A particle moves in an infinite potential well described by The eigenfunctions are of the form...
A particle moves in an infnite potential well described by V(r) o, l> a/2. are of the forn vn (z)-A" cos (k,,e), or Un(r) B," sin (knz), depending on the value of n. For n 3, (r)-(V2/a) cos (3Tr/a) for lrl S a/2 and var t are the expectation values of r and a2 in the n 3 state. ) What are the expectation values of p and p2 in the n-3 state. To calculate the expectation value for momentum,...
Quantum Mechanics question about an infinite square well. A particle in an infinite square well potential has an initial state vector 14() = E1) - %|E2) where E) is the n'th eigenfunctions of the Hamiltonian operator. (a) Find the time evolution of the state vector. (b) Find the expectation value of the position as a function of time.
A particle of mass m is subject to a doubly infinite square well, with widths L, located at (a/2, a/2). The eigenstate wave functions for this are v(x, y) = L, = a and centre %3D %3D sin () sin ("). nyTy a) Find an expression for the position operator in bra-ket notation. b) Find an expression for the momentum operator in bra-ket notation. c) The particle is initially in the state |) : for position and momentum to find...
3. For a particle moving in an infinite, one-dimensional, symmetric square well of width 2a, show that the (normalized) wave functions are of the form ?-kx).va. cos?x): "-1. 3.5 ,.. COS ? -?? r")(x)=?sin n-r | ; n-2, 4, 6 Express the state ?(x)=N sin,(rx/a) as a linear superposition eigenstates, and find its normalization constant N. of the above HINT sin39-3sin ?-4sin'?
4) A particle in an infinite square well 0 for 0
A particle on a sphere is described by the state function Ψ = N {1 + cos(θ)} Find a) the value of the normalization constant N b) the expectation value of the energy E c) the possible values of the z component of angular momentum (Lz) that might be measured, and which of these possibilities is most likely.
3 At a given time, the normalised wave function for a particle in a one-dimensional infinite square well -a < x < a is given by 2 sin2 V inside the well and zero outside. Find the probability that a measurement of energy yields the eigenvalue En. (Hint: use data on page 6.) [6] Useful Data and Formulas = 1.60 x 10-19 C Elementary charge e h/2T=1.05 x 10-34 Js Planck's constant 3.00 x 108 m s-1 Speed of light...
Consider a particle of mass in a 10 finite potential well of height V. the domain – a < x < a. a) Show that solutions for – a < x < a take the form on (x) = A cos(knx) for odd n, and on (x) = A sin(knx) for even n. . Show a) Match the boundary conditions at x = a to prove that cos(ka) = Bk where k is the wave vector for -a < x...
2. A particle of mass m in the infinite square well of width a at time 1 - 0 has wave function that is an equal weight mixture of the two lowest n= 1,2 energy stationary states: (x,0) - C[4,(x)+42(x)] (a) Normalize the wave function. Hints: 1. Exploit the orthonormality of W, 2. Recall that if a wave function is normalized at t = 0, it stays normalized. (b) Find '(x, t) and (x,1)1at a later time 1>0. Express Y*...
A particle with mass m is in a one-dimensional simple harmonic oscillator potential. At time t = 0 it is described by the state where lo and l) are normalised energy eigenfunctions corresponding to energies E and Ey and b and c are real constants. (a) Find b and c so that (x) is as large as possible. b) Write down the wavefunction of this particle at a time t later c)Caleulate (x) for the particle at time t (d)...