Comparing Charge Radius & Compton Wavelength of a Proton

In summary, there is a discrepancy between the commonly cited charge radius of a proton, which is .8*10^-15m, and a formula proposed by an acquaintance on a forum which uses a constant R0 of 1.2*10^-15m to 1.5*10^-15m and the number of nucleons to determine the radius of a nucleus. This formula is based on empirical data and is not a definitive rule. The charge radius of a proton is the root mean square of the charge density distribution and is different from the Compton wavelength. The significance of these values is still being researched and understood, and they have different applications in
  • #1
derekmcd
16
2
I often see the charge radius of a proton at .8 * 10^-15m. An acquaintance on a different forum said he would use, if asked to determine the radius of a nucleus, to be:

R = R0 * A^(1/3) where R0 = 1.2 * 10 ^ -15 to 1.5 * 10 ^ -15 and A is number of nucleons.

He cited the sources:

Principles of Modern Physics by Roberth Leighton or Concepts of Modern Physics by Arthur Beuser, or Nuclear Physics by Enrico Fermi.

I do see 1.3 * 10^-15 used in the formula above often. Is this the Compton wavelength? If not, then where is this value coming from? If it is the Compton wavelength, I have a follow up question (or 4)...

What is the difference between the Compton wavelength and the charge radius? If someone asks me what the diameter of a proton is, what value would I quote? Does it depend on the context of the question and what situation you are applying it to? What is the significance of the value of each?

I tried educating myself through reading several wiki articles and arxiv papers. I, somewhat, understand how you arrive at the values of each, but fail to understand the significance of each and how and to what they are applied.

I appreciate any insight you can offer and/or online sources you can lead me to.
 
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  • #2
The figure R0 = 1.2 * 10 ^ -15 to 1.5 * 10 ^ -15

is just an emperical constant; you measure the radius of nucleis as a function of A, and then you see that the radius is a function of A^(1/3), and R0 is the constant that fits the data.

http://www.tsl.uu.se/~tord/KP/Material/KP08_material/K2.pdf

slide #5
 
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  • #3
Ok. I think I finally have it figured out. If someone were to ask, "what is the radius of a proton", I would cite 1.2 fm.

Would I be correct in stating the charge radius is the exchange force range between two protons? In other words, when they reach a distance of around .875 fm, the strong force overwhelms the repulsive force. If that's the case, then doubling that figure to get the diameter of the proton would make no sense.

Thanks for the PDF... nothing like pretty pictures to help things make sense :smile:
 
  • #4
no the "charge radius" of the proton is the root mean square of the <r^2>, in the charge density distribution of the proton.

See for instance http://cnr2.kent.edu/~pichowsk/IntroNuc/hw3.pdf (eq 6)

http://books.google.com/books?id=Yg...&oi=book_result&resnum=10&ct=result#PPA109,M1 (page 109 and forward)

That is the same thing for the proton itself, since the proton is made up of three valance quarks and a lot of sea-quarks, which carries electric charge.
 
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  • #5
If I haven't already made it obvious... I have no formal education in nuclear physics. I just like to try to figure stuff out and came across 2 completely different radii for the proton. I'm just trying to understand the distinction between the two.

The reason this question came up was from discussing how long a "beam" of photons would be at the LHC. I know they are not really beams, but it was a hypothetical.

I understand discussing the spatial dimensions of a proton (or any other subatomic particle) is a bit more complicated that what a simple question presents.

If I were to make certain, unrealistic assumptions like ignoring the repulsive force and line up 10^15 protons side by side, would that string of protons be 2.4 meters in length?

I see now that the exchange force isn't related to the charge radius, but what is the significance of it? What's the purpose of knowing the rms charge radius and what can you apply it to? It has nothing to do with the spatial dimensions of the proton, right?

One of the reasons I'm curious about the spatial dimension is that Wikipedia states the diameter of the proton to be 1.65 fm. In the discussion section, the reasoning was simply doubling the rms charge radius to get that figure. Given that determining the radius of a nucleus uses the standard radius of 1.2 fm, wouldn't it be more appropriate to cite the diameter to be 2.4 fm?

