课程名称︰量子力学一 课程性质︰选修 课程教师︰蒋正伟 开课学院：理学院 开课系所︰物理学系 考试日期（年月日）︰108年10月23日 考试时限（分钟）：unknown 是否需发放奖励金：是 （如未明确表示，则不予发放） 试题 : 注：为方便表示数学符号，部分符号以LaTeX码输入。 如：a^{b}_{c}表a上标b下标c；\vec{v}表v向量；\hat{x}表x单位向量；\cdot表向量内积 10/23/2019 PHYS7014 Quantum Mechanics I Midterm Exam Instructions This is an open-book, 120-minute exam. Your are only allowed to use the main textbook (by Sakurai and Napolitano) and your own handwritten notes. Only deri- vedresults in the main text of Sakurai and Napolitano up to the range of the exam (i.e., Chapter 1) can be used. The score of each sub-problem is indicated by the number in square brackets. To avoid any misunderstanding, ask if you have any questions about the problems or notations. In your answers, define clearly your notations if they differ from those in the main textbook. Problems Consider a spin-1/2 particle placed in a uniform magnetic field, \vec{B}=\frac{B_0}{\sqrt{2}}(\hat{x}+\hat{z}), where B_0 >0. The dynamics of the particles are governed by the Hamiltonian H=-γ\vec{S}\cdot\vec{B}, where \vec{S} is the vector spin operator for the particle, and γ is a positi- ve constant. 1.[15]In the original Stern-Gerlach experiment, a beam of silver atoms (each carries 47 electrons) goes through a magnetic field \vec{B}=B_0\hat{z}, where B_0 has a spatial dependence, and split into two. (a)Explain why B_0 cannot be a constant. (b)Explain why they can be seen as a spin-1/2 particles. (c)Explain why the nuclear spin can be safely ignored in this case. 2.[5]Calculate the matrixof the Hamiltonian in the {|+>,|->} basis with S_Z|±>=±\hbar/2|±>. 3.[10]Calculate the eigenvalues and the normalized eigenvectors of H. For the normalized eigenvectors, write them in the form of N(1 ), where N and α α are numbers. 4.[5]What is the matrix that diagonalizes H, with the elements of the diagon- alized H listed in the ascending order? 5.[10]At time t=0, the system is in the state |->, and the energy is measured. What are the possible outcomes of the energy measurement and with what prob- abilities? 6.[5]In the previous problem, what is the expectation value of the energy mea- surement? 7.[10]Evaluate Δs_xΔs_z for the lower energy eigenstate, where Δs_x and Δs_z denote the uncertainties of S_x and S_z operators, respectively. 8.[5]Explain whether your result in the previous problem violates the uncerta- inty relation. 9.[10]Suppose the spin-1/2 particle is initially in the spin-up state along the z axis, and has a fixed momentum \vec{p}. Define a ket vector to descri- be such a state. Derive the final ket vector after one performs a finite tr- anslation of Δ\vec{x} to the particle. Explain what happens to the spin st- ate. 10.[10]Suppose \hat{n} is a unit vector in the (θ,φ) direction, as shown in Fig.1(a). Find the normalized |ψ> such that (\vec{S}\cdot\hat{n})|ψ>=+\hbar/2|ψ>. (4) Express your result in the {|+>,|->} basis. Take the convention that the coefficient of |+> is real. 11.[10]any spin-1/2 state can be visualized in the three dimensional space, called the Bloch sphere as shown in Fig. 1(b), as a Bloch vector, (<σ_x>, <σ_y>,<σ_z>), evaluated with respect to the given state. Compute the Bloch vector for |ψ> in the previous problem, and show that it falls on the surface of the Bloch sphere. (The last property is a characteristic of pure states.) 12.[5]In the textbook, the spin raising and lower operators of the spin-1/2 particle are introduced respectively as S_+ ≡\hbar|+><-|, S_- ≡\hbar|-><+|. (5) Suppose we know that S_±=S_x±iS_y even for higher spin systems. Explain whether one can assume for a spin-s particle that the raising and lowering operators are S_+ =N\hbar[|s,s><s,s-1|+|s,s-1><s,s-2|+...+|s,-s+1><s,-s|], (6) S_- =N\hbar[|s,s-1><s,s|+|s,s-2><s,s-1|+...+|s,-s><s,-s+1|], where |s,m> denotes a spin-s state with s_z =m, and N is some overall fact- or. --

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