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Beilstein J. Nanotechnol. 2013, 4, 103–110, doi:10.3762/bjnano.4.12
Figure 1: (a) Smooth ripple-like structure where the first and last six rows of carbon-dimers are surface-cla...
Figure 2: Calculated reaction barriers for hydrogenation of bent graphene as a function of the local radius o...
Figure 3: Electronic transmission through a single kink normalised by the transmission of pristine graphene (T...
Figure 4: (Left) Band structures for H-passivated armchair ribbons with varying width, N. The ribbons are a z...
Figure 5: Projected band structure and transmission through structures with multiple kinks. The top (section S...
Beilstein J. Nanotechnol. 2011, 2, 814–823, doi:10.3762/bjnano.2.90
Figure 1: The system considered in the present study is a four-atom carbon chain bridging two graphene electr...
Figure 2: Current–Voltage (I−Vb) curves at different Vg.
Figure 3: (a) Motion of the two phonon modes around 200 meV. (b) Motion of the runaway mode at Vg = 0.6 V, an...
Figure 4: (a) Inverse Q-factor (1/Q) as a function of gate voltage, Vg, at Vb = 1 V for the two modes around ...
Figure 5: (a) Effective phonon number (N) for the two phonon modes around 200 meV as a function of gate volta...
Figure 6: (a) Definition of the system regions with different types of noise contributions. Leads (L,R) have ...