Abid .

Mr. Abid .

jamia millia islamia
orcid

Research Focus & Metrics

Academic Career Length

9Years (2018-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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1 July 2018 in Sensors and Actuators A: Physical
Verified
Journal Article
Closed access
NCNahid Chaudhary
Nahid Chaudhary
MKManika Khanuja
Manika Khanuja
Abid .Abid .
Abid .
SIS.S. Islam
S.S. Islam

1 April 2018 in Sensors and Actuators B: Chemical
Verified
Journal Article
Closed access
Poonam SehrawatPoonam Sehrawat
Poonam Sehrawat
Abid .Abid .
Abid .
SIS.S. Islam
S.S. Islam
PMPrabhash Mishra
Prabhash Mishra

18 August 2020 in ACS Applied Materials & Interfaces
Verified
Journal Article
Closed access
Abid .Abid .
Abid .
Poonam SehrawatPoonam Sehrawat
Poonam Sehrawat
CJC. M. Julien
C. M. Julien
S.S. IslamS.S. Islam
S.S. Islam

2 April 2019 in ACS Omega
Verified
Journal Article
Open access
MTMohammad Talib
Mohammad Talib
RTRana Tabassum
Rana Tabassum
Abid .Abid .
Abid .
SISaikh Safiul Islam
Saikh Safiul Islam
PMPrabhash Mishra
Prabhash Mishra
We report the fabrication and characterization of visible and near-infrared-resistive photodetector using horizontally aligned titanium tri sulfide (TiS3) nanoribbons. The fabrication process employed micro-electromechanical system, photolithography and dielectrophoretic (DEP) methods. The interdigitated electrodes (IDE) fingers were fabricated using photolithography and thin-film metallization techniques onto the Si/SiO2 substrate, and then TiS3 nanoribbons were horizontally aligned in between IDE using DEP. The fabricated device was first characterized in absence of light and then, the photodetector-based characteristics were obtained by illuminating it with fiber-coupled laser beam. These characteristics were optimized by varying wavelength and power density of the laser beam. The present photodetector shows a maximum responsivity of 5.22 × 102 A/W, quantum efficiency of 6.08 × 102, and detectivity of 1.69 × 109 Jones. The switching times, i.e., response and recovery times were found to be 1.53 and 0.74 s, respectively, with 1064 nm wavelength and 3.4 mW/mm2 power density of the laser beam. Also, the effect of O2 adsorption on nanoribbons has been studied and it is found that adsorbed O2 acts as electron acceptor and decreases the conductivity of the photodetector. Experimentally, it is found that the photoresponse of the horizontally aligned TiS3 nanoribbons is better than that of a randomly oriented TiS3 nanoribbon-based photodetector. Finally, the performance of the present photodetector was compared to that of the previous ones that were found to outperform the reported ones. The additional advantages of the photodetector include excellent stability and portability from which it may be concluded that TiS3 nanoribbons can be a promising candidate for application in nanoscale electronic and optoelectronic devices.

1 January 2018 in Sensors and Actuators A: Physical
Verified
Journal Article
Closed access
Abid .Abid .
Abid .
Poonam SehrawatPoonam Sehrawat
Poonam Sehrawat
SIS.S. Islam
S.S. Islam
PGPayal Gulati
Payal Gulati
MTMohammad Talib
Mohammad Talib
MKManika Khanuja
Manika Khanuja

17 April 2019 in Journal of Applied Physics
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Journal Article
Open access
PDF file
Abid .Abid .
Abid .
Poonam SehrawatPoonam Sehrawat
Poonam Sehrawat
SIS. S. Islam
S. S. Islam
Exfoliation of bulk WS2 powder has been conducted by ultrasonication, and its layer by layer peeling is monitored by HRTEM, XRD, UV-Vis, and Raman spectroscopy. HRTEM confirms the peeling process and selected area electron diffraction pattern shows the crystallinity of nanosheets which is in accordance with the X-ray diffraction results. Raman and UV-visible spectroscopies further confirm the exfoliation of WS2 to nanosheets having a few layers. A photodetector developed from a few-layered WS2 film is used for photodetection over wide wavelength and temperature ranges. The detector exhibits the highest sensitivity at 635 nm with a value of 382% at 77 K against a value of 138% at 300 K, while the response and the recovery time are ∼78 ms and ∼40 ms, respectively. Temperature, excitation wavelength, and laser power-dependent studies show the threshold limit of its faithful operation. Temperature-dependent photoresponsivity and sensitivity are explained in terms of the carrier–phonon scattering dependent transport mechanism. The scattering cross-section analysis using the density functional theory model reveals that it is the in-plane and out-of-plane acoustic modes that play a key role in carrier transport, rather than the optical phonons. The influence of atmospheric constituents (N2, O2) on detector performance is checked by a successive exposure to dry N2 and ambient air flow. A 14% reduction in photoresponsivity under O2 exposure is observed and suitable analysis is given in terms of O2 induced enhancement of the electron–hole recombination process, leading to a loss of photogenerated carriers. The sensor's cycling performance remains unaffected even after a prolonged exposure in ambient conditions (55% RH), showing its chemical stability even for long-term use.