Can the center of charge and center of mass of an electron differ in quantum mechanics?
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Traditionally for a free electron, we presume the expectation of its location (place of the center of mass) and the center of charge at the same place. Although this seemed to be reasonable for a classical approximation
(see: Why isn't there a centre of charge? by Lagerbaer), I wasn't sure if it's appropriate for quantum models, and especially for some extreme cases, such as high energy and quark models.
My questions are:
Is there any experimental evidence to support or suspect that the center of mass and charge of an electron must coincide?
Is there any mathematical proof that says the center of mass and charge of an electron must coincide? Or are they permitted to be separated? (By electric field equation from EM, it didn't give enough evidence to separate $E$ field with $G$ field. But I don't think it's the same case in quantum or standard model, i.e. although electrons are leptons, consider $uud$ with $2/3,2/3,-1/3$ charges.)
What's the implication for dynamics if the expectation of centers does not coincide?
electromagnetism mass charge field-theory point-particles
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up vote
15
down vote
favorite
Traditionally for a free electron, we presume the expectation of its location (place of the center of mass) and the center of charge at the same place. Although this seemed to be reasonable for a classical approximation
(see: Why isn't there a centre of charge? by Lagerbaer), I wasn't sure if it's appropriate for quantum models, and especially for some extreme cases, such as high energy and quark models.
My questions are:
Is there any experimental evidence to support or suspect that the center of mass and charge of an electron must coincide?
Is there any mathematical proof that says the center of mass and charge of an electron must coincide? Or are they permitted to be separated? (By electric field equation from EM, it didn't give enough evidence to separate $E$ field with $G$ field. But I don't think it's the same case in quantum or standard model, i.e. although electrons are leptons, consider $uud$ with $2/3,2/3,-1/3$ charges.)
What's the implication for dynamics if the expectation of centers does not coincide?
electromagnetism mass charge field-theory point-particles
add a comment |Â
up vote
15
down vote
favorite
up vote
15
down vote
favorite
Traditionally for a free electron, we presume the expectation of its location (place of the center of mass) and the center of charge at the same place. Although this seemed to be reasonable for a classical approximation
(see: Why isn't there a centre of charge? by Lagerbaer), I wasn't sure if it's appropriate for quantum models, and especially for some extreme cases, such as high energy and quark models.
My questions are:
Is there any experimental evidence to support or suspect that the center of mass and charge of an electron must coincide?
Is there any mathematical proof that says the center of mass and charge of an electron must coincide? Or are they permitted to be separated? (By electric field equation from EM, it didn't give enough evidence to separate $E$ field with $G$ field. But I don't think it's the same case in quantum or standard model, i.e. although electrons are leptons, consider $uud$ with $2/3,2/3,-1/3$ charges.)
What's the implication for dynamics if the expectation of centers does not coincide?
electromagnetism mass charge field-theory point-particles
Traditionally for a free electron, we presume the expectation of its location (place of the center of mass) and the center of charge at the same place. Although this seemed to be reasonable for a classical approximation
(see: Why isn't there a centre of charge? by Lagerbaer), I wasn't sure if it's appropriate for quantum models, and especially for some extreme cases, such as high energy and quark models.
My questions are:
Is there any experimental evidence to support or suspect that the center of mass and charge of an electron must coincide?
Is there any mathematical proof that says the center of mass and charge of an electron must coincide? Or are they permitted to be separated? (By electric field equation from EM, it didn't give enough evidence to separate $E$ field with $G$ field. But I don't think it's the same case in quantum or standard model, i.e. although electrons are leptons, consider $uud$ with $2/3,2/3,-1/3$ charges.)
What's the implication for dynamics if the expectation of centers does not coincide?
electromagnetism mass charge field-theory point-particles
electromagnetism mass charge field-theory point-particles
edited 20 mins ago
ACuriousMindâ¦
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68.1k17118290
asked 11 hours ago
J C
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3 Answers
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active
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up vote
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accepted
Can the center of charge and center of mass of an electron differ in quantum mechanics?
They can. Particle physics does allow for electrons (and other point particles) to have their centers of mass and charge in different locations, which would give them an intrinsic electric dipole moment. For the electron, this is unsurprisingly known as the electron electric dipole moment (eEDM), and it is an important parameter in various theories.
The basic picture to keep in mind is something like this:
Image source
Now, because of complicated reasons caused by quantum mechanics, this dipole moment (the vector between the center of mass and the center of charge) needs to be aligned with the spin, though the question of which point the dipole moment uses as a reference isn't all that trivial. (Apologies for how technical that second answer is - I raised a bounty to attract more accessible responses but none came.) Still, complications aside, it is a perfectly standard concept.
That said, the presence of a nonzero electron electric dipole moment does have some important consequences, because this eEDM marks a violation of both parity and time-reversal symmetries. This is because the dipole moment $mathbf d_e$ must be parallel to the spin $mathbf S$, but the two behave differently under the two symmetries (i.e. $mathbf d_e$ is a vector while $mathbf S$ is a pseudovector; $mathbf d_e$ is time-even while $mathbf S$ is time-odd) which means that their projection $mathbf d_ecdotmathbf S$ changes sign under both $P$ and $T$ symmetries, and that is only possible if the theory contains those symmetry violations from the outset.
As luck would have it, the Standard Model of particle physics does contain violations of both of those symmetries, coming from the weak interaction, and this means that the SM does predict a nonzero value for the eEDM, which falls in at about $d_e sim 10^-40 ecdotmathrm m$. For comparison, the proton sizes in at about $10^-15:mathrm m$, a full 25 orders of magnitude bigger than that separation, which should be a hint at just how small the SM's prediction for the eEDM is (i.e. it is absolutely tiny). Because of this small size, this SM prediction has yet to be measured.
