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"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).

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"Hyperspace"*: Physics as Geometry

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  1. "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)

  2. Talk outline: • examples of recasting phenomena as rotations in new spaces • application to gauges • visualizing the “internal spaces” of the gauge theories

  3. 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

  4. unfamiliar example: Kaluza-Klein Theory • in ~1919, Kaluza (and others, long story) looked at "Christoffel symbols" Γαβγ used in general relativity, thought "wow, Fand Γαβγlook similar!" • hmm, F would need another index to match up properly, or Γαβγ 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)

  5. Brief aside:Christoffel symbols, “Γαβγ” • 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

  6. What Kaluza did: • Kaluza added the vector potential along the sides of the metric tensor essentially like so - • Then, when you calculate Christoffels involving extra dimension, Γ5  F  • figure after Kaku, “Hyperspace”

  7. 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 :

  8. 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

  9. Their immediate legacy • surely, the genius of these giants of unification would be lauded by their peers for decades!

  10. D’OH! • actually their theory was totally eclipsed by quantum mechanics for 60 years or so

  11. But THEN their theory was much celebrated • theories such as Supergravity & String theory invoke yet more compactified, ~ Planck-scale dimensions • figure after Greene, Fabric of the Cosmos • with 10 dimensions, you can fit everything! • sorta. • (long story) • figure after Kaku, Hyperspace

  12. 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?

  13. 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 = ijkjek • let i  ijkjek • 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

  14. 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 • tis 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

  15. 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, [01-10] 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)

  16. 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!)

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

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

  19. Further reading • Video Lecturesfrom 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

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