{"id":18,"date":"2019-09-30T20:53:12","date_gmt":"2019-09-30T20:53:12","guid":{"rendered":"http:\/\/annalisadecia.com\/site\/?page_id=18"},"modified":"2019-10-14T10:51:15","modified_gmt":"2019-10-14T10:51:15","slug":"slsn","status":"publish","type":"page","link":"https:\/\/annalisadecia.com\/site\/slsn\/","title":{"rendered":"Superluminous Supernovae"},"content":{"rendered":"\n<p>Superluminous Supernovae (SLSNe) are a recent and rare class of supernovae that are more than 10 times higher than normal SNe. The inferred energetics of SLSNe require processes that are different from classical SNe, probably involving either extremely massive stars with likely very low metallicities, interaction with circumstellar material, or additional energy input from a central engine such as a magnetar or accretion onto the compact remnant. The physical mechanism powering these explosions is poorly understood and hotly debated. See <a rel=\"noreferrer noopener\" aria-label=\"Gal-Yam 2019 (opens in a new tab)\" href=\"https:\/\/ui.adsabs.harvard.edu\/abs\/2019ARA%26A..57..305G\/abstract\" target=\"_blank\">Gal-Yam 2019<\/a> for a review on SLSNe.<\/p>\n\n\n\n<p class=\"has-text-color has-light-green-cyan-color\"><strong>The luminosities and light curves of SLSNe<\/strong><\/p>\n\n\n\n<p>In <a rel=\"noreferrer noopener\" aria-label=\"De Cia et al. 2018b (opens in a new tab)\" href=\"https:\/\/ui.adsabs.harvard.edu\/abs\/2018ApJ...860..100D\/abstract\" target=\"_blank\">De Cia et al. 2018b<\/a> we characterized the light-curve properties of the largest and homogeneous sample of SLSNe-I (H-poor), from the (i)Palomar Transient Factory. We characterized the distribution of SLSN peak luminosities and found that H-poor SLSNe have absolute magnitudes -22 &lt;~ M &lt;\u223c \u221220 mag (rest-frame g-band). This is brighter than SNe Ib\/c and SNe Ic-BL, on average, by about 4 and 2 mag, respectively. The rise timescales are longer for SLSNe-I than for normal SNe Ib\/c. SLSNe-I decay with a wide range of slopes, with no obvious gap between rapidly declining and slowly declining events. At late times, the SLSN-I light curves slow down and cluster around the 56Co radioactive decay rate.<\/p>\n\n\n\n<div class=\"wp-block-image\"><figure class=\"aligncenter is-resized\"><img loading=\"lazy\" src=\"https:\/\/annalisadecia.com\/site\/wp-content\/uploads\/2019\/10\/SLSN-peak-mag-distribution-Annalisa-De-Cia-769x1024.jpg\" alt=\"\" class=\"wp-image-217\" width=\"454\" height=\"604\" srcset=\"https:\/\/annalisadecia.com\/site\/wp-content\/uploads\/2019\/10\/SLSN-peak-mag-distribution-Annalisa-De-Cia-769x1024.jpg 769w, https:\/\/annalisadecia.com\/site\/wp-content\/uploads\/2019\/10\/SLSN-peak-mag-distribution-Annalisa-De-Cia-225x300.jpg 225w, https:\/\/annalisadecia.com\/site\/wp-content\/uploads\/2019\/10\/SLSN-peak-mag-distribution-Annalisa-De-Cia-768x1023.jpg 768w, https:\/\/annalisadecia.com\/site\/wp-content\/uploads\/2019\/10\/SLSN-peak-mag-distribution-Annalisa-De-Cia.jpg 885w\" sizes=\"(max-width: 454px) 100vw, 454px\" \/><figcaption>The peak-magnitude distribution of SLSNe and Type Ib\/c SNe from PTF <br>(De Cia et al. 2018)<\/figcaption><\/figure><\/div>\n\n\n\n<p class=\"has-text-color has-light-green-cyan-color\"><strong>The host galaxies of SLSNe<\/strong><\/p>\n\n\n\n<p>SLSNe-I explode in low-mass and low-metallicity galaxies, with a heavily suppressed rate in galaxies with metallicities above half solar. On the other hand, SLSNe-II (hydrogen-rich) can explode in galaxies with a wide range of masses and metallicities. [<a rel=\"noreferrer noopener\" aria-label=\"Perley, Quimby, Yan, Vreeswijk, De Cia et al. 2016 (opens in a new tab)\" href=\"https:\/\/ui.adsabs.harvard.edu\/abs\/2016ApJ...830...13P\/abstract\" target=\"_blank\">Perley, Quimby, Yan, Vreeswijk, De Cia et al. 2016<\/a>, SLSNe host galaxies from iPTF]<\/p>\n\n\n\n<p>In <a rel=\"noreferrer noopener\" aria-label=\"Cikota, De Cia et al. 2017 (opens in a new tab)\" href=\"https:\/\/ui.adsabs.harvard.edu\/abs\/2017MNRAS.469.4705C\/abstract\" target=\"_blank\">Cikota, De Cia et al. 2017<\/a> we did a spatially resolved analysis of two nearby SLSNe-I (PTF 11hrq and PTF 12dam), using HST and VLT\/MUSE data. Both host galaxies have overall blue colors, however the SLSNe did not explode in the bluest parts. PTF 11hrq exploded close to a region with disturbed kinematics, bluer color, stronger [O III], and lower metallicity, and its host galaxy is likely interacting with a companion. PTF 12dam exploded in one of the brightest pixels of a clumpy sturbursting galaxy with a tidal tail. These results suggest that these SLSNe may have been produced by stars generated in episodes of starformation triggered by interaction.