Importance of layer thermal conductivity on the sharpness of patterns produced by laser interference
Identifikátory výsledku
Kód výsledku v IS VaVaI
<a href="https://www.isvavai.cz/riv?ss=detail&h=RIV%2F68378271%3A_____%2F16%3A00474074" target="_blank" >RIV/68378271:_____/16:00474074 - isvavai.cz</a>
Nalezeny alternativní kódy
RIV/68407700:21340/16:00366579
Výsledek na webu
<a href="http://dx.doi.org/10.1016/j.apsusc.2015.09.110" target="_blank" >http://dx.doi.org/10.1016/j.apsusc.2015.09.110</a>
DOI - Digital Object Identifier
<a href="http://dx.doi.org/10.1016/j.apsusc.2015.09.110" target="_blank" >10.1016/j.apsusc.2015.09.110</a>
Alternativní jazyky
Jazyk výsledku
angličtina
Název v původním jazyce
Importance of layer thermal conductivity on the sharpness of patterns produced by laser interference
Popis výsledku v původním jazyce
In this work, we compare patterns produced in Ag layers having similar thickness in the range 8.3-10.8 nm but having different initial nanostructure, i.e. behaving either as discontinuous or continuous layers and thus having very different thermal conductivities. The patterns are produced by exposing a phase mask to an excimer laser operating at 193 nm and using a projection optics that leads to similar fringed patterns with periods in the range 6.3-6.7 μm. The layer breaks up into isolated NPs due to laser induced melting at the regions around the intensity maxima sites. The resulting fringes have sharp interfaces in the case of discontinuous layers while a variety of regions across the pattern with no sharp interfaces are produced in the case of continuous layers. The results show that while the temperature distribution across the pattern matches almost perfectly the laser beam intensity profile for the former case, it becomes smeared due to lateral heat flow for the latter case.n
Název v anglickém jazyce
Importance of layer thermal conductivity on the sharpness of patterns produced by laser interference
Popis výsledku anglicky
In this work, we compare patterns produced in Ag layers having similar thickness in the range 8.3-10.8 nm but having different initial nanostructure, i.e. behaving either as discontinuous or continuous layers and thus having very different thermal conductivities. The patterns are produced by exposing a phase mask to an excimer laser operating at 193 nm and using a projection optics that leads to similar fringed patterns with periods in the range 6.3-6.7 μm. The layer breaks up into isolated NPs due to laser induced melting at the regions around the intensity maxima sites. The resulting fringes have sharp interfaces in the case of discontinuous layers while a variety of regions across the pattern with no sharp interfaces are produced in the case of continuous layers. The results show that while the temperature distribution across the pattern matches almost perfectly the laser beam intensity profile for the former case, it becomes smeared due to lateral heat flow for the latter case.n
Klasifikace
Druh
J<sub>imp</sub> - Článek v periodiku v databázi Web of Science
CEP obor
—
OECD FORD obor
10302 - Condensed matter physics (including formerly solid state physics, supercond.)
Návaznosti výsledku
Projekt
—
Návaznosti
I - Institucionalni podpora na dlouhodoby koncepcni rozvoj vyzkumne organizace
Ostatní
Rok uplatnění
2016
Kód důvěrnosti údajů
S - Úplné a pravdivé údaje o projektu nepodléhají ochraně podle zvláštních právních předpisů
Údaje specifické pro druh výsledku
Název periodika
Applied Surface Science
ISSN
0169-4332
e-ISSN
—
Svazek periodika
374
Číslo periodika v rámci svazku
Jun
Stát vydavatele periodika
NL - Nizozemsko
Počet stran výsledku
4
Strana od-do
61-64
Kód UT WoS článku
000375937300011
EID výsledku v databázi Scopus
2-s2.0-84942068484