{"id":20280,"date":"2021-03-23T14:28:20","date_gmt":"2021-03-23T14:28:20","guid":{"rendered":"https:\/\/www.upjs.sk\/prirodovedecka-fakulta\/pracoviska\/ufv\/vv\/infr\/laboratorium-kvantoveho-magnetizmu\/"},"modified":"2022-11-13T21:31:07","modified_gmt":"2022-11-13T20:31:07","slug":"laboratorium-kvantoveho-magnetizmu","status":"publish","type":"cpt_pracoviska","link":"https:\/\/www.upjs.sk\/prirodovedecka-fakulta\/pracoviska\/ustavy-pf\/ufv\/vv\/infr\/laboratorium-kvantoveho-magnetizmu\/","title":{"rendered":"Laborat\u00f3rium kvantov\u00e9ho magnetizmu"},"content":{"rendered":"

Osoba zodpovedn\u00e1 za laborat\u00f3rium, kontakt, financovanie<\/strong><\/h4>\n

Laborat\u00f3rium kvantov\u00e9ho magnetizmu Pr\u00edrodovedeckej fakulty UPJ\u0160 bolo vybudovan\u00e9 v r\u00e1mci rie\u0161enia projektu zo \u0161truktur\u00e1lnych fondov \u201eExtrem – Dobudovanie Centra pokroko\u010dil\u00fdch fyzik\u00e1lnych \u0161t\u00fadi\u00ed materi\u00e1lov v extr\u00e9mnych podmienkach\u201d (EU ERDF European Regional Development Fund, Grant No. ITMS 26220120047<\/strong>).
Prof. RNDr. Alexander Feher, DrSc – alexander.feher@upjs.sk
Prof. Ing. Martin Orend\u00e1\u010d, CSc. – martin.orendac@upjs.sk
doc. RNDr. Al\u017ebeta Orend\u00e1\u010dov\u00e1, DrSc – alzbeta.orendacova@upjs.sk
RNDr. Erik Cizmar, PhD. – erik.cizmar@upjs.sk
RNDr. Marcela Kaj\u0148akov\u00e1, PhD. – marcela.kajnakova@upjs.sk
\u00a0<\/p>\n

Umiestnenie laborat\u00f3ria<\/strong><\/h4>\n

Laborat\u00f3rium kvantov\u00e9ho magnetizmu je umiestnen\u00e9 v priestoroch \u00dastavu fyzik\u00e1lnych vied Pr\u00edrodovedeckej fakulty UPJ\u0160 v Ko\u0161iciach, Park Angelinum 9.
\u00a0<\/p>\n

Charakteristika<\/strong><\/h4>\n

Zameran\u00edm Laborat\u00f3ria je \u0161t\u00fadium prejavov kvantov\u00e9ho magnetizmu v r\u00f4znych typoch materi\u00e1lov s r\u00f4znou mierou elektrickej vodivosti, po\u010dn\u00fac od magnetick\u00fdch izol\u00e1torov cez magnetick\u00e9 polovodi\u010de a kovy na b\u00e1ze i\u00f3nov prechodov\u00fdch kovov, vz\u00e1cnych zem\u00edn a organick\u00fdch materi\u00e1lov. \u0160tuduj\u00fa sa materi\u00e1ly s r\u00f4znou magnetickou dimenziou (nula rozmern\u00e9 – magnetick\u00e9 klastre resp. molekulov\u00e9 magnety, jednorozmern\u00e9 – spinov\u00e9 re\u0165azce a rebr\u00edky, dvojrozmern\u00e9 – napr. magnetik\u00e1 na \u0161tvorcovej, trojuholn\u00edkovej mrie\u017eke, trojrozmern\u00e9 – spinov\u00e9 \u013eady, spinov\u00e1 kubick\u00e1 mrie\u017eka, at\u010f.). Navy\u0161e, pri v\u0161etk\u00fdch typoch uveden\u00fdch materi\u00e1lov je d\u00f4le\u017eit\u00e1 spinov\u00e1 dimenzia, t.j. ve\u013ekos\u0165 a typ magnetickej anizotropie, ktor\u00e1 stabilizuje orient\u00e1ciu magnetick\u00fdch momentov v priestore, \u010do ovplyv\u0148uje napr. formovanie magneticky usporiadanej f\u00e1zy. Variabilita uveden\u00fdch fyzik\u00e1lnych vlastnost\u00ed vedie na mno\u017estvo nekonven\u010dn\u00fdch javov ako je frustr\u00e1cia, kvantov\u00e9 v\u00edry, stav spinov\u00e9ho \u013eadu, spinovej kvapaliny, vlny spinovej hustoty at\u010f. Tieto javy \u0161pecifick\u00fdm sp\u00f4sobom ovplyv\u0148uj\u00fa vytv\u00e1ranie termodynamickej rovnov\u00e1hy medzi magnetick\u00fdm syst\u00e9mom a okol\u00edm (tvoren\u00fdm mrie\u017ekou a vodivostn\u00fdmi elektr\u00f3nmi) ke\u010f magnetick\u00fd syst\u00e9m alebo jeho okolie vyvedieme z rovnov\u00e1hy aplik\u00e1ciou elektromagnetick\u00e9ho \u017eiarenia, tepeln\u00fdm pulzom, pr\u00edpadne striedav\u00fdm magnetick\u00fdm po\u013eom. Okrem \u0161t\u00fadia fundament\u00e1lnych fyzik\u00e1lnych vlastnost\u00ed, do \u00favahy prich\u00e1dzaj\u00fa aj mo\u017en\u00e9 praktick\u00e9 aplik\u00e1cie, spojen\u00e9 s tak\u00fdmi materi\u00e1lov\u00fdmi vlastnos\u0165ami ako je tepeln\u00fd transport, dynamick\u00e9 vlastnosti, magnetick\u00e9 chladenie a pod.
\u00a0<\/p>\n

