/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 26 Particle Iifetime. The unstable ... [FREE SOLUTION] | 91Ó°ÊÓ

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Particle Iifetime. The unstable \(W^{*}\) particle has a rest energy of 80.41 GeV \(\left(1 \mathrm{GeV}=10^{9} \mathrm{eV}\right)\) and an uncertainty in rest energy of 2.06 \(\mathrm{GeV}\) . Estimate the lifetime of the \(\mathrm{W}^{+}\) particle.

Short Answer

Expert verified
The lifetime of the \( W^{*} \) particle is approximately \( 1.595 \times 10^{-25} \, \text{s} \).

Step by step solution

01

Recall the Uncertainty Principle for Energy and Time

The uncertainty principle for energy and time states that the uncertainty in energy, \( \Delta E \), and the uncertainty in time, \( \Delta t \), are related by the formula: \[ \Delta E \cdot \Delta t \geq \frac{\hbar}{2} \]where \( \hbar \) (h-bar) is the reduced Planck's constant, approximately \( 1.0545718 \times 10^{-34} \, \text{J}\cdot\text{s} \).
02

Identify Given Values

From the problem, we have the rest energy uncertainty of the particle, \( \Delta E = 2.06 \, \text{GeV} \). We need to convert this to joules because Planck's constant is given in joules.\( 1 \, \text{GeV} = 1 \times 10^{9} \, \text{eV} = 1.60218 \times 10^{-10} \, \text{J} \).Thus, \( \Delta E = 2.06 \, \text{GeV} \times 1.60218 \times 10^{-10} \, \text{J/GeV} = 3.3024978 \times 10^{-10} \, \text{J} \).
03

Solve for Particle Lifetime

Using the uncertainty principle, \[ \Delta t \geq \frac{\hbar}{2 \cdot \Delta E} \]Substituting in the known values: \[ \Delta t \geq \frac{1.0545718 \times 10^{-34} \, \text{J}\cdot\text{s}}{2 \cdot 3.3024978 \times 10^{-10} \, \text{J}} \]Calculating, \[ \Delta t \geq 1.595 \times 10^{-25} \, \text{s} \].

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Key Concepts

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

Particle Lifetime
When we talk about particle lifetime, we are focusing on the duration a particle exists before it decays. The lifetime of a particle gives us an idea of how stable or unstable it is. For example, the particle in question, a type of unstable particle, has a very short lifetime.
The particle lifetime relates closely to concepts in quantum mechanics, particularly the Uncertainty Principle. This principle tells us that there is a certain degree of uncertainty in simultaneous measurements of energy and time. Specifically:
  • The more precisely we know a particle's energy change, \( \, \Delta E \, \, \), the less precisely we know the time over which that energy change occurs, \( \, \Delta t \, \), and vice versa.
This is expressed mathematically by: \[ \Delta E \cdot \Delta t \geq \frac{\hbar}{2} \] where \( \hbar \, \) is the reduced Planck's constant. In simpler terms, a short particle lifetime usually corresponds to larger uncertainties in energy.
Rest Energy
Rest energy is a fundamental concept from Einstein's theory of relativity. It's the energy contained in a particle when it is at rest relative to an observer. This energy is a measure of how much energy the particle has simply by existing, without any motion.
In formula terms, rest energy \( \, E_0 \, \), is calculated by \( \, E_0 = m c^2 \, \) where:
  • \( m \) is the rest mass of the particle
  • \( c \) is the speed of light in vacuum, approximately \( \scriptsize{3 \times 10^8} \, \text{m/s} \)
In the exercise concerning the particle, the rest energy is given as 80.41 GeV, reflecting how much energy the particle contains in its mass at rest.
When dealing with concepts in quantum mechanics and particle physics, keeping track of rest energy is crucial, as it plays a key role in determining the behavior of particles and how they interact.
Planck's Constant
Planck's constant is a cornerstone of quantum physics. It's a tiny number that helps bridge the gap between the macroscopic and quantum worlds by allowing us to calculate the energy of photons based on their frequency.
Its reduced form, shown as \( \hbar \, \), or h-bar, is indispensable in equations dealing with quantized physics. In the exercise involving particle lifetime, \( \hbar \, \) is used in the Uncertainty Principle formula, emphasizing its role in connections between energy uncertainties and time uncertainties.
  • The value of Planck's constant \( \hbar \, \) is approximately \( 1.0545718 \times 10^{-34} \, \text{J} \cdot \text{s} \), used for calculations in quantum physics.
In a broader sense, Planck's constant represents the quantization of action, implying that particles at quantum levels don’t follow the same rules as larger, observable objects do. Understanding this constant is essential for delving deeper into particle physics and quantum mechanics.

