Is Higgs boson an elementary particle? If so why does it decays?
$begingroup$
Higgs boson is excitation of Higgs field and is very massive and short lived, it also interact with the Higgs field and thus is able to experience mass. My question is if according to standard model it is supposedly to be an elementary particle then why does it decays?
standard-model higgs elementary-particles
$endgroup$
add a comment |
$begingroup$
Higgs boson is excitation of Higgs field and is very massive and short lived, it also interact with the Higgs field and thus is able to experience mass. My question is if according to standard model it is supposedly to be an elementary particle then why does it decays?
standard-model higgs elementary-particles
$endgroup$
add a comment |
$begingroup$
Higgs boson is excitation of Higgs field and is very massive and short lived, it also interact with the Higgs field and thus is able to experience mass. My question is if according to standard model it is supposedly to be an elementary particle then why does it decays?
standard-model higgs elementary-particles
$endgroup$
Higgs boson is excitation of Higgs field and is very massive and short lived, it also interact with the Higgs field and thus is able to experience mass. My question is if according to standard model it is supposedly to be an elementary particle then why does it decays?
standard-model higgs elementary-particles
standard-model higgs elementary-particles
edited 30 mins ago
Qmechanic♦
102k121831166
102k121831166
asked 3 hours ago
user6760user6760
2,53611738
2,53611738
add a comment |
add a comment |
3 Answers
3
active
oldest
votes
$begingroup$
Most fundamental particles in the standard model decay: muons, tau leptons, the heavy quarks, W and Z bosons. There’s nothing problematic about that, nor about Higgs decays.
Your question may come from a misconception about particle decay: that it’s somehow the particle ‘coming apart’ into preexisting constituents. It’s not like that. Decays are transformations into things that weren’t there before.
$endgroup$
$begingroup$
Hi I'm still not clear about this transformation, I just read it is probabilistic so higgs boson can in fact decay into many things including 2 photons so can the same 2 photons cannot transform back into higgs boson? I highly doubt so but dunno why?
$endgroup$
– user6760
2 hours ago
$begingroup$
Generally, particle physics reactions can go either way. Yes, if you had sufficiently energetic photons appropriately arranged, the SM says they could combine to form a Higgs particle.
$endgroup$
– Bob Jacobsen
2 hours ago
1
$begingroup$
@safesphere the diagram for 2gamma to e+e- certainly exists and has a non-zero amplitude. I agree that phase factors make it small (that’s the “appropriately arranged” bit). But it was a major part of Big Bang thermalization before freeze-out, and its the mechanism for photon to e+e- pair production (via a photon from a nucleus)
$endgroup$
– Bob Jacobsen
1 hour ago
$begingroup$
@safesphere I don't understand why ATLAS should be left out of scope? Photon fusion does occur - (dde.web.cern.ch/dde/presentations/fp420_dec09/…) but if you want to say that photon fusion too rare; there's always the more common gluon fusion? nikhef.nl/pub/services/biblio/preprints/05-007.pdf Or is your problem more with the on-shell-ness of things?
$endgroup$
– Joshua Lin
1 hour ago
1
$begingroup$
@safesphere as G.Smith points out, the amplitude of the diagram is exactly the same. The cross section (probability) and event rate can differ because of the actual ongoing & outgoing particles: it’s easier to make electrons than high energy photons in a small space.
$endgroup$
– Bob Jacobsen
46 mins ago
|
show 6 more comments
$begingroup$
Another way to answer this question is that particles are not "elementary," not even in a given quantum field theory. Quantum field theories (like the Standard Model) are expressed in terms of fields, not particles. Particles are phenomena that the model predicts; some of them are stable, some are transient (they decay). The Standard Model is constructed using an elementary Higgs field, and it predicts a Higgs particle, which is unstable.
Although the language "elementary particle" is very common and probably can't be revised at this point, it might be less confusing and more accurate to talk about the elementary fields used to express a model. Even that language isn't perfect, though, because some models can be expressed in more than one way, using seemingly-unrelated sets of fields. Quantum field theory is a rich subject with many surprises!
