• Journal of Semiconductors
  • Vol. 40, Issue 2, 022804 (2019)
P. Vigneshwara Raja1 and N. V. L. Narasimha Murty2
Author Affiliations
  • 1Micro-Fabrication and Characterization Lab, School of Electrical Sciences, IIT Bhubaneswar, Odisha-752050, India
  • 2Electrical Engineering, IIT Tirupati, Tirupati, Andhra Pradesh-517506, India
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    DOI: 10.1088/1674-4926/40/2/022804 Cite this Article
    P. Vigneshwara Raja, N. V. L. Narasimha Murty. Thermally annealed gamma irradiated Ni/4H-SiC Schottky barrier diode characteristics[J]. Journal of Semiconductors, 2019, 40(2): 022804 Copy Citation Text show less

    Abstract

    Thermal annealing effects on gamma irradiated Ni/4H-SiC Schottky barrier diode (SBD) characteristics are analyzed over a wide range of temperatures (400–1100 °C). The annealing induced variations in the concentration of deep level traps in the SBDs are identified by thermally stimulated capacitance (TSCAP). A little decrease in the trap density at EC – 0.63 eV and EC – 1.13 eV is observed up to the annealing temperature of 600 °C. Whereas, a gamma induced trap at EC – 0.89 eV disappeared after annealing at 500 °C, revealing that its concentration (< 1013 cm-3) is reduced below the detection limit of the TSCAP technique. The electrical characteristics of irradiated SBDs are considerably changed at each annealing temperature. To understand the anomalous variations in the post-annealing characteristics, the interface state density distribution in the annealed SBDs is extracted. The electrical properties are improved at 400 °C due to the reduction in the interface trap density. However, from 500 °C, the electrical parameters are found to degrade with the annealing temperature because of the increase in the interface trap density. From the results, it is noted that the rectifying nature of the SBDs vanishes at or above 800 °C.
    ${E_ {\rm{T}}} = k{T_{1/2}} \ln {\frac{{vk{T_{1/2}}}}{{q\left( {{E_ {\rm{T}}} + 2k{T_{1/2}}} \right)}}} ,$(1)

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    ${N_ {\rm{T}}} = \frac{{2\left( {{C_2} - {C_1}} \right)}}{{{C_1}}}{N_ {\rm{d}}},$(2)

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    ${\varPhi _ {\rm{eff}}} = {\varPhi _ {\rm{B}}} + \left( {1 - \frac{1}{{n({V_ {\rm{F}}})}}} \right){V_ {\rm{F}}},$(3)

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    $n({V_ {\rm{F}}}) = \frac{{q{V_ {\rm{F}}}}}{{kT \ln ({I_ {\rm{F}}}/{I_ {\rm{S}}})}},$(4)

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    ${N_ {\rm{SS}}} = \frac{1}{q}\left\{ {\frac{{{\varepsilon _ {\rm{i}}}}}{\delta }\left[ {n({V_ {\rm{F}}}) - 1} \right] - \frac{{{\varepsilon _ {\rm{s}}}}}{W}} \right\},$(5)

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    ${E_ {\rm{C}}} - {E_ {\rm{SS}}} = q({\varPhi _ {\rm{eff}}} - {V_ {\rm{F}}}).$(6)

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    P. Vigneshwara Raja, N. V. L. Narasimha Murty. Thermally annealed gamma irradiated Ni/4H-SiC Schottky barrier diode characteristics[J]. Journal of Semiconductors, 2019, 40(2): 022804
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