QUANTUM MECHANICS Problem 4 Consider a one-dimensional charged harmonic oscillator. Let the coordinate be, charge be...
A particle of charge q and mass m is bound in the ground state of a one-dimensional harmonic oscillator potential with frequency oo. At time t-0 a weak spatially uniform electric field (E) is turned on, so that the perturbation to the Hamiltonian can be described as R'(t) =-q Exe-t/t for t> 0. Using first order, time-dependent perturbation theory, calculate the following probabilities: (a) the particle is detected in the first excited state after a very long time (t »...
please solve with explanations 3. (20 pts) A particle of mass m and charge q is in a one dimensional harmonic oscillator potential ()1ma'. A time dependent uniform electric field E, ()E, os eris 2 applied in the x direction. The particle is in the harmonic oscillator ground state at time a) What is the time dependent perturbation Hamiltonian H'(t) - the potential enegy of the charge in this electric field? b) Find the amplitude ci(t) of finding the particle...
Quantum mechanics Consider a two-dimensional harmonic oscillator . If find the energy of the base state until second order in theory of disturbances and the energies of the first level excited to first order in . We were unable to transcribe this imageWe were unable to transcribe this imageWe were unable to transcribe this image
1. Consider a spin-0 particle of mass m and charge q moving in a symmetric three-dimensional harmonic oscillator potential with natural frequency W.Att-0 an external magnetic field is turned on which is uniform in space but oscillates with temporal frequency W as follows. E(t)-Bo sin(at) At time t>0, the perturbation is turned off. Assuming that the system starts off at t-0 in the ground state, apply time-dependent perturbation theory to estimate the probability that the system ends up in an...
Quantum mechanics. Consider a quadratic oscillator with time dependent frequency (1). Find the rules of selection for transitions between eigenstates of (2). If at t=0 the system is in the ground state of H_0, calculate the probabilities of transition to the different excited states. ) 2 mwL1+esin (Bt] x H(e)= + 2m H. HCe=0) . 2) ) 2 mwL1+esin (Bt] x H(e)= + 2m H. HCe=0) . 2)
3. (a) Consider a 1-dim harmonic oscillator in its ground state (0) of the unperturbed Hamiltonian at t--0o. Let a perturbation Hi(t)--eEXe t2 (e, E and rare constants) be applied between - and too. What is the probability that the oscillator will be in the state n) (of the unperturbed oscillator) as t-> oo?(15%) (b) The bottom of an infinite well is changed to have the shape V(x)-ε sin® for 0Sxa. Calculate the energy shifts for all the excited states...
19. Suppose that an electron in a one-dimensional harmonic-oscillator potential muo2 is subjected to an oscillating electric field o) cos wt in the x direction (a) If the electron is initially in the ground state, what is the proba- bility that the electron will be in the nth excited state at time t? (b) I , perturbation theory will fail at some time t. What is the critical time?
Suppose a particle is in a one-dimensional harmonic oscillator potential. Suppose that a perturbation is added at time t = 0 of the form . Assume that at time t = 0 the particle is in the ground state. Use first order perturbation theory to find the probability that at some time t1 > 0 the particle is in the first excited state of the harmonic oscillator. H' = ext.
Quantum Mechanics. Consider a one-dimensional harmonic oscillator of frequency found in the ground state. At a perturbation is activated. Obtain an expression for the expected value of as a function of time using time-dependent perturbation theory. A step by step process is deeply appreciated. The best handwriting possible, please. Thank you very much. We were unable to transcribe this imageWe were unable to transcribe this imageV (t) = Fox cos (at) We were unable to transcribe this image V (t)...
Intro to Quantum Mechanics problem: . In a harmonic oscillator a normalized "coherent" state ya(x) is defined in terms of the lowering operator a. by aXa(x) = a Xa(x) for some (complex) number a. /Coherent states have many applications in atomic, molecular, and optical physics, for instance lasers and Bose-Einstein condensates]. (a) Using the properties for any wavefunctions f(x) and g(x) that 00 00 if ag dx (a.f)g dx f a+g dx (a.)'g dx -00 -00 -00 calculate <x >...