Back To Sleep in a Sea of Stars Save as PDF
Chapters (67)
  1. Title Page
  2. Copyright Notice
  3. Dedication
  4. PART ONE
  5. CHAPTER I
  6. CHAPTER II
  7. CHAPTER III
  8. CHAPTER IV
  9. CHAPTER V
  10. CHAPTER VI
  11. CHAPTER VII
  12. CHAPTER VIII
  13. CHAPTER IX
  14. EXEUNT I
  15. PART TWO
  16. CHAPTER I
  17. CHAPTER II
  18. CHAPTER III
  19. CHAPTER IV
  20. CHAPTER V
  21. CHAPTER VI
  22. CHAPTER VII
  23. CHAPTER VIII
  24. CHAPTER IX
  25. CHAPTER X
  26. CHAPTER XI
  27. CHAPTER XII
  28. EXEUNT II
  29. PART THREE
  30. CHAPTER I
  31. CHAPTER II
  32. CHAPTER III
  33. CHAPTER IV
  34. CHAPTER V
  35. CHAPTER VI
  36. CHAPTER VII
  37. CHAPTER VIII
  38. EXEUNT III
  39. PART FOUR
  40. CHAPTER I
  41. CHAPTER II
  42. CHAPTER III
  43. CHAPTER IV
  44. EXEUNT IV
  45. PART FIVE
  46. CHAPTER I
  47. CHAPTER II
  48. CHAPTER III
  49. CHAPTER IV
  50. CHAPTER V
  51. CHAPTER VI
  52. EXEUNT V
  53. PART SIX
  54. CHAPTER I
  55. CHAPTER II
  56. CHAPTER III
  57. EXEUNT VI
  58. ADDENDUM
  59. APPENDIX I
  60. APPENDIX II
  61. APPENDIX III
  62. APPENDIX IV
  63. AFTERWORD & ACKNOWLEDGMENTS
  64. Also by Christopher Paolini
  65. A Conversation between Brandon Sanderson and Christopher Paolini
  66. ABOUT THE AUTHOR
  67. Newsletter Sign-up

In any case, it has proven possible to convert ordinary EM radiation from abelian to nonabelian by modulating the polarization of the wave energy emitted from antennas or apertures, or by tuning the frequencies of alternating current to the toroidal geometries through which the currents are driven (this is the method used by a Markov Drive). Doing so results in EM radiation with an underlying field of SU(2) symmetry and nonabelian form, as described in Maxwell’s expanded equations. This couples in an orthogonal direction with the spacetime fields via a shared quantity: the “A vector potential.” (Orthogonal, as tardyons and tachyons exhibit opposite motion directions along their packet lengths, and the conditioned EM field is interacting with both the subluminal and superluminal surfaces of spacetime.) This has often been described as traveling in a straight line along a right angle.

Once the EM field is coupled with the spacetime fabric, it becomes possible to manipulate the density of the medium. By injecting an appropriate amount of energy, spacetime itself can be made increasingly thin and permeable. So much so that at a certain point the energy density of subluminal space causes the affected area to pop into superluminal space, like a high-pressure bubble expanding/rising into an area of lower pressure.

As long as the conditioned EM field is maintained, the encompassed subluminal space can be kept suspended within superluminal space.

From the point of view of an STL observer, everything within the bubble has vanished and can only be detected by its gravitational “hill” from the other side of the spacetime membrane.

From inside the bubble, an observer will see themselves surrounded by a perfect, spherical mirror where the surface of the bubble interfaces with the outer FTL space.

From the point of view of an FTL observer, a perfectly spherical, perfectly reflective bubble will have just popped into existence in superluminal space.

Mass and momentum remain conserved throughout. Your original heading will be the same in FTL as in STL, and your original speed will be converted to the superluminal energy-equivalent.

Once the EM field is discontinued, the bubble will vanish, and everything inside will drop back into subluminal space (a process no doubt familiar to many of you). Often this is accompanied by a bright flash and a burst of thermal energy as the light and heat that built up inside the bubble during the trip are released.

A few points on the specific features of Markov Bubbles are worth mentioning: