In mathematics, a differential operator is an operator defined as a function of the differentiation operator. It is helpful, as a matter of notation first, to consider differentiation as an abstract operation that accepts a function and returns another function (in the style of a higher-order function in computer science).
This article considers mainly linear differential operators, which are the most common type. However, non-linear differential operators also exist, such as the Schwarzian derivative.
If you consider a bounded linear operator between two Hausdorff topological vector spaces, isn't the kernel *always* closed? I mean, if you assume singleton sets are closed, then the set \{0\} in the image is closed, so that means T^{-1}(\{0\}) is closed, right (since T is assumed continuous)? I...
Homework Statement
Why does <0|\frac{1}{(2\pi)^3}∫ \hat{a}^{\dagger}(t,r) \hat{a}(t,r) d^{3} \textbf{k} |0> = \frac{1}{\pi^2}∫|β|^2 k^2 dk.
Where \hat{a} and \hat{a}^{\dagger} and its conjugate are bogulobov transformations given by:
\hat{a}(t,k) = \alpha(t)a(k) + β(t)b^{\dagger}(-k)...
Homework Statement
Stationary states are related by 1/m*pij = Ei-Ej/(i*hbar) *xij where pij = ∫ψi(x)*p*ψj (x) and similarly for xij
Homework Equations
Classical correspondence for equation of motion is d<x>/t = <p>/m
Schrodinger equation
Ehrenfest Theorem
Fourier Transform
The...
Homework Statement
Verify whether or not the operator
L(u) = u_x + u_y + 1
is linear.
Homework Equations
An operator L is linear if for any functions u, v and any constants c, the property
L(c_1 u + c_2 v) = c_1 L(u) + c_2 L(v)
holds true.
The Attempt at a Solution
I feel...
Hey,
I'm having trouble interpreting a question, as the solutions say something different... Anyways the question part d) below:
So we want to determine the expectation value of the y-component of the electron spin on the eigenstate of Sx, now I would of thought this was given by...
Hey,
I have a question on showing how the raising operator in QM raises a particular eigenstate by 1 unit, the question is showed below:
I think I know how to do this but not sure if what I'm doing is sufficient:
\hat{N}a^{\dagger}|n>=([\hat{N},a^{\dagger}]+a^{\dagger}\hat{N})|n>...
"Del" operator crossed with a scalar times a vector proof
Homework Statement
Prove the following identity (we use the summation convention notation)
\bigtriangledown\times(\phi\vec{V})=(\phi \bigtriangledown)\times\vec{V}-\vec{V}\times(\bigtriangledown)\phi
Homework Equations
equation for...
I have the following situation: About the polarization of the photon, I introduce the basis:
Horizontal polarization $|\leftrightarrow>=\binom{1}{0}$
Vertical polarization $|\updownarrow>=\binom{0}{1}$
The density matrix in this problem is:
$$\rho =\frac{1}{2}\begin{pmatrix}
1+\xi...
Hello. I have some questions on operations.
Suppose in the course of a derivation there is a mathematical statement of the form
A+1=B+C
then "+" is an operator acting on inputs "B" and "C".
Question 1: Is the output of the operation "A" or the expression "B+C"?
The reason I think the...
I have a problem where it's said that the operator Q is likely to be:
Q=\sum^3_{i=1}[\frac{1}{2}B_i + I_{3,i}]
I have to apply this to the proton wave function which is the same as you can see in equation (3.20) here...
Homework Statement
How to prove that for any representation of the spin, the state e^{-i{\pi}J_x/\hbar}|j,m\rangle
is proportional to |j,-m\rangle
The exponential term is the rotation operator where J_x is the x-component of the total angular momentum operator,
and |j,m\rangle is an...
Hey,
I have the following question on Hermitian operators
Initially I thought this expectation value would have to be zero as the eigenvectors are mutually orthogonal due to Hermitian Operator and so provided the eigenvectors are distinct then the expectation would be zero... Though...
The book I am going through says this :
The below proposition is false for real inner product spaces. As an example, consider the operator T in R^2 that is a counter clockwise rotation of 90 degrees around the origin. Thus , T(x,y) = (-y,x). Obviously, Tv is orthogonal to v for every v in...
For the free particle the solution to the SE are eigenstates of the momentum.
You get something like:
ψ = Aexp(ik(x-vt)) + Bexp(-ik(x+vt)) , where k is a constant
And my book then says that first term represents a wave traveling to the right and the second a wave traveling to the left. But I...
I was looking for a hint on a problem in my professor's notes (class is over and I was just auditing).
