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
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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![### Consider a rectangular barrier given by the potential
\[
V(x) = V_0 > 0 \quad \text{for } |x| < a
\]
\[
V(x) = 0 \quad \text{for } |x| > a
\]
#### (a) Transmission Probability
Show that the transmission probability \(|T|^2\) for a particle of energy \(E < V_0\) to tunnel completely through the barrier is determined by the expression:
\[
T^{-1} = 1 + \frac{{[V_0 \sinh(2ta)]^2}}{{4E(V_0 - E)}}
\]
where
\[
\hbar t = \sqrt{2m(V_0 - E)}
\]
#### (b) Energy Approaching Barrier Height
What is \(T^{-1}\) in the limit that the energy approaches the barrier height \(E \rightarrow V_0\)?
#### (c) Calculate \(|T|^2\)
Calculate \(|T|^2\) for an electron of energy 1 eV incident on a barrier of height 1 eV and width 1 Å.
---
### Additional Information
**Hyperbolic Sine Function:**
\[
\sinh y = \frac{1}{2} (e^y - e^{-y})
\]
**Taylor Series:**
\[
e^y = 1 + y + \frac{1}{2}y^2 + \ldots
\]](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2F62a79166-ba2c-43d7-9fa1-94c5c5be2063%2F112224cf-b012-4272-b804-9c33bc4d66b5%2Fl8pag0am_processed.png&w=3840&q=75)
Transcribed Image Text:### Consider a rectangular barrier given by the potential
\[
V(x) = V_0 > 0 \quad \text{for } |x| < a
\]
\[
V(x) = 0 \quad \text{for } |x| > a
\]
#### (a) Transmission Probability
Show that the transmission probability \(|T|^2\) for a particle of energy \(E < V_0\) to tunnel completely through the barrier is determined by the expression:
\[
T^{-1} = 1 + \frac{{[V_0 \sinh(2ta)]^2}}{{4E(V_0 - E)}}
\]
where
\[
\hbar t = \sqrt{2m(V_0 - E)}
\]
#### (b) Energy Approaching Barrier Height
What is \(T^{-1}\) in the limit that the energy approaches the barrier height \(E \rightarrow V_0\)?
#### (c) Calculate \(|T|^2\)
Calculate \(|T|^2\) for an electron of energy 1 eV incident on a barrier of height 1 eV and width 1 Å.
---
### Additional Information
**Hyperbolic Sine Function:**
\[
\sinh y = \frac{1}{2} (e^y - e^{-y})
\]
**Taylor Series:**
\[
e^y = 1 + y + \frac{1}{2}y^2 + \ldots
\]
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Step 1: a) Calculate the T^-1:
VIEWStep 2: Calculate the T^-1:
VIEWStep 3: Calculate the T^-1:
VIEWStep 4: Calculate the T^-1:
VIEWStep 5: Calculate the T^-1:
VIEWStep 6: Calculate the T^-1:
VIEWStep 7: Calculate the T^-1:
VIEWStep 8: b) Use of E tends to V(0) limit:
VIEWStep 9: c) Calculate the value of T^2:
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