Dielectric Properties of La<sub>2</sub>O<sub>3</sub> Doped Composite (Pb<sub><i>x</i></sub>Sr<sub>1−<i>x</i></sub>)TiO<sub>3</sub> Borosilicate Glass Ceramic

<table class="table-group" id="tab1"><tr><td><table class="table"><tr><td class="thead-hr" colspan="7"><hr/></td></tr><tr class="thead"><td align="left">Glass ceramic codes</td><td align="center">Grain size <br/>(<i>μ</i>m)</td><td align="center"><svg height="15.8375" id="M43" style="vertical-align:-3.3907pt" version="1.1" viewbox="0 0 16.9 15.8375" width="16.9" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink">
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</svg> at 1 KHz <br/>(°C)</td><td align="center"><svg height="11.9625" id="M44" style="vertical-align:-3.3907pt" version="1.1" viewbox="0 0 12.7375 11.9625" width="12.7375" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink">
<g transform="matrix(.017,-0,0,-.017,.062,7.675)"><path d="M387 375q0 -16 -17 -31t-29 -15q-9 0 -12 13q-13 74 -80 74q-36 0 -61 -24.5t-25 -56.5t24 -51.5t68 -19.5q33 0 47 2l2 -7l-32 -42q-20 2 -54 2q-45 0 -74 -21.5t-29 -60.5q0 -41 28 -65.5t73 -24.5q78 0 145 67l17 -23q-33 -47 -84.5 -75t-111.5 -28q-70 0 -114.5 35.5
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<g transform="matrix(.012,-0,0,-.012,7.037,11.762)"><path d="M393 379q-9 -16 -28 -29q-15 -10 -23 -2q-19 19 -36 19q-21 0 -52 -38q-57 -72 -82 -126l-40 -197q-23 -3 -75 -18l-7 7q49 196 74 335q7 43 -2 43q-7 0 -30 -14.5t-47 -37.5l-16 23q37 42 82 73t67 31q41 0 15 -113l-11 -50h4q41 71 85 117t77 46q29 0 45 -26
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</svg> at 1 KHz at RT</td><td align="center">Dissipation factor <svg height="11.175" id="M45" style="vertical-align:-0.0pt" version="1.1" viewbox="0 0 13.775 11.175" width="13.775" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink">
<g transform="matrix(.017,-0,0,-.017,.062,11.113)"><path d="M780 372q0 -191 -178 -297q-128 -75 -335 -75h-250l7 27q61 7 77 22t28 76l77 398q11 62 0 76.5t-77 22.5l6 28h292q164 0 258.5 -67.5t94.5 -210.5zM678 375q0 119 -73 180.5t-201 61.5q-62 0 -82 -13q-17 -7 -25 -53l-80 -427q-8 -47 -4 -62t26 -20q24 -6 80 -6
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</svg> at 1 KHz at RT</td><td align="center"><svg height="11.9625" id="M46" style="vertical-align:-3.3907pt" version="1.1" viewbox="0 0 12.7375 11.9625" width="12.7375" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink">
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</svg> at <svg height="15.8375" id="M47" style="vertical-align:-3.3907pt" version="1.1" viewbox="0 0 16.9 15.8375" width="16.9" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink">
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</svg></td><td align="center"><svg height="15.8375" id="M48" style="vertical-align:-3.3907pt" version="1.1" viewbox="0 0 16.9 15.8375" width="16.9" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink">
<g transform="matrix(.017,-0,0,-.017,.062,11.55)"><path d="M649 676l-22 -187l-33 -2q3 56 -12 94q-8 20 -31.5 26.5t-86.5 6.5h-74l-90 -491q-4 -23 -6 -36.5t1 -25t7 -16.5t18 -9t27 -5t41 -3l-6 -28h-286l4 28q68 5 84 18.5t28 76.5l94 491h-55q-74 0 -100.5 -6t-41.5 -23q-24 -29 -54 -98l-32 1q32 98 53 188h22q7 -18 15 -22
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</svg> ceramics [<a href="/journals/jceram/2013/879758/#B4">4</a>]</td></tr><tr><td class="thead-hr" colspan="7"><hr/></td></tr><tr><td align="left">PTL5B700T</td><td align="center">2.25</td><td align="center">481</td><td align="center">40</td><td align="center">0.0102</td><td align="center">542</td><td align="center">495</td></tr><tr><td align="left">8PL5B726T</td><td align="center">3.01</td><td align="center">320</td><td align="center">114</td><td align="center">0.1990</td><td align="center">1852</td><td align="center">323</td></tr><tr><td align="left">7PL5B739T</td><td align="center">1.05</td><td align="center">250</td><td align="center">275</td><td align="center">0.2706</td><td align="center">2158</td><td align="center">283</td></tr><tr><td align="left">6PL5B730T</td><td align="center">0.80</td><td align="center">219</td><td align="center">726</td><td align="center">0.0877</td><td align="center">8260</td><td align="center">211</td></tr><tr><td align="left">5PL5B806T</td><td align="center">2.22</td><td align="center">140</td><td align="center">494</td><td align="center">0.6636</td><td align="center">1921</td><td align="center">120</td></tr><tr class="table-tr"><td colspan="7"><hr class="tbody-hr"/></td></tr></table></td></tr></table>

Dielectric characteristics of various glass-ceramic samples in the system [(Pb<sub><i>x</i></sub>Sr<sub>1−<i>x </i></sub>)O·TiO<sub>2</sub>]-[2SiO<sub>2</sub>·B<sub>2</sub>O<sub>3</sub>]-[K<sub>2</sub>O]-[BaO]-La<sub>2</sub>O<sub>3</sub>.

Journal of Ceramics

tab1

Table 1

Table 1: Dielectric Properties of La<sub>2</sub>O<sub>3</sub> Doped Composite (Pb<sub><i>x</i></sub>Sr<sub>1−<i>x</i></sub>)TiO<sub>3</sub> Borosilicate Glass Ceramic 

Journal of Ceramics

Dielectric Properties of La2O3 Doped Composite (PbxSr1−x)TiO3 Borosilicate Glass Ceramic

Table 1

Dielectric Properties of La₂O₃ Doped Composite (Pb_xSr_1−x)TiO₃ Borosilicate Glass Ceramic