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Dive into the research topics where Pragya Tiwari is active.

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Featured researches published by Pragya Tiwari.


Journal of Physics: Condensed Matter | 2007

Magnetocaloric effect in Heusler alloys Ni50Mn34In16 and Ni50Mn34Sn16

Veerendra Kumar Sharma; M. K. Chattopadhyay; Ravi Kumar; Tapas Ganguli; Pragya Tiwari; S. B. Roy

We present results of detailed ac susceptibility, magnetization and specific heat measurements in Heusler alloys Ni50Mn34In16 and Ni50Mn34Sn16. These alloys undergo a paramagnetic to ferromagnetic transition around 305 K, which is followed by a martensitic transition in the temperature regime around 220 K. Inside the martensite phase both the alloys show signatures of field-induced transition from martensite to austenite phase. Both field- and temperature-induced martensite–austenite transitions are relatively sharp in Ni50Mn34In16. We estimate the isothermal magnetic entropy change and adiabatic temperature change across the various phase transitions in these alloys and investigate the possible influence of these transitions on the estimated magnetocaloric effect. The sharp martensitic transition in Ni50Mn34In16 gives rise to a comparatively large inverse magnetocaloric effect across this transition. On the other hand the magnitudes of the conventional magnetocaloric effect associated with the paramagnetic to ferromagnetic transition are quite comparable in these alloys.


Journal of Applied Physics | 2007

Growth and characterization of α-Fe2O3 nanowires

Himanshu Srivastava; Pragya Tiwari; A. K. Srivastava; R. V. Nandedkar

Hematite (α-Fe2O3) nanowires have been synthesized on a large surface area by thermal oxidation of iron foil in an ozone-rich environment. The effects of annealing time, temperature, and oxidizing environment on the growth of nanowires have been systematically studied. The samples were characterized using scanning electron microscope (SEM), transmission electron microscope (TEM), x-ray diffraction (XRD), and x-ray photoelectron spectroscopy (XPS). It was found that annealing in ozone-rich environment for 2–4 h at 700 °C yielded the best results in terms of number density and diameter of nanowires. The average diameter of the nanowires was found to be 85 nm. It was found that nanowires are bicrystal in nature with a length around 4 μm, which grows uniquely along the [110] direction.


Journal of Physics: Condensed Matter | 2010

The effect of substitution of Mn by Fe and Cr on the martensitic transition in the Ni50Mn34In16 alloy

Veerendra Kumar Sharma; M. K. Chattopadhyay; S K Nath; K J S Sokhey; Ravi Kumar; Pragya Tiwari; S. B. Roy

The potential shape memory alloy Ni(50)Mn(34)In(16) is studied with partial substitution of Mn with Fe and Cr to investigate the effect of such substitution on the martensitic transition in the Ni-Mn-In alloy system. The results of ac susceptibility, magnetization and electrical resistivity measurements show that while the substitution with Cr increases the martensitic transition temperature, the substitution with Fe decreases it. Possible reasons for this shift in martensitic transition are discussed. Evidence of kinetic arrest of the austenite to martensite phase transition in the Fe substituted alloys is also presented. Unlike the kinetic arrest of the austenite to martensite phase transition in the parent Ni(50)Mn(34)In(16) alloy which takes place in the presence of high external magnetic field, the kinetic arrest of the austenite to martensite phase transition in the Fe doped alloy occurs even in zero magnetic field. The Cr substituted alloys, on the other hand, show no signature of kinetic arrest of this phase transition.


Journal of Applied Physics | 2012

Photoluminescence study of β-Ga2O3 nanostructures annealed in different environments

R. Jangir; S. Porwal; Pragya Tiwari; Puspen Mondal; S. K. Rai; Tapas Ganguli; S. M. Oak; S. K. Deb

β-Ga2O3 nanostructures (nanowires, nanoribbons, and nanosheets) were synthesized via vapor transport method on gold coated silicon substrate in N2 ambient and these β-Ga2O3 nanostructures grown on silicon substrates were taken as the starting material to study the effect of annealing in the different environments (oxygen, water vapour, and ammonia solution) on the structural front and photoluminescence (PL) properties. The PL spectra of β-Ga2O3 nanostructures exhibit a UV-blue emission band whose intensity is strongly affected by the annealing in different environments. Annealing modifies the surface of the nanostructures by creating surface states which quench the PL by creating competitive nonradiative paths. This study also indicates the dominance of the formation of water induced surface states over ammonia induced surface states. The irreversible nature of these defects significantly affects the applicability of this system in moist high temperature environments.