$endgroup$
$begingroup$
are u saying the excitation of the field can disturb other fields too? So the reality is just fields interacting with one another.
$endgroup$
– user6760
2 hours ago
$begingroup$
@user6760 I'll shy away from using the word "reality" here (because different-looking descriptions can make equivalent predictions), but yes: The way quantum field theory describes things is as quantum fields interacting with each other. A particle is one manifestation of all those fields interacting with each other. The Higgs particle involves more than just the Higgs field.
$endgroup$
– Dan Yand
2 hours ago
$begingroup$
@user6760 A common approximation method in QFT involves starting with a different model that has only non-interacting fields, then adding a series of "corrections" to gradually scootch the results closer to what the real model with interacting fields would predict. That's what Feynman diagrams are about, and that's what the "virtual particle" langauge is about. In a model with non-interacting fields, there is a relatively direct correspondence between fields and particles; but that correspondence becomes less direct (to say the least) in models where the fields interact.
$endgroup$
– Dan Yand
1 hour ago
$begingroup$
Yes it makes sense to me now the virtual particle that you have mentioned.
$endgroup$
– user6760
1 hour ago
add a comment |
$begingroup$
A particle is elementary when there aren't subcomponents that we can identify.
This has nothing to do with the concept of decay, and you can easily convince yourself of this fact by observing that whereas a particle (elementary or not) may decay in many different ways, the number and type of its constituents is univocally determined.
$endgroup$
add a comment |
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3 Answers
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active
oldest
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3 Answers
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oldest
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active
oldest
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active
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$begingroup$
Most fundamental particles in the standard model decay: muons, tau leptons, the heavy quarks, W and Z bosons. There’s nothing problematic about that, nor about Higgs decays.
Your question may come from a misconception about particle decay: that it’s somehow the particle ‘coming apart’ into preexisting constituents. It’s not like that. Decays are transformations into things that weren’t there before.
$endgroup$
$begingroup$
Hi I'm still not clear about this transformation, I just read it is probabilistic so higgs boson can in fact decay into many things including 2 photons so can the same 2 photons cannot transform back into higgs boson? I highly doubt so but dunno why?
$endgroup$
– user6760
2 hours ago
$begingroup$
Generally, particle physics reactions can go either way. Yes, if you had sufficiently energetic photons appropriately arranged, the SM says they could combine to form a Higgs particle.
$endgroup$
– Bob Jacobsen
2 hours ago
1
$begingroup$
@safesphere the diagram for 2gamma to e+e- certainly exists and has a non-zero amplitude. I agree that phase factors make it small (that’s the “appropriately arranged” bit). But it was a major part of Big Bang thermalization before freeze-out, and its the mechanism for photon to e+e- pair production (via a photon from a nucleus)
$endgroup$
– Bob Jacobsen
1 hour ago
$begingroup$
@safesphere I don't understand why ATLAS should be left out of scope? Photon fusion does occur - (dde.web.cern.ch/dde/presentations/fp420_dec09/…) but if you want to say that photon fusion too rare; there's always the more common gluon fusion? nikhef.nl/pub/services/biblio/preprints/05-007.pdf Or is your problem more with the on-shell-ness of things?
$endgroup$
– Joshua Lin
1 hour ago
1
$begingroup$
@safesphere as G.Smith points out, the amplitude of the diagram is exactly the same. The cross section (probability) and event rate can differ because of the actual ongoing & outgoing particles: it’s easier to make electrons than high energy photons in a small space.
$endgroup$
– Bob Jacobsen
46 mins ago
|
show 6 more comments
$begingroup$
Most fundamental particles in the standard model decay: muons, tau leptons, the heavy quarks, W and Z bosons. There’s nothing problematic about that, nor about Higgs decays.