On the other hand, there's multiple theories that extend the Standard Model in various directions, particularly to deal with things like baryogenesis where we observe the universe to have much more asymmetry (say, having much more matter than antimatter) than what the Standard Model predicts. And because things have consequences, those theories $-$ the various variants of supersymmetry, and their competitors $-$ generally predict much larger values for the eEDM than what the SM does: more on the order of $d_e sim 10^-30 ecdotmathrm m$, which do fall within the range that we can measure.
How do you actually measure them? Basically, by forgetting about high-energy particle colliders (which would need much higher collision energies than they can currently achieve to detect those dipole moments), and turning instead to the precision spectroscopy of atoms and molecules, and how they respond to external electric fields. The main physics at play here is that an electric dipole $mathbf d$ in the presence of an external electric field $mathbf E$ acquires an energy
$$
U = -mathbf dcdot mathbf E,
$$
and this produces a (minuscule) shift in the energies of the various quantum states of the electrons in atoms and molecules, which can then be detected using spectroscopy. (For a basic introduction, see this video; for more technical material see e.g. this talk or this one.)
The bottom line, though, as regards this,
Is there any experimental evidence to support or suspect the center of mass and charge of an electron must coincide?
is that the current experimental results provide bounds for the eEDM, which has been demonstrated to be no larger than $|d_e|<8.7times 10^âÂÂ31: e cdotmathrmm$ (i.e. the current experimental results are consistent with $d_e=0$), but the experimental search continues. We know that there must be some spatial separation between the electron's centers of mass and charge, and there are several huge experimental campaigns currently running to try and measure it, but (as is often the case) the only results so far are constraints on the values that it doesn't have.
Nice answer, perhaps you could mention at the end an example or two of experiments where this is being measured? (I personally don't know)
â Kai
1 hour ago
@Kai See the talks already linked to.
â Emilio Pisanty
1 hour ago
Can the center of electric charge, and color charge differ in a quark?
â Anders Gustafson
13 mins ago
@AndersGustafson My knowledge of SU(3) theory is nowhere near up to scratch to answer that. It's an interesting question; you should ask it separately.
â Emilio Pisanty
11 mins ago
add a comment |Â
up vote
6
down vote
For the simple reason that the current standard model of particle physics has the electron as a point particle, i.e. volume =0 , and the charge,spin and mass all reside at that zero point. The same is true for all particles in the table. The model is validated continually by experiments, and is the mainstream one at this time.
1)Is there any experimental evidence to support or suspect the center of mass and charge of an electron must coincide ?
When one defines a point particle mathematically, as in the standard model, it is a mathematical constraint.
Please note that the statement " the center of mass and the center of charge must be the same", can arise by mathematical symmetry arguments. Even if charge distributions vary in composite objects, depending on the geometry, the symmetry also for free particles will mathematically give a coincidence.
This answers 2) also
What's the implication for dynamics if the expectation of centers does not coincide
It might be connected with the hypothesis of compositeness, i.e. that the elementary particles are not elementary, but have an internal structure. One would need an experiment that would distort the mathematical symmetry of the charge distribution, possibly with a strong electric field, and a model where the point particle and the composite hypothetical charge interactions are studied.
There are limits given by experiments on the compositeness scale. See my answer here to a related question.
Even if it turns out that elementary particles at some high scale display compositness, I would be surpised if they would display asymmetry in the charge distribution versus the mass distribution.
This answer is rather wide of the mark, I think. You do not need to assume any compositeness hypothesis to have a nonzero electron dipole model (which is the only serious way to understand "the centers of mass and charge do not coincide"), and indeed the Standard Model already predicts a nonzero separation. (It's some ten orders of magnitude beyond the current molecular-spectroscopy experiments, but still.)
â Emilio Pisanty
6 hours ago
As for the claim that "symmetry arguments" entail that the center of mass and the center of charge must be the same -- I don't doubt that one can come up with such arguments, but they'd be wrong. The electron isn't symmetric enough (it has spin) and the SM isn't symmetric enough (it contains both P, T, and C violations) to provide enough symmetry grounds for such an argument to hold. This is clearly seen in the fact that the SM predicts a nonzero eEDM.
â Emilio Pisanty
6 hours ago
@EmilioPisanty please enlighten me , isn't the quantum mechanical charge distribution of a dipole symmetric? The center would be at the center which would coincide with the center of mass distribution as seen in the link I gave for the molecules. Maybe we have a different definition? The center of mass of a rod is at the center. A charged rod + on one side - on another would be a dipole, but the center of charge would be at the center of the rod.
â anna v
5 hours ago
In my definition one would need more charge on one side in order to have a different center of charge to center of mass.
â anna v
5 hours ago
@annav To the extent that classical pictures make sense (which is obviously extremely limited), the symmetric dipolar charge distribution is entirely the wrong model; the correct mental picture is an offset between the charge distribution and the mass distribution, as shown at the 2:30-2:45 mark in this video. Perhaps you're thinking that only neutral systems can have dipole moments? That's a common misconception, but it's just not true.
â Emilio Pisanty
5 hours ago
 |Â
show 5 more comments
up vote
-1
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you'd see that in the bubble/cloud chamber, if the center of mass and charge were different, then you'd have some torque effect that would completely change the electrons trajectories(when they are under electric/magnetic field).
add a comment |Â
3 Answers
3
active
oldest
votes
3 Answers
3
active
oldest
votes
active
oldest
votes
active
oldest
votes
up vote
18
down vote
accepted
Can the center of charge and center of mass of an electron differ in quantum mechanics?
