Photo and cathodoluminescence of commercial YAG:Ce based phosphors in UV region

https://doi.org/10.1016/j.nimb.2020.06.004Get rights and content

Abstract

The luminescence spectral kinetic characteristics in UV and visible spectral regions of a group of commercial YAG:Ce based phosphors are investigated under excitation by UV radiation in the spectral range of 300–210 nm (photoluminescence, PL) and high-energy electrons (0.25 MeV, pulse cathodoluminescence, PCL). It was established that UV luminescence appears in all phosphors, whose spectrum consists of bands in the region of 312, 320, 380 nm and 530–565 nm. The kinetics of the PCL UV luminescence decay in all phosphors shows at least one, two components in different phosphors but is differ from kinetics of luminescence in the visible region. The possible structure of luminescence centers responsible for UV luminescence is discussed.

Introduction

Yttrium aluminum garnet Y3Al5O12 (YAG) together with Gd3Ga5O12 and Lu3Al5O12 belongs to the family of complex oxide materials with the garnet structure of the composition A3B2C3O12, which have been successfully grown as single crystals or synthesized as nano and micro-materials through different methods [1], [2], [3], [4], [5], [6], [7], [8], [9], [10]. When these materials are doped with one or two rare-earth ions (Ce3+, Eu3+, Tb3+ and etc) [1], [2], [3], [10], [11], [12], [13], [14], [15], [16], [17], [18], [19], which are considered to be excellent luminescence dopants, they exhibit unique and outstanding optical and luminescent properties, thereby receiving tremendous attention due to their potential application as laser crystals, fast scintillators, ionizing radiation dosimeters, light emitting devices and converters of optical radiation [1], [2], [3], [8], [9], [10], [12], [20], [21], [22], [23]. In particular, YAG doped by cerium Ce3+ is excellent phosphor used in white LED as an efficient light converter, providing a high efficiency of UV (450–460 nm) light conversion into a visible light (500–780 nm) [1], [2], [3]. The same spectral range is the light emission of the most efficient LED chip based on InGaN blue chip [21], [22]. The combination of light emission from such a chip with YAG phosphor luminescence allow one to obtain an efficient white light LED. It is also important to note that YAG:Ce based single crystals and composites are also promising materials for radiation detection and dosimetry [23]. When YAG phosphors were excited by the electron beam

When YAG phosphors were excited by the electron beam of nanosecond pulse duration with an electron energy of 250 keV, the luminescence for YAG phosphor doped with cerium ions is located at 2.17 eV (570 nm), while for undoped YAG phosphor at 2.12 eV (585 nm) [12]. Furthermore, the luminescence band of YAG:Ce phosphors has an asymmetric shape and could be decomposed into the two Gaussian components with maxima at 2.4 eV and 2.19 eV [12]. The excitation of YAG:Ce in the exciton absorption region [24], [25] leads to the luminescence appearance in the region of 250–450 nm with bands at 260, 301, 372, 394 nm, which are different for crystals, ceramics, and films. The UV luminescence was observed [26] at 460 nm when excited by radiation at 258 and 292 nm. Furthermore, in the cathodoluminescence spectrum of (LuYGd)3(AlGa)5O12:Ce, a broad luminescence band was observed [27] in the region of 200–400 nm and narrow at 312 nm. It was also reported [28], that X-ray excitation induces the luminescence in Lu3Al5O12 (LuAG) and Y3Al5O12 (YAG) crystals at 315 and 380 nm, the band at 315 nm being dominant. Two well-resolved emission bands at 300 and 360 nm were found in [29] in the x-ray luminescence spectrum. Lastly, UV luminescence in the region of 300–500 nm was observed in ref. [30] with bands at 380, 415, 435 nm.

Thus, the available information about YAG:Ce luminescence, especially on crystal structure/defects responsible for luminescence centers in the UV region is still fragmentary, and so far has not been studied enough. Thus, the detailed study of UV luminescence is of great interest both for understanding the processes of transfer of excitation energy to luminescence centers and for the development of scintillators and specialized LEDs

This article presents the results of the study of the UV excitation spectra and luminescence in a series of commercial YAG phosphors of different firms. In the article, the UV excitation area is defined as the spectrum range from 200 to 310 nm, the UV luminescence −300–450 nm. The visible spectrum luminescence used in an LED to produce white light, in the text is called VL, UV luminescence- abbreviated as UVL.

Section snippets

Methods of research and objects

YAG phosphors of the MG 397 and AWS 5 (Billion Light Co., LTD, Taiwan) series, YAG 01-YAG 06 (GrandLux Optoelectronics Co., LTD China) and SDL 2700, 3500, 4000 (NPO «Platan», RF) were selected for research.

