JFP:Originally Posted by johanfprins
You think that after you have published one manuscript which was written by you supervisor and got one citation (probably by somebody else who also studied under the same supervisor) you can teach me physics!
RC: How idiotic. The fact that you do not even know how to apply Gauss's law to the Cu-Fe_Cu sandwuch shows that you are incapable of learning physics.
It seems that you will never catch on: It is not about “knowing how” to apply Gauss’ law, but about whether one
can apply classical electrodynamics to a system that is modelled by Schroedinger’s many-body differential equation.
For a metal, the latter equation is solved under the assumption that during a steady-state, the negative and positive charges screen each other. When an Ohmic current flows through a circuit, you have such a steady-state at every cross-sectional area: Also a cross-sectional area between two different metals. Thus the change of electric-field across such an interface cannot be ascribed to an accumulation of charge-carriers within such an interface. An accumulation is only possible when the charge carriers cannot flow everywhere along the circuit with the same current I.
You remarks just make your ignorance of scientific publishing obvious.
Read the paper: Effect of localized spin fluctuations on transport properties in the one-band Wolff model
Who is the first author?
That still does not mean that you have been the primary brains behind the paper.
I wrote the paper together with my supervisor. I would guess that you got at least one paper form you thesis - can I assume that your supervisor wrote it since you do the same?
To some extent yes: After publishing two joint papers with my supervisor, I was definitely not so arrogant to claim that I am an expert in writing papers until after I have at least published my first solo paper; of which more than 60 then followed. I knew that there was still a hard slog ahead; and would definitely not have thought that I have the ability to “check” the “reality” of people who are obviously light years ahead of me. If I had stopped where you have stopped in publishing, I would have remained very-very humble.
It actually has been cited twice - and yes my supervisor was the sole author on one and a contributing author on another.
Will you give the names of the authors of the two papers who cited you?
JFP:
Originally Posted by johanfprins
I do not stop them: Nature stops them since, even while they transport a current, they remain at the lowest energy that they can be at: They have no energy to dissipate.
RC: That is ridiculus. They have kinetic energy (they are moving!) So they do have "energy to dissipate".
If they have energy that can dissipate, they
cannot transfer a superconducting current. READ MY MODEL on my website: The kinetic energy is supplied by quantum fluctuations and therefore it is not kinetic energy that can dissipate.
But that is not the question: johanfprins: How do you stop your charge-carriers from scattering?
JFP:
Originally Posted by johanfprins
The charge carriers within any conductor are NOT electrons.
RC: And once again: nothing to do with my question: johanfprins: What are your charge-carriers?
I have answered this many times AND it is on my website: Let me do it again: They are localised waves (orbitals) like those you find in an insulator after a metal-insulator transition.
The charge carriers within any conductor can be electrons.
Nope! An electron cannot have less energy than its rest mass energy m
e*c
2. The charge-carriers within a metal with work function W has an energy of m
e*c
2-W: This is less than the lowest energy an electron can have.
The charge carriers may also be electron holes, ions (e.g. electrolytes) or even protons (e.g. solid electrolytes).
Here you go overboard again. We are talking about metals for which Ohm’s law is valid. The charge-carriers are then negatively charged wave-packets (pseudo-electrons): NOT actual electrons.
JFP: In my model, the charge carriers within all superconductors are localised electron-states which have the lowest energy that they can have.
RC: That is idiotic: As you state - you now have an insulator!
Firstly you ask me what my charge-carriers are; and then you suddenly remember what they are: Why did you then ask in the first instance? Stop playing games! All superconductors
must first become insulators before they can super-conduct.
Why do you think the ceramics form a Mott-type insulator, with localised, anchored, electronic-orbitals, before they become superconducting at a lower temperature? The required charge-carriers are forming within this temperature interval (pseudogap), but their density is too low to super-conduct. By cooling further, their density increases until it is high enough for superconduction to occur. Owing to the different electronic energy spectrum in metals, the density of localised states is already high enough when the metal goes through the required metal-insulator transition, to transfer a superconducting current. Therefore, in this case, there is not a pseudogap as is measured in the case of the ceramics.
JFP: When the density of these localised states becomes high enough, they can exchange places by means of quantum fluctuations.