They can. Particle physics does allow for electrons (and other point particles) to have their centers of mass and charge in different locations, which would give them an intrinsic electric dipole moment. For the electron, this is unsurprisingly known as the electron electric dipole moment (eEDM), and it is an important parameter in various theories.
The basic picture to keep in mind is something like this:
Image source
Now, because of complicated reasons caused by quantum mechanics, this dipole moment (the vector between the center of mass and the center of charge) needs to be aligned with the spin, though the question of which point the dipole moment uses as a reference isn't all that trivial. (Apologies for how technical that second answer is - I raised a bounty to attract more accessible responses but none came.) Still, complications aside, it is a perfectly standard concept.
That said, the presence of a nonzero electron electric dipole moment does have some important consequences, because this eEDM marks a violation of both parity and time-reversal symmetries. This is because the dipole moment $mathbf d_e$ must be parallel to the spin $mathbf S$, but the two behave differently under the two symmetries (i.e. $mathbf d_e$ is a vector while $mathbf S$ is a pseudovector; $mathbf d_e$ is time-even while $mathbf S$ is time-odd) which means that their projection $mathbf d_ecdotmathbf S$ changes sign under both $P$ and $T$ symmetries, and that is only possible if the theory contains those symmetry violations from the outset.
As luck would have it, the Standard Model of particle physics does contain violations of both of those symmetries, coming from the weak interaction, and this means that the SM does predict a nonzero value for the eEDM, which falls in at about $d_e sim 10^-40 ecdotmathrm m$. For comparison, the proton sizes in at about $10^-15:mathrm m$, a full 25 orders of magnitude bigger than that separation, which should be a hint at just how small the SM's prediction for the eEDM is (i.e. it is absolutely tiny). Because of this small size, this SM prediction has yet to be measured.
On the other hand, there's multiple theories that extend the Standard Model in various directions, particularly to deal with things like baryogenesis where we observe the universe to have much more asymmetry (say, having much more matter than antimatter) than what the Standard Model predicts. And because things have consequences, those theories $-$ the various variants of supersymmetry, and their competitors $-$ generally predict much larger values for the eEDM than what the SM does: more on the order of $d_e sim 10^-30 ecdotmathrm m$, which do fall within the range that we can measure.
How do you actually measure them? Basically, by forgetting about high-energy particle colliders (which would need much higher collision energies than they can currently achieve to detect those dipole moments), and turning instead to the precision spectroscopy of atoms and molecules, and how they respond to external electric fields. The main physics at play here is that an electric dipole $mathbf d$ in the presence of an external electric field $mathbf E$ acquires an energy
$$
U = -mathbf dcdot mathbf E,
$$
and this produces a (minuscule) shift in the energies of the various quantum states of the electrons in atoms and molecules, which can then be detected using spectroscopy. (For a basic introduction, see this video; for more technical material see e.g. this talk or this one.)
The bottom line, though, as regards this,
Is there any experimental evidence to support or suspect the center of mass and charge of an electron must coincide?
is that the current experimental results provide bounds for the eEDM, which has been demonstrated to be no larger than $|d_e|<8.7times 10^âÂÂ31: e cdotmathrmm$ (i.e. the current experimental results are consistent with $d_e=0$), but the experimental search continues. We know that there must be some spatial separation between the electron's centers of mass and charge, and there are several huge experimental campaigns currently running to try and measure it, but (as is often the case) the only results so far are constraints on the values that it doesn't have.
Nice answer, perhaps you could mention at the end an example or two of experiments where this is being measured? (I personally don't know)
â Kai
1 hour ago
@Kai See the talks already linked to.
â Emilio Pisanty
1 hour ago
Can the center of electric charge, and color charge differ in a quark?
â Anders Gustafson
13 mins ago
@AndersGustafson My knowledge of SU(3) theory is nowhere near up to scratch to answer that. It's an interesting question; you should ask it separately.
â Emilio Pisanty
11 mins ago
add a comment |Â
up vote
18
down vote
accepted
Can the center of charge and center of mass of an electron differ in quantum mechanics?
They can. Particle physics does allow for electrons (and other point particles) to have their centers of mass and charge in different locations, which would give them an intrinsic electric dipole moment. For the electron, this is unsurprisingly known as the electron electric dipole moment (eEDM), and it is an important parameter in various theories.
The basic picture to keep in mind is something like this:
Image source
Now, because of complicated reasons caused by quantum mechanics, this dipole moment (the vector between the center of mass and the center of charge) needs to be aligned with the spin, though the question of which point the dipole moment uses as a reference isn't all that trivial. (Apologies for how technical that second answer is - I raised a bounty to attract more accessible responses but none came.) Still, complications aside, it is a perfectly standard concept.
That said, the presence of a nonzero electron electric dipole moment does have some important consequences, because this eEDM marks a violation of both parity and time-reversal symmetries. This is because the dipole moment $mathbf d_e$ must be parallel to the spin $mathbf S$, but the two behave differently under the two symmetries (i.e. $mathbf d_e$ is a vector while $mathbf S$ is a pseudovector; $mathbf d_e$ is time-even while $mathbf S$ is time-odd) which means that their projection $mathbf d_ecdotmathbf S$ changes sign under both $P$ and $T$ symmetries, and that is only possible if the theory contains those symmetry violations from the outset.
