Temp: Difference between revisions
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Consider a simplified model of a 2DEG where electron gas is in external potential <math>V=0</math> for <math>z < d/2</math> and <math> V=V_0</math> for <math>|z| > d/2</math>. | Consider a simplified model of a 2DEG where electron gas is in external potential <math>V=0</math> for <math>z < d/2</math> and <math> V=V_0</math> for <math>|z| > d/2</math>. | ||
::(a) What is the density of states (DOS) as a function of energy for <math>V_0 \rightarrow \infty</math>? Discuss what happens at low energies and how DOS behaves in the limit of high energies. | |||
::(b) Assume <math>V_0 \rightarrow \infty</math> and <math> d = 100 \AA</math>. Up to what temperatures can we consider the electrons to be two-dimensional? (HINT: The electrons will behave two-dimensionally if <math>k_BT</math> is less then the difference between the ground and first excited energy level in the confining potential). | |||
::(c) In real systems we can only produce a finite potential well. This puts a lower limit on <math> d </math> since the ground state must be a bound state in the ''z'' direction with a clear energy gap up to the first excited state. If we can produce a potential of <math>V_0=100</math> meV and reach a temperature of 20 mK, what is the range of thicknesses feasible for the study of such two-dimensional electron gas? | |||
==Problem 3== | ==Problem 3== | ||
Revision as of 22:01, 11 September 2009
Problem 1
Problem 2
The dimensionality of a system can be reduced by confining the electrons in certain directions. A two-dimensional electron gas (2DEG) is produced in semiconductor heterostructures and is used for the investigation of the quantum Hall effect, creation of semiconductor quantum dots, quantum point contacts, nanowires, etc.
Consider a simplified model of a 2DEG where electron gas is in external potential Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle V=0} for Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle z < d/2} and Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle V=V_0} for Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle |z| > d/2} .
- (a) What is the density of states (DOS) as a function of energy for Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle V_0 \rightarrow \infty} ? Discuss what happens at low energies and how DOS behaves in the limit of high energies.
- (b) Assume Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle V_0 \rightarrow \infty} and Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle d = 100 \AA} . Up to what temperatures can we consider the electrons to be two-dimensional? (HINT: The electrons will behave two-dimensionally if Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle k_BT} is less then the difference between the ground and first excited energy level in the confining potential).
- (c) In real systems we can only produce a finite potential well. This puts a lower limit on Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle d } since the ground state must be a bound state in the z direction with a clear energy gap up to the first excited state. If we can produce a potential of Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle V_0=100} meV and reach a temperature of 20 mK, what is the range of thicknesses feasible for the study of such two-dimensional electron gas?
