Avanendra Singh
National Institute of Science Education and Research
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by Avanendra Singh.
RSC Advances | 2015
Avanendra Singh; Samir Kumar; Ritwick Das; Pratap K. Sahoo
We have investigated the effect that manganese (Mn)-doping in ZnO sub-wavelength rods (or nanorods) has on nonlinear optical properties, namely two-photon absorption (TPA) and nonlinear refraction using the single-beam Z-scan technique. Mn-doped ZnO nanorods (NRs) were prepared by a low temperature aqueous growth technique. The results show that the Mn-doping concentration primarily determines whether ZnO NRs will exhibit saturable absorption (SA) or two-photon-absorption (TPA) characteristics in an open-aperture experiment. At high Mn-doping concentrations, ZnO NRs exhibit SA behaviour which can be attributed to a high occupation probability of defect states as well as the saturation of linear absorption of sub-wavelength rod aggregates at high optical fluence. In contrast to high Mn-doping concentration in ZnO NRs, we observed TPA features in 0.5% Mn-doped ZnO NRs. The employability of such structures in the area of optical limiting and switching is essentially derived from the possibility to tune the nonlinear optical absorption which could be realized by appropriate Mn-doping in ZnO NR architecture.
Journal of Nonlinear Optical Physics & Materials | 2016
Rudrashish Panda; Sayantan Bhattacharya; Rudranarayan Samal; Avanendra Singh; Pratap K. Sahoo; P. K. Datta; S. K. Das
We report efficient second harmonic generation (SHG) of femtosecond (fs) pulses using ZnO nanorods grown by chemical bath deposition (CBD) method with drop-casted seed layer. The SHG behavior of the nanorods are tested using an amplified Ti:sapphire fs laser of pulse duration of 100fs at 800nm. The SHG signal from the ZnO nanorods is found to be of very high intensity as detected by a low cost, compact spectrometer. In a comparative study, the SHG signal from ZnO nanorods grown over seed layer is found to be 12 times higher than the SHG signal observed from the ZnO nanorods grown on substrate without any seed layer. The efficient SHG in former case is due to the growth of high density, well oriented nanorods whereas the lower signal in the later case is due to growth of low density, randomly oriented nanorods. The polarization dependence behavior of the SHG signal is studied both experimentally and theoretically.
Advances in X-Ray/EUV Optics and Components XII | 2017
S. Bhartiya; Avanendra Singh; A. Majhi; A. Gome; R. Dhawan; Maheswar Nayak; Pratap K. Sahoo; S. K. Rai; V. R. Reddy; P. C. Pradhan
We present fabrication and structural analysis of two different multilayer grating structures. W/B4C based lamellar multilayer grating (LMG) was studied for high resolution monochomator application near soft x-ray region (~1.5 keV). Whereas NbC/Si based multilayer phase-shift reflector (MPR) was studied for high reflection at normal incidence near Si L-edge (~99 eV) and simultaneously to suppress the unwanted vacuum ultraviolet / infrared radiation. The grating patterns of different periods down to D = 10 micron were fabricated on Si substrates by using photolithography, and multilayers (MLs) of different periodicity (d = 10 to 2 nm) and number of layer pairs (15 to 100) were coated using sputtering techniques by optimizing the process parameters. The LMG and MPR samples are characterized by x-ray reflectivity (XRR) and atomic force microscopy (AFM) measurements. XRR results show successive higher order Bragg peaks that reveal a well-defined vertical periodic structure in LMG, MPR and ML structures. The lateral periodicity of the grating and depth of the rectangular groves were analyzed using AFM. The AFM results show good quality of lateral periodic structures in terms of groove profile. The effect of the process parameters on the microstructure (both on vertical and lateral patterns) of ML, LMG and MPR were analyzed.
Applied Surface Science | 2017
Ranveer Singh; Mohit Kumar; Mahesh Saini; Avanendra Singh; Biswarup Satpati; T. Som
Physical Chemistry Chemical Physics | 2015
Avanendra Singh; K. Senapati; Biswarup Satpati; Mohit Kumar; Pratap K. Sahoo
Applied Surface Science | 2017
Avanendra Singh; K. Senapati; Mohit Kumar; T. Som; A. K. Sinha; Pratap K. Sahoo
Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms | 2016
D.P. Datta; Vantari Siva; Avanendra Singh; Shalik Ram Joshi; D. Kanjilal; Pratap K. Sahoo
MRS Advances | 2016
Avanendra Singh; K. Senapati; Karuna Kar Nanda; Pratap K. Sahoo
Solar RRL | 2018
Mohit Kumar; Biswarup Satpati; Avanendra Singh; T. Som
Science of Sintering | 2018
Lizina Khatua; Rudrashish Panda; Avanendra Singh; Arpan Nayak Kumar; Pravakar Satapathy; Debabrata Pradhan; Kumar Sahoo Pratap; S.K.S. Parashar; Kumar Das Susanta