Is there a coordinate independent Dirac delta function?

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Discussion Overview

The discussion centers around the concept of the Dirac delta function and its potential coordinate-independent expressions, particularly in the context of curved spaces. Participants explore whether an intrinsic definition exists that does not rely on coordinates or metrics, and they examine related concepts such as the Dirac measure.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • Some participants question whether the Dirac delta function can be defined without reference to coordinates, suggesting that it may inherently require a coordinized space for its distribution.
  • One participant proposes that the Dirac delta could be viewed as the identity element for convolution, hinting at a potential coordinate-independent property.
  • Another participant introduces the concept of the Dirac measure, arguing that it is defined in terms of elements and sets rather than coordinates, and questions if this qualifies as a coordinate-independent form.
  • There is a discussion about the meaning of "coordinate free," with some suggesting that changing coordinates should not alter the expression of the Dirac delta.
  • Participants explore the implications of integrating the Dirac delta and whether its integral remains unchanged under coordinate transformations, raising the question of whether this could support a coordinate-independent definition.
  • Some participants note that while the Dirac measure can be integrated against certain functions, it may not behave the same way as a Schwartz distribution, leading to further questions about the nature of integration in this context.
  • There is a suggestion that one could sum over points in a manifold to derive properties of the Dirac delta, but this is met with skepticism regarding the triviality of such an approach.

Areas of Agreement / Disagreement

Participants express differing views on the existence and nature of a coordinate-independent Dirac delta function. The discussion remains unresolved, with multiple competing perspectives on the definitions and implications of the Dirac delta and Dirac measure.

Contextual Notes

Participants highlight the need for clarity in definitions, particularly regarding what constitutes a "coordinate free" expression. There are also discussions about the limitations of integrating measures and the conditions under which such integrations are valid.

friend
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I have been wondering exactly how one would express the Dirac delta in arbitrary spaces with curvature. And that leads me to ask if the Dirac delta function has a coordinate independent expression. Is there an intrinsic definition of a Dirac delta function free of coordinates and metrics? Or as a distribution does it inherently need a coordinized space on which to distribute its values? Thanks.
 
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The only possibility I can think of would be "Dirac is the identity element for convolution".
 
What about the Dirac measure? This is called a "measure", and any measure can be integrated, right? This Dirac delta measure is defined in terms of elements and sets and not on coordinates. So does this qualify as a coordinate independent form of the Dirac delta function? Or would the coordinate free expression have to be in terms of elements/points only and not sets?
 
friend said:
What about the Dirac measure? This is called a "measure", and any measure can be integrated, right? This Dirac delta measure is defined in terms of elements and sets and not on coordinates. So does this qualify as a coordinate independent form of the Dirac delta function? Or would the coordinate free expression have to be in terms of elements/points only and not sets?

It depends on what "coordinate free" means right? Normally we represent Dirac like
##\int_X f(t) \delta(t-a) dt = f(a)##
or something similar. The problem is we use coordinate systems to express "a" itself, so if you change the coordinate system you change how you write "a". So my interpretation of "coordinate free" would be "changing coordinates doesn't change the expression", at least in the context this question. If you meant something else well you'll need to define it.

Secondly, you wrote "any measure can be integrated". Well you mean "integrate with respect to the measure" not "integrate the measure itself". And yes there is a concept of "derivative of a measure" but it's very different.

Now does the Dirac measure satisfy the problem? Well that depends on whether you can pick an isolated point from a set without reference to a coordinate system (remember coordinate system is really just a systematic way of writing elements with respect to each other). Can you pick 0 without knowing where it is? And if you can do this, how is this any different to "normal" way we write Dirac?
 
pwsnafu said:
It depends on what "coordinate free" means right? Normally we represent Dirac like
##\int_X f(t) \delta(t-a) dt = f(a)##
or something similar. The problem is we use coordinate systems to express "a" itself, so if you change the coordinate system you change how you write "a". So my interpretation of "coordinate free" would be "changing coordinates doesn't change the expression", at least in the context this question. If you meant something else well you'll need to define it.
Let me turn this around and ask, if it can be proved that the integral of the dirac delta does not change its value or its appearance (a change of coordinates only changes the variable used in the integral, but otherwise stays the same), would that prove that there does exist a coordinate independent intrinsic definition of the dirac delta?

pwsnafu said:
Secondly, you wrote "any measure can be integrated". Well you mean "integrate with respect to the measure" not "integrate the measure itself". And yes there is a concept of "derivative of a measure" but it's very different.
Does the measure have to be integrated against a function of compact support? What about integrating against f(x)=1?

pwsnafu said:
Now does the Dirac measure satisfy the problem? Well that depends on whether you can pick an isolated point from a set without reference to a coordinate system (remember coordinate system is really just a systematic way of writing elements with respect to each other). Can you pick 0 without knowing where it is? And if you can do this, how is this any different to "normal" way we write Dirac?
I suppose you could do a formal sum over every point, p, in the set of your manifold, M, without referring to coordinate system. If you did this for every point in M, you'd get 1 for every p \in A \subset M for which δp(A)=1. Then Ʃpδp(A) would give you the size of A, right?
 
friend said:
Let me turn this around and ask, if it can be proved that the integral of the dirac delta does not change its value or its appearance (a change of coordinates only changes the variable used in the integral, but otherwise stays the same), would that prove that there does exist a coordinate independent intrinsic definition of the dirac delta?

You need to be more rigorous in what you want from "coordinate independent intrinsic definition". I say this because "Dirac is the identity element of the convolution" is a coordinate independent intrinsic definition. Proving that there really is a distribution that satisfies that definition is long and tedious (it uses a technique called "approximating the identity") but is doable.

As to your specific question, I guess so?

Does the measure have to be integrated against a function of compact support? What about integrating against f(x)=1?

Ah. First consider this: suppose we have a smooth function whose domain is ℝ, ##f\in C^\infty(\mathbb{R})##. Now is this function an element of ##C(0,\infty)##? Well it isn't because the domains are different, but we can take f and restrict it to the positives and that restriction is an element of ##C(0,\infty)##.

Same thing here. The Dirac as a measure can be integrated against f(x)=1, but the Dirac as a Schwartz distribution can't. Nonetheless, you can take the Dirac measure and restrict is to become a Schwartz measure.

I suppose you could do a formal sum over every point, p, in the set of your manifold, M, without referring to coordinate system. If you did this for every point in M, you'd get 1 for every p \in A \subset M for which δp(A)=1. Then Ʃpδp(A) would give you the size of A, right?

Yes, but in a trivial manner. p is always an element of A, so really you are just evaluating ##\sum_{p\in A}1##.

Edit: Oh wait you're summing over ##p \in M##? Then that means M is countable.
 

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