Editing field effect

{{title|Field Effect}}
'''Field effect''' is a principle that refers to the modulation of [[conductance]] of a material through the use of an external [[electric field]].

== Overview ==
In an [[insulator]], most atoms hold on to their [[electrons]] tightly. Contrary to an insulator, in a conductor, the [[valence electrons]] of the atoms are loosely bound and are free to roam through the lattice of the material. Those [[free electrons]] are always in random and ccontinuous motion due to the thermal energy of the conductor.

[[File:free electron in a conductor.gif]]

As they travel in random motion, free electrons collide with each other. In between collisions, electrons acquire relatively high velocity. However, due to their random motion, those charge carriers continue to suffer collisions so frequently that the net flow in any particular direction is roughly zero. That is, those electrons do not go anywhere.

The average distance traveled by those free electrons between any two successive collisions, or the [[mean free path]] (<math>\lambda</math>, [cm]), can be calculated as the product of the time between collisions (<math>\tau_C</math>, [s]) and the [[thermal velocity]] (<math>V_\text{th}</math>, [cm/s]). For example, [[silicon]] at ambient temperature (somewhere around <math>V_\text{th}</math> = 10^7 cm/s) with <math>\tau_C</math> = 0.1ps would mean the average distance traveled is 10nm.

When an external [[electric field]] is applied to the conductor, that is when some potential difference is applied across the semiconductor, each of the free electrons in the conductor now experience a force in the direction opposite to the direction of the electric field.

[[File:free electron in a conductor with electric field.gif]]

That is, when under the effect of an electric field, the free electrons now flow in the a direction that is opposite to the direction of the electric field, in addition to their thermal velocities.
@@ Line 3: / Line 3: @@
 == Overview ==
-In an [[insulator]], most atoms hold on to their [[electrons]] tightly. Contrary to an insulator, in a conductor, the [[valence electrons]] of the atoms are loosely bound and are free to roam through the lattice of the material. Those [[free electrons]] are always in random and ccontinuous motion due to the [[thermal energy]] of the conductor.
+In an [[insulator]], most atoms hold on to their [[electrons]] tightly. Contrary to an insulator, in a conductor, the [[valence electrons]] of the atoms are loosely bound and are free to roam through the lattice of the material. Those [[free electrons]] are always in random and ccontinuous motion due to the thermal energy of the conductor.
 [[File:free electron in a conductor.gif]]
-As they travel in random motion, free electrons collide with each other. In between collisions, electrons acquire relatively high velocity. However, due to their random motion, those [[charge carriers]] continue to suffer collisions so frequently that the net flow in any particular direction is roughly zero. That is, those electrons do not go anywhere.
+As they travel in random motion, free electrons collide with each other. In between collisions, electrons acquire relatively high velocity. However, due to their random motion, those charge carriers continue to suffer collisions so frequently that the net flow in any particular direction is roughly zero. That is, those electrons do not go anywhere.
-The average distance traveled by those free electrons between any two successive collisions, or the [[mean free path]] (<math>\lambda</math>, [cm]), can be calculated as the product of the [[mean free time|time between collisions]] (<math>\tau_C</math>, [s]) and the [[thermal velocity]] (<math>V_\text{th}</math>, [cm/s]). For example, [[silicon]] at ambient temperature (somewhere around <math>V_\text{th}</math> = 10^7 cm/s) with <math>\tau_C</math> = 0.1ps would mean the average distance traveled is 10nm.
+The average distance traveled by those free electrons between any two successive collisions, or the [[mean free path]] (<math>\lambda</math>, [cm]), can be calculated as the product of the time between collisions (<math>\tau_C</math>, [s]) and the [[thermal velocity]] (<math>V_\text{th}</math>, [cm/s]). For example, [[silicon]] at ambient temperature (somewhere around <math>V_\text{th}</math> = 10^7 cm/s) with <math>\tau_C</math> = 0.1ps would mean the average distance traveled is 10nm.
 When an external [[electric field]] is applied to the conductor, that is when some potential difference is applied across the semiconductor, each of the free electrons in the conductor now experience a force in the direction opposite to the direction of the electric field.
@@ Line 16: / Line 16: @@
 That is, when under the effect of an electric field, the free electrons now flow in the a direction that is opposite to the direction of the electric field, in addition to their thermal velocities.
-== Theory ==
-Below is a rectangular [[conductor]] with length <math>L_c</math>, width <math>W_c</math>, and tickness <math>t_c</math>.
-[[File:field effect rect conductor.svg|600px]]
-In this conductor, the [[valence electrons]] of the atoms are loosely bound and are free to roam around. There are <math>n</math> free electrons per cubic meter of this material, each with have an [[elementary charge]] <math>q</math>.
-We will call this conductor a ''[[channel]]''. Applying a [[electric field]] <math>E</math> [V/cm] across the channel will result in a net force on the carriers.
-:<math>F = \pm q E</math>
-That is, in between their collisions, [[charge carriers]] will acquire a [[drift velocity|new average velocity]].
-:<math>v_d = \pm \mu_{n,p} E</math>
-Where the [[carrier mobility]] (<math>\mu_{n,p}</math> [cm<sup>2</sup>/Vs]) refers to the ease of [[carrier drift]]. Note that for electrons, <math>\mu_n</math> is positive, therefore the direction of <math>v</math> opposes the direction of <math>E</math>.
-:<math>v_{dn} = - \mu_n E</math>
-Likewise, for holes, the mobility <math>\mu_p</math> is positive.
-:<math>v_{dp} = \mu_p E</math>
-The [[drift current]] density is the net velocity of charged particles. That is, the total current density is the product of the mobile charge density and the average carrier velocity.
-:<math>J_n^{\text{drift}} = -q n v_{dn} = q n \mu_n E</math>
-:<math>J_p^{\text{drift}} = q p v_{dp} = q p \mu_p E</math>
-The total drift current density is the sum of the two drift current densities.
-=== Gate ===
-Suppose a gate electrode is now situated above the channel and is physically separated by an insulator of thickness <math>t_\text{ins}</math>.
-[[File:field effect rect conductor - gate.svg|600px]]
-A change in the voltage of the gate <math>V_g</math> will affect the total drift current density in the channel. Therefore a change in the gate voltage will change the gate charge.
-:<math>\Delta Q_g = C_g \Delta V_g</math>
-That is,
-:<math>C_g \Delta V_g = W L t_c \Delta \rho</math>