In the mathematical field of graph theory, a Hamiltonian path (or traceable path) is a path in an undirected or directed graph that visits each vertex exactly once. A Hamiltonian cycle (or Hamiltonian circuit) is a Hamiltonian path that is a cycle. Determining whether such paths and cycles exist in graphs is the Hamiltonian path problem, which is NP-complete.
Hamiltonian paths and cycles are named after William Rowan Hamilton who invented the icosian game, now also known as Hamilton's puzzle, which involves finding a Hamiltonian cycle in the edge graph of the dodecahedron. Hamilton solved this problem using the icosian calculus, an algebraic structure based on roots of unity with many similarities to the quaternions (also invented by Hamilton). This solution does not generalize to arbitrary graphs.
Despite being named after Hamilton, Hamiltonian cycles in polyhedra had also been studied a year earlier by Thomas Kirkman, who, in particular, gave an example of a polyhedron without Hamiltonian cycles. Even earlier, Hamiltonian cycles and paths in the knight's graph of the chessboard, the knight's tour, had been studied in the 9th century in Indian mathematics by Rudrata, and around the same time in Islamic mathematics by al-Adli ar-Rumi. In 18th century Europe, knight's tours were published by Abraham de Moivre and Leonhard Euler.
I'm having some trouble grasping the meaning of the exchange term in the Hamiltonian Heisenberg gives in his classic 1932 paper (the one typically given as the first to describe nucleons via a spin-like degree of freedom; NOTE: I realize this isn't the same as what is today called isospin, but...
Homework Statement
H = \frac{2e^2}{\hbar^2 C} \hat{p^2} - \frac{\hbar}{2e} I_c cos\hat\theta ,
where [\hat\theta , \hat{p}] = i \hbar
How can we write the expression for the Hamiltonian in the basis |\theta>
Homework EquationsThe Attempt at a Solution
I have already solved most part of...
Could someone please explain Hψ = Eψ? I understand that H = Hamiltonian operator and ψ is a wavefunction, but how is H different from E? I am confused. I am trying to understand "Hψ = Eψ" approach
Homework Statement
Prove the relationship
$$\left(\frac{\partial H}{\partial\lambda}\right)_{nn} = \frac{\partial E_{nn}}{\partial\lambda},$$
where ##\lambda## is a parameter in the Hamiltonian. Using this relationship, show that the average force exerted by a particle in an infinitely deep...
If the hamiltonian is defined as ##\mathcal{H}\equiv \sum _{ i }^{ all }{ p_{ i }\dot { q } _{ i } } - \mathcal{L} ##, how is it considered a function of ##p## and ##q## instead of ##p## and ##\dot{q}##?
Chris
I've read a couple of places that a hamiltonian can be a tool used in classical mechanics and that it's eigenvalues are useful pieces of information. I've tried finding info on the subject matter, as I want to see something that actually requires linear algebra, or at least makes good use of it...
In the lagrangian formalism, we treat the position ##q## and the velocity ##\dot q## as dependent variables and talk about configuration space, which is just the space of positions. In the hamiltonian formalism we talk about canonical positions and momenta, and we consider them independent. Is...
Homework Statement
Prove that for any stationary state the average of the commutator of any operator with the Hamiltonian is zero: \langle\left[\hat{A},\hat{H}\right]\rangle = 0.
Substitute for \hat{A} the (virial) operator:\hat{A} = \frac{1}{2}\sum\limits_i\left(\hat{p}_ix_i...
So, I was reading about the exchange interaction, and trying to work out what it referred to, and came across something strange in the treatment of the hydrogen molecule (I think it was on wikipedia):
The hamiltonian given for the system included a term e2/(4πε0 * Rab) for the repulsion between...
Homework Statement
A magnetic field pointing in ##\hat{x}##. The Hamiltonian for this is:
##H= \frac{eB}{mc}\begin{pmatrix}
0 & \frac{1}{2}\\
\frac{1}{2} & 0
\end{pmatrix}##
where the columns and rows represent ##{|u_z\rangle, |d_z\rangle}##.
(a) Write this out in Dirac...
According to my book, and wiki http://en.wikipedia.org/wiki/Hamiltonian_mechanics#As_a_reformulation_of_Lagrangian_mechanics,
##\frac{\partial{H}}{\partial{t}} = - \frac{\partial{L}}{\partial{t}}##, where ##L## is the Lagrangian.
But how can this be? This assumes the generalized...
Is there any difference between Hamiltonian operator and E? Or do we describe H as an operation that is performed over (psi) to give us E as a function of (psi)??
Homework Statement
So I just learned how to derive the equation of motion under the Lagrangian formulation which involves finding the euler-lagrange equation when setting the change in action to zero, chain rule, integration by parts etc.. Then I learned how to find the equations of motion...