Your question may come from a misconception about particle decay: that it’s somehow the particle ‘coming apart’ into preexisting constituents. It’s not like that. Decays are transformations into things that weren’t there before.
$endgroup$
$begingroup$
Hi I'm still not clear about this transformation, I just read it is probabilistic so higgs boson can in fact decay into many things including 2 photons so can the same 2 photons cannot transform back into higgs boson? I highly doubt so but dunno why?
$endgroup$
– user6760
2 hours ago
$begingroup$
Generally, particle physics reactions can go either way. Yes, if you had sufficiently energetic photons appropriately arranged, the SM says they could combine to form a Higgs particle.
$endgroup$
– Bob Jacobsen
2 hours ago
1
$begingroup$
@safesphere the diagram for 2gamma to e+e- certainly exists and has a non-zero amplitude. I agree that phase factors make it small (that’s the “appropriately arranged” bit). But it was a major part of Big Bang thermalization before freeze-out, and its the mechanism for photon to e+e- pair production (via a photon from a nucleus)
$endgroup$
– Bob Jacobsen
1 hour ago
$begingroup$
@safesphere I don't understand why ATLAS should be left out of scope? Photon fusion does occur - (dde.web.cern.ch/dde/presentations/fp420_dec09/…) but if you want to say that photon fusion too rare; there's always the more common gluon fusion? nikhef.nl/pub/services/biblio/preprints/05-007.pdf Or is your problem more with the on-shell-ness of things?
$endgroup$
– Joshua Lin
1 hour ago
1
$begingroup$
@safesphere as G.Smith points out, the amplitude of the diagram is exactly the same. The cross section (probability) and event rate can differ because of the actual ongoing & outgoing particles: it’s easier to make electrons than high energy photons in a small space.
$endgroup$
– Bob Jacobsen
46 mins ago
|
show 6 more comments
$begingroup$
Most fundamental particles in the standard model decay: muons, tau leptons, the heavy quarks, W and Z bosons. There’s nothing problematic about that, nor about Higgs decays.
Your question may come from a misconception about particle decay: that it’s somehow the particle ‘coming apart’ into preexisting constituents. It’s not like that. Decays are transformations into things that weren’t there before.
$endgroup$
Most fundamental particles in the standard model decay: muons, tau leptons, the heavy quarks, W and Z bosons. There’s nothing problematic about that, nor about Higgs decays.
Your question may come from a misconception about particle decay: that it’s somehow the particle ‘coming apart’ into preexisting constituents. It’s not like that. Decays are transformations into things that weren’t there before.
answered 3 hours ago
Bob JacobsenBob Jacobsen
4,436616
4,436616
$begingroup$
Hi I'm still not clear about this transformation, I just read it is probabilistic so higgs boson can in fact decay into many things including 2 photons so can the same 2 photons cannot transform back into higgs boson? I highly doubt so but dunno why?
$endgroup$
– user6760
2 hours ago
$begingroup$
Generally, particle physics reactions can go either way. Yes, if you had sufficiently energetic photons appropriately arranged, the SM says they could combine to form a Higgs particle.
$endgroup$
– Bob Jacobsen
2 hours ago
1
$begingroup$
@safesphere the diagram for 2gamma to e+e- certainly exists and has a non-zero amplitude. I agree that phase factors make it small (that’s the “appropriately arranged” bit). But it was a major part of Big Bang thermalization before freeze-out, and its the mechanism for photon to e+e- pair production (via a photon from a nucleus)
$endgroup$
– Bob Jacobsen
1 hour ago
$begingroup$
@safesphere I don't understand why ATLAS should be left out of scope? Photon fusion does occur - (dde.web.cern.ch/dde/presentations/fp420_dec09/…) but if you want to say that photon fusion too rare; there's always the more common gluon fusion? nikhef.nl/pub/services/biblio/preprints/05-007.pdf Or is your problem more with the on-shell-ness of things?
