Welcome back to PHYS 3305

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Welcome back to PHYS 3305 Otto Stern 1888-1969 Walther Gerlach 1889-1979 Today s Lecture: Angular Momentum Quantization Stern-Gerlach Experiment

AnNouncements Reading Assignment for Nov 14th: Harris 8.2-8.5. Problem set 13 is due Tuesday, Nov 21st at 12:30 pm. Regrade for problem set 12 is due Tuesday, Nov 21st at 12:30 pm. Problem sets 14 and 15 will have no regrade attempts. Final presentations are due MONDAY, NOVEMBER 203th at 3 pm. Email your pdf to cooley@physics.smu.edu before due date and time. If your talk is late less than one hour, your maximum grade will drop one increment (i.e. A > A- ). If your talk is late 1-2 hours, your maximum grade drops two increments (A > B+) and so on.

Review Question What are the quantum numbers n and l for a hydrogen atom with E = 13.6 9 ev L = 2 h Answer: n = 3, l = 1, m l = 0, ±1 E n = 13.6 n 2 (` =0, 1, 2,...(n 1)) L = l(l +1) h L z = m l h (m l =0, ±1, ±2,...± l)

Demo: Gyroscope ω Initially L is directed to the left (positive x-direction. The weight of the wheel produces a torque about the origin. τ = r F = r m g τ = mgr (positive y-direction) Torque is related to angular momentum: τ = d L Change is in direction only > L rotates around z-axis dt

The figure shows a spinning ball of negative charge. Does the magnetic moment of this spinning charge point up, point down, to the right, or to the left? From Lecture Video: Ans: Points Down The magnetic moment for an electron orbiting CCW is given by µ L = e 2m e L

A bar magnet is moving to the right though a nonuniform magnetic field. The field is weaker toward the bottom of the page and stronger toward the top. a) Is there a force on the magnet? If so, in which direction? S N Ans: Yes, the magnet will feel a downward force. The South pole of the bar magnet will feel a downward force. This force is greater than the upward force felt by the North pole of the bar magnet.

A bar magnet is moving to the right though a nonuniform magnetic field. The field is weaker toward the bottom of the page and stronger toward the top. N b) Will the magnet be deflected by the field? If so, in which direction? S Ans: Yes, the bar magnet will be deflected downward because the downward force will be greater than the upward force.

A bar magnet is moving to the right though a nonuniform magnetic field. The field is weaker toward the bottom of the page and stronger toward the top. N c) Would the magnet be deflected by a UNIFORM magnetic field? If so, in which direction? Ans: No, the net force would be 0. S

From Lecture Video: A dipole in a magnetic field also feels a torque: ~ = ~µ L ~ B What direction is the torque? Counterclockwise We also know that torque is related to angular frequency by the rotational second law: ~ = d~ L dt = e 2m e ~ L ~ B d dt = eb 2m e Larmor frequency

From Lecture Video: The magnetic quantum number, m l, is an important factor for governing the effect of the magnetic field. Question: Consider hydrogen in the ground state. What force do we expect and why? Answer: F = 0. For the ground state, l = 0, thus, ml would equal zero.

From Lecture Video: Stern Gerlach: - Take hydrogen atoms in the l = 0 state and pass them through the magnetic field. - Expect to see 1 line on the screen corresponding to the only possible m l state (m l = 0) (no magnetic moment). What was seen -- 2 lines! - Take hydrogen atoms in the l = 1 state and pass them through the magnetic field. - Expect to see 3 lines on the screen corresponding to the 3 possible m l states. What was seen -- Only 2 lines!

From Lecture Video: Intrinsic Angular Momentum is given the name SPIN, ( S) ~. S = p s(s + 1)~ (length of spin vector) Remember: an intrinsic property is one that is fundamental to the particles nature. The magnitude of a particle s spin vector depends on a dimensionless value s. s is not a quantum number and can not take on different values!

From Lecture Video: Similar to orbital angular momentum, the z-component of intrinsic angular momentum is quantized. S z = m s ~ m s = s, ( s + 1),...(s 1),s Spin is a new Quantum Number bringing the total number to 4. The spin quantum number is given by m s. (n, l, m l,m s )

Can the spin angular momentum vector lie in the xy-plane? Justify your answer. Answer: No, m s = +1/2 or -1/2. Thus, the z-component of the intrinsic angular momentum, S z, cannot be zero.

The subatomic particle Ω has spin s = 3/2. What angles might its intrinsic angular momentum vector make with the x-axis? We know S = p s(s + 1)~ = r 3 2 (3 2 + 1)~ = p 15 2 ~ The S z components are ± 3 2 ~, ±1 2 ~ Thus, = cos 1 ( S z S ) = 140.8 o, 105 o, 75 o, 39.2 o

Example: Stern-Gerlach In a Stern-Gerlach type of experiment, the magnetic field varies with distance in the z direction according to db z /dz = 1.4 T/mm. Silver atoms travel a distance x = 3.5 cm through the magnet. The most probable speed of the atoms emerging from the oven is v=750 m/s. Find the separation of the two beams as they leave the magnet. The mass of a silver atom is 1.8 x 10-25 kg, and its magnetic moment is about 1 Bohr magneton. Hint: Use a combination of what we just learned about Forces and B-fields and what we know of kinematics to solve this problem.

Step 1: Find the force felt by the atom. The magnetic field is acting only in the z-direction. So, we can use the expression we just derived to relate the magnetic moment and the magnetic field to the force. Step 2: Relate force to the acceleration of the atom. The acceleration of a silver atom of mass m as it passes through the magnet is

Step 3: The vertical deflection of the beam can be found from kinematics. z = 1 2 at2 The time, t, to transverse the magnet is given by t = x v z = 1 2 a(x v )2 The spread in the beam is two times the distance Δz. d =0.16mm

A particle s intrinsic magnetic dipole moment is related to its intrinsic angular momentum. ~µ s = g q 2m ~ S q = charge m = mass g = gyromagnetic ratio NOTE: μ s is related to the intrinsic angular momentum, S μ L is related to the orbital angular momentum, L Values of g depend upon the particle. For an electron the value is close to 2. For a proton it is 5.6. The predominant effect in the Stern-Gerlach experiment is due to the hydrogen atom s electron. Why? Although the gryromagnetic ratio is greater for the proton than for the electron, the mass of the proton is much, much larger than the mass of the electron. Thus, it s magnetic moment is quite small compared to that of the electron.

From Lecture Video: Revisit Wave Functions Now that we have a 4th quantum number, we need to adjust our wave functions. n,`,m`,m s = n,`,m`m s spacial state spin state For an electron (spin 1/2), m s can take on only two values:

By including electron spin, what is the degeneracy of the n = 2 energy level of hydrogen? Answer: 8 Each n, l and ml value has 2 possible spin states. Without m s, the degeneracy was given by (2l+1) at each level. Thus, our new degeneracy would be 2(2l+1) at each level. l=0: 2(0+1) = 2 l=1: 2(2+1) = 6 degeneracy = 8

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