Au/(nanocarbon-PVP)/n-Si SDs were fabricated and their current-conduction mechanisms (CCMs) have been examined in elaborative by utilizing current-voltage (I-V) characteristics in temperature range of 60-340K at (± 3V) ranges. The values of ideality factor (n) and zero-bias barrier height (ΦBo) determined from the linear-part of semilogarithmic forward bias IF-VF properties based on Thermionic-Emission (TE) theory revealed that decrease in ΦBo and increase in n with deccreasing temperature. Additionally, Richardson constant (A*) value was found several orders lower than its theoretical value. The values of ΦBo and n changed from 0.173 eV to 0.837 eV and 6.60 to 2.85 with increasing temperature from 60 K to 340 K. This positive temperature-coefficient (α) of ΦBo is inagreement with the bandgap of semiconductor or barrier height (BH) for the ideal diode. The calculated higher value of n at low temperatures was attributed to the inhomogeneities of BH rather than the interlayer, surface-states (Nss), and image-force lowering. With lowing temperatures, CCMs may be governed by tunneling over the lower barriers, via Nss, and generation recombination (GR), as well as TE and hence a complete description of CCM and understanding of the formation BH, remain a compelling problem. Nss-(Ec-Ess) profile was also obtained from IF-VF data for each temperature.

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Posted 09 Feb, 2021
Posted 09 Feb, 2021
Au/(nanocarbon-PVP)/n-Si SDs were fabricated and their current-conduction mechanisms (CCMs) have been examined in elaborative by utilizing current-voltage (I-V) characteristics in temperature range of 60-340K at (± 3V) ranges. The values of ideality factor (n) and zero-bias barrier height (ΦBo) determined from the linear-part of semilogarithmic forward bias IF-VF properties based on Thermionic-Emission (TE) theory revealed that decrease in ΦBo and increase in n with deccreasing temperature. Additionally, Richardson constant (A*) value was found several orders lower than its theoretical value. The values of ΦBo and n changed from 0.173 eV to 0.837 eV and 6.60 to 2.85 with increasing temperature from 60 K to 340 K. This positive temperature-coefficient (α) of ΦBo is inagreement with the bandgap of semiconductor or barrier height (BH) for the ideal diode. The calculated higher value of n at low temperatures was attributed to the inhomogeneities of BH rather than the interlayer, surface-states (Nss), and image-force lowering. With lowing temperatures, CCMs may be governed by tunneling over the lower barriers, via Nss, and generation recombination (GR), as well as TE and hence a complete description of CCM and understanding of the formation BH, remain a compelling problem. Nss-(Ec-Ess) profile was also obtained from IF-VF data for each temperature.

Figure 1

Figure 2

Figure 3

Figure 4

Figure 5

Figure 6

Figure 7

Figure 8

Figure 9

Figure 10

Figure 12

Figure 13
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