$endgroup$
– Joshua Lin
1 hour ago
1
$begingroup$
@safesphere as G.Smith points out, the amplitude of the diagram is exactly the same. The cross section (probability) and event rate can differ because of the actual ongoing & outgoing particles: it’s easier to make electrons than high energy photons in a small space.
$endgroup$
– Bob Jacobsen
46 mins ago
|
show 6 more comments
$begingroup$
Hi I'm still not clear about this transformation, I just read it is probabilistic so higgs boson can in fact decay into many things including 2 photons so can the same 2 photons cannot transform back into higgs boson? I highly doubt so but dunno why?
$endgroup$
– user6760
2 hours ago
$begingroup$
Generally, particle physics reactions can go either way. Yes, if you had sufficiently energetic photons appropriately arranged, the SM says they could combine to form a Higgs particle.
$endgroup$
– Bob Jacobsen
2 hours ago
1
$begingroup$
@safesphere the diagram for 2gamma to e+e- certainly exists and has a non-zero amplitude. I agree that phase factors make it small (that’s the “appropriately arranged” bit). But it was a major part of Big Bang thermalization before freeze-out, and its the mechanism for photon to e+e- pair production (via a photon from a nucleus)
$endgroup$
– Bob Jacobsen
1 hour ago
$begingroup$
@safesphere I don't understand why ATLAS should be left out of scope? Photon fusion does occur - (dde.web.cern.ch/dde/presentations/fp420_dec09/…) but if you want to say that photon fusion too rare; there's always the more common gluon fusion? nikhef.nl/pub/services/biblio/preprints/05-007.pdf Or is your problem more with the on-shell-ness of things?
$endgroup$
– Joshua Lin
1 hour ago
1
$begingroup$
@safesphere as G.Smith points out, the amplitude of the diagram is exactly the same. The cross section (probability) and event rate can differ because of the actual ongoing & outgoing particles: it’s easier to make electrons than high energy photons in a small space.
$endgroup$
– Bob Jacobsen
46 mins ago
$begingroup$
Hi I'm still not clear about this transformation, I just read it is probabilistic so higgs boson can in fact decay into many things including 2 photons so can the same 2 photons cannot transform back into higgs boson? I highly doubt so but dunno why?
$endgroup$
– user6760
2 hours ago
$begingroup$
Hi I'm still not clear about this transformation, I just read it is probabilistic so higgs boson can in fact decay into many things including 2 photons so can the same 2 photons cannot transform back into higgs boson? I highly doubt so but dunno why?
$endgroup$
– user6760
2 hours ago
$begingroup$
Generally, particle physics reactions can go either way. Yes, if you had sufficiently energetic photons appropriately arranged, the SM says they could combine to form a Higgs particle.
$endgroup$
– Bob Jacobsen
2 hours ago
$begingroup$
Generally, particle physics reactions can go either way. Yes, if you had sufficiently energetic photons appropriately arranged, the SM says they could combine to form a Higgs particle.
$endgroup$
– Bob Jacobsen
2 hours ago
1
1
$begingroup$
@safesphere the diagram for 2gamma to e+e- certainly exists and has a non-zero amplitude. I agree that phase factors make it small (that’s the “appropriately arranged” bit). But it was a major part of Big Bang thermalization before freeze-out, and its the mechanism for photon to e+e- pair production (via a photon from a nucleus)
$endgroup$
– Bob Jacobsen
1 hour ago
$begingroup$
@safesphere the diagram for 2gamma to e+e- certainly exists and has a non-zero amplitude. I agree that phase factors make it small (that’s the “appropriately arranged” bit). But it was a major part of Big Bang thermalization before freeze-out, and its the mechanism for photon to e+e- pair production (via a photon from a nucleus)
$endgroup$
– Bob Jacobsen
1 hour ago
$begingroup$
@safesphere I don't understand why ATLAS should be left out of scope? Photon fusion does occur - (dde.web.cern.ch/dde/presentations/fp420_dec09/…) but if you want to say that photon fusion too rare; there's always the more common gluon fusion? nikhef.nl/pub/services/biblio/preprints/05-007.pdf Or is your problem more with the on-shell-ness of things?