Opis poskytovan\u00fdch \u010dinnost\u00ed<\/strong><\/h4>\n

Z\u00e1kladn\u00e1 konven\u010dn\u00e1 charakteristika magnetick\u00e9ho syst\u00e9mu tzv. magneto-\u0161trukt\u00farne korel\u00e1cie a f\u00e1zov\u00e9 prechody sa \u0161tuduj\u00fa pomocou merania tepelnej kapacity relaxa\u010dnou met\u00f3dou \u201edual-slope\u201c v rozsahu tepl\u00f4t od 40 mK do 4 K v nulovom magnetickom poli a v poli do 9 T. Ve\u013ekos\u0165\/hmotnos\u0165 vzoriek sa pohybuje od 1mm\/10mg do 1 cm\/200 mg. Okrem monokry\u0161t\u00e1lov je mo\u017en\u00e9 \u0161tudova\u0165 aj pr\u00e1\u0161kov\u00e9, pr\u00edpadne polykry\u0161talick\u00e9 vzorky v tvare zlisovan\u00fdch tabliet. Pri fixovan\u00ed vzorky je potrebn\u00fd \u00fadaj o citlivosti vzorky na chemick\u00e9 zlo\u017eenie fixa\u010dn\u00e9ho materi\u00e1lu.
Zmeny \u0161trukt\u00fary vzorky a f\u00e1zov\u00e9 prechody je mo\u017en\u00e9 sledova\u0165 \u0161t\u00fadiom dielektrick\u00fdch vlastnost\u00ed meran\u00edm striedavej permitivity vo frekven\u010dnom rozsahu od 50 Hz do 20 kHz v teplotnej oblasti od 35 mK do 2.5 K a poliach do 7 T.
Tepeln\u00fd transport je mo\u017en\u00e9 \u0161tudova\u0165 tzv. steady-state met\u00f3dou v nulovom magnetickom poli v teplotnej oblasti od 100 mK do 4 K. Vzorky sa pou\u017e\u00edvaj\u00fa v tvare ty\u010dinky d\u013a\u017eky od 5mm do 5 cm. Pri fixovan\u00ed vzorky je potrebn\u00fd \u00fadaj o citlivosti vzorky na chemick\u00e9 zlo\u017eenie fixa\u010dn\u00e9ho materi\u00e1lu.
Magnetick\u00e9 chladenie je mo\u017en\u00e9 testova\u0165 pomocou merania magnetokalorick\u00e9ho javu vo forme namagnetovania vzorky v kv\u00e1zi-adiabatick\u00fdch podmienkach v teplotnej oblasti od 100 mK do 4 K a v poli do 9 T. Ve\u013ekos\u0165\/hmotnos\u0165 vzoriek sa pohybuje do 1 cm\/500 mg. Okrem monokry\u0161t\u00e1lov je mo\u017en\u00e9 \u0161tudova\u0165 aj pr\u00e1\u0161kov\u00e9, pr\u00edpadne polykry\u0161talick\u00e9 vzorky v tvare zlisovan\u00fdch tabliet. Pri fixovan\u00ed vzorky je potrebn\u00fd \u00fadaj o citlivosti vzorky na chemick\u00e9 zlo\u017eenie fixa\u010dn\u00e9ho materi\u00e1lu.
Dynamiku, resp. magnetick\u00fa relax\u00e1ciu je mo\u017en\u00e9 sledova\u0165 pomocou merania striedavej susceptibility v nulovom magnetickom poli pomocou \u0161tandardnej met\u00f3dy induk\u010dn\u00fdch cievok v teplotnej oblasti od 100 mK do 4 K a frekvenci\u00e1ch od 1 Hz do 1 kHz. Ve\u013ekos\u0165\/hmotnos\u0165 vzoriek sa pohybuje do 1 cm\/500 mg. Okrem monokry\u0161t\u00e1lov je mo\u017en\u00e9 \u0161tudova\u0165 aj pr\u00e1\u0161kov\u00e9, pr\u00edpadne polykry\u0161talick\u00e9 vzorky v tvare zlisovan\u00fdch tabliet. Pri fixovan\u00ed vzorky je potrebn\u00fd \u00fadaj o citlivosti vzorky na chemick\u00e9 zlo\u017eenie fixa\u010dn\u00e9ho materi\u00e1lu.
\u00a0<\/p>\n

