Still Another Conservation Law — Question 9

Section 44-5 · Physics pages 7388–7389

Question 9 An ideal neutral-kaon mixing model rotates a strangeness state Ignore decay and CP violation. Let |K1⟩= (|K0⟩+ | ¯K0⟩)/ √ 2 and |K2⟩= (|K0⟩−| ¯K0⟩)/ √ 2 have energies E1, E2. Initially the state is |K0⟩. Define ∆E = E2 −E1. t P ¯ K Schematic; labels, not drawing lengths, specify the data. (a) Derive the probability to observe an antikaon at time t. (b) Find the first full-conversion time for ∆E = 4.00 × 10−6 eV using ℏ= 6.582 × 10−16 eV s.
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Question 9 - Solution An ideal neutral-kaon mixing model rotates a strangeness state t P ¯ K (a) Method and calculation |ψ(t)⟩= e−iE1t/ℏ|K1⟩+ e−iE2t/ℏ|K2⟩ √ 2 . P(K0 →¯K0) = 1 4|e−iE1t/ℏ−e−iE2t/ℏ|2 = sin2 ∆Et 2ℏ . (b) Interpretation and further calculation ∆Et/(2ℏ) = π/2 ⇒tfull = πℏ/|∆E| . tfull = 5.16949 × 10−10 s . Physical check Real neutral kaons decay and exhibit CP violation. The supplied unitary two-state model isolates oscillation rather than predicting the full experimental time distribution.

Question 9

An ideal neutral-kaon mixing model rotates a strangeness state

Ignore decay and CP violation. Let |K1⟩=(|K0⟩+|K‾0⟩)/2|K_1\rangle=(|K^0\rangle+|\bar K^0\rangle)/\sqrt2 and |K2⟩=(|K0⟩−|K‾0⟩)/2|K_2\rangle=(|K^0\rangle-|\bar K^0\rangle)/\sqrt2 have energies E1,E2E_1,E_2. Initially the state is |K0⟩|K^0\rangle. Define ΔE=E2−E1\Delta E=E_2-E_1.

Diagram shown in the original SVG worksheet.

  1. Derive the probability to observe an antikaon at time t.

  2. Find the first full-conversion time for ΔE=4.00×10−6\Delta E=4.00\times10^{-6} eV using ℏ=6.582×10−16\hbar=6.582\times10^{-16} eV s.

Question 9 - Solution

An ideal neutral-kaon mixing model rotates a strangeness state

Diagram shown in the original SVG worksheet.

(a) Method and calculation

|ψ(t)⟩=e−iE1t/ℏ|K1⟩+e−iE2t/ℏ|K2⟩2.|\psi(t)\rangle=\frac{e^{-iE_1t/\hbar}|K_1\rangle+e^{-iE_2t/\hbar}|K_2\rangle}{\sqrt2}.P(K0→K‾0)=14|e−iE1t/ℏ−e−iE2t/ℏ|2=sin⁡2ΔEt2ℏ.\boxed{P(K^0\to\bar K^0)=\frac14|e^{-iE_1t/\hbar}-e^{-iE_2t/\hbar}|^2=\sin^2\frac{\Delta Et}{2\hbar}}.

(b) Interpretation and further calculation

ΔEt/(2ℏ)=π/2⇒tfull=πℏ/|ΔE|.\Delta Et/(2\hbar)=\pi/2\Rightarrow\boxed{t_{\mathrm{full}}=\pi\hbar/|\Delta E|}.tfull=5.16949×10−10s.\boxed{t_{\mathrm{full}}=5.16949\times10^{-10}\,\mathrm s}.

Physical check

Real neutral kaons decay and exhibit CP violation. The supplied unitary two-state model isolates oscillation rather than predicting the full experimental time distribution.