$endgroup$
– Joshua Lin
1 hour ago
$begingroup$
@safesphere I don't understand why ATLAS should be left out of scope? Photon fusion does occur - (dde.web.cern.ch/dde/presentations/fp420_dec09/…) but if you want to say that photon fusion too rare; there's always the more common gluon fusion? nikhef.nl/pub/services/biblio/preprints/05-007.pdf Or is your problem more with the on-shell-ness of things?
$endgroup$
– Joshua Lin
1 hour ago
1
1
$begingroup$
@safesphere as G.Smith points out, the amplitude of the diagram is exactly the same. The cross section (probability) and event rate can differ because of the actual ongoing & outgoing particles: it’s easier to make electrons than high energy photons in a small space.
$endgroup$
– Bob Jacobsen
46 mins ago
$begingroup$
@safesphere as G.Smith points out, the amplitude of the diagram is exactly the same. The cross section (probability) and event rate can differ because of the actual ongoing & outgoing particles: it’s easier to make electrons than high energy photons in a small space.
$endgroup$
– Bob Jacobsen
46 mins ago
|
show 6 more comments
$begingroup$
Another way to answer this question is that particles are not "elementary," not even in a given quantum field theory. Quantum field theories (like the Standard Model) are expressed in terms of fields, not particles. Particles are phenomena that the model predicts; some of them are stable, some are transient (they decay). The Standard Model is constructed using an elementary Higgs field, and it predicts a Higgs particle, which is unstable.
Although the language "elementary particle" is very common and probably can't be revised at this point, it might be less confusing and more accurate to talk about the elementary fields used to express a model. Even that language isn't perfect, though, because some models can be expressed in more than one way, using seemingly-unrelated sets of fields. Quantum field theory is a rich subject with many surprises!
$endgroup$
$begingroup$
are u saying the excitation of the field can disturb other fields too? So the reality is just fields interacting with one another.
$endgroup$
– user6760
2 hours ago
$begingroup$
@user6760 I'll shy away from using the word "reality" here (because different-looking descriptions can make equivalent predictions), but yes: The way quantum field theory describes things is as quantum fields interacting with each other. A particle is one manifestation of all those fields interacting with each other. The Higgs particle involves more than just the Higgs field.
$endgroup$
– Dan Yand
2 hours ago
$begingroup$
@user6760 A common approximation method in QFT involves starting with a different model that has only non-interacting fields, then adding a series of "corrections" to gradually scootch the results closer to what the real model with interacting fields would predict. That's what Feynman diagrams are about, and that's what the "virtual particle" langauge is about. In a model with non-interacting fields, there is a relatively direct correspondence between fields and particles; but that correspondence becomes less direct (to say the least) in models where the fields interact.
$endgroup$
– Dan Yand
1 hour ago
$begingroup$
Yes it makes sense to me now the virtual particle that you have mentioned.
$endgroup$
– user6760
1 hour ago
add a comment |
$begingroup$
Another way to answer this question is that particles are not "elementary," not even in a given quantum field theory. Quantum field theories (like the Standard Model) are expressed in terms of fields, not particles. Particles are phenomena that the model predicts; some of them are stable, some are transient (they decay). The Standard Model is constructed using an elementary Higgs field, and it predicts a Higgs particle, which is unstable.
Although the language "elementary particle" is very common and probably can't be revised at this point, it might be less confusing and more accurate to talk about the elementary fields used to express a model. Even that language isn't perfect, though, because some models can be expressed in more than one way, using seemingly-unrelated sets of fields. Quantum field theory is a rich subject with many surprises!
$endgroup$
$begingroup$
are u saying the excitation of the field can disturb other fields too? So the reality is just fields interacting with one another.