RC: Wow - mysterious "quantum fluctuations"!
But this sounds like vacuum fluctuations
Yes it does sound like “vacuum fluctuations”: The latter does not exist since the fluctuation in energy can only occur whithin a matter wave with mass-energy: Not without a matter wave being present.
which have their own problems for your idea (see below).
These “problems” are only within your mind.
Since the energy during a quantum fluctuation is used (to move on) and it then disappears, the charge-carriers have the same potential energy when they reach the target contact than the potential energy they have started off with from the injection contact.
Wrong: You now have "charge-carriers" within the superconductor that ignore any electric field.
Correct! This is exactly what you
MUST have in a superconductor, or else the charge-carriers will be accelerated to gain energy; which
demands that the potential energy at the injection contact and the ejection contact
MUST BE DIFFERENT: This means a non-zero voltage across the contacts an thus
NO SUPERCONDUCTION.
They go off in random directions., i.e. there is no current!
Not when you inject charge carriers at a contact. When you inject charge carriers, the energy of the total ensemble of charge-carriers increases, and therefore the ensemble must then eject charge-carriers at the other contact in order to keep the energy of the whole ensemble at the lowest level. This is the
ACTUAL reason why you have superconduction.
Let me try and explain it in simpler terms with the hope that you can grasp the situation: Assume that the superconducting phase is a black box so that we do not really know what is going on within it. What we know is that when we inject charge carriers into the box at an injection contact, an equal number of charge-carriers eject at the ejection contact having
THE SAME POTENTIAL ENERGY . This is obviously
NOT possible if the charge-carriers have been accelerated within the black box. Thus any mechanism required to model superconduction
MUST explain how the charge-carriers injected at the injection contact causes an equal amount of charge-carriers, which have the same potential energy, to be ejected at the other contact. This means no acceleration.
Really wrong: vacuum fluctuations create virtual particles.
Yes “vacuum-fluctuations” are themselves virtual: But even if you want to claim that quantum fluctuations are the same as “vacuum fluctuations”, then it still supports my model, since the energy they represent appears, to move the charge-carriers along, and then disappears: The potential energy of the charge-cvarriers thus remains the same and there is thus no increase in kinetic-energy which can dissipate as entropy. Exactly as it must be when you have superconduction.
Furthermore, if the ground-state energy of the superconducting phase must increase in order for a current to flow, the superconducting phase must be increasing its energy to be more than its ground-state energy. This means that it has gained energy that can dissipate: And the most important law of physics is that when you have energy that can dissipate
IT WILL DISSIPATE. When a current flows by dissipating energy, it cannot be a superconducting current
EVER. Simple high school physics my boy!
These can never be real particles unless energy is provided.
Exactly! This is why “these virtual particles” can supply the required energy and disappear before this energy decreases the potential energy and thus dissipates as entropy.
So your charge-carriers can never leave the superconductor. But currents do flow through superconductors!
When you inject charge-carriers at one contact, charge-carriers MUST eject at the other contact for the superconducting phase to maintain its lowest energy. Therefore a current will flow!
JFP:
Originally Posted by johanfprins
Nope! No matter whether the charge-carriers are fermions or bosons, if you can accelerate them, you create states into which the can scatter.
...snipped rant about acceleration...
RC: That is ignorant. The available states are created by the quantum system, not the ability to accelerate particles.
Now you suddenly want to remember that quantum mechanics plays a role. Why
now only, when you totally ignored this when you claimed that Gauss’ law, which is a classical law, can be applied to a quantum system? You are really hilariously funny.
Obviously, if there are not energy states within which the charge carriers can be accelerated, they will not accelerate. But you claim that they are being accelerated: Thus, in your model there must be such states and therefore the energy of your charge-carriers must increase when a current is flowing. This means that their potential energy must decrease on their way from the injection contact to the ejection contcat, and that they must dissipate the kinetic energy that they have gained: They can therefore not transfer a super-current. In fact in one of your previous posts you clearly stated that there are not such energy levels available for Cooper pairs, and now you claim that Cooper pairs are being accelerated, which mandates that there must be such energy levels available. Please make up your mind, and start to argue sense!