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Dive into the research topics where Brajesh S. Yadav is active.

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Featured researches published by Brajesh S. Yadav.


Journal of Applied Physics | 2007

Growth and structure of sputtered gallium nitride films

Brajesh S. Yadav; S.S. Major; R.S. Srinivasa

GaN films have been deposited by radio frequency sputtering of a GaAs target with pure nitrogen. The growth, composition, and structure of the films deposited on quartz substrates have been studied by x-ray diffraction, transmission electron microscopy, and Raman spectroscopy. Films deposited below 300°C are amorphous and As rich. Above 300°C, polycrystalline, hexagonal GaN is formed, along with As rich amorphous phase, which reduces with increasing substrate temperature. At a substrate temperature of 700°C, GaN films, practically free of amorphous phase, and As (<0.5at.%) are formed. The preferred orientation depends strongly on the substrate temperature and is controlled by surface diffusion of adatoms during growth stage. Below 500°C, the surface diffusion between planes dominates and results in the (101¯1) preferred orientation. Above 500°C, the surface diffusion between grains takes over and results in (0002) preferred orientation.


Applied Physics Letters | 2006

Hexagonal diamond synthesis on h-GaN strained films

Abha Misra; Pawan K. Tyagi; Brajesh S. Yadav; Padmnabh Rai; D. S. Misra; V. Pancholi; I. Samajdar

Chemical vapor deposited diamond films grown on strained gallium nitride-coated quartz substrate are found to display a dominantly hexagonal diamond phase. The phase identification is done using Raman spectroscopy and orientation imaging microscopy (OIM). The presence of a 1324.4cm−1 band in the Raman spectra is attributed to a hexagonal diamond symmetry, but the unambiguous signature of the hexagonal phase is confirmed by OIM. A phase map of the sample clearly shows that 88% of the scanned sample area is hexagonal diamond.


RSC Advances | 2015

Structural, optical and electronic properties of homoepitaxial GaN nanowalls grown on GaN template by laser molecular beam epitaxy

S. S. Kushvaha; M. Senthil Kumar; A. K. Shukla; Brajesh S. Yadav; Dilip K. Singh; Mukesh Jewariya; Srinivasa Ragam; K. K. Maurya

We have grown homoepitaxial GaN nanowall networks on GaN template using an ultra-high vacuum laser assisted molecular beam epitaxy system by ablating solid GaN target under a constant r.f. nitrogen plasma ambient. The effect of laser repetition rate in the range of 10 to 30 Hz on the structural properties of the GaN nanostructures has been studied using high resolution X-ray diffraction, field emission scanning electron microscopy and Raman spectroscopy. The variation of the laser repetition rate affected the tip width and pore size of the nanowall networks. The z-profile Raman spectroscopy measurements revealed the GaN nanowall network retained the same strain present in the GaN template. The optical properties of these GaN nanowall networks have been studied using photoluminescence and ultrafast spectroscopy and an enhancement of optical band gap has been observed for the nanowalls having a tip width of 10–15 nm due to the quantum carrier confinement effect at the wall edges. The electronic structure of the GaN nanowall networks has been studied using X-ray photoemission spectroscopy and it has been compared to the GaN template. The calculated Ga/N ratio is largest (∼2) for the GaN nanowall network grown at 30 Hz. Surface band bending decreases for the nanowall network with the lowest tip width. The homoepitaxial growth of porous GaN nanowall networks holds promise for the design of nitride based sensor devices.


CrystEngComm | 2016

Influence of laser repetition rate on the structural and optical properties of GaN layers grown on sapphire (0001) by laser molecular beam epitaxy

