Mooney Lab - Physics of Semiconductor Defects
Projects (2005-2016)

 

Defects at Insulator/Semiconductor Interfaces
SiO2/SiC Interfaces

Wide bandgap semiconductors are of interest for applications requiring devices capable of operating at elevated temperature and at high power, for example, in circuits used in hybrid cars and for electric power distribution. In addition to a bandgap of 3.26 eV, 4H-SiC is especially promising for high-frequency MOSFET applications because of the high electron mobility, ~800 cm2/Vs, and because an SiO2 layer can be formed on the wafer surface by thermal oxidation. However, the high density of interface states near the conduction band edge reduces electron mobility to only ~5 cm2/Vs in n-channel MOSFETs. Recently it was shown that annealing in NO after thermal oxidation of 4H-SiC reduces the interface state density by a factor of ~10 with a corresponding increase in the electron mobility in MOSFETs. But the mobility remains about an order of magnitude lower than in bulk 4H-SiC. We use high frequency capacitance techniques, both temperature dependent capacitance-voltage and transient capacitance measurements, to investigate near-interface defects. These techniques allow us to detect electrons captured and emitted at defect energy states. From their trapping behavior, we can distinguish different defect species and investigate their properties. Our measurements revealed several diferent near-interface defect species in NO annealed samples. Two are located in the oxide, likely C dimers on oxygen sites and Si interstitials, and a third, possibly C di-interstitials, is located in the SiC [1,2]. Another method of delivering N to the SiO2/SiC interface is by ion-implantation of N into the SiC prior to oxidation. In these samples we found the same oxide traps, but at a higher density than in NO annealed samples. The C-related defect in SiC was not observed, and this may account in part for the higher electron mobility in MOSFETS fabricated by this process [3]. Recently the effects of Na contamination on interface defects in the oxide were investigated [4]. The C-related defect in SiC was not observed in samples prepared by sodium enhanced oxidation.

1. 

“Effects of antimony (Sb) on electron trapping near SiO2/4H-SiC interfaces”, P.M. Mooney, Zenan Jiang, A.F. Basile, Yongju Zheng, and Sarit Dhar, J. Appl. Phys. 120, 034503 (2016).

2.  “Channel mobility and threshold voltage characterization of 4H-SiC MOSFET with antimony channel implantation”, Yongju Zheng, T. Isaacs-Smith, A.C Ahyi, S. Dhar and P.M. Mooney, in 2015 IEEE 3rd Workshop on Wide-Bandgap Power Devices and Applications (WiPDA), 253 (2015).
3. 

"Effects of sodium ions on trapping and transport of electrons at the SiO2/4H-SiC interface", A.F. Basile, A.C. Ahyi, L.C. Feldman, J.R. Williams, and P.M. Mooney, J. Appl. Phys. 115, 034502 (2014).

4. 

"Modeling of high-frequency capacitance-voltage characteristics to quantify trap distrubutions near SiO2/SiC interfaces", A.F. Basile and P.M. Mooney, J. Appl. Phys. 111, 094509 (2012).

5. 

"Capacitance-voltage and deep-level-transient spectroscopy characterization of defects near SiO2/SiC interfaces", A. F. Basile, J. Rozen, J. R. Williams, L. C. Feldman, and P. M. Mooney, J. Appl. Phys, 109, 064514 (2011).

6. 

"Electron trapping in 4H-SiC MOS capacitors fabricated by pre-oxidation nitrogen implantation", A.F. Basile, S. Dhar, and P.M. Mooney, J. Appl. Phys. 109, 114505 (2011).

 

Defects in Compound Semiconductors
Defect Energy Levels in Dilute GaAsBi Alloys

The alloying of GaAs with small amounts of N or Bi produces large changes in the bandgap, making these materials of interest for optoelectronic applications including quantum well lasers, heterojunction bipolar transisters, and multi quantum well solar cells. Although N and Bi are isolelectronic with As, these atoms behave more like impurities than conventional alloying elements. The bandgap reduction in the dilute nitride alloy is due to a resonant interaction of a nitrogen state with the bottom of the conduction band. Similarly the bandgap reduction in the Bi alloy is believed to be due to a resonant interaction with the top of the valence band. Deep level transient spectroscopy (DLTS) measurements are employed to investigate bandgap electronic states in GaAsBi alloys. Such states, which originate from semiconductor defects, are of concern because GaAsBi alloys are grown at temperatures below 400˚C. DLTS measuremernts of p-i-n diodes having a thin (<50nm) GaAsBi layer in the center of the 100nm-thick i-layer, which was grown at temperatures close to 300˚C, reveal defects in signficant concentrations located in these i-layers. These defect studies complement measurements of the optical and transport properties of these alloys, which are grown by molecular beam epitaxy in Prof. Tom Tiedje's lab at UVic. More recently p+/n junction diodes were investigated and electron traps previously identified as As anti-site defect complexes were found in GaAs and GaAsBi layers at 300˚C.

