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Dive into the research topics where S. Dhara is active.

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Featured researches published by S. Dhara.


Applied Physics Letters | 2003

Enhanced dynamic annealing in Ga ¿ ion-implanted GaN nanowires

S. Dhara; A. Datta; Chien-Ting Wu; Zon-Huang Lan; K. H. Chen; Y. L. Wang; L. C. Chen; Chi-Wei Hsu; H.-M. Lin; Chia-Chun Chen

Ga+ ion implantation of chemical-vapor-deposited GaN nanowires (NWs) is studied using a 50-keV Ga+ focused ion beam. The role of dynamic annealing (defect-annihilation) is discussed with an emphasis on the fluence-dependent defect structure. Unlike heavy-ion-irradiated epitaxial GaN film, large-scale amorphization is suppressed until a very high fluence of 2×1016 ions cm−2. In contrast to extended-defects as reported for heavy-ion-irradiated epitaxial GaN film, point-defect clusters are identified as major component in irradiated NWs. Enhanced dynamic annealing induced by high diffusivity of mobile point-defects in the confined geometry of NWs is identified as the probable reason for observed differences.


Applied Physics Letters | 2007

Multiphonon Raman scattering in GaN nanowires

S. Dhara; Sharat Chandra; G. Mangamma; S. Kalavathi; P. Shankar; K. G. M. Nair; A. K. Tyagi; Chuang-Han Hsu; Chung Chiu Kuo; L. C. Chen; K. H. Chen; K. K. Sriram

UV Raman scattering studies show longitudinal optical (LO) mode up to fourth order in wurtzite GaN nanowire system. Frohlich interaction of electron with the long range electrostatic field of ionic bonded GaN gives rise to enhancement in LO phonon modes. Good crystalline quality, as indicated by the crystallographic as well as luminescence studies, is thought to be responsible for this significant observation. Calculated size dependence, incorporating size corrected dielectric constants, of electron-phonon interaction energy agrees well with measured values and also predict stronger interaction energy than that of the bulk for diameter below ∼3nm.


RSC Advances | 2014

Plasmon-mediated, highly enhanced photocatalytic degradation of industrial textile dyes using hybrid ZnO@Ag core–shell nanorods

V. P. Dinesh; P. Biji; Anuradha Ashok; S. Dhara; M. Kamruddin; A. K. Tyagi; Baldev Raj

Hybrid ZnO@Ag core–shell heterojunction nanorods were synthesized using a novel, facile two-step process based on hydrothermal and seed mediated growth techniques. The material was characterized by UV-visible spectroscopy, Fourier transform-infrared spectroscopy (FT-IR), room temperature photoluminescence spectroscopy (RTPL), Raman spectroscopy, thermogravimetric analysis (TGA), X-ray diffraction (XRD), high resolution transmission electron microscopy (HRTEM) and X-ray photoelectron spectroscopy (XPS). The hybrid ZnO@Ag core–shell nanorods were comprised of one-dimensional (1D) ZnO nanorods serving as a core material, over which surface-doped Ag nanoclusters (∼2.5 nm) were anchored as a heterogeneous shell. The presence of oxygen vacancies and Zn interstitials were confirmed by RTPL and Raman spectroscopic analysis. The photocatalytic activity of the hybrid ZnO@Ag core–shell nanorods was studied in comparison to bare ZnO nanorods using standard R6G dye and industrial textile dyes such as Congo red and Amido black 10B under UV and visible light (solar) irradiations. Moreover, the material was tested for real time industrial textile effluents under ambient conditions and was found to be highly efficient. The enhanced photocatalytic property observed for ZnO@Ag hybrid core–shell nanorods is attributed to a phenomenal increase in oxygen related defects in the core that generate photo-induced charge carriers and the presence of plasmonic Ag nanoclusters in the shell, which act as a sink for the photo-induced charge carriers.


