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classes:2009:fall:phys4101.001:q_a_1120 [2009/11/20 18:39] kuehlerclasses:2009:fall:phys4101.001:q_a_1120 [2009/12/19 17:15] (current) x500_sohnx020
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 ====Daniel Faraday 11/20 1030am==== ====Daniel Faraday 11/20 1030am====
 I am still confused about all the different, equivalent(?) terminology we used on Wednesday to describe spin eigenfunctions. Can someone explain what they mean and/or how it is that they are equivalent to each other? I am still confused about all the different, equivalent(?) terminology we used on Wednesday to describe spin eigenfunctions. Can someone explain what they mean and/or how it is that they are equivalent to each other?
 +
 +===Devlin===
 +I'm confused by this as well.
  
 ===David Hilbert's Hat 11/20 11am=== ===David Hilbert's Hat 11/20 11am===
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 I was also confused about this as well. Thanks for the input. Now maybe I'll be able to do problem 18 in the homework. I was also confused about this as well. Thanks for the input. Now maybe I'll be able to do problem 18 in the homework.
  
 +====Jake22 11/22 8:10pm====
 +We have seen examples of the nature of coupling between spin and electromagnetic interactions (Stern-Gerlach). For example we know that any charged particle with spin also has a magnetic moment. What can we say about the nature of coupling between spin and strong or weak interactions?
 +
 +====Blackbox 11/23 11am ====
 +Can you explain the meaning of (1) and (2) of <math> S = S^{(1)}+S^{(2)} </math> on page 184.
 +
 +===Jake22 11/23 3:50pm ===
 +They are referring to particles 1 and 2, respectively.
 +
 +====ice IX 11/23 18:44====
 +On page 182 Griffiths discusses the Stern-Gerlach experiment, and uses the specific case of the silver atom to show that the net spin is s=1/2. This net spin comes from the unpaired valence electron. What happens when the valence contains a pair (or pairs) of electrons, but no unpaired electrons? Will there be no beam splitting in such a situation?
 +
 +====Jake22 11/30 18:34====
 +In the Stern-Gerlach experiment, why must we have a beam of relatively heavy atoms in order to construct localized wave packets and treat the motion in terms of classical particle trajectories? How heavy must they be?
  
 +=== Blackbox 19:10 ===
 +The experiment can be used to demonstrate that electrons and atoms have intrinsically quantum properties, and how measurement in quantum mechanics affects the system being measured. I think that the purpose of relatively heavy atoms are to prevent the gross deflection of the orbit of a charged particle in a magnetic field and bring out the spin-dependent effect. 
  
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classes/2009/fall/phys4101.001/q_a_1120.1258763975.txt.gz · Last modified: 2009/11/20 18:39 by kuehler