Massless fermions Klein tunneling

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Discussion Overview

The discussion revolves around the phenomenon of Klein tunneling as it pertains to massless fermions in graphene, exploring the implications of this tunneling behavior, the nature of quasiparticles, and the conditions under which tunneling occurs. Participants examine theoretical and experimental aspects, including potential barriers and the characteristics of tunneling in different media.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • Some participants note that Klein tunneling allows quasiparticles in graphene to tunnel through energy barriers regardless of their width and height, raising questions about the feasibility of creating a graphene tunnel diode over large distances.
  • Others clarify that it is not the electrons themselves that are tunneling, but rather the quasiparticles that represent collective electron behavior, and that the potential barriers involved are specifically electrical in nature.
  • Some participants express uncertainty about whether quasiparticles can tunnel through dielectric barriers in the same manner as through electric barriers, suggesting that classical tunneling properties may apply in those cases.
  • A few participants assert that Klein tunneling is not applicable to quasiparticles in the absence of a specific medium, such as graphene, and that traditional tunneling behavior would dominate in vacuum or air.
  • There is a discussion about the potential for quasiparticles to carry energy or information during tunneling and whether air could serve as a dielectric medium.
  • Some participants reference experimental results involving tunneling through thin dielectric barriers, questioning how this aligns with the theoretical framework of Klein tunneling.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the nature of tunneling in graphene, the role of quasiparticles versus electrons, and the conditions under which Klein tunneling can occur. The discussion remains unresolved on several key points, particularly regarding the applicability of Klein tunneling to different types of barriers.

Contextual Notes

Participants highlight limitations in understanding the conditions necessary for Klein tunneling, including the dependence on specific media and the nature of potential barriers. There is also mention of unresolved mathematical steps and the need for further clarification on the behavior of quasiparticles in various contexts.

Stanley514
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QUOTE:
"In 1929, physicist Oskar Klein[1] obtained a surprising result by applying the Dirac equation to the familiar problem of electron scattering from a potential barrier. In nonrelativistic quantum mechanics, electron tunneling into a barrier is observed, with exponential damping. However, Klein’s result showed that if the potential is of the order of the electron mass, [PLAIN]https://upload.wikimedia.org/math/5/e/a/5ead404e0410a13fa323d3e8de6b2ced.png, the barrier is nearly transparent. Moreover, as the potential approaches infinity, the reflection diminishes and the electron is always transmitted."

These results were expanded to higher dimensions, and to other types of potentials, such as a linear step, a square barrier, etc. Many experiments in electron transport in graphene rely on the Klein paradox for massless particles.

https://en.wikipedia.org/wiki/Klein_paradox

QUOTE:
However, the Dirac electrons found in graphene can tunnel through energy barriers regardless of their width and energy height; a phenomenon called Klein tunneling, described theoretically for 3D massive Dirac electrons by the Swedish physicist Oskar Klein in 1929. Graphene was the first material in which Klein tunneling was observed experimentally, as massive Dirac electrons required energy barriers too large to be observed.

http://www.springer.com/about+springer/media/springer+select?SGWID=0-11001-6-1292222-0
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QUESTION:
If electrons in graphene can tunnel throug energy barriers regardless of their width and energy height, does it mean they could tunnel through any distance? So, we could make a graphene tunnel diode with 1 km distance between cathode and anode and an empty space (air) in between?
 
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Your springer link has incorrect wording (for some reason). It's not electrons that are tunneling, but quasiparticles in graphene (of which, of course, electrons are the physical substratum, but electrons aren't actually tunneling). The potential barrier also is of an electrical nature, not just "any" barrier::http://arxiv.org/abs/cond-mat/0604323 "Such a barrier can be created by the electric field effect using a thin insulator or by local chemical doping".
 
ddd123 said:
Your springer link has incorrect wording (for some reason). It's not electrons that are tunneling, but quasiparticles in graphene (of which, of course, electrons are the physical substratum, but electrons aren't actually tunneling). The potential barrier also is of an electrical nature, not just "any" barrier::http://arxiv.org/abs/cond-mat/0604323 "Such a barrier can be created by the electric field effect using a thin insulator or by local chemical doping".
They claim they created graphene tunneling diode with very thing layer of dielectric between graphene sheets.

