The Basic Forces and Messenger Particles — Question 5

Section 44-8 · Physics pages 7440–7441

Question 5 Weak effective-interaction scaling cannot be extrapolated indefinitely In a low-energy model σ = CG2E2, where G has dimensions energy to the power -2 and C is dimensionless in natural units. The approximation requires E much smaller than a mediator mass M=80 GeV. E σ Schematic; labels, not drawing lengths, specify the data. (a) Find the cross-section ratio at energies 2 and 5 GeV and check dimensions. (b) If a reference unitarity scale is σmax = 4π/E2, solve symbolically where the extrapolated formulas meet.
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Question 5 - Solution Weak effective-interaction scaling cannot be extrapolated indefinitely E σ (a) Method and calculation σ(5)/σ(2) = (5/2)2 = 6.25 . [G2E2] = E−4E2 = E−2 as required for area in natural units. (b) Interpretation and further calculation CG2E2 = 4π/E2 ⇒E4 = 4π/(CG2). Emeet = (4π/C)1/4G−1/2 . Physical check The meeting scale is an estimate within the supplied toy comparison. A complete high-energy theory changes the low-energy growth.

Question 5

Weak effective-interaction scaling cannot be extrapolated indefinitely

In a low-energy model σ=CG2E2\sigma=C G^2E^2, where G has dimensions energy to the power -2 and C is dimensionless in natural units. The approximation requires E much smaller than a mediator mass M=80 GeV.

Diagram shown in the original SVG worksheet.

  1. Find the cross-section ratio at energies 2 and 5 GeV and check dimensions.

  2. If a reference unitarity scale is σmax=4π/E2\sigma_{\max}=4\pi/E^2, solve symbolically where the extrapolated formulas meet.

Question 5 - Solution

Weak effective-interaction scaling cannot be extrapolated indefinitely

Diagram shown in the original SVG worksheet.

(a) Method and calculation

σ(5)/σ(2)=(5/2)2=6.25.\boxed{\sigma(5)/\sigma(2)=(5/2)^2=6.25}.[G2E2]=E−4E2=E−2as required for area in natural units.[G^2E^2]=E^{-4}E^2=E^{-2}\quad\text{as required for area in natural units}.

(b) Interpretation and further calculation

CG2E2=4π/E2⇒E4=4π/(CG2).CG^2E^2=4\pi/E^2\Rightarrow E^4=4\pi/(CG^2).Emeet=(4π/C)1/4G−1/2.\boxed{E_{\mathrm{meet}}=(4\pi/C)^{1/4}G^{-1/2}}.

Physical check

The meeting scale is an estimate within the supplied toy comparison. A complete high-energy theory changes the low-energy growth.