S. S. Kushvaha; M. Senthil Kumar; Brajesh S. Yadav; Pawan K. Tyagi; Sunil Ojha; K.K. Maurya; Barjinder Pal Singh

High-quality GaN layers were grown on sapphire (0001) substrates using laser molecular beam epitaxy (LMBE) by laser ablating a solid GaN target at different laser repetition rates (10–40 Hz) under a constant supply of r.f. nitrogen plasma. The effect of laser repetition rate on the structural and optical properties of GaN layers was systematically studied using high-resolution X-ray diffraction (HRXRD), field emission scanning electron microscopy, atomic force microscopy, Raman spectroscopy and photoluminescence (PL) spectroscopy. High-resolution X-ray rocking curve measurements revealed highly c-axis oriented GaN layers on sapphire grown at 30 Hz with a calculated screw dislocation density of ~1.42 × 107 cm−2, whereas the GaN layers grown at 10 or 40 Hz consisted the screw dislocation density in the range of 108–109 cm−2. Surface morphological analysis revealed a change in grain size as well as surface roughness as a function of laser repetition rate and is explained on the basis of growth kinetics. Vibrational Raman spectroscopy revealed that the GaN layer grown at 10 Hz shows an in-plane compressive stress of ~1 GPa, while the film grown at 30 Hz exhibits a minimum stress of ~0.3 GPa. The PL measurements show a highly luminescent band-to-band emission of GaN at 3.44 eV for the 10 Hz grown highly strained GaN layer and at 3.41 eV for the less strained film grown at 30 Hz along with a broad defect band emission centered around 2.28 eV. It is found that the GaN layers grown at 30 Hz have excellent structural and optical properties. We expect that the less strained thin and highly oriented GaN film grown by LMBE can further be utilized for developing prodigious low-temperature-grown nitride-based multilayer structures and devices.


Journal of Applied Physics | 2008

Spectroscopic ellipsometry studies of GaN films deposited by reactive rf sputtering of GaAs target

A. Biswas; D. Bhattacharyya; N. K. Sahoo; Brajesh S. Yadav; S.S. Major; R.S. Srinivasa

GaN films have been deposited by reactive rf sputtering of GaAs target in 100% nitrogen ambient on quartz substrates at different substrate temperatures ranging from room temperature to 700°C. A series of films, from arsenic-rich amorphous to nearly arsenic-free polycrystalline hexagonal GaN, has been obtained. The films have been characterized by phase modulated spectroscopic ellipsometry to obtain the optical parameters, viz., fundamental band gap, refractive index, and extinction coefficient, and to understand their dependence on composition and microstructure. A generalized optical dispersion model has been used to carry out the ellipsometric analysis for amorphous and polycrystalline GaN films and the variation of the optical parameters of the films has been studied as a function of substrate temperature. The refractive index values of polycrystalline films with preferred orientation of crystallites are slightly higher (2.2) compared to those for amorphous and randomly oriented films. The dominantly ...


RSC Advances | 2017

Deposition potential controlled structural and thermoelectric behavior of electrodeposited CoSb3 thin films

Suchitra Yadav; Brajesh S. Yadav; Sujeet Chaudhary; Dinesh K. Pandya

In this study, the deposition potential has been used to exercise control on structural and electrical properties, and associated tuning of thermoelectric properties of CoSb3 thin films prepared by electrochemical synthesis. Deposition potential is observed to have a strong effect on the stoichiometry of films and orientation of crystallites, and consequently on the physical properties. X-ray diffraction patterns reveal that the films grown at lower deposition potentials (≤−0.9 V) have (013) preferred orientation whereas (420) orientation is observed at higher negative deposition potentials. A correlation of the deposition potential controlled composition from a Sb-rich to a Co-rich regime and the resulting tuning of electrical transport parameters and thermoelectric properties of the CoSb3 thin films is established. With enlarged crystallites and enhanced textured structure at a deposition potential of −0.97 V, a significantly large Seebeck coefficient (58 μV K−1) with a simultaneously large electrical conductivity (2.1 × 103 Ω−1 cm−1) are achieved as a result of the high mobility (60 cm2 V−1 s−1). A high value for room temperature power factor (706 ± 9 μW K−2 m−1) observed in the as-grown CoSb3 thin films without any further post-deposition annealing makes their synthesis and thermoelectric studies interesting for their potential applications in power generation and refrigeration.


