The Quark Model — Question 7

Section 44-7 · Physics pages 7424–7425

Question 7 Confining string energy predicts a pair-production length scale Use a toy confining potential V (r) = κr with κ = 0.90 GeV/fm. Producing an effective light quark-antiquark pair requires 0.60 GeV. Neglect kinetic and other field energies. q ¯q r V = κr Schematic; labels, not drawing lengths, specify the data. (a) Find the separation at which the stored energy reaches this threshold. (b) Calculate the energy at 1.2 fm and the excess above threshold; explain why this favors fragmentation over isolating a quark.
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Question 7 - Solution Confining string energy predicts a pair-production length scale q ¯q r V = κr (a) Method and calculation κrbreak = 2meffc2 = .60 GeV. rbreak = .60/.90 = .666667 fm . (b) Interpretation and further calculation V (1.2 fm) = 1.08 GeV, Eexcess = .48 GeV . q—¯q −→(q¯qnew) + (qnew¯q). Physical check The effective pair mass and linear potential are a model. Energy accounting suggests new color-singlet hadrons, not a sharp universal string-breaking distance.

Question 7

Confining string energy predicts a pair-production length scale

Use a toy confining potential V(r)=κrV(r)=\kappa r with κ=0.90\kappa=0.90 GeV/fm. Producing an effective light quark-antiquark pair requires 0.60 GeV. Neglect kinetic and other field energies.

Diagram shown in the original SVG worksheet.

  1. Find the separation at which the stored energy reaches this threshold.

  2. Calculate the energy at 1.2 fm and the excess above threshold; explain why this favors fragmentation over isolating a quark.

Question 7 - Solution

Confining string energy predicts a pair-production length scale

Diagram shown in the original SVG worksheet.

(a) Method and calculation

κrbreak=2meffc2=.60GeV.\kappa r_{\mathrm{break}}=2m_{\mathrm{eff}}c^2=.60\ {\mathrm{GeV}}.rbreak=.60/.90=.666667fm.\boxed{r_{\mathrm{break}}=.60/.90=.666667\ {\mathrm{fm}}}.

(b) Interpretation and further calculation

V(1.2fm)=1.08GeV,Eexcess=.48GeV.\boxed{V(1.2\ {\mathrm{fm}})=1.08\ {\mathrm{GeV}},\quad E_{\mathrm{excess}}=.48\ {\mathrm{GeV}}}.q—q‾→(qq‾new)+(qnewq‾).q\text{---}\bar q\ \longrightarrow\ (q\bar q_{\mathrm{new}})+(q_{\mathrm{new}}\bar q).

Physical check

The effective pair mass and linear potential are a model. Energy accounting suggests new color-singlet hadrons, not a sharp universal string-breaking distance.