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Chapter 44: Problem 23

In which of the following reactions or decays is strangeness conserved? In each case, explain your reasoning. (a) \(\mathbf{K}^{+} \rightarrow \boldsymbol{\mu}^{+}+\boldsymbol{\nu}_{\boldsymbol{\mu}}\) (b) \(\mathbf{n}+\mathbf{K}^{+} \rightarrow \mathbf{p}+\boldsymbol{\pi}^{0} ;(\mathbf{c}) \mathbf{K}^{+}+\mathbf{K}^{-} \rightarrow \boldsymbol{\pi}^{0}+\boldsymbol{\pi}^{0} ;(\mathrm{d}) \mathbf{p}+\mathbf{K}^{-} \rightarrow\) \(\Lambda^{0}+\pi^{0}\)

Short Answer

Expert verified
Strangeness is conserved in reactions (c) and (d).

Step by step solution

01

Identify Strangeness for Each Particle

Strangeness is a quantum number assigned to particles. \(K^+\) has a strangeness of +1, \(K^-\) has -1, and \(\Lambda^0\) has -1. The other particles (\(\mu^+\), neutrinos, protons \(p\), neutrons \(n\), and \(\pi^0\)) have strangeness of 0.
02

Analyze Reaction (a)

For the reaction \(K^+ \rightarrow \mu^+ + u_{\mu}\), the initial strangeness is +1 (from \(K^+\)), and the final state has zero strangeness (as both products have strangeness zero). Strangeness is not conserved.
03

Analyze Reaction (b)

In \(n + K^+ \rightarrow p + \pi^0\), the initial strangeness is +1 (from \(K^+\)). The final state has strangeness of 0, as both \(p\) and \(\pi^0\) have 0 strangeness. Strangeness is not conserved.
04

Analyze Reaction (c)

For \(K^+ + K^- \rightarrow \pi^0 + \pi^0\), the initial strangeness is 0 because \(K^+\) is +1 and \(K^-\) is -1, canceling each other out. The final state with two \(\pi^0\) each having strangeness of 0 maintains a total strangeness of 0. Strangeness is conserved.
05

Analyze Reaction (d)

In \(p + K^- \rightarrow \Lambda^0 + \pi^0\), the initial strangeness is -1 due to \(K^-\). The final products show \(\Lambda^0\) with -1 and \(\pi^0\) with 0, totaling a strangeness of -1. Strangeness is conserved.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Quantum Numbers
Quantum numbers are essential in classifying particles and understanding their behavior in reactions. These numbers help describe certain properties of particles and can be compared to an address that helps locate something in space. Just as a house can have a unique address, each particle has a unique set of quantum numbers. These characteristics include the particle's electric charge, spin, and other intrinsic properties.
For the concept of strangeness, which is a specific type of quantum number, its significance lies in particle physics. Strangeness was introduced to explain certain reaction rates and decays that did not comply with older conservation laws. Assigning a value like 0, +1, or -1 to particles, helps physicists track how these particles react or decay. Therefore, understanding quantum numbers is crucial for analyzing how particles transform in reactions.
Particle Reactions
Particle reactions are powerful events where particles interact with one another. These can occur naturally, like in cosmic events, or can be replicated in particle accelerators here on Earth. When particles collide or decay, they transform into new particles, much like chemical reactions involve the transformation of compounds.
During a reaction, it's important to keep track of the initial and final states. You can think of it like a recipe, where you start with raw ingredients and end up with a cooked dish. The ingredients change, but the total amount remains the same due to conservation principles. However, unlike cooking, particle reactions follow strict rules related to quantum numbers and other conservation laws.
Conservation Laws
Conservation laws are the pillars that govern the rules of particle interactions and reactions. They ensure that certain quantities remain constant, no matter what transformations occur during a reaction. Imagine conservation laws as the rules of the chess game, guiding which moves are possible.
Some known conservation laws include conservation of energy, momentum, charge, and some quantum numbers like baryon number and strangeness. In the context of strangeness, this particular quantum number must remain unchanged for reactions that obey the conservation of strangeness. However, not all reactions conserve strangeness 鈥� it depends on the type of interaction involved, such as strong, weak, or electromagnetic forces. Understanding these laws is fundamental to predicting whether a particle reaction is possible and maintaining the balance in the universe's particles.
Particle Decay Reactions
Particle decay reactions involve a single particle converting into several different particles. This process is somewhat similar to breaking a block of ice into smaller cubes; the overall material remains, but its form changes.
In decay reactions, conservation laws, like those involving quantum numbers, play a crucial role in determining which decays are possible. For example, a particle like the kaon can decay into other particles through different reactions, but it must adhere to conservation principles such as strangeness.
Analyzing decay reactions involves examining both the initial particle and the resulting particles. The sum of strangeness in the products should match the initial particle if strangeness needs to be conserved in that particular interaction. By applying these rules, physicists can uncover the hidden symmetries and laws of the universe.

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Most popular questions from this chapter

(a) According to the Hubble law, what is the distance \(r\) from us for galaxies that are receding from us with a speed \(c ?\) (b) Explain why the distance calculated in part (a) is the size of our observable universe (ignoring any slowing of the expansion of the universe due to gravitational attraction).

In the LHC, each proton will be accelerated to a kinetic energy of 7.0 TeV. (a) In the colliding beams, what is the available energy \(E_{\mathrm{a}}\) in a collision? (b) In a fixed-target experiment in which a beam of protons is incident on a stationary proton target, what must the total energy (in TeV) of the paricles in the beam be to produce the same available energy as in part (a)?

The magnetic field in a cyclotron that accelerates protons is 1.30 T. (a) How many times per second should the potential across the dees reverse? (This is twice the frequency of the circulating protons.) (b) The maximum radius of the cyclotron is 0.250 \(\mathrm{m}\) . What is the maximum speed of the proton? (c) Through what potential difference would the proton have to be accelerated from rest to give it the same speed as calculated in part (b)?

Each of the following reactions is missing a single particle. Calculate the baryon number, charge, strangeness, and the three lepton numbers (where appropriate) of the missing particle, and from this identify the particle. (a) \(p+p \rightarrow p+\Lambda^{0}+?\) (b) \(K^{-1}+n \rightarrow \Lambda^{0}+7 ;(c) p+\overline{p} \rightarrow n+7 ;(d) \overline{\nu}_{\mu}+p \rightarrow n+?\)

Pair Annihilation. Consider the case where an electron \(\mathrm{e}^{-}\) and a positron \(\mathrm{e}^{+}\) annihilate each other and produce photons. Assume that these two particles collide head-on with eqnal, but slow, speeds. (a) Show that it is not possible for only one photon to be produced. (Hint: Consider the conservation law that must be true in any collision. (b) Show that if only two photons are produced, they must travel in opposite directions and have equal energy. (c) Calculate the wavelength of each of the photons in part (b). In what part of the electromagnetic spectrum do they lie?
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