QSIT FS 2015 Questions 1 ‐ Solutions
... a. A neutron is a spin 1/2 particle. In a constant magnetic field it will have two non‐degenerate states. Hence, The Hilbert space describing such a neutron in a magnetic field is two dimensional b. In a gradient field, the splitting of the neutron's eigenstate energies will depend on the position. ...
... a. A neutron is a spin 1/2 particle. In a constant magnetic field it will have two non‐degenerate states. Hence, The Hilbert space describing such a neutron in a magnetic field is two dimensional b. In a gradient field, the splitting of the neutron's eigenstate energies will depend on the position. ...
Advanced Analysis Spring 2006
... Exercises for April 10st: E1: Let X be a topological space. Let x, y ∈ X. Let f : X → C be continuous and assume that f (x) 6= f (y). 1. Show that there exist disjoint open neighborhoods of x and y. 2. Let C(X) be the algebra of continuous functionals on X. Show that A is a subalgebra of C(X) that s ...
... Exercises for April 10st: E1: Let X be a topological space. Let x, y ∈ X. Let f : X → C be continuous and assume that f (x) 6= f (y). 1. Show that there exist disjoint open neighborhoods of x and y. 2. Let C(X) be the algebra of continuous functionals on X. Show that A is a subalgebra of C(X) that s ...
Document
... • Usually, when reasoning about or interacting with a system, an entity (e.g. a physicist) has in mind a description of the system. • A description that contains every property of the system is an exact ...
... • Usually, when reasoning about or interacting with a system, an entity (e.g. a physicist) has in mind a description of the system. • A description that contains every property of the system is an exact ...
Solutions to Homework 1, Quantum Mechanics
... an orthonormal basis set? If not, use Gram-Schmidt algorithm to turn them into an othomormal set. Answ: The 2 vectors are linearly independent. Since the space has only 2 dimensions, they therefore form a basis. However, they are neither normalized nor orthogonal to each other. To turn them into an ...
... an orthonormal basis set? If not, use Gram-Schmidt algorithm to turn them into an othomormal set. Answ: The 2 vectors are linearly independent. Since the space has only 2 dimensions, they therefore form a basis. However, they are neither normalized nor orthogonal to each other. To turn them into an ...
Physics 451 - BYU Physics and Astronomy
... I have noticed in recent homeworks that more students quit to do entire problem(s). They are either short in time or overwhelmed by the length of the problems. It is understandable that this is an intense course, and the homework is time consuming. And as it is approaching the middle of the semester ...
... I have noticed in recent homeworks that more students quit to do entire problem(s). They are either short in time or overwhelmed by the length of the problems. It is understandable that this is an intense course, and the homework is time consuming. And as it is approaching the middle of the semester ...
Lecture 24: Tensor Product States
... Definition of Tensor product • Suppose you have a system with 10 possible states • Now you want to enlarge your system by adding ten more states to its Hilbert space. – The dimensionality of the Hilbert space increases from 10 to 20 – The system can now be found in one of 20 possible states – This ...
... Definition of Tensor product • Suppose you have a system with 10 possible states • Now you want to enlarge your system by adding ten more states to its Hilbert space. – The dimensionality of the Hilbert space increases from 10 to 20 – The system can now be found in one of 20 possible states – This ...
3.1 Linear Algebra Vector spaces
... Note that the operator x̂ is not linear in P (N ) since it is able to promote the (N − 1)th-order polynomial into the N th-order polynomial, which is not a member of P (N ). But, x̂ is linear in P (∞) x̂ is also Hermitian in P (∞) Note, however, that it has no eigenfunctions in P (∞)! In fact, it c ...
... Note that the operator x̂ is not linear in P (N ) since it is able to promote the (N − 1)th-order polynomial into the N th-order polynomial, which is not a member of P (N ). But, x̂ is linear in P (∞) x̂ is also Hermitian in P (∞) Note, however, that it has no eigenfunctions in P (∞)! In fact, it c ...
