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.
According to Daniel Gillespie in A Quantum Mechanics Primer (1970),
" . . . any observable which in classical mechanics is some well behaved function of position and momentum, f(x,p), is represented in quantum mechanics by the operator f ( \hat{x} , \hat {p} ) . That is,
a = f (x,p) . . ...
Hi!
First of all I want apologize for my bad english!
Second, I'm doing a physical chemystry course about the main concepts of quantum mechanics !
The Professor has given to me this definition of "the adjoint operator":
<φ|Aψ> = <A†φ|ψ>
My purpose is to verificate this equivalence so i...
Probably trivial, but for matrices with different ranks, Det is not closed for addition?
I think it is closed under multiplication?
So really I must show Det not closed under addition for square matrices of the same order...
$ D(A_n) = \sum_{j=1}^{n} a_{1j}C_{ij} $ and $ D(B_n) =...
Hi, I'm having difficulty with this program in a textbook. The instructions are as follows:
Overload the + operator as indicated. Sample output for the given program:
First vacation: Days: 7, People: 3
Second vacation: Days: 12, People: 3
This is the code that follows
#include <iostream>...
I am trying to perform the operation a on a translated Gaussian, ie. the ground state of the simple harmonic oscillator (for which the ground state eigenfunction is e^-((x/xNot)^2). First, I was able to confirm just fine that a acting on phi-ground(x) = 0. But when translating by xNot, so a...
I need to find a matrix representation for operator A=x\frac{d}{dx} using Legendre polinomials as base.
I would use a_{mn}=\int^{-1}_{-1}P_m(x)\,x\frac{d}{dx}\,P_n(x)\,dx, but I have the problem that Legendre polinomials aren't orthonormal \langle P_{i}|P_{l}\rangle=\delta_{il}\frac{2}{2i+1}.
I...
Homework Statement
The problem originally asks to evaluate ##exp(\frac{-i\pi L_x}{h})## in a ket |l,m>. So I am wondering if I can treat the operator as a parity operator or if I really have to expand that exponential, maybe in function of ##L_+## and ##L_-##.
2. The attempt at a solution
If...
Homework Statement
A function of a hermitian operator H can be written as f(H)=Σ (H)n with n=0 to n=∞.
When is (1-H)-1 defined?
Homework Equations
(1-x)-1 = Σ(-x)n= 1-x+x2-x3+...
The Attempt at a Solution
(1-H)-1 converges if each element of H converges in this series, that is (1-hi)-1...
Hey all,
I got some question referring to the interaction picture. For example:
I have the Hamiltonian ##H=sum_k w_k b_k^\dagger b_k + V(t)=H1+V(t)##
When I would now have a time evolution operator:
##T exp(-i * int(H+V))##.
(where T is the time ordering operator)
How can I transform it...
Hi
can someone direct me to a free software to calculate eigenvalues and normalized eigenfunctions of a linear integral operator. I am trying to solve a fredholm integral equation with degenerate kernel using it instead of linear equations
thanks
sarrah
From P. Meystre's book elements of quantum optics (Many labels of equations are wrong:H) Page 83, the annihilation operator and creation operator, which are helpful to discuss harmonic oscillator, are defined as
##
a=\frac{1}{\sqrt{2\hbar\Omega}}(\Omega q+ip),\\...
I have a linear integral operator
$K\psi=\int_{a}^{b} \,k(x,s) \psi(s) ds$
$L\psi=\int_{a}^{b} \,l(x,s) \psi(s) ds$
both are continuous
I know how to obtain the eigenvalues of each alone.
But how can I calculate the eigenvalues of the operator $I-{L}^{-1} K$ or at least the norm...
Hi everyone,
I tried to find the Eigenstate of the angular momentum operator myself, more specifically I tried to find a Function Y_{lm}(\theta,\phi) with
L_zY_{lm}=mħY_{lm} and L^2Y_{lm}=l(l+1)ħ^2Y_{lm}
where L_z=-iħ\frac{\partial}{\partial \phi}
and...
I am a beginner in quantum mechanics and I am confused about the operator ΔA defined to be ΔA Ξ A - <A>. Can someone please tell me how to interpret <A>? From what I can understand, <A> is the expectation value and is defined to be <Ψ|A|Ψ>. But that is just a scalar correct? How do subtract a...
Hi, I have some trouble with the following problem:
Let E be a Banach space.
Let A ∈ L(E), the space of linear operators from E.
Show that the linear operator φ: L(E) → L(E) with φ(T) = T + AT is an isomorphism if ||A|| < 1.
So the idea here is to use the Neumann series but I can't really...
A basic question, not a homework problem.