$endgroup$
– user6760
2 hours ago
$begingroup$
@user6760 I'll shy away from using the word "reality" here (because different-looking descriptions can make equivalent predictions), but yes: The way quantum field theory describes things is as quantum fields interacting with each other. A particle is one manifestation of all those fields interacting with each other. The Higgs particle involves more than just the Higgs field.
$endgroup$
– Dan Yand
2 hours ago
$begingroup$
@user6760 A common approximation method in QFT involves starting with a different model that has only non-interacting fields, then adding a series of "corrections" to gradually scootch the results closer to what the real model with interacting fields would predict. That's what Feynman diagrams are about, and that's what the "virtual particle" langauge is about. In a model with non-interacting fields, there is a relatively direct correspondence between fields and particles; but that correspondence becomes less direct (to say the least) in models where the fields interact.
$endgroup$
– Dan Yand
1 hour ago
$begingroup$
Yes it makes sense to me now the virtual particle that you have mentioned.
$endgroup$
– user6760
1 hour ago
add a comment |
$begingroup$
Another way to answer this question is that particles are not "elementary," not even in a given quantum field theory. Quantum field theories (like the Standard Model) are expressed in terms of fields, not particles. Particles are phenomena that the model predicts; some of them are stable, some are transient (they decay). The Standard Model is constructed using an elementary Higgs field, and it predicts a Higgs particle, which is unstable.
Although the language "elementary particle" is very common and probably can't be revised at this point, it might be less confusing and more accurate to talk about the elementary fields used to express a model. Even that language isn't perfect, though, because some models can be expressed in more than one way, using seemingly-unrelated sets of fields. Quantum field theory is a rich subject with many surprises!
$endgroup$
Another way to answer this question is that particles are not "elementary," not even in a given quantum field theory. Quantum field theories (like the Standard Model) are expressed in terms of fields, not particles. Particles are phenomena that the model predicts; some of them are stable, some are transient (they decay). The Standard Model is constructed using an elementary Higgs field, and it predicts a Higgs particle, which is unstable.
Although the language "elementary particle" is very common and probably can't be revised at this point, it might be less confusing and more accurate to talk about the elementary fields used to express a model. Even that language isn't perfect, though, because some models can be expressed in more than one way, using seemingly-unrelated sets of fields. Quantum field theory is a rich subject with many surprises!
answered 2 hours ago
Dan YandDan Yand
8,34211234
8,34211234
$begingroup$
are u saying the excitation of the field can disturb other fields too? So the reality is just fields interacting with one another.
$endgroup$
– user6760
2 hours ago
$begingroup$
@user6760 I'll shy away from using the word "reality" here (because different-looking descriptions can make equivalent predictions), but yes: The way quantum field theory describes things is as quantum fields interacting with each other. A particle is one manifestation of all those fields interacting with each other. The Higgs particle involves more than just the Higgs field.
$endgroup$
– Dan Yand
2 hours ago
$begingroup$
@user6760 A common approximation method in QFT involves starting with a different model that has only non-interacting fields, then adding a series of "corrections" to gradually scootch the results closer to what the real model with interacting fields would predict. That's what Feynman diagrams are about, and that's what the "virtual particle" langauge is about. In a model with non-interacting fields, there is a relatively direct correspondence between fields and particles; but that correspondence becomes less direct (to say the least) in models where the fields interact.
$endgroup$
– Dan Yand
1 hour ago
$begingroup$
Yes it makes sense to me now the virtual particle that you have mentioned.
$endgroup$
– user6760
1 hour ago
add a comment |
$begingroup$
are u saying the excitation of the field can disturb other fields too? So the reality is just fields interacting with one another.
$endgroup$
– user6760
2 hours ago
$begingroup$
@user6760 I'll shy away from using the word "reality" here (because different-looking descriptions can make equivalent predictions), but yes: The way quantum field theory describes things is as quantum fields interacting with each other. A particle is one manifestation of all those fields interacting with each other. The Higgs particle involves more than just the Higgs field.