As luck would have it, the Standard Model of particle physics does contain violations of both of those symmetries, coming from the weak interaction, and this means that the SM does predict a nonzero value for the eEDM, which falls in at about $d_e sim 10^-40 ecdotmathrm m$. For comparison, the proton sizes in at about $10^-15:mathrm m$, a full 25 orders of magnitude bigger than that separation, which should be a hint at just how small the SM's prediction for the eEDM is (i.e. it is absolutely tiny). Because of this small size, this SM prediction has yet to be measured.
On the other hand, there's multiple theories that extend the Standard Model in various directions, particularly to deal with things like baryogenesis where we observe the universe to have much more asymmetry (say, having much more matter than antimatter) than what the Standard Model predicts. And because things have consequences, those theories $-$ the various variants of supersymmetry, and their competitors $-$ generally predict much larger values for the eEDM than what the SM does: more on the order of $d_e sim 10^-30 ecdotmathrm m$, which do fall within the range that we can measure.
How do you actually measure them? Basically, by forgetting about high-energy particle colliders (which would need much higher collision energies than they can currently achieve to detect those dipole moments), and turning instead to the precision spectroscopy of atoms and molecules, and how they respond to external electric fields. The main physics at play here is that an electric dipole $mathbf d$ in the presence of an external electric field $mathbf E$ acquires an energy
$$
U = -mathbf dcdot mathbf E,
$$
and this produces a (minuscule) shift in the energies of the various quantum states of the electrons in atoms and molecules, which can then be detected using spectroscopy. (For a basic introduction, see this video; for more technical material see e.g. this talk or this one.)
The bottom line, though, as regards this,
Is there any experimental evidence to support or suspect the center of mass and charge of an electron must coincide?
is that the current experimental results provide bounds for the eEDM, which has been demonstrated to be no larger than $|d_e|<8.7times 10^âÂÂ31: e cdotmathrmm$ (i.e. the current experimental results are consistent with $d_e=0$), but the experimental search continues. We know that there must be some spatial separation between the electron's centers of mass and charge, and there are several huge experimental campaigns currently running to try and measure it, but (as is often the case) the only results so far are constraints on the values that it doesn't have.
Nice answer, perhaps you could mention at the end an example or two of experiments where this is being measured? (I personally don't know)
â Kai
1 hour ago
@Kai See the talks already linked to.
â Emilio Pisanty
1 hour ago
Can the center of electric charge, and color charge differ in a quark?
â Anders Gustafson
13 mins ago
@AndersGustafson My knowledge of SU(3) theory is nowhere near up to scratch to answer that. It's an interesting question; you should ask it separately.
â Emilio Pisanty
11 mins ago
add a comment |Â
up vote
18
down vote
accepted
up vote
18
down vote
accepted
Can the center of charge and center of mass of an electron differ in quantum mechanics?
They can. Particle physics does allow for electrons (and other point particles) to have their centers of mass and charge in different locations, which would give them an intrinsic electric dipole moment. For the electron, this is unsurprisingly known as the electron electric dipole moment (eEDM), and it is an important parameter in various theories.
The basic picture to keep in mind is something like this:
Image source
Now, because of complicated reasons caused by quantum mechanics, this dipole moment (the vector between the center of mass and the center of charge) needs to be aligned with the spin, though the question of which point the dipole moment uses as a reference isn't all that trivial. (Apologies for how technical that second answer is - I raised a bounty to attract more accessible responses but none came.) Still, complications aside, it is a perfectly standard concept.
That said, the presence of a nonzero electron electric dipole moment does have some important consequences, because this eEDM marks a violation of both parity and time-reversal symmetries. This is because the dipole moment $mathbf d_e$ must be parallel to the spin $mathbf S$, but the two behave differently under the two symmetries (i.e. $mathbf d_e$ is a vector while $mathbf S$ is a pseudovector; $mathbf d_e$ is time-even while $mathbf S$ is time-odd) which means that their projection $mathbf d_ecdotmathbf S$ changes sign under both $P$ and $T$ symmetries, and that is only possible if the theory contains those symmetry violations from the outset.
As luck would have it, the Standard Model of particle physics does contain violations of both of those symmetries, coming from the weak interaction, and this means that the SM does predict a nonzero value for the eEDM, which falls in at about $d_e sim 10^-40 ecdotmathrm m$. For comparison, the proton sizes in at about $10^-15:mathrm m$, a full 25 orders of magnitude bigger than that separation, which should be a hint at just how small the SM's prediction for the eEDM is (i.e. it is absolutely tiny). Because of this small size, this SM prediction has yet to be measured.
On the other hand, there's multiple theories that extend the Standard Model in various directions, particularly to deal with things like baryogenesis where we observe the universe to have much more asymmetry (say, having much more matter than antimatter) than what the Standard Model predicts. And because things have consequences, those theories $-$ the various variants of supersymmetry, and their competitors $-$ generally predict much larger values for the eEDM than what the SM does: more on the order of $d_e sim 10^-30 ecdotmathrm m$, which do fall within the range that we can measure.
How do you actually measure them? Basically, by forgetting about high-energy particle colliders (which would need much higher collision energies than they can currently achieve to detect those dipole moments), and turning instead to the precision spectroscopy of atoms and molecules, and how they respond to external electric fields. The main physics at play here is that an electric dipole $mathbf d$ in the presence of an external electric field $mathbf E$ acquires an energy
$$
U = -mathbf dcdot mathbf E,
$$
and this produces a (minuscule) shift in the energies of the various quantum states of the electrons in atoms and molecules, which can then be detected using spectroscopy. (For a basic introduction, see this video; for more technical material see e.g. this talk or this one.)
