"hyperspace"*: physics as geometry

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"Hyperspace"*: Physics as Geometry Fritz Reitz, Ph.D. (it’s not in physics, as will become obvious shortly) 5/18/09 *a la Michio Kaku's sensionalization of the invocation of unseen dimensions (e.g. isospin space) in physics

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"Hyperspace"*: Physics as Geometry. Fritz Reitz, Ph.D. (it’s not in physics, as will become obvious shortly) 5/18/09 *a la Michio Kaku's sensionalization of the invocation of unseen dimensions (e.g. isospin space) in physics (hey Fritz, don’t forget to run vi’s ahead of time). - PowerPoint PPT Presentation

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Page 1: "Hyperspace"*:   Physics as Geometry

"Hyperspace"*: Physics as Geometry

Fritz Reitz, Ph.D. (it’s not in physics, as will become obvious shortly)

5/18/09

*a la Michio Kaku's sensionalization of the invocation of unseen dimensions (e.g. isospin space) in physics

(hey Fritz, don’t forget to run vi’s ahead of time)

Page 2: "Hyperspace"*:   Physics as Geometry

Talk outline:

• examples of recasting phenomena as rotations in new spaces

• application to gauges

• visualizing the “internal spaces” of the gauge theories

Page 3: "Hyperspace"*:   Physics as Geometry

familiar example: special relativity recasts/simplifies motion

• add "time" direction to space

• with new concept of 4-velocity,

dr/d =(c, vx, vy, vz), |dr/d| = c for everything

• if someone's clock seems slow, it's because they've steered away (via boost) from your "time" direction, just as one goes north slower in an airplane pointed NNE

• adding a dimension has cast motion in a different light, and simplified things

Page 4: "Hyperspace"*:   Physics as Geometry

unfamiliar example: Kaluza-Klein Theory

• in ~1919, Kaluza (and others, long story) looked at "Christoffel symbols" Γα

βγ used in general relativity, thought "wow, F and Γα

βγ look similar!"• hmm, F would need another index to match up properly, or Γα

βγ one less

• why, that would only happen if there was another spatial dimension ( goes from 0 to 4), that was connected less intimately (g/x = 0)

Page 5: "Hyperspace"*:   Physics as Geometry

Brief aside:Christoffel symbols, “Γα

βγ”• directional derivative in Euclidean coordinates:

• directional derivative in Polar coordinates:

• Christoffel symbols account for the "extra" part of the derivative due to changing coordinates (e.g. d scales with r, dr changes direction with )

• handy when spacetime itself is curved, hence its use in GR

Page 6: "Hyperspace"*:   Physics as Geometry

What Kaluza did:

• Kaluza added the vector potential along the sides of the metric tensor essentially like so -

• figure after Kaku, “Hyperspace”

• Then, when you calculate Christoffels involving extra dimension, Γ5 F

Page 7: "Hyperspace"*:   Physics as Geometry

and charge is velocity in this extra direction (BONUS!)

• short version is charge x velocity is a current density which is the derivative of F Ricci curvature flat space stress tensor u5 x velocity, so 0 u5!

•I don't get it either, but wow! 0 u5!

•long version is 0u J, J F/x, F/x R5, R5 T5, T5 u5u 0u, 0 u5 :

Page 8: "Hyperspace"*:   Physics as Geometry

Klein’s paper• Oskar Klein is late to the party again

(story of his life -- long story), but then curls up the extra dimension tightly

u5 and thus momentum, and thus 1 / (de Broglie wavelength h/p)

• he imagined the extra dimension wrapped in a circle, with an integer number of standing waves

• charge thus quantized, and quantum of charge specifies radius of extra dimension < 10-30 in.

• bunch of other stuff including repeated use of the word “simply”

after Greene, Fabric of the Cosmos, Fig. 12-7

Page 9: "Hyperspace"*:   Physics as Geometry

Their immediate legacy

• surely, the genius of these giants of unification would be lauded by their peers for decades!

Page 10: "Hyperspace"*:   Physics as Geometry

• actually their theory was totally eclipsed by quantum mechanics for 60 years or so

D’OH!

