<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JAMP</journal-id><journal-title-group><journal-title>Journal of Applied Mathematics and Physics</journal-title></journal-title-group><issn pub-type="epub">2327-4352</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jamp.2018.64058</article-id><article-id pub-id-type="publisher-id">JAMP-83653</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Phosphor Converted White Led with Improved CRI
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>P.</surname><given-names>J. Yadav</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>N.</surname><given-names>D. Meshram</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>C.</surname><given-names>P. Joshi</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>S.</surname><given-names>V. Moharil</given-names></name><xref ref-type="aff" rid="aff4"><sup>4</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Shri Mathuradas Mohota College of Science, Sakkardara, Nagpur, India</addr-line></aff><aff id="aff3"><addr-line>Physics Department, Shri Ramdeobaba K. N. Engineering College, Nagpur, India</addr-line></aff><aff id="aff1"><addr-line>Kamla Nehru Mahavidyalaya, Sakkardara, Nagpur, India</addr-line></aff><aff id="aff4"><addr-line>Department of Physics, R.T.M. Nagpur University, Nagpur, India</addr-line></aff><pub-date pub-type="epub"><day>02</day><month>04</month><year>2018</year></pub-date><volume>06</volume><issue>04</issue><fpage>657</fpage><lpage>662</lpage><history><date date-type="received"><day>5,</day>	<month>January</month>	<year>2018</year></date><date date-type="rev-recd"><day>9,</day>	<month>April</month>	<year>2018</year>	</date><date date-type="accepted"><day>12,</day>	<month>April</month>	<year>2018</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  
    Most of the commercial white LED lamps use blue chip coated with yellow emitting phosphor. YAG:Ce3+ phosphor is coated on blue chip to obtain white light. Though this is commercially successful, there are several drawbacks such as “halo effect”, poor colour rendition, etc. In recent years several efforts have been made to improve LED lamp performance. In this paper modifica-tion of YAG:Ce phosphor for improving CRI, by introducing Gd
   <sup>3+</sup>, Pr
   <sup>3+</sup> or Tb
   <sup>3+</sup> at Ce
   <sup>3+</sup> site is reported. 
  
 
</p></abstract><kwd-group><kwd>YAG</kwd><kwd> Phosphors</kwd><kwd> White LED</kwd><kwd> CRI and Commercial Phosphor etc.</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Solid state lighting based on high-brightness LEDs has emerged as a new potentially revolutionary technology that could save up to half the energy used for lighting applications. Compared with the traditional lighting, white LED has the following advantages; small (use of many kinds of associations and flexible array device), robust, long lifetime (more than 10,000 hours), low power consumption and low pollution. Thus, White LED would be the most important light source in the 21<sup>st</sup> century [<xref ref-type="bibr" rid="scirp.83653-ref1">1</xref>].</p><p>White LEDs, based on blue LED chips coated with a yellow emitting phosphor (YAG:Ce), were first reported in 1997 [<xref ref-type="bibr" rid="scirp.83653-ref2">2</xref>]. The blue chip/YAG:Ce system has many advantages. But the lamps fabricated in this manner give a poor colour rendering because the resulting light is typically deficient in the green and red colours. There are two approaches which are being followed to overcome this problem. In the first approach, white LEDs are made by coating near ultraviolet (n-UV) emitting LED with a mixture of high efficiency red, green and blue emitting phosphors [<xref ref-type="bibr" rid="scirp.83653-ref3">3</xref>], analogous to the fluorescent lamp. This method yields lamps with better colour rendition. Addition of a yellow emitting phosphor improves colour rendition index (CRI) further. Recently, much progress has been made for the emission efficiency of LED chips in the near UV-to-deep blue range [<xref ref-type="bibr" rid="scirp.83653-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.83653-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.83653-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.83653-ref7">7</xref>]. However, cost and light output wise, near UV chips are much inferior to blue chips. Thus, the second approach [<xref ref-type="bibr" rid="scirp.83653-ref8">8</xref>] comprising of coating blue excitable, green and red phosphors on blue chip, is considered to be more practicable for the time being. At present, LED lamps with YAG:Ce phosphor coated on the blue chip are dominating the market. In this paper modification of YAG:Ce phosphor for improving CRI, by introducing Gd<sup>3+</sup>, Pr<sup>3+</sup> or Tb<sup>3+</sup> at Ce<sup>3+</sup> site is reported.