2023
DOI: 10.35848/1347-4065/acc70d
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The improvement of Schottky barrier diodes fabricated only by B ion implantation doping accomplished by refinement of the electrode structure

Abstract: In this study, we fabricated p-type diamond Schottky barrier diodes, and performed selective B doping for the p-type channel and Ohmic region by double ion implantation. Schottky barrier diodes were redesigned the configuration and the shape of Ohmic and Schottky electrodes to improve device characteristics. The fabricated device exhibited a rectification ratio of approximately 2400 because of decreasing the parasitic resistance to 2.7 × 107 Ω and the ideality factor to 2.7. The Schottky barrier height was obt… Show more

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Cited by 3 publications
(3 citation statements)
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“…Details of the fitting process can be referred in the previous letter. [ 19 ] To estimate the ionization energy of dopants, we should best‐fit the theoretically estimated carrier concentration by Equation () to the experimentally obtained one with three fitting parameters of acceptor concentration ( N A ), compensation ratio ( K = N D / N A ), and ionization energy ( E A ). Particularly at the low carrier concentration limit false( p N D N A $\left(\right.…”
Section: Resultsmentioning
confidence: 99%
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“…Details of the fitting process can be referred in the previous letter. [ 19 ] To estimate the ionization energy of dopants, we should best‐fit the theoretically estimated carrier concentration by Equation () to the experimentally obtained one with three fitting parameters of acceptor concentration ( N A ), compensation ratio ( K = N D / N A ), and ionization energy ( E A ). Particularly at the low carrier concentration limit false( p N D N A $\left(\right.…”
Section: Resultsmentioning
confidence: 99%
“…We then reluctantly estimate the ionization energy of these samples by Equation () as fitting parameters of A and E A in the mainly high‐temperature region of T < 0.002 K 1 $T &amp;#x00026;amp;amp;amp;amp;amp;amp;amp;amp;amp;amp;lt; 0.002 \left(\text{K}\right)^{- 1}$ , in which the influence of hopping conduction will be neglected. [ 19,20 ] Here, the arbitrary parameter A was merely introduced to adjust the magnification of the vertical axis in the fitting process. The estimated ionization energy is summarized in Table 1.…”
Section: Resultsmentioning
confidence: 99%
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