Petar Mali
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I have a few questions about this effect. If I have some semiconductor of N type in which I have electrical field in x direction, and magnetic field in z direction
\vec{E}=E\vec{e}_x
\vec{B}=B\vec{e}_z
Then Lorence force is in the -y direction because in N type of semiconductor n>>p so
F_l=-e\vec{\upsilon_D}x\vec{B}
And for this case Hall constant R_H=-\frac{1}{ne} is negative. Am I right?
And in same case but for P type Lorentz force will be
F_l=e\vec{\upsilon_D}x\vec{B}
so in y direction, and Hall constant
R_H=\frac{1}{pe}?
\vec{E}=E\vec{e}_x
\vec{B}=B\vec{e}_z
Then Lorence force is in the -y direction because in N type of semiconductor n>>p so
F_l=-e\vec{\upsilon_D}x\vec{B}
And for this case Hall constant R_H=-\frac{1}{ne} is negative. Am I right?
And in same case but for P type Lorentz force will be
F_l=e\vec{\upsilon_D}x\vec{B}
so in y direction, and Hall constant
R_H=\frac{1}{pe}?