The photoluminescence (PL) and the appropriate excitation spectra were measured with an Agilent Cary Eclipse spectrophotometer in the spectral range from 200 to 800 nm. To excite UV luminescence, we used radiation sources from deeper UV radiation: xenon lamps, specialized emitting chips,

Excitation and luminescence spectra of YAG:Ce phosphors

The excitation and luminescence spectra of the above-mentioned phosphors were measured. Fig. 1 shows, for example, in a general form, the excitation spectra of VL, UVL, and luminescence spectra. In the luminescence spectra of all investigated phosphors the band is observed due to radiative transitions in the Ce3+ ions 5d12F7/2 and 5d12F5/2. The maximum position of this band in all phosphors is different and falls on the region from 530 to 565 nm. In addition, after excitation by UV

Discussion and conclusion

The excitation of phosphors by photons in the range of 4.0–6.2 eV (310–200 nm) and by high-energy electron beam (0.25 MeV) leads in addition to VL also to the appearance of UVL. In all studied commercial phosphors, the excitation induced the UV luminescence with similar spectra, with the maximuma at 315–320 nm and 360–380 nm. The exact position of the bands depends on the phosphor prehistory.

The main results of the study allow us to draw the following conclusions.

  • 1.

    The intensities ratio of the

Declaration of Competing Interest

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

References (60)

  • Y. Qiang et al.

    J. Lumin.

    (2016)
  • Q. Sai et al.

    Opt. Mater.

    (2013)
  • A. Lushchik et al.

    Nucl. Instr. Meth. B

    (2012)
  • Y. Zhydachevskii et al.

    Opt. Mater.

    (2012)
  • A.O. Matkovskii et al.

    Opt. Mater.

    (1996)
  • S.M. Kaczmarek et al.

    Nucl. Instrum. Meth. Phys. Res. B

    (1997)
  • E. Polisadova et al.

    Opt. Mater.

    (2019)
  • A. Platonenko et al.

    Opt. Mater.

    (2020)
  • E. Elsts et al.

    Opt. Mater.

    (2015)
  • U. Rogulis et al.

    Radiation Measurements

    (2013)
  • P.V. Savchyn et al.

    Nucl. Instrum. Methods B

    (2012)
  • Yu. Zorenko et al.

    J. Lumin.

    (2014)
  • S. Nakamura

    InGaN quantum-well structure blue LEDs and LDs

    J. Lumin.

    (1997)
  • Y. Zorenko et al.

    Optical Mater.

    (2012)
  • M. Kucera et al.

    J. Lumin.

    (2016)
  • M. Nikl et al.

    J. Cryst. Growth.

    (2006)
  • X. Yang et al.

    Growth

    (2009)
  • Z. Onderisinova et al.

    J. Lumin.

    (2015)
  • V. Singh et al.

    Optik

    (2018)
  • E.A. Kotomin et al.

    Nucl. Instr. Meth. B

    (1998)
  • A.I. Popov et al.

    Nucl. Instr. Meth B

    (2010)
  • S.V. Nikiforov et al.

    Radiation Measurements.

    (2019)
  • D.V. Ananchenko et al.

    Nuclear Inst. Meth. B

    (2020)
  • A. Luchechko et al.

    Nucl. Instrum. Methods, B

    (2019)
  • M.L. Crespillo et al.

    App. Mat. Tod.

    (2018)
  • A. Lushchik et al.

    Nuclear Inst. and Meth. Phys. Res. B

    (2018)
  • A.V. Uklein et al.

    Opt. Mater.

    (2018)
  • A. Akilbekov et al.

    Nuclear Inst. Meth. Phys. Res. B

    (2020)
  • L. Bosi et al.

    Phys. Lett.

    (1970)
  • V. Lisitsyn et al.

    Nucl. Instrum. Methods Phys. Res. Sect. B

    (2016)
  • Cited by (6)

    • Investigation of brightness and decay characteristics of YAG:Ce<sup>3+</sup>, Ca-α-Sialon:Eu<sup>2+</sup> and CaAl<inf>12</inf>O<inf>19</inf>:Mn<sup>4+</sup> phosphors incorporated with Ni-doped SnO<inf>2</inf> particles

      2021, Journal of Luminescence
      Citation Excerpt :

      Also, the microsecond time scale measurement results were similar for both free- and metal oxide-doped YAG:Ce3+ blends. In accordance with the literature, the phosphor exhibited 9 μs (98.5%) and 236 μs (1.5%) of biexponential decay times [65]. The average decay time was calculated as 16 μs when combined with Ni-doped SnO2 particles.

    • Time-resolved luminescence of YAG:Ce and YAGG:Ce ceramics prepared by electron beam assisted synthesis

      2020, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and Atoms
      Citation Excerpt :

      Already the first attempts on such synthesis of magnesium fluoride (MgF2) and yttrium-aluminum garnet (YAG) ceramics demonstrated usefulness of this method [25–27]. Note that YAG:Ce is thoroughly studied and widely used for many applications [3,7–15,28–32]. The present paper is devoted to the study of luminescent characteristics (both steady-state and time-resolved ones) of YAG: Ce polycrystalline ceramics prepared by means of a powerful electron beam and their comparison with those of commercial YAG:Ce phosphors synthesized by various conventional methods.

    View full text