Given my lack of formal training, I'll understand if you can't describe in simple enough enough terms for me to understand...

I appreciate any attempt, though.
 
  • #6
derekmcd said:
If I haven't already made it obvious... I have no formal education in nuclear physics. I just like to try to figure stuff out and came across 2 completely different radii for the proton. I'm just trying to understand the distinction between the two.

Where is your source? You are first given me:

"I often see the charge radius of a proton at .8 * 10^-15m."

Then you writes:

R = R0 * A^(1/3) where R0 = 1.2 * 10 ^ -15 to 1.5 * 10 ^ -15 and A is number of nucleons.

Are you meaning that if you stick in A = 1 in that eq, you get 1.2-1.5 fm?

Remember that R = R0 * A^(1/3) is an empirical formula, trying to fit nuclei to data, and is not a RULE. If you want to measure the radius of a nuclei, you can do it, the forumula above is just an approximative relation, there are many nuclei that is deviating from that relation.

This is for all kind of 'fit to data', some values are below the curve, and some are under the curve. For example: http://support.sas.com/documentation/cdl/en/grstateditug/61006/HTML/default/images/ex-carlabel.gif

The same thing you do with nuclear radii, you measure the individual radius of each nuclei and then trying to fit a curve, as a function of A.

You got it now?

When you have grasped this, that the relation R = R0*A^(1/3), is just an emperical estimation - I'll explain more about radii in quantum mechanical obejcts, and also what 'strong radius' is.
 
  • #7
I might be approaching my search for an answer the wrong way...

malawi_glenn said:
Where is your source? You are first given me:

"I often see the charge radius of a proton at .8 * 10^-15m."

http://en.wikipedia.org/wiki/Proton

"a diameter of about 1.65×10−15".


In the discussion section:

"It's a bit hard to say what "proton diameter" means. Most experiments seem focused on determining the "proton root-mean-squared charge radius". This value is not very well known, but is about 0.87 fm. So by that measure, the proton diameter is about a fermi and a half. -- Xerxes"


from http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html

"Various types of scattering experiments suggest that nuclei are roughly spherical and appear to have essentially the same density. The data are summarized in the expression called the Fermi model:

http://hyperphysics.phy-astr.gsu.edu/hbase/nuclear/imgnuc/nrad1.gif


They are saying the radius of the proton is 1.2 fm which doesn't agree with the wiki article.

Who is correct? Or are they both correct depending on the context of what each individual is attempting to describing?
 
  • #8
derekmcd said:
they are both correct depending on the context of what each individual is attempting to describing
That would be the case :smile:

Look at that picture :
nucradius.gif

Nuclear matter is not like a hard sphere with a well-defined radius. You need a convention, such as the root-mean-square (RMS) of the distribution, which happens to be convenient because of its relation with the form factors (FF). The FF basically are what you observe directly, they parameterize your cross-section. Under a few simple and reasonable hypothesis, the shape of the FFs will be related to the RMS of the corresponding charge distribution.

0.87 fm would come from the nucleon FF measurements. It definitely tells you about them directly.

2*0.6 fm would come from an approximate fit to the radius as a function of A. You certainly are courageous to take it as such, plug in A=1, and claim a disagreement with the previous number. First hypothesis : the nucleon is the same in a nucleus and in a free state. This is daring. Second (most important here) : the fit does good near the specific low A region, even down to A=1. I would like to see that :smile:
 
  • #9
I guess my answer was not clear enough, and I hope Humaninos will shed more light upon your question. If not, then I try again:

1) The 'radius' of a proton, nucleus, atom - is often defined as the R.M.S of the charge distribution, since it is related to the Form Factor, which is then related to scattering amplitud, which is the quantity we measure in lab.