I want to show that if T:V→V is a linear operator on finite dimensional inner product space, then if T is diagonalizable (not necessarily orth-diagonalizable), so is the adjoint operator of...
http://upload.wikimedia.org/math/2/b/2/2b2fe1336915a03e04930c11b27f4585.png
The above link shows the material derivative. Which is the derivative that follows a volume of fluid throughout its movement through a fluid. How is this derived from a chain rule? Is the v in that equation the...
Homework Statement
Homework Equations
The Attempt at a Solution
I don't know what's wrong with my work. I can't obtain the eigenvector provided in the model answer.
My work
Model Answer
Homework Statement
I'm trying to find the divergence of a vector field (a fluid flow vector), but the vector takes the form u = u(x,y,z,t)
The Attempt at a Solution
I only really know how to take the divergence of a time-independent vector, so I'm guessing I just take the partial...
eigenvalues of a compact positive definite operator!
Let A be a compact positive definite operator on Hilbert space H.
Let ψ1,...ψn be an orthonormal set in H.
How to show that <Aψ1,ψ1>+...+<Aψn,ψn> ≤ λ1(A)+...+λn(A), where
λ1≥λ2≥λ3≥... be the eigenvalues of A in decreasing order.
Can...
I have bumped into a term
a^\dagger \hat{O}_S | \psi \rangle
I would really like to operate on the slater determinant \psi directly, but I fear I cannot. Is there any easy manipulation I can perform?
Hi
I am reading a paper (http://arxiv.org/abs/0901.3105), where they after eq. (3) mention something I can't understand. First of all, (3) comes from the master equation of a collection of N atoms in a cavity. They say that (page 2, right after (3)):
The last term describes the coupling of...
In the QM Hamiltonian, I keep seeing h-bar/2m instead of p/2m for the kinetic energy term. H-bar is not equivalent to momentum. What am I missing here?
Hey, I recently had an exam where the quantum state were on the form
|\psi\rangle = \frac{1}{\sqrt{2}} ( |+\rangle + i |-\rangle )
Here I formed the density operator for the pure state
\rho(t) = |\psi\rangle \langle \psi| = \frac{1}{2} ( |+\rangle + i |-\rangle )( \langle +| - i \langle...
So, I'm studying Second Quantization for fermions and came across this equation. I was just wondering why there is a summation needed? And why do we do it with (i≠p).? Please can someone explain this to me?
Reply and help is much appreciated.
Homework Statement
Show that the expectation operator E() is a linear operator, or, implying:
E(a\bar{x}+b\bar{y})=aE(\bar{x})+bE(\bar{y})
Homework Equations
E(\bar{x})=\int_{-\infty}^{+\infty}xf_{\bar{x}}(x)dx
With f_{\bar{x}} the probability density function of random variable x...
I was wondering about this: The identity operator writes a vector in the basis that is used to express the identity operator:
1 = Ʃlei><eil
But if you are to apply it to a vector in a given basis A should the lei> then be expressed in terms of their own basis or in terms of A?
We all know the greek letter delta is the mathematical symbol that represents "change in."
I though about a new form of delta: Δn. Where n2 = the # of terms when you expand the delta operator.
For example: the usual Δx = x2 - x1
But now: Δ2x = (X4-X3) - (X2-X1). We can see that for Δ2...
What are the eigenfunctions of the spin operators? I know the spin operators are given by Pauli matricies (https://en.wikipedia.org/wiki/Spin_operator#Mathematical_formulation_of_spin), and I know what the eigenvalues are (and the eigenvectors), but I have no idea what the eigenfunctions of the...
when we have a certain state ψ(t)
and it is acted on by an operator A of eigenstates a, b, c and eigen vectors la>, lb>, lc>
does it mean that after measuring A ( if the result was 'a'), the state lψ(t)> becomes in state la>?
Homework Statement
I have a number of problems, to be completed in the next day or so (!) that I am pretty stuck with where to begin. They involve calculating the spectra of various different linear operators.
Homework Equations
The first was:
Let X be the space of complex-valued...
Homework Statement
Consider the set of functions {f(x)} of the real variable x defined on the interval -\infty< x < \infty that go
to zero faster than 1/x for x\rightarrow ±\infty , i.e.,
\lim_{n\rightarrow ±\infty} {xf(x)}=0
For unit weight function, determine which of the...
I'm trying to understand the construction of the T(ε) operator and why it is equal to I-iεG/hbar.
