Rajendra Singh’s research while affiliated with Indian Institute of Technology Delhi and other places

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Publications (113)


Figure 1: Molecular Beam epitaxy Growth of1T ′ -WTe2. (a) Schematic of the pre-growth tellurisation of the substrate and consequent growth of 1T ′ -WTe2 while opening both cracker cell of Tellurine and Tungsten (b) Typical in-situ reflection high-energy electron diffraction (RHEED) image of grown flim. (c) Optical image of large-scale growth of 1T ′ -WTe2 (d) Raman spectroscopy of grown film. (e-g) EDX mapping of tungsten, tellurium, and their combination at Position-5, as marked in figure 1c. (h) UV vis of MBE grown 1T ′ -WTe2. (i) Voltage vs current plot of MBE grown 1T ′ -WTe2 using four-probe method.
Figure 2: Dry etching of MBE grown WTe 2 flim: Optical image of (a) MBE grown WTe 2 on substrate.(b) Photoresist (PR) coated hard mask on the WTe 2 flim (c) Etched WTe 2 flim and correspond WTe 2 pad on substrate (d) etched large area of WTe 2 flim. (e) AFM image of etched WTe 2 film.
Figure 3: Dry transfer of InSe on etched WTe 2 pad : Schematic of (a) MBE grown WTe 2 flim of substrate (b) Formation of WTe 2 contact pad after RIE (c) PDMS stamp preparation on transparent glass slide (d) Transfer of InSe from nitto tape to PDMS. (e) Dry stamping of InSe on etched WTe 2 in our 2D material transfer setup. (f) Final transfer of Inse at desired etched position. (g) Real optical image of Inse on etched WTe 2 pad.
Figure 4: XPS of InSe/1T ′ -WTe 2 : XPS analysis indicates that 1T ′ -WTe 2 and InSe have a stoichiometric composition. (a) High resolution spectrum of 1T ′ -WTe 2 for (a) W 4f core orbitals (b) Te 3d core orbitals. (c) High resolution spectrum of InSe for (a) Se 3d core orbitals (b) In 3d core orbitals.
Figure 6: Band diagram of 1T ′ -WTe2/InSe and InSe/Ti-Au based device by KPFM : Surface potential picture and CPD picture of (a) HOPG (b) 1T ′ -WTe2 in 1T ′ -WTe2/InSe device (c) InSe in 1T ′ -WTe2/InSe device. (d) valance band spectra of InSe in 1T ′ -WTe2/InSe device from XPS (e) Band diagram of 1T ′ -WTe2/InSe device before connection (f) Band diagram of 1T ′ -WTe2/InSe device after connection. Energy band diagram of (e) InSe/ 1T ′ -WTe 2 device and (f) InSe/Ti-Au device before connection respectively. Energy band diagram of (g) 1T ′ -WTe2/InSe device and (h) InSe/Ti-Au device under equllibrium respectively.

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Engineering 2D Van der Waals Electrode via MBE Grown Weyl Semimetal 1T-WTe2 for Enhanced Photodetection in InSe
  • Preprint
  • File available

February 2025

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58 Reads

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Taslim Khan

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Achieving low contact resistance in advanced electronic devices remains a significant challenge. As the demand for faster and more energy-efficient devices grows, 2D contact engineering emerges as a promising solution for next-generation electronics. Beyond graphene, 1T-WTe2 has gained attention due to its outstanding electrical transport properties, quantum phenomena, and Weyl semimetallic characteristics. We demonstrate the direct wafer-scale growth of 1T-WTe2 via molecular beam epitaxy (MBE) and use it as a 2D contact for layered materials like InSe, which exhibits broad photoresponsivity. The performance of this 2D electrode in InSe-based photodetectors is compared with conventional metal electrodes. Under near-infrared (NIR) to deep ultraviolet (DUV) illumination, the InSe/1T-WTe2 configuration shows a broad photoresponsivity range from 0.14 to 217.58 A/W, with fast rise/fall times of 42/126 ms in the visible region. In contrast, the InSe/Ti-Au configuration exhibits a peak photoresponsivity of 3.64 A/W in the DUV range, with an overall lower responsivity spanning from 0.000865 A/W to 3.64 A/W under NIR and DUV illumination, respectively. Additionally, in the visible regime, it exhibits slower rise and fall times of 150 ms and 144 ms, respectively, compared to InSe/1T-WTe2. These findings indicate that MBE-grown 1T-WTe2 serves as an effective 2D electrode, delivering higher photoresponsivity and faster photodetection compared to traditional metal contacts. This approach offers a simplified, high-performance alternative for layered material-based devices, eliminating the need for complex heterostructure configurations.