Journal of Nanoscience and Nanotechnology | 2018

Facile Synthesis of Semiconducting Ultrathin Layer of Molybdenum Disulfide

Sarvottam K Jha; Reetu Kumari; Shubham Choudhary; Puspendu Guha; P. V. Satyam; Brajesh S. Yadav; Zainab Naqvi; S. S. Kushvaha; R. K Ratnesh; M. S Mehata; Aditya Jain; Amrish K. Panwar; Fouran Singh; Pawan K. Tyagi

In this paper, we have reported a simple and efficient method for the synthesis of uniform, highly conducting single or few layer molybdenum disulfide (MoS2) on large scale. Scanning Electron Microscopy (SEM) and High Resolution Transmission Electron Microscopy (HRTEM) have been used for the confirmation of mono or few layered nature of the as-synthesized MoS2 sheets. X-ray Photoelectron Spectroscopy (XPS), X-Ray Diffraction (XRD) and Raman Spectroscopy have also been used to study the elemental, phase, and molecular composition of the sample. Optical properties of as-synthesized sample have been probed by measuring absorption and photoluminescence spectra which also compliment the formation of mono and few layers MoS2 Current-voltage (I-V ) characteristics of as-synthesized sample in the pellet form reveal that MoS2 sheets have an ohmic character and found to be highly conducting. Besides characterizing the as-synthesized sample, we have also proposed the mechanism and factors which play a decisive role in formation of high quality MoS2 sheets.


AIP Advances | 2018

Non-destructive determination of ultra-thin GaN cap layer thickness in AlGaN/GaN HEMT structure by angle resolved x-ray photoelectron spectroscopy (ARXPS)

Anshu Goyal; Brajesh S. Yadav; R. Raman; Ashok K. Kapoor

Angle resolved X-ray photoelectron spectroscopy (ARXPS) and secondary ion mass spectrometry (SIMS) investigations have been carried out to characterize the GaN cap layer in AlGaN/GaN HEMT structure. The paper discusses the qualitative (presence or absence of a cap layer) and quantitative (cap layer thickness) characterization of cap layer in HEMT structure non-destructively using ARXPS measurements in conjunction with the theoretical modeling. Further the relative sensitive factor (RSF=σGaσAl) for Ga to Al ratio was estimated to be 0.963 and was used in the quantification of GaN cap layer thickness. Our results show that Al/Ga intensity ratio varies with the emission angle in the presence of GaN cap layer and otherwise remains constant. Also, the modeling of this intensity ratio gives its thickness. The finding of ARXPS was also substantiated by SIMS depth profiling studies.


Archive | 2014

Structural and Optical Characterization of β-Ga2O3 Thin Films Grown by Pulsed Laser Deposition

Anshu Goyal; Brajesh S. Yadav; O. P. Thakur; Ashok K. Kapoor

Polycrystalline β-Ga2O3 thin films were grown on sapphire substrate (0001) by pulsed laser deposition (PLD) technique. The crystalline structure and optical band gap were studied as a function of growth temperature, laser beam energy, annealing temperature and time. To tailor the band gap of β-Ga2O3 thin films by Al diffusion from the sapphire substrate the films were annealed for 24 h at different temperatures. The amount of Al diffusion was different for different temperatures of annealing which resulted in the increase of band gap as well as the shift of diffraction peaks to higher angles with increasing temperature. The annealed films showed high transparency in the deep UV region of the spectrum.


Physical Chemistry Chemical Physics | 2016

Correction: One step in situ synthesis of CeO2 nanoparticles grown on reduced graphene oxide as an excellent fluorescent and photocatalyst material under sunlight irradiation

Sachin Kumar; Animesh K. Ojha; Donfack Patrice; Brajesh S. Yadav; Arnulf Materny

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Pawan K. Tyagi

Delhi Technological University

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S. S. Kushvaha

National Physical Laboratory

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M. Senthil Kumar

Indian Institute of Technology Madras

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R.S. Srinivasa

Indian Institute of Technology Bombay

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Reetu Kumari

Delhi Technological University

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S.S. Major

Indian Institute of Technology Bombay

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Ashok K. Kapoor

Solid State Physics Laboratory

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K. K. Maurya

National Physical Laboratory

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Lucky Krishnia

Delhi Technological University

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Prashant Tyagi

Academy of Scientific and Innovative Research

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