The bottom line, though, as regards this,
Is there any experimental evidence to support or suspect the center of mass and charge of an electron must coincide?
is that the current experimental results provide bounds for the eEDM, which has been demonstrated to be no larger than $|d_e|<8.7times 10^âÂÂ31: e cdotmathrmm$ (i.e. the current experimental results are consistent with $d_e=0$), but the experimental search continues. We know that there must be some spatial separation between the electron's centers of mass and charge, and there are several huge experimental campaigns currently running to try and measure it, but (as is often the case) the only results so far are constraints on the values that it doesn't have.
Can the center of charge and center of mass of an electron differ in quantum mechanics?
They can. Particle physics does allow for electrons (and other point particles) to have their centers of mass and charge in different locations, which would give them an intrinsic electric dipole moment. For the electron, this is unsurprisingly known as the electron electric dipole moment (eEDM), and it is an important parameter in various theories.
The basic picture to keep in mind is something like this:
Image source
Now, because of complicated reasons caused by quantum mechanics, this dipole moment (the vector between the center of mass and the center of charge) needs to be aligned with the spin, though the question of which point the dipole moment uses as a reference isn't all that trivial. (Apologies for how technical that second answer is - I raised a bounty to attract more accessible responses but none came.) Still, complications aside, it is a perfectly standard concept.
That said, the presence of a nonzero electron electric dipole moment does have some important consequences, because this eEDM marks a violation of both parity and time-reversal symmetries. This is because the dipole moment $mathbf d_e$ must be parallel to the spin $mathbf S$, but the two behave differently under the two symmetries (i.e. $mathbf d_e$ is a vector while $mathbf S$ is a pseudovector; $mathbf d_e$ is time-even while $mathbf S$ is time-odd) which means that their projection $mathbf d_ecdotmathbf S$ changes sign under both $P$ and $T$ symmetries, and that is only possible if the theory contains those symmetry violations from the outset.
As luck would have it, the Standard Model of particle physics does contain violations of both of those symmetries, coming from the weak interaction, and this means that the SM does predict a nonzero value for the eEDM, which falls in at about $d_e sim 10^-40 ecdotmathrm m$. For comparison, the proton sizes in at about $10^-15:mathrm m$, a full 25 orders of magnitude bigger than that separation, which should be a hint at just how small the SM's prediction for the eEDM is (i.e. it is absolutely tiny). Because of this small size, this SM prediction has yet to be measured.
On the other hand, there's multiple theories that extend the Standard Model in various directions, particularly to deal with things like baryogenesis where we observe the universe to have much more asymmetry (say, having much more matter than antimatter) than what the Standard Model predicts. And because things have consequences, those theories $-$ the various variants of supersymmetry, and their competitors $-$ generally predict much larger values for the eEDM than what the SM does: more on the order of $d_e sim 10^-30 ecdotmathrm m$, which do fall within the range that we can measure.
How do you actually measure them? Basically, by forgetting about high-energy particle colliders (which would need much higher collision energies than they can currently achieve to detect those dipole moments), and turning instead to the precision spectroscopy of atoms and molecules, and how they respond to external electric fields. The main physics at play here is that an electric dipole $mathbf d$ in the presence of an external electric field $mathbf E$ acquires an energy
$$
U = -mathbf dcdot mathbf E,
$$
and this produces a (minuscule) shift in the energies of the various quantum states of the electrons in atoms and molecules, which can then be detected using spectroscopy. (For a basic introduction, see this video; for more technical material see e.g. this talk or this one.)
The bottom line, though, as regards this,
Is there any experimental evidence to support or suspect the center of mass and charge of an electron must coincide?
is that the current experimental results provide bounds for the eEDM, which has been demonstrated to be no larger than $|d_e|<8.7times 10^âÂÂ31: e cdotmathrmm$ (i.e. the current experimental results are consistent with $d_e=0$), but the experimental search continues. We know that there must be some spatial separation between the electron's centers of mass and charge, and there are several huge experimental campaigns currently running to try and measure it, but (as is often the case) the only results so far are constraints on the values that it doesn't have.
edited 17 mins ago
answered 7 hours ago
Emilio Pisanty
75.6k18180372
75.6k18180372
Nice answer, perhaps you could mention at the end an example or two of experiments where this is being measured? (I personally don't know)
â Kai
1 hour ago
@Kai See the talks already linked to.
â Emilio Pisanty
1 hour ago
Can the center of electric charge, and color charge differ in a quark?
â Anders Gustafson
13 mins ago
@AndersGustafson My knowledge of SU(3) theory is nowhere near up to scratch to answer that. It's an interesting question; you should ask it separately.
â Emilio Pisanty
11 mins ago
add a comment |Â
Nice answer, perhaps you could mention at the end an example or two of experiments where this is being measured? (I personally don't know)
â Kai
1 hour ago
@Kai See the talks already linked to.
â Emilio Pisanty
1 hour ago
Can the center of electric charge, and color charge differ in a quark?
â Anders Gustafson
13 mins ago
@AndersGustafson My knowledge of SU(3) theory is nowhere near up to scratch to answer that. It's an interesting question; you should ask it separately.
â Emilio Pisanty
11 mins ago
Nice answer, perhaps you could mention at the end an example or two of experiments where this is being measured? (I personally don't know)
â Kai
1 hour ago
Nice answer, perhaps you could mention at the end an example or two of experiments where this is being measured? (I personally don't know)
â Kai
1 hour ago
@Kai See the talks already linked to.
â Emilio Pisanty
1 hour ago
@Kai See the talks already linked to.
â Emilio Pisanty
1 hour ago
Can the center of electric charge, and color charge differ in a quark?