Biosensors and Bioelectronics | 2013

Direct label free ultrasensitive impedimetric DNA biosensor using dendrimer functionalized GaN nanowires

Prasana Sahoo; Sumathi Suresh; S. Dhara; Garima Saini; S. Rangarajan; A. K. Tyagi

We demonstrate a very simple and generic protocol for ultrasensitive in-situ label-free detection of DNA hybridization using third generation poly(amidoamine)dendrimer (G3-PAMAM) functionalized GaN nanowires (NWs). PAMAM modified GaN NWs provides large density of docking site to immobilize significant number of probe (p-) DNA covalently. These p-DNA/PAMAM/GaN NWs sensor probes are employed to achieve an ultra-high detection limit down to attomolar level concentration of complementary target (t-) DNA. Comparative in-situ studies on single/triple base-pair mismatched, γ-irradiated and complementary t-DNA in the hybridization process reveal selectivity and specificity of the p-DNA/PAMAM/GAN NWs sensor probe over a wide range, 10(-8) to 10(-19)M, of analyte concentration. During the hybridization process, there is a substantial change in t-DNA concentration dependent interfacial polarization resistance during electrochemical impedance measurement, which forms the basis of the present DNA biosensor. This novel methodology for specific DNA sequence detection, as compared with the existing methods, is found to be very robust, highly sensitive, and reproducible.


Applied Surface Science | 1997

XPS studies on silicide formation in ion beam irradiated Au/Si system

D.K Sarkar; Santanu Bera; S. Dhara; K. G. M. Nair; S.V. Narasimhan; S. Chowdhury

Abstract X-ray photoelectron spectroscopic (XPS) studies were carried out on ion-beam irradiated Au/Si system. Thin films of Au (500 A) were vapour deposited on Si〈111〉 and irradiated with 120 keV Ar + ions at different temperatures. The XPS investigation showed the formation of gold silicide. Even in the case of the sample irradiated at room temperature silicide phase was observed at the top surface indicating the out-diffusion of silicon. Increase in the concentration of silicide phase at the top surface with increasing temperature of irradiation was observed suggesting higher out-diffusion of silicon at elevated irradiation temperature. The paper presents the results of the above study and proposes a simple model to explain the growth of the silicide phase.


Journal of Materials Chemistry C | 2013

The role of SnO2 quantum dots in improved CH4 sensing at low temperature

A. Das; Venkataramana Bonu; Arun K. Prasad; D. Panda; S. Dhara; Ashok Kumar Tyagi

The role of quantum dots (QDs) of SnO2 in detecting low concentrations of methane (CH4) at a relatively low temperature of ∼150 °C with high response (S ∼ 3.5%) and response time below 1 min is reported. A simple room temperature single step chemical process was adopted for the growth of SnO2 nanoparticles of a size around 2.4 nm. These nanoparticles were subsequently annealed at 800 °C to increase the grain size to 25 nm. The as-prepared SnO2 nanoparticles, being smaller than the corresponding Bohr radius (2.7 nm), showed a strong quantum confinement effect with a blue shift in the band gap energy from 3.6 eV for the bulk SnO2 to 4.37 eV for the QDs. These QDs exhibited a strong sensing response to CH4 in comparison to the annealed sample. A low activation energy of 90 meV, as estimated from the temperature dependent S plot for SnO2 QDs, was found to be the driving force for such unusual high sensitivity at a low operating temperature. X-ray diffraction, transmission electron microscopy, along with Raman spectroscopy measurements are used for the detailed structural studies. The critical role of the chemisorbed oxygen species present at different operating temperatures on the surface of the off-stoichiometric quantum sized SnO2 and bulk-like annealed samples are discussed in light of the adsorption kinetics.


International Journal of Nanotechnology | 2010

Surface optical modes in GaN nanowires

Prasana Sahoo; S. Dhara; S. Dash; A. K. Tyagi; Baldev Raj; C. R. Das; P. Chandramohan; M.P. Srinivasan

We investigate the optical phonons in crystalline GaN nanowires using Raman spectroscopy. Reduced phonon lifetime in the nanostructures is attributed to the increased anisotropy in lattice vibrations. Apart from the group theoretically allowed optical phonons, new phonon modes around 652 cm−1 and 691 cm−1 have been observed. In view of its good agreement with values in GaN, the observed phonon mode is assigned as surface optical (SO) phonon. This could be attributed to the surface modulation along the GaN nanowire diameter and it is quantitatively evaluated with observed surface morphology and the calculated dispersion relation corresponding to SO phonon modes. The modulation in the surface morphology, observed in the present study, is typical of the vapour-liquid-solid growth process. The instability in the surface phonon potential activates the SO phonon modes, which is well explained in this present study.


