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Master Equation - Based Numerical Simulation in a Single Electron ...

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242<br />

<strong>Numerical</strong> <strong>Simulation</strong>s of Physical and Eng<strong>in</strong>eer<strong>in</strong>g Processes<br />

3.1 Total charg<strong>in</strong>g energy<br />

In order to calculate total charg<strong>in</strong>g energy, it is necessary to determ<strong>in</strong>e the voltage applied<br />

on the tunnel capacitor ( ) and tunnel capacitor ( ) us<strong>in</strong>g the follow<strong>in</strong>g step. The<br />

configuration of the charges on each capacitor <strong>in</strong> the s<strong>in</strong>gle-electron transistor circuit<br />

(Figure1) can be expressed as (Tucker, 1992),<br />

= = ( − ), (6a)<br />

= , (6b)<br />

=( −). (6c)<br />

It is noted that the is also subjected to the voltage <strong>in</strong> the dot. Charge <strong>in</strong> the dot is given by,<br />

=− − =−. (7)<br />

Here, =− is a number of electrons <strong>in</strong> the dot.<br />

If the equations (6a), (6b) and (6c) are <strong>in</strong>serted <strong>in</strong>to an equation (7), it can be obta<strong>in</strong>ed the as a function of dra<strong>in</strong> voltage and gate voltage , as follows,<br />

− ( − ) − ( − ) =,<br />

= 1<br />

(<br />

<br />

+ +)<br />

(8)<br />

<br />

From equation (8) and relationship of + =, it can be obta<strong>in</strong>ed the value of voltage on<br />

capacitor , as follows,<br />

=− 1<br />

(<br />

<br />

+ +)<br />

<br />

= 1<br />

( +<br />

<br />

) − −<br />

(9)<br />

<br />

Note that both and are a function of , which is the number of electrons <strong>in</strong> the dot<br />

because of =−. Next, total charg<strong>in</strong>g energy on the SET system can be calculated as follows,<br />

= <br />

+<br />

2 <br />

+<br />

2 <br />

2 = 1<br />

<br />

2<br />

( −) <br />

+ + + <br />

(10)<br />

S<strong>in</strong>ce the values of external power supply and is constant, the effect on electron<br />

tunnel<strong>in</strong>g process only <strong>in</strong>fluences the term of ⁄ 2. 3.2 Work done by external voltage source due to tunnel event<br />

There are two types of tunnel events, i.e., electron tunnels through the capacitor and the<br />

electron tunnels through the capacitor . The amount of the work done by external voltage<br />

source is different from one event to another one. Therefore, the detail explanation of the<br />

work done for these two types is discussed. Figure 3 shows the charge flow enter/exit from<br />

the voltage source when the electron tunnel through the capacitor (right direction).

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