The Group Velocity in a One-Dimensional Material

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The discussion focuses on calculating the electron group velocity in a one-dimensional material subjected to a time-varying electric field. The band structure is defined as E = ħν|k|, and the group velocity is expressed as v_g = (1/ħ)(dE/dk). Participants suggest incorporating the electric field into the equation by relating the change in wave vector k to the electric field through the equation dk/dt = -eE(t). The conversation highlights challenges in integrating the electric field into the group velocity calculation, emphasizing the need for clarity in the mathematical approach. Understanding the relationship between the electric field and the resulting group velocity is crucial for solving the problem.
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Homework Statement


A one-dimensional material has an applied time varying e-field as shown below:

<br /> \epsilon(t)=\left\{\begin{array}{cc}A_1,&amp;0\le t \le 2<br /> \\0,&amp; 2\le t \le 4<br /> \\-A_1,&amp; 4\le t \le 6<br /> \end{array}\right<br />

The band structure of the material is E=\hbar\nu\|k\|, where \nu is a constant with units of velocity. What is the electron gorup velocity as a function of time from 0 to 6?

Homework Equations


<br /> v=\frac{d\omega}{dk}=\frac{dE}{dp}<br />

The Attempt at a Solution


<br /> v_g=\frac{1}{\hbar}\frac{dE}{dk}<br />

I'm not sure on how to include the e-field into this equation. Any suggestions?
 
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soekdi said:

Homework Statement


A one-dimensional material has an applied time varying e-field as shown below:

<br /> \epsilon(t)=\left\{\begin{array}{cc}A_1,&amp;0\le t \le 2<br /> \\0,&amp; 2\le t \le 4<br /> \\-A_1,&amp; 4\le t \le 6<br /> \end{array}\right<br />

The band structure of the material is E=\hbar\nu\|k\|, where \nu is a constant with units of velocity. What is the electron gorup velocity as a function of time from 0 to 6?

Homework Equations


<br /> v=\frac{d\omega}{dk}=\frac{dE}{dp}<br />

The Attempt at a Solution


<br /> v_g=\frac{1}{\hbar}\frac{dE}{dk}<br />

I'm not sure on how to include the e-field into this equation. Any suggestions?

Probably you just want to account for the fact that k depends on time via
<br /> \frac{d\bold{k}}{dt}=-e\bold{E}(t)\;,<br />
where
<br /> \bold{E}(t)<br />
is the electric field and -e is the charge of the electron.
 
olgranpappy said:
Probably you just want to account for the fact that k depends on time via
<br /> \frac{d\bold{k}}{dt}=-e\bold{E}(t)\;,<br />
where
<br /> \bold{E}(t)<br />
is the electric field and -e is the charge of the electron.

Now I'm having trouble with the math part:
<br /> dE=\hbar \nu dk<br />

<br /> dk=-e\epsilon(t)dt<br />

<br /> v_g=\frac{1}{\hbar}\frac{dE}{dk}=\frac{\nu dk}{-e\epsilon(t)dt}<br />

where \epsilon is the e-field. This doesn't really look right?
 
soekdi said:
Now I'm having trouble with the math part:
<br /> dE=\hbar \nu dk<br />

<br /> dk=-e\epsilon(t)dt<br />

<br /> v_g=\frac{1}{\hbar}\frac{dE}{dk}=\frac{\nu dk}{-e\epsilon(t)dt}<br />

where \epsilon is the e-field. This doesn't really look right?

mmm... if you just forget about the electric field for a second and just look at
<br /> E=\hbar v |k|\;,<br />
what is the group velocity?
 
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