'Massless' Electrons in Graphene

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Discussion Overview

The discussion centers on the behavior of electrons in graphene, particularly the concept of "massless" electrons and the implications of this behavior in terms of energy, work, and forces within the material. Participants explore theoretical aspects, potential applications, and the underlying physics of quasiparticles in graphene.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants interpret "massless" electrons in graphene as having "zero apparent mass" rather than zero actual mass, questioning the implications of this behavior.
  • There is a proposal that the massless behavior of electrons could suggest that work has been done on them, prompting inquiries about the source of this energy and what is performing the work.
  • One participant introduces the concept of quasiparticles, noting that electrons at the corners of the irreducible Brillouin zone behave like massless Dirac particles.
  • Another participant questions whether applying an electric field to a moving quasiparticle would result in a Newtonian type of force acting on the surrounding graphene, exploring the relationship between the quasiparticle's motion and the crystal structure.
  • There is a discussion about the asymmetrical movement of quasiparticles and whether this would exert a net directional force on the graphene when alternating between massless and non-massless motion.
  • A participant compares the behavior of quasiparticles in graphene to that of photons in a gravitational field, discussing momentum and energy changes under the influence of an electric field.

Areas of Agreement / Disagreement

Participants express various interpretations and hypotheses regarding the massless behavior of electrons in graphene, with no consensus reached on the implications of this behavior or the nature of forces involved.

Contextual Notes

The discussion includes assumptions about the definitions of mass and energy in the context of quasiparticles, as well as the effects of external fields on their behavior, which remain unresolved.

sanman
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So I've read that electrons traveling inside a sheet of graphene are said to travel "masslessly". I'm interpreting this as meaning "zero apparent mass" and not zero actual mass. Presumably, the graphene doesn't somehow weigh less than the sum of its constituent electrons and nuclei.

But given this extraordinary massless behavior by the electrons in the graphene, can it be said that work has been done on the electrons to make them behave this way? If so, then what is doing the work? Where is the energy coming from to cause this unusual behavior of the electrons?
 
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sanman said:
So I've read that electrons traveling inside a sheet of graphene are said to travel "masslessly". I'm interpreting this as meaning "zero apparent mass" and not zero actual mass. Presumably, the graphene doesn't somehow weigh less than the sum of its constituent electrons and nuclei.

But given this extraordinary massless behavior by the electrons in the graphene, can it be said that work has been done on the electrons to make them behave this way? If so, then what is doing the work? Where is the energy coming from to cause this unusual behavior of the electrons?
The electron in Graphene at the corners of the irreducible brillioun zone where Fermi surface lies behaves like massless Dirac particle. It does not refer to the massless of the electron but the quasiparticle.
 
Thank you for your reply.

So the quasi-particle exists inside the crystal(graphene), and can move masslessly.
But if I apply an electric field while it's moving, then it will move non-masslessly (ie. move in a way that exihibits mass)
In each of these cases, will the surrounding crystal(graphene) feel some action-reaction type of force in relation to the motion of the quasi-particle? Is there a Newtonian type of force that occurs in either of these cases?

Now suppose I arrange to have the quasi-particle move back and forth in the graphene, then it will do so masslessly.
But suppose I allow the quasi-particle to move masslessly in one direction, and then when it is returning back I apply the electric field so that it now moves in a way that exhibits mass.

Due to the asymmetry in this cycle (ie. moving masslessly in one direction, and then moving non-masslessly in the other direction) then is the surrounding crystal (graphene) feeling any net directional force on it?
 
sanman said:
So I've read that electrons traveling inside a sheet of graphene are said to travel "masslessly". I'm interpreting this as meaning "zero apparent mass" and not zero actual mass. Presumably, the graphene doesn't somehow weigh less than the sum of its constituent electrons and nuclei.

But given this extraordinary massless behavior by the electrons in the graphene, can it be said that work has been done on the electrons to make them behave this way? If so, then what is doing the work? Where is the energy coming from to cause this unusual behavior of the electrons?

Maybe, this could be of help: [PDF]The effective mass in graphene - Philip Hofmann
 
The absolute value ##v## of a (quasi-)electron in graphene near the Dirac point is constant (this velocity is not equal to the velocity of light c).
If an electric field acts on such an electron, its (quasi-)momentum will increase ##\dot{p} = -e E ##. Hence it's energy ##E=pv## will increase, too.
Compare this to the increase of a photon which enters a gravitational field. It's momentum and energy will also increase, but it's speed ##c## will remain constant, so that ##E=\hbar \nu =pc=\hbar k c##.
 
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