Can Stone-Weierstrass Theorem Solve Quantum Physics Equations?

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In summary, the conversation discusses the use of Stone-Weierstrass theorem to solve problems with quantum physics, specifically using the Fourier transform and series expansions. The theorem has three main conditions and involves finding coefficients and a dot product to yield sines. It is also mentioned that this is a standard way to prove the density of polynomials and trigonometric polynomials in continuous functions on a compact interval. The discussion also touches on the construction of compactifications for non-compact spaces.
  • #1
mplltt
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This has something to do with all of physics and particularly equations used to solve problems with quantum physics.

I need to solve this using Stone-Weierstrauss theorem for {sin(nx)} (n=1 to infinity) over the interval (0,pi/2)

This involves the Fourier transform which would solve the series expansion starting with a0, am, & bm. This involves the use of a0=1/(2pi) INT(f(x))dx from (0,pi/2) and am=1/pi <cos(mx), f(x)> = 1/pi INT(f(x)*cos(mx))dx and bm=1/pi<sin(mx), f(x)> =1/pi INT(f(x)*sin(mx))dx. This is the dot product of the trig function and the function in L^2.

The Stone-Weierstrauss uses three main conditions:
1) All x,y are in [a,b] there exists n,s,t Phi(sub n)(x) does not equal Phi(sub n)(y)
2) Phi(sub n)(x)*Phi(sub m)(x) = sum of Gamma(sub n)*Phi(sub n)(x) =1
3) "closed under multiplication." all n,m exists {Gnu(sub j)^(n,m)} (j=0-infinity) such that Phi(sub m)(x)*Phi(sub n)(x) = Sum of Gnu(sub j)*Phi(sub j)(x)

Phi(sub j)(x) is in this case {sin(nx)}(n=1 to inifinity)

-M
 
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  • #2
Sorry but I can't make heads or tales of this.
 
  • #3
He *might* be trying to say that he wants to prove that any function can be aproximated by a sum of the form

[tex]\sum a_n\sin (nx) [/tex]

Using Stone-Weierstrass. Just a guess though.
 
  • #4
I concur.

There appears to be no question or problem in the OP's post.
 
  • #5
some ways to help

The Stone-Weierstrauss uses three main conditions:
1) All x are in [a,b] there exists n,s,t Psi(sub n)(x) does not equal Psi(sub n)(y)
2) Psi(sub n)(x)*Psi(sub m)(x) = sum of Gamma(sub n)*Psi(sub n)(x) =1
3) "closed under multiplication." all n,m exists {Gnu(sub j)^(n,m)} (j=0-infinity) such that Psi(sub m)(x)*Psi(sub n)(x) = Sum of Gnu(sub j)*Psi(sub j)(x)

Psi(sub j)(x) is in this case {sin(nx)}(n=1 to inifinity)

So my question is I want to find Gamma as a coefficient to Psi=sin(nx) =1 for all n. [as per 2)]

The next question to this is that I would like to find a sufficient dot product of <Psi(nx), Psi(mx)> that will yield sines. [as per 3)]

-M
 
  • #6
here is a relevant theorem that will only be intelligible to a somewhat sophisticated reader: A compactification of a (completely regular) space, corresponds to a subalgebra (condition 3)) of the algebra of continuous functions, which is constant containing, point separating (condition 1)) and closed under uniform limits.

this si not precise but neither is the question posed. this is a o convergenve theorem. poresuymably the compactification is the closure or one point closure of the given interval. the poster may not comprehend this, but it is relevant as someone may see.
 
  • #7
i think you are right deadwolfe, as perhaps the stone weierstrass he is thikning of is a set of criteria (popint separating and constant containing) for an algebra of functions to be uniformly dense in the algebra of continuous functions on a given space.

this is a standard way to prove that polynomials and trig polynomials are dense in the continuous functions on a compact interval.


If the space involved is not compact, the discussion I was giving relates to constructing various compactifications from similar considerations.
 
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  • #8
weierstrass, not strauss.
 

FAQ: Can Stone-Weierstrass Theorem Solve Quantum Physics Equations?

What is the Stone-Weierstraus theorem?

The Stone-Weierstraus theorem is a fundamental mathematical result in functional analysis that states any continuous function on a compact interval can be approximated by a polynomial. This means that a polynomial function can be used to closely approximate any continuous function on a compact interval.

What is the significance of the Stone-Weierstraus theorem?

The Stone-Weierstraus theorem is significant because it provides a powerful tool for approximating functions. It is used in many areas of mathematics and science, including physics, engineering, and economics, to name a few. It also has important implications in the theory of Fourier series and the theory of Banach spaces.

What is a compact interval?

A compact interval is a closed and bounded interval on the real number line. It can be defined as a set of numbers between a minimum and maximum value, including those values. For example, the interval [0,1] is a compact interval, while the interval (0,1) is not, because it does not include its boundary points.

What does it mean for a function to be continuous?

A function is continuous if it has no sudden jumps or breaks, and it can be drawn without lifting the pen from the paper. More formally, a function is continuous if the limit of the function at a given point is equal to the value of the function at that point. In other words, small changes in the input produce small changes in the output.

Can the Stone-Weierstraus theorem be generalized to other spaces?

Yes, the Stone-Weierstraus theorem can be generalized to other spaces, such as metric spaces, topological spaces, and normed vector spaces. In fact, there are several variations of the theorem, each with its own conditions and implications. However, the original theorem deals with functions on compact intervals, and it is one of the most well-known and widely used versions.

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