The textbook I'm using (Shankar) talks defines the translation operator with the phase factor:
T(ε)\left|x\right\rangle=e^{i \epsilon g(x)/\hbar}\left|x+\epsilon\right\rangle
and...
I cannot quite understand why expression \frac{1-\gamma_5 \slashed{s}}{2} is covariant? We defined it in the rest frame, and then said that because it is in the slashed expression, it's covariant, what does that mean? s is the direction of polarization, s \cdot s = -1
Hello,
I am having trouble when solving non-homogeneous DE's how to find the annihilator to find my particular solution.
For example, if you have a DE that equals 24x^2cos(x), how do I find something that will annihilate this? It seems to me no matter how many derivatives you take, you...
I just have two questions relating to what I have been studying recently.
1) I know that the total energy and momentum operators don't commute, while the kinetic energy and momentum operators do. Why is this the case? (explanation rather than mathematically).
2) One form of the HUP says that...
Homework Statement
I need to express the rotation operator as follows
R(uj) = cos(u/2) + 2i(\hbar) S_y sin(u/2)
given the fact that
R(uj)= e^(iuS_y/(\hbar))
using |+-z> as a basis,
expanding R in a taylor series
express S_y^2 as a matrix
Homework Equations
I know...
I know that the average momentum <p> is defined as m\frac{d}{dt}<x>. But why is this also equal to :
\intψ*\frac{h}{(2\pi)i}\frac{\partial ψ}{\partial x}dx ?
the integral goes from negative inf to inf, * indicates conjugate,ψ the wavefunction.
Also, why is it in general that for any average...
Let M be the space of all 2 × 2 complex matrices,
satisfying 〖(X)bar〗^t = -X (skew-hermitian).
Consider M as a vector space over R.
Define a bilinear form B on M by B(X,Y) = -tr(XY)
(1) Show that B takes real values, is symmetric and positive definite.
(2) For any A ∈ M , define the...
I should Use
the fact that in general the eigenvalues of the square of the angular momentum
operator is J(J + 1)h and show the spin of the electron.
I have J= L+S and J2 = L2+ S2
Homework Statement
But how could i find the spin of the electron
Like the title says, why are the only possible values of an operator its eigenvalues?
reading shankar right now and I'm having difficulty understanding why this has to be the case, given some operator/variable Ω
Suppose T belongs to L(V,V) where L(A,W) denotes the set of linear mappings from Vector spaces A to W, is such that every subspace of V with dimension dim V - 1 is invariant under T. Prove that T is a scalar multiple of the identity operator.
My attempt : Let U be one of the sub spaces of V...
Change of the "Del" operator in two particle interactions
Ok,so John Taylor's Classical Mechanics has this small subtopic "energy interactions between 2 particles".And,in that,hes defined a "del1" operator as the vector differential operator with respect to particle 2 at the origin.Hence,the...
There are 2 operators such that [A,B] = 0. Does [F(A),B]=0 ?
Specifically, let's say we had the Hamiltonian of a 3-D oscillator H and L^2. We know that L^2 = Lx^2+Ly^2+Lz^2, and it is known that [H,Lz] = 0. Can we say that since H and Lz commute, H and Lz^2 also commute, by symmetry H and...
Hi
Often in the context of multi-atom systems, such as in cavity QED, it is customary to introduce a so-called "collective pseudospin operator". An example of this is for the inversion for some atom j, \sigma_{j, z}, which becomes
\sum_{j} \sigma_{z, j} = \sigma_z
To me this seems very...
I want to be on the cutting edge of nuclear engineering, but I am afraid that I might not have the genius necessary to do it. I'm in my first semester of taking NucE classes, and my Fluid Mechanics class is tearing me up! Not to mention my Fundamentals of Nuclear Science/Engineering class is...
Hi all
Homework Statement
Given is a Hermitian Operator H
H= \begin{pmatrix}
a & b \\
b & -a
\end{pmatrix}
where as a=rcos \phi , b=rsin \phi
I shall find the Eigen values as well as the Eigenvectors. Furthermore I shall show that the normalized quantum states are:
\mid +...
Homework Statement
Consider a Hilbert space with a (not necessarily orthogonal) basis \{f_i\} Show that G=\sum_i |f_i\rangle\langle f_i| has strictly positive eigenvalues.
Homework Equations
The Attempt at a Solution
I know that G=\sum_i |f_i\rangle\langle f_i| is hermitian...
I am reading a quantum mechanics book. I did not clearly understand one particular idea.
When the book talks about the time-evolution operator U(t,t_0), it says that one very important property is the unitary requirement for U(t,t_0) that follows from probability conservation.
My question is...