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.
Homework Statement
Show that for a particle in a central potential; V=f(|r|)
H is conserved.
Homework Equations
THe hamiltonian is
H=\sum(piq'i)-L
It is conserved if dH/dt=0
Euler-Lagrange equation
d/dt(dL/dq')=dL/dq
Noether's Theorem
For a continuous transformation, T such...
I understand how to use Hamiltonian mechanics, but I never understood why you construct the Hamilitonian by first constructing the Langrangian, and then performing a Legendre transform on it.
Why can't you just construct the Hamiltonian directly? Does it have to do with the generalized...
Hi. I hope this is in the right spot - I am not a physics major so not sure if it qualifies as classical, quantum, or other type of physics). I am asking the following to check the calculations of my graduate math thesis
I am simulating a one dimensional chain of masses and linear springs...
Homework Statement
The hamiltonian of a simple anti-ferromagnetic dimer is given by
H=JS(1)\bulletS(2)-μB(Sz(1)+Sz(2))
find the eigenvalues and eigenvectors of H.
Homework Equations
The Attempt at a Solution
The professor gave the hint that the eigenstates are of...
Please, help me with this problem!
Two distinguishable particles of spin 1/2 interact with Hamiltonian
H=A*S1,z*S2,x
with A a positive constant. S1,z and S2,x are the operators related to the z-component of the spin of the first particle and to the x-component of the spin of the second...
I often see the EM Hamiltonian written as $$H=\frac1{2m}\left(\vec p-\frac ec\vec A\right)^2+e\phi,$$ but this confuses me because it doesn't seem to have the right units. Shouldn't it just be $$H=\frac1{2m}\left(\vec p-e\vec A\right)^2+e\phi,$$ since the vector potential has units of momentum...
Homework Statement
The Hamiltonian for two particles with angular momentum j_1 and j_2 is given by:
\hat{H} = \epsilon [ \hat{\bf{j}}_1 \times \hat{\bf{j}}_2 ]^2,
where \epsilon is a constant. Show that the Hamiltonian is a Hermitian scalar and find the energy spectrum.Homework Equations...
Hello everyone, this is my first thread. Hope to be helpful here, as well as to find some help! :D
Homework Statement
Given a Hamiltonian H(q,p)(known) and given a transformation of coordinates (q,p)\rightarrow (Q,P):
a) Show that it is a canonic transformation
b) Solve the...
Homework Statement
Let be q(t)=e^{-t}\alpha and p(t)=e^{-t}\beta
Can this be a Hamiltonian Evolution
Homework Equations
The Hamilton equations for \dot{p} and \dot{q}.
The Attempt at a Solution
Can be a Hamiltonian evolution if verifies Hamilton equations...
Homework Statement
Find the eigenvalues of the following
and the eigenvelctor which corresponds to the smallest eigenvalue
Homework Equations
I know how to find the eigenvalues and eigenvectors of a 2x2 matric but this one I'm not so sure so any help would be appreciated
The...
Homework Statement
This problem has to do with a canonical transformation and Hamiltonian formalism. Below is my attempt at solving it, but I am not too sure about it. Please help!
Let \theta be some parameter.
And
X_1=x_1\cos \theta-y_2\sin\theta\\
Y_1=y_1\cos \theta+x_2\sin\theta\\...
Suppose G is a HC (Hamiltonian-connected) graph on n >= 4 vertices. Show that connectivity of G is 3.
I tried starting by saying that there would be at least 4C2=6 unique hamiltonian paths. But then I'm not sure where to go from here.
Any hints would be appreciated.
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?
I'm a little confused about why the Lagrangian is Lorentz invariant and the Hamiltonian is not. I keep reading that the Lagrangian is "obviously" Lorentz invariant because it's a scalar, but isn't the Hamiltonian a scalar also?
I've been thinking this issue must be somewhat more complex...
When I write down the Hamiltonian for the hydrogen atom why do we not include a radiation term or a radiation reaction term? If I had an electron moving in a B field it seems like I would need to have these terms included.
I'm watching a lecture on the Hamiltonian and can't figure out something. Here it is. Take a generic function G, and differentiate it with respect to p and q. What you get is the partial of G with respect to p TIMES the derivative of p (or p-dot), plus the derivative of G with respect to q...
Homework Statement
The JCM has the Hamiltonian:
\hat{H} = \hbar \omega \left(\hat{a}\hat{a}^{*} + 1/2 \right) + \frac{\hbar\omega_{0}\hat{\sigma}_{z}}{2} + \hbar g (\hat{\sigma}_{+}\hat{a} + \hat{\sigma}_{-}\hat{a}^{*}
Find the eigenstates and energy eigenvalues in this non-resonant case...
given the Schroedinger equation with an exponential potential
-D^{2}y(x)+ae^{bx}y(x)-E_{n}y(x)= 0
with the boudnary conditons y(0)=0=y(\infty)
is this solvable ?? what would be the energies and eigenfunction ? thanks.
