How to Convert a Cross Section from GeV2 to Barn | Helpful Tips

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Discussion Overview

The discussion revolves around the conversion of cross section units from GeV2 to barns, addressing both the mathematical and conceptual aspects of unit conversion in the context of particle physics. Participants explore the implications of using different unit systems, particularly in relation to quantum gravity and dimensional analysis.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning
  • Conceptual clarification

Main Points Raised

  • One participant inquires about the validity of having a cross section in GeV2 and seeks help for conversion to barns.
  • Another participant suggests a mistake in the original computation, indicating that the correct unit should be 1/GeV2 and provides the conversion factor \hbar c = 200 MeV fm.
  • A different participant states that GeV2 is equivalent to 1.752 x 10-80 barns in the context of quantum gravity.
  • Concerns are raised about the clarity of the conversion process, particularly regarding the treatment of \hbar and c in the original question.
  • Some participants argue that using natural units simplifies calculations, while others caution against neglecting dimensional analysis, especially for beginners.
  • There is a discussion about the importance of maintaining unit consistency and the potential pitfalls of using dimensionless quantities without proper context.
  • Participants express differing views on the pedagogical approach to teaching unit conversions and the implications of using various unit systems.
  • One participant emphasizes the need to keep track of powers of mass and energy to avoid errors in calculations.
  • Another participant argues that setting G = 1 in certain contexts may obscure the ability to check dimensional consistency.

Areas of Agreement / Disagreement

There is no clear consensus among participants. While some agree on the importance of dimensional analysis and the use of natural units, others express differing opinions on the appropriateness of these approaches for beginners. The discussion remains unresolved regarding the best practices for unit conversion in this context.

Contextual Notes

Participants highlight the complexity of unit conversions in particle physics, particularly when involving constants like \hbar, c, and G. There are unresolved questions about the proper treatment of these constants and their implications for dimensional analysis.

maani
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Hi I have computed a cross section to 10-6 GeV2. Now I have to convert it to barn, but don't know how. Can anybody help me? Is it ok to have a cross section in units of GeV2 or is my result completely wrong?
Thanks!
 
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You made a mistake somewhere. It should be 1/GeV2.

The conversion factor you need is \hbar c = 200 MeV fm.
 
Vanadium 50 said:
\hbar c = 200 MeV fm.
Equivalently, \left(\hbar c\right)^{2}=0.389\text{ GeV}^2\text{mbarn}
 
If you're doing quantum gravity, then:

GeV^2 = 1.752*10^(-80) barn
 
Count Iblis said:
If you're doing quantum gravity, then:

GeV^2 = 1.752*10^(-80) barn
It seems to me confusing in the context of the original question to hide \hbar and c. Vanadium 50's and my result are on the first page of the particle data group booklet or review, so I think we were justified not to give further details (unless requested). I'd like to request a clarification about your formula. It seems to me, energy and length have inverse dimension for instance. Can you please re-establish the proper \hbar, c and (probably) G factors ?
 
humanino said:
It seems to me confusing in the context of the original question to hide \hbar and c. Vanadium 50's and my result are on the first page of the particle data group booklet or review, so I think we were justified not to give further details (unless requested). I'd like to request a clarification about your formula. It seems to me, energy and length have inverse dimension for instance. Can you please re-establish the proper \hbar, c and (probably) G factors ?

Well, I agree that the OP really meant GeV^(-2) and agree with your answers. Now, if you put G = 1, then of course, any power of GeV could be a cross section (because you've made physics dimensionless).

Now, I don't work in particle physics so, I don't have the conversion factors in my head. So, what I always do is use a few well known formulae that contain hbar, c and G to do the conversion.

To convert GeV^2 to a cross section, you can use that in General Relativity, mass and length have the same dimensions (if you put c = G = 1). So, GeV^2 is already a cross section and no additional conversion using hbar needs to be performed.

To restore G and c, we just hijack the formula for gravitational potential energy, so:

m^2 G/r = energy = m c^2

this is a dimensionally correct expression, that doesn't need to make sense. So, we have:

m G/(c^2 r) = dimensionless

Or:

E G/(c^4) = length

where E is an energy. So, we see that:

cross section = E^2 G^2/c^8


If you know the formulas for Planck length, Planck energy etc. etc., you can do the conversion directly. To convert GeV^n to a cross section, you simply divide this by the Planck energy to the power n and multiply by the Planck length squared.
 
I think this is singularly unhelpful.

