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start [2016/03/24 11:33] – janetstart [2016/03/24 11:37] – janet
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 ^Week 5^^Topic^Reading^Summary^Assignments| ^Week 5^^Topic^Reading^Summary^Assignments|
 |[[13]]|M 4/25|Superconductivity|Ibach chapter|{{::day12_2013.pdf|}}: The experimental observations. Note about Type I vs. Type II. Composite bosons. Ionic lattice can be deformed: trail of deformation. Size scale for attractive interaction. The Cooper pair wavefunction. The Cooper pair binding energy at T = 0.  The number density of Cooper pairs. Temperature dependence of Cooper pair binding energy.  |[[hw5|HW #5]]| |[[13]]|M 4/25|Superconductivity|Ibach chapter|{{::day12_2013.pdf|}}: The experimental observations. Note about Type I vs. Type II. Composite bosons. Ionic lattice can be deformed: trail of deformation. Size scale for attractive interaction. The Cooper pair wavefunction. The Cooper pair binding energy at T = 0.  The number density of Cooper pairs. Temperature dependence of Cooper pair binding energy.  |[[hw5|HW #5]]|
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 |[[14]]|W 4/27|Superconductivity|Ibach chapter|{{::day13_2013.pdf|}}: Center of mass motion of Cooper pairs. Critical current density. London equation. London penetration depth. Solenoid field generated by a solid cylinder of superconductor. Critical B field for Type I superconductor. Explaining the difference between Type I and Type II superconductors. | | |[[14]]|W 4/27|Superconductivity|Ibach chapter|{{::day13_2013.pdf|}}: Center of mass motion of Cooper pairs. Critical current density. London equation. London penetration depth. Solenoid field generated by a solid cylinder of superconductor. Critical B field for Type I superconductor. Explaining the difference between Type I and Type II superconductors. | |
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 |[[15]]|F 4/29 | | | || |[[15]]|F 4/29 | | | ||
  
start.txt · Last modified: 2020/03/06 09:14 by 127.0.0.1