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Controlling the Mott–Peierls transition in epitaxial VO2 (M1) film grown by PLD for near-IR photodetection

February 2025

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14 Reads

Vanadium dioxide (VO2) (M1) exhibits a unique metal–insulator transition (MIT) near room temperature, garnering considerable attention for its applications in bolometer, terahertz/infrared detectors, and microelectronic devices. Here, we explore the potential of epitaxially grown VO2 (M1) thin films for near-infrared (IR) detection by optimizing the growth conditions, followed by structural characterization and device fabrication. Alongside the VO2 (M1) phase, two other oxides from the vanadium oxide family, VO2 (A) and V2O5, were also grown on a c-cut sapphire substrate using a pulsed laser deposition (PLD) system. In-depth analysis using temperature-dependent XRD and Raman spectroscopy confirmed the crystalline structure and the quality of epitaxial thin film formation of VO2 (M1), while also unveiling structural phase transition (SPT) behavior and the critical temperature of transition. At elevated temperatures during electrical measurement, the VO2 (M1) epilayer exhibits a first-order phase transition from the metallic to the insulating state, accompanied by a significant change in resistance exceeding three orders of magnitude unveiling its potential in thermal switches, memory-based devices etc. In depth, electrical analysis on all the grown oxides shows that VO2 (M1) and V2O5 exhibit a higher temperature coefficient of resistance (TCR) (3%/K and 2%/K) and a lower 1/f noise (in the order pA / Hz at 0.1 Hz) as compared to VO2 (A), paving scope for further analysis of these two oxides toward important applications in the domain of thermal sensors. Additionally, VO2 (M1) exhibited good bolometric response (in the order of ms) to IR radiation, proving its candidature for the application in IR detectors as well.



Optically Pumped Ultrafast and Broadband Terahertz Modulation with Scalable Molecular Beam Epitaxy Grown MoTe2/Si Heterostructures

Despite advancements in terahertz (THz) modulators, achieving a balance between large modulation depth (MD) and fast modulation speed in scalable devices remains a significant challenge. Optically pumped THz modulators with high MD, broad bandwidth, and fast response times are essential for progress in THz technology. Here, scalable MoTe2/Si van der Waals (vdW) heterostructures are grown via molecular beam epitaxy (MBE) as an optically pumped THz modulators, leveraging its favorable band alignment and seamless integration with silicon complementary metal‐oxide semiconductor (CMOS) technology. High‐quality bilayer, 5‐layer, and 7‐layer MoTe2 films are grown on high‐resistivity silicon, with the bilayer modulator achieving a maximum 74.6% modulation depth under 355 nm illumination of 4.8 W mm⁻² at 0.25 THz. The bilayer device exhibited fast rise and fall times of 1.8 and 0.6 µs, respectively, and provided broadband modulation across the 0.1 to 1.0 THz range. Furthermore, this work demonstrates that higher modulation depth significantly enhances THz imaging quality with promising applications in detecting pharmaceutical forgeries. Overall, these ultrafast, broadband THz modulators provide a promising route for advancing next‐generation THz technology, enhancing applications in wireless communication, precision detection, and high‐resolution THz imaging, fostering future innovation.


Figure 3. Output DC characteristics of GaN-on-Si power MIS-HEMT (a) ID-VDS curve at 420 K, (b) ID-VDS curve at 300 K, (c) ID-VDS curve at 4 K, (d) extracted ID Sat, (e) extracted RON and (f) ID at VGS-VTH = 5 V with temperature from 420 K to 4 K.
Figure 4. Low-frequency noise characteristics of GaN-on-Si power MIS-HEMT (a) SIDS/IDS 2 -f curve at 420 K, (b) SIDS/IDS 2 -f curve at 300 K, (c) SIDS/IDS 2 -f curve at 4 K, (d) SIDS/IDS 2 -f curve from 420 K to 4 K at VGS -VTH = 2 V, (e) SIDS/IDS 2 -ID curve at 420 K, (f) SIDS/IDS 2 -ID curve at 300 K, (g) SIDS/IDS 2 -ID curve at 4 K, (h) extracted Svfb and (i) extracted Nit as a function of temperature from 420 K to 4 K.
Investigation of DC and Low-Frequency Noise performance in GaN-on-Si Power MIS-HEMTs Over a Temperature Range of 4 K to 420 K

