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Dive into the research topics where Surajit Saha is active.

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Featured researches published by Surajit Saha.


Applied Physics Letters | 2001

Large reduction of leakage current by graded-layer La doping in (Ba0.5, Sr0.5)TiO3 thin films

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

Anisotropic two dimensional electron gas at the LaAlO3/SrTiO3(110) interface

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

Graphene versus Multi-Walled Carbon Nanotubes for Electrochemical Glucose Biosensing

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

Microstructure related influence on the electrical properties of pulsed laser ablated (Ba, Sr)TiO3 thin films

Surajit Saha; S. B. Krupanidhi

The microstructural dependence of electrical properties of


Journal of Applied Physics | 2000

Impact of microstructure on the electrical stress induced effects of pulsed laser ablated (Ba, Sr)TiO3 thin films

Surajit Saha; S. B. Krupanidhi

(Ba, Sr)TiO_3 (BST)


ACS Nano | 2012

Electronic Properties of Nanodiamond Decorated Graphene

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

Selective growth of single phase VO2(A, B, and M) polymorph thin films

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

Manifestation of geometric frustration on magnetic and thermodynamic properties of the pyrochlores Sm 2 X 2 O 7 ( X = Ti , Zr )

Surjeet Singh; Surajit Saha; S. K. Dhar; R. Suryanarayanan; A. K. Sood; A. Revcolevschi

and


EPL | 2012

Optical conductivity study of screening of many-body effects in graphene interfaces

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

Raman evidence for orbiton-mediated multiphonon scattering in multiferroic TbMnO3.

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.

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A. K. Sood

Indian Institute of Science

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D. V. S. Muthu

Indian Institute of Science

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S. K. Dhar

Tata Institute of Fundamental Research

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Abhijeet Patra

National University of Singapore

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K. Gopinadhan

National University of Singapore

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Amar Srivastava

National University of Singapore

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