Science and Technology of Welding and Joining | 2007

Effect of active flux addition on laser welding of austenitic stainless steel

R. Kaul; P. Ganesh; N. Singh; R. Jagdheesh; M. S. Bhagat; Harish Kumar; Pragya Tiwari; H. S. Vora; A. K. Nath

Abstract The use of active flux in tungsten inert gas (TIG) welding is known to increase its weld depth. The present paper involves study of active flux laser beam welding (ALBW) of austenitic stainless steel sheets with respect to its effect on plasma plume, microstructure and mechanical properties of the resultant weldments. ALBW performed with SiO2 as the flux significantly modified shape of the fusion zone (FZ) to produce narrower and deeper welds. Plasma plume associated with the process was considerably smaller and of lower intensity than that produced during bead on plate laser beam welding (LBW). Flux addition during LBW produced thin and rough weld bead associated with humping. The development of such a weld bead is cause by reversal in the direction of Marangoni flow by oxygen induced inversion of surface tension gradient, widely fluctuating plasma plume and presence of oxides on the weld pool surface preventing free flow of the melt. Active flux laser weldments exhibited lower ductility than that of bead on plate laser weldments.


Surface Engineering | 2012

Studies on laser peening using different sacrificial coatings

R Sundar; Harish Kumar; R. Kaul; K Ranganathan; Pragya Tiwari; L. M. Kukreja; S. M. Oak

Abstract Laser shock peening usually requires the presence of a sacrificial coating to protect the substrate from undesirable thermal effects generated by laser irradiation. This paper describes an experimental study to identify an adherent sacrificial coating for laser peening of smooth metallic surfaces where black paint does not adhere well. Normal black polyvinyl chloride electrical insulation tape has been found to be a good choice as a sacrificial coating. Laser peening with black insulation tape generated effective laser peening in three different substrates, namely, Ti6Al4V alloy, SAE 9260 spring steel and DIN X20Cr13 martensitic stainless steel. The depth of peening was comparable or better than that generated with black paint. With respect to widely used black paint, black insulation tape not only provides clean, simple and uniform coating but also literally eliminates the time involved in its application (black paint requires multilayer coating with long intermediate curing periods) and removal.


Journal of Applied Physics | 2010

Contrasting magnetic behavior of Ni50Mn35In15 and Ni50Mn34.5In15.5 alloys

M. K. Chattopadhyay; Meghmalhar Manekar; V. K. Sharma; Parul Arora; Pragya Tiwari; M. K. Tiwari; S B Roy

We have studied the electrical resistivity, magnetization, and heat capacity of the off-stoichiometric Heusler alloys Ni50Mn35In15 and Ni50Mn34.5In15.5 as functions of temperature and magnetic field. The results show that the alloy system is more sensitive to the composition than what is apparent from the established phase diagram. We have found that the ground states as well as the nature of phase transitions strongly depend on concentration differences as low as 0.5 at. %. While in the case of Ni50Mn34.5In15.5 we do observe a magnetic field induced martensite to austenite phase transition, there is no detectable signature of any field induced transition in the Ni50Mn35In15 alloy even up to fields as high as 80 kOe. Accordingly, the functional properties of these two alloys are also drastically different.


