A state is described in terms of vectors A),2) and |9,) with state: |w) = 6,)+l.)- ) of operator ở where G |6.) = (n +1)|6.) a) Find the normalization of the state W) b) Find the expectation value of G c) Find the expectation value of G?
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- The general state |w) is given in terms of three orthonormal vectors lo1), lo2), and o3) as follows: =162)+ where lon) are eigenstates to an operator B such that: Blon) = (2n – 1)iøn) with n = 1, 2, 3. (a) Find the norm of the state lw). (b) Find the expectation value of B for the state |w). (c) Find the expectation value of B? for the state w).5The Hamiltonian for the one dimensional quantum oscillator is 1 p² 1 Ĥ = 1² + ½ k²² = 12 + √ mw² ಠ2m 2m 2 where k = mw². 1) Define the operators ₁₁ and ₁₁ such that Ĥ = ½ħw (p² + ²). Define Ĥ2 as a function of 1 and p₁ such that Ĥ = hwĤ₂. - 2) Let us define the new operators â (1 + i₁) and ↠= ½(î₁ — ip₁). Express ₁ and p₁ as a function of â and â³. Knowing that [^^1,î₁] = i and [1, 1] = -i, calculate âât and â†â. Express Ĥ2 as a function of a and at. 3) Let us define Ñ such that Ĥ₂ = Ñ + ½. Knowing that Ĥ, Ĥ₂ and Ñ have the same eigenstates, what are their corresponding eigenvalues?
- V = {0, (0 < x s a, 0sysa) {00, other values of x and y %3D Answer for the particle with mass m under the effect of the potential defined as: a) Find the energy eigenvalues and eigenfunctions of the particle using the Schrödinger Wave Equation. Most Determine the energies of the first three low-energy states. Discuss whether these situations are degenerate. b) Too small to system H' = 8xy %3D By applying Perturbation Theory in perturbation (where 8 is a small number) and 2nd order energy for the ground state considering only the first three states with the lowest energy case of calculate the correction term.H. Mc | 4 — 14₁7 — 19₂ > > 1917 of orthonormal eigen state Q Consider astate >= which as given interm 3 14 > 10 > 1437 of an operator B such that 19 B² | o₂ >= n² | On> find the expectation value of B² beNone
- A qubit is in state |) = o|0) +₁|1) at time t = 0. It then evolves according to the Schrödinger equation with the Hamiltonian Ĥ defined by its action on the basis vectors: Ĥ0) = 0|0) and Ĥ|1) = E|1), where E is a constant with units of energy. a) Solve for the state of the qubit at time t. b) Find the probability to observe the qubit in state 0 at time t. Explain the result by referring to the way that the time-evolution transforms the Bloch sphere.Consider a particle of mass μ bound in an infinite square potential energy well in three dimensions: U(x, y, z) = {+00 0 < x4. A particle is in the state 2 1 Y (0,0)+ V5 Y, '(0,ø) – Y (0,¢), V5 which is a superposition of the normalized eigenstates, Y;" (0,¢), of the L² operator. Calculate the value of the total angular momentum of the particle in this state. Also, calculate the expectation value of the operator L+L_ in this state.