Problem 34
Question
(1) The measured width of the \(\psi(3686)\) meson is about 300 \(\mathrm{keV}\) . Estimate its mean life.
Step-by-Step Solution
Verified Answer
The mean life of the \( \psi(3686) \) meson is approximately \( 2.194 \times 10^{-21} \text{ seconds}.\)
1Step 1: Understanding the relationship
The mean life of a particle is related to its decay width via the uncertainty principle. Specifically, this is expressed as the relationship between the lifetime ( \( \tau \)) and the decay width ( \( \Gamma \)): \[ \tau = \frac{\hbar}{\Gamma} \]where \( \hbar \) is the reduced Planck's constant (\( \hbar \approx 6.582 \times 10^{-22} \text{ MeV} \cdot \text{s}\)). In this problem, the decay width \( \Gamma \) is given as 300 keV.
2Step 2: Converting units for consistency
We need to ensure that the units are consistent to calculate the mean life. So, we convert the decay width from keV to MeV since \( \hbar\) is in MeV \( \cdot \) s:\[ 300 \text{ keV} = 0.300 \text{ MeV} \]
3Step 3: Substitute values and calculate mean life
Using the relationship \( \tau = \frac{\hbar}{\Gamma} \), substitute \( \hbar \approx 6.582 \times 10^{-22} \text{ MeV} \cdot \text{s} \) and \( \Gamma = 0.300 \text{ MeV} \):\[ \tau = \frac{6.582 \times 10^{-22}}{0.300} \approx 2.194 \times 10^{-21} \text{ s} \]Thus, the mean life of \( \psi(3686) \) is approximately \( 2.194 \times 10^{-21} \text{ seconds} \).
Key Concepts
Uncertainty PrincipleDecay WidthMean LifePlanck's Constant
Uncertainty Principle
The Uncertainty Principle is a fundamental concept in quantum mechanics. It states that there is a limit to how precisely we can know certain pairs of properties of a particle, such as position and momentum.
In the context of particle physics, this principle is crucial because it establishes a relationship between the lifetime of a particle and its decay width. This principle is beautifully captured in the formula:
This relationship indicates that particles with a very short lifetime must have a higher decay width, and vice versa. It suggests a fundamental trade-off: the more accurately we know a particle's energy level (related to \( \Gamma \)), the less accurately we can know its lifetime.
In the context of particle physics, this principle is crucial because it establishes a relationship between the lifetime of a particle and its decay width. This principle is beautifully captured in the formula:
- \( \tau = \frac{\hbar}{\Gamma} \)
This relationship indicates that particles with a very short lifetime must have a higher decay width, and vice versa. It suggests a fundamental trade-off: the more accurately we know a particle's energy level (related to \( \Gamma \)), the less accurately we can know its lifetime.
Decay Width
Decay width, denoted by \( \Gamma \), is an important concept in studying unstable particles. It describes the range or spread in the energy levels of the particle due to its instability.
Think of decay width as a measure of how quickly a particle decays or transitions to a lower energy state. More simply, it's like measuring how 'wide' the particle's potential to decay is.
In our exercise, the decay width of the \( \psi(3686) \) meson is given as 300 keV, which is a small energy value indicating a very short but significant measure of lifetime. When particles have a larger decay width, they tend to decay faster compared to those with a smaller decay width.
Think of decay width as a measure of how quickly a particle decays or transitions to a lower energy state. More simply, it's like measuring how 'wide' the particle's potential to decay is.
In our exercise, the decay width of the \( \psi(3686) \) meson is given as 300 keV, which is a small energy value indicating a very short but significant measure of lifetime. When particles have a larger decay width, they tend to decay faster compared to those with a smaller decay width.
Mean Life
The mean life, also called lifetime, is the average time a particle will exist before it decays. It’s often represented by \( \tau \) in equations.
The mean life is directly related to the decay width: the larger the lifetime, the smaller the decay width, indicating a stable particle. Conversely, particles that decay rapidly have shorter lifetimes and larger corresponding decay widths.
In terms of calculation, as seen in the exercise, when we know the decay width \( \Gamma \), we can compute the mean life \( \tau \) using the formula:
The mean life is directly related to the decay width: the larger the lifetime, the smaller the decay width, indicating a stable particle. Conversely, particles that decay rapidly have shorter lifetimes and larger corresponding decay widths.
In terms of calculation, as seen in the exercise, when we know the decay width \( \Gamma \), we can compute the mean life \( \tau \) using the formula:
- \( \tau = \frac{\hbar}{\Gamma} \)
Planck's Constant
Planck's constant is a fundamental quantity in quantum mechanics, and it's often denoted by \( h \). However, in many calculations, especially in particle physics, we use the reduced Planck's constant \( \hbar \), which is \( h/2\pi \).
This constant is extremely small, with a value of approximately \( 6.626 \times 10^{-34} \) Js in its full form. The reduced Planck’s constant is \( 6.582 \times 10^{-22} \text{ MeV} \cdot \text{s} \).
Planck’s constant appears in the uncertainty principle formula, providing a bridge between quantum mechanics and classical physics.
Understanding and using Planck's constant helps us to quantify the highly constrained and sensitive measurements of energy and time in the quantum realm. Its significance underlies many fundamental concepts and constants within the field of physics.
This constant is extremely small, with a value of approximately \( 6.626 \times 10^{-34} \) Js in its full form. The reduced Planck’s constant is \( 6.582 \times 10^{-22} \text{ MeV} \cdot \text{s} \).
Planck’s constant appears in the uncertainty principle formula, providing a bridge between quantum mechanics and classical physics.
Understanding and using Planck's constant helps us to quantify the highly constrained and sensitive measurements of energy and time in the quantum realm. Its significance underlies many fundamental concepts and constants within the field of physics.
Other exercises in this chapter
Problem 33
(1) The mean life of the \(\Sigma^{0}\) particle is \(7 \times 10^{-20}\) s. What is the uncertainty in its rest energy? Express your answer in MeV.
View solution Problem 34
The measured width of the \(\psi(3686)\) meson is about \(300 \mathrm{keV}\). Estimate its mean life.
View solution Problem 36
(I) The B \(^{-}\) meson is a b\overline{u} \text { quark combination. } ( a ) \text { Show that } this is consistent for all quantum numbers. (b) What are the
View solution Problem 38
(II) Which of the following decays are possible? For those that are forbidden, explain which laws are violated. (a) \(\Xi^{0} \rightarrow \Sigma^{+}+\pi^{-}\) \
View solution