To cut to the chase, I have to solve for the evolution of a two-state system where the system's state at time t satisfies the equation
\mathrm{i}\hbar\left(
\begin{array}{cc}
\dot{c}_1(t)\\
\dot{c}_2(t)
\end{array}
\right)=\left(
\begin{array}{cc}
0 & \gamma...
Homework Statement
If I have a Hamiltonian matrix, \mathcal{H}, that only depends on a kinetic energy operator, do the energy eigenvalues have to be non-negative? I have an \mathcal{H} like this, and some of its eigenvalues are negative, so I was wondering if they have any physical...
Hi,
I just started self studying solid state and I'm having trouble figuring out what the hamiltonian for a square lattice would be when considering the Heisenberg interaction.
I reformulated the dot product into 1/2( Si+Si+δ+ +Si+δ+S-- ) + SizSi+δz
and use
Siz = S-ai+ai
Si+ =...
Hi,
I was calculating the Edwards-Anderson Hamiltonian of a Hopf link. A hopf link is like attachment 1. I have drawn the Seifert surface of that link. The surface is shown in attachment 2. It also contains the Boltzmann weight. So, this is an Ising model. I am confused as there are more than...
My book writes a 5-step recipe for detemining the hamiltonian, which I have attached. However I see a problem with arriving at the last result. Doesn't it only follow if the matrix M is a symmetric matrix - i.e. the transpose of it is equal to itself.
Homework Statement
Consider a charged particle of charge e traveling in the electromagnetic
potentials
\mathbf{A}(\mathbf{r},t) = -\mathbf{\nabla}\lambda(\mathbf{r},t)\\
\phi(\mathbf{r},t) = \frac{1}{c} \frac{\partial \lambda(\mathbf{r},t)}{\partial t}
where \lambda(\mathbf{r},t) is...
Given the hamiltonian in this form: H=\hbar\omega(b^{+}b+.5)
b\Psi_{n}=\sqrt{n}\Psi_{n-1}
b^{+}\Psi_{n}=\sqrt{n+1}\Psi_{n+1}
Attempt:
H\Psi_{n}=\hbar\omega(b^{+}b+.5)\Psi_{n}
I get to
H\Psi_{n}=\hbar\omega\sqrt{n}(b^{+}\Psi_{n-1}+.5\Psi_{n-1})
But now I'm stuck. Where can I...
As the title suggests, I am interested in symmetries of QM systems.
Assume we have a stationary nonrelativistic quantum mechanical system H\psi = E\psi where we have a unique ground state.
I am interested in the conditions under which the stationary states of the system inherit the...
Title says it all, confused as to how I'm supposed to define the phase space of a system, in my lecture notes I have the phase space as {(q, p) ϵ ℝ2} for a 1 dimensional free particle but then for a harmonic oscillator its defined as {(q, p)}, why is the free particles phase space all squared...
Homework Statement
Find the energy eigenvalue.
Homework Equations
H = (p^2)/2m + 1/2m(w^2)(x^2) + λ(x^2)
Hψ=Eψ
The Attempt at a Solution
So this is what I got so far:
((-h/2m)(∂^2/∂x^2)+(m(w^2)/2 - λ)(x^2))ψ=Eψ
I'm not sure if I should solve this using a differential...
I need to elaborate the equation ,and need to know what is the physical significance and how matrices will manipulate in the equation $$
\hat{H} = (\hat{\tau_3}+i\hat{\tau_2})\frac{\hat{p}^2}{2m_0}+ \hat{\tau_3}m_0 c^2 = \frac{\hat{p}^2}{2m_0}
\left| \begin{array}{ccc}
1 & 1 \\
-1 &...
Given H=p^2/2 - 1/(2q^2)
How to show that there is a constant of motion for this one dimensional system D=pq/2 - Ht ?
I tried doing it in my usual way i.e. p'=-∂H/∂q and q'=∂H/∂p and then finding the constants of motion but that doesn't match with what I have to show.
Please guide me as...
In Rovelli's book, in chapter 7 it talks about the Hamiltonian operator for LQG. In manipulating the form for the Hamiltonian operator Rovelli makes the following expansions
U(A,\gamma_{x,u})=1+\varepsilon u^a A_a(x)+\mathcal{O}(\varepsilon^2)
where by fixing a point x and a tangent...
hi friends. i don't know how can i write a fortran code for expressing spins in Heisenberg model which have 3 dimension spin operator, sx,sy,sz?
thanks for your help
Homework Statement
The total energy may be given by the hamiltonian in terms of the coordinates and linear momenta in Cartesian coordinates (that is, the kinetic energy term is split into the familiar pi2/2m. When transformed to spherical coordinates, however, two terms are angular momentum...