 

1. 

“Deep level defects in dilute GaAsBi alloys grown under intense UV illumination”,  P.M. Mooney, Marianne Tarun, D.A. Beaton, A. Mascarenhas, and K. Alberi, Semicond. Sci. and Technol. 31, 085014 (2016).

2. 

“Defect energy levels in p-type GaAsBi and GaAs grown by MBE at low temperatures”, P.M. Mooney, M.C. Tarun, V. Bahrami-Yekta, T. Tiedje, R.B. Lewis and M. Masnadi-Shirazi, Semicond. Sci. Technol. 31, 065007 (2016).

3. 

"Deep level defects in n-type GaAsBi and GaAs grown at low temperatures”, P.M. Mooney, K.P. Watkins, Zenan Jiang, A.F. Basile, R.B. Lewis, V. Bahrami-Yekta, M. Masnadi-Shirazi, D.A. Beaton and T. Tiedje, J. Appl. Phys. 113, 133707 (2013).

4. 

“Deep Level Defects in GaAs1-xBix/GaAs Heterostructures", Zenan Jiang, D.A. Beaton, R.B. Lewis, A. Basile, T.Tiedje and P.M. Mooney, Semicond. Sci and Technol, 26, 055020 (2011).

Elastically Strain-Relaxed Nano-Membranes

The performance of semiconductor devices for applications in computing and telecommunications is limited by the lattice constant mismatch of the single crystal semiconductor films with which they are fabricated. To expand the range of materials that can be employed, engineered or "virtual" substrates having lattice constants that are difference from the available bulk semiconductor substrates have been fabricated by bonding elastically strain relaxed nano-membranes to standard bulk semiconductor substrates.

Solution-Bonding of InGaAs/GaAs Nano-Membranes to GaAs Substrates

A long-term goal of this project is to fabricate engineered substrates for III-V semiconductor devices that have a surface lattice constant which is different from that of the bulk substrate material such as GaAs, InP or GaSb. As a first step toward this goal, elastically strain-relaxed (defect-free) In0.08Ga0.92As/GaAs heterostructures on GaAs(001) substrates were fabricated. Pseudomorphic heterostructures grown by MOCVD were patterned using conventional photolithography and a sacrificial AlAs layer was removed by selective etching [1-3]. As etching proceeds and the GaAs/InGaAs/GaAs structure is released from the substrate, elastic strain relaxation occurs and the strain-relaxed structures are weakly bonded in-place to the substrate. The bond between the strain-relaxed structure and the substrate was then strengthened by annealing under conditions similar to those used for whole wafer bonding of GaAs. The strain, composition and thickness of the layers were determined using high resolution X-Ray diffraction and the sample surface quality was examined using atomic force microscopy. The degree of strain relaxation of the InGaAs layer is determined by the relative thickness of the GaAs and InGaAs layers in agreement with a force balance model. The in-plane lattice constant of the bonded GaAs/In0.08Ga0.92As/GaAs structures is 0.25-0.44% larger than the lattice constant of the GaAs substrate.

1. 

“Electrical Characterization of In-Place Bonded Interfaces”, O. Salehzadeh, B. Cawston-Grant, S.P. Watkins, and P.M. Mooney, Semicond. Sci. Technol. 29, 085002 (2014).

2.

“Characterization of solution-bonded GaAs/InGaAs/GaAs features on GaAs”, P.M. Mooney, K.L. Kavanagh, D. Owen, D. Lackner, B. Cawston-Grant, A.F. Basile, O. Salehzadeh, and S.P. Watkins, Semicond. Sci, Technol. 29, 075009 (2014).

3.

“In-place bonding of GaAs/InGaAs/GaAs heterostructures to GaAs(001)”, D.L. Owen, D. Lackner, O.J. Pitts, S.P. Watkins and P.M. Mooney, Semicond. Sci and Technol. 24, 035011 (2009).