â Anders Gustafson
13 mins ago
Can the center of electric charge, and color charge differ in a quark?
â Anders Gustafson
13 mins ago
@AndersGustafson My knowledge of SU(3) theory is nowhere near up to scratch to answer that. It's an interesting question; you should ask it separately.
â Emilio Pisanty
11 mins ago
@AndersGustafson My knowledge of SU(3) theory is nowhere near up to scratch to answer that. It's an interesting question; you should ask it separately.
â Emilio Pisanty
11 mins ago
add a comment |Â
up vote
6
down vote
For the simple reason that the current standard model of particle physics has the electron as a point particle, i.e. volume =0 , and the charge,spin and mass all reside at that zero point. The same is true for all particles in the table. The model is validated continually by experiments, and is the mainstream one at this time.
1)Is there any experimental evidence to support or suspect the center of mass and charge of an electron must coincide ?
When one defines a point particle mathematically, as in the standard model, it is a mathematical constraint.
Please note that the statement " the center of mass and the center of charge must be the same", can arise by mathematical symmetry arguments. Even if charge distributions vary in composite objects, depending on the geometry, the symmetry also for free particles will mathematically give a coincidence.
This answers 2) also
What's the implication for dynamics if the expectation of centers does not coincide
It might be connected with the hypothesis of compositeness, i.e. that the elementary particles are not elementary, but have an internal structure. One would need an experiment that would distort the mathematical symmetry of the charge distribution, possibly with a strong electric field, and a model where the point particle and the composite hypothetical charge interactions are studied.
There are limits given by experiments on the compositeness scale. See my answer here to a related question.
Even if it turns out that elementary particles at some high scale display compositness, I would be surpised if they would display asymmetry in the charge distribution versus the mass distribution.
This answer is rather wide of the mark, I think. You do not need to assume any compositeness hypothesis to have a nonzero electron dipole model (which is the only serious way to understand "the centers of mass and charge do not coincide"), and indeed the Standard Model already predicts a nonzero separation. (It's some ten orders of magnitude beyond the current molecular-spectroscopy experiments, but still.)
â Emilio Pisanty
6 hours ago
As for the claim that "symmetry arguments" entail that the center of mass and the center of charge must be the same -- I don't doubt that one can come up with such arguments, but they'd be wrong. The electron isn't symmetric enough (it has spin) and the SM isn't symmetric enough (it contains both P, T, and C violations) to provide enough symmetry grounds for such an argument to hold. This is clearly seen in the fact that the SM predicts a nonzero eEDM.
â Emilio Pisanty
6 hours ago
@EmilioPisanty please enlighten me , isn't the quantum mechanical charge distribution of a dipole symmetric? The center would be at the center which would coincide with the center of mass distribution as seen in the link I gave for the molecules. Maybe we have a different definition? The center of mass of a rod is at the center. A charged rod + on one side - on another would be a dipole, but the center of charge would be at the center of the rod.
â anna v
5 hours ago
In my definition one would need more charge on one side in order to have a different center of charge to center of mass.
â anna v
5 hours ago
@annav To the extent that classical pictures make sense (which is obviously extremely limited), the symmetric dipolar charge distribution is entirely the wrong model; the correct mental picture is an offset between the charge distribution and the mass distribution, as shown at the 2:30-2:45 mark in this video. Perhaps you're thinking that only neutral systems can have dipole moments? That's a common misconception, but it's just not true.
â Emilio Pisanty
5 hours ago
 |Â
show 5 more comments
up vote
6
down vote
For the simple reason that the current standard model of particle physics has the electron as a point particle, i.e. volume =0 , and the charge,spin and mass all reside at that zero point. The same is true for all particles in the table. The model is validated continually by experiments, and is the mainstream one at this time.
1)Is there any experimental evidence to support or suspect the center of mass and charge of an electron must coincide ?
When one defines a point particle mathematically, as in the standard model, it is a mathematical constraint.
Please note that the statement " the center of mass and the center of charge must be the same", can arise by mathematical symmetry arguments. Even if charge distributions vary in composite objects, depending on the geometry, the symmetry also for free particles will mathematically give a coincidence.
This answers 2) also
What's the implication for dynamics if the expectation of centers does not coincide
It might be connected with the hypothesis of compositeness, i.e. that the elementary particles are not elementary, but have an internal structure. One would need an experiment that would distort the mathematical symmetry of the charge distribution, possibly with a strong electric field, and a model where the point particle and the composite hypothetical charge interactions are studied.
There are limits given by experiments on the compositeness scale. See my answer here to a related question.
Even if it turns out that elementary particles at some high scale display compositness, I would be surpised if they would display asymmetry in the charge distribution versus the mass distribution.
This answer is rather wide of the mark, I think. You do not need to assume any compositeness hypothesis to have a nonzero electron dipole model (which is the only serious way to understand "the centers of mass and charge do not coincide"), and indeed the Standard Model already predicts a nonzero separation. (It's some ten orders of magnitude beyond the current molecular-spectroscopy experiments, but still.)
â Emilio Pisanty
6 hours ago
As for the claim that "symmetry arguments" entail that the center of mass and the center of charge must be the same -- I don't doubt that one can come up with such arguments, but they'd be wrong. The electron isn't symmetric enough (it has spin) and the SM isn't symmetric enough (it contains both P, T, and C violations) to provide enough symmetry grounds for such an argument to hold. This is clearly seen in the fact that the SM predicts a nonzero eEDM.