January 2025

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22 Reads

IEEE Journal of the Electron Devices Society

This study investigates the electrical DC and Low-frequency noise (LFN) characteristics of GaN-on-Si power MIS-HEMTs across an extensive temperature spectrum from 4 K to 420 K to assess their viability for high to cryogenic temperatures. As the temperature drops, improvements are observed in the input DC characteristics, including enhanced transconductance and an increased ON-to-OFF current ratio. Correspondingly, the output DC characteristics affirmed the significant enhancements in drain current and reduced ON-resistance across the same temperature span. These improvements in DC performance are achieved without any evidence of carrier-freeze out throughout the temperature expanse. Furthermore, the LFN characteristics from 10 Hz to 100 KHz reveal a consistent 1/f noise behavior within the measured temperature domain. The trap density inferred from the LFN characteristics increases substantially by two orders of magnitude at deep cryogenic temperatures. Collectively, these experimental outcomes demonstrate that GaN-on-Si power MIS-HEMTs maintain a robust electrical performance over a wide temperature range, providing valuable insights for enhancing their deployment in quantum computing and space-based applications.



Investigation of traps in halide vapor-phase epitaxy-grown β-Ga2O3 epilayers/n-Ga2O3 using deep-level transient spectroscopy

November 2024

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66 Reads

A detailed investigation of deep traps in halide vapor-phase epitaxy (HVPE)-grown β-Ga2O3 epilayers has been done by performing deep-level transient spectroscopy (DLTS) from 200 K to 500 K on Pt/β-Ga2O3 and Ni/β-Ga2O3 Schottky diodes. Similar results were obtained with a fill pulse width of 100 ms irrespective of the different Schottky metal contacts and epilayers. Two electron traps at E2 (EC–ET = 0.65 eV) and E3 (EC–ET = 0.68–0.70 eV) with effective capture cross-sections of 4.10 × 10⁻¹⁴ cm² and 5.75 × 10⁻¹⁵ cm² above 300 K were observed. Below 300 K, a deep trap with a negative DLTS signal peak was also observed at E1 (EC–ET = 0.34–0.35 eV) with a very low capture cross-section of 3.28 × 10⁻¹⁷ cm². For a short pulse width of 100 μs, only two electron traps, E2 and E3, at energies of 0.72 eV and 0.73 eV were observed, and one order of higher corresponding effective capture cross-sections. All traps were found to be unaffected by the electric field during the field-dependent DLTS study. From the filling pulse width dependence DLTS study, a decrease in the capacitance transient amplitude with the increasing pulse width was observed opposite to the capture barrier kinetics of the traps and attributed to the emission of carriers during the capture process. Trap concentrations were found to be high at the interface using depth profiling DLTS. Based on the available literature, it is suggested that these traps are related to FeGa, Fe-related centers, and complexes with hydrogen or shallow donors, and might be affected or generated during metallization by the electron beam evaporator and chemical mechanical polishing.





Citations (67)


... FNC is widely used in energy storage devices, such as high-performance capacitors, where their high dielectric constant and low energy loss enable efficient energy storage and rapid charge-discharge cycles [1,2]. Additionally, their piezoelectric properties make them ideal for sensors and actuators, commonly found in microelectromechanical systems (MEMS) for pressure measuring [3], selfpowered systems [4], motion detection [5] with high sensitivity and precision. FNC also finds applications in non-volatile memory devices like FeRAM [6], ferroelectrics cathodes [7], and thermistors [8]. ...

Reference:

Influence of pristine and oxidized MWCNT fillers on ferroelectricity and dielectric dispersion of a classical ferroelectric of Rochelle salt
PVDF/N-rGO nanofibers based sustainable triboelectric nanogenerator for self-powered wireless motion sensor
  • Citing Article
  • December 2024

Carbon

... Based on the model proposed by Maire and Mering, the degree of graphitization can be calculated from the following equation: [22,23] ...

Design considerations for sodium dual ion batteries: Insights into electrolyte, anode, and cathode materials
  • Citing Article
  • November 2024

Journal of Energy Storage

... For example, band gaps of semiconducting TMD/TMDCs can be tuned by controlling layer numbers, growth processes, chemical compositions, strains of the materials, etc 9 . On semiconductor TMDCs, significant efforts are being provided towards synthesis, structure, and defect characterization 10 . Among various semiconducting TMDCs, MoS2 is the one that attracted the most attention first. ...

