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Massachusetts Institute of Technology 6.763 2003 Lecture 13
Generalized Josephson Junctions
Outline
1. Junctions with Resistive Channel2. RCSJ Model3. DC Current Drive
• Overdamped and Underdamped Junctions• Return Current• Dynamical Analysis
4. Pendulum Model
October 16, 2003
Massachusetts Institute of Technology 6.763 2003 Lecture 13
Junctions with Resistive Channel
G(v) the resistive conductance
Massachusetts Institute of Technology 6.763 2003 Lecture 13
Tunneling between two superconductors
Giaever Tunneling
Josephson Tunneling
S-I-S G(v)
Massachusetts Institute of Technology 6.763 2003 Lecture 13
Normal and Superconducting AnalogySuperconductor Superconducting Josephson Junction
LJ-1
For a normal junction, the phase is constantly being driven back to zero so linearize near zero and add a damping time
Normal metal
for dc drivefor dc drive
andand
Massachusetts Institute of Technology 6.763 2003 Lecture 13
ICRn Product
The condition is equivalent to
Experimentally, For Nb at 2K,
Massachusetts Institute of Technology 6.763 2003 Lecture 13
Capacitance of a Josephson Junction
Massachusetts Institute of Technology 6.763 2003 Lecture 13
Generalized Josephson Junction
and
Therefore,
Massachusetts Institute of Technology 6.763 2003 Lecture 13
RCSJ Modeli
and
Therefore,
Massachusetts Institute of Technology 6.763 2003 Lecture 13
DC Current drive in the RSCJ Model
and
Therefore,
The equation of motion can be rewritten as
where
Stewart-McCumber Parameter Q2Josephson Time Constant
Massachusetts Institute of Technology 6.763 2003 Lecture 13
Overdamped Junction βc << 1τJ >> τRC
A. Static Solution:
B. Dynamical Solution for i > Ic
This is periodic with period
Massachusetts Institute of Technology 6.763 2003 Lecture 13
Overdamped Junction βc << 1
v(t)/IcR
t
<v>/(IcR)
i/Ic
The time averaged voltage is
Use the voltage-phase relation,
Therefore,
Non-hysteretic
Massachusetts Institute of Technology 6.763 2003 Lecture 13
Underdamped Junction βc >> 1τRC >> τJ
A. Static Solution:
B. Dynamical Solution
The phase changes quickly compared to RC, so the voltage is just from R and C.Therefore,
<v(t)> i R
Hysteretic
Massachusetts Institute of Technology 6.763 2003 Lecture 13
Junction with arbitrary βc
A. Static Solution:
Return CurrentB. Dynamical Solution
Massachusetts Institute of Technology 6.763 2003 Lecture 13
Return CurrentEnergy Loss per cycle = Energy supplied by sourc
where V= IR and τ = Φ0 / (2 π I R), therefore
So that
Massachusetts Institute of Technology 6.763 2003 Lecture 13
Dynamical Analysis
andwhere
Massachusetts Institute of Technology 6.763 2003 Lecture 13
βc = 4
(t)
V(φ)
<V>/ICR
i/ICΒ
Β
A A
C
C
V(t)
φ(t)
V(φ)
V(t)V(t)
φ(t)
V(φ)
Massachusetts Institute of Technology 6.763 2003 Lecture 13
βc =0.5
V(t)
φ(t)
V(φ)
φ(t)
V(φ)
i/IC
<V>/ICR
C
C
B
AA V(t)
φ(t)
V(t)B
Massachusetts Institute of Technology 6.763 2003 Lecture 13
Pendulum Model for a Josephson Junction
τapp
mg
ϕ
l
R
-
+
Icsinϕ
CIapp
• Single junction (RCSJ model) pendulum (damped)• Coupled junctions – can support non-linear excitations (breathers and
moving vortices)
Massachusetts Institute of Technology 6.763 2003 Lecture 13
Pendulum Model for a vortex