Recent content by Morto

  1. M

    Ground state of Hamiltonian describing fermions

    Ahah. Thank you for your help. What about for the Hamiltonian H = \sum_k \left(\epsilon_k - \mu\right) c^{\dag}_k c_k + \gamma \sum_{kp} c_k^{\dag}c_p Can I use the same method to determine the ground state? What does this Hamiltonian represent?
  2. M

    Ground state of Hamiltonian describing fermions

    Nope, I was just given that Hamiltonian and told to find the ground state, the energy of the ground state E_0 and the derivate wrt \mu, so if E_0 = \epsilon_k - \mu then \frac{\partial E_0}{\partial \mu} = -1. (and if E_0 = 0, then obviously the derivate is zero). Is this a 'famous' result?
  3. M

    Ground state of Hamiltonian describing fermions

    Ah, yes, of course. H_k = \epsilon_k\left(\begin{array}{cc}1&0\\0&0\end{array}\right)-\mu\left(\begin{array}{cc}1&0\\0&0\end{array}\right) = \left(\begin{array}{cc}\epsilon_k - \mu&0\\0&0\end{array}\right) So calculating the eigenvalues det\left(\begin{array}{cc}\epsilon_k -...
  4. M

    Ground state of Hamiltonian describing fermions

    Okay, so the matrix representation of these operators is c^{\dag}c = \left(\begin{array}{cc}0 & 1 \\ 0 & 0\end{array}\right)\left(\begin{array}{cc}0 & 0 \\ 1 & 0\end{array}\right) = \left(\begin{array}{cc}1 & 0 \\ 0 & 0\end{array}\right) And the Hamiltonian of the kth term will be H_k =...
  5. M

    Ground state of Hamiltonian describing fermions

    Homework Statement I have been given the Hamiltonian H = \sum_{k} (\epsilon_k - \mu) c^{\dag} c_k where c_k and c^{\dag}_k are fermion annihilation and creation operators respectively. I need to calculate the ground state, the energy of the ground state E_0 and the derivative...
  6. M

    Magnetic Field of Magnetic Dipole Moment

    I'm seeking some clarification on a topic found in Jackson 'Classical Electrodynamics' Chapter 5. This deals with the magnetic field of a localised current distribution, where the magnetic vector potential is given by \vec{A}(\vec{x}) = \frac{\mu_0}{4\pi}...
  7. M

    Conformal Transformation for Perpendicular Charged Sheets

    Can I consider the line of charge as a sum over an infinite number of point charges?
  8. M

    Conformal Transformation for Perpendicular Charged Sheets

    How? That works with the symmetry of parallell plates, but there is no such symmetry here.
  9. M

    Conformal Transformation for Perpendicular Charged Sheets

    So, I've solved many problems involving parallel sheets of conductors (finite, semi-infinite, and infinite) and also finite sheets at a given angle to each other. I can post the results to these if it may be useful, but I'm more interested in sheets that are perpendicular. Consider a...
  10. M

    Complex analysis of electrostatic problem

    I'm not sure whether to post this in the Mathematics or Physics forums, but I figure this problem is easily reduced to its transformation irrespective of the physics it describes. Consider a semi-infinite sheet of (infinitely thin) conductor charged to a potential V. It is placed at a distance...
  11. M

    How to Integrate x^2 e^(-|x|/b) from -Infinity to Infinity?

    Hello! I need to calculate \int_{-\infty}^{\infty} x^{2} e^{-\frac{|x|}{b} dx and I know the answer should involve \pi. I've tried splitting the integral for x and -x with limits from 0 to infty and -infinty to 0, which gives me the answer of 2b. But I don't think this is correct. Does...
  12. M

    How do I solve the integral of exp(-x^2) between -a and a?

    Hello! Sorry to hash up this very old thread, but I need help with this exact problem and I don't understand the solution given. I'm trying to find the integral of x2exp(-x2 / a2) from -infinity to infinity. I've done what's recommended here, but I end up with a double integral of 1/4...
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