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Most popular questions from this chapter

A particle moving in one dimension (the \(x\) -axis) is described by the wave function $$ \psi(x)=\left\\{\begin{array}{ll} A e^{-b x}, & \text { for } x \geq 0 \\ A e^{k x}, & \text { for } x<0 \end{array}\right. $$ where \(b=2.00 \mathrm{~m}^{-1}, A>0,\) and the \(+x\) -axis points toward the right. (a) Determine \(A\) so that the wave function is normalized. (b) Sketch the graph of the wave function. (c) Find the probability of finding this particle in cach of the following regions: (i) within \(50.0 \mathrm{~cm}\) of the origin, (ii) on the left side of the origin (can you first guess the answer by looking at the graph of the wave function?), (iit) betwcen \(x=0.500 \mathrm{mand} x=1.00 \mathrm{~m}\)

The wave nature of particles results in the quantum- mechanical situation that a particle confined in a box can assume only wavelengths that result in standing waves in the box, with nodes at the box walls, (a) Show that an electron confined in a one- dimensional box of length \(L\) will have energy levels given by $$E_{n}=\frac{n^{2} h^{2}}{8 m L^{2}}$$ (Hint: Recall that the relationship between the de Broglic wave- length and the speed of a nonrelativistic particle is \(m v=h / \lambda\) . The energy of the particle is \(\frac{1}{2} m v^{2}, )(b)\) If a hydrogen atom is modeled as a one-dimensional box with length equal to the Bohr radius, what is the energy (in electron volts) of the lowest energy level of the electron?

A 10.0 -g marble is gently placed on a horizontal tabletop that is 1.75 \(\mathrm{m}\) wide. (a) What is the maximum uncertainty in the horizontal position of the marble? (b) According to the Heisenberg uncertainty principle. what is the minimum uncertainty in the horizontal velocity of the marble? (c) In light of your answer to part (b), what is the longest time the marble could remain on the table? Compare this time to the age of the universe, which is approximately 14 billion years. (Hint Can you know that the horizontal velocity of the marble is exactly zero?)

(a) What is the energy of a photon that has wavelength 0.10\(\mu \mathrm{m} ?\) (b) Through approximately what potential difference must electrons be accelerated so that they will exhibit wave nature in passing through a pinhole 0.10\(\mu \mathrm{m}\) in diameter? What is the speed of these electruns? (c) If protons rather than electrons were used, through what potential difference would protons have to be accelerated so they would exhibit wave nature in passing through this pinhole? What would be the speed of these protons?

Imagine another universe in which the value of Planck's constant is \(0.0663 \mathrm{J} \cdot \mathrm{s},\) but in which the physical laws and all other physical constants are the same as in our universe. In this universe, two physics students are playing catch. They are 12 \(\mathrm{m}\) apart, and one throws a \(0.25-\mathrm{kg}\) ball directly toward the other with a speed of 6.0 \(\mathrm{m} / \mathrm{s}\) (a) What is the uncertainty in the ball's horizontal momentum, in a direction perpendicular to that in which it is being thrown, if the student throwing the ball knows that it is located within a cube with volume 125 \(\mathrm{cm}^{3}\) at the time she throws it? (b) By what horizontal distance could the ball miss the second student?

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