Constantinos,
let me try once again, hopefully this time with more success:
1) It seems that either "integrable" is synonymous to "continuous on closed intervals" in your essay/papers, or you questioning some well known mathematical results. As I wrote, only the general statements involving "any integrable function" are problematic. If still in doubt, then consult a reasonable calculus handbook or ask a friendly mathematician.
2) Well, just try the same with the Fermi-Dirac distribution, with the Ansatz E(t)=E0e-rt and apropriate "fit", this time fitting for -rt, and voila, you have it!
But it is only "the art of fitting", nothing more.
You skipped my point 3), does it mean that you agree with me here ?
In the following 3) below refers to my point 4), and so on.
3) "Mathematical truth" refers to formal constructions, developed in an axiomatical/deductive way, while "physical truth" reflects the knowledge gained from experiments. In theoretical physics, mathematical methods are used to model the "physical truth", maybe with predictive results, but nothing more. Even the most elegant results have to be rejected if not confirmed experimentally. Sure, Pythagorean theorem may be used to measure distances, but this theorem does not impose that the physical space is Euclidean!
4) You wrote "What rules am I changing ?" Let me cite your answer on the pointed out contradiction:"Perhaps the mathematical limit enforces that \eta= 0. But since we cannot measure in physics below the threshold h, we have for all experimental purposes the mathematical limit produces once again Planck's Law"
It seems that you simply ignore the results that are inconvenient.
5) The blackbody radiation is a property of the blackbody, therefore in a sense "blackbody radiates because it is a blackbody" as I wrote in my previous posting in a somewhat strange-looking wording.
If you determine the radiation spectrum of some object, and it can be identified as blackbody spectrum corresponding to a definite temperature T, then this object is identified as a blackbody heated to the temperature T.
It seems that you ignored the rest of my point 6) ? Because I think it is important, let me repeat it below:
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The measurement of the blackbody radiation is another story, and if we want to measure the radiation itself, we have to eliminate somehow the detector influence, usually through proper setup and calibration. The detector radiates too !
The model presented in your essay tries to describe the interaction between the radiating blackbody and a detector working in a very specific way and it is at the same time claimed that it reflects exactly the radiating blackbody. This is a wrong approach in my opinion, although it may lead to a correct formula. The Ansatz for E(t) (I mean here the formula itself) does not allow for a differentiation between the "source" and the "sensor".
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In other words, a blackbody radiates in approximately the same way when measured or not. Just imagine a device for remote temperature measurement, do you think that the temperature of the measured object is as indicated on the device only during the measurement ? And what when the device is broken ?
6) Although I agree with your statement about Torah, I'm still confused by the contradicting statements about \eta, see below
7) You wrote: "I left eta as an undefined quantity in my essay. Thus, all the results I have listed are purely mathematical and very general."
Pardon me, but it is simply impossible to derive _any_ results for an undefined quantity. Or I'm missing something important here ? Maybe you mean the physical interpretation of \eta, not the definition ?
Any mathematical construction needs a non-contradictory set of axioms, definitions, etc., otherwise it is _not_ mathematics for sure.
You wrote also: "Perhaps you can do more ..." Maybe, but I'll definitely start from checking the present status of such approaches, look for similarities, etc. One could waste a lot of time trying to crack open doors!
Best regards,
-Joachim.