Barrier Tunneling — Question 5

Section 38-8 · Physics pages 6400–6401

Question 5 A tunneling-current slope gives an effective vacuum barrier height In a simplified tunneling microscope, current follows I(d) = I0e−2κd with gap d and fixed bias. Retracting the tip by .200 nm reduces current by a factor of 100. Model the barrier with κ = √2meΦ/ℏ, where Φ is the effective barrier energy. For electrons use ℏ2/(2me) = .0381 eV nm2. d sample tip Schematic; labels, not drawing lengths, specify the data. (a) Infer κ from the current ratio. (b) Infer Φ and state the role of the assumed fixed prefactor.
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Question 5 - Solution A tunneling-current slope gives an effective vacuum barrier height d sample tip (a) Method and calculation ln[I(d)/I(d + ∆d)] = 2κ∆d = ln 100. κ = ln 100 .400 nm = 11.5129 nm−1 . (b) Interpretation and further calculation Φ = ℏ2κ2 2me = (.0381)(11.5129255)2 eV. Φ = 5.05006 eV , d ln I dd = −2κ if I0 is fixed. Physical check This is an effective barrier inferred within the supplied model. Changes of electronic structure, bias or prefactor would also affect the measured slope.

Question 5

A tunneling-current slope gives an effective vacuum barrier height

In a simplified tunneling microscope, current follows I(d)=I0e−2κdI(d)=I_0e^{-2\kappa d} with gap d and fixed bias. Retracting the tip by .200nm.200\,\mathrm{nm} reduces current by a factor of 100. Model the barrier with κ=2meΦ/ℏ\kappa=\sqrt{2m_e\Phi}/\hbar, where Φ\Phi is the effective barrier energy. For electrons use ℏ2/(2me)=.0381eVnm2\hbar^2/(2m_e)=.0381\,\mathrm{eV\,nm^2}.

Diagram shown in the original SVG worksheet.

  1. Infer κ\kappa from the current ratio.

  2. Infer Φ\Phi and state the role of the assumed fixed prefactor.

Question 5 - Solution

A tunneling-current slope gives an effective vacuum barrier height

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ln⁡[I(d)/I(d+Δd)]=2κΔd=ln⁡100.\ln[I(d)/I(d+\Delta d)]=2\kappa\Delta d=\ln100.κ=ln⁡100.400nm=11.5129nm−1.\boxed{\kappa=\frac{\ln100}{.400\,\mathrm{nm}}=11.5129\,\mathrm{nm}^{-1}}.

(b) Interpretation and further calculation

Φ=ℏ2κ22me=(.0381)(11.5129255)2eV.\Phi=\frac{\hbar^2\kappa^2}{2m_e}=(.0381)(11.5129255)^2\,\mathrm{eV}.Φ=5.05006eV,dln⁡Idd=−2κif I0 is fixed.\boxed{\Phi=5.05006\,\mathrm{eV}},\quad\frac{d\ln I}{dd}=-2\kappa\quad\text{if }I_0\text{ is fixed}.

Physical check

This is an effective barrier inferred within the supplied model. Changes of electronic structure, bias or prefactor would also affect the measured slope.