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We discuss the basic concepts of waves, including phase velocity, dispersion, group velocity. We show how to use the Fourier principle to construct any general wave from the harmonic waves.
We explore the energy eigenvalues and eigenstates of a periodic series of potential energy wells with the purpose of creating a rudimentary model of a solid. Our model uses an approximate approach that emphasizes the interaction between neighboring atoms. We learn how the eigenstates of the periodic potential can be constructed from the eigenstates of the single elements of the periodic potential. We also learn that the eigenstates of a solid are characterized by a wavelength, and that the energies of those eigenstates form bands centered near the atomic energy eigenvalues. We model electron motion in solids with the use of a wave packet, a superposition of delocalized Bloch states.
We introduce the idea of orbital angular momentum and illustrate its importance in solving the three-dimensional differential equation that is the energy eigenvalue equation for the hydrogen atom. By separating variables in the eigenvalue equation, we isolate the differential equations for the angular variables from the differential equation for the radial variable. We solve the angular equations to discover the spherical harmonics and the angular momentum quantum numbers.
We learn how to use perturbation theory to solve more realistic problems that do not admit exact solutions. We learn degenerate and nondegenerate perturbation theory and apply them to a variety of problems, including spin magnetic moments in magnetic fields and the Stark effect in hydrogen.
We introduce the concept of adding or coupling angular momenta. We introduce the angular momentum ladder operators and learn to transform from the uncoupled basis to the coupled basis. We use these new ideas to study the hyperfine structure of the ground state of hydrogen.
Quantum mechanics is inherently a probabilistic theory, so we present a brief review of some important concepts in probability theory. We distinguish between discrete probabilities, encountered in spin measurements, and continuous probabilities, encountered in position measurements.
We study further perturbations of the hydrogen atom due to both external and internal magnetic fields. The internal fields give rise to the fine structure of the hydrogen energy levels. The external fields give rise to the Zeeman effect. We also study internal perturbations due to relativistic effects, which are part of the fine structure.
We solve the radial differential equation to find the quantized energies and the radial wave functions of the bound states of the hydrogen atom. We present the energy spectrum of hydrogen and the electron probability densities of the energy eigenstates and of superposition states.
We show that the geometric realisation of the poset of proper parabolic subgroups of a large-type Artin group has a systolic geometry. We use this geometry to show that the set of parabolic subgroups of a large-type Artin group is stable under arbitrary intersections and forms a lattice for the inclusion. As an application, we show that parabolic subgroups of large-type Artin groups are stable under taking roots and we completely characterise the parabolic subgroups that are conjugacy stable.
We also use this geometric perspective to recover and unify results describing the normalisers of parabolic subgroups of large-type Artin groups.
How many 2-cells must two finite CW-complexes have to admit a common, but not finite common, covering? Leighton’s theorem says that both complexes must have 2-cells. We construct an almost (?) minimal example with two 2-cells in each complex.
As a general framework for the studies of t-structures on triangulated categories and torsion pairs in abelian categories, we introduce the notions of extriangulated categories with negative first extensions and s-torsion pairs. We define a heart of an interval in the poset of s-torsion pairs, which naturally becomes an extriangulated category with a negative first extension. This notion generalises hearts of t-structures on triangulated categories and hearts of twin torsion pairs in abelian categories. In this paper, we show that an interval in the poset of s-torsion pairs is bijectively associated with s-torsion pairs in the corresponding heart. This bijection unifies two well-known bijections: one is the bijection induced by the HRS-tilt of t-structures on triangulated categories. The other is Asai–Pfeifer’s and Tattar’s bijections for torsion pairs in an abelian category, which is related to $\tau$-tilting reduction and brick labelling.
This textbook offers a detailed and uniquely self-contained presentation of quantum and gauge field theories. Writing from a modern perspective, the author begins with a discussion of advanced dynamics and special relativity before guiding students steadily through the fundamental principles of relativistic quantum mechanics and classical field theory. This foundation is then used to develop the full theoretical framework of quantum and gauge field theories. The introductory, opening half of the book allows it to be used for a variety of courses, from advanced undergraduate to graduate level, and students lacking a formal background in more elementary topics will benefit greatly from this approach. Williams provides full derivations wherever possible and adopts a pedagogical tone without sacrificing rigour. Worked examples are included throughout the text and end-of-chapter problems help students to reinforce key concepts. A fully worked solutions manual is available online for instructors.