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.
Hi All,
I have spent hours trying to understand the matrix form of Density Operator. But, I fail. Please see page 2 of the attached file. (from the book "Quantum Mechanics - The Theoretical Minimum" page 199).
Most appreciated if someone could enlighten me this.
Many thanks in advance.
Peter Yu
Homework Statement
let A be a lowering operator.
Homework Equations
Show that A is a derivative respects to raising operator, A†,
A=d/dA†
The Attempt at a Solution
I start by defining a function in term of A†, which is f(A†) and solve it using [A , f(A†)] but i get stuck after that. Can...
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I have a linear integral operator (related to integral equations)
$(Ky)(x)=\int_{a}^{b} \,k(x,s) y(s) ds$ and another one $(Ly)(x)=\int_{a}^{b} \,l(x,s) y(s) ds$ both are continuous
Before I proceed can I write:
$Ky=\int_{a}^{b} \,k(.,s) y(s) ds$ ? (I saw...
Homework Statement
Suppose A^ and B^ are linear quantum operators representing two observables A and B of a physical system. What must be true of the commutator [A^,B^] so that the system can have definite values of A and B simultaneously?
Homework Equations
I will use the bra-ket notation for...
Hello, could you please give me an insight on how to get through this proof involving operators?
Proof: Given an eigenvalue-eigenvector equation, suppose that the vectorstate depends on an external parameter, e.g. time, and that over it acts an operator that is the fourth derivative w.r.t...
a
In the formula above, on the left hand side, ρ(0) is a system's density operator in its initial state. a is the annihilator operator of the system, and a+ is the create operator of the system. ρss is the system's density operator in its steady state.
But I don't understand why this formula...
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## [V_i,J_j] = i\hbar \epsilon_{ijk}V_k##
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Homework Statement
I am working through a time independent perturbation problem and I am calculating the first order correction to the energy, and I am stuck operating the perturbation : v = i b (Exp[i g x]-Exp[-i g x]) on the ground state |0>.
Homework Equations
<0| v |0> = 1st order...
Suppose I have a system of fermions in the ground state ##\Psi_0##. If I operate on this state with the number operator, I get
\langle \Psi_0 | c_k^{\dagger} c_k | \Psi_0 \rangle = \frac{1}{e^{(\epsilon_k - \mu)\beta} + 1}
which is, of course, the fermi distribution. What if I operate with...
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I was also wondering how to derive the following for the ##l^{th}## partial wave of the above operator:
##-\frac{d^2}{dr^2}-\frac{3}{r}\frac{d}{dr} + \frac{l(l+2)}{r}+...
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For the spin angular momentum operator, the eigenvalue problem can be formed into matrix form. I will use ##S_{z}## as my example
$$S_{z} | \uparrow \rangle = \begin{pmatrix} a & b \\ c & d \end{pmatrix} \begin{pmatrix} 1 \\ 0 \end{pmatrix} = \frac {\hbar}{2} \begin{pmatrix} 1 \\ 0...
Homework Statement
Derive the infinitesimal rotation operator around the z-axis.
Homework Equations
My book gives this equation (which I follow) with epsilon the infinitesimal rotation angle:
$$ \hat{R}(\epsilon) \psi(r,\theta, \phi) = \psi(r,\theta, \phi - \epsilon) $$
but I just don't get...
Homework Statement
I have quite a straightforward question on the taylor expansion however I will try to provide as much context to the problem as possible:
##T(a)## is unitary such that ##T(-a) = T(a)^{-1} = T(a)^{\dagger}## and operates on states in the position basis as ##T(a)|x\rangle =...
Homework Statement
Homework EquationsThe Attempt at a Solution
This whole thing about angular momentum has me totally confused and stumped, but I am trying this problem given in a youtube video lecture I watched.
I know of this equation
##L^{2} = L_{\pm}L_{\mp} + L_{z}^{2} \mp \hbar L_{z}##...
Homework Statement
A measurement is described by the operator:
|0⟩⟨1| + |1⟩⟨0|
where, |0⟩ and |1⟩ represent orthonormal states.
What are the possible measurement outcomes?
Homework Equations
[/B]
Eigenvalue Equation: A|Ψ> = a|Ψ>
The Attempt at a Solution
Apologies for the basic...
Trying to derive two functions which are eigenfunctions of the hamiltonian of 2 identical and indistinguishable particles and also eigenfunctions of the 2-particle exchange operator P.
Need some help with my workings I think.Have particle '1' and particle '2' in a hamiltonian given as...
As far as I know, the momentum operator is as follows:
-iħ(∂/∂x)
Now let's say that I enact this operator on the famous solution to the 1-D particle in a box example:
Ψ= squrt(2/L) sin(πnx/L)
If the momentum operator operates on the above wave function, it yields:
-iħ * squrt(2/L) * (πn/L)...
