Adam J. Simbeck
Rensselaer Polytechnic Institute
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Featured researches published by Adam J. Simbeck.
Scientific Reports | 2013
Chandra Sekhar Rout; Padmashree D. Joshi; Ranjit V. Kashid; Dilip S. Joag; Mahendra A. More; Adam J. Simbeck; Morris Washington; Saroj K. Nayak; Dattatray J. Late
We report here the field emission studies of a layered WS2-RGO composite at the base pressure of ~1 × 10−8 mbar. The turn on field required to draw a field emission current density of 1 μA/cm2 is found to be 3.5, 2.3 and 2 V/μm for WS2, RGO and the WS2-RGO composite respectively. The enhanced field emission behavior observed for the WS2-RGO nanocomposite is attributed to a high field enhancement factor of 2978, which is associated with the surface protrusions of the single-to-few layer thick sheets of the nanocomposite. The highest current density of ~800 μA/cm2 is drawn at an applied field of 4.1 V/μm from a few layers of the WS2-RGO nanocomposite. Furthermore, first-principles density functional calculations suggest that the enhanced field emission may also be due to an overalp of the electronic structures of WS2 and RGO, where graphene-like states are dumped in the region of the WS2 fundamental gap.
Applied Physics Letters | 2014
Chandra Sekhar Rout; Padmashree D. Joshi; Ranjit V. Kashid; Dilip S. Joag; Mahendra A. More; Adam J. Simbeck; Morris Washington; Saroj K. Nayak; Dattatray J. Late
We report here our experimental investigations on p-doped graphene using tin sulfide (SnS2), which shows enhanced field emission properties. The turn on field required to draw an emission current density of 1 μA/cm2 is significantly low (almost half the value) for the SnS2/reduced graphene oxide (RGO) nanocomposite (2.65 V/μm) compared to pristine SnS2 (4.8 V/μm) nanosheets. The field enhancement factor β (∼3200 for the SnS2 and ∼3700 for SnS2/RGO composite) was calculated from Fowler-Nordheim (F-N) plots, which indicates that the emission is from the nanometric geometry of the emitter. The field emission current versus time plot shows overall good emission stability for the SnS2/RGO emitter. The magnitude of work function of SnS2 and a SnS2/graphene composite has been calculated from first principles density functional theory (DFT) and is found to be 6.89 eV and 5.42 eV, respectively. The DFT calculations clearly reveal that the enhanced field emission properties of SnS2/RGO are due to a substantial lowe...
Physical Review B | 2013
Adam J. Simbeck; Deyang Gu; Neerav Kharche; P. V. Satyam; Phaedon Avouris; Saroj K. Nayak
The electronic and magnetic properties of varying width, oxygen-functionalized armchair graphene nanoribbons (AGNRs) are investigated using first-principles density functional theory (DFT). Our study shows that O-passivation results in a rich geometrical environment which in turn determines the electronic and magnetic properties of the AGNR. For planar systems a degenerate magnetic ground state, arising from emptying of O lone-pair electrons, is reported. DFT predicts ribbons with ferromagnetic coupling to be metallic whereas antiferromagnetically coupled ribbons present three band gap families: one metallic and two semiconducting. Unlike hydrogen functionalized AGNRs, the oxygen functionalized ribbons can attain a lower energy configuration by adopting a non-planar geometry. The non-planar structures are non-magnetic and show three semiconducting families of band gap behavior. Quasiparticle corrections to the DFT results predict a widening of the band gaps for all planar and non-planar, semiconducting systems. This suggests that oxygen functionalization could be used to manipulate the electronic structures of AGNRs.
ACS Nano | 2012
Adam J. Simbeck; Nick Lanzillo; Neerav Kharche; Matthieu Verstraete; Saroj K. Nayak
Using a first-principles density functional method, we have studied the electronic structure, electron-phonon coupling, and quantum transport properties of atomic wires of Ag, Al, Au, and Cu. Non-equilibrium Greens function-based transport studies of finite atomic wires suggest that the conductivity of Al atomic wires is higher than that of Ag, Au, and Cu in contrast to the bulk where Al has the lowest conductivity among these systems. This is attributed to the higher number of eigenchannels in Al wires, which becomes the determining factor in the ballistic limit. On the basis of density functional perturbation theory, we find that the electron-phonon coupling constant of the Al atomic wire is lowest among the four metals studied, and more importantly, that the value is reduced by a factor of 50 compared to the bulk.
Applied Physics Letters | 2014
Satyajit Ratha; Adam J. Simbeck; Dattatray J. Late; Saroj K. Nayak; Chandra Sekhar Rout
We report high performance IR photocurrent response of two-dimensional hybrid materials consisting of layered WS2 nanosheets and reduced graphene oxide (RGO). Comparative photocurrent response studies of WS2 nanosheets, RGO, and WS2/RGO hybrids were carried out by performing current-voltage (I-V) and time-dependent current measurements with a laser excitation source having a wavelength of 808 nm. The experimental investigations indicate that WS2/RGO hybrids show negative photocurrent response, whereas WS2 and RGO show positive photocurrent response. The negative photocurrent response of the WS2/RGO hybrids is explained using a band alignment diagram and attributed to a charge transfer mechanism between WS2 and RGO. This analysis is further corroborated by first-principles density functional calculations. The fabricated device based on WS2/RGO hybrids shows a photosensitivity Rλ of about 6 AW−1 and a quantum efficiency η of ∼924%, which demonstrates high sensitivity of the hybrid material towards IR detect...
Journal of Physics: Condensed Matter | 2015
Nicholas A. Lanzillo; Adam J. Simbeck; Saroj K. Nayak
Surface Science | 2012
Adam J. Simbeck; Guoguang Qian; Saroj K. Nayak; G.-C. Wang; Kim M. Lewis
Computational Materials Science | 2016
Adam J. Simbeck; Nicholas A. Lanzillo; Neerav Kharche; Saroj K. Nayak
ACS Nano | 2015
Adam J. Simbeck; Nick Lanzillo; Neerav Kharche; Matthieu Verstraete; Saroj K. Nayak
Bulletin of the American Physical Society | 2014
Adam J. Simbeck; Saroj K. Nayak