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Calculate the threshold kinetic energy for the reaction \(\pi^{-}+\mathrm{p} \rightarrow \Sigma^{0}+\mathrm{K}^{0}\) if a \(\pi^{-}\) beam is incident on a stationary proton target. The \(\mathrm{K}^{0}\) has a mass of 497.7 \(\mathrm{MeV} / c^{2} .\)

Short Answer

Expert verified
The threshold kinetic energy is 612.36 MeV.

Step by step solution

01

Understand the Reaction

The reaction given is \( \pi^{-} + \mathrm{p} \rightarrow \Sigma^{0} + \mathrm{K}^{0} \). Here, a \( \pi^{-} \) meson collides with a stationary proton to produce a \( \Sigma^{0} \) baryon and a \( \mathrm{K}^{0} \) meson.
02

Sum of Initial Masses

First, find the total mass of the initial particles. Use the well-known masses: the mass of the proton is approximately 938.27 MeV/c² and the mass of the \( \pi^{-} \) is about 139.57 MeV/c². Thus, sum these masses: \[ m_{\text{initial}} = m_{\pi^{-}} + m_{p} = 139.57 + 938.27 = 1077.84 \, \text{MeV}/c^2. \]
03

Sum of Final Masses

Next, calculate the total mass of the final particles. The mass of \( \Sigma^{0} \) is approximately 1192.5 MeV/c² and the mass of \( \mathrm{K}^{0} \) is given as 497.7 MeV/c². So, the total mass is: \[ m_{\text{final}} = m_{\Sigma^{0}} + m_{K^{0}} = 1192.5 + 497.7 = 1690.2 \, \text{MeV}/c^2. \]
04

Calculate the Threshold Kinetic Energy

To find the threshold kinetic energy, we determine the energy required to make up for the deficiency between the final and initial masses, as rest mass energy needs to be provided by kinetic energy. The threshold energy is: \[ K_{\text{threshold}} = m_{\text{final}} - m_{\text{initial}} = 1690.2 - 1077.84 = 612.36 \, \text{MeV}. \]
05

Final Result

Thus, the threshold kinetic energy, which is the minimum kinetic energy required by the \( \pi^{-} \) to initiate the reaction with a stationary proton, is 612.36 MeV.

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Key Concepts

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

Particle Physics
Particle physics is the branch of physics that studies the smallest and most fundamental constituents of matter. These include particles like protons, neutrons, electrons, and an array of subatomic particles known as mesons and baryons.
In the realm of particle physics, reactions and forces at the quantum level can be completely different from what we observe in our everyday lives. For instance, in the exercise provided, we discuss particles like the \( \pi^{-} \) meson and \( \Sigma^{0} \) baryon, which are not commonly found in nature.
In collisions within particle physics, it's essential to consider the conservation laws, notably the conservation of energy and momentum. These principles help in predicting the outcome of reactions such as the ones given in the exercise.
The goal of these studies is to understand the underlying principles that govern the universe at both the smallest scales and in the cosmos.
Relativistic Energy
Relativistic energy is a concept that arises from Einstein's theory of relativity. It accounts for the fact that as particles approach the speed of light, their behavior deviates from classical expectations.
In simple terms, energy in a relativistic context comprises not only kinetic energy caused by motion but also the energy stored in the mass of the particle itself. The total energy \( E \) in relativistic systems is given by the famous equation \( E = \gamma mc^2 \), where \( \gamma \) is the Lorentz factor which increases with speed, \( m \) is mass, and \( c \) is the speed of light.
When dealing with high-speed particles in collisions, it's crucial to use relativistic equations to accurately determine kinetic energy and other properties. Like in the given problem, where kinetic energy needs to be calculated in the context of relativistic systems.
Mass-Energy Equivalence
Mass-energy equivalence is one of the most profound concepts from Einstein's special relativity. It's best represented by the equation \( E = mc^2 \), indicating that mass can be converted into energy and vice versa.
In collision reactions, particularly in particle physics, this principle is pivotal. Particles can annihilate, transforming their mass into energy, which can then create new particles. This conversion is fundamental to understanding how energy and mass interplay during high-energy particle interactions.
For the exercise, the need for calculating threshold kinetic energy stems from the necessity to make up the mass difference in reaction products and reactants, illustrating mass-energy equivalence in action. The initial kinetic energy essentially compensates for the rest mass difference between the initial and final states.
Collision Reactions
In particle physics, a collision reaction occurs when particles come in close proximity and exert forces on each other, often resulting in the exchange or transformation of energy or the creation of new particles.
Analyzing collision reactions involves understanding both initial and final states. Initial states are characterized by particles that approach each other with certain velocities and energies, while final states reveal the products of the reaction and their energies.
In the problem, we observed a collision-induced transformation where the \( \pi^{-} \) meson and proton react to form a \( \Sigma^{0} \) baryon and \( K^{0} \) meson. Calculating the threshold energy is crucial, as it determines the minimum energy needed for the reaction to occur. This energy ensures that the products are formed, upholding the conservation laws pivotal in physics.

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Most popular questions from this chapter

(a) A high-energy beam of alpha particles collides with a stationary helium gas target. What must the total energy of a beam particle be if the available energy in the collision is 16.0 GeV? (b) If the alpha particles instead interact in a colliding-beam experiment, what must the energy of each beam be to produce the same available energy?

One proposed proton decay is \(\mathrm{p}^{+} \rightarrow \mathrm{e}^{+}+\pi^{0}\) which violates both baryon and lepton number conservation, so the proton lifetime is expected to be very long. Suppose the proton half-life were \(1.0 \times 10^{18} \mathrm{y}\) . (a) Calculate the energy deposited per kilogram of body tissue (in rad) due to the decay of the protons in your body in one year. Model your body as consisting entirely of water. Only the two protons in the hydrogen atoms in each \(\mathrm{H}_{2} \mathrm{O}\) molecule would decay in the manner shown; do you see why? Assume that the \(\pi^{0}\) decays to two \(\gamma\) rays, that the positron annihilates with an electron, and that all the energy produced in the primary decay and these secondary decays remains in your body (b) Calculate the equivalent dose (in rem) assuming an RBE of 1.0 for all the radiation products, and compare with the 0.1 rem due to the natural background and the 5.0 -rem guidelinefor industrial workers. Based on your calculation, can the proton lifetime be as short as \(1.0 \times 10^{18} \mathrm{y} ?\)

Deuterons in a cyclotron travel in a circle with radius Deuterons in a cyclotron travel in a circle with radius 32.0 \(\mathrm{cm}\) just before emerging from the dees. The frequency of the applied alternating voltage is 9.00 \(\mathrm{MHz}\) . Find (a) the magnetic field and (b) the kinetic energy and speed of the deuterons upon emergence.

Which of the following reactions obey the conservation of baryon number? (a) \(\mathrm{p}+\mathrm{p} \rightarrow \mathrm{p}+\mathrm{e}^{+} ;\) (b) \(\mathrm{p}+\mathrm{n} \rightarrow 2 \mathrm{e}^{+}+\mathrm{e}^{-}\) ; (c) \(\mathrm{p} \rightarrow \mathrm{n}+\mathrm{e}^{-}+\overline{\nu}_{\mathrm{c}} ;(\mathrm{d}) \mathrm{p}+\overline{\mathrm{p}} \rightarrow 2 \gamma\)

Estimate the range of the force mediated by an \(\omega^{0}\) meson that has mass 783 MeVle?

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