Navigating the Quantum Maze: Spin State Vectors and the Magic of Projection

Welcome to the Spin Vector Universe

Today, we embark on a cosmic adventure, learning how to navigate through a space where the points are none other than spin ½ state vectors. These vectors, much like secret agents, carry both the “observable information” that we can detect and a hefty dose of hidden data that remains mysterious—at least for now. Who knows what tomorrow’s physicists will uncover about these enigmatic vectors? Perhaps one day, even consciousness itself (and even  "psi" phenomena) will be written into the math.

These vectors, much like secret agents, carry both the “observable information”...

That’s right, physicists may finally crack the "consciousness code," but until then, let's stick to the basics—like juggling four numbers in a multidimensional space.

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The Joy of Four Numbers

We initially presented the state vector as a pair of points on a two-dimensional sphere. But why settle for simplicity when we can dive into complexity? We now represent it by four real numbers: X, Y, Z, and W. And if you’re keeping score, the squares of these four beauties add up to 1:

X² + Y² + Z² + W² = 1

But wait, there's more! We can rewrite these numbers using angular coordinates φ, θ, and ψ. Let’s get fancy:

• X = sin(φ/2) cos(ψ)
• Y = sin(φ/2) sin(ψ)
• Z = cos(φ/2) cos(ψ+θ)
• W = cos(φ/2) sin(ψ+θ)

The ranges of variation of these angles are:

•  φ from 0 to π. (latitude)
• θ, ψ from 0 to 2 π.

 Cue the applause from the programmers in the room! Of these three angles, only θ and φ are observable in our space; ψ remains the mysterious guest who refuses to show their face.

Note: In quantum mechanics we usually present the spin vector as a column of two complex numbers, the "Pauli spinor":

X + iY

Z + iW

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A Tour of Spherical Spaces

To keep things simple (or at least as simple as quantum mechanics gets), here’s a quick refresher:

• X² + Y² = 1: Points on the plane (X, Y) lie on a one-dimensional circle.
• X² + Y² + Z² = 1: Points in three-dimensional space lie on a two-dimensional sphere.
• X² + Y² + Z² + W² = 1: Points with coordinates (X, Y, Z, W) lie on a… wait for it… three-dimensional sphere embedded in four-dimensional space.

Wrap your head around that one! But don’t worry, mathematicians have our backs. Using stereographic projection, they can help us visualize these four-dimensional wonders in our humble three-dimensional world.

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Stereographic Projections: Cartography for the Quantum Age

Remember those flat maps of the Earth that distort everything around the poles? That’s stereographic projection in action. We can apply the same trick to our three-dimensional sphere, squishing it down into a more manageable three-dimensional space. Here’s the cartographer’s recipe:

• If X, Y, Z are the coordinates on a 2-sphere, the projection onto a plane gives:
  • x = X / (1 - Z)
  • y = Y / (1 - Z)

To up the ante for our four-dimensional friends:

• For X, Y, Z, W, the projection into 3D space becomes:
  • x = X / (1 - W)
  • y = Y / (1 - W)
  • z = Z / (1 - W)

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What Do We Gain? What Do We Lose?

Through stereographic projection, we lose just one point: the North Pole, or in this case, the point where W = 1. When W = 1, X, Y, and Z all vanish into thin air, leaving us with a single state vector that escapes to infinity. But don’t worry, we’ll survive this minor loss.

On the plus side, we get to visualize the structure of spin state vectors in all their three-dimensional glory, and the angles between intersecting lines remain preserved. Cartographers everywhere are cheering in solidarity.

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The Aesthetics of Spin Space

Is it worth painting a picture of the spin state vector space? Absolutely! 

Both for its educational value and sheer aesthetic beauty. We can craft these images with relative ease (shout-out to the programmers) and even delve into the lovely world of Villarceau circles, which have graced the stairs of Strasbourg Cathedral for centuries. Talk about a deep cut!

In our next post, we’ll dive into how to create such images and translate them into physicist-friendly terms. For now, imagine a torus—a mathematical donut—and the intricate circles that define its geometry. Doesn’t quantum physics just make you hungry?

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PS: For Your Viewing Pleasure

If you’re curious about more stunning images and videos (probably better than the ones I can whip up), check out the “Dimensions” website: Dimensions. Just a heads-up, though—they skip the spin physics. You’ll have to come back here for that!

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And there you have it—our journey through the quirky, brain-bending world of spin state vectors. Let’s call it the appetizer for the main course, which will be served in the coming posts. Until then, keep your angles sharp and your vectors spinning! 

P.S.07-10-24 13:26 In the meantime I am working on my paper about positive and negative energy conformal universe. Have just created a nice illustration for 1+1 spacetime dimensions. Matter and antimatter are separated by "conformal infinity". Here it is:

Universe as a yummy donut

P.S. 07-10-24 20:38 Minus for Igor - From "Современные геометрические структуры и поля", p. 279:

P.S. 09-10-24 10:56 My new post will be delayed, as I am learning how to use the 3D graphics program that I have discovered yesterday.

Hopefully I will be able to figure it out later today.

P.S. 09-10-24 19:07:56 Finally I have managed to use this software and draw what I wanted to draw. Still lacking Villarceau circles though.

Explanations will follow tomorrow, with a new post.