@Jedi_Sawyer - please read the reference materials provided in post #2 and make your comments appropriate to the original question.
You brief run-through of various FTL examples seems garbled and barely coherent to me, but at heart I suspect you are questioning the experimental basis for special relativity when you say:
I do not think they have any real particle examples of anything going that fast.
I don't know who "they" are, but the scientific cimmunity does have many real-particle examples which are very close to lightspeed indeed - though there is only one class going at lightspeed and none at all faster. Please see the following list of the experimental basis for special relativity-
http://math.ucr.edu/home/baez/physics/Relativity/SR/experiments.html
... for some of the experiments that
have been conducted.
It is a routine experiment, for example, to accelerate particles such as electrons and protons to different speeds with different energies ... plotting a graph of energy vs speed confirms the special relativity relationship.
I don't know how fast you mean by "going
that fast" but - the fastest particle recorded was a proton from cosmic rays:
http://www.fourmilab.ch/documents/ohmygodpart.html/
... managed 0.9999999999999999999999951c. Fast enough for ya?
But there are ways to have an FTL experience besides the examples in post #1.
Riding the expansion of the Universe is one way. This is a geometric/coordinate expansion, and it's details are covered by
general relativity. There are other examples.
- you can shine a spot of light on a distant surface: a small rotation of the light source produces a big movement in the spot. You can easily find the geometry which allows the spot to move faster than light across the surface.
- if two objects travel in opposite directions at 0.75c, in the lab, then their separation increases at 1.5c when also measured in the lab.
... both of these are simpler examples of the geometric "exception" to the no-FTL rule.
These are allowed because the rule, in it's simplest form, is that all observers measure the same value for the speed of light in a vacuum.
Entanglement, and non-locality, is another kettle of piranhas though.
Please see the following:
http://curious.astro.cornell.edu/question.php?number=612
... tldr: in an entanglement experiment
nothing actually travels.
popular reports of ftl communication are exaggerated and misleading.
(Unfortunately the example given is a hidden variables example, which is not quite the same thing, but it does illustrate how you can know two things across vast distances instantly without violating relativity.)
I think that, before trying to discuss the advanced concepts, you really need to get the basics down. Please read the FAQ. It's accessible and contains useful tools to help you talk about relativity issues in a clear way.
Cheers :)