I was introduced to the d operator to help solve constant coefficient differential equations for the particular integral without using trial solutions:
http://en.wikipedia.org/wiki/Differential_operator
http://en.wikipedia.org/wiki/Shift_theorem
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I'm trying to show that \int d^3x \,x^\mu \left(\partial_\mu \partial_0-g_{\mu 0} \partial^2 \right)\phi^2(x)=0 . This term represents an addition to a component of the energy-momentum tensor \theta_{\mu 0} of a scalar field and I want to show that this does not change the dilation operator...
Homework Statement
Homework EquationsThe Attempt at a Solution
a) I am having some trouble understanding the notation. I'm uncertain whether it should be
$$ \langle {f} | \hat {O_{2}} | g \rangle = \int_{-\infty}^{\infty} f^{*}g \frac {dg}{dx} dx $$
or
$$ \langle {f} | \hat {O_{2}} | g...
Hi,
I've learned that material derivative is equal to local derivative + convective derivative, but can't seem to find out which way the convective derivative acts, like for example in velocity fields:
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Acceleration = material...
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If I apply the Divergence Operator on the incompressible Navier-Stokes equation, I get this equation:
$$\nabla ^2P = -\rho \nabla \cdot \left [ V \cdot \nabla V \right ]$$
In 2D cartesian coordinates (x and y), I am supposed to get:
$$\nabla ^2P = -\rho \left[ \left( \frac...
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The question is as follows:
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So I've started by writing...
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Homework Statement
Simplify the following commutator involving the creation and annihilation operators.
[a^{\dagger}a,a \sqrt{a^\dagger a} ]
Homework Equations
I know that [a,a^\dagger] = 1.
The Attempt at a Solution
I think I should be trying to put the creation operators to the left...
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Hello everyone. What it the result for a Gaussian functional integral when the "matrix" is nothing but a number? Mathematically speaking is the following true?
$$
\int \mathcal{D}\phi e^{-\int d^3k f(k) |\phi(k)|^2}\propto \left(f(k)\right)^{-1/2}
$$
Here ##f(k)## is just a function of k, not...
Homework Statement
I know that Unitary operators act similar to hermitean operators.
I want to prove that the eigenvalues of unitary operators are complex numbers of modulus 1, and that Unitary operators produce orthogonal eigenvectors.
Homework Equations
U†U = I
U-1=U†
λ = eiΦ{/SUP]...
Homework Statement
Consider a two-dimensional space spanned by two orthonormal state vectors \mid \alpha \rangle and \mid \beta \rangle . An operator is expressed in terms of these vectors as
A = \mid \alpha \rangle \langle \alpha \mid + \lambda \mid \beta \rangle \langle \alpha \mid +...
I am currently reading up on some algebraic topology\differential geometry and have reached the section on de Rham theory. This is my first encounter with such notions and I am a little confused by what is meant when one applies a boundary operator to a simplex. Conceptually, I know that it...
One can represent the mean of the angular momentum operator as a vector. But what is the (mathematical) justification to represent the operator by a vector which has a direction that the operator has not. Yet worse, l(l+1) h2 is the proper value of operator L^2 and from such result it is assumed...
Homework Statement
Given the series of three Stern-Gerlach devices:
Represent the action of the last two SG devices as matrices ##\hat{A}## and ##\hat{B}## in the ##|+z\rangle, |-z\rangle## basis.
Homework Equations
##|+n\rangle = cos(\frac{\theta}{2})|+z\rangle +...
This paper is about momentum operator in curvilinear coordinates. The author says that using \vec p=\frac{\hbar}{i} \vec \nabla is wrong and this form is only limited to Cartesian coordinates. Then he tries to find expressions for momentum operator in curvilinear coordinates. He's starting...
Anyone having an idea of how to solve problem 3a) file:///C:/Users/Administrator/Downloads/handin1%20(2).pdf ?
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How do I prove that the parity operator Af(x) = f(-x) commutes with the second derivative operator. I am tempted to write:
A∂^2f(x)/∂x^2 = ∂^2f(-x)/∂(-x)^2 = ∂^2f(-x)/∂x^2 = ∂^2Af(x)/∂x^2
But that looks to be abuse of notation..
hello,
i am trying to learn the derivation of the momentum operator and i found 2 ways of deriving it. one is using Fourier transform and the other is taking the time derivative of the expectation value of x.
i just want to know what is the physical interpretation of the time rate of change...
Homework Statement
Let C be the composition operator on the Hilbert space L_{2}(\mathbb{R}) with the usual inner product. Let f\in L_{2}(\mathbb{R}), then C is defined by
(Cf)(x) = f(2x-1), \hspace{9pt}x\in\mathbb{R}
give a demonstration, which shows that C does not have any eigenvalues...
Homework Statement
Given that the function f can be expanded in a power series of a and a^\dagger, show that:
[a,f(a,a^{\dagger})]=\frac{\partial f }{\partial a^\dagger}
and that
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I've tied using...