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Search for "dopants" in Full Text gives 83 result(s) in Beilstein Journal of Nanotechnology.
Tensile properties of a boron/nitrogen-doped carbon nanotube–graphene hybrid structure
Beilstein J. Nanotechnol. 2014, 5, 329–336, doi:10.3762/bjnano.5.37
- with different dopants. It is found that with the presence of dopants, the hybrid structures usually exhibit lower yield strength, Young’s modulus, and earlier yielding compared to that of a pristine hybrid structure. For dopant concentrations below 2.5% no significant reduction of Young’s modulus or
- impact of dopant atoms on the mechanical properties of graphene. Huge efforts are still lying ahead especially for the newly synthesized CNT–graphene hybrid structure. Therefore, in this work, we will examine the impact of different densities and species of dopants on the tensile properties of the GNHS
- . The emphasis will be placed on Young’s modulus, E, yield strength, YS, and yield strain, YP. Computational details In order to acquire the influence of the dopants on the mechanical properties of GNHSs, the large-scale atomic/molecular massively parallel simulator (LAMMPS) [17] is utilized to carry
En route to controlled catalytic CVD synthesis of densely packed and vertically aligned nitrogen-doped carbon nanotube arrays
Beilstein J. Nanotechnol. 2014, 5, 219–233, doi:10.3762/bjnano.5.24
- ] atoms has been frequently used to enhance or tune their physicochemical properties. Among the elemental dopants, nitrogen emerges as of particular interest in electronics since N-CNTs should be characterized by a higher electrical conductivity (n-doping). Consequently, the significance of N-CNTs in a
Ferromagnetic behaviour of Fe-doped ZnO nanograined films
Beilstein J. Nanotechnol. 2013, 4, 361–369, doi:10.3762/bjnano.4.42
- cobalt demonstrates only one oxidation state Co3+ whereas manganese can possess several oxidation states, namely +2, +3 and +4 [17][18]. Together with cobalt and manganese, iron is one of the most important dopants in ZnO. Similar to manganese, iron has different oxidation states (Fe2+ and Fe3+). This
- solubility of Fe-doped ZnO are now in progress; they give comparable results and will be published elsewhere. Simple calculations performed in [4][5] showed that the drastic increase of the total solubility of Co and Mn with decreasing grain size is due to the multilayer adsorption of dopants in GBs (up to
High-resolution electrical and chemical characterization of nm-scale organic and inorganic devices
Beilstein J. Nanotechnol. 2013, 4, 318–319, doi:10.3762/bjnano.4.35
- , threading dislocations, and microtwins that affect the diffusion of dopants and the material mobility (due to scattering). When growth is performed in narrow trenches, dislocations are trapped within the confined volume (aspect-ratio trapping) and, theoretically, defect-free layers can be obtained. However
Influence of diffusion on space-charge-limited current measurements in organic semiconductors
Beilstein J. Nanotechnol. 2013, 4, 180–188, doi:10.3762/bjnano.4.18
- will focus on acceptor-like traps in electron-only devices, i.e., situations where the traps are negatively charged when below the Fermi level. These negative charges will behave like p-type dopants and create a barrier for electrons. The electrons first have to diffuse over the barrier created by the
- an electron. The rationale of using acceptor-like defects is that many organic semiconductors are known to be p-type, i.e., to have acceptor like defects, and to show improved transport after compensation of the p-type dopants with n-type dopants [8][23][26][37][38]. Because organic semiconductors
Diamond nanophotonics
Beilstein J. Nanotechnol. 2012, 3, 895–908, doi:10.3762/bjnano.3.100
- small reaction volume is that neither the reactor base plate nor the quartz walls of the surrounding bell jar is touched by the plasma. Major contaminations from the reactor walls were therefore avoided. Gaseous nickel and tungsten precursors - The controlled and targeted addition of dopants during
The memory effect of nanoscale memristors investigated by conducting scanning probe microscopy methods
Beilstein J. Nanotechnol. 2012, 3, 722–730, doi:10.3762/bjnano.3.82
- thickness of the film, RON and ROFF correspond to the resistance of the memristor for completely uniformly doped or undoped cases, respectively, and µ is the drift velocity of the dopants under an electric field E across the doped region in the presence of a current I(t). The switching characteristic
- –sample contact is a factor of ~20 larger than that in region of the film closer to the substrate interface [6]. The influence of a nonuniform electric field significantly suppresses the drift of the dopants. Nonlinear dopant drift can be taken into account in the memristor simulation I–V curve by
Synthesis and electrical characterization of intrinsic and in situ doped Si nanowires using a novel precursor
Beilstein J. Nanotechnol. 2012, 3, 564–569, doi:10.3762/bjnano.3.65
- adding HCl to the growth atmosphere [18]. For such VLS grown NW dopants can be introduced either through particular catalyst particles, such as In [19], Al [20] or Ga [21], which become partly incorporated into the NW during growth and thus work as p-type dopants themselves, or by adding a small amount
- . Such epitaxial NWs grow preferentially along the [112] direction, like their B-doped counterparts. The NWs themselves are rod-like, exhibit good crystallinity, and feature no observable defects or stacking faults. To test the activation of the dopants in the NWs, electrical characterization was
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