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Non-Ideal p-n junction Diode of Sb[sub x]Se[sub 1−x] (x = 0.4, 0.5, 0.6, 0.7) Thin Films

Falah I. MustafaShikha GuptaDepartment of Physics, Panjab University, Chandigarh ‐160014, IndiaNavdeep GoyalDepartment of Physics, Panjab University, Chandigarh ‐160014, IndiaS. K. TripathiDepartment of Physics, Panjab University, Chandigarh ‐160014, IndiaKeya DharamvirRanjan KumarG. S. S. Saini
2011en
ABI

Annotatsiya

We have made diodes consisting of the same alloy i.e. SbxSe1−x (⁠x = 0.4, 0.5, 0.6 and 0.7), but change the concentration of Sb metal from 40% to 70% atomic weight percentage. It is observed from the Hall measurements that the nature of charge carriers have changed from p‐ to n‐type at x = 0.6 for SbxSe1−x. We have measured I‐V characteristics of four p‐n junction diodes i.e. p‐Sb2Se3/n‐Sb3Se2, p‐Sb2Se3/n‐Sb7Se3, p‐SbSe/n‐Sb3Se2, p‐SbSe/n‐Sb7Se3. From the I‐V plots we have calculated the parameters as built‐in voltage (Vbi), forward resistance (Rf), ideal factor (n), saturation current (Io), breakdown current (IBd) and breakdown voltage (VBd).

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