Semiconductor Science and Technology | 2011

Water-vapour-assisted growth of ZnO nanowires on a zinc foil and the study of the effect of synthesis parameters

Himanshu Srivastava; Pragya Tiwari; A. K. Srivastava; S. Porwal; S K Deb

Dense and large-aspect-ratio ZnO nanowires have been synthesized by thermal oxidation of a Zn foil under the flow of moist nitrogen. The effects of annealing temperature and time have been systematically studied in detail. It was observed that the length, diameter and number density increase with time and temperature before they saturate at the optimum synthesis condition of 600 °C annealing temperature and 16 h annealing time. The nanowires have been characterized by a scanning electron microscope, a transmission electron microscope, UV–Vis absorption and room temperature photoluminescence. The nanowires grow uniquely along the [1 1 0] direction up to ~14–16 µm length and are of good crystalline and optical quality. It was found that the formation of nanowires enhances greatly in the presence of water vapour. We have also shown by TEM observations that nanowires grow by surface diffusion of Zn ions from root to tip.


Journal of Applied Physics | 2011

X-ray enhancement in a nanohole target irradiated by intense ultrashort laser pulses

U. Chakravarty; V. Arora; J. A. Chakera; P. A. Naik; Himanshu Srivastava; Pragya Tiwari; A. K. Srivastava; P. D. Gupta

In this paper, we present a comparative study of the laser energy absorption, soft x-ray emission (in the water window region: 2.3–4.4 nm) and hard x-ray emission (in the 2–20 keV range) from planar aluminum and nanohole alumina of 40 nm average diameter, when irradiated by Ti:sapphire laser pulses. The laser pulse duration was varied from 45 to 500 fs, and the focused intensity on the target ranged from ∼3 × 1016 W/cm2 to 3×1017 W/cm2. The x-ray yield enhancement from the nanoholes shows an increased coupling of the laser energy to the target. The effect of laser pulse duration on the x-ray emission was also studied, where a resonance like phenomenon was observed. The laser energy absorption measurements in the nanoholes showed a marginal enhancement in absorption as compared to planar Al. The integrated keV x-ray yield, from nanohole alumina and planar Al, at an intensity of 3 × 1017 W/cm2, was 25 and 3.5 μJ, respectively. The results can be explained by considering the hydrodynamic expansion of the las...


Journal of Applied Physics | 2015

Fabrication of large area plasmonic nanoparticle grating structure on silver halide based transmission electron microscope film and its application as a surface enhanced Raman spectroscopy substrate

Sudheer; Pragya Tiwari; S. Bhartiya; C. Mukherjee; M. N. Singh; A. K. Sinha; V. N. Rai; A. K. Srivastava

The plasmonic responses of silver nanoparticle grating structures of different periods made on silver halide based electron microscope film are investigated. Raster scan of the conventional scanning electron microscope (SEM) is used to carry out electron beam lithography for fabricating the plasmonic nanoparticle grating (PNG) structures. Morphological characterization of the PNG structures, carried out by the SEM and the atomic force microscope, indicates that the depth of the groove decreases with a decrease in the grating period. Elemental characterization performed by the energy dispersive spectroscopy and the x-ray diffraction shows the presence of nanoparticles of silver in the PNG grating. The optical characterization of the gratings shows that the localized surface plasmon resonance peak shifts from 366 to 378 nm and broadens with a decrease in grating period from 10 to 2.5 μm. The surface enhanced Raman spectroscopy of the Rhodamine-6G dye coated PNG structure shows the maximum enhancement by two orders of magnitude in comparison to the randomly distributed silver nanoparticles having similar size and shape as the PNG structure.

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A. K. Srivastava

Raja Ramanna Centre for Advanced Technology

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Tapas Ganguli

Raja Ramanna Centre for Advanced Technology

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S. K. Rai

Raja Ramanna Centre for Advanced Technology

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Himanshu Srivastava

Raja Ramanna Centre for Advanced Technology

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L. M. Kukreja

Raja Ramanna Centre for Advanced Technology

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R. Kaul

Raja Ramanna Centre for Advanced Technology

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S. M. Oak

Raja Ramanna Centre for Advanced Technology

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S. Porwal

Raja Ramanna Centre for Advanced Technology

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P. Ganesh

Raja Ramanna Centre for Advanced Technology

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R. Jangir

Raja Ramanna Centre for Advanced Technology

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