{"id":174917,"date":"2016-01-14T18:00:00","date_gmt":"2016-01-14T15:00:00","guid":{"rendered":"http:\/\/www.fyysika.ee\/?guid=a4f4a1b65b4f315e343ef941e18204c2"},"modified":"2016-01-14T18:00:00","modified_gmt":"2016-01-14T15:00:00","slug":"anomalous-depletion-of-pore-confined-carbon-dioxide-upon-cooling-below-the-bulk-triple-point-an-iin-situi-neutron-diffraction-study","status":"publish","type":"post","link":"https:\/\/www.fyysika.ee\/?p=174917","title":{"rendered":"Anomalous Depletion of Pore-Confined Carbon Dioxide upon Cooling below the Bulk Triple Point: An &lt;i&gt;In Situ&lt;\/i&gt; Neutron Diffraction Study"},"content":{"rendered":"<p>Author(s): K.\u2009L. Stefanopoulos, F.\u2009K. Katsaros, Th.\u2009A. Steriotis, A.\u2009A. Sapalidis, M. Thommes, D.\u2009T. Bowron, and T.\u2009G.\u2009A. Youngs<\/p>\n<p>Neutron scattering experiments indicate that CO<math xmlns=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\"><msub><mrow><\/mrow><mn>2<\/mn><\/msub><\/math> confined in nanopores does not freeze when cooled below the triple point but instead vacates the pores and solidifies in the bulk. Upon reheating the CO<math xmlns=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\"><msub><mrow><\/mrow><mn>2<\/mn><\/msub><\/math> refills the nanopores.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/d22izw7byeupn1.cloudfront.net\/journals\/PRL\/key_images\/10.1103\/PhysRevLett.116.025502.png\" width=\"200\" height=\"100\"><\/p>\n<p>[Phys. Rev. Lett. 116, 025502] Published Thu Jan 14, 2016<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Author(s): K.&thinsp;L. Stefanopoulos, F.&thinsp;K. Katsaros, Th.&thinsp;A. Steriotis, A.&thinsp;A. Sapalidis, M. Thommes, D.&thinsp;T. Bowron, and T.&thinsp;G.&thinsp;A. Youngs<\/p>\n<p>Neutron scattering experiments indicate that CO2 confined in nanopores does not freeze when cooled below the triple point but instead vacates the pores and solidifies in the bulk. Upon reheating the CO2 refills the nanopores.<\/p>\n<p><img decoding=\"async\" src=\"http:\/\/d22izw7byeupn1.cloudfront.net\/journals\/PRL\/key_images\/10.1103\/PhysRevLett.116.025502.png\" width=\"200\" height='\"100\"'><br \/>[Phys. Rev. Lett. 116, 025502] Published Thu Jan 14, 2016<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"_genesis_hide_title":false,"_genesis_hide_breadcrumbs":false,"_genesis_hide_singular_image":false,"_genesis_hide_footer_widgets":false,"_genesis_custom_body_class":"","_genesis_custom_post_class":"","_genesis_layout":"","footnotes":""},"categories":[182],"tags":[],"class_list":{"0":"post-174917","1":"post","2":"type-post","3":"status-publish","4":"format-standard","6":"category-rss-teadus","7":"entry"},"_links":{"self":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/174917","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=174917"}],"version-history":[{"count":0,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/174917\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=174917"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=174917"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=174917"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}