Further Exploration of String Theory

Further Exploration of String Theory
Sven Gelbhaar
15 November 2008

In a previous paper, called The Unraveling of String Theory (Sven Gelbhaar,
25 January 2008), we postulated that if gravitons can escape into alternate
dimensions, thereby accounting for the weak force of gravity, that the
inverse should also be true – that gravitons should be able to traverse
back from these alternate dimensions exerting gravitational force
apparently out of nowhere. What we failed to take into consideration is
that what is true for these ‘graviton’ particles must surely also be true
for any particles.

[Figure 1]

In the above picture we see two bodies of mass. One is dense and therefore
doesn’t move at all when a smaller, or perhaps less dense, object collides
with it. Obviously the denser object would move as well, but for brevity’s
sake we shall neglect that eventuality. The point to take away from this
image is that when objects collide with enough force, they will invariably
be dispersed into all directions/dimensions.

String Theory makes the claim that there are 11 dimensions (1), and what
holds true for gravitons should certainly hold true for all particles
(including baryonic mass itself), therefore in collisions involving enough
force we should in fact be seeing a loss of matter as they should be
propelled into other (spatial) dimensions. This, however, has yet to be
observed.

We have sundry particle accelerators which collide tiny bodies of mass, and
no decay in observable mass has yet to be discerned as one would expect
given the above premises. Our most powerful accelerator, the Large Hadron
Collider, is slated to be fully operational sometime in 2009; hopefully it
will shed some more light onto this situation.

References

  1. http://en.wikipedia.org/wiki/String_theory 15 November 2008
  2. http://en.wikipedia.org/wiki/Particle_accelerators 15 November 2008

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