| Thread Closed |
Higgs field popular descriptions |
Share Thread | Thread Tools |
| Jul16-12, 05:02 AM | #1 |
|
|
Higgs field popular descriptions
With the recent announcement at Cern there have been many video clips published describing the Higgs field. They show heavy and light particles passing through a field and the commentary says that the effect of the field is to slow down particles and thus give them mass. The Higgs field supposedly permeates empty space. As we know particles travelling through empty space continue with constant velocity and momentum. The Higgs field description suggests that particles travelling through the Higgs field are slowed so the more they travel through the Higgs field the more they should be slowed down. The Higgs field theory seems to be inconsistent with observation. Can anyone explain?
Regards WaveHarmony |
| Jul16-12, 05:49 AM | #2 |
|
|
How is it inconsistent with observations?
|
| Jul16-12, 06:01 AM | #3 |
|
|
Well, the popular descriptions suggest that the Higgs field slows down particles. Particles in empty space will continue in a state of uniform motion without being slowed.
WaveHarmony |
| Jul16-12, 06:10 AM | #4 |
|
|
Higgs field popular descriptions
WaveHarmony, The Higgs field is (partially) responsible for particle masses, but the popular description that it "slows them down" is quite misleading. Especially, it does not mean that they get slower and slower and eventually come to a stop, like traveling through a jar of molasses!
|
| Jul17-12, 03:55 AM | #5 |
|
|
yeah, I think Physicists need to 'dumb it down' for the layman to help explain their mathematics and particle observations.
|
| Jul17-12, 05:03 AM | #6 |
|
|
I can be easily explained by saying that the Higgs field couples to the particle's acceleration. A particle indeed is being slowed down, but the opposing force is proportional to its acceleration.
|
| Jul17-12, 06:17 AM | #7 |
|
|
It's comparable to me explaining a championship winning play in american football when you've never even seen a game before and I'm not allowed to explain the basic rules first. |
| Jul17-12, 06:23 AM | #8 |
|
|
This is exactly the case I was referring to in my above post. It's much more difficult than one might think to correctly describe theories in science without using scientific vocabulary and math. The Balloon Analogy for cosmology is another perfect example. |
| Jul17-12, 02:44 PM | #9 |
|
|
|
| Jul18-12, 02:57 AM | #10 |
|
|
The problem is compounded by the fact that I thought I understood the nature of mass as described by general relativity. I am happy with the explanation of the observed properties of mass in terms of spacetime curvature. The mass of the Earth curves spacetime so the moon responds to the spacetime curvature and follows its orbit. GR explains that any object with mass curves spacetime and the effect is cummulative. So electrons protons and neutrons curve spacetime. It seems to me that this explanation of the nature of mass is very clear and the only missing piece of the puzzle is 'how does an electron curve spacetime?' The Higgs field description doesn't seem to help with this aspect of the problem.