Definition/Summary
The Hamiltonian, like the Lagrangian, is a function that summarizes equations of motion. It has the additional interpretation of giving the total energy of a system.
Though originally stated for classical mechanics, it is also an important part of quantum mechanics...
I've got a problem which is asking for the eigenvalues and eigenstates of the Hamiltonian H_0=-B_0(a_1 \sigma_z^{(1)}+a_2 \sigma_z^{(2)}) for a system consisting of two spin half particles in the magnetic field \vec{B}=B_0 \hat z .
But I think the problem is wrong and no eigenstate and...
How does one think about, and apply, in the classical mechanical Hamiltonian formalism?
From the Lagrangian perspective, Noether's theorem (in 1-D) states that the quantity
\sum_{i=1}^n \frac{\partial \mathcal{L}}{\partial ( \frac{d y_i}{dx})} \frac{\partial y_i^*}{\partial \varepsilon} -...
This is related to classical Hamiltonian mechanics. There is something wrong
in the following argument but I cannot pinpoint where exactly the pitfall is:
Consider an arbitrary (smooth) Hamiltonian (let us assume conservative) and 2n
phase space coordinates (q,p). The Hamiltonian flow gives...
Hello,
The question says that we can write the Hamiltonian of the harmonic oscilator like this:
H=0.5*[P^2/m + (4*h^2*x^2)/(m*σ^4)] where h is h-bar
I need to calculate the expectation value of energy of the oscilator with the next function: ψ(x)=A*exp{-[(x-bi)^2]/σ^2}.
I tried to the...
I am working through Leonard Susskinds 'the theoretical minimum' and one of the exercises is to show that H=ω/2(p^2+q^2).
The given equations are H=1/2mq(dot)^2 + k/2q^2, mq(dot)=p and ω^2=k/m.
q is a generalisation of the space variable x, and (dot) is the time derivative if this helps...
I'm learning ray optics and feeling so confused by the definition of "Hamiltonian of light".
What I learned was that the "Hamiltonian of light" defined by H = n-|\vec{p}| = 0 indicates the momentum conservation, where n is refractive index and \vec{p} here is the canonical momentum. The...
Hi all,
I am working on DFT calculations using SIESTA. I have obtained the Hamiltonian file (.HSX) from the calculations. But, I cannot read the file it. How do I read the .HSX file .
Hi, The following contains two questions that I encountered in the books of Claude Cohen-Tannoudji, "Atom-Photon Interactions" and "Atoms and Photons: Introduction to Quantum Electrodynamics". The first one is about how to calculate two Fourier transforms, and the second one is a example of...
I completely do not understand How they work .
Here is a link to my unanswered stack exchange question.
Could anyone help me? Would you like any clarifications?
http://physics.stackexchange.com/questions/112034/can-someone-explain-to-me-the-rocksar-kivelson-hamiltonian
Homework Statement
a) The operators ##a## and ##a^{\dagger}## satisfy the commutation relation ##[a,a^{\dagger}] = 1##. Find the normalization of the state ##|\psi \rangle = C (a^{\dagger} )^2 |0\rangle##, where the vacuum state ##|0\rangle## is such that ##a|0\rangle = 0##
b)A one...
Homework Statement
Part (a): Show the Commutation relation [x, [H,x] ]
Part (b): Show the expression by taking expectation value in kth state.
Part (c): Show sum of oscillator strength is 1. What's the significance of radiative transition rates?Homework Equations
The Attempt at a Solution...
1. Is the root(det(q)) term in the Hamiltonian Constraint what makes it non polynomial
2. Is the motivation for Ashtekar Variables to remove the non polynomial terms by replacing the Hamiltonian with a densitised Hamiltonian
Homework Statement
I'm working (self-study) through Goldstein et al, Classical Mechanics, 3rd Edition, and I'm currently stuck on Problem 8.11:
A particle is confined to a one-dimensional box. The ends of the box (let these be at \pm l(t)) move slowly towards the middle. By slowly we mean...
Homework Statement
We want to get the time evolution of a wavefunction and the expectation value of the Hamiltonian, and from there we can show that it's the same as the time-independent result. So to be clear: given a wavefunction, get the time evolution of that function and the expectation...
Helloo,
I don't understand how one arrives at the conclusion that the hamiltonian is a generating function.
When you have an infinitesimal canonical transformation like:
Q_{i}=q_{i}+ \delta q_{i}
P_{i}=p_{i}+\delta p_{i}
Then the generating function is:
F_{2}=q_{i}P_{i}+ \epsilon...
Homework Statement
The point of suspension of a simple pendulum of length l and mass m is constrained to move on
a parabola z = ax^2 in the vertical plane. Derive a Hamiltonian governing the motion of the
pendulum and its point of suspension. This is a two-dimensional problem...
