Undergrad What Are Kets and Vectors in 3-D Representation?

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SUMMARY

Kets |x⟩ and |p⟩ are not traditional 3-D vectors; instead, they represent elements in an infinite-dimensional space. In the position representation, |x⟩ corresponds to the Dirac delta function δ_x, which is part of a function space rather than a numerical coordinate. The discussion clarifies that while |x⟩ and |p⟩ may appear to be vectors due to their labels, they are actually distributions within the dual space of a Schwartz space of smooth functions. This distinction is crucial for understanding quantum mechanics and the mathematical framework behind kets.

PREREQUISITES
  • Understanding of quantum mechanics terminology, specifically kets and Dirac notation.
  • Familiarity with infinite-dimensional spaces and function spaces.
  • Knowledge of the Dirac delta function and its properties.
  • Basic understanding of complex numbers and operations in quantum mechanics.
NEXT STEPS
  • Study the properties of the Dirac delta function and its applications in quantum mechanics.
  • Learn about Schwartz spaces and their role in functional analysis.
  • Explore the mathematical foundations of quantum mechanics, focusing on kets and operators.
  • Investigate the use of Pauli matrices in quantum mechanics and their implications for spin representation.
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This discussion is beneficial for physicists, mathematicians, and students of quantum mechanics who seek to deepen their understanding of kets, infinite-dimensional spaces, and the mathematical structures underlying quantum theory.

dyn
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Hi. I have read that when working in 3-D the following kets | x > and | p > are not vectors in 3-D. If that is correct what are they ? I know | ψ > is an abstract vector but I thought | x > and | p > would be 3-D vectors in the position and momentum representation ?
Thanks
 
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They are vectors in an infinite-dimensional space. It is natural to feel that ##|x\rangle## should be in a 3d space because ##x##, without the enclosing symbols, is a coordinate in 3D space. But ##|x\rangle## is not a coordinate or any other type of number. In the position representation it is the Dirac delta function ##\delta_x##, which is an element of a space of functions, which - like most function spaces - is infinite-dimensional.
 
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<a is conjugate of a>
<a|b> kind of dot(a.conjugate , b)
b><b|a> projection into other direction like b*dot(b.conjugate , a)

v2=pol><pol|v> is equivalent with this pseudo code
amp=dot(v,pol)
v2.x = pol.x*amp
v2.y = pol.y*amp

conjugate of V is V.imaginary=-V.imaginary
 
The Pauli matrices transform the 3d direction into 2d complex vector like spin.
 
Why do we need conjugation?
because there is a minus sign in real part of multiplication of complex numbers.

complex operator *(complex c)
{
complex e;
e.real = this->real*c.real - this->img*c.img;
e.img = this->img*c.real + this->real*c.img;
return e;
}
 
dyn said:
x > and | p > are not vectors in 3-D. If that is correct what are they ?
They are distributions, elements in the dual space of a Schwartz space of smooth functions. Only the labels are vectors in 3D.
 
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