4 research outputs found
Erbium upconversion luminescence from sol-gel derived multilayer porous inorganic perovskite film
Erbium-doped barium titanate (BaTiO3:Er) xerogel film with a thickness of about 500 nm was formed on the porous strontium titanate (SrTiO3) xerogel film on Si substrate after annealing at 800 Β°C or 900 Β°C. The elaborated structures show room temperature upconversion luminescence under 980 nm excitation with the photoluminescence (PL) bands at 523, 546, 658, 800 and 830 nm corresponding to 2H11/2β4I15/2, 4S3/2β4I15/2, 4F9/2β4I15/2 and 4I9/2β4I15/2 transitions of trivalent erbium. Raman and X-ray diffraction (XRD) analysis of BaTiO3:Er\porous SrTiO3\Si structure showed the presence of perovskite phases. Its excellent up-conversion optical performance will greatly broaden its applications in perovskite solar cells and high-end anti-counterfeiting technologies
Optical Properties and Upconversion Luminescence of BaTiO3 Xerogel Structures Doped with Erbium and Ytterbium
Erbium upconversion (UC) photoluminescence (PL) from sol-gel derived barium titanate (BaTiO3:Er) xerogel structures fabricated on silicon, glass or fused silica substrates has been studied. The fabricated structures under continuous-wave excitation at 980 nm and nanosecond laser excitation at 980 and 1540 nm demonstrate room temperature PL with the bands at 410, 523, 546, 658, 800 and 830 nm, which correspond to the 2H9/2 β 4I15/2, 2H11/2 β 4I15/2, 4S3/2 β 4I15/2, 4F9/2β 4I15/2 and 4I9/2β 4I15/2 transitions in Er3+ ions. The intensity of erbium UΠ‘ PL increases when an additional macroporous layer of strontium titanate is used beneath the BaTiO3 xerogel layer. It is enhanced for BaTiO3 xerogel films codoped with erbium and ytterbium (BaTiO3:Er,Yb). The redistribution of the intensity of the PL bands is observed for the latter and it depends on the excitation conditions. Finally, a Bragg reflector and a microcavity structure comprising of alternating (BaTiO3:Er,Yb) and SiO2 xerogel layers were fabricated with the cavity mode near the red PL band of Er3+ ions. Enhancement of UC PL from the microcavity was observed for the sample annealed from 450Β°C to 600Β°C. The fabricated cavity structures annealed at 450Β°C allow us to tune the cavity mode with 10 nm shift within the temperature range from +20Β°C to +130Β°C. Photonic application of BaTiO3 xerogel structures doped with lanthanides is discussed