â Emilio Pisanty
6 hours ago
@EmilioPisanty please enlighten me , isn't the quantum mechanical charge distribution of a dipole symmetric? The center would be at the center which would coincide with the center of mass distribution as seen in the link I gave for the molecules. Maybe we have a different definition? The center of mass of a rod is at the center. A charged rod + on one side - on another would be a dipole, but the center of charge would be at the center of the rod.
â anna v
5 hours ago
In my definition one would need more charge on one side in order to have a different center of charge to center of mass.
â anna v
5 hours ago
@annav To the extent that classical pictures make sense (which is obviously extremely limited), the symmetric dipolar charge distribution is entirely the wrong model; the correct mental picture is an offset between the charge distribution and the mass distribution, as shown at the 2:30-2:45 mark in this video. Perhaps you're thinking that only neutral systems can have dipole moments? That's a common misconception, but it's just not true.
â Emilio Pisanty
5 hours ago
 |Â
show 5 more comments
up vote
6
down vote
up vote
6
down vote
For the simple reason that the current standard model of particle physics has the electron as a point particle, i.e. volume =0 , and the charge,spin and mass all reside at that zero point. The same is true for all particles in the table. The model is validated continually by experiments, and is the mainstream one at this time.
1)Is there any experimental evidence to support or suspect the center of mass and charge of an electron must coincide ?
When one defines a point particle mathematically, as in the standard model, it is a mathematical constraint.
Please note that the statement " the center of mass and the center of charge must be the same", can arise by mathematical symmetry arguments. Even if charge distributions vary in composite objects, depending on the geometry, the symmetry also for free particles will mathematically give a coincidence.
This answers 2) also
What's the implication for dynamics if the expectation of centers does not coincide
It might be connected with the hypothesis of compositeness, i.e. that the elementary particles are not elementary, but have an internal structure. One would need an experiment that would distort the mathematical symmetry of the charge distribution, possibly with a strong electric field, and a model where the point particle and the composite hypothetical charge interactions are studied.
There are limits given by experiments on the compositeness scale. See my answer here to a related question.
Even if it turns out that elementary particles at some high scale display compositness, I would be surpised if they would display asymmetry in the charge distribution versus the mass distribution.
For the simple reason that the current standard model of particle physics has the electron as a point particle, i.e. volume =0 , and the charge,spin and mass all reside at that zero point. The same is true for all particles in the table. The model is validated continually by experiments, and is the mainstream one at this time.
1)Is there any experimental evidence to support or suspect the center of mass and charge of an electron must coincide ?
When one defines a point particle mathematically, as in the standard model, it is a mathematical constraint.
Please note that the statement " the center of mass and the center of charge must be the same", can arise by mathematical symmetry arguments. Even if charge distributions vary in composite objects, depending on the geometry, the symmetry also for free particles will mathematically give a coincidence.
This answers 2) also
What's the implication for dynamics if the expectation of centers does not coincide
It might be connected with the hypothesis of compositeness, i.e. that the elementary particles are not elementary, but have an internal structure. One would need an experiment that would distort the mathematical symmetry of the charge distribution, possibly with a strong electric field, and a model where the point particle and the composite hypothetical charge interactions are studied.
There are limits given by experiments on the compositeness scale. See my answer here to a related question.
Even if it turns out that elementary particles at some high scale display compositness, I would be surpised if they would display asymmetry in the charge distribution versus the mass distribution.
answered 8 hours ago
anna v
151k7144432
151k7144432
This answer is rather wide of the mark, I think. You do not need to assume any compositeness hypothesis to have a nonzero electron dipole model (which is the only serious way to understand "the centers of mass and charge do not coincide"), and indeed the Standard Model already predicts a nonzero separation. (It's some ten orders of magnitude beyond the current molecular-spectroscopy experiments, but still.)
â Emilio Pisanty
6 hours ago
As for the claim that "symmetry arguments" entail that the center of mass and the center of charge must be the same -- I don't doubt that one can come up with such arguments, but they'd be wrong. The electron isn't symmetric enough (it has spin) and the SM isn't symmetric enough (it contains both P, T, and C violations) to provide enough symmetry grounds for such an argument to hold. This is clearly seen in the fact that the SM predicts a nonzero eEDM.
â Emilio Pisanty
6 hours ago
@EmilioPisanty please enlighten me , isn't the quantum mechanical charge distribution of a dipole symmetric? The center would be at the center which would coincide with the center of mass distribution as seen in the link I gave for the molecules. Maybe we have a different definition? The center of mass of a rod is at the center. A charged rod + on one side - on another would be a dipole, but the center of charge would be at the center of the rod.
â anna v
5 hours ago
In my definition one would need more charge on one side in order to have a different center of charge to center of mass.
â anna v
5 hours ago
@annav To the extent that classical pictures make sense (which is obviously extremely limited), the symmetric dipolar charge distribution is entirely the wrong model; the correct mental picture is an offset between the charge distribution and the mass distribution, as shown at the 2:30-2:45 mark in this video. Perhaps you're thinking that only neutral systems can have dipole moments? That's a common misconception, but it's just not true.
â Emilio Pisanty
5 hours ago
 |Â
show 5 more comments
This answer is rather wide of the mark, I think. You do not need to assume any compositeness hypothesis to have a nonzero electron dipole model (which is the only serious way to understand "the centers of mass and charge do not coincide"), and indeed the Standard Model already predicts a nonzero separation. (It's some ten orders of magnitude beyond the current molecular-spectroscopy experiments, but still.)
