{"id":27295,"date":"2012-05-07T13:04:25","date_gmt":"2012-05-07T10:04:25","guid":{"rendered":"http:\/\/www.fyysika.ee\/uudised\/?p=27295"},"modified":"2012-05-07T13:04:25","modified_gmt":"2012-05-07T10:04:25","slug":"grafeeni-akustiline-alternatiiv","status":"publish","type":"post","link":"https:\/\/www.fyysika.ee\/?p=27295","title":{"rendered":"Grafeeni akustiline alternatiiv"},"content":{"rendered":"<p><strong>See v\u00f5ib k\u00f5lada k\u00fcll veidi kujuteldamatuna, kuid kaks Hispaania f\u00fc\u00fcsikut valmistasid grafeeni akustilise alternatiivi lihtsalt plastmasslehte puuritud k\u00e4rjelise struktuuri abil. Daniel Torrent ja Jos\u00e9 S\u00e1nchez-Dehesa Valencia Pol\u00fctehnilisest \u00dclikoolist v\u00e4idavad, et nad t\u00e4heldasid ,,Diraci koonuseid&#8221; &#8211; grafeenile iseloomuliku elektronriba omadust &#8211; helilainetes, mis plastiku pinnal levivad. Kuigi veel on vaja teha palju t\u00f6\u00f6d, enne kui sellest nii\u00f6elda grafeeni akustilisest analoogist praktilisi rakendusi saab teha, saaks seda kasutada akustiliste s\u00fcsteemide parandamisel v\u00f5i isegi grafeeni paremaks m\u00f5istmiseks.<\/strong><\/p>\n<div id=\"attachment_27296\" style=\"width: 310px\" class=\"wp-caption alignleft\"><a href=\"http:\/\/www.fyysika.ee\/uudised\/wp-content\/uploads\/2012\/05\/dirac-cones.jpg\"><img loading=\"lazy\" decoding=\"async\" aria-describedby=\"caption-attachment-27296\" class=\"size-medium wp-image-27296\" title=\"dirac-cones\" src=\"http:\/\/www.fyysika.ee\/uudised\/wp-content\/uploads\/2012\/05\/dirac-cones-300x204.jpg\" alt=\"\" width=\"300\" height=\"204\" srcset=\"https:\/\/www.fyysika.ee\/wp-content\/uploads\/2012\/05\/dirac-cones-300x204.jpg 300w, https:\/\/www.fyysika.ee\/wp-content\/uploads\/2012\/05\/dirac-cones-250x170.jpg 250w, https:\/\/www.fyysika.ee\/wp-content\/uploads\/2012\/05\/dirac-cones.jpg 400w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><\/a><p id=\"caption-attachment-27296\" class=\"wp-caption-text\">Diraci koonuste kuulamine pleksiklaasil.<\/p><\/div>\n<p>Torrent ja S\u00e1nchez-Dehesa otsustasid uurida, kas Diraci koonustele leidub ka akustiline vastand. Esmalt arvutasid nad v\u00e4lja k\u00e4rjelise struktuuriga pleksiklaasi pinnal levivate helilainete omadused. Eriti huvitatud olid teadlased lainete dispersiooni suhtest, mis on suhe helilaine energia ning impulsi vahel, kirjutab <a href=\"http:\/\/physicsworld.com\/cws\/article\/news\/2012\/may\/02\/acoustic-analogue-to-graphene-announced\">Physicsworld.com<\/a>.<\/p>\n<p>Nii Diraci punkti kui ka Diraci koonuste olemasolu n\u00e4idanud arvutustest selgus, et pinna helilaineid saab k\u00f5ige paremini kirjeldada Diraci v\u00f5rrandiga. Antud mudel ennustab kindla Diraci sageduse ja kiirusega pinna-helilainete olemasolu &#8211; sellised lained peaksid ainet l\u00e4bima kergesti ning praktiliselt ilma hajumiseta.<\/p>\n<p>Nende lainete leidmiseks v\u00f5tsid teadlased 300 x 100 millimeetrise pleksiklaasi t\u00fcki ning puurisid sellesse 1113 auku. Iga augu diameeter oli 3mm ning s\u00fcgavus 3,33 mm. Nagu pildilt ka n\u00e4ha v\u00f5ib, siis oli tulemuseks suure hulga materjali eemaldamine, j\u00e4ttes alles k\u00e4rje-sarnase struktuuri.