Never mind all that. How much wood could a woodchuck chuck if a woodchuck could chuck wood?
http://gizmodo.com/so-about-that-physics-defying-nasa-thruster-that-suppos-1790525676Ultimately, the biggest concern Sedwick had was the popular press that surrounded this paper. “People were taking the fact that this peer review paper came out as saying that this technology was valid and the truth and was real. That’s not what the paper says. The paper says ‘hey, we did some experiments and did our best to drive down the uncertainty, and we still have this anomalous thrust that can’t be explained in classical physics,’” he said. “The paper does not say that this is a real, definite thing.”
...Jing and I have contemplated an interesting idea: that baryogenesis becomes easier in the presence of Lorentz violation. Ordinarily, successful baryogenesis requires three ingredients, as first elucidated by Andrei Sakharov: violation of baryon number (i.e., processes which produce different numbers of baryons than antibaryons), violation of charge and charge-parity symmetries (i.e., processes which behave differently for particles and antiparticles), and a departure from thermal equilibrium (i.e., things don’t have a chance to settle down in to a quiescent state, in which baryons and antibaryons would presumably be equally abundant).
Sakharov’s argument, sensibly enough, assumes that everything is nice and Lorentz invariant. If you violate that assumption, an interesting thing happens — you can get different numbers of baryons and anti-baryons even in thermal equilibrium! This is an old idea, actually — suggested by Cohen, Kaplan and Nelson under the name “spontaneous baryogenesis,” and explored more recently in the context of evolving dark-energy (quintessence) fields by Mark and his students Antonio De Felice and Salah Nasri, as well as in the context of simple Lorentz-violating vector fields by Bertolami et al.
The loophole is easy enough to state (although more difficult to appreciate). In quantum field theory there is something called the CPT theorem, which (among other things) guarantees that particles and antiparticles have equal masses. But Lorentz invariance is an assumption of the CPT theorem, and a vector field with a nonzero value in the vacuum can violate it. If the vector interacts with baryons in a certain way (not so hard to arrange, really), it can make antibaryons be just a bit heavier than baryons. That means that the baryons can be more abundant, even in equilibrium, and this slight asymmetry can persist to this day — and provide the particles out of which we are all made.
Probably as much use as the snake in my boot.
We use essential cookies to make this site work, and optional cookies to enhance your experience.