$endgroup$
– Dan Yand
2 hours ago
$begingroup$
@user6760 A common approximation method in QFT involves starting with a different model that has only non-interacting fields, then adding a series of "corrections" to gradually scootch the results closer to what the real model with interacting fields would predict. That's what Feynman diagrams are about, and that's what the "virtual particle" langauge is about. In a model with non-interacting fields, there is a relatively direct correspondence between fields and particles; but that correspondence becomes less direct (to say the least) in models where the fields interact.
$endgroup$
– Dan Yand
1 hour ago
$begingroup$
Yes it makes sense to me now the virtual particle that you have mentioned.
$endgroup$
– user6760
1 hour ago
$begingroup$
are u saying the excitation of the field can disturb other fields too? So the reality is just fields interacting with one another.
$endgroup$
– user6760
2 hours ago
$begingroup$
are u saying the excitation of the field can disturb other fields too? So the reality is just fields interacting with one another.
$endgroup$
– user6760
2 hours ago
$begingroup$
@user6760 I'll shy away from using the word "reality" here (because different-looking descriptions can make equivalent predictions), but yes: The way quantum field theory describes things is as quantum fields interacting with each other. A particle is one manifestation of all those fields interacting with each other. The Higgs particle involves more than just the Higgs field.
$endgroup$
– Dan Yand
2 hours ago
$begingroup$
@user6760 I'll shy away from using the word "reality" here (because different-looking descriptions can make equivalent predictions), but yes: The way quantum field theory describes things is as quantum fields interacting with each other. A particle is one manifestation of all those fields interacting with each other. The Higgs particle involves more than just the Higgs field.
$endgroup$
– Dan Yand
2 hours ago
$begingroup$
@user6760 A common approximation method in QFT involves starting with a different model that has only non-interacting fields, then adding a series of "corrections" to gradually scootch the results closer to what the real model with interacting fields would predict. That's what Feynman diagrams are about, and that's what the "virtual particle" langauge is about. In a model with non-interacting fields, there is a relatively direct correspondence between fields and particles; but that correspondence becomes less direct (to say the least) in models where the fields interact.
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– Dan Yand
1 hour ago
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@user6760 A common approximation method in QFT involves starting with a different model that has only non-interacting fields, then adding a series of "corrections" to gradually scootch the results closer to what the real model with interacting fields would predict. That's what Feynman diagrams are about, and that's what the "virtual particle" langauge is about. In a model with non-interacting fields, there is a relatively direct correspondence between fields and particles; but that correspondence becomes less direct (to say the least) in models where the fields interact.
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– Dan Yand
1 hour ago
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Yes it makes sense to me now the virtual particle that you have mentioned.
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– user6760
1 hour ago
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Yes it makes sense to me now the virtual particle that you have mentioned.
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– user6760
1 hour ago
add a comment |
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A particle is elementary when there aren't subcomponents that we can identify.
This has nothing to do with the concept of decay, and you can easily convince yourself of this fact by observing that whereas a particle (elementary or not) may decay in many different ways, the number and type of its constituents is univocally determined.
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add a comment |
$begingroup$
A particle is elementary when there aren't subcomponents that we can identify.
This has nothing to do with the concept of decay, and you can easily convince yourself of this fact by observing that whereas a particle (elementary or not) may decay in many different ways, the number and type of its constituents is univocally determined.
$endgroup$
add a comment |
$begingroup$
A particle is elementary when there aren't subcomponents that we can identify.
This has nothing to do with the concept of decay, and you can easily convince yourself of this fact by observing that whereas a particle (elementary or not) may decay in many different ways, the number and type of its constituents is univocally determined.
$endgroup$
A particle is elementary when there aren't subcomponents that we can identify.
This has nothing to do with the concept of decay, and you can easily convince yourself of this fact by observing that whereas a particle (elementary or not) may decay in many different ways, the number and type of its constituents is univocally determined.
answered 2 hours ago
Francesco BernardiniFrancesco Bernardini
4345
4345
add a comment |
add a comment |
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