For an up-to-date publications list, please visit my Google Scholar Profile [https://scholar.google.com/citations?hl=en&user=CClEdEEAAAAJ], or download my CV above.
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Embedded Files
BOOK
BOOK
"Integrated Electronics on Aluminum Nitride : Materials and Devices"
Springer Nature Publications, 2022
"Integrated Electronics on Aluminum Nitride : Materials and Devices"
Springer Nature Publications, 2022
SELECTED PUBLICATIONS
SELECTED PUBLICATIONS
P1. A polarization-induced 2D hole gas in undoped gallium nitride quantum wells
P1. A polarization-induced 2D hole gas in undoped gallium nitride quantum wells
Science (2019) [Direct download link]
R. Chaudhuri, S. Bader, Z. Chen, D. Muller, H. Xing, D. Jena
Featured in Cornell Chronicle, Semiconductor Today, EurekaAlert!, ScienceDaily, Phys.org
(Editor's Feature) A Hole Flatland :
When two distinct materials are placed on top of each other, the difference in polarization between the two layers can induce charge carriers at the interface. Many such two-dimensional (2D) electron gases have been observed, but engineering a 2D hole gas without the help of doping has been much trickier. Chaudhuri et al. used molecular beam epitaxy to grow a layer of gallium nitride on top of aluminum nitride without introducing dopants. This approach resulted in a high-density 2D hole gas at the interface in this technologically relevant system.
P2. Very High Density (>10^14 cm−2 ) Polarization-Induced 2D Hole Gases Observed in Undoped Pseudomorphic InGaN/ AlN Heterostructures
P2. Very High Density (>10^14 cm−2 ) Polarization-Induced 2D Hole Gases Observed in Undoped Pseudomorphic InGaN/ AlN Heterostructures
Advanced Electronics Materials (2022)
R. Chaudhuri, Z. Zhang, H. Xing, D. Jena
Building on the recently discovered undoped, polarization-induced GaN/AlN 2D hole gas (2DHG), this work demonstrates the tuning of the piezoelectric polarization difference across the heterointerface by introducing indium in the GaN channel. Using careful design and epitaxial growths, these pseudomorphic (In)GaN/AlN heterostructures result in some of the highest carrier densities of >10^14 cm−2 in a III-nitride heterostructure—just an order below the intrinsic crystal limit of ~10^15 cm−2 . A characteristic alloy fluctuation energy of 1.0 eV for hole scattering in InGaN alloy is proposed based on the experiments.
P3. in-situ crystalline AlN Passivation for Reduced RF Dispersion in strained-channel AlN/GaN/AlN HEMTs
P3. in-situ crystalline AlN Passivation for Reduced RF Dispersion in strained-channel AlN/GaN/AlN HEMTs
physica status solidi (a) (2021)
R. Chaudhuri, A. Hickman, J. Singhal, J. Casamento, H. Xing, D. Jena
Herein, a novel in-situ passivation technique for III-nitride high electron mobility transistors (HEMTs) is demonstrated using a crystalline AlN layer to move the surface states away from the 2D electron gas (2DEG) channel. In-situ passivated AlN/GaN/AlN HEMTs show drastic reduction in DC-RF dispersion of ∼ 2 − 6% compared to ∼ 20% in current state-of-art ex-situ silicon nitride (SiN) passivated AlN HEMTs.
P4. High conductivity Polarization-induced 2D hole gases in Undoped GaN/AlN Heterojunctions enabled by Impurity Blocking Layers
P4. High conductivity Polarization-induced 2D hole gases in Undoped GaN/AlN Heterojunctions enabled by Impurity Blocking Layers
Journal of Applied Physics (2021)
Reet Chaudhuri, Zhen Chen, David A. Muller, Huili Grace Xing, Debdeep Jena
High-conductivity undoped GaN/AlN 2D hole gases (2DHGs), the p-type dual of the AlGaN/GaN 2D electron gases (2DEGs), have offered valuable insights into hole transport in GaN and enabled the first GaN GHz RF p-channel FETs. They are an important step towards high-speed and high-power complementary electronics with wide-bandgap semiconductors. These technologically and scientifically relevant 2D hole gases are perceived to be not as robust as the 2DEGs because structurally similar heterostructures exhibit wide variations of the hole density over ∆ps > 7e13 cm−2 , and low mobilities. In this work, we uncover that the variations are tied to undesired dopant impurities such as Silicon and Oxygen floating up from the nucleation interface. By introducing impurity blocking layers (IBLs) in the AlN buffer layer, we eliminate the variability in 2D hole gas densities and transport properties, resulting in a much tighter-control over the 2DHG density variations to ∆ps ≤ 1 e13 cm−2 across growths, and a 3× boost in the Hall mobilities. These changes result in a 2-3× increase in hole conductivity when compared to GaN/AlN structures without IBLs.