</p></sec><sec id="s2"><title>2. Experimental</title><p>Instead of the conventional solution combustion synthesis, we used the modified procedure which led to the formation of the desired compounds in a single step. Reagent grade (Indian Rare Earths, Ltd.) rare earth oxides/carbonates were converted to the corresponding nitrates by dissolving in nitric acid. The nitrates were dried by prolonged, gentle warming. Stoichiometric amounts of hydrated nitrates of yttrium, aluminium and cerium were thoroughly mixed with urea/ glycine. The nitrate to fuel ratios were calculated by the method described earlier [<xref ref-type="bibr" rid="scirp.83653-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.83653-ref10">10</xref>]. <xref ref-type="table" rid="table1">Table 1</xref> gives the details of the ingredients used in syntheses of various phosphors.</p><p>Due to the presence of large water of crystallization in aluminium nitrate, a thick paste was formed. A china dish containing the paste was inserted in a furnace preheated to 500˚C. Within minutes the paste foamed and a flame was produced which lasted for several seconds. The china dish was immediately removed from the furnace. X-ray diffraction patterns were recorded on Philips PANalytical X’pert Pro diffractometer. PL characteristics in the range of 200 - 700 nm, at room temperature were studied using a Hitachi F-4000 spectrofluorimeter, with 1.5 nm spectral slit width.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Combustion mixtures used in preparation of various phosphors</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Sr. No.</th><th align="center" valign="middle"  rowspan="2"  >Composition</th><th align="center" valign="middle"  colspan="6"  >Ingredients mol ratios</th><th align="center" valign="middle"  rowspan="2"  >CRI</th></tr></thead><tr><td align="center" valign="middle" >YN:</td><td align="center" valign="middle" >CeN:</td><td align="center" valign="middle" >Tb/Gd/PrN:</td><td align="center" valign="middle" >AlN:</td><td align="center" valign="middle" >Glycine:</td><td align="center" valign="middle" >Urea</td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >Y<sub>3</sub>Al<sub>5</sub>O<sub>12</sub></td><td align="center" valign="middle" >3.0:</td><td align="center" valign="middle" >0:</td><td align="center" valign="middle" >0:</td><td align="center" valign="middle" >5:</td><td align="center" valign="middle" >5:</td><td align="center" valign="middle" >12.5</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >Y<sub>2.979</sub>Ce<sub>0.021</sub>Al<sub>5</sub>O<sub>12</sub></td><td align="center" valign="middle" >2.985:</td><td align="center" valign="middle" >0.015:</td><td align="center" valign="middle" >0:</td><td align="center" valign="middle" >5:</td><td align="center" valign="middle" >5:</td><td align="center" valign="middle" >12.5</td><td align="center" valign="middle" >65 - 70</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >Y<sub>2.964</sub>Ce<sub>0.021</sub>Pr<sub>0.015</sub>Al<sub>5</sub>O<sub>12</sub></td><td align="center" valign="middle" >2.964:</td><td align="center" valign="middle" >0.021:</td><td align="center" valign="middle" >0.015:</td><td align="center" valign="middle" >5:</td><td align="center" valign="middle" >5:</td><td align="center" valign="middle" >12.5</td><td align="center" valign="middle" >78 - 81</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >Y<sub>2.879</sub>Ce<sub>0.021</sub>Gd<sub>0.100</sub>Al<sub>5</sub>O<sub>12</sub></td><td align="center" valign="middle" >2.879:</td><td align="center" valign="middle" >0.021:</td><td align="center" valign="middle" >0.100:</td><td align="center" valign="middle" >5:</td><td align="center" valign="middle" >5:</td><td align="center" valign="middle" >12.5</td><td align="center" valign="middle" >77 - 82</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >Y<sub>2.179</sub>Ce<sub>0.021</sub>Tb<sub>0.800</sub>Al<sub>5</sub>O<sub>12</sub></td><td align="center" valign="middle" >2.179:</td><td align="center" valign="middle" >0.021:</td><td align="center" valign="middle" >0.800:</td><td align="center" valign="middle" >5:</td><td align="center" valign="middle" >5:</td><td align="center" valign="middle" >12.5</td><td align="center" valign="middle" >77 - 82</td></tr></tbody></table></table-wrap><p>YN&#224;Y(NO<sub>3</sub>)<sub>3</sub>.6H<sub>2</sub>O,Ce/Tb/Gd/PrN&#224;Ce/Tb/Gd/PrN(NO<sub>3</sub>)<sub>3</sub>.6H<sub>2</sub>O, AlN&#224;Al(NO<sub>3</sub>)<sub>3</sub>.9H<sub>2</sub>O.</p><p>The phosphor (3 wt.%) was dispersed in a transparent silicone resin (Wells Electronic Materials Company, 5012-2A and 5012-2B), and LED was then fabricated by coating the blue LED chip (CREE 458 nm, 300 micron) with the epoxy resin. The electroluminescence (EL) spectra, colour temperature, CIE chromaticity coordinates, CRI and lumen output at room temperature were measured using a 300 mm integrating sphere and lumen meter (Hangzhou Zhongwei Photoelectricity Company ZVision ZW 3900). The measurements were carried out at 3.2 V, 20 mA.</p></sec><sec id="s3"><title>3. Results and Discussion</title><p>Yang et al. [<xref ref-type="bibr" rid="scirp.83653-ref11">11</xref>] prepared YAG using combustion synthesis with urea as a fuel. However, the combustion product was admixture of YAG and YAP . Repeated sintering for 5 hrs at 1000 C was necessary to obtain YAG. More or less similar results were obtained by Pan et al. [<xref ref-type="bibr" rid="scirp.83653-ref12">12</xref>]. Fu et al. [<xref ref-type="bibr" rid="scirp.83653-ref13">13</xref>] used carbohydrazide fuel, but annealing at 1150 C for 6 hours was required to achieve good crystallinity and PL intensity. In our experiments, when urea was used as a fuel, the combustion products were poorly crystallized. Yttrium nitrate does not have exothermic reaction with urea. Hence we tried mixed (Glycine + urea) fuel. Glycine has exothermic reaction with Yttrium nitrate and urea with aluminum nitrate. XRD pattern of the product obtained with this fuel is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>.</p><p>An excellent match is obtained with ICDD file 88 - 2048 corresponding to YAG. No lines corresponding to YAP (2 theta = 33.36), YAM (2 theta = 29.289) or YAH (2 theta = 32.832) could be seen.</p><p>Phase pure YAG is thus obtained in a single step combustion process without any additional thermal treatment when mixed fuel (Glycine + urea) was used. Activation with Ce<sup>3+</sup> was also attempted by adding cerous nitrate to the combustion mixture.</p><p><xref ref-type="fig" rid="fig2">Figure 2</xref> shows PL results for the phosphor so prepared. For 465 nm excitation, intense emission was observed with a broad maximum at 528 nm and</p><p>a shoulder around 540 nm (<xref ref-type="fig" rid="fig2">Figure 2</xref>, curve b). This is in excellent agreement with the recent literature results [<xref ref-type="bibr" rid="scirp.83653-ref14">14</xref>]. The excitation spectrum (<xref ref-type="fig" rid="fig2">Figure 2</xref>, curve a), consists of several bands; those around 460 and 340 nm being prominently seen. These positions are also in close agreement with the most of the literature results on YAG:Ce phosphors. Moreover, no emission attributable to YAP or YAM phases was observed.</p><p>LEDs fabricated by coating YAG:Ce on blue chip have poor CRI, typically in the range 65 - 70. Shifting the spectrum to longer wavelengths or adding red component can improve CRI. <xref ref-type="fig" rid="fig2">Figure 2</xref> shows effect of replacing Y partly by Gd on the emission spectrum. It is seen that with increasing Gd concentration, maxmimum shifts to longer wavelengths. However, intensity also decreases at the same time. Similar effect can be achieved by substituting Tb at Y site (<xref ref-type="fig" rid="fig3">Figure 3</xref>, curve c).</p><p>The shift is related to the lattice expansion caused by substituting smaller Y ion by bigger rare earth ions. In Pr<sup>3+</sup> co-doped sample, there is partial energy transfer from Ce<sup>3+</sup> to Pr<sup>3+</sup>. Pr<sup>3+</sup> emission corresponding to <sup>3</sup>P<sub>o</sub>-- &gt; <sup>3</sup>H<sub>6</sub>, <sup>3</sup>F<sub>2</sub> is around 605 nm. Pr<sup>3+</sup> co-doping thus adds red component to YAG: Ce PL (<xref ref-type="fig" rid="fig3">Figure 3</xref>, curve b).