Shape defined by x∈ℂ^3 and x⋅x = 0.

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In summary: So a spinor is just a vector that represents a point in ℂ3, and a particular spinor representation is just a particular vector that represents the same point.In summary, a spinor is a vector that represents a point in ℂ3, and a particular spinor representation is just a particular vector that represents the same point.
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Shape defined by x∈ℂ^3 and x⋅x = 0.

From, http://www.sjsu.edu/faculty/watkins/spinor.htm

"The concept of spinor is now important in theoretical physics but it is a difficult topic to gain acquaintance with. Spinors were defined by Elie Cartan, the French mathematician, in terms of three dimensional vectors whose components are complex. The vectors which are of interest are the ones such that their dot product with themselves is zero.

Let X=(x1, x2, x3) be an element of the vector space C^3. The dot product of X with itself, X·X, is x1x1+x2x2+x3x3. Note that if x=a+ib then x·x=x^2=a^2+b^2 + i(2ab), rather that a^2+b^2, which is x times the conjugate of x.

A vector X is said to be isotropic if X·X=0. Isotropic vectors could be said to be orthogonal to themselves, but that terminology causes mental distress.

It can be shown that the set of isotropic vectors in C3 form a two dimensional surface."

Are there some simple ways to try and understand a bit about the shape of this surface?
 
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Spinnor said:
Let X=(x1, x2, x3) be an element of the vector space C^3. The dot product of X with itself, X·X, is x1x1+x2x2+x3x3. Note that if x=a+ib then x·x=x^2=a^2+b^2 + i(2ab), rather that a^2+b^2, which is x times the conjugate of x.
Since a and b are real, the above requires that every coordinate of a point in the set ##\{X\in\mathbb{C}^3 | X \cdot X=0\}## is zero. So the set is simply the origin of ##\mathbb{C}^3##.

When I went web-searching for isotropic vectors I didn't come up with any definition for them except for the thread you posted here in 2009 asking about the same topic.

'Isotropic' is a term that can be applied to bilinear forms. Metrics in spacetime are isotropic in that sense. In that context, we can call null vectors, which are lightlike vectors, isotropic.

But the standard metric on ##\mathbb{C}^3## that you have described above is not isotropic, so the set of all isotropic vectors in ##\mathbb{C}^3## with that metric is just the zero vector. There is no 2D surface.
 
  • #3
I am sorry, there is an important typo in the link above. As written,

"x·x=x^2=a^2+b^2 + i(2ab), rather that a^2+b^2"

should be,

x·x=x^2=a^2-b^2 + i(2ab), rather that a^2+b^2. The minus sign is important.

So we have,

x⋅x = (x_1 + iy_1)^2 + (x_2 + iy_2)^2 + (x_3 + iy_3)^2 = 0

I hope the above is clear as the original quote was not..

Thanks.
 
  • #4
So a post of andrewkirk's disappeared but think I remember most of it. So as for the physics content of my question I agree that this is probably a dead end, but still maybe an interesting math question. The link I gave of Thayer Watkins website was material that he probably got from the book of the famous mathematician Elie Cartan, The Theory of Spinors? I butchered the question, sorry. Here is a relevant page from that book, (which Google let's you read a bit)

https://books.google.com/books?id=f-_DAgAAQBAJ&printsec=frontcover&dq=the+theory+of+spinors&hl=en&sa=X&ved=0ahUKEwi9063Y-K_LAhWLFx4KHWFvCGAQ6AEIHTAA#v=onepage&q=the theory of spinors&f=false

upload_2016-3-7_20-35-51.png


So what is the shape of the surfacec defined by x∈ℂ^3 and x⋅x = 0? My first guess is that it is a
boring 4 dimensional infinite space. My second guess is that because it is complex maybe something interesting is going on. We have,

x⋅x = (x_1 + iy_1)^2 + (x_2 + iy_2)^2 + (x_3 + iy_3)^2 = 0 or

(x_1^2 + x_2^2 + x_3^2) - (y_1^2 + y_2^2 + y_3^2) = 0 and

(x_1y_1 + x_2y_2 + x_3y_3) = 0 So what?

Also
x⋅x = (x_1 + iy_1)^2 + (x_2 + iy_2)^2 + (x_3 + iy_3)^2 = z_1^2 + z_2^2 + z_3^2 = 0 or

z_1^2 + z_2^2 = - z_3^2 So what?