Say I have the expression:
5x = 10
Can I apply the derivative operator, d/dx, to both sides?
d/dx(5x)=d/dx(10) would imply 5=0.
I thought you can apply operators to both sides of an equation. Why can't you not do it in this case?
Consider two self-adjoint operators A and B with commutator [A,B]=C such that [A,C]=0.
Now I consider an operator which is a function of A and is defined by the series ## F(A)=\sum_n a_n A^n ## and try to calculate its commutator with B:
## [F(A),B]=[\sum_n a_n A^n,B]= \\ \sum_n a_n...
Homework Statement
I think there may be something wrong with a problem I'm doing for homework. The problem is:
Solve the IVP with the differential operator method:
[D^2 + 5D + 6D], y(0) = 2, y'(0) = \beta > 0
a) Determine the coordinates (t_m,y_m) of the maximum point of the solution as a...
I was studying quantum states in quantum field theory and I came across the formula for defining eigenstates:
|n> = [(a†)n / sqrt(n!)] * |0>
However, my book did not actually define ground state |0> (meaning the book did not give some function or numbers or anything like that to define what...
Homework Statement
Find the eigenvector of the annhilation operator a.
Homework Equations
a|n\rangle = \sqrt{n}|{n-1}\rangle
The Attempt at a Solution
Try to show this for an arbitrary wavefunction:
|V\rangle = \sum_{n=1}^\infty c_{n}|n\rangle
a|V\rangle = a\sum_{n=1}^\infty c_{n}|n\rangle...
Suppose y is a positive vector. Let p and x be two positive matrices with N rows, where ##p_j## and ##x_j## denotes the j:th row in these matrices, so that j = 1,…,N.
Does the following hold:
\inf_{k=1,...,N} [\sup_{l=1,...,N} [p_k(y-x_k)]] = \inf_{k=1,...,N} [p_k(y-x_k)]
where ##p_k(y-x_k)##...
Hi, those who have seen my recent posts will know that I am trying to put together a simple table that I am certain will help me get through a cloud of uncertainty that is proving a major obstacle to my on-going studies. I refer to...
Let (X,d) be a metric space. An operator $T:X\to X$ is said to be quasi nonexpansive if T has at least one fixed point in X and, for each fixed point p, we have
$d\left(Tx,p\right)\le d\left(x,p\right)$ (1)
And also we give a...
Hi, I wish to get position operator in momentum space using Fourier transformation, if I simply start from here,
$$ <x>=\int_{-\infty}^{\infty} dx \Psi^* x \Psi $$
I could do the same with the momentum operator, because I had a derivative acting on |psi there, but in this case, How may I get...
Hi, I feel thoroughly muddled like I am drowning in a soup of terminology and notation, and I have assignment deadlines.
So I have tried to compile a rough table that will give me a consistent base which I can use now - and add to going forward; trying also to stick with the usage in my...
1) Given $\mathcal{L}u=0$ and $ g\mathcal{L}u$ is self-adjoint, show that for the adjoint operator $ \bar {\mathcal{L}}, \bar{\mathcal{L}}(gu)=0$
Is it enough to say that if self-adjoint, then $ \mathcal{L}= \bar {\mathcal{L}} $. I assume g represents a function of x (so no inner products with...
Hi all,
I have a severe confusion about the time-ordering operator. It is the best thing ever, I think, since it simplifies many proofs, due to the fact that operators commute (or anti-commute, but let's take bosonic operators for simplicity) under the time-ordering.
However, sometimes I...
Hello,
This is probably a very easy questions about the one-dimension momentum operator derivation. So you take the d<x>/dt to find the "velocity" of the expectation value. At one point in the derivation early on, you bring in the d/dt into the integral of the expectation value. The book I'm...
I've been given the question "What is ∇exp(ip⋅r/ħ) ?"
I recognise that this is the del operator acting on a wave function but using the dot product of momentum and position in the wave function is new to me. The dot product is always scalar so I was wondering if it would be correct in writing...
Hi guys, I'm trying to understand why does the amplitude of the electric field operator in a cavity is fixed at
\left ( \displaystyle\frac{\hbar\omega}{\epsilon_{0}V} \right )^\frac{1}{2}
Every book I read says it is a normalization factor... but, normalizing an operator?, what is the meaning...
Homework Statement
py and pz are components of the momentum . Do they compatible operators?
Homework Equations
compatible operators equation
The Attempt at a Solution
i think I have to use commutation
Homework Statement
Find the action of the operator ## e^{\vec{a} . \vec{\nabla}} \big( f(\theta,\phi) . g(r) \big) ## where \nabla is the gradient operator given in spherical coordinates, f and g are respectively scalar functions of the angular part ## ( \theta, \phi) ## and the radial part ##...
