Surajit Saha
Indian Institute of Science
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by Surajit Saha.
Applied Physics Letters | 2001
Surajit Saha; S. B. Krupanidhi
A large reduction in the leakage current behavior in (Ba, Sr)TiO3 (BST) thin films was observed by graded-layer donor doping. The graded doping was achieved by introducing La-doped BST layers in the grown BST films. The films showed a large decrease (about six orders of magnitude) in the leakage current in comparison to undoped films at an electric field of 100 kV/cm. The large decrease in leakage current was attributed to the formation of highly resistive layers, originating from compensating defect chemistry involved for La-doped films grown in oxidizing environment. Temperature-dependent leakage-current behavior was studied to investigate the conduction mechanism and explanations of the results were sought from Poole–Frenkel conduction mechanism.
Nature Communications | 2013
A. Annadi; Xiao Wang; K. Gopinadhan; W. M. Lü; A. Roy Barman; Z. Q. Liu; Amar Srivastava; Surajit Saha; Y. L. Zhao; S. W. Zeng; S. Dhar; Nikolina Tuzla; Eva Olsson; Qinfang Zhang; Bo Gu; Seiji Yunoki; Sadamichi Maekawa; H. Hilgenkamp; T. Venkatesan; A. Ariando
The observation of a high-mobility two-dimensional electron gas between two insulating complex oxides, especially LaAlO3/SrTiO3, has enhanced the potential of oxides for electronics. The occurrence of this conductivity is believed to be driven by polarization discontinuity, leading to an electronic reconstruction. In this scenario, the crystal orientation has an important role and no conductivity would be expected, for example, for the interface between LaAlO3 and (110)-oriented SrTiO3, which should not have a polarization discontinuity. Here we report the observation of unexpected conductivity at the LaAlO3/SrTiO3 interface prepared on (110)-oriented SrTiO3, with a LaAlO3-layer thickness-dependent metal-insulator transition. Density functional theory calculation reveals that electronic reconstruction, and thus conductivity, is still possible at this (110) interface by considering the energetically favourable (110) interface structure, that is, buckled TiO2/LaO, in which the polarization discontinuity is still present. The conductivity was further found to be strongly anisotropic along the different crystallographic directions with potential for anisotropic superconductivity and magnetism, leading to possible new physics and applications.
Materials | 2013
Dan Zheng; Sandeep Kumar Vashist; Michal Marcin Dykas; Surajit Saha; Khalid Al-Rubeaan; Edmond Lam; John H. T. Luong; Fwu-Shan Sheu
A simple procedure was developed for the fabrication of electrochemical glucose biosensors using glucose oxidase (GOx), with graphene or multi-walled carbon nanotubes (MWCNTs). Graphene and MWCNTs were dispersed in 0.25% 3-aminopropyltriethoxysilane (APTES) and drop cast on 1% KOH-pre-treated glassy carbon electrodes (GCEs). The EDC (1-ethyl-(3-dimethylaminopropyl) carbodiimide)-activated GOx was then bound covalently on the graphene- or MWCNT-modified GCE. Both the graphene- and MWCNT-based biosensors detected the entire pathophysiological range of blood glucose in humans, 1.4–27.9 mM. However, the direct electron transfer (DET) between GOx and the modified GCE’s surface was only observed for the MWCNT-based biosensor. The MWCNT-based glucose biosensor also provided over a four-fold higher current signal than its graphene counterpart. Several interfering substances, including drug metabolites, provoked negligible interference at pathological levels for both the MWCNT- and graphene-based biosensors. However, the former was more prone to interfering substances and drug metabolites at extremely pathological concentrations than its graphene counterpart.
Journal of Applied Physics | 2000
Surajit Saha; S. B. Krupanidhi
The microstructural dependence of electrical properties of
Journal of Applied Physics | 2000
Surajit Saha; S. B. Krupanidhi
(Ba, Sr)TiO_3 (BST)
ACS Nano | 2012
Yu Wang; Manu Jaiswal; Ming Lin; Surajit Saha; Barbaros Özyilmaz; Kian Ping Loh
thin films were studied from the viewpoint of dc and ac electrical properties. The films were grown using a pulsed laser deposition technique in a temperature range of 300 to 600 °C, inducing changes in grain size, structure, and morphology. Consequently, two different types of films were realized, of which type I, was polycrystalline, multigrained, while type II was [100] oriented possessing a densely packed fibrous microstructure. Leakage current measurements were done at elevated temperatures to provide evidence of the conduction mechanism present in these films. The results revealed a contribution from both electronic and ionic conduction. In the case of type I films, two trapping levels were identified with energies around 0.5 and 2.73 eV, which possibly originate from oxygen vacancies
APL Materials | 2015
Amar Srivastava; Helene Rotella; Surajit Saha; Banabir Pal; Gopinadhan Kalon; Sinu Mathew; M. Motapothula; Michal Marcin Dykas; Ping Yang; Eiji Okunishi; D. D. Sarma; T. Venkatesan
V_O
Physical Review B | 2008
Surjeet Singh; Surajit Saha; S. K. Dhar; R. Suryanarayanan; A. K. Sood; A. Revcolevschi
and
EPL | 2012
Pranjal Kumar Gogoi; Iman Santoso; Surajit Saha; Sihao Wang; Antonio H. Castro Neto; Kian Ping Loh; T. Venkatesan; Andrivo Rusydi
Ti^{3+}
Journal of Physics: Condensed Matter | 2010
Pradeep Kumar; Surajit Saha; D. V. S. Muthu; Jyoti Ranjan Sahu; A. K. Sood; C. N. R. Rao
centers, respectively. These levels act as shallow and deep traps and are reflected in the current–voltage characteristics of the BST thin films. The activation energy associated with oxygen vacancy motion in this case was obtained as 1.28 eV. On the contrary, type II films showed no evidence of deep trap energy levels, while the identified activation energy associated with shallow traps was obtained as 0.38 eV. The activation energy obtained for oxygen vacancy motion in type II films was around 1.02 eV. The dc measurement results were further elucidated through ac impedance analysis, which revealed a grain boundary dominated response in type I in comparison to type II films where grain response is highlighted. A comparison of the mean relaxation time of the two films revealed three orders of magnitude higher relaxation time in the case of type I films. Due to smaller grain size in type I films the grains were considered to be completely depleted giving rise to only grain boundary response for the bulk of the film. The activation energy obtained from conductivity plots agree very well with that of dc measurements giving values 1.3 and 1.07 eV for type I and type II films, respectively. Since oxygen vacancy transport have been identified as the origin of resistance degradation in BST thin films, type I films with their higher value of activation energy for oxygen ion mobility explains the improvement in breakdown characteristics under constant high dc field stress. The role of microstructure in controlling the rate of degradation is found useful in this instance to enhance the film properties under high electric field stresses.