<\/p>\n<p>Seej\u00e4rel \u00fchendati pleksiklaas k\u00f5lariga ning heli m\u00f5\u00f5deti kahest kohast mikrofonidega. Helideks olid l\u00fchikesed heliimpulsid sagedusega 22 kHz ning impulsi intervall umbes 5kHz &#8211; need n\u00e4itajad valiti seet\u00f5ttu, et materjali ennustatud Diraci sagedus pidi j\u00e4\u00e4ma sellesse vahemikku.<\/p>\n<p>Torrent ja S\u00e1nchez-Dehesa leidsid, et faasiviivis &#8211; igasse mikrofoni j\u00f5udvate helilainete aegade vahe &#8211; langess teravalt umbes 22 kHz juures, mis teadlaste s\u00f5nul langeb kokku Diraci koonuse tipuga. Lisaks m\u00e4rkasid nad, et ka arvutatud lainete dispersioonisuhe n\u00e4itas Diraci koonuse tippu umbes 22 kHz juures. T\u00e4psemalt leiti Diraci punkti l\u00e4heduses eksisteeriv impulsi ja energia lineaarne suhe, mis on Diraci koonuse heaks m\u00e4\u00e4rajaks.<\/p>\n<p>,,See on v\u00e4ga muljetavaldav, sest teooriast tulenevalt v\u00f5iks arvata, et sellise Diraci koonuse n\u00e4gemine akustilises s\u00fcsteemis n\u00f5uaks materjali v\u00e4ga t\u00e4pset kuju ja ruumala,&#8221; lausus MIT teadlane Nicholas Fang uurimuse kohta.<\/p>\n<p>Nii Fangi kui ka t\u00f6\u00f6 autorite meelest on veel liiga vara \u00f6elda, kas Diraci koonustega materjale saaks ka praktikas rakendada. \u00dcheks v\u00f5imaluseks v\u00f5iks aga olla kasutada neid akustilistes l\u00e4\u00e4tsedes, mis suudavad koguda heli ilma seda peegeldamata.<\/p>\n<p><a href=\"http:\/\/physicsworld.com\/cws\/article\/news\/2012\/may\/02\/acoustic-analogue-to-graphene-announced\">Allikas<\/a><\/p>\n<p>Teadusartikkel: &#8220;<a href=\"http:\/\/prl.aps.org\/abstract\/PRL\/v108\/i17\/e174301\">Acoustic Analogue of Graphene: Observation of Dirac Cones in Acoustic Surface Waves<\/a>&#8220;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>See v\u00f5ib k\u00f5lada k\u00fcll veidi kujuteldamatuna, kuid kaks Hispaania f\u00fc\u00fcsikut valmistasid grafeeni akustilise alternatiivi lihtsalt plastmasslehte puuritud k\u00e4rjelise struktuuri abil. Daniel Torrent ja Jos\u00e9 S\u00e1nchez-Dehesa Valencia Pol\u00fctehnilisest \u00dclikoolist v\u00e4idavad, et nad t\u00e4heldasid ,,Diraci koonuseid&#8221; &#8211; grafeenile iseloomuliku elektronriba omadust &#8211; helilainetes, mis plastiku pinnal levivad. Kuigi veel on vaja teha palju t\u00f6\u00f6d, enne kui sellest [&hellip;]<\/p>\n","protected":false},"author":32,"featured_media":27296,"comment_status":"open","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":[31,16],"tags":[45,110],"class_list":{"0":"post-27295","1":"post","2":"type-post","3":"status-publish","4":"format-standard","5":"has-post-thumbnail","7":"category-rakenduslik-teadus","8":"category-teadusuudis","9":"tag-grafeengrafaan","10":"tag-materjal","11":"entry"},"_links":{"self":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/27295","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\/32"}],"replies":[{"embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=27295"}],"version-history":[{"count":0,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/27295\/revisions"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/media\/27296"}],"wp:attachment":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=27295"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=27295"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=27295"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}