P5. GaN/AlN p-channel HFETs with Imax >420 mA/mm and ~20 GHz f_T / f_MAX
P5. GaN/AlN p-channel HFETs with Imax >420 mA/mm and ~20 GHz f_T / f_MAX
IEEE International Electron Devices Meeting (IEDM) (2020)
K. Nomoto, R. Chaudhuri, S. Bader, L. Li, A. Hickman, S. Huang, H Lee, HW Then, A Molnar, HG Xing, and D Jena.
Featured in EE World Online, Industrial News
The first p-channel nitride transistors that break the GHz speed barrier are demonstrated. By leveraging the unique single-channel high-density polarization-induced 2D hole gas of the GaN/AlN heterostructure, best-in-class contact resistances, and scaled T-gate design, p-channel transistor on-currents of 428 mA/mm are observed, with cutoff frequencies in the 20 GHz regime. These observations demonstrate the unique enabling role of the polarization discontinuity at the GaN/AlN semiconductor heterojunction and offer significant hope for a new high-speed and high-voltage wide-bandgap CMOS device platform for applications in RF and power electronics domains.
P6. Electric Fields and Surface Fermi Level in Undoped GaN/AlN Two-Dimensional Hole Gas Heterostructures
P6. Electric Fields and Surface Fermi Level in Undoped GaN/AlN Two-Dimensional Hole Gas Heterostructures
physica status solidi rrl (2021)
Łukasz Janicki*, Reet Chaudhuri*, Samuel James Bader, Huili Grace Xing, Debdeep Jena, Robert Kudrawiec
*co-first author
III-nitride heterostructures have a high built-in electric field due to the intrinsic polarization. Contactless electro-reflectance (CER) spectroscopy is used to porbe and measure the built-in electric field in GaN/AlN 2DHG heterostructures. Comparing to electrostatic simulations, a surface barrier height of ≈1.9 eV for holes is proposed in these technologically relevant heterostructures.
P7. Molecular Beam Epitaxy Growth of Large-Area GaN/AlN 2D Hole Gas Heterostructures
P7. Molecular Beam Epitaxy Growth of Large-Area GaN/AlN 2D Hole Gas Heterostructures
physica status solidi (b) (2020)
Reet Chaudhuri, S. Bader, Z. Chen, D. Muller, H. Xing , D. Jena
A study of the growth conditions during molecular beam epitaxy (MBE) growth of metal‐polar GaN/AlN heterostructures is presented for optimal transport of the polarization‐induced 2D hole gases (2DHGs), along with the demonstration of large‐area growths of the 2DHGs on 2 in. wafers using optimized growth conditions.
Other Selected Publications
Other Selected Publications
P8. Prospects for wide bandgap and ultrawide bandgap CMOS devices.
P8. Prospects for wide bandgap and ultrawide bandgap CMOS devices.
IEEE Transactions on Electron Devices (2020)
Samuel James Bader, Hyunjea Lee, Reet Chaudhuri, Shimin Huang, Austin Hickman, Alyosha Molnar, Huili Grace Xing, Debdeep Jena, Han Wui Then, Nadim Chowdhury, et al.
P9. First RF Power Operation of AlN/GaN/AlN HEMTs with >3 A/mm and 3 W/mm at 10 GHz.
P9. First RF Power Operation of AlN/GaN/AlN HEMTs with >3 A/mm and 3 W/mm at 10 GHz.
IEEE Journal of the Electron Devices Society (2021)
Austin Hickman, Reet Chaudhuri, Kazuki Nomoto, Lei Li, James CM Hwang, Huili Grace Xing, and Debdeep Jena.
P10. Large Signal Response of AlN/GaN/AlN HEMTs at 30 GHz.
P10. Large Signal Response of AlN/GaN/AlN HEMTs at 30 GHz.
Device Research Conference (DRC) (2021)
Austin Hickman, Reet Chaudhuri, Neil Moser, Micheal Elliot, Kazuki Nomoto, Lei Li, James CM Hwang, Huili Grace Xing, and Debdeep Jena.
P11. Polarization induced 2D hole gases in pseudomorphic undoped GaN/AlN heterostructures on single-crystal AlN substrates.
P11. Polarization induced 2D hole gases in pseudomorphic undoped GaN/AlN heterostructures on single-crystal AlN substrates.
Applied Physics Letters (2021)
Zexuan Zhang, Jimy Encomendero, Reet Chaudhuri, Yongjin Cho, Vladamir Protasenko, Kazuki Nomoto, Kevin Lee, Masato Toita, Huili Grace Xing, and Debdeep Jena.
P12. Quantitative scanning microwave microscopy of 2D electron and hole gases in AlN/GaN heterostructures.