6.1.5. Number Representation: Operators
... where, to avoid ambiguity, we have used subscript to indicate the particle occupying the state. Taking the hermitian conjugate, we obtain the adjoint basis vector ...
... where, to avoid ambiguity, we have used subscript to indicate the particle occupying the state. Taking the hermitian conjugate, we obtain the adjoint basis vector ...
Linear Algebra, Norms and Inner Products I. Preliminaries A. Definition
... space V iff for every x ∈ V , there exist scalars α1 , . . . , αn , such that x = i=1 αi xi • Fact: all bases of a space have the same number of vectors (the dimension of the space). • Fact: every vector x has a unique representation in a given basis. Thus we can represent a vector by its coefficien ...
... space V iff for every x ∈ V , there exist scalars α1 , . . . , αn , such that x = i=1 αi xi • Fact: all bases of a space have the same number of vectors (the dimension of the space). • Fact: every vector x has a unique representation in a given basis. Thus we can represent a vector by its coefficien ...
finm314F06.pdf
... Instructions: Show your work in the spaces provided below for full credit. Use the reverse side for additional space, but clearly so indicate. You must clearly identify answers and show supporting work to receive any credit. Exact answers (e.g., π ) are preferred to inexact (e.g., 3.14). Point value ...
... Instructions: Show your work in the spaces provided below for full credit. Use the reverse side for additional space, but clearly so indicate. You must clearly identify answers and show supporting work to receive any credit. Exact answers (e.g., π ) are preferred to inexact (e.g., 3.14). Point value ...
LOYOLA COLLEGE (AUTONOMOUS), CHENNAI – 600 034
... by these vectors. If s > r, show that any s vectors u1, u2, . . . , us in U must be linearly dependent. 14. If a vector space V = W1 W2, show that dim V = dim W1 + dim W2. 15. State and prove Bessel’s inequality. 16. Show that T A(V) is invertible if and only if the constant term of the minimal ...
... by these vectors. If s > r, show that any s vectors u1, u2, . . . , us in U must be linearly dependent. 14. If a vector space V = W1 W2, show that dim V = dim W1 + dim W2. 15. State and prove Bessel’s inequality. 16. Show that T A(V) is invertible if and only if the constant term of the minimal ...
Instanton representation of Plebanski gravity
... • Plebanski equations of motion imply Einstein equations ...
... • Plebanski equations of motion imply Einstein equations ...
UE Funktionalanalysis 1
... 5. Let U ⊆ V be subsets of a metric space X. Show that if U is dense in V and V is dense in X, then U is dense in X. 6. Show that any open set O ⊆ R can be written as a countable union of disjoint intervals. (Hint: Let {Iα } be the set of all maximal subintervals of O; that is, Iα ⊆ O and there is n ...
... 5. Let U ⊆ V be subsets of a metric space X. Show that if U is dense in V and V is dense in X, then U is dense in X. 6. Show that any open set O ⊆ R can be written as a countable union of disjoint intervals. (Hint: Let {Iα } be the set of all maximal subintervals of O; that is, Iα ⊆ O and there is n ...
Recap of Lectures 12-2
... Harmonic oscillator illustrates quantum-classical transition at high quantum number n. Truly classical behaviour (observable change with time) requires physical state to be a superposition of energy states. ...
... Harmonic oscillator illustrates quantum-classical transition at high quantum number n. Truly classical behaviour (observable change with time) requires physical state to be a superposition of energy states. ...
Chapter 3 Mathematical Formalism of Quantum Mechanics
... This means that every sequence whose elements get even closer to each other as the sequence progresses – i.e. a Cauchy sequence – has a limit in the space, i.e., the space includes all the limits of its converging sequences and is therefore called complete. Such a property can be visualized as a spa ...
