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First Definitive Higgs Result In 7 Years
PhysicsDavid writes "In a suite of new results about the Higgs boson, Fermilab presents the first new definitive evidence on the (lack of) existence of the Higgs boson since the Large Electron Positron collider shut down in 2000. Fermilab hasn't found the Higgs, but can rule out a certain range of masses for the particle that is believed to create mass for all the other particles of nature. Other Higgs news suggests a new likeliest mass range of 115 to 135 GeV for the Higgs. These results were among those presented at the ICHEP 2008 conference currently wrapping up in Philadelphia."
Knowing the mass of the higgs is important because it tells us which of our theories is on the right track. For example, a very large higgs would rule out huge branches of string theory, almost killing it. Not finding it at all would rule super symmetry would destroy the standard model, with nothing left to stand it in place.
The 'worst' case is that we find the higgs exactly where we expect it to be, confirming what we pretty much knew already, without adding any new real information.
Don't joke about that, I'm sure I read about a paper last year which predicted a minimum Higgs mass just outside of the LHC's range. It must keep those involved awake at night.
No kidding!!! What do you say at this point?
The electron volt is a measure of energy. It is the energy gained by an electron accelerating through an electric field potential of one volt. And since energy and mass are equivalent, this miniscule measure of energy also makes for a useful miniscule measure of mass.
If you mod me Overrated, you are admitting that you have no penis.
Not to diminish the importance of the work done at Fermilab, but the headline is very misleading.
And 1 GeV = 1.783×1027 kg
Slashdot ate your formatting it looks like. I'll write it as 1.783E-27 kg to get around it.
The enemies of Democracy are
It sounds like you're thinking about the Higgs giving mass to particles by being a constituent of them. (That is a perfectly reasonable linguistic interpretation of ``give mass to'', but it doesn't reflect the physics.)
In these theories, mass arises of interactions with the Higgs boson. Thus, the Higgs being massive doesn't exclude less massive particles.
The "rest mass" of particles has to do with how strongly they couple to the Higgs field (as well as the intrinsic value of the H field in a vacuum), and doesn't really have anything to do with the mass of the Higgs. Particles do not have mass because they are composed of (presumably lighter) Higgs particles, they have mass because they interact with the Higgs field, if the theory is correct. The problem is that we don't understand very well how the Higgs quanta couple to the H field, so it's difficult to predict what mass(es) they should have.
If particle masses were an additive quantity based on the mass of the Higgs, as your intuition seems to tell you, then as long as there are massless particles like the photon, then the Higgs would also have to be massless and, by induction, so would every other particle we observe.
Thanks for that hint, I've now found the Higgs mechanism which is currently in the process of giving me a headache.
Having a degree in physics means nothing if you didn't do
anything in this branch of physics.
That seems a bit strong. A physics degree does mean that you can
reasonably expect an explanation to be understood without too much
effort on your part.
First off, the electron is not the lightest particle. Strictly
speaking, the electron neutrino weighs in at less than 2.2 eV, where the
electron weighs in at 0.511 MeV. Then you have the tau neutrino, which
weighs in at 15.5 MeV. Then you have the proton, which weighs 938 MeV.
After that we have the tauon, which has a mass of 1.7 GeV. All of which,
so far, are leptons.
I can see where you're going, but you made a careless error. The proton
is not a lepton.
In the standard model, leptons and quarks are fundamental particles.
Leptons and quarks are reflections of each other through a certain
symmetry. But a quark never appears by itself. A quark-antiquark pair
is called a meson (which is a boson because it has whole-integer quantum
spin), and a triplet of quarks, like a proton or neutron, is called a
baryon (which is a fermion because it has half-integer quantum spin). A
hadron is any particle that interacts through the strong force; this
includes mesons and baryons but not leptons.
actually when I first heard about it, I thought it was a fermilab discovery. Theres been a lot of rumors flying around that CDF had something big. If this was it, I'm disappointed. Also for the record, fermilab is still very relevent. The most likely place for the Higgs given current experimental evidence is in the second easiest place for the Tevatron experiments to see it (115 GeV) but the hardest place for the LHC experiments to see it. So the Tevatron could well scoop the LHC, its not over.
Incidently, why is 115 GeV so hard for the LHC to see. Well at this point the Higgs is too light to decay to WW or ZZ (the W has mass of 80 GeV, Z 91GeV so needs Higgs mass of 160-180 GeV to open those channels). This means that a light Higgs of 115 GeV will decay into the heaviest particle availible to it (remember the more massive the particle, the strong the Higgs coupling) which is the bottom quark. At the Tevatron, the backgrounds to two bottom quarks isnt soo bad and the experimenters are all very experienced at tagging b quarks using their detectors. At the LHC you might as well give up so you have to go through the very rare vector boson fusion channel using a top quark loop to get two photons which itself has a bit of nasty background. Hence you will need 10 fb-1 of data which is *atleast* a years running at the LHC.
At the Tevatron, the backgrounds to two bottom quarks isnt soo bad and the experimenters are all very experienced at tagging b quarks using their detectors.
Actually the background for b quarks at the Tevatron is ENORMOUS. b-quarks are produced by the strong interaction at rates far higher than they are produced from any possible Higgs decay. Identifying them is only half the problem: determining what produced them is the other half! The only way that we can see anything is via associated production of a Higgs and a W or Z boson (which are a lot easier to spot). This is a far rarer process than simple Higgs production.
At the LHC you might as well give up so you have to go through the very rare vector boson fusion channel using a top quark loop to get two photons which itself has a bit of nasty background.
You are actually a little out of date here. While the vector boson fusion channel is still used the decay is actually Higgs to two taus or VBF Higgs production with the two associated quarks being top quarks. At least in ATLAS we think that both of these channels will have a higher significance than the photon channel which was the original choice for a low mass Higgs.
FAIL.
Try again.
They filled it with a ton of European magnets (that worked), Japanese detectors (that worked), and US final focus magnets (that failed).
Sorry to burst your patriotic bubble.