/*! 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 67 Given that each particle contain... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

Given that each particle contains only combinations of \(u, d,\) \(s, \overline{u}, \overline{d},\) and \(\overline{s},\) deduce the quark content of (a) a particle with charge \(+e,\) baryon number \(0,\) and strangeness \(+1 ;\) (b) a particle with charge \(+e,\) baryon number \(-1,\) and strangeness \(+1 ;\) (c) a particle with charge \(0,\) baryon number \(+1,\) and strangeness \(-2 .\)

Short Answer

Expert verified
(a) su\(\overline{d}\), (b) \(\overline{d}\,\overline{s}\,\overline{u}\), (c) uss.

Step by step solution

01

Analyze Particle (a)

To find the quark content of a particle with charge \(+e\), baryon number \(0\), and strangeness \(+1\), we start by considering mesons, which are quark-antiquark combinations and have baryon number \(0\). The charge \(+e\) suggests a quark content of \(ud\overline{s}\) or \(su\overline{d}\). Considering strangeness \(+1\), the quark content is \(su\overline{d}\), as the quark \(s\) has strangeness \(-1\) and its antiparticle has strangeness \(+1\).
02

Analyze Particle (b)

For a particle with charge \(+e\), baryon number \(-1\), and strangeness \(+1\), we are likely dealing with an anti-baryon. Anti-baryons, composed of three antiquarks, have a baryon number of \(-1\). For charge \(+e\) and strangeness \(+1\), the structure might be \(\overline{d}\,\overline{s}\,\overline{u}\), where \(\overline{s}\) contributes \(+1\) strangeness and \(\overline{u}\) contributes \(+e\) charge.
03

Analyze Particle (c)

A particle with charge \(0\), baryon number \(+1\), and strangeness \(-2\) leads us to consider a baryon since it has baryon number \(+1\). Baryons are combinations of 3 quarks. To achieve \(S = -2\), we need two strange quarks \(s\). Therefore, possible quark content is \(uss\), where charge is \(0\) and strangeness \(-2\). This baryon content explains a charge of \(0\) with the required quark components.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

Key Concepts

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

Particle Physics
Particle physics is a fascinating field that explores the smallest building blocks of the universe. It deals with subatomic particles, like quarks, and how they interact with each other. These interactions occur through fundamental forces: strong, weak, electromagnetic, and gravitational. Quarks are a particular focus because they combine to form hadrons, such as protons and neutrons, which constitute the nuclei of atoms.

The study of these particles allows us to understand the fundamental structures and forces that make up the universe. Particle physicists use huge accelerators to smash particles together, to discover new particles and study their properties. This field has confirmed the existence of quarks and created the Standard Model—a theory that explains how these particles interact. In this realm, properties like charge, baryon number, and strangeness become particularly meaningful as they define how particles behave and influence the universe at a subatomic level.
Baryon Number
The baryon number is an important quantum number in particle physics. It is a conserved quantity, meaning that it doesn't change over time during particle interactions.

Typically, baryons, which include protons and neutrons, have a baryon number of +1. On the other hand, anti-baryons, made up of antiquarks, have a baryon number of -1. Mesons and other particles, not categorized as baryons or anti-baryons, generally have a baryon number of 0. This attribute helps scientists track the behavior of particles in reactions.

Understanding baryon numbers is crucial in solving problems like the one in the original exercise. By preserving the baryon number, scientists deduce possible quark combinations for a given particle. This conservation principle helps maintain the stability of particle interactions by ensuring no net creation or destruction of baryons occurs.
Strangeness
Strangeness is a property that helps classify particles containing strange quarks. It's an intriguing idea introduced to understand certain particle interactions that seemed to defy other known conservation laws. In the context of quarks, the strange quark \(s\) has a strangeness of \(-1\), and its antiquark \(\overline{s}\) has a strangeness of \(+1\).

This notion of strangeness aids physicists in categorizing and predicting particle behavior in high-energy environments, like those in particle accelerators. The conservation of strangeness during some interactions guides what kind of particles can be produced or transformed in reactions. In many interactions, strangeness conservation is respected, especially under strong and electromagnetic forces, but not always under weak force interactions. Understanding strangeness was pivotal in resolving the characteristics of exotic particles detected in cosmic rays and experiments, further enriching our understanding of subatomic physics.
Quark Model
The quark model is a fundamental part of understanding particle physics. It describes hadrons—particles like protons, neutrons, mesons, and baryons—as combinations of quarks. In this model, six flavors of quarks exist: up (u), down (d), strange (s), charm (c), bottom (b), and top (t). Each of these has unique properties like charge and mass.

Hadrons are divided into two categories: baryons, made of three quarks, and mesons, consisting of one quark and one antiquark. This model helps predict and categorize the possible states and interactions of these particles.
  • Baryons, like protons and neutrons, are stable due to their specific quark content.
  • Mesons, often less stable, are pivotal in mediating nuclear forces.
By utilizing the quark model, scientists can explain the behavior of particles under various conditions, including understanding properties like baryon number and strangeness. It provides a systematic framework that elucidates the dynamics of subatomic particles and their interactions, acting as a theoretical backbone in particle physics.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

A nuclear chemist receives an accidental radiation dose of 5.0 Gy from slow neutrons \((R B E=4.0) .\) What does she receive in rad, rem, and \(J / k g ?\)

An unstable isotope of cobalt, \(^{60} \mathrm{Co}\) , has one more neutron in its nucleus than the stable \(^{59}\mathrm{Co}\) and is a beta emitter with a half-life of 5.3 years. This isotope is widely used in medicine. A certain radiation source in a hospital contains 0.0400 \(\mathrm{g}\) of \(^{60} \mathrm{Co.}\) (a) What is the decay constant for that iso- tope? (b) How many atoms are in the source? (c) How many decays occur per second? (d) What is the activity of the source, in curies?

Radioactive isotopes used in cancer therapy have a "shelf- life," like pharmaceuticals used in chemotherapy. Just after it has been manufactured in a nuclear reactor, the activity of a sample of \(^{60} \mathrm{Co}\) is 5000 Ci. When its activity falls below 3500 Ci, it is considered too weak a source to use in treatment. You work in the radiology department of a large hospital. One of these \(^{60} \mathrm{Co}\) sources in your inventory was manufactured on October \(6,2008 .\) It is now April \(6,2011 .\) Is the source still usable? The half-life of \(^{60} \mathrm{Co}\) is 5.271 years.

What is the energy of each of the photons resulting from an annihilation event? A. \(\frac{1}{2} m_{\mathrm{e}} v^{2},\) where \(v\) is the speed of the positron. B. \(m_{\mathrm{e}} v^{2}\) C. \(\frac{1}{2} m_{\mathrm{e}} c^{2}\) D. \(m_{\mathrm{e}} c^{2}\)

A radioactive isotope has a half-life of 76.0 min. A sample is prepared that has an initial activity of \(16.0 \times 10^{10}\) Bq. (a) How many radioactive nuclei are initially present in the sample? (b) How many are present after 76.0 min? What is the activity at this time? (c) Repeat part (b) for a time of 152 min after the sample is first prepared.

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.