Homework Statement
From Linear Algebra with applications 7th Edition by Keith Nicholson.
Chapter 9.2 Example 2.
Let T: R3 → R3 be defined by T(a,b,c) = (2a-b,b+c,c-3a).
If B0 denotes the standard basis of R3 and B = {(1,1,0),(1,0,1),(0,1,0)}, find an invertible matrix P such that...
Hi everyone,
I am currently preparing myself for my Bachelor thesis in local quantum field theory. I was encouraged by my advisor to read the books of M. Reed and Simon because of my lag of functional analysis experience but I have quite often problems understand the “obvious” conclusions.
For...
During a course of QFT my teacher said that in this theory is not possible to use the operator X for the position in order to construct with the momentum P and the spin S a set of irreducible operators that charachterize particles, and that we need a different point of wiev: the irreducible...
As fields ##\phi ## are ill defined at precise time and position i read that fields have to be smeared. So we have test functions f in bounded regions in space time. We have a Hilbert space and ##\phi (f) ## is an operator which acts on H.
Maybe we can retrieved the usual wave function when it...
Hamiltonian operator commutes with the linear momentum operator
and for a particle in the box its wavefunction is Nsin(nπx/a) , N is the normalization constant
But I found this wavefuntion is not a eigenfuntion for the momentum operator, why? Isn't the two operators commut with each other?
Homework Statement
Let T:V→V be a linear operator on a vector space V over C:
(a) Give an example of an operator T:C^2→C^2 such that R(T)∩N(T)={0} but T is not a projection
(b) Find a formula for a linear operator T:C^3→C^3 over C such that T is a projection with R(T)=span{(1,1,1)} and...
Sorry if the answer is very simple, but I just had a question regarding error propagation when using a modulo operator in intermediate steps. For example, I have ## \theta = arctan(\frac {A}{B}) ## and then I do ## \theta ## % ##2\pi## (modulo ##2\pi##). This gives me an answer between ##...
Hey JO.
The Hamiltonian is:
H= \frac{p_{x}^{2}+p_{y}^{2}}{2m}
In quantum Mechanics:
\hat{H}=-\frac{\hbar^{2}}{2m}(\frac{\partial^{2}}{\partial x^{2}}+\frac{\partial^{2}}{\partial x^{2}})
In polar coordinates:
\hat{H}=-\frac{\hbar^{2}}{2m}( \frac{\partial^{2}}{\partial r^{2}}+\frac{1}{r}...
Hi all,
Quick quantum question. I understand the total angular momentum operation \hat{L}^2 \psi _{nlm} = \hbar\ell(\ell + 1) \psi _{nlm} which means the total angular momentum is L = \sqrt{\hbar\ell(\ell + 1)} But how about applying this to an arbitrary superposition of eigenstates such as...
The experiment is described at p26 of http://arxiv.org/abs/quant-ph/0402001
In this experiment we see that we sum measurement results and not measure the sum.
Is then the quantum measurement operator not :
$$S=A\otimes B\otimes\mathbb{1_{64}}-\mathbb{1_{4}}\otimes A\otimes...
For particle in the box wave function, it is the eigenfunction of kinetic energy operator but not the eigenfunction of momentum operator. So, do these two operators commute? (or it has nothing to do with commutator stuff?)
How about for free particle? For free particle, the wave function is...
In a multi-particle system, the total state is defined by the tensor product of the individual states. Why is it the case that operators, say position of 2 particles, is of the form X⊗I + I⊗Y and not X⊗Y where I are the identities for the respective spaces and X and Y are the position operators...
Hello, I'm sorry if this question sounds silly, but in QM the Momentum Operator is ##{\hat{p}}=-i{\hbar}{\nabla}## . In Relativistic QM in Flat Space, this operator can be written ##{\hat{P}_{\mu}}=-i{\hbar}{\partial}_{\mu}## . Would it be correct, then, to say that in curved spacetime the...
Hello. I need help with the following:
Suppose a basis set of states $\varphi_i$. Calculate the effect of the operator $\widehat{R} \equiv \Pi_i \left( \widehat{Q} -q_i \right)$ on an arbitrary state $\Psi$, assuming that the equation $\widehat{Q} \varphi_i = q_i \varphi_i$ is satisfied.
I'm...
Hi
I know Fredholm linear integral equations i.e.
$y(x)=f(x)+\lambda\int_{a}^{b} \,k(x,s)y(s)ds$
can be written compactly in the operator form as $y=f+\lambda Ky$
this facilitates many proofs. Usually there is a condition on $\lambda$ for the convergence of say successive approximations method...