We have someone who is doing their first calculation - we know this, because they are having unit problems. Suggesting they start popping Planck masses in until the units come out right is not going to help them get the right answer. It's simply the wrong thing to do.
 
Thanks to all of you for the fast answers. This was really my first computation and it was completely wrong. I am still working on it. But i have learned at least how to convert the units.
 
It's very smart to carry along the units, at least until you gain more facility with these calculations. People will say, "who cares if you drop an hbar or a c", but I would respond, "but who knows what else you dropped?" Then later when you get more experience, taking the shortcut becomes more reasonable.
 
  • #10
Vanadium 50 said:
I think this is singularly unhelpful.

We have someone who is doing their first calculation - we know this, because they are having unit problems. Suggesting they start popping Planck masses in until the units come out right is not going to help them get the right answer. It's simply the wrong thing to do.

It is very unhelpful to keep students indoctrinated in the wrongful use of units. Students learn units the wrong way in high school and even at university, the false myth of the meaning of units is promoted, to the detriment of science. Then what you see is that advanced university level students are struggeling with what should be a trivial high school physics exercise.

Even many professional physicisist do not understand units as
http://arxiv.org/abs/hep-th/0208093" . :mad:
 
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  • #11
Vanadium 50 said:
It's very smart to carry along the units, at least until you gain more facility with these calculations. People will say, "who cares if you drop an hbar or a c", but I would respond, "but who knows what else you dropped?" Then later when you get more experience, taking the shortcut becomes more reasonable.

It's not just a shortcut, natural units are a bona fide unit system. The conversion back to SI units is very simple. With some minor practice, the chances of making mistakes are much less likely if you use natural units than if you use SI units.

The constants c, hbar, G, k_b, etc. etc. are nothing more than irrelevant conversion factor. Then, if we intend to use SI units when actually inserting numbers in the equation, we should make sure the correct conversion factors are present in the final result. But it can be extremely cumbersome to derive the equation with the conversion factors already present in the intermediary steps.

It is a bit like the complicated formulas frequently used by engineers were e.g. pressure appears in different ways, e.g. in atmospheres and in mm Hg. Then the formula also contains a conversion factor which has exactly the same interpretation as c, hbar, G, k_b etc.
 
  • #12
Count Iblis said:
It is a bit like the complicated formulas frequently used by engineers were e.g. pressure appears in different ways, e.g. in atmospheres and in mm Hg.
Not really. Keeping track of the powers of mass is quite a useful consistency check. I'd say it helps to avoid errors. Anyway, unless the original posters intends to go into quantum gravity, in which case this is not the appropriate sub-forum, advising him to overlook all dimensions together is certainly not very pedagogical. First he should learn the dimensions of the various fields, like spinors/vectors etc... at the very least.
 
  • #13
Yes, I agree that it's useful to keep track of the powers of the mass. But then you can put hbar = c = 1. The fact that inverse mass is a length should be common knowledge. Even I know that and I don't work with this stuff on a daily basis.
 
  • #14
Count Iblis said:
Yes, I agree that it's useful to keep track of the powers of the mass. But then you can put hbar = c = 1. The fact that inverse mass is a length should be common knowledge. Even I know that and I don't work with this stuff on a daily basis.
When I said power, I meant both positive and negative. That's indeed what we do all the time. The problem comes about with m^2 G/r=E and setting G=1. With an arbitrary number of hidden G factors, you loose the ability to check the number of powers of mass (or energy, or length, or time) on both sides of the equation. For instance, with
cross section = 1/(E^2)
 
  • #15
humanino said:
When I said power, I meant both positive and negative. That's indeed what we do all the time. The problem comes about with m^2 G/r=E and setting G=1. With an arbitrary number of hidden G factors, you loose the ability to check the number of powers of mass (or energy, or length, or time) on both sides of the equation. For instance, with
cross section = 1/(E^2)

Indeed, but then, you're not going to set G = 1 in ordinary QFT computations. And if one contemplates a fundamental theory, then one has to be reasonble and accept the fact that Nature may be fundamentally dimensionless.

If you formulate some lattice statistical mechanics model, like the Ising model, you only have pure numbers. But close to the critical temperature you can look at some scaling limit in which you can formulate hte model as some effective field theory. The correlation length then enters the effective theory as an inverse mass.

Cardy writes in one of his books that the Renormalization Group is simply a sophisticated way of doing dimensional analysis. :smile:
 

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