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Rawat, Rajdeep Singh
- PublicationOpen AccessComputing plasma focus pinch current from total current measurement(American Institute of Physics, 2008)
;Lee, Sing ;Saw, Sor Heoh; ; Schmidt, H.The total current Itotal waveform in a plasma focus discharge is the most commonly measured quantity, contrasting with the difficult measurement of Ipinch. However, yield laws should be scaled to focus pinch current Ipinch rather than the peak Itotal. This paper describes how Ipinch may be computed from the Itotal trace by fitting a computed current trace to the measured current trace using the Lee model. The method is applied to an experiment in which both the Itotal trace and the plasma sheath current trace were measured. The result shows good agreement between the values of computed and measured Ipinch.
WOS© Citations 52Scopus© Citations 63 232 334 - PublicationOpen AccessOn the plume splitting of pulsed laser ablated Fe and AI plasmas(American Institute of Physics, 2010)
;Mahmood, S.; ;Darby, M. S. B. ;Zakaullah, M.; ; A time resolved imaging study of pulsed laser ablated Fe and Al plasma plumes with specific interest in the splitting of plumes into the slow and fast moving components as they expand through the background argon gas at different pressures is reported. The material ablation was achieved using a Q-switched Nd:YAG yttrium aluminum garnet laser operating at 532 nm with a pulse duration of 8 ns full width at half maximum and a fluence of 30 Jcm−2 at the target surface. Typical time resolved images with low magnification show that the splitting occurs at moderate background gas pressures 0.5 and 1.0 mbar for Fe, and 0.2 mbar for Al plasma plumes. The plume splitting did not occur for higher background gas pressures.WOS© Citations 36Scopus© Citations 42 340 323 - PublicationOpen AccessBackward high energy ion beams from plasma focus(American Institute of Physics, 2009)
;Roshan, M. V.; ;Lee, Sing ;Talebitaher, A.; High energy neutrons, more than 2.45 MeV from deuteron-deuteron fusion reaction, have been measured in backward direction of plasma focus devices in many laboratories. However the experimental evidence for high energy deuterons responsible for such neutrons has not been reported so far. In this brief communication, backward high energy deuteron beam from NX2 plasma focus [M. V. Roshan et al., Phys. Lett. A 373, 851 (2009)] is reported, which was measured with a direct and unambiguous technique of nuclear activation. The relevant nuclear reaction for the target activation is 12C (d, n)13N , which has a deuteron threshold energy of 328 keV.
WOS© Citations 14Scopus© Citations 16 394 184 - PublicationMetadata onlyTailoring structural and magnetic viz. static and dynamic properties of soft magnetic CoFeB film with Ta incorporation(Elsevier, 2022)
;Vardhan, Harsh ;Surendra Singh ;Gupta, Surbhi ;Sharma, Kavita ;Yasmeen Jafri ;Gupta, Mukul ;Reddy, V. R.; ;Gupta, Ajay ;Gome, AnilSharma, GaganPresent study provides an insight of tailoring magnetic properties (static and dynamic) driven by structural modifications, with controlled incorporation of Ta in soft magnetic CoFeB films. Unlike conventional thermal annealing, stress induced in-plane uniaxial magnetic anisotropy of CoFeB have observed to be release with incorporation of Ta, as confirmed from in-plane rotation dependent magneto-optical Kerr effect (MOKE). Increasing atomic percent of Ta in CoFeB is accompanied with decreasing saturation magnetization of soft-magnetic layer and film densification, as confirmed from polarized neutron and X-ray reflectivities. Ferromagnetic resonance (FMR) confirms the reduction of effective magnetization of the samples with Ta incorporation, with rise of damping parameter because of increasing magnetic inhomogenities. Further, the effect of vacuum annealing on these films has been investigated. Post annealing measurements suggest rapid elimination of magnetic anisotropy for Ta doped CoFeB films. Annealing at a temperature beyond CoFeB crystallization temperature results in an increase of magnetization, relative to as-prepared samples, amplitude of which modifies with incorporated Ta concentration. Such enhancement is accompanied with the structural changes as confirmed from X-ray diffraction (XRD) measurements, resulting an increase of magnetic coercivity. The results are important in view of tailoring the functional properties of CoFeB films for wide range of applications.WOS© Citations 3Scopus© Citations 6 286 - PublicationMetadata onlyModelling in-device inference and classification of binary digits using nonlinear dynamics of spin Hall Oscillator(2023)
