jctyler said:
In other words, until that algorithm is proven correct, nobody knows for sure how mass is generated? And if the LHC proved the algorithm incorrect, this would destabilize the main theory?
We really shouldn't be calling it an algorithm -- it's not. It's a physical mechanism described as part of the theory. The presence of the Higgs field in the standard model is necessitated by the apparent need for
gauge symmetry in the Standard Model (SM). (This is technical so I won't go into details on a first pass, but I'm happy to discuss more if you have questions.) Essentially, if the particles have masses at the level of their equations of motion (e.g., the Dirac equation for a massive particle is -i\hbar \gamma^\mu \partial_\mu \psi + mc\psi = 0, the 2nd term on the LHS is the mass term) then the theory does not exhibit the gauge symmetry. Why is the gauge symmetry important? Imposing gauge invariance on a free field (such as the free fermion described by the Dirac equation) generates
interactions. One finds that in order for the Dirac equation to exhibit gauge invariance it must interact with forces. So, the simplest gauge symmetry (called U(1)), results in the coupling of charged fermions to the electromagnetic potential -- one ends up with quantum electrodynamics. Other gauge symmetries (SU(2), SU(3)) result in additional forces. But all this only works if there are
no explicit mass terms in the equations! The Higgs mechanism is an elegant way of retaining the vitally important gauge symmetry while allowing for masses to be introduced into the theory. The Higgs mechanism makes use of a process called
spontaneous symmetry breaking (which, admittedly, sounds confusing since it's supposed to help
retain the symmetry, not break anything. In a way, it does both.)
This iI don't understand. Wherever I try to find answers to what bosons are it always says that in essence they are massless and have a certain spin which makes them different from those particles that have mass and have another spin. So this boson would be a freak?
Yes, bosons have integer spin (this is what makes them bosons.) They differ from fermions that have spin 1/2. The only bosons that have been seen in nature are the ones that mediate the fundamental forces (so-called
gauge bosons for reasons that I briefly sketched above). The photon is one such boson that is in fact massless; the W and Zs of the weak force are actually massive (as a result of the Higgs mechanism). So having a mass does not make a boson a freak. The mass of the Higgs boson itself comes from the fact that it self-interacts, something that is possible because it is a spin zero particle. Additional mass comes from its interactions with other particles, more on this below...
Do physicists think of mass as infinite or is that part of what bugs them about the Higgs mechanism?
It bugs them. The Higgs interacts with all massive particles in the SM. Quantum mechanically, these interactions occur through the exchange of gauge bosons. However, quantum mechanics tells us that we should sum over all possible such exchanges (think perturbation expansion if you are familiar). Each exchange contributes to the mass of the Higgs. If you naively count up all these contributions, it goes off to infinity. This is a problem. (The technical term for this process would be to say that the Higgs field receives
radiative corrections from all the other particles in the theory.) So, something must stop this counting process, i.e. there needs to be a cutoff where we say, "OK, we're done counting." Of course, we should stop counting at the Planck scale, but this is still way too high. So there needs to be a much lower energy cutoff that protects the Higgs mass and keeps it relatively light. Nobody knows yet how this happens; supersymmetry is probably the best guess right now.
If the Higgs boson did not exist, wouldn't that disprove the concept of the Higgs mechanism?
Excellent question. No! Spontaneous symmetry breaking, and the Higgs mechanism in particular (as concepts), are seen in condensed matter systems. For example, the Misner effect and ferromagnetism, below the Curie temperature are examples and consequences of spontaneous symmetry breaking. Although I have a feeling you're referring to the Higgs mechanism in particle physics. If there is no Higgs boson discovered at the LHC, we of course can't rule out the possible existence of the Higgs mechanism operating elsewhere at higher energies in the SM. However, it would complicate our understanding of electroweak processes.