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Fe:ZnMnSe laser active material properties at room and cryogenic temperature

Identifikátory výsledku

  • Kód výsledku v IS VaVaI

    <a href="https://www.isvavai.cz/riv?ss=detail&h=RIV%2F68407700%3A21340%2F16%3A00304690" target="_blank" >RIV/68407700:21340/16:00304690 - isvavai.cz</a>

  • Výsledek na webu

    <a href="http://dx.doi.org/10.1117/12.2228844" target="_blank" >http://dx.doi.org/10.1117/12.2228844</a>

  • DOI - Digital Object Identifier

    <a href="http://dx.doi.org/10.1117/12.2228844" target="_blank" >10.1117/12.2228844</a>

Alternativní jazyky

  • Jazyk výsledku

    angličtina

  • Název v původním jazyce

    Fe:ZnMnSe laser active material properties at room and cryogenic temperature

  • Popis výsledku v původním jazyce

    Fe:Zn(1-x)Mn(x)Se solid solution spectroscopic and laser properties were investigated in the temperature range 80290 K. Two novel samples with different zinc - manganese (Zn-Mn) ratio described by the Mn content x (0.1 or 0.2) were used and the results were compared to the known Fe:ZnSe crystal. The samples had a broad absorption spectra with the maximum around 3 mu m and therefore an Er:YAG laser (2.94 mu m, 10 mJ, 120 ns) was used as a pump radiation source. The Fe:ZnMnSe fluorescence spectra are generally broad in the range 3.5 - 5.5 mu m. In the case of Fe: ZnMnSe x = 0.1, the fluorescence spectrum at 290 K is ranging from 3.5 to 5.5 mu m. Lowering the temperature down to 80 K lead to the spectral narrowing mainly in the mid-IR part, but the fluorescence is still up to 5 mu m at 80 K. In the case of Fe: ZnMnSe x = 0.2 the fluorescence is shifted towards mid-IR up to 5.2 mu m even at 80 K. The fluorescence lifetime decreases from tens of us at 80 K down to 1 us at 240 K. The laser oscillations were successfully achieved with both novel Fe: ZnMnSe crystals in the temperature range 80-290 K. In the case of x = 0.1, the central wavelength was similar to 4.2 mu m at 80 K and the temperature increase up to 290 K led to almost linear increase of the wavelength up to similar to 4.75 mu m. The tendency was similar in the case of Fe: ZnMnSe x = 0.2: the output wavelength increased from similar to 4.3 mu m up to similar to 4.8 mu m with the temperature increase from 80 to 290 K. The laser spectral linewidth was about 300 nm. In comparison with the Fe:ZnSe crystal, the laser output wavelength shift toward mid-IR region without any spectrally tunable element in the laser cavity can be clearly observed.

  • Název v anglickém jazyce

    Fe:ZnMnSe laser active material properties at room and cryogenic temperature

  • Popis výsledku anglicky

    Fe:Zn(1-x)Mn(x)Se solid solution spectroscopic and laser properties were investigated in the temperature range 80290 K. Two novel samples with different zinc - manganese (Zn-Mn) ratio described by the Mn content x (0.1 or 0.2) were used and the results were compared to the known Fe:ZnSe crystal. The samples had a broad absorption spectra with the maximum around 3 mu m and therefore an Er:YAG laser (2.94 mu m, 10 mJ, 120 ns) was used as a pump radiation source. The Fe:ZnMnSe fluorescence spectra are generally broad in the range 3.5 - 5.5 mu m. In the case of Fe: ZnMnSe x = 0.1, the fluorescence spectrum at 290 K is ranging from 3.5 to 5.5 mu m. Lowering the temperature down to 80 K lead to the spectral narrowing mainly in the mid-IR part, but the fluorescence is still up to 5 mu m at 80 K. In the case of Fe: ZnMnSe x = 0.2 the fluorescence is shifted towards mid-IR up to 5.2 mu m even at 80 K. The fluorescence lifetime decreases from tens of us at 80 K down to 1 us at 240 K. The laser oscillations were successfully achieved with both novel Fe: ZnMnSe crystals in the temperature range 80-290 K. In the case of x = 0.1, the central wavelength was similar to 4.2 mu m at 80 K and the temperature increase up to 290 K led to almost linear increase of the wavelength up to similar to 4.75 mu m. The tendency was similar in the case of Fe: ZnMnSe x = 0.2: the output wavelength increased from similar to 4.3 mu m up to similar to 4.8 mu m with the temperature increase from 80 to 290 K. The laser spectral linewidth was about 300 nm. In comparison with the Fe:ZnSe crystal, the laser output wavelength shift toward mid-IR region without any spectrally tunable element in the laser cavity can be clearly observed.

Klasifikace

  • Druh

    D - Stať ve sborníku

  • CEP obor

    JA - Elektronika a optoelektronika, elektrotechnika

  • OECD FORD obor

Návaznosti výsledku

  • Projekt

    <a href="/cs/project/GA15-05360S" target="_blank" >GA15-05360S: Vliv teploty na spektroskopické a laserové vlastnosti pevnolátkových aktivních materiálů pro viditelnou až střední infračervenou oblast</a><br>

  • Návaznosti

    P - Projekt vyzkumu a vyvoje financovany z verejnych zdroju (s odkazem do CEP)

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 statě ve sborníku

    Proc. SPIE 9893, Laser Sources and Applications III

  • ISBN

    978-1-5106-0138-3

  • ISSN

    0277-786X

  • e-ISSN

  • Počet stran výsledku

    6

  • Strana od-do

  • Název nakladatele

    SPIE

  • Místo vydání

    Bellingham (stát Washington)

  • Místo konání akce

    Brusel

  • Datum konání akce

    3. 4. 2016

  • Typ akce podle státní příslušnosti

    WRD - Celosvětová akce

  • Kód UT WoS článku

    000381704500006