Homework Statement
A massless spring of length b and spring constant k connects two particles of masses m_1 and m_2 .
The system rests on a smooth table and may oscillate and rotate.
a) Determine the Lagrange's equations of motion.
b) What are the generalized momenta associated with...
Homework Statement
To try and relate the three ways of calculating motion, let's say you have a particle of some mass, completely at rest, then is acted on by some force, where F equals a constant, C, times time. (C*t).
I want to find the equations of motion using Lagrangrian, but also Newton...
Hello,
there are several papers on QCD in Hamiltonian formulation, especially in Coulomb gauge. Unfortunately the Hamiltonian H is rather formel and highly complex.
Question: is there a paper discussing the contribution of individual terms of H to the nucleon mass?
How many ways can we change the Hamiltonian without affecting the wave functions (eigenvectors) of it.
Like multiply all the elements in the matrix by a constant.
I'm facing a very difficult Hamiltonian,:cry: I want to simplify it, so the wave function will be much easier to derive.
Thanks in...
I know I've seen this point about roots discussed somewhere but I can't for the life of me remember where. I'm hoping someone can point me the right direction.
Here's the situation:-
The standard derivation of the quantum HO starts with the classic Hamiltonian in the form H = p2 + q2...
Hi
I have been looking at canonical transformation using generating functions. I am using the Goldstein book and it gives the following example -
F1=qQ ⇔ Q=p and P=-q
F2=qP ⇔ Q=q and P=p
F3=pQ ⇔ Q=-q and P=-p
F4=pP ⇔ Q=p and P=-q
I'm confused ! Obviously functions 1 and 4 give the...
Hi All,
Greetings!
I have a 3d material and I use result from first principal for getting the potential (U(x,y,z)). I then find average U(x) from U(x,y,z). Now if I write one dimensional Hamiltonian in X direction and use this value of U(x), can I get bandgap of the original 3d material (I...
Hi All,
Greetings !
Here is what I wish to know. Specifying a tight binding hamiltonian requires values of potential (U). Consider a 3d solid. If I have potential profile in x direction (U1, U2, U3...so on) can I directly plug in these U values into the tight binding hamiltonian or do I...
I am reading an article on the "energy surface" of a Hamiltonian. For a simple harmonic oscillator, I am assuming this "energy surface" has one (1) degree of freedom. For this case, the article states that the "dimensionality of phase space" = 2N = 2 and "dimensionality of the energy surface" =...
For two electron system ##\vec{S}_1##, ##\vec{S}_2##
\mathcal{H}=J\vec{S}_1\cdot \vec{S}_2=J(\frac{1}{2}(S_{tot})^2-\frac{3}{4}) (1)
How you get relation (1)?
Just a little doubt.
When we are performing a canonical transformation on a Hamiltonian and we have the equations of the new coordinates in terms of the old ones we have to find the Kamiltonian/new Hamiltonian using K = H +\frac{\partial G}{\partial t}. My question is: do we have to derive the...
I have a question if you have an Hamiltonian given by
H = \sum_{i,i+1} \sigma_i \cdot \sigma_{i+1}
where i can even or odd bonds so in a 1D lattice so if you have 4 sites(1 2 3 4 1) then (12) and (34) are even bonds and (23) and (41) are odd bonds. and I was checking if
[H_{x...
Homework Statement
Hi,
I want to diagonalize the Hamiltonian:
Homework Equations
H=\phi a^{\dagger}b + \phi^{*} b^{\dagger}a
a and b are fermionic annihilation operators and \phi is some complex number.
The Attempt at a Solution
Should I use bogoliubov tranformations? I...
How to select the good basis for the special Hamiltonian??
For the Hamiltonian H=\frac{P^2}{2\mu} -\frac{Ze^2}{r}+ \frac{\alpha}{r^3} L.S (which we can use L.S=\frac{1}{2} (J^2-L^2-S^2)in the third term) how to realize that the third term,\frac{\alpha}{r^3} L.S, commutes with sum of the...
For an exercise I am given the attached Hamiltonian, but I don't understand it completely. We sum over spin -½ and ½ and the paulimatrices seem to be dependent on this since they are labeled by σσ'. What does this mean? I mean the pauli matrices are just operators for the spin in the...
Homework Statement
The vector \psi =\psi_{n} is a normalized eigenvector for the energy level E=E_{n}=(n+\frac{1}{2})\hbar\omega of the harmonic oscillator with Hamiltonian H=\frac{P^{2}}{2m}+\frac{1}{2}m\omega^{2}X^{2}. Show that...
Homework Statement
I have problem where I need to commutate my hamiltonian H with a fermionic anihillation operator. Had H been written in terms of fermionic operators I would know how to do this, but the problem is that it describes phonon oscillations, i.e. is written in terms of bosonic...