http://www.researchgate.net/publication/260520206_High_performance_vertical_tunneling_diodes_using_graphenehexagonal_boron_nitridegraphene_hetero-structure

If electrons tunnel through dielectric, does it mean they do actually tunnel through, as you said? And if yes, then their unusual properties apply only to tunneling through electric barrier, but when they tunnel through dielectric, classical tunneling properties stay in the force?
 
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Again, the electrons aren't tunneling, the graphene quasiparticles resulting from the collective behavior of the electrons are tunneling. If actual electrons were to tunnel, then the non-relativistic way of tunneling with exponential dampening of the amplitude applies, but it's most likely irrelevant to that article if the purpose is Klein tunneling.
 
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ddd123 said:
Again, the electrons aren't tunneling, the graphene quasiparticles resulting from the collective behavior of the electrons are tunneling. If actual electrons were to tunnel, then the non-relativistic way of tunneling with exponential dampening of the amplitude applies, but it's most likely irrelevant to that article if the purpose is Klein tunneling.
So, graphene quasiparticles could tunnel through any kind of electric barrier (electric field?), but through dielectric barrier they tunnel on very small distance only, like regular tunneling particles?
 
I think the quasiparticles also tunnel Klein-like through the dielectric barrier (not sure, the abstract isn't very clear). It's just the electrons that tunnel normally.
 
ddd123 said:
I think the quasiparticles also tunnel Klein-like through the dielectric barrier (not sure, the abstract isn't very clear). It's just the electrons that tunnel normally.
1) Could this quasiparticles carry energy or information while they tunnel?
2) Could you use just an empty air as a dielectric (in principle)?
3) If they Klain-tunneling through a dielectric barrier, what maximal thickness of such barrier could be acheived?
 
The answer to 1) is yes. The Dirac theory predicts 2) - yes; 3) - infinite. But graphene is a realistic case, it's probably different. You should ask in the atomic and solid state subforum.
 
The (quasi-)electrons in graphene behave like 2D Dirac particles. However, the arrangement they are talking about in this article is a 3D structure. So that's certainly not Klein tunneling.Furthermore, you certainly can't use a dielectric barrier. Rather, the barrier has to be "vacuum like", i.e. graphene like in our case , up to some applied electric potential.

In graphene, the electrons only behave Dirac like in a small energy band around the Dirac point. This limits the height of the barrier. So there will be no complete transmission.
 
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  • #10
So, Klein tunneling (of electrons or charged quasiparticles) through the air is not possible under any practical conditions?
This one article mentions Photonic Klein tunneling through a dielectric slab.
http://arxiv.org/pdf/1101.3519.pdf

And if it would be possible, what distance could we achieve?

If common tunneling of electrons through dielectric barrier is possible, then why Klain tunneling of either electrons or quasi-particles is impossible?
 
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  • #11
Klein tunnelling is possible for electrons through air (or even better vacuum), but not for quasi-particles for the simple reason that the definition of a quasi particle requires a specific medium (like graphene). No specific medium, no quasi-particles, hence also no tunnelling of quasi particles through no medium (=vacuum).
 
  • #12
DrDu said:
Klein tunnelling is possible for electrons through air (or even better vacuum), but not for quasi-particles for the simple reason that the definition of a quasi particle requires a specific medium (like graphene). No specific medium, no quasi-particles, hence also no tunnelling of quasi particles through no medium (=vacuum).
But they claim created graphene tunneling diode in which quasiparticles(?) tunnel through dielectric barrier (just few atoms thick). How do you explain that?

QUOTE:
Here we report resonant tunnelling of Dirac fermions through a boron nitride barrier, a few atomic layers thick, sandwiched between two graphene electrodes.
http://www.nature.com/ncomms/journal/v4/n4/full/ncomms2817.html
 

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