Nanotechnology | 2015

Catalyst free growth of ZnO nanowires on graphene and graphene oxide and its enhanced photoluminescence and photoresponse

Ravi K. Biroju; Nikhil Tilak; Gone Rajender; S. Dhara; P. K. Giri

We demonstrate the graphene assisted catalyst free growth of ZnO nanowires (NWs) on chemical vapor deposited (CVD) and chemically processed graphene buffer layers at a relatively low growth temperature (580 °C) in the presence and absence of ZnO seed layers. In the case of CVD graphene covered with rapid thermal annealed ZnO buffer layer, the growth of vertically aligned ZnO NWs takes place, while the direct growth on CVD graphene, chemically derived graphene (graphene oxide and graphene quantum dots) without ZnO seed layer resulted in randomly oriented sparse ZnO NWs. Growth mechanism was studied from high resolution transmission electron microscopy and Raman spectroscopy of the hybrid structure. Further, we demonstrate strong UV, visible photoluminescence (PL) and enhanced photoconductivity (PC) from the CVD graphene-ZnO NWs hybrids as compared to the ZnO NWs grown without the graphene buffer layer. The evolution of crystalinity in ZnO NWs grown with ZnO seed layer and graphene buffer layer is correlated with the Gaussian line shape of UV and visible PL. This is further supported by the strong Raman mode at 438 cm(-1) significant for the wurtzite phase of the ZnO NWs grown on different graphene substrates. The effect of the thickness of ZnO seed layers and the role of graphene buffer layers on the aligned growth of ZnO NWs and its enhanced PC are investigated systematically. Our results demonstrate the catalyst free growth and superior performance of graphene-ZnO NW hybrid UV photodetectors as compared to the bare ZnO NW based photodetectors.


Applied Physics Letters | 2008

Surface optical Raman modes in InN nanostructures

Satyaprakash Sahoo; Ming-Shien Hu; Chuang-Han Hsu; C. T. Wu; K. H. Chen; Li-Chyong Chen; Akhilesh K. Arora; S. Dhara

Raman spectroscopic investigations are carried out on one-dimensional nanostructures of InN, such as nanowires and nanobelts synthesized by chemical vapor deposition. In addition to the optical phonons allowed by symmetry A1, E1, and E2 (high) modes, two additional Raman peaks are observed around 528 and 560 cm−1 for these nanostructures. Calculations for the frequencies of surface optical (SO) phonon modes in InN nanostructures yield values close to those of the new Raman modes. A possible reason for large intensities for SO modes in these nanostructures is also discussed.


Applied Physics Letters | 2004

Blueshift of yellow luminescence band in self-ion-implanted n-GaN nanowire

S. Dhara; A. Datta; Chien-Ting Wu; Zon-Huang Lan; K. H. Chen; Yuh-Lin Wang; Yang-Fang Chen; Chuang-Han Hsu; L. C. Chen; Hung-Min Lin; Chia-Chun Chen

Optical photoluminescence studies are performed in self-ion (Ga+)-implanted nominally doped n-GaN nanowires. A 50 keV Ga+ focused ion beam in the fluence range of 1×1014–2×1016 ions cm−2 is used for the irradiation process. A blueshift is observed for the yellow luminescence (YL) band with increasing fluence. Donor–acceptor pair model with emission involving shallow donor introduced by point-defect clusters related to nitrogen vacancies and probable deep acceptor created by gallium interstitial clusters is responsible for the shift. High-temperature annealing in nitrogen ambient restores the peak position of YL band by removing nitrogen vacancies.

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A. K. Tyagi

Indira Gandhi Centre for Atomic Research

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S. Dash

Indira Gandhi Centre for Atomic Research

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A. K. Sivadasan

Indira Gandhi Centre for Atomic Research

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A. Das

Indira Gandhi Centre for Atomic Research

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Avinash Patsha

Indira Gandhi Centre for Atomic Research

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K. G. M. Nair

Indira Gandhi Centre for Atomic Research

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P. Magudapathy

Indira Gandhi Centre for Atomic Research

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S. Amirthapandian

Indira Gandhi Centre for Atomic Research

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Ashok Kumar Tyagi

Indira Gandhi Centre for Atomic Research

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