;Mohan, John Rex ;Yamanaka, Chisato ;Feng, Ryoyan ;Mathew, Arun Jacob ;Nakamura, Yoji ;Medwal, Rohit ;Gupta, Surbhi; Fukuma, YosuhiroIn this work, we employ micromagnetic modelling of a spin Hall oscillator for a direct inference and classification of binary digit inputs. The spectral characteristics of the oscillation is utilized for the classification. We observed a direct inference of binary digit inputs up to a sequence of four binary digits. Subsequently, handwritten digit image recognition is tested with the Modified National Institute of Standards and Testing (MNIST) handwritten digit database and acquired an accuracy of 88.6% with a linear classifier network.27 - PublicationMetadata onlyFacet control of nickel nitride nano‐framework for efficient hydrogen evolution electrocatalysis via auxiliary cooling assisted plasma engineering(Wiley, 2022)
;Ouyang, Bo ;Zhang, Yongqi ;Wang, Xi ;Deng, Yilin ;Liu, Feng ;Fang, Zhi; Kan, ErjunThe precise facet modulation of transition metal nitrides (TMNs) has been regarded as an essential issue in boosting electrocatalytic H2 production. Compared to thermal nitridation, the plasma technique serves as a favorable alternative to directly achieve TMNs, but the apparent surface heating effect during plasma treatment inevitably causes the thermally stabilized nitride formation, resulting in the deterioration of the highly reactive facet. To optimize the hydrogen evolution reaction (HER) behavior, an auxiliary cooling assisted plasma system to selectively expose Ni3N (2-10) with favorable activity by controlling surface heating during plasma nitridation is designed. The resultant nickel nitride (cp-Ni3N) nano-framework delivers exceptional catalytic performance, evidenced by its low overpotential of 58 and 188 mV at the current density of 10 and 100 mA cm−2 for HER, in stark comparison with that of normal plasma and thermally fabricated Ni3N. Operando plasma diagnostics along with numerical simulation further confirm the effect of surface heating on typical plasma parameters as well as the Ni3N nanostructure, indicating the key factor responsible for the high-performance nitride electrocatalyst.
6 - PublicationOpen AccessCurrent sheath formation dynamics and structure for different insulator lengths of plasma focus deviceThe breakdown phase of the UNU-ICTP plasma focus (PF) device was successfully simulated using the electromagnetic particle in cell method. A clear uplift of the current sheath (CS) layer was observed near the insulator surface, accompanied with an exponential increase in the plasma density. Both phenomena were found to coincide with the surge in the electric current, which is indicative of voltage breakdown. Simulations performed on the device with different insulator lengths showed an increase in the fast ionization wave velocity with length. The voltage breakdown time was found to scale linearly with the insulator length. Different spatial profiles of the CS electron density, and the associated degree of uniformity, were found to vary with different insulator lengths. The ordering, according to the degree of uniformity, among insulator lengths of 19, 22, and 26 mm agreed with that in terms of soft X-ray radiation yield observed from experiments. This suggests a direct correlation between CS density homogeneity near breakdown and the radiation yield performance. These studies were performed with a linearly increasing voltage time profile as input to the PF device.
