XPost: sci.physics.relativity   
   From: nospam@de-ster.demon.nl   
      
   Bill Sloman wrote:   
      
   > On 23/02/2026 8:38 am, J. J. Lodder wrote:   
   > > Bill Sloman wrote:   
   > >   
   > >> On 22/02/2026 9:25 pm, J. J. Lodder wrote:   
   > >>> Bill Sloman wrote:   
   > >>>   
   > >>>> On 21/02/2026 10:46 pm, J. J. Lodder wrote:   
   > >>>>> Bill Sloman wrote:   
   > >>>>>   
   > >>>>>> On 21/02/2026 5:52 am, Ross Finlayson wrote:   
   > >>>>>>> On 02/20/2026 10:31 AM, Bill Sloman wrote:   
   > >>>>>>>> On 21/02/2026 3:47 am, Ross Finlayson wrote:   
   > >>>>>>>>> On 02/19/2026 11:45 PM, Bill Sloman wrote:   
   > >>>>>>>>>> On 20/02/2026 10:48 am, Ross Finlayson wrote:   
   > >>>>>>>>>>> On 02/19/2026 11:19 AM, Bill Sloman wrote:   
   > >>>>>>>>>>>> On 20/02/2026 2:44 am, Ross Finlayson wrote:   
   > >>>>>>>>>>>>> On 02/19/2026 01:45 AM, Bill Sloman wrote:   
   > >>>>>>>>>>>>>> On 19/02/2026 6:13 am, Ross Finlayson wrote:   
   > >>>>>>>>>>>>>>> On 02/18/2026 11:06 AM, Ross Finlayson wrote:   
   > >>>>>>>>>>>>>>>> On 02/17/2026 08:35 PM, Bill Sloman wrote:   
   > >>>>>>>>>>>>>>>>> On 18/02/2026 5:37 am, Ross Finlayson wrote:   
   > >>>>>>>>>>>>>>>>>> On 02/17/2026 09:47 AM, Thomas 'PointedEars' Lahn wrote:   
   > >>>>>>>>>>>>>>>>>>> Ross Finlayson wrote:   
   > >>>>>>>>>>>>>>>>>>>> On 02/17/2026 03:49 AM, J. J. Lodder wrote:   
   > >>>>>>   
   > >>>>>>    
   > >>>>>>   
   > >>>>>>> I.e., mathematics _owes_ physics more and better mathematics   
   > >>>>>>> of continuity and infinity.   
   > >>>>>>   
   > >>>>>> Mathematics doesn't owe physics anything. Physics exploits tools   
   > >>>>>> developed by mathematicians, which makes physicists customers for the   
   > >>>>>> work of some mathematicians.   
   > >>>>>   
   > >>>>> That is quite arguable.   
   > >>>>> Much of mathematics wouldn't exist   
   > >>>>> without (what was once) new input from physics.   
   > >>>>> Many a luminary, Von Neumann for example,   
   > >>>>> has said that mathematics will go stale   
   > >>>>> without regular fresh input from the natural sciences,   
   > >>>>> bringing new needs.   
   > >>>>>   
   > >>>>>> A mathematical physicist like Paul Dirac is an interesting hybrid, but   
   > >>>>>> his biography is titled "The strangest man".   
   > >>>>>>   
   > >>>>>> https://en.wikipedia.org/wiki/Paul_Dirac   
   > >>>>>   
   > >>>>> Why discredit him by calling him 'a mathematical physicist'?   
   > >>>>> He was a theoretical physicist,   
   > >>>>   
   > >>>> He invented the Dirac function, and bra-ket notation. He was notably   
   > >>>> more deft with math than most of his contemporaries.   
   > >>>   
   > >>> Arguably. The real inventor was Oliver Heavidise.   
   > >>> (who loved to pester mathematicians with it)   
   > >>>   
   > >>> Dirac just gave it another, more elegant name. [1]   
   > >>> ( \delta(x) versus D H(x) or 1/2 D \signum(x) )   
   > >>>   
   > >>> And that 'most of' will depend on how wide you want to draw the circle.   
   > >>>   
   > >>>> https://en.wikipedia.org/wiki/Bra%E2%80%93ket_notation   
   > >>>   
   > >>> Nothing but notation. You can do without just as well.   
   > >>> Mathematicians object to it,   
   > >>> because the notation assumes without proof that adjoints exist.   
   > >>> (which often needs to be shown, by their standards)   
   > >>>   
   > >>>> He reconciled several ostensibly different quantum theories by pointing   
   > >>>> out that they were notational variations of the same basic idea.   
   > >>>   
   > >>> Yes. But imho his most important contribution   
   > >>> was getting quantum field theory started,   
   > >>   
   > >> "Quantum field theory" is just words to me.   
   > >   
   > > That is just too bad.   
   >   
   > I'm good at learning what I need to, and getting deep into quantum   
   > physics never turned out to be necessary.   
   >   
   > > All of physics is quantum field theory these days,   
   > > at least in principle.   
   > >   
   > >>> [1] Dirac was an electrotechnical engineer by training.   
   > >>> He must have known about Heaviside and his operational calculus.   
   > >>   
   > >> Perhaps. He did his first degree at Bristol in 1921, and went on to do a   
   > >> separate degree in math in 1923. Heaviside was a controversial figure,   
   > >> and might not have been much cited at Bristol back then.   
   > >   
   > > Being controversial leads to being well-know.   
   > > And Heaviside solved a number of fundamental problems   
   > > in electromagnetism, so any electrical engineer   
   > > must know about his work.   
   > >   
   > > Even Maxwell's equations are only known nowadays   
   > > in the form Heaviside gave them.   
   > > Some people even call them the Maxwell-Heaviside equations.   
   >   
   > Heaviside's version wasn't quite what Maxwell had originally produced.   
      
   Indeed, it was much better.   
   Maxwell was still stuck on potentials,   
   and his formulation was not properly gauge-invariant.   
   Heaviside's version, which focussed on the directly observable fields   
   made practicl applications much easier.   
   But Maxwell made the crucial step of identifying,   
   and adding the missing term.   
      
   > >> Looking at Heaviside's wikipedia page, I note that he was the first to   
   > >> use the impulse function (now known as the Dirac function). If Dirac had   
   > >> known much about Heaviside's work, he probably would have called it the   
   > >> Heaviside function when he first used it.   
   > >   
   > > 'Heaviside function' is already in use for the unit step function,   
   > > (don't know about when that name originated, guess well before Dirac)   
   >   
   > The Heaviside step function is just the integral of the Dirac function.   
   > If Dirac had known about it he'd probably have called the impulse   
   > function the derivative of the step function.   
      
   It is obvious that you have not seen Dirac's original work,   
   where he introduces the \delta-function.   
   He explicitly says there that introducing the \delta-function   
   as the derivative of the unit step function,   
   (which he calls the \epsilon-function)   
   is an alternative and equivalent way of introducing the \delta-function.   
   He doesn't mention Heaviside by name,   
      
   Jan   
      
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