scholarly journals Tunneling time and Hartman effect in a ferromagnetic graphene superlattice

AIP Advances ◽  
2012 ◽  
Vol 2 (1) ◽  
pp. 012123 ◽  
Author(s):  
Farhad Sattari ◽  
Edris Faizabadi
2012 ◽  
Vol 111 (9) ◽  
pp. 093724 ◽  
Author(s):  
Edris Faizabadi ◽  
Farhad Sattari

2010 ◽  
Vol 19 (11) ◽  
pp. 117305 ◽  
Author(s):  
Cheng Yin ◽  
Zhi-Jing Wu ◽  
Xian-Ping Wang ◽  
Jing-Jing Sun ◽  
Zhuang-Qi Cao

2019 ◽  
Vol 33 (12) ◽  
pp. 1950107 ◽  
Author(s):  
Natascha Riahi

We use the method of Laplace transformation to determine the dynamics of a wavepacket that passes a barrier by tunneling. We investigate the transmitted wavepacket and find that it can be resolved into a sequence of subsequent wave packages. This result sheds new light on the Hartman effect for the tunneling time and gives a possible explanation for an experimental result obtained by Spielmann et al.


2020 ◽  
Vol 34 (05) ◽  
pp. 2050026 ◽  
Author(s):  
Farhad Sattari ◽  
Soghra Mirershadi ◽  
Mohammad Hamdipour ◽  
Farshad Majidi

We theoretically study the spin-dependent group delay time through ferromagnetic bilayer graphene superlattice in the absence and presence of the bandgap. It is found that the group delay time depends on the spin degree of freedom and exhibits an oscillatory behavior with respect to the Fermi energy and barrier width. Furthermore, in the absence of the bandgap, the superluminal or Hartman effect exists only for the normal angle of incidence. Moreover, when bandgap value is large enough [Formula: see text], the Hartman effect can be observed for all angles of incidence. These results are contrary to the observed behavior for monolayer graphene superlattice.


2017 ◽  
Vol 31 (01) ◽  
pp. 1650250 ◽  
Author(s):  
Mohammad Esmailpour ◽  
Hakimeh Mohammadpour ◽  
Hamideh Hadavifar

The present paper investigates that the tunneling time for bilayer graphene potential barrier with monolayer graphene leads to all range of energy. Numerical results reveal that parameters such as the incident energy and angle plays a significant role in inducing of the Hartman effect. In contrast to single-layer graphene, in the bilayer graphene, due to the chirality of quasi-particles induction of Klein and Hartman effects occur in the normal incidence case. Moreover, it is demonstrated that even for energy levels above barrier, the Hartman effect is present.


2004 ◽  
Vol 70 (3) ◽  
Author(s):  
V. S. Olkhovsky ◽  
V. Petrillo ◽  
A. K. Zaichenko

1996 ◽  
Vol 32 (11) ◽  
pp. 1932-1936 ◽  
Author(s):  
D. Dragoman ◽  
M. Dragoman

2020 ◽  
Vol 59 (1) ◽  
pp. 243-251
Author(s):  
Josh Lofy ◽  
Vladimir Gasparian ◽  
Zhyrair Gevorkian ◽  
Esther Jódar

AbstractIn the present work, we study the rotations of the polarization of light propagating in right and left-handed films and layered structures. Through the use of complex values representing the rotations we analyze the transmission (Faraday effect) and reflections (Kerr effect) of light. It is shown that the real and imaginary parts of the complex angle of Faraday and Kerr rotations are odd and even functions for the refractive index n, respectively. In the thin film case with left-handed materials there are large resonant enhancements of the reflected Kerr angle that could be obtained experimentally. In the magnetic clock approach, used in the tunneling time problem, two characteristic time components are related to the real and imaginary portions of the complex Faraday rotation angle . The complex angle at the different propagation regimes through a finite stack of alternating right and left-handed materials is analyzed in detail. We found that, in spite of the fact that Re(θ) in the forbidden gap is almost zero, the Im(θ) changes drastically in both value and sign.


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