The Basic Forces and Messenger Particles — Question 3

Section 44-8 · Physics pages 7436–7437

Question 3 Charge conservation fixes the sign of an exchanged weak boson In a charged-current event, u →d + W and the W then couples to e+ + νe. Quark charges are +2e/3 and -e/3. W ± Schematic; labels, not drawing lengths, specify the data. (a) Determine the W charge at both vertices. (b) For the conjugate process, write the quark and lepton transitions and verify electron-family number.
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Question 3 - Solution Charge conservation fixes the sign of an exchanged weak boson W ± (a) Method and calculation QW /e = 2/3 −(−1/3) ⇒W + . W + →e+ + νe : +1 = +1 + 0, Le = −1 + 1 = 0 . (b) Interpretation and further calculation ¯u →¯d + W −, W −→e−+ ¯νe . −2/3 = +1/3 −1, Le = 1 −1 = 0 . Physical check The diagram is charge-flow bookkeeping; whether the W is on shell depends on available invariant energy.

Question 3

Charge conservation fixes the sign of an exchanged weak boson

In a charged-current event, u→d+Wu\to d+W and the W then couples to e++νee^++\nu_e. Quark charges are +2e/3 and -e/3.

Diagram shown in the original SVG worksheet.

  1. Determine the W charge at both vertices.

  2. For the conjugate process, write the quark and lepton transitions and verify electron-family number.

Question 3 - Solution

Charge conservation fixes the sign of an exchanged weak boson

Diagram shown in the original SVG worksheet.

(a) Method and calculation

QW/e=2/3−(−1/3)⇒W+.Q_W/e=2/3-(-1/3)\Rightarrow\boxed{W^+}.W+→e++νe:+1=+1+0,Le=−1+1=0.W^+\to e^++\nu_e:\quad\boxed{+1=+1+0,\quad L_e=-1+1=0}.

(b) Interpretation and further calculation

u‾→d‾+W−,W−→e−+ν‾e.\boxed{\bar u\to\bar d+W^-,\quad W^-\to e^-+\bar\nu_e}.−2/3=+1/3−1,Le=1−1=0.\boxed{-2/3=+1/3-1,\quad L_e=1-1=0}.

Physical check

The diagram is charge-flow bookkeeping; whether the W is on shell depends on available invariant energy.