ΠΠΏ-ΠΊΠΎΠ½Π²Π΅ΡΡΠΈΠΎΠ½Π½Π°Ρ Π»ΡΠΌΠΈΠ½Π΅ΡΡΠ΅Π½ΡΠΈΡ Π² ΠΊΡΠ΅ΡΠΎΠ³Π΅Π»Π΅ ΡΠΈΡΠ°Π½Π°ΡΠ° Π±Π°ΡΠΈΡ, Π»Π΅Π³ΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΌ ΡΡΠ±ΠΈΠ΅ΠΌ ΠΈ ΠΈΡΡΠ΅ΡΠ±ΠΈΠ΅ΠΌ, Π² ΠΏΠΎΡΠΈΡΡΠΎΠΌ Π°Π½ΠΎΠ΄Π½ΠΎΠΌ ΠΎΠΊΡΠΈΠ΄Π΅ Π°Π»ΡΠΌΠΈΠ½ΠΈΡ
In this work, sol-gel synthesis and luminescence properties of erbium and ytterbium doped BaTiO3 (BaTiO3:Er,Yb) in porous anodic alumina are reported. Porous anodic alumina with its well-known tailor-made honeycomb structure was chosen as a template for the sol-gel synthesis of BaTiO3:Er,Yb. Porous anodic alumina was fabricated either on silicon wafer or aluminum foil. The sol corresponding to xerogel content of Ba0,76Er0,04Yb0,20TiO3 was deposited on porous anodic alumina by spinning, which was followed by drying and heat treatment at a relatively low temperature 450 Β°C on aluminum foil or 800 Β°C on silicon. Porous anodic alumina known also as an optically anisotropic structure differed in the experiments by diameter of the pores and thickness. Evidently, all fabricated samples demonstrated a roomtemperature erbium upconversion luminescence under excitation in the continuous-wave (CW) mode with a focused 980 nm laser beam of a 200 mW diode module. Erbium upconversion luminescence is characterized by the bands at 410, 523, 546, and 658 nm, corresponding to the 2H9/2 β 4I15/2, 2H11/2 β 4I15/2, 4S3/2 β 4I15/2 and 4F9/2 β 4I15/2.Π ΡΡΠ°ΡΡΠ΅ ΡΠ°ΡΡΠΌΠΎΡΡΠ΅Π½ Π·ΠΎΠ»Ρ-Π³Π΅Π»Ρ-ΡΠΈΠ½ΡΠ΅Π· ΠΈ Π»ΡΠΌΠΈΠ½Π΅ΡΡΠ΅Π½ΡΠ½ΡΠ΅ ΡΠ²ΠΎΠΉΡΡΠ²Π° ΡΠΈΡΠ°Π½Π°ΡΠ° Π±Π°ΡΠΈΡ, Π»Π΅Π³ΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΡΡΠ±ΠΈΠ΅ΠΌ ΠΈ ΠΈΡΡΠ΅ΡΠ±ΠΈΠ΅ΠΌ (BaTiO3:Er,Yb), Π² ΠΏΠΎΡΠΈΡΡΠΎΠΌ Π°Π½ΠΎΠ΄Π½ΠΎΠΌ ΠΎΠΊΡΠΈΠ΄Π΅ Π°Π»ΡΠΌΠΈΠ½ΠΈΡ. ΠΠΎΡΠΈΡΡΡΠΉ Π°Π½ΠΎΠ΄Π½ΡΠΉ ΠΎΠΊΡΠΈΠ΄ Π°Π»ΡΠΌΠΈΠ½ΠΈΡ Ρ Π΅Π³ΠΎ Ρ
ΠΎΡΠΎΡΠΎ ΠΈΠ·Π²Π΅ΡΡΠ½ΠΎΠΉ ΡΡΠ΅ΠΈΡΡΠΎΠΉ ΡΡΡΡΠΊΡΡΡΠΎΠΉ Π±ΡΠ» Π²ΡΠ±ΡΠ°Π½ Π² ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅ ΠΌΠ°ΡΡΠΈΡΡ Π΄Π»Ρ Π·ΠΎΠ»Ρ-Π³Π΅Π»Ρ-ΡΠΈΠ½ΡΠ΅Π·Π° BaTiO3:Er,Yb. ΠΠΎΡΠΈΡΡΡΠΉ Π°Π½ΠΎΠ΄Π½ΡΠΉ ΠΎΠΊΡΠΈΠ΄ Π°Π»ΡΠΌΠΈΠ½ΠΈΡ ΠΈΠ·Π³ΠΎΡΠ°Π²Π»ΠΈΠ²Π°Π»ΠΈ Π½Π° ΠΊΡΠ΅ΠΌΠ½ΠΈΠ΅Π²ΠΎΠΉ ΠΏΠ»Π°ΡΡΠΈΠ½Π΅ ΠΈ Π°Π»ΡΠΌΠΈΠ½ΠΈΠ΅Π²ΠΎΠΉ ΡΠΎΠ»ΡΠ³Π΅. Π Π°ΡΡΠ²ΠΎΡ, ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΡΡΡΠΈΠΉ ΡΠΎΡΡΠ°Π²Ρ ΠΊΡΠ΅ΡΠΎΠ³Π΅Π»Ρ Ba0,76Er0,04Yb0,20TiO3, ΠΎΡΠ°ΠΆΠ΄Π°Π»ΡΡ Π½Π° ΠΏΠΎΡΠΈΡΡΡΠΉ Π°Π½ΠΎΠ΄Π½ΡΠΉ ΠΎΠΊΡΠΈΠ΄ Π°Π»ΡΠΌΠΈΠ½ΠΈΡ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ ΡΠ΅Π½ΡΡΠΈΡΡΠ³ΠΈΡΠΎΠ²Π°Π½ΠΈΡ Ρ ΠΏΠΎΡΠ»Π΅Π΄ΡΡΡΠ΅ΠΉ ΡΡΡΠΊΠΎΠΉ ΠΈ ΡΠ΅ΡΠΌΠΎΠΎΠ±ΡΠ°Π±ΠΎΡΠΊΠΎΠΉ ΠΏΡΠΈ ΠΎΡΠ½ΠΎΡΠΈΡΠ΅Π»ΡΠ½ΠΎ Π½ΠΈΠ·ΠΊΠΎΠΉ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ΅ 450 Β°C Π½Π° Π°Π»ΡΠΌΠΈΠ½ΠΈΠ΅Π²ΠΎΠΉ ΡΠΎΠ»ΡΠ³Π΅ ΠΈΠ»ΠΈ ΠΏΡΠΈ 800 Β°C Π½Π° ΠΊΡΠ΅ΠΌΠ½ΠΈΠΈ. ΠΠΎΡΠΈΡΡΡΠΉ Π°Π½ΠΎΠ΄Π½ΡΠΉ ΠΎΠΊΡΠΈΠ΄ Π°Π»ΡΠΌΠΈΠ½ΠΈΡ, ΠΈΠ·Π²Π΅ΡΡΠ½ΡΠΉ ΡΠ°ΠΊΠΆΠ΅ ΠΊΠ°ΠΊ ΠΎΠΏΡΠΈΡΠ΅ΡΠΊΠΈ Π°Π½ΠΈΠ·ΠΎΡΡΠΎΠΏΠ½Π°Ρ ΡΡΡΡΠΊΡΡΡΠ°, Π² ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ΅ ΠΎΡΠ»ΠΈΡΠ°Π»ΡΡ ΡΠ°Π·ΠΌΠ΅ΡΠΎΠΌ ΠΏΠΎΡ ΠΈ ΡΠΎΠ»ΡΠΈΠ½ΠΎΠΉ. ΠΠΎ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ°ΠΌ ΠΈΡΠΏΡΡΠ°Π½ΠΈΠΉ ΡΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ Π²ΡΠ΅ ΠΈΠ·Π³ΠΎΡΠΎΠ²Π»Π΅Π½Π½ΡΠ΅ ΠΎΠ±ΡΠ°Π·ΡΡ Π΄Π΅ΠΌΠΎΠ½ΡΡΡΠΈΡΡΡΡ Π°ΠΏ-ΠΊΠΎΠ½Π²Π΅ΡΡΠΈΠΎΠ½Π½ΡΡ Π»ΡΠΌΠΈΠ½Π΅ΡΡΠ΅Π½ΡΠΈΡ ΡΡΠ±ΠΈΡ ΠΏΡΠΈ ΠΊΠΎΠΌΠ½Π°ΡΠ½ΠΎΠΉ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ΅ ΠΏΡΠΈ Π²ΠΎΠ·Π±ΡΠΆΠ΄Π΅Π½ΠΈΠΈ Π΄ΠΈΠΎΠ΄Π½ΡΠΌ ΠΌΠΎΠ΄ΡΠ»Π΅ΠΌ Π² Π½Π΅ΠΏΡΠ΅ΡΡΠ²Π½ΠΎΠΌ ΡΠ΅ΠΆΠΈΠΌΠ΅ ΡΡΠΎΠΊΡΡΠΈΡΠΎΠ²Π°Π½Π½ΡΠΌ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΠ΅ΠΌ Π»Π°Π·Π΅ΡΠ½ΠΎΠ³ΠΎ Π΄ΠΈΠΎΠ΄Π° Π½Π° Π΄Π»ΠΈΠ½Π΅ Π²ΠΎΠ»Π½Ρ 980 Π½ΠΌ ΠΌΠΎΡΠ½ΠΎΡΡΡΡ 200 ΠΌΠΡ. ΠΠΏ-ΠΊΠΎΠ½Π²Π΅ΡΡΠΈΠΎΠ½Π½Π°Ρ Π»ΡΠΌΠΈΠ½Π΅ΡΡΠ΅Π½ΡΠΈΡ ΡΡΠ±ΠΈΡ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΠ·ΡΠ΅ΡΡΡ ΠΏΠΎΠ»ΠΎΡΠ°ΠΌΠΈ Ρ ΠΌΠ°ΠΊΡΠΈΠΌΡΠΌΠΎΠΌ Π½Π° Π΄Π»ΠΈΠ½Π°Ρ
Π²ΠΎΠ»Π½ 410, 523, 546 ΠΈ 658 Π½ΠΌ ΠΈ ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΡΡΡΠΈΠΌΠΈ ΠΈΠΌ ΠΏΠ΅ΡΠ΅Ρ
ΠΎΠ΄Π°ΠΌΠΈ 2H9/2 β 4I15/2, 2H11/2 β 4I15/2, 4S3/2 β 4I15/2 ΠΈ 4F9/2 β 4I15/2
Upconversion Luminescence of Er3+ Ions from Barium Titanate Xerogel Powder and Target Fabricated by Explosive Compaction Method
Photo- and cathodoluminescence in the visible range from erbium-doped barium titanate xerogels obtained in the form of a powder and a target pressed from it by explosive compaction are investigated. The powder and target exhibit upconversion luminescence of erbium ions excited at wavelengths in the regions 950β1000 and 1450β1550 nm that is characterized by strong bands at 650 and 520β560 nm and a weak band at ~820 nm that correspond to the 4F9/2 β 4I15/2, 2H11/2 β 4I15/2, 4S3/2 β 4I15/2, and 4I9/2 β 4I15/2 transitions of Er3+. The target also demonstrates cathodoluminescence at room temperature and liquid nitrogen temperature with the strongest bands at 650, 520, and 538 nm