WOS© Citations 6Scopus© Citations 6 234 227 - PublicationOpen AccessCoded aperture imaging of alpha source spatial distribution(Elsevier, 2012)
;Alireza Talebitaher; ; ; The Coded Aperture Imaging (CAI) technique has been applied with CR-39 nuclear track detectors to image alpha particle source spatial distributions. The experimental setup comprised: a 226Ra source of alpha particles, a laser-machined CAI mask, and CR-39 detectors, arranged inside a vacuum enclosure. Three different alpha particle source shapes were synthesized by using a linear translator to move the 226Ra source within the vacuum enclosure. The coded mask pattern used is based on a Singer Cyclic Difference Set, with 400 pixels and 57 open square holes (representing ρ = 1/7 = 14.3% open fraction). After etching of the CR-39 detectors, the area, circularity, mean optical density and positions of all candidate tracks were measured by an automated scanning system. Appropriate criteria were used to select alpha particle tracks, and a decoding algorithm applied to the (x, y) data produced the de-coded image of the source. Signal to Noise Ratio (SNR) values obtained for alpha particle CAI images were found to be substantially better than those for corresponding pinhole images, although the CAI-SNR values were below the predictions of theoretical formulae. Monte Carlo simulations of CAI and pinhole imaging were performed in order to validate the theoretical SNR formulae and also our CAI decoding algorithm. There was found to be good agreement between the theoretical formulae and SNR values obtained from simulations. Possible reasons for the lower SNR obtained for the experimental CAI study are discussed.WOS© Citations 4Scopus© Citations 6 373 268 - PublicationMetadata onlyElectrically tunable singular phase and Goos–Hänchen shifts in phase‐change‐material‐based thin‐film coatings as optical absorbers(Wiley, 2021)
;Sreekanth, Kandammathe Valiyaveedu ;Das, Chandreyee Manas ;Medwal, Rohit ;Mishra, Mayank ;Ouyang, Qingling; ;Yong, Ken-TyeSingh, RanjanThe change of the phase of light under the evolution of a nanomaterial with time is a promising new research direction. A phenomenon directly related to the sudden phase change of light is the Goos–Hänchen (G–H) shift, which describes the lateral beam displacement of the reflected light from the interface of two media when the angles of incidence are close to the total internal reflection angle or Brewster angle. Here, an innovative design of lithography-free nanophotonic cavities to realize electrically tunable G–H shifts at the singular phase of light in the visible wavelengths is reported. Reversible electrical tuning of phase and G–H shifts is experimentally demonstrated using a microheater integrated optical cavity consisting of a dielectric film on an absorbing substrate through a Joule heating mechanism. In particular, an enhanced G–H shift of 110 times of the operating wavelength at the Brewster angle of the thin-film cavity is reported. More importantly, electrically tunable G–H shifts are demonstrated by exploiting the significant tunable phase change that occurs at the Brewster angles, due to the small temperature-induced refractive index changes of the dielectric film. Realizing efficient electrically tunable G–H shifts with miniaturized heaters will extend the research scope of the G–H shift phenomenon and its applications.9 - PublicationMetadata onlyEffect of light and heat on polymer‐based resistive random access memory(Wiley, 2021)
;Mahato, Bipul Kumar ;Medwal, Rohit ;Deen, Ghulam Roshan ;Piramanayagam, S. N.Highly repeatable, photosensitive nonvolatile resistive random access memory (ReRAM) made of a Si/SiO2/Cu/PRPC/Ta stack with a photoresponsive polymer composite (PRPC) as the active medium is presented. The device shows errorless bipolar resistive switching with more than 100 cycles repeatability and stable SET and RESET voltages. It changes its resistive states in response to white light and recovers completely after removal of the light source. It also changes its state in response to heat and recovers randomly after the removal of the heat source. The phenomenon is explained by valance charge transfer along with a space-charge-limited conduction (SCLC) mechanism. The initial state of the device is low resistance state (LRS) because of electric-field-induced formation of valance charge transfer states. It switches to a high resistance state (HRS) due to electric-field-induced dissociation of the charge transfer states.7