Still Another Conservation Law — Question 3

Section 44-5 · Physics pages 7376–7377

Question 3 Missing-hadron quantum numbers can be inferred before its identity is known An observed strong reaction is π−+ p →K+ + X. The kaon has Q=+e, B=0 and S=+1. Initial total values are Q=0, B=1 and S=0. π−+ p K+ + X Schematic; labels, not drawing lengths, specify the data. (a) Infer Q, B and S of X. (b) Compare X with candidate A having (-e,1,-1) and candidate B having (-e,0,-1). State what further information is needed after these tests.
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Question 3 - Solution Missing-hadron quantum numbers can be inferred before its identity is known π−+ p K+ + X (a) Method and calculation QX = 0 −(+e) = −e . BX = 1 −0 = 1, SX = 0 −(+1) = −1 . (b) Interpretation and further calculation A : matches; B : fails baryon number . (Q, B, S)X = (−e, 1, −1) does not uniquely fix mass or spin. Physical check Conservation narrows possible identities. Mass reconstruction, spin information and decay channels can distinguish states with identical additive numbers.

Question 3

Missing-hadron quantum numbers can be inferred before its identity is known

An observed strong reaction is π−+p→K++X\pi^-+p\to K^++X. The kaon has Q=+e, B=0 and S=+1. Initial total values are Q=0, B=1 and S=0.

Diagram shown in the original SVG worksheet.

  1. Infer Q, B and S of X.

  2. Compare X with candidate A having (-e,1,-1) and candidate B having (-e,0,-1). State what further information is needed after these tests.

Question 3 - Solution

Missing-hadron quantum numbers can be inferred before its identity is known

Diagram shown in the original SVG worksheet.

(a) Method and calculation

QX=0−(+e)=−e.\boxed{Q_X=0-(+e)=-e}.BX=1−0=1,SX=0−(+1)=−1.\boxed{B_X=1-0=1,\quad S_X=0-(+1)=-1}.

(b) Interpretation and further calculation

A: matches;B: fails baryon number.\boxed{A:\text{ matches};\quad B:\text{ fails baryon number}}.(Q,B,S)X=(−e,1,−1)does not uniquely fix mass or spin.(Q,B,S)_X=(-e,1,-1)\quad\text{does not uniquely fix mass or spin}.

Physical check

Conservation narrows possible identities. Mass reconstruction, spin information and decay channels can distinguish states with identical additive numbers.