How Is the Resonance Peak Area Calculated in Charmonium Production?

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The discussion revolves around the calculation of the resonance peak area in the context of charmonium production, specifically focusing on the cross section for scattering in e+e− collisions and the implications of beam energy spread on measured versus true resonance areas.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the relationship between the measured area under the resonance peak and the true area, questioning how the energy spread of the beams affects this relationship. There is a discussion about manipulating integrals and the role of the probability distribution function f(E-E').

Discussion Status

The conversation is ongoing, with participants attempting to clarify the mathematical relationships involved. Some guidance has been offered regarding the manipulation of integrals, but there is no consensus on the exact steps or methods to prove the relationship mathematically.

Contextual Notes

Participants note the importance of correctly formatting equations and the need for clarity in the mathematical expressions being discussed. There is an acknowledgment of the complexity introduced by the energy spread of the beams and its impact on the measurements.

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The Question:

The cross section for the scattering of two particles with spins sa and sb via a resonance with
spin J is:
\sigma(E)=\frac{\pi\lambda^{2}(2J+1)}{(2S_{a}+1)(2s_{b}+1)} \frac{\Gamma_{i}\Gamma_{j}}{(E-E_{0})^{2}+\frac{\Gamma^{2}}{4}}
with \lambda=1/p, E is the centre-of-mass energy, E0 is the rest
mass energy of the resonance, \Gamma is the total width of the resonance and \Gamma_{i, f} are the partial widths for the decay of the resonance into the initial and final states, respectively.

The cross section for the production of the J/ψ resonance in e+e− collisions,
followed by its decay into e+e−, integrated over the centre-of-mass energy is:
\int \sigma(E)dE=\frac{3\pi^{2}}{2}\lambda^{2}B^{2}_{J/\psi\rightarrow e^+e^-\Gamma}
with
B_{J/\psi\rightarrow e^+e^-}=\frac{\Gamma_{J/\psi\rightarrow e^+e^-}}{\Gamma}
and we took the limits on the integral to be \pm \infty and lambda is constant

The cross section for the production of (a) hadrons, (b) μ+μ− and (c)
e+e− is shown at http://imgur.com/94OYTaM. The measurements were made during a scan of the beam energies at the SPEAR
storage ring at SLAC using beams of e+ and e− circulating in opposite directions with the same
energy.
The observed width of the peak is due to the energy spread of the beams at each point in
the scan, the actual J/ width is much smaller than the observed width of the distributions.
However the relative centre-of-mass energies are known to about 1 part in 104.

At each scan point the beam energy spread produces a spread in the centre-of-mass energies
E′ distributed about the average centre-of-mass energy with a probability distribution
f (E − E′). Show that the measured area under the resonance peak is the same as the true
area under the peak, i.e.

\int \sigma_{int}=\int \sigma_{measured}dEMy attempt:

Measured is wider than the actual resonance peak. So for the area to be the same, the actual peak has to be taller. All I can think of is that! How can I prove that mathematically?

[For some reason, the equations haven't come out well so please use this to view them http://www.codecogs.com/latex/eqneditor.php]

Thanks
 
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The equations will be fine if you use correct tags: "[/itex]" instead of "[\itex]".

I think this can be solved with a simple manipulation of a double-integral (with E and E' as variables).
 
Thanks for pointing the [/itex] out.

But how would you involve the f(E-E')?
 
Is \int\int \sigma f(E,E')dEdE' = \int\int \sigma dEdE' correct then?
 
σ depends on E, f(E,E') depends on the difference between those only, and I don't know what you mean with d.
In addition, some explanation or even steps how to get your integral would be useful.
 

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