Page 11: "Hyperspace"*:   Physics as Geometry

But THEN their theory was much

celebrated

• figure after Kaku, Hyperspace

• theories such as Supergravity & String theory invoke yet more compactified, ~ Planck-scale dimensions

• with 10 dimensions, you can fit everything!

• sorta.

• (long story)

• figure after Greene, Fabric of the Cosmos

Page 12: "Hyperspace"*:   Physics as Geometry

on to gauges, and D + iq/hbarc A

• if we insist on local gauge invariance of the Lagrangian ( is function of x), there’s trouble as (e-i) e-i

• can redefine D, but isn’t that cheating? aren't we just sweeping terms under the rug?

• what is "D"now? is it still a "partial derivative" even?

Page 13: "Hyperspace"*:   Physics as Geometry

classical analogy for D + iq/hbarc A

• consider a spinning top and a vector x in the top's frame such that x = xi ei , where ei are themselves ei(t)

• dt x = (dt xi) ei + xi ( dt ei ) [need product rule]• for rotating frame, dt ei = ei = ijkjek • let i ijkjek

• dt x = (dt xi) ei + xi i

• let t dt, local + , or, if ’ hbarc/iq

t dt + iq/hbarc ’

• "Why don't we call [choosing a gauge] choosing coordinates in the extra space? It's an unfortunate historical accident." -- C. Bloom

Page 14: "Hyperspace"*:   Physics as Geometry

D + iq/hbarc A &t t + iq/hbarc ’

• an ant living in the rotating frame might not realize that ei changed with time, they might think dt x = (dt xi) ei was the whole story, would think Coriolis and centrifugal forces were real

tis thus the derivative of the "real" x

• the suggestion is that we are like the ant, immersed in and yet oblivious to some mode of motion, like rotation in Kaluza's 5th dimension, and EM is like the "fictitious" Coriolis force

Page 15: "Hyperspace"*:   Physics as Geometry

visualizing the “internal spaces” of the gauge theories

• different gauge theories span different internal spaces, with differing numbers of generators

• generators contain the essence of their transformation, e.g.

(x+a) = exp( a d/dx ) (x) (per Taylor series; see footnote 1)

(+z) = exp( [01

-10]) ()

• in a sense, d/dx is translation; it’s the rule for how to go from here to there. similarly, [0

1-1

0] is how to rotate• generators of internal spaces correspond to bosons that

act on their corresponding fermions • what is the “essence” of a weak bosons? of a gluon?

(1): (x-a) = (x) - a d/dx (x) / 1! + a2 d2/dx2 (x) / 2! - ... = e-a d/dx (x)

Page 16: "Hyperspace"*:   Physics as Geometry

simulations of SU(2), SU(3)

• spin, weak isospin are SU(2), generated by Pauli matrices, color SU(3) & Gell-Mann

• SU(2) “like” 3D rotations, and quark state is “possible to represent”, but how meaningful is it really to draw a continuous, classical pictures of unpicturable quantum processes?

• answer: kinda (to simulation!)

Page 17: "Hyperspace"*:   Physics as Geometry

A favorite quote:

• “If I have seen further than others, it is by standing upon the shoulders of giants.” -- Isaac Newton

Page 18: "Hyperspace"*:   Physics as Geometry

Personal footnote

• “If I have seen less than others, it is because I as yet but cling to the buttocks of giants.” -- Fritz Reitz

Page 19: "Hyperspace"*:   Physics as Geometry

Further reading• Video Lectures from ASTI conference, intro to symmetry, group

theory, strings, supersymmetry, QFT at http://www.asti.ac.za/lectures.php

• Griffiths has a particle physics text!: Introduction to Elementary Particles, 2nd ed. (just as accessible as his EM & QM texts)

• Popularizations re: particles, electro-weak mixing, U(1), SU(2), SU(3): Schumm’s Deep Down Things

• Popularizations re: Kaluza-Klein, string theory Halpern’s The Great Beyond (much biographical history), Kaku’s Hyperspace, Greene’s The Elegant Universe

• Popularizations re: quantum gravity, critique of string theory: Smolin's Three Roads to Quantum Gravity, Smolin's The Trouble with Physics

• Original K-K papers: reprinted in Appelquist et al. Modern Kaluza-Klein Theories

fin