Zoznam aparat\u00far<\/strong><\/h4>\n

Laborat\u00f3rium kvantov\u00e9ho magnetizmu tvoria fyzicky tri laborat\u00f3ri\u00e1 umiestnen\u00e9 v budove \u00dastavu fyzik\u00e1lnych vied pr\u00edrodovedeckej fakulty Univerzity Pavla Jozefa \u0160af\u00e1rika, Park Angelinum 9 v Ko\u0161iciach.
Laborat\u00f3rium fyziky n\u00edzkych tepl\u00f4t I<\/strong> disponuje analytick\u00fdmi v\u00e1hami Sartorius s presnos\u0165ou na 0.1 mg, presnou reza\u010dkou vzoriek s diamantov\u00fdm dr\u00f4tom a kryostatom s 1 K stup\u0148om umo\u017e\u0148uj\u00facim dosahovanie tepl\u00f4t v intervale 1.2 K a\u017e 10 K a magnetick\u00fdch pol\u00ed do 3 T. V aparat\u00fare je implementovan\u00e1 steady-state met\u00f3da merania tepelnej vodivosti a tepelnej kapacity.
Laborat\u00f3rium fyziky n\u00edzkych tepl\u00f4t II<\/strong> disponuje zmie\u0161avac\u00edm refriger\u00e1torom TTL 200 Oxford Instruments operuj\u00facim bez kvapaln\u00e9ho dus\u00edka v teplotnom intervale 50 mK – 3 K a v magnetickom poli do 9 T. V aparat\u00fare s\u00fa implementovan\u00e9 met\u00f3dy merania tepelnej kapacity, tepelnej vodivosti, magnetokalorick\u00e9ho javu a striedavej susceptibility.
Laborat\u00f3rium fyziky n\u00edzkych tepl\u00f4t \u2013 Minirefriger\u00e1tor<\/strong> disponuje zmie\u0161avac\u00edm minirefriger\u00e1torom MINIDIL firmy Air Liquid operuj\u00facim bez kvapaln\u00e9ho dus\u00edka v teplotnom intervale 35 mK – 2.5 K a v magnetickom poli do 7 T. V aparat\u00fare s\u00fa implementovan\u00e9 met\u00f3dy merania tepelnej kapacity a striedavej permitivity. Pri pr\u00edprave vzoriek je mo\u017en\u00e9 pou\u017ei\u0165 optick\u00fd mikroskop s digit\u00e1lnou kamerou.
\u00a0<\/p>\n

Fotogal\u00e9ria<\/strong><\/h4>\n","protected":false},"author":1,"featured_media":15067,"parent":20272,"menu_order":7,"template":"","meta":{"_editorskit_title_hidden":false,"_editorskit_reading_time":0,"_editorskit_is_block_options_detached":false,"_editorskit_block_options_position":"{}"},"categories":[],"tags":[],"tax_aktuality":[],"class_list":["post-20280","cpt_pracoviska","type-cpt_pracoviska","status-publish","has-post-thumbnail","hentry"],"acf":{"acf_link_na_externy_obsah":""},"yoast_head":"\nLaborat\u00f3rium kvantov\u00e9ho magnetizmu - Pr\u00edrodovedeck\u00e1 fakulta | UPJ\u0160<\/title>\n<meta name=\"robots\" content=\"index, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<link rel=\"canonical\" href=\"https:\/\/www.upjs.sk\/prirodovedecka-fakulta\/pracoviska\/ustavy-pf\/ufv\/vv\/infr\/laboratorium-kvantoveho-magnetizmu\/\" \/>\n<meta property=\"og:locale\" content=\"sk_SK\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"Laborat\u00f3rium kvantov\u00e9ho magnetizmu - Pr\u00edrodovedeck\u00e1 fakulta | UPJ\u0160\" \/>\n<meta property=\"og:description\" content=\"Osoba zodpovedn\u00e1 za laborat\u00f3rium, kontakt, financovanie Laborat\u00f3rium kvantov\u00e9ho magnetizmu Pr\u00edrodovedeckej fakulty UPJ\u0160 bolo vybudovan\u00e9 v r\u00e1mci rie\u0161enia projektu zo \u0161truktur\u00e1lnych fondov \u201eExtrem – Dobudovanie Centra pokroko\u010dil\u00fdch fyzik\u00e1lnych \u0161t\u00fadi\u00ed materi\u00e1lov v extr\u00e9mnych podmienkach\u201d (EU ERDF European Regional Development Fund, Grant No. ITMS 26220120047). 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