P12. Quantitative scanning microwave microscopy of 2D electron and hole gases in AlN/GaN heterostructures.
Applied Physics Letters (2022)
Xiaopeng Wang, Gianluca Fabi, Reet Chaudhuri, Austin Hickman, Mohammad Javad Asadi, Kazuki Nomoto, Huili Grace Xing, Debdeep Jena, Marco Farina, and James C. M. Hwang
P13. Next generation electronics on the ultrawide-bandgap aluminum nitride platform
P13. Next generation electronics on the ultrawide-bandgap aluminum nitride platform
Semicond. Sci. Technol. 36 (2021)
Austin Lee Hickman, Reet Chaudhuri, Samuel James Bader, Kazuki Nomoto, Lei Li, James Hwang, Huili Grace Xing, and Debdeep Jena.
P14. GaN/AlN Schottky-gate p-channel HFETs with InGaN contacts and 100 mA/mm on-current
P14. GaN/AlN Schottky-gate p-channel HFETs with InGaN contacts and 100 mA/mm on-current
IEEE International Electron Devices Meeting ( IEDM ) (2019)
S. Bader, Reet Chaudhuri, A. Hickman, K. Nomoto, S. Bharadwaj , H.W. Then, H. Xin g , D. Jena
P15. Molecular beam epitaxial growth of scandium nitride on hexagonal SiC, GaN, and AlN
P15. Molecular beam epitaxial growth of scandium nitride on hexagonal SiC, GaN, and AlN
Applied Physics Letters (2019)
J Casamento, J. Wright, Reet Chaudhuri, H. Xing , D. Jena
P16. Wurtzite phonons and the mobility of a GaN/AlN 2D hole gas
P16. Wurtzite phonons and the mobility of a GaN/AlN 2D hole gas
Appl. Phys. Lett. 114, 253501 (2019)
S.J. Bader, R. Chaudhuri, M. Schubert, H. Then, H. Xing, D. Jena
P17. High Breakdown Voltage in RF AlN/GaN/AlN Quantum Well HEMTs
P17. High Breakdown Voltage in RF AlN/GaN/AlN Quantum Well HEMTs
IEEE Electron Device Letters (2018)
A. Hickman, R. Chaudhuri, S.J. Bade, K. Nomoto, K. Lee, H. Xing, D. Jena
P18. GaN-based multi-channel transistors with lateral gate for linear and efficient millimeter-wave power amplifiers
P18. GaN-based multi-channel transistors with lateral gate for linear and efficient millimeter-wave power amplifiers
IEEE MTT-S International Microwave S y m p osium ( IMS ), (2019)
K. Shinohara, C. King , E. Regan, J. Bergman, A. Carter, A. Arias, M. Urteaga, B. Brar, R. Page, Reet Chaudhuri, SM Islam, H. Xing , D. Jena
P19. Gate-recessed E-mode p-channel HFET with high on-current based on GaN/AlN 2D hole gas
P19. Gate-recessed E-mode p-channel HFET with high on-current based on GaN/AlN 2D hole gas
IEEE Electron Device Letters, vol. 39, no. 12 (2018)
S.J. Bader, R. Chaudhuri, K. Nomoto, A. Hickman, H. Then, Z. Chen, D. Muller, H. Xing, D. Jena
P20. Terahertz spectroscopy of an electron-hole bilayer system in AlN/GaN/AlN
P20. Terahertz spectroscopy of an electron-hole bilayer system in AlN/GaN/AlN
Appl. Phys. Lett. 111, 073102 (2017)
H. Condori Quispe, S. M. Islam, S.J. Bader, A. Chanana, K. Lee, R. Chaudhuri, A. Nahata, H. Xing, D. Jena and B. Sensale-Rodriguez
INVENTIONS AND PATENTS
INVENTIONS AND PATENTS
PT1. RF High-Electron-Mobility Transistors including Group III-N Stress Neutral Barrier Layers with High Breakdown Voltages
PT1. RF High-Electron-Mobility Transistors including Group III-N Stress Neutral Barrier Layers with High Breakdown Voltages
US Patent 11710785B2, Granted Jul 2023.
PT2. High-voltage p-channel FET based on III-Nitride Heterostructures
PT2. High-voltage p-channel FET based on III-Nitride Heterostructures
US Patent 11522080B2, Granted Dec 2022
PT3. Polarization-induced 2D Hole Gases for High-voltage p-channel Transistors
PT3. Polarization-induced 2D Hole Gases for High-voltage p-channel Transistors
US Patent US11158709B2, Granted Oct 2021.
PT4. Integrated electronics on the aluminum nitride platform
PT4. Integrated electronics on the aluminum nitride platform
US Patent Application No.: US2022/0199782, Filed 2021
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