</p><p><xref ref-type="fig" rid="fig4">Figure 4</xref> shows emission spectra for LEDs fabricated by coating (a) Y<sub>2.879</sub>Ce<sub>0.021</sub>Pr<sub>0.010</sub>Al<sub>5</sub>O<sub>12</sub>,Y<sub>2.879</sub>Gd<sub>0.1</sub>Ce<sub>0.021</sub>Al<sub>5</sub>O<sub>12</sub> (b) or Y<sub>2.879</sub>Ce<sub>0.021</sub>Tb<sub>0.010</sub>Al<sub>5</sub>O<sub>12</sub> (c) on blue chip. As shown in <xref ref-type="table" rid="table1">Table 1</xref>, CRI improves considerably compared to that for LED fabricated using YAG:Ce. Colour temperature for all the LEDs is around 6000 K and colour co-ordinates are typically 0.319, 0.326.</p></sec><sec id="s4"><title>4. Conclusion</title><p>Using Gd or Tb co-dopants, Ce<sup>3+</sup> emission in YAG:Ce could be shifted to longer wavelengths. The shift is due to lattice expansion. On the other hand, co-dopant</p><p>Pr<sup>3+</sup> results in adding red component to PL emission due to partial energy transfer from Ce<sup>3+</sup> to Pr<sup>3+</sup>. All these modification lead to LEDs with considerably improved CRI.</p></sec><sec id="s5"><title>Acknowledgements</title><p>PJY thanks the Department of Science and Technology, New Delhi for Women Scientist award.</p></sec><sec id="s6"><title>Cite this paper</title><p>Yadav, P.J., Meshram, N.D., Joshi, C.P. and Moharil, S.V. (2018) Phosphor Converted White Led with Improved CRI. Journal of Applied Mathematics and Physics, 6, 657-662. https://doi.org/10.4236/jamp.2018.64058</p></sec></body><back><ref-list><title>References</title><ref id="scirp.83653-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Zhang, X.M., Park, B., Choi, N., Kim, J., Kim, G.C. and Yoo, J.H. (2009) Mater.lett., 63, 700.</mixed-citation></ref><ref id="scirp.83653-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Nakamura, S. and Fasol, G. (1997) The Blue Laser Diode: GaN Based Light Emitters and Lasers. Spring, Heidelberg.</mixed-citation></ref><ref id="scirp.83653-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Xu, Y., Chen, L., Li, Y., Song, G., Wang, Y., Zhuang, W. and Long, Z. (2008) Appl Phys Lett., 92, 021129.</mixed-citation></ref><ref id="scirp.83653-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Khizar, M., Fan, Z.Y., Kim, K.H., Lin, J.Y. and Jiang H.X. (2005) Appl Phys Lett, 86, Article ID: 173504.</mixed-citation></ref><ref id="scirp.83653-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Chen, L., Lin, C.-C., Yeh, C.-W. and Liu, R.-S. (2010) Materials, 3, 2172.</mixed-citation></ref><ref id="scirp.83653-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Xie, R.-J., Hirosaki, N., Li, Y.Q. and Takeda, T. (2010) Materials, 3, 3777.</mixed-citation></ref><ref id="scirp.83653-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Ye, S., Xiao, F., Pan, Y.X., Ma, Y.Y. and Zhang, Q.Y. (2010) Mater. Sci. Engg. R, 71, 1.</mixed-citation></ref><ref id="scirp.83653-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Shimizu, Y., Sakano, K., Noguchi, Y. and Moriguchi, T. (1999) U.S. Patent 1999; 5998925.</mixed-citation></ref><ref id="scirp.83653-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Kingsley, J.J., Suresh, K. and Patil, K.C. (1990) J. Mater. Sci., 25 1305.</mixed-citation></ref><ref id="scirp.83653-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Kingsley, J.J., Manickam, N. and Patil, K.C. (1990) Bull. Mater. Sci., 13, 179.</mixed-citation></ref><ref id="scirp.83653-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Yang, Z.P., Li, X., Yang, Y. and Li, X.M. (2006) Proc. SPIE 6033 60330N.</mixed-citation></ref><ref id="scirp.83653-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Pan, Y., Wu, M. and Su, Q. (2004) J. Phys. Chem. Solids, 65, 845. https://doi.org/10.1016/j.jpcs.2003.08.018</mixed-citation></ref><ref id="scirp.83653-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">Fu, Y.-P., Wen, S.-B. and Hsu, C.-S. (2008) J.Alloys.Compd., 458, 318.</mixed-citation></ref><ref id="scirp.83653-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">Jiao, H., Ma, Q., He, L., Liu, Z. and Wu, Q. (2010) Powder Technology, 198, 229.</mixed-citation></ref></ref-list></back></article>