Recent content by thecourtholio

  1. thecourtholio

    Hamiltonian conjugate dynamic variables

    I was just using the indecies as good practice so i remember to use all indecies of Q or P later if they need it. But for [Q,P] I find $$[Q,P] = \bigg[\frac{\partial Q}{\partial x}\frac{\partial P}{\partial p_x} - \frac{\partial Q}{\partial p_x}\frac{\partial P}{\partial x}\bigg] + \bigg[...
  2. thecourtholio

    Hamiltonian conjugate dynamic variables

    Homework Statement Consider a charge ##q##, with mass ##m##, moving in the ##x-y## plane under the influence of a uniform magnetic field ##\vec{B}=B\hat{z}##. Show that the Hamiltonian $$ H = \frac{(\vec{p}-q\vec{A})^2}{2m}$$ with $$\vec{A} = \frac{1}{2}(\vec{B}\times\vec{r})$$ reduces to $$...
  3. thecourtholio

    Using generating function to normalize wave function

    Ok I think I understand it all now. Thank you so much for y'all's help!
  4. thecourtholio

    Using generating function to normalize wave function

    Ok I got $$ \int e^{2\xi y-y^2}e^{2\xi z-z^2}e^{-\xi^2}d\xi = \sqrt{\pi}e^{2yz} = \sqrt{\pi} \sum \frac{y^lz^l}{l!} $$ Is this the correct series? Cause in comparison to $$ \int \frac{y^m}{m!}H_m \frac{z^n}{n!}H_n e^{-\xi^2} d\xi $$ the series and gaussian would cancel for m=n=l leaving just...
  5. thecourtholio

    Using generating function to normalize wave function

    Ok I think I see what you are saying. So I evaluate ## \int e^{2\xi y-y^2}e^{2\xi z-z^2} e^{-\xi^2} d\xi ## and compare it to ##\int \bigg[\sum \frac{y^m}{m!}H_m\bigg]\bigg[\sum \frac{z^n}{n!}H_n\bigg] e^{-\xi^2}d\xi ## something like that?
  6. thecourtholio

    Using generating function to normalize wave function

    Oh yeah I see. I should've noticed that after seeing everyones comments about mod squared. Yeah I was questioning that as I was typing it since ##e^{2\xi-z^2} = \sum \frac{z^n}{n!}H_n## and not just ##H_n## but I wasn't sure if it was possible to rearrange the summation. So combining your...
  7. thecourtholio

    Using generating function to normalize wave function

    Oh thank you I hadn't caught that mistake! So it should be ##\int_{-\infty}^{\infty} A^2 e^{4\xi z-z^2}e^{-\xi^2}d\xi## ? And should it be an integral of ##d\xi## or ##dx##? But I'm still not sure how ## e^{4\xi z-2z^2} = \sum \frac{z^{2n}}{(n!)^2}H_n^2## gives me cross terms that vanish? What...
  8. thecourtholio

    Using generating function to normalize wave function

    Homework Statement Prove that ##\psi_n## in Eq. 2.85 is properly normalized by substituting generating functions in place of the Hermite polynomials that appear in the normalization integral, then equating the resulting Taylor series that you obtain on the two sides of your equation. As a...
  9. thecourtholio

    Energy for Linear 1D Systems - 1D potential

    Oh okay. So if the particle's energy is lower than the maximums of ##U(x)## it will oscillate indefinitely but if its energy is greater than that potential maximum then it can escape right? In this case that means that if ##E<U(\pm\sqrt{\frac{a}{b}})## it will oscillate but if...
  10. thecourtholio

    Energy for Linear 1D Systems - 1D potential

    What would quantify "how deep" the valley is? And that was another thing that was confusing me was the constant energy. I've seen a lot of the plots of ##U(x)## vs. ##x## in the literature include a horizontal line indicating the total energy but none of them really explained why they chose...
  11. thecourtholio

    Energy for Linear 1D Systems - 1D potential

    Homework Statement A particle of mass m moves along the x–axis under the influence of force ##F_x=-ax+bx^3## , where a and b are known positive constants. (a) Find, and sketch, the particle's potential energy, taking U(0) = 0 (b) Identify and classify all equilibrium points (c) Find the...
  12. thecourtholio

    Interaction Energy For Two Point Charges

    Omg I think I got it. So ##\vec{r}## would be the vector describing the distance from the point charge to the reference point right? So then at some reference point P, the vector from ##q_1## would be ##\vec{r}=x\hat{x}+y\hat{y}+z\hat{z}## and from ##q_2## it would be...
  13. thecourtholio

    Interaction Energy For Two Point Charges

    Well my thinking was that if ##q_1## is at the origin then ##\vec{r_1}=(0,0,0)## and if ##q_2## is on the z axis then ##\vec{r_2}=(0,0,a)##. So then ##\vec{r_1}\cdot\vec{r_2}=r_{x1}r_{x2}+r_{y1}r_{y2}+r_{z1}r_{z2}=(0)(0)+(0)(0)+(0)(a)=0## right?
  14. thecourtholio

    Interaction Energy For Two Point Charges

    Homework Statement Find the interaction energy ( ##\epsilon_0 \int \vec{E_1}\cdot\vec{E_2}d\tau##) for two point charges, ##q_1## and ##q_2##, a distance ##a## apart. [Hint: put ##q_1## at the origin and ##q_2## on the z axis; use spherical coordinates, and do the ##r## integral first.]Homework...
  15. thecourtholio

    Angular diameter distance to surface of last scattering

    Homework Statement 1) Calculate the angular diameter distance to the last scattering surface in the following cosmological models: i) Open universe, ΩΛ= 0.65, Ωm = 0.30 ii) Closed universe, ΩΛ = 0.75, Ωm = 0.30 ii) Flat universe, ΩΛ = 0.75, Ωm = 0.25 Describe how the CMB power spectrum...
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