Hi there,
If the evolution operator is given as follows
U(t) = \exp[-i (f(p, t) + g(x))/\hbar]
where p is momentum, t is time. Can I conclude that the Hamiltonian is
H(t) = f(p, t) + g(x)
if no, why?
I'm currently reading Sakurai's 'Modern Quantum Mechanics' (Revised Edition) and at page 76 he introduces a spin half hamiltonian
H = - (\frac{e}{mc}) \vec S \cdot \vec B.
But what is c doing in this hamiltonian? Clasically the energy of a magnetic moment in a magnetic field is
E = -...
Homework Statement
"Show that if the Hamiltonian depends on time and [H(t_1),H(t_2)]=0, the time development operator is given by
U(t)=\mathrm{exp}\left[-\frac{i}{\hbar}\int_0^t H(t')dt'\right]."
Homework Equations
i\hbar\frac{d}{dt}U=HU
U(dt)=I-\frac{i}{\hbar}H(t)dt
The Attempt at a...
Theorem: Prove that there exist $n$ edge disjoint Hamiltonian cycles in the complete graph $K_{2n+1}$.
----------------------------------------------------------------------------------
I have found two constructive proofs of this over the internet. But I would like to prove it...
Hi, I have a question about two different expressions of Jaynes-Cummings Hamiltonian
H=\Delta_c a^{\dagger}a+\Delta_a \sigma_{+} \sigma_{-} +
g (a^{\dagger}\sigma_{-} +a\sigma_{+} )
and
H=\Delta_c a^{\dagger}a+\Delta_a \sigma_{+} \sigma_{-} +i
g (a^{\dagger}\sigma_{-} -a\sigma_{+}...
Hi
I have a question regarding the pump-term in the Hamiltonian on page 9 (equation 2.9b) of this thesis: http://mediatum2.ub.tum.de/download/652711/652711.pdf. This term is not very intuitive to me. a is followed by a CCW phase, whereas a^\dagger is followed by a CW phase. How does this...
I don't understand this idea. For example we have cubic crystal which has a lot of unit cells. We define spin variable of center of cell like S_c. And spin variable of nearest neighbour cells with S_{c+r}. So the cell hamiltonian is...
I have a Hamiltonian, consisting only of angular momentum components Lx,Ly,Lz. I need to go from it to some coordinate representation. But I don't have derivatives Lx' etc. in H. So, when I'll go to coordinates and momenta I'll have Hamiltonian equations like p_i=0, which doesn't have sense...
How can you tell if the Klein-Gordan Hamiltonian, H=\int d^3 x \frac{1}{2}(\partial_t \phi \partial_t \phi+\nabla^2\phi+m^2\phi^2) is time-independent? Don't you have to plug in the expression for the field to show this? But isn't the only way you know how the field evolves with time is...
I'm currently using David J. Griffiths 'Introduction to Quantum Mechanics' to teach myself quantum mechanics and I had a quick question about the way he factors the Hamiltonian into the raising and lowering operators for the potential V(x)=(1/2)kx²
On page 42 he writes the Hamiltonian as...
In this paper called "Stepping out of Homogeneity in Loop quantum Cosmology" - http://arxiv.org/pdf/0805.4585.pdf. On page 4 they say "where the sum is over the couples of distinct faces at each tetrahedron, U_{ff'} = U_f U_{f_1} U_{f_2} \dots U^{-1}_{f'} where l_{ff'} = \{ f , f_1; f_2; \dots...
Hi there. I need help to work this out.
A particle with mass m is studied over a rotating reference frame, which rotates along the OZ axis with angular velocity \dot\phi=\omega, directed along OZ. It is possible to prove that the potential (due to inertial forces) can be written as:
V=\omega...
Homework Statement
A particle moves in a one dimensional potential : V(x) = 1/2(mω2x
Show that the function ψ(x) = a0exp(-βx2) is an eigenfunction for the Hamiltonian for a suitable value of β and calculate the value of energy E1
Homework Equations
The Attempt at a Solution...
Not sure I am posting this in the right subforum, if this is not the case, please feel free to move it.
Anyway, the title about sums it up - I need to find a good source which offers a thourough treatment of Hamiltonian formalism for the explicitly time-dependent case - could someone possibly...
Homework Statement
The problem is from Ashcroft&Mermin, Ch32, #2(a). (This is for self-study, not coursework.)
The mean energy of a two-electron system with Hamiltonian
\mathcal{H} = -\frac{\hbar^2}{2m}(∇_1^2 + ∇_2^2) + V(r_1, r_2)
in the state ψ can be written (after an integration by...