Tuesday 13 January 2015

universe - What did electroweak symmetry breaking actually look like?


Approximately one picosecond after the Big Bang, the universe cooled down enough to pass through the electroweak phase transition. At this point the Higgs mechanism kicked in, the weak force became short-ranged and observationally distinct from electromagnetism, particles gained mass, the electroweak era ended, and the quark era began (and lasted one whole microsecond!).


I'm sure that this is gigantic subject, but could anyone explain in just a few sentences what the actual dynamical process of symmetry breaking looked like as the universe passed through the critical temperature? What would you have observed right at the critical moment? A sudden shower of Higgs bosons appearing out of nowhere?


As I understand it, the transition is believed to have been weakly first-order, and the fields are believed to have equilibrated fast enough that it was effectively adiabatic, despite only lasting a fraction of a picosecond. Were the spatial temperature fluctuations strong enough that there was a moment of phase coexistence, with particles having mass in some parts of the universe but not others? How would that work? (You wouldn't have sharp domain walls between regions where the Higgs field had different values though, because the broken symmetry is continuous.)


Note that I'm asking about the phenomenology of actual dynamical symmetry breaking, not the phenomenology of broken symmetry.




No comments:

Post a Comment

Understanding Stagnation point in pitot fluid

What is stagnation point in fluid mechanics. At the open end of the pitot tube the velocity of the fluid becomes zero.But that should result...