2018
DOI: 10.1063/1.4994241
|View full text |Cite
|
Sign up to set email alerts
|

Single photon sources in 4H-SiC metal-oxide-semiconductor field-effect transistors

Abstract: We present single photon sources (SPSs) embedded in 4H-SiC metal-oxide-semiconductor fieldeffect transistors (MOSFETs). They are formed in the SiC/SiO 2 interface regions of wet-oxidation C-face 4H-SiC MOSFETs and were not found in other C-face and Si-face MOSFETs. Their bright room-temperature photoluminescence (PL) was observed in the range from 550 to 750 nm and revealed variable multi-peak structures as well as variable peak shifts. We characterized a wide variety of their PL spectra as the inevitable vari… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

2
15
1

Year Published

2018
2018
2022
2022

Publication Types

Select...
8
1

Relationship

1
8

Authors

Journals

citations
Cited by 25 publications
(31 citation statements)
references
References 16 publications
2
15
1
Order By: Relevance
“…The low-temperature PL spectrum at the radiation point exhibits a very sharp peak at 580 nm, while a broad peak is observed around 610 nm at RT. The spectra in the inset of figure 4, derived by subtracting the background spectrum, also indicate that the broad peak at RT is red-shifted from the sharp peak at 80 K. Thus, the broad peak observed at RT is entirely composed of PSB, which is observed as the ZPL solely at 80 K. This interpretation corroborates a previous study [20] but contradicts another study [21]. This will be discussed further in a future report.…”
Section: Resultssupporting
confidence: 80%
“…The low-temperature PL spectrum at the radiation point exhibits a very sharp peak at 580 nm, while a broad peak is observed around 610 nm at RT. The spectra in the inset of figure 4, derived by subtracting the background spectrum, also indicate that the broad peak at RT is red-shifted from the sharp peak at 80 K. Thus, the broad peak observed at RT is entirely composed of PSB, which is observed as the ZPL solely at 80 K. This interpretation corroborates a previous study [20] but contradicts another study [21]. This will be discussed further in a future report.…”
Section: Resultssupporting
confidence: 80%
“…Each consists of sharp high-energy local-vibration modes between 150 and 220 meV. These are greater in energy than the highest first-order Raman mode found in SiC (120 meV, or 960 cm −1 ) and have energy ranges consistent with the vibrational modes of carbon and possibly oxygen-related bonds in SiC [26,42,43]. The source of the excess C is a by-product of the thermal-oxidation process and is known to make a considerable contribution to defects near or at the SiC/SiO 2 interface [3,44,45].…”
Section: Resultsmentioning
confidence: 89%
“…Photoluminescence (PL) has also been used extensively to characterize deep-level defects in bulk SiC. Recently, the optical properties of defects formed after oxidation near the SiC/SiO 2 interface were also investigated [22][23][24][25][26][27][28][29][30][31]. These defects can be addressed individually when an appropriate excitation wavelength is used.…”
Section: Introductionmentioning
confidence: 99%
“…Contradicting explanations of the nature of these dangling bonds can be found in the literature, suggesting either carbon [33][34][35][36] or silicon dangling bonds [37][38][39]. Considering the large number of zero-phonon lines observed in low and room temperature PL for similar oxidation processes on 4H-C [40,41], correlated C dangling bonds with large varieties of possible geometries and backbone structures as proposed in Ref. [33] might be likely candidates.…”
Section: Discussionmentioning
confidence: 77%