2020
DOI: 10.1007/s41871-020-00061-8
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Photoluminescence and Raman Spectroscopy Study on Color Centers of Helium Ion-Implanted 4H–SiC

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Cited by 19 publications
(5 citation statements)
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“…Although some previous studies have investigated B diffusion for p-type doping [3], a high density of boron-related deep levels [4] is generated, which degrade electrical activation. On the other hand, due to the smaller energy gap to the valence band and a strong tendency to occupy atomic sites in the silicon sublattice [5,6], and since Al does not appear an abnormal out-diffusion phenomenon as B-doped SiC during annealing [7], Al is preferred. Influenced by constraints such as doping amount and impurity atomic distribution, lowresistance p-type SiC preparation is still a difficult problem to be solved [8], because of ion implantation-induced defects which severely limit carrier lifetime and the effectiveness of doping [9].…”
Section: Introductionmentioning
confidence: 99%
“…Although some previous studies have investigated B diffusion for p-type doping [3], a high density of boron-related deep levels [4] is generated, which degrade electrical activation. On the other hand, due to the smaller energy gap to the valence band and a strong tendency to occupy atomic sites in the silicon sublattice [5,6], and since Al does not appear an abnormal out-diffusion phenomenon as B-doped SiC during annealing [7], Al is preferred. Influenced by constraints such as doping amount and impurity atomic distribution, lowresistance p-type SiC preparation is still a difficult problem to be solved [8], because of ion implantation-induced defects which severely limit carrier lifetime and the effectiveness of doping [9].…”
Section: Introductionmentioning
confidence: 99%
“…It saturates at 5 × 10 13 cm −2 and then drops down due to ion‐induced damage of the SiC crystalline structure. [ 27 ] The grayscale for focused ion‐beam writing [ 28 ] is chosen such that the maximum logical 8‐bit state is coded with Φ max σ HIM . Here, σ HIM is the area determined by the lateral straggling obtained from SRIM (Stopping and Range of Ions in Matter) simulation.…”
Section: Resultsmentioning
confidence: 99%
“…The system also has a coincident secondary electron microscope (SEM) to allow for nondestructive imaging and sample localization. Current applications being explored with the P-NAME tool include developing nanotechnologies such as solid-state impurity-ion and defect qubit devices (e.g., Sb in silicon, [23] color centers across a range of materials such as in diamond, [24][25][26] hexagonal boron nitride, [27,28] and also in silicon carbide [29,30] ) and isotopic materials synthesis (and enrichment), the doping of nanoscale systems (e.g., Mn doping of epitaxial quantum dots and nanowires), ion beam lithography, doping of photonic waveguide structures (e.g., Er implanted into LiNbO 3 [31] ), and others. In this work, we present the isotopic mass spectra of a range of LMAISs that have been developed for the P-NAME tool.…”
Section: Introductionmentioning
confidence: 99%