Consider a rectangular barrier given by the potential for x 0 V(x) = 0 for xa (a) Show that the transmission probability |T|² for a particle of energy E < Vo to tunnel completely through the barrier is determined by the expression T-¹ = 1 + [Vo sinh (2 t a)] 4E (Vo - E) where ht = [2 m (Vo - E)]¹/2 (b) What is T-¹ in the limit that the energy approaches the barrier height E Vo? (c) Calculate |T|² for an electron of energy 1 eV incident on a barrier of height 1 eV and width 1 Å

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4. Consider a rectangular barrier given by the potential
V(x) = Vo > 0 for x <a
V(x) = 0
for xa
(a) Show that the transmission probability |T|² for a particle of energy E < Vo to tunnel completely
through the barrier is determined by the expression
T-¹ = 1 +
[Vo sinh (2 t a)]
4 E (Vo - E)
where ht= [2 m (Vo - E)] ¹1/2
(b) What is T -¹ in the limit that the energy approaches the barrier height E
-1
Vo?
(c) Calculate |T|² for an electron of energy 1 eV incident on a barrier of height 1 eV and width 1 Å
Hyperbolic Sine Function: sinh y = ½ (e-e).
Taylor series: ey = 1 + y + ¹ y² +
Transcribed Image Text:4. Consider a rectangular barrier given by the potential V(x) = Vo > 0 for x <a V(x) = 0 for xa (a) Show that the transmission probability |T|² for a particle of energy E < Vo to tunnel completely through the barrier is determined by the expression T-¹ = 1 + [Vo sinh (2 t a)] 4 E (Vo - E) where ht= [2 m (Vo - E)] ¹1/2 (b) What is T -¹ in the limit that the energy approaches the barrier height E -1 Vo? (c) Calculate |T|² for an electron of energy 1 eV incident on a barrier of height 1 eV and width 1 Å Hyperbolic Sine Function: sinh y = ½ (e-e). Taylor series: ey = 1 + y + ¹ y² +
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