Quantized Alternate Current on Curved Graphene
Round 1
Reviewer 1 Report
This is an excellent manuscript worthy of publication. The authors get to the salient points, make them clearly and make no attempt to obfuscate the methods employed to arrive at their results. I do not know of any other work that has employed QRWs to curved graphene. I am much less familiar with the computational scheme used to calculate the center of charge results, but the authors do a good job of laying out the procedure to the point where a patient reader could implement the method his or herself without undue difficulty.
A few minor issues may be worthy of consideration:
In several sentences in the manuscript statement, there should not be a comma’s preceding the reference bracket; please bear in mind this may be a stylistic convention and may not be followed in the first language of the authors. In any case, the ‘rule’ is not applied uniformly throughout the work.
I would ask that the authors clarify via reference to a textbook, which convention they have chosen for their verbeins. It appears they have chosen one that appears in Kaku’s Quantum Field Theory text, but I cannot verify my memory is accurate; I am not in a location that allows me to check.
Finally, I believe this statement needs further elaboration:
“The frequency of these Bloch-like oscillations is quantized according to η. Finally, as the center103 of mass density is equivalent to a driven oscillating current, the system might be implemented as a104 periodic, quantized oscillating current device.”
It’s not immediately clear to me why the COMD is equivalent to a driven current if no voltage source is there for which a comparison could be drawn.
Author Response
a ) This is an excellent manuscript worthy of publication. The authors get to the salient
points, make them clearly and make no attempt to obfuscate the methods employed
to arrive at their results. I do not know of any other work that has employed QRWs
to curved graphene. I am much less familiar with the computational scheme used to
calculate the center of charge results, but the authors do a good job of laying out the
procedure to the point where a patient reader could implement the method his or herself
without undue difficulty.
A few minor issues may be worthy of consideration:
In several sentences in the manuscript statement, there should not be a commas preceding
the reference bracket; please bear in mind this may be a stylistic convention and may
not be followed in the first language of the authors. In any case, the rule is not applied
uniformly throughout the work.
We thank the referee for this comment. The commas have been accordingly removed
in the revised manuscript.
b ) I would ask that the authors clarify via reference to a textbook, which convention they
have chosen for their verbeins. It appears they have chosen one that appears in Kakus
Quantum Field Theory text, but I cannot verify my memory is accurate; I am not in a
location that allows me to check.
We apologize for neglecting this reference, we have added the following reference in the
manuscript:
”[35] M. Kaku,Quantum Field Theory: A Modern Introduction. Oxford University
Press, 1993.”
c ) Finally, I believe this statement needs further elaboration:
The frequency of these Bloch-like oscillations is quantized according to . Finally, as the
center103 of mass density is equivalent to a driven oscillating current, the system might
be implemented as a104 periodic, quantized oscillating current device.
Its not immediately clear to me why the COMD is equivalent to a driven current if no
voltage source is there for which a comparison could be drawn.
We thank the referee for this excellent remark. The conclusion was indeed poorly
justified. We have added the following:
”Finally, some forward moving charge,even if driven, will experience an equivalent
transverse oscillating motion, therefore the system might be implemented as a periodic,
quantized oscillating current device.”
Author Response File: Author Response.pdf
Reviewer 2 Report
See report
Comments for author File: Comments.pdf
Author Response
a ) REFEREES REPORT ON THE MANUSCRIPT ENTITLED: QUANTIZED ALTER-
NATE CURRENT ON CURVED GRAPHENE BY K. FLOURIS, S. SUCCI, AND H. J.
HERRMANN SUBMITTED TO CONDENSED MATTER REF. CONDENSEDMATTER-
469937
In their submitted paper, the authors propose the generation of a quantized oscillating
current on curved graphene by introducing and numerically solving a Dirac equation in
curved space. They also consider a set of semi-classical equations of motion, relating
Berry to real space curvature.They have in view applications in conjunction with trapped
fermions for the realization of quantum cellular automata. The authors claim that
The Dirac equation in curved space describes quantum relativistic Dirac particles (e.g.
electrons ) moving on arbitrary manifold trajectories. I think that such a statement is
rather audacious. What is the physical meaning of the mass term appearing in such
(respectable, of course) mathematical generalisations? The physical foundations of the
original Dirac equations for massive spin 1/2 particles derive from Poincare Wigner
symmetry requirements for Physics in flat Minkowskian space-time, for which the mass
term is the invariant rest mass of the particle. I invite the authors to support their
statement with sound explanations and physical justifications.
We thank the referee for this excellent comment. The following has been added the
manuscript to clarify and justify the comment.
”The covariant derivative ensures the independence of the Dirac equation of the coordinate basis. The covariance is satisfied by the connection coefficients which can be
interpreted physically as a vector potential. The Poincare symmetries are obeyed by
the Dirac equation ensuring the special relativistic nature of the wavefunctions. The
mass term represents the Minkowski metric invariant rest mass. Interactions add to
an effective mass by the very definition of covariant derivative, which places the vector
potential on the same mathematical basis as a physical mass. Graphene is modeled by
a mass-less Dirac Hamiltonian.”
b ) Besides this point, one can understand that the use of Dirac equation in curved space
time in the case of Graphene is justified from the similar forms of Hamiltonians (5) and
(6).
Moreover, the content is correct, well motivated, illustrated and documented. Particu-
larly interesting is the authors interpretation of their result as a geometrical analogue of
the Bloch oscillations, Just a typo: Page 1, line 15, Ahronov
The typo was corrected.
Author Response File: Author Response.pdf