hemisphere arrays will cover the low-energy sensitivity between 20 and 150 GeV. Each LST is a giant 23 metre diameter telescope with a mirror area of about 400 square meters and a fine pixelized camera made of 1855 light sensors capable of detecting individual photons with high efficiency. Although the LST stands 45 metres tall and weighs around 100 tonnes, it is extremely nimble, with the ability to re-position within 20 seconds to capture brief, low-energy gamma-ray signals. Both the fast re-positioning speed and the low energy threshold provided by the LSTs are critical for CTA\u2019s studies of transient gamma-ray sources in our own Galaxy and for the study of active galactic nuclei and gamma-ray bursts at high redshift.&nbsp;<\/p>\n\n\n\n<p>The LST collaboration, consists of more than 200 scientists from 11 countries: Brazil, Bulgaria, Croatia, France, Germany, India, Italy, Japan, Poland, Spain and Switzerland. The LST-1, the first telescope constructed on a CTA site, was <a href=\"https:\/\/www.cta-observatory.org\/lst-1_inauguration\/\">inaugurated in October 2018<\/a> and has been undergoing commissioning testing ever since. Soon after the inauguration, the <a href=\"https:\/\/www.cta-observatory.org\/lst-prototype-records-its-first-light\/\">prototype detected its \u2018first light\u2019<\/a> on the evening of 14-15 December, and it <a href=\"https:\/\/www.cta-observatory.org\/lst1-detects-first-gamma-ray-signal\/\">detected its first gamma-ray signal from the Crab Nebula in November 2019<\/a> on its first attempt.<\/p>\n\n\n\n<p>The LST-\uff11 recently <a href=\"https:\/\/www.cta-observatory.org\/lst1-passes-cdr\/\">passed the Critical Design Review<\/a> (CDR) by the CTA Observatory (CTAO), the first CTA element to pass such a review. The telescope is foreseen to become the first CTAO telescope once the CDR is closed out and it is formally accepted by the CTAO, which is expected in 2021.<\/p>\n\n\n\n<p><strong>About CTA<\/strong><\/p>\n\n\n\n<p>The <a href=\"https:\/\/www.cta-observatory.org\/\">Cherenkov Telescope Array<\/a> (CTA) is a global initiative to build the world\u2019s largest and most sensitive high-energy gamma-ray observatory with tens of &nbsp;telescopes planned on two sites: one in the northern hemisphere on the island of La Palma, Spain, and the other in the southern hemisphere near Paranal, Chile. CTA will be the foremost global observatory for very high-energy gamma-ray astronomy over the next decade and beyond and will be the first ground-based gamma-ray astronomy observatory open to the world-wide astronomical and particle physics communities. CTA will address some of the greatest mysteries in astrophysics, detecting gamma rays with an unprecedented sensitivity and expanding the cosmic source catalogue tenfold. CTA is a unique, ambitious large-scale infrastructure that will expand observations up to a region of the spectrum that has never been seen, opening an entirely new window to our Universe. The CTAO gGmbH serves to prepare the design and implementation of the CTA Observatory. The CTAO works in close cooperation with the CTA Consortium composed of 1500+ members from 31 countries, which is responsible for directing the science goals of the Observatory and is involved in the design and supply of instrumentation. The CTAO is governed by a <a href=\"https:\/\/www.cta-observatory.org\/about\/governance\/\">council of shareholders<\/a> from 11 countries and one intergovernmental organization, as well as associate members from two countries.<\/p>\n\n\n\n<p><strong>Contacts:<\/strong><\/p>\n\n\n\n<p>Masahiro Teshima<br>LST Principal Investigator<br>MPP Munich and ICRR University of Tokyo<br><a href=\"mailto:mteshima@mpp.mpg.de\">mteshima@mpp.mpg.de<\/a><\/p>\n\n\n\n<p>Juan Cortina<br>LST Co-Principal Investigator<br>CIEMAT, Madrid<br><a href=\"mailto:cortina@ciemat.es\">cortina@ciemat.es<\/a><\/p>\n\n\n\n<p>Daniel Mazin<br>LST Project Manager<br>ICRR University of Tokyo and MPP Munich<br><a href=\"mailto:mazin@icrr.u-tokyo.ac.jp\">mazin@icrr.u-tokyo.ac.jp<\/a><\/p>\n\n\n\n<p>Megan Grunewald<br>Outreach and Communications Officer<br>CTAO gGmbH<br><a href=\"mailto:mgrunewald@cta-observatory.org\">mgrunewald@cta-observatory.org<\/a><\/p>\n\n\n\n<p><\/p>\n","protected":false},"excerpt":{"rendered":"<p>La Palma, Canary Islands, Spain \u2013Between January and February 2020, the prototype Large-Sized Telescope (LST),&#8230;<\/p>\n","protected":false},"featured_media":9049,"parent":0,"template":"","taxo_news":[18],"tag_news":[],"class_list":["post-8999","news","type-news","status-publish","has-post-thumbnail","hentry","taxo_news-topics","en-US"],"aioseo_notices":[],"_links":{"self":[{"href":"https:\/\/www.icrr.u-tokyo.ac.jp\/wp-json\/wp\/v2\/news\/8999","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.icrr.u-tokyo.ac.jp\/wp-json\/wp\/v2\/news"}],"about":[{"href":"https:\/\/www.icrr.u-tokyo.ac.jp\/wp-json\/wp\/v2\/types\/news"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.icrr.u-tokyo.ac.jp\/wp-json\/wp\/v2\/media\/9049"}],"wp:attachment":[{"href":"https:\/\/www.icrr.u-tokyo.ac.jp\/wp-json\/wp\/v2\/media?parent=8999"}],"wp:term":[{"taxonomy":"taxo_news","embeddable":true,"href":"https:\/\/www.icrr.u-tokyo.ac.jp\/wp-json\/wp\/v2\/taxo_news?post=8999"},{"taxonomy":"tag_news","embeddable":true,"href":"https:\/\/www.icrr.u-tokyo.ac.jp\/wp-json\/wp\/v2\/tag_news?post=8999"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}