â Emilio Pisanty
6 hours ago
As for the claim that "symmetry arguments" entail that the center of mass and the center of charge must be the same -- I don't doubt that one can come up with such arguments, but they'd be wrong. The electron isn't symmetric enough (it has spin) and the SM isn't symmetric enough (it contains both P, T, and C violations) to provide enough symmetry grounds for such an argument to hold. This is clearly seen in the fact that the SM predicts a nonzero eEDM.
â Emilio Pisanty
6 hours ago
@EmilioPisanty please enlighten me , isn't the quantum mechanical charge distribution of a dipole symmetric? The center would be at the center which would coincide with the center of mass distribution as seen in the link I gave for the molecules. Maybe we have a different definition? The center of mass of a rod is at the center. A charged rod + on one side - on another would be a dipole, but the center of charge would be at the center of the rod.
â anna v
5 hours ago
In my definition one would need more charge on one side in order to have a different center of charge to center of mass.
â anna v
5 hours ago
@annav To the extent that classical pictures make sense (which is obviously extremely limited), the symmetric dipolar charge distribution is entirely the wrong model; the correct mental picture is an offset between the charge distribution and the mass distribution, as shown at the 2:30-2:45 mark in this video. Perhaps you're thinking that only neutral systems can have dipole moments? That's a common misconception, but it's just not true.
â Emilio Pisanty
5 hours ago
This answer is rather wide of the mark, I think. You do not need to assume any compositeness hypothesis to have a nonzero electron dipole model (which is the only serious way to understand "the centers of mass and charge do not coincide"), and indeed the Standard Model already predicts a nonzero separation. (It's some ten orders of magnitude beyond the current molecular-spectroscopy experiments, but still.)
â Emilio Pisanty
6 hours ago
This answer is rather wide of the mark, I think. You do not need to assume any compositeness hypothesis to have a nonzero electron dipole model (which is the only serious way to understand "the centers of mass and charge do not coincide"), and indeed the Standard Model already predicts a nonzero separation. (It's some ten orders of magnitude beyond the current molecular-spectroscopy experiments, but still.)
â Emilio Pisanty
6 hours ago
As for the claim that "symmetry arguments" entail that the center of mass and the center of charge must be the same -- I don't doubt that one can come up with such arguments, but they'd be wrong. The electron isn't symmetric enough (it has spin) and the SM isn't symmetric enough (it contains both P, T, and C violations) to provide enough symmetry grounds for such an argument to hold. This is clearly seen in the fact that the SM predicts a nonzero eEDM.
â Emilio Pisanty
6 hours ago
As for the claim that "symmetry arguments" entail that the center of mass and the center of charge must be the same -- I don't doubt that one can come up with such arguments, but they'd be wrong. The electron isn't symmetric enough (it has spin) and the SM isn't symmetric enough (it contains both P, T, and C violations) to provide enough symmetry grounds for such an argument to hold. This is clearly seen in the fact that the SM predicts a nonzero eEDM.
â Emilio Pisanty
6 hours ago
@EmilioPisanty please enlighten me , isn't the quantum mechanical charge distribution of a dipole symmetric? The center would be at the center which would coincide with the center of mass distribution as seen in the link I gave for the molecules. Maybe we have a different definition? The center of mass of a rod is at the center. A charged rod + on one side - on another would be a dipole, but the center of charge would be at the center of the rod.
â anna v
5 hours ago
@EmilioPisanty please enlighten me , isn't the quantum mechanical charge distribution of a dipole symmetric? The center would be at the center which would coincide with the center of mass distribution as seen in the link I gave for the molecules. Maybe we have a different definition? The center of mass of a rod is at the center. A charged rod + on one side - on another would be a dipole, but the center of charge would be at the center of the rod.
â anna v
5 hours ago
In my definition one would need more charge on one side in order to have a different center of charge to center of mass.
â anna v
5 hours ago
In my definition one would need more charge on one side in order to have a different center of charge to center of mass.
â anna v
5 hours ago
@annav To the extent that classical pictures make sense (which is obviously extremely limited), the symmetric dipolar charge distribution is entirely the wrong model; the correct mental picture is an offset between the charge distribution and the mass distribution, as shown at the 2:30-2:45 mark in this video. Perhaps you're thinking that only neutral systems can have dipole moments? That's a common misconception, but it's just not true.
â Emilio Pisanty
5 hours ago
@annav To the extent that classical pictures make sense (which is obviously extremely limited), the symmetric dipolar charge distribution is entirely the wrong model; the correct mental picture is an offset between the charge distribution and the mass distribution, as shown at the 2:30-2:45 mark in this video. Perhaps you're thinking that only neutral systems can have dipole moments? That's a common misconception, but it's just not true.
â Emilio Pisanty
5 hours ago
 |Â
show 5 more comments
up vote
-1
down vote
you'd see that in the bubble/cloud chamber, if the center of mass and charge were different, then you'd have some torque effect that would completely change the electrons trajectories(when they are under electric/magnetic field).
add a comment |Â
up vote
-1
down vote
you'd see that in the bubble/cloud chamber, if the center of mass and charge were different, then you'd have some torque effect that would completely change the electrons trajectories(when they are under electric/magnetic field).
add a comment |Â
up vote
-1
down vote
up vote
-1
down vote
you'd see that in the bubble/cloud chamber, if the center of mass and charge were different, then you'd have some torque effect that would completely change the electrons trajectories(when they are under electric/magnetic field).
you'd see that in the bubble/cloud chamber, if the center of mass and charge were different, then you'd have some torque effect that would completely change the electrons trajectories(when they are under electric/magnetic field).
edited 10 hours ago
answered 10 hours ago
Manu de Hanoi
1029
1029
add a comment |Â
add a comment |Â
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