Optical Properties of Nanoscale-Thick 2H and 1T′ MoTe 2 Films via Spectroscopic Ellipsometry: Implications for Optoelectronic Devices
  • Citing Article
  • October 2024

ACS Applied Nano Materials

... 6 Recent advancements in broadband PDs have leveraged various materials, such as 2D materials, 7,8 perovskites, 9 and organic semiconductors. 10 Several solar-blind PDs, such as p-i-n, 11 p-n, 12 and bidirectional devices based on nanowires, have been made possible by wide-band-gap semiconductor materials. 13 Because of their exceptional optoelectronic characteristics, detectors based on GaN and AlGaN 14 have made great strides in this regard. ...

Unveiling Superior Solar-Blind Photodetection with a NiO/ZnGa 2 O 4 Heterojunction Diode
  • Citing Article
  • October 2024

ACS Applied Materials & Interfaces

... Transition metal dichalcogenides (TMDCs) are a large family of materials with tunable electronic and topological properties [6][7][8] . For example, band gaps of semiconducting TMD/TMDCs can be tuned by controlling layer numbers, growth processes, chemical compositions, strains of the materials, etc 9 . On semiconductor TMDCs, significant efforts are being provided towards synthesis, structure, and defect characterization 10 . ...

Film thickness-induced optical and electrical modifications in large-area few-layer 2H-MoSe2 grown by MBE
  • Citing Article
  • September 2024

Nanoscale

... In the past few years, 2D materials such as graphene, TMDs, and TMDCs snatched a new stream in the nano/quantum electronics field due to multiple easily tunable properties, e.g., mechanical, optical, and electrical [1][2][3][4][5] . Transition metal dichalcogenides (TMDCs) are a large family of materials with tunable electronic and topological properties [6][7][8] . ...

High-Performance Visible-to-SWIR Photodetector Based on the Layered WS 2 Heterojunction with Light-Trapping Pyramidal Black Germanium
  • Citing Article
  • August 2024

ACS Applied Materials & Interfaces

... Because mesa device designs incorporate the advantages of tiny pixel dimensions, large pixel densities, minimal cross-talk, and complicated heterostructures, they are now the preferred design for producing contemporary FPAs [149]. Moreover, MBE has demonstrated significant progress in the production of avalanche photodiodes (APDs), such as InGaAs/ AlGaAsSb Geiger mode APDs [150], ZnTe-based photodiodes [151], UV photodiode [152], and others [153][154][155]. ...

MBE-grown ZnTe epitaxial layer based broadband photodetector with high response and excellent switching characteristics

... 3 This capability is essential for diverse applications, including optical image sensing, 4 optical communications, 5 and environmental monitoring. 6 Recent advancements in broadband PDs have leveraged various materials, such as 2D materials, 7,8 perovskites, 9 and organic semiconductors. 10 Several solar-blind PDs, such as p-i-n, 11 p-n, 12 and bidirectional devices based on nanowires, have been made possible by wide-band-gap semiconductor materials. ...

Quasi-dry layer transfer of few-layer MBE-grown MoTe2 sheets for optoelectronic applications

Sensors and Actuators A Physical

... The CdTe buffer layer is used to reduce the large lattice mismatch (∼14.3%) between HgCdTe and alternate substrates. The thin interfacial ZnTe layer reduces the lattice mismatch between the CdTe buffer layer and Si, Ge, GaSb, InAs and GaAs-based alternate substrates, thus preserving the growth orientation of the CdTe layer [11][12][13][14][15]. Generally, GaSb and InAs have low bandgaps, which restricts infrared transmission in back-illuminated devices. ...

Annealing of MBE-grown CdTe epitaxial layer at various tellurium overpressure for reduced defect density

Journal of Materials Science: Materials in Electronics

... The GaN power MIS-HEMT utilized for the current study is grown epitaxially on a 6-inch GaN-on-Silicon (Si) substrate via Metal-Organic Chemical Vapor Deposition (MOCVD). The comprehensive details of the AlGaN/GaN epitaxial structure, including the insulator and passivation layer, are documented in a previous publication by our group [22]. A 30 nm silicon nitride (SiN) insulating layer was deposited on top of the AlGaN barrier layer using the Low-Pressure Chemical Vapor Deposition (LPCVD) technique at a temperature of 780 o C. The ohmic contact metal stack of Ti/Al/Ti/Au is deposited for the source and drain contacts, while the gate contact incorporates a Ni/Au Schottky contact metal stack, both metal stacks are deposited using an e-beam evaporation system. ...

Investigation of DC Characteristics in GaN-on-Si power MIS-HEMTs over a Wide Temperature Range (4 K to 550 K) for Space and Quantum Computing Applications
  • Citing Conference Paper
  • March 2024