... This means that every sequence whose elements get even closer to each other as the sequence progresses – i.e. a Cauchy sequence – has a limit in the space, i.e., the space includes all the limits of its converging sequences and is therefore called complete. Such a property can be visualized as a spa ...
Quantum Computing Lecture 3 Principles of Quantum Mechanics
... complex inner product space. Postulate 2: The evolution of a closed system in a fixed time interval is described by a unitary transform. Postulate 3: If we measure the state |ψi of a system in an orthonormal basis |0i · · · |n − 1i, we get the result |ji with probability |hj|ψi|2 . After the measure ...
... complex inner product space. Postulate 2: The evolution of a closed system in a fixed time interval is described by a unitary transform. Postulate 3: If we measure the state |ψi of a system in an orthonormal basis |0i · · · |n − 1i, we get the result |ji with probability |hj|ψi|2 . After the measure ...
1 Towards functional calculus
... and look at f (M). We see that f (M) is the zero matrix exactly if λ is not an eigenvalue! (And otherwise, it’s the projection onto the λ eigenspace.) This somewhat abstract idea — that we understand a linear transformation exactly if we can apply functions to it — motivates the main question for t ...
... and look at f (M). We see that f (M) is the zero matrix exactly if λ is not an eigenvalue! (And otherwise, it’s the projection onto the λ eigenspace.) This somewhat abstract idea — that we understand a linear transformation exactly if we can apply functions to it — motivates the main question for t ...
Many-body Quantum Mechanics
... the Fock space, and the first that this basis in not orthogonal and thus overcomplete. In spite of this the coherent states are very useful in particular for deriving path integrals. In this course they will be important as an example of states where the creation and annihilation operators have non- ...
... the Fock space, and the first that this basis in not orthogonal and thus overcomplete. In spite of this the coherent states are very useful in particular for deriving path integrals. In this course they will be important as an example of states where the creation and annihilation operators have non- ...
Hilbert space
The mathematical concept of a Hilbert space, named after David Hilbert, generalizes the notion of Euclidean space. It extends the methods of vector algebra and calculus from the two-dimensional Euclidean plane and three-dimensional space to spaces with any finite or infinite number of dimensions. A Hilbert space is an abstract vector space possessing the structure of an inner product that allows length and angle to be measured. Furthermore, Hilbert spaces are complete: there are enough limits in the space to allow the techniques of calculus to be used.Hilbert spaces arise naturally and frequently in mathematics and physics, typically as infinite-dimensional function spaces. The earliest Hilbert spaces were studied from this point of view in the first decade of the 20th century by David Hilbert, Erhard Schmidt, and Frigyes Riesz. They are indispensable tools in the theories of partial differential equations, quantum mechanics, Fourier analysis (which includes applications to signal processing and heat transfer)—and ergodic theory, which forms the mathematical underpinning of thermodynamics. John von Neumann coined the term Hilbert space for the abstract concept that underlies many of these diverse applications. The success of Hilbert space methods ushered in a very fruitful era for functional analysis. Apart from the classical Euclidean spaces, examples of Hilbert spaces include spaces of square-integrable functions, spaces of sequences, Sobolev spaces consisting of generalized functions, and Hardy spaces of holomorphic functions.Geometric intuition plays an important role in many aspects of Hilbert space theory. Exact analogs of the Pythagorean theorem and parallelogram law hold in a Hilbert space. At a deeper level, perpendicular projection onto a subspace (the analog of ""dropping the altitude"" of a triangle) plays a significant role in optimization problems and other aspects of the theory. An element of a Hilbert space can be uniquely specified by its coordinates with respect to a set of coordinate axes (an orthonormal basis), in analogy with Cartesian coordinates in the plane. When that set of axes is countably infinite, this means that the Hilbert space can also usefully be thought of in terms of infinite sequences that are square-summable. Linear operators on a Hilbert space are likewise fairly concrete objects: in good cases, they are simply transformations that stretch the space by different factors in mutually perpendicular directions in a sense that is made precise by the study of their spectrum.
