View the particle system in a one-dimensional box in the range ≤ x ≤ of m-mass and q- charged particles. The system is then plagued with an electric field as a function of time t such that the potential energy of the fault can be expressed as for t < 0 0 v (t) = {-xe-At for t > 0 with e amplitude of electric field Calculate the probability of transition from state n to state m as a time function t. And state which n-m transitions are allowed and not allowed to occur.
View the particle system in a one-dimensional box in the range ≤ x ≤ of m-mass and q- charged particles. The system is then plagued with an electric field as a function of time t such that the potential energy of the fault can be expressed as for t < 0 0 v (t) = {-xe-At for t > 0 with e amplitude of electric field Calculate the probability of transition from state n to state m as a time function t. And state which n-m transitions are allowed and not allowed to occur.
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box in the range ≤ x ≤ of m-mass and q-
charged particles. The system is then plagued with an electric field as a function of time t such that
the potential energy of the fault can be expressed as
0
for t < 0
v(t) = (-Exe
-q©xe-At for t > 0
with e amplitude of electric field
Calculate the probability of transition from state n to state m as a time function t.
And state which n-m transitions are allowed and not allowed to occur."
Transcribed Image Text:View the particle system in a one-dimensional
box in the range ≤ x ≤ of m-mass and q-
charged particles. The system is then plagued with an electric field as a function of time t such that
the potential energy of the fault can be expressed as
0
for t < 0
v(t) = (-Exe
-q©xe-At for t > 0
with e amplitude of electric field
Calculate the probability of transition from state n to state m as a time function t.
And state which n-m transitions are allowed and not allowed to occur.
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