\u00a0<\/p>\n\n\n\n<div class=\"wp-block-image\"><figure class=\"aligncenter is-resized\"><img loading=\"lazy\" src=\"https:\/\/annalisadecia.com\/site\/wp-content\/uploads\/2019\/10\/PTF-12dam-host-galaxy-HST-Annalisa-De-Cia.jpg\" alt=\"\" class=\"wp-image-218\" width=\"443\" height=\"333\" srcset=\"https:\/\/annalisadecia.com\/site\/wp-content\/uploads\/2019\/10\/PTF-12dam-host-galaxy-HST-Annalisa-De-Cia.jpg 681w, https:\/\/annalisadecia.com\/site\/wp-content\/uploads\/2019\/10\/PTF-12dam-host-galaxy-HST-Annalisa-De-Cia-300x226.jpg 300w\" sizes=\"(max-width: 443px) 100vw, 443px\" \/><figcaption>The host galaxy of PTF 12dam, HST WFC3\/UVIS composite. The SLSN explosion site is encircled  (see Cikota et al. 2017)<\/figcaption><\/figure><\/div>\n\n\n\n<p class=\"has-text-color has-light-green-cyan-color\"><strong>The ISM in SLSN host galaxies<\/strong><\/p>\n\n\n\n<p>Mid\/high-resolution spectra of SLSNe covering the rest-frame UV are scarse, but the ISM of SLSNe-I hosts seems to show very narrow absorption lines, hinting at small galaxy masses. These metal lines have very low column densities or equivalent widths (<a rel=\"noreferrer noopener\" aria-label=\"Vreeswijk, Savaglio, Gal-Yam, De Cia et al. 2014 (opens in a new tab)\" href=\"https:\/\/ui.adsabs.harvard.edu\/abs\/2014ApJ...797...24V\/abstract\" target=\"_blank\">Vreeswijk, Savaglio, Gal-Yam, De Cia et al. 2014<\/a>). The far-UV HST spectrum of the nearby SN 2017egm showed an HI column of ~10^19 cm\u22122, which is extremely low compared to other starforming galaxies, such as GRB hosts, and a solar or higher metallicity of the host galaxy (<a rel=\"noreferrer noopener\" aria-label=\"Yan, Perley, De Cia et al. 2018 (opens in a new tab)\" href=\"https:\/\/ui.adsabs.harvard.edu\/abs\/2018ApJ...858...91Y\/abstract\" target=\"_blank\">Yan, Perley, De Cia et al. 2018<\/a>).<\/p>\n\n\n\n<p class=\"has-text-color has-light-green-cyan-color\"><strong>The spectra of SLSNe<\/strong><\/p>\n\n\n\n<p>In <a rel=\"noreferrer noopener\" aria-label=\"Quimby, De Cia, et al. 2018 (opens in a new tab)\" href=\"https:\/\/ui.adsabs.harvard.edu\/abs\/2018ApJ...855....2Q\/abstract\" target=\"_blank\">Quimby, De Cia, et al. 2018<\/a> we characterized the spectral properties of SLSNe-I from the (i)Palomar Transient Factory. We found that SLSNe-I can be spectrally classified, e.g. they can be distinguished from normal supernovae based on their spectral features.\u00a0<br><\/p>\n","protected":false},"excerpt":{"rendered":"<p>Superluminous Supernovae (SLSNe) are a recent and rare class of supernovae that are more than 10 times higher than normal SNe. The inferred energetics of SLSNe require processes that are different from classical SNe, probably involving either extremely massive stars with likely very low metallicities, interaction with circumstellar material, or additional energy input from a &hellip; <\/p>\n<p class=\"link-more\"><a href=\"https:\/\/annalisadecia.com\/site\/slsn\/\" class=\"more-link\">Continue reading<span class=\"screen-reader-text\"> &#8220;Superluminous Supernovae&#8221;<\/span><\/a><\/p>\n","protected":false},"author":1,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":[],"_links":{"self":[{"href":"https:\/\/annalisadecia.com\/site\/wp-json\/wp\/v2\/pages\/18"}],"collection":[{"href":"https:\/\/annalisadecia.com\/site\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/annalisadecia.com\/site\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/annalisadecia.com\/site\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/annalisadecia.com\/site\/wp-json\/wp\/v2\/comments?post=18"}],"version-history":[{"count":11,"href":"https:\/\/annalisadecia.com\/site\/wp-json\/wp\/v2\/pages\/18\/revisions"}],"predecessor-version":[{"id":300,"href":"https:\/\/annalisadecia.com\/site\/wp-json\/wp\/v2\/pages\/18\/revisions\/300"}],"wp:attachment":[{"href":"https:\/\/annalisadecia.com\/site\/wp-json\/wp\/v2\/media?parent=18"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}