8
views
0
recommends
+1 Recommend
0 collections
    0
    shares
      • Record: found
      • Abstract: found
      • Article: found
      Is Open Access

      Intense photoluminescence in CaTiO 3:Sm 3+ phosphors, effect of co-doping singly, doubly and triply ionized elements and their applications in LEDs

      research-article
      a , b , b , , a ,
      RSC Advances
      The Royal Society of Chemistry

      Read this article at

      Bookmark
          There is no author summary for this article yet. Authors can add summaries to their articles on ScienceOpen to make them more accessible to a non-specialist audience.

          Abstract

          In this work, Sm 3+-doped and Sm 3+/Li +/K +/Mg 2+/Ba 2+/Gd 3+/Bi 3+ co-doped CaTiO 3 phosphors were synthesized by a solid-state reaction method at 1473 K. The phase of phosphors was identified to be orthorhombic with space group Pnma (62) by XRD measurements. The morphological properties of the prepared samples were studied by SEM measurements. The average crystallite and particle sizes were found to increase in the presence of modifiers and they follow the trend Li + > Mg 2+ > Gd 3+ > K + > Bi 3+ > Ba 2+. EDX measurements were used to verify the presence of Ca, Ti, O, Sm, K, Mg, Ba, Gd and Bi atoms in the prepared phosphor samples. The Sm 3+ ion shows emission peaks at 564, 599 and 646 nm due to 4G 5/26H 5/2, 6H 7/2 and 6H 9/2 transitions upon 407 nm excitation, among which the peak situated at 599 nm has maximum emission intensity. Concentration quenching was observed above 2 mol% of Sm 3+ ions in this host. However, the emission intensity of Sm 3+ peaks can be enhanced using different modifier (Li +/K +/Mg 2+/Ba 2+/Gd 3+/Bi 3+) ions. It was found that the size (ionic radii) and charge compensation of the ion together play a dominant role. The enhancement is more after co-doping with smaller radius ions (Li +, Mg 2+ and Gd 3+), among which Li + shows the largest enhancement. This is because ions of smaller size will be able to go closer to the activator ion and the charge imbalance causes a larger field. The CIE color coordinates, correlated color temperature (CCT) and color purity of the phosphors were calculated and show orange-red color emissions with a maximum color purity of ∼93% in the case of CaTiO 3:2Sm 3+/1.0Li + phosphor. The lifetime value is increased in the presence of these ions. It is again maximum for the Li + co-doped CaTiO 3:2Sm 3+ phosphor sample. Thus, the prepared phosphor samples are suitable sources for orange-red light.

          Abstract

          Enhancement in emission intensity of Sm 3+ ion in the presence of smaller and larger ionic radii ions and the emitted orange-red color used in LED applications.

          Related collections

          Most cited references42

          • Record: found
          • Abstract: found
          • Article: not found

          Simultaneous phase and size control of upconversion nanocrystals through lanthanide doping.

          Doping is a widely applied technological process in materials science that involves incorporating atoms or ions of appropriate elements into host lattices to yield hybrid materials with desirable properties and functions. For nanocrystalline materials, doping is of fundamental importance in stabilizing a specific crystallographic phase, modifying electronic properties, modulating magnetism as well as tuning emission properties. Here we describe a material system in which doping influences the growth process to give simultaneous control over the crystallographic phase, size and optical emission properties of the resulting nanocrystals. We show that NaYF(4) nanocrystals can be rationally tuned in size (down to ten nanometres), phase (cubic or hexagonal) and upconversion emission colour (green to blue) through use of trivalent lanthanide dopant ions introduced at precisely defined concentrations. We use first-principles calculations to confirm that the influence of lanthanide doping on crystal phase and size arises from a strong dependence on the size and dipole polarizability of the substitutional dopant ion. Our results suggest that the doping-induced structural and size transition, demonstrated here in NaYF(4) upconversion nanocrystals, could be extended to other lanthanide-doped nanocrystal systems for applications ranging from luminescent biological labels to volumetric three-dimensional displays.
            Bookmark
            • Record: found
            • Abstract: found
            • Article: not found

            Lanthanide ions as spectral converters for solar cells.