Can anyone explain to me in clear unambiguous terms how a Higgs field gives mass? WaveHarmony |
| Jul18-12, 08:57 AM | #11 |
|
|
|
| Jul18-12, 09:39 AM | #12 |
|
|
The weak force is mediated by three massive particles, called the W+, W-, and Z bosons. One important aspect of the Standard Model is electroweak symmetry - at a sufficiently high temperature (at a time immediately after the big bang), the weak force becomes indiscernible from the electromagnetic force. Of course, this means that the W and Z bosons were massless. Breaking this symmetry is the job of the Higgs. Spin 1 particles like the W and Z bosons have at least two degrees of freedom. One way a massless particle could gain mass is by the absorption of a scalar (spin 0) particle as it's longitudinal mode (as it's second degree of freedom). A scalar particle that does this is called a Nambu-Goldstone boson. Originally, the Higgs had four degrees of freedom - H+, H-, H0, and h. The thing about the first three is that they are equivalent to the longitudinal modes of W and Z bosons. So, they played the role of Goldstone bosons, and they were absorbed (or 'eaten' as it's often described) by the W and Z bosons, becoming their second degree of freedom, giving them mass. This leaves us with one degree of freedom for the Higgs, h. This ends up being the scalar Higgs boson, the quantum of the Higgs field. Now, the Higgs field takes a constant value at every point in space - called the vacuum expectation value. Through Yukawa coupling, fermions interact with this vacuum expectation value (in terms if Feynman diagrams, you can think of a particle as interacting with the VEV at various vertices). By interacting with the VEV they attain mass, determined by the exact value of the VEV. Note that, of course, this is a simplified explanation that leaves out more explicit details. |
| Jul20-12, 03:52 PM | #13 |
|
|
Prior to symmetry breaking, there is no electromagnetic force as such. There are the W and B forces. The latter would behave just as electromagnetism does now, except it would be a bit stronger, but is separate. |
| Jul20-12, 04:26 PM | #14 |
|
|
The Higgs mechanism breaks the electroweak symmetry [itex] SU(2) X U(1)_{Y} [/itex] to [itex] U(1)_{em} [/itex]. The generator of [itex] U(1)_{em} [/itex], Q, is given by [tex] Q = \frac {Y} {2} + I_{3} [/tex] Where Y is the weak hypercharge, and I3 is a component of the weak isospin. As you mention, this symmetry breaking mixes W0 and B0 to produce the photon and the Z, by [tex] \begin{pmatrix} \gamma \\ Z^{0} \end{pmatrix} = \begin{pmatrix} cos \theta_{w} & sin \theta_{w} \\ -sin \theta_{w} & cos \theta_{w} \end{pmatrix} \begin{pmatrix} B^{0} \\ W^{0} \end{pmatrix} [/tex] Thanks for pointing that out. |
| Jul21-12, 05:16 AM | #15 |
|
|
Thank you very much for your explanation. I can't form a clear picture of the meaning of the descriptions but this is my lack of understanding of the fundamental concepts of the standard model. The big disappointment for me is that the concept of mass which is so nearly fully explained by General Relativity is treated in a completely different way in particle physics with no apparent link between the concepts involved.
Does anyone else feel that physics is in need of a conceptual revitalisation to provide a single unified picture of everything? WaveHarmony |
| Jul21-12, 05:22 AM | #16 |
|
|
How is mass fully explained in General Relativity?
|
| Jul22-12, 10:38 AM | #17 |
|
|
We experience mass in our everyday lives and in experiments in two forms: gravitational mass and inertial mass. General relativity explains that a mass distribution has the effect of curving spacetime. GR also indicates that the effect of mass in curving spacetime is cummulative so that the greater the mass the greater the spacetime curvature. Mass also responds to spacetime curvature resulting in objects with mass seeking to move closer together. This so called gravitational force is really due to the objects seeking a lower energy. (Actually all so called fundamental forces can be treated as a search for a lower energy state).
Einstein also showed that there is an equivalence between an object in a curved spacetime environment (so called gravitational field) and an object under uniform acceleration indicating an equivalence between inertial and gravitational mass. So my claim is that GR fully explains the property we observe as mass with the one missing point that GR does not explain how mass curves spacetime. We can assume that the way mass curves spacetime is consistent so that electrons neutrons and protons which have mass do indeed curve spacetime in a similar way. So if we could explain how the electron curves spacetime then we would have a full explanation of the property mass. WaveHarmony |
| Thread Closed |
| Tags |
| higgs field boson |
| Thread Tools | |
Similar Threads for: Higgs field popular descriptions
|
||||
| Thread | Forum | Replies | ||
| What specific field in physics is the most popular for industry jobs? | Career Guidance | 2 | ||
| Relationship between higgs field and EM field | High Energy, Nuclear, Particle Physics | 7 | ||
| What is the most popular field in Quantum physics for a new researcher? | Academic Guidance | 0 | ||
| Gravity as a Goldstone-Higgs field, instead of a Gauge Field | General Physics | 0 | ||
| the Higgs field: so gravitational field by itself cannot confer mass? | High Energy, Nuclear, Particle Physics | 4 | ||