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Reddish-orange,neutral and warm white emissions in Eu3+, Dy3+ and Dy3+/Eu3+ doped CdO-GeO2-TeO2 glasses
Institution:1. Departamento en Física, Universidad de Sonora, Hermosillo, Sonora, 83000, Mexico;2. CONACYT-Benemérita Universidad Autónoma de Puebla, Postgrado en Física Aplicada, Facultad de Ciencias Físico-Matemáticas, Av. San Claudio y Av. 18 sur, Col. San Manuel Ciudad Universitaria, Puebla, Pue. C. P. 72570, Mexico;3. Departamento de Física, Universidad Autónoma Metropolitana-Iztapalapa, P.O. Box 55-534, México, D.F. 09340, Mexico;4. Benemérita Universidad Autónoma de Puebla, Postgrado en Física Aplicada, Facultad de Ciencias Físico-Matemáticas, Av. San Claudio y Av. 18 sur, Col. San Manuel Ciudad Universitaria, Puebla, Pue. C. P. 72570, Mexico;5. Departamento de Investigación en Física de la Universidad de Sonora, Edificio 3I, Blvd., Luís Encinas s/n, Col. Centro, 83000 Hermosillo, Sonora, Mexico;1. Laboratoire des Matériaux Minéraux et leurs Applications, Centre National de Recherches en Sciences des Matériaux, Technopole de Borj-Cedria - B.P. 95, Hammam-Lif, 2050, Tunisia;2. Département de Physique, Faculté des Sciences de Tunis, University of Tunis El Manar, 2092, Tunisia;3. Center for Photonic and Smart Materials (CPMS), Zewail City of Science and Technology, Sheikh Zayed District, 6th of October City, 12588, Giza, Egypt;1. Department of Physics, Abdul Wali Khan University (AWKUM), Mardan 23200, Pakistan;2. Center of Excellence in Glass Technology and Materials Science (CEGM), Nakhon Pathom Rajabhat University, Nakhon Pathom 73000, Thailand;3. Physics Program, Faculty of Science and Technology, Nakhon Pathom Rajabhat University, Nakhon Pathom 73000, Thailand;4. Department of Physics, Kyungpook National University, Deagu 702-701, Republic of Korea;1. Department of Physics, Abdul Wali Khan University, Mardan, 23200, Pakistan;2. Center of Excellence in Glass Technology and Materials Science (CEGM), Nakhon Pathom Rajabhat University, Nakhon Pathom, 73000, Thailand;3. Physics Program, Faculty of Science and Technology, Nakhon Pathom Rajabhat University, Nakhon Pathom, 73000, Thailand;4. Department of Physics, Kyungpook National University, Daegu 702-701, Republic of Korea;1. Laser & Spectroscopy Laboratory, Department of Physics, Banaras Hindu University, Varanasi 221005, India;2. Department of Physics & Astrophysics, University of Delhi, 110007, India;1. Wireless and Photonic Networks Research Centre, Faculty of Engineering, Universiti Putra Malaysia, 43400 Serdang, Selangor, Malaysia;2. Department of Physics, Faculty of Science, Universiti Putra Malaysia, Serdang, Selangor, Malaysia;3. Department of Physics, Faculty of Science, Autonomous University of Mexico State, C.P. 50000 Toluca, Mexico;4. Faculty of Electrical Engineering, Czestochowa University of Technology, Armii Krajowej 17, PL-42-217 Czestochowa, Poland;5. Departamento de Física, Universidad Autónoma Metropolitana-Iztapalapa, P.O. Box 55-534, México D.F. 09340, Mexico
Abstract:Eu3+, Dy3+ and Dy3+/Eu3+ doped CdO-GeO2-TeO2 glasses were prepared using the melt-quenching process and analyzed by X-diffraction, Raman spectroscopy, excitation and emission spectra, and emission decay time profiles. The lack of X ray diffraction peaks revealed that all samples are amorphous. Vibrational modes associated with Tesingle bondOsingle bondTe and Gesingle bondOsingle bondGe related bonds and molecular oxygen were detected by Raman spectroscopy. The luminescence characteristics were studied upon excitations that correspond with the emission of InGaN (370–420 nm) based LEDs. The Eu3+ singly doped glass displayed reddish-orange global emission, with x = 0.601 and y = 0.349 CIE1931 chromaticity coordinates, upon 393 nm excitation. Neutral emission with x = 0.373 and y = 0.412 CIE1931 chromaticity coordinates and correlated color temperature (CCT) of 4400 K, was achieved in the Dy3+ singly doped glass excited at 388 nm. The Dy3+/Eu3+ co-doped glass exhibited warm, neutral and soft warm white emissions with CCT values of 3435, 4153 and 2740 K, under excitations at 382, 388 and 393 nm, respectively, depending mainly on the Dy3+ and Eu3+ relative excitation. The Dy3+ excitation bands observed in the Dy3+/Eu3+ glass by monitoring the 611 nm Eu3+ emission, suggest that Dy3+ → Eu3+ energy transfer takes place, despite the fact that the Dy3+ emission decays in the Dy3+ and Dy3+/Eu3+ doped glass, remain without changes. The shortening of Eu3+ decay in presence of Dy3+ was attributed to an Eu3+ → Dy3+ non-radiative energy transfer process, which according with the Inokuti-Hirayama model might be dominated through an electric quadrupole-quadrupole interaction, with efficiency and probability of 5.5% and 51.6 s−1, respectively.
Keywords:Reddish-orange emission  Neutral and warm white emission  Energy transfer
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