            The use of lanthanide ions to convert photons to different, more useful, wavelengths is well-known from a wide range of applications (e.g. fluorescent tubes, lasers, white light LEDs). Recently, a new potential application has emerged: the use of lanthanide ions for spectral conversion in solar cells. The main energy loss in the conversion of solar energy to electricity is related to the so-called spectral mismatch: low energy photons are not absorbed by a solar cell while high energy photons are not used efficiently. To reduce the spectral mismatch losses both upconversion and downconversion are viable options. In the case of upconversion two low energy infrared photons that cannot be absorbed by the solar cell, are added up to give one high energy photon that can be absorbed. In the case of downconversion one high energy photon is split into two lower energy photons that can both be absorbed by the solar cell. The rich and unique energy level structure arising from the 4f(n) inner shell configuration of the trivalent lanthanide ions gives a variety of options for efficient up- and downconversion. In this perspective an overview will be given of recent work on photon management for solar cells. Three topics can be distinguished: (1) modelling of the potential impact of spectral conversion on the efficiency of solar cells; (2) research on up- and downconversion materials based on lanthanides; and (3) proof-of-principle experiments. Finally, an outlook will be given, including issues that need to be resolved before wide scale application of up- and downconversion materials can be anticipated.
              Bookmark
              • Record: found
              • Abstract: found
              • Article: not found

              Near-infrared emissive lanthanide hybridized carbon quantum dots for bioimaging applications.

              Lanthanide hybridized carbon quantum dots (Ln-CQDs) were synthesized by a facile one-pot hydrothermal method using citric acid as a carbon precursor and Yb3+ or Nd3+ as a doping ion. The morphology and chemical structures of Ln-CQDs were investigated by TEM, XRD, XPS, and FTIR spectroscopy. The obtained Ln-CQDs are spherical and well dispersed in water, and their aqueous solutions emit strong blue emission under UV excitation. The Ln-CQDs exhibit excitation-dependent PL behavior with the emission maximum ranging from 443 to 552 nm under 300-520 nm excitation. Moreover, the carbon quantum dots can not only act as visible imaging agents, but also as antennae for photoluminescence (PL) of lanthanide ions. Hence, CQDs hybridized with Yb3+ or Nd3+ ions exhibit the characteristic emission in the near-infrared region with the emission maximum centered at about 998 and 1068 nm, respectively. The MTT assay against HeLa cells verified the low cytotoxicity of Ln-CQDs. They have been used as excellent optical probes for multicolor cell-imaging, demonstrating their great potential for both visible/NIR bioimaging and biomedical applications in vivo.
                Bookmark

                Author and article information

                Journal
                RSC Adv
                RSC Adv
                RA
                RSCACL
                RSC Advances
                The Royal Society of Chemistry
                2046-2069
                26 July 2023
                26 July 2023
                26 July 2023
                : 13
                : 33
                : 22663-22674
                Affiliations
                [a ] Laser and Spectroscopy Laboratory, Department of Physics, Institute of Science, Banaras Hindu University Varanasi 221005 India sbrai49@ 123456yahoo.co.in
                [b ] Physics Section, Mahila Maha Vidyalaya, Department of Physics, Banaras Hindu University Varanasi 221005 India hmishra@ 123456bhu.ac.in
                Author information
                https://orcid.org/0009-0004-3449-6910
                https://orcid.org/0000-0003-3734-2832
                Article
                d3ra04468h
                10.1039/d3ra04468h
                10369130
                83b1ac71-3302-46da-93b6-ea6da3e75c89
                This journal is © The Royal Society of Chemistry
                History
                : 4 July 2023
                : 9 July 2023
                Page count
                Pages: 12
                Funding
                Funded by: University Grants Commission, doi 10.13039/501100001501;
                Award ID: Unassigned
                Funded by: Banaras Hindu University, doi 10.13039/501100002742;
                Award ID: 6031
                Categories
                Chemistry
                Custom metadata
                Paginated Article

                Comments

                Comment on this article