Is it true that 2z_1dz_1 + 2z_2dz_2 = - 2z_3dz_3 ? Can this help to understand the surface or do we need more powerful mathematics? Looking for simple ways at first to understand this surface.

Thanks.
 
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  • #5
I don't really know about spinors, but this is an interesting math question.

Let's say a typical point in ℂ3 is called (u, v, w), so we can avoid subscripts. Then according to the Watkins notes*, a spinor is the locus S of the equation

u2 + v2 + w2 = 0,​

or in other words, the set

S = {(u, v, w) ∈ ℂ3 | u2 + v2 + w2 = 0}.​

Note that this is a homogeneous polynomial, meaning that each monomial has the same degree (in this case, 2). Homogeneity implies that if (u, v, w) ∈ S, then the same is true of any complex multiple of it:

K(u, v, w) = (Ku, Kv, Kw) ∈ S​

where K is an arbitrary complex number, which is easy to verify. Now let's ignore the point (0, 0, 0) of S, which means that we will also exclude the complex number K from taking the value 0. Then the set

S* = S - {0, 0, 0}​

is the disjoint union of sets of the form

P(a, b, c) = {K(a, b, c) | K ∈ ℂ*},​

where ℂ* denotes ℂ - {0} and (a, b, c) is any arbitrary but fixed point of ℂ3.

Now, each such set P(a, b, c) is just a copy of ℂ*, which may be thought of as determining a "complex line" (actually a 2-dimensional real plane) in ℂ3.

The set of all complex lines in ℂ3 is a 4-dimensional manifold (i.e., it has 2 complex dimensions) known as the "complex projective plane" and denote by the symbol ℂℙ2. It turns out to be the most natural space to study the locus of a homogeneous polynomial in 3 complex variables.

A beautiful fact is that the topology of the set of points in ℂℙ2 that occur as complex lines P(a, b, c) that form part of the locus S is a compact orientable surface of genus g (i.e., a "g-holed torus") — and that the genus g is a simple function of the degree d of the original homogeneous polynomial, as follows:

g = (d-1)(d-2)/2.

In our case, d = 2 and so g = 0. This means that topologically, the locus in ℂℙ2 is a 2-dimensional sphere S2.

Backing up to the original locus S, this means that if we remove (0, 0, 0) from S to get what we called S*, then S* is the union of one copy of C* for each point of a 2-sphere S2.

_______________________________
* Of course, u2 + v2 + w2 is not the usual "Hermitian" inner product on ℂ3 of (u, v, w) with itself, which would be u conj(u) + v conj(v) + w conj(w) = |u|2 + |v|2 + |w|2.
 
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Spinnor said:
So a post of andrewkirk's disappeared
Yes. I wrote something, then decided after a few minutes that it was actually rubbish, so I deleted it.

That happens sometimes :biggrin:
 
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Thank you Zinq! Much to digest this evening.
 

Related to Shape defined by x∈ℂ^3 and x⋅x = 0.

1) What is the shape defined by x∈ℂ^3 and x⋅x = 0?

The shape defined by x∈ℂ^3 and x⋅x = 0 is a two-dimensional surface known as a complex cone. This shape is defined in a three-dimensional complex space and resembles a cone, but with complex values instead of real values.

2) How is the shape defined by x∈ℂ^3 and x⋅x = 0 different from a regular cone?

The shape defined by x∈ℂ^3 and x⋅x = 0, or complex cone, differs from a regular cone in that it exists in a three-dimensional complex space rather than a three-dimensional real space. It also has complex values instead of real values, making it a more complex and abstract shape.

3) What is the significance of x⋅x = 0 in defining this shape?

The equation x⋅x = 0 is a defining characteristic of a complex cone because it signifies the points on the surface where the vector x is perpendicular to itself. This creates a cone-like shape with an apex at the origin in three-dimensional complex space.

4) What are some real-world applications of this shape?

One possible application of this shape is in physics, specifically in quantum mechanics. The concept of a complex cone can be used to describe certain physical phenomena, such as the behavior of particles in a magnetic field. It can also be used in computer graphics to create complex and visually interesting shapes.

5) How does the shape defined by x∈ℂ^3 and x⋅x = 0 relate to other mathematical concepts?

The complex cone is related to other mathematical concepts such as complex numbers, vectors, and matrices. It can also be thought of as a generalization of a regular cone in three-dimensional space. The equation x⋅x = 0 is also similar to the equation for a circle, x^2 + y^2 = r^2, in two-dimensional space, showing a connection between two- and three-dimensional shapes.

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