Transport Critical Current Density of (Bi<sub>1.6</sub>Pb<sub>0.4</sub>)Sr<sub>2</sub>Ca<sub>2</sub>Cu<sub>3</sub>O<sub>10</sub> Ceramic Superconductor with Different Nanosized Co<sub>3</sub>O<sub>4</sub> Addition

<table>The critical current density as function of temperature for (a) 10 nm, (b) 30 nm, and (c) 50 nm Co<sub>3</sub>O<sub>4</sub> added Bi-2223 samples. </table>

Advances in Condensed Matter Physics

fig6

Figure 6

Figure 6: Transport Critical Current Density of (Bi<sub>1.6</sub>Pb<sub>0.4</sub>)Sr<sub>2</sub>Ca<sub>2</sub>Cu<sub>3</sub>O<sub>10</sub> Ceramic Superconductor with Different Nanosized Co<sub>3</sub>O<sub>4</sub> Addition 

Advances in Condensed Matter Physics

Transport Critical Current Density of (Bi1.6Pb0.4)Sr2Ca2Cu3O10 Ceramic Superconductor with Different Nanosized Co3O4 Addition

Figure 6

Transport Critical Current Density of (Bi_1.6Pb_0.4)Sr₂Ca₂Cu₃O₁₀ Ceramic Superconductor with Different Nanosized Co₃O₄ Addition