2) If one does that, the radius of the proton is 0.87fm

3) One has found that if one plots the 'radius' of different stable nuclei as a function of A^(1/3), one can fit a linear curve to that data set, and the constant for the slope of that line is approx 1.2fm.

4) #3 does not saying that ALL nuclei HAS radius 1.2*A^(1/3)fm, when one does a fit, some data goes above the curve, and some of the data goes below is, just as the image I showed you where a fit to data was done. #3 means that nuclei radii behaves, on AVERAGE, as 1.2*A^(1/3)fm.

5) The fit 1.2*A^(1/3)fm is not good for low mass nuclei, as humanino pointed out, it fits "best" for intermediate nuclei.

here is how the 1.2*A^(1/3)fm fit is done - http://www.aanda.org/articles/aa/full/2005/25/aa2003-04/img180.gif

You can also find this in the textbook by Krane.
 
  • #10
malawi_glenn said:
I guess my answer was not clear enough, and I hope Humaninos will shed more light upon your question. If not, then I try again:

1) The 'radius' of a proton, nucleus, atom - is often defined as the R.M.S of the charge distribution, since it is related to the Form Factor, which is then related to scattering amplitud, which is the quantity we measure in lab.

2) If one does that, the radius of the proton is 0.87fm

3) One has found that if one plots the 'radius' of different stable nuclei as a function of A^(1/3), one can fit a linear curve to that data set, and the constant for the slope of that line is approx 1.2fm.

4) #3 does not saying that ALL nuclei HAS radius 1.2*A^(1/3)fm, when one does a fit, some data goes above the curve, and some of the data goes below is, just as the image I showed you where a fit to data was done. #3 means that nuclei radii behaves, on AVERAGE, as 1.2*A^(1/3)fm.

5) The fit 1.2*A^(1/3)fm is not good for low mass nuclei, as humanino pointed out, it fits "best" for intermediate nuclei.

here is how the 1.2*A^(1/3)fm fit is done - http://www.aanda.org/articles/aa/full/2005/25/aa2003-04/img180.gif

You can also find this in the textbook by Krane.

Forgot to be clear about this:

"They are saying the radius of the proton is 1.2 fm which doesn't agree with the wiki article."

No, they are not saying that, it is your intepretation of what that forumula is doing that gives you another proton radius.
 
  • #11
slide 5

http://www4.tsl.uu.se/~tord/KP/Material/KP08_material/K2.pdf
 
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Related to Comparing Charge Radius & Compton Wavelength of a Proton

1. What is the difference between charge radius and Compton wavelength of a proton?

The charge radius of a proton refers to the distance at which the electric charge of the proton is distributed. It is a measure of the size of the proton. On the other hand, the Compton wavelength of a proton is a measure of the average distance that the proton travels before undergoing a scattering event. It is related to the momentum of the proton and is affected by its mass and energy.

2. How are charge radius and Compton wavelength of a proton measured?

The charge radius of a proton can be measured through experiments such as electron scattering or spectroscopy. The Compton wavelength of a proton can be calculated using its mass and velocity, which can be determined through experiments such as particle accelerators.

3. Why is it important to compare the charge radius and Compton wavelength of a proton?

Comparing the charge radius and Compton wavelength of a proton can provide insights into the fundamental properties of the proton, such as its mass and charge distribution. It can also help in understanding the behavior of subatomic particles and their interactions.

4. How do the charge radius and Compton wavelength of a proton relate to the uncertainty principle?

The uncertainty principle states that it is impossible to know the exact position and momentum of a particle at the same time. The charge radius and Compton wavelength of a proton are both affected by the uncertainty principle as they are related to the position and momentum of the proton.

5. Are there any theories or models that attempt to explain the relationship between the charge radius and Compton wavelength of a proton?

Yes, there are various theories and models, such as quantum electrodynamics and the Standard Model, that attempt to explain the relationship between the charge radius and Compton wavelength of a proton. These theories use mathematical equations and principles to describe the behavior of subatomic particles and their interactions.

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