About the Hall Coefficient
The Hall effect occurs when a magnetic field is applied perpendicular to the current flowing through a conductor or semiconductor: the moving charge carriers feel a sideways Lorentz force and pile up along one edge of the sample, building a small transverse voltage — the Hall voltage — across it. The Hall coefficient, R_H, is the material property that links this voltage to the current, magnetic field, and sample geometry, and it reveals both the density and the sign (electron or hole) of the dominant charge carrier.
Deriving the Hall coefficient formula
In steady state, the electric force from the built-up Hall field balances the magnetic force on the carriers: qE_y = qv_xB_z. Since the current density is J_x = nqv_x, substituting gives E_y = J_xB_z / (nq), so the Hall coefficient is defined as R_H = E_y / (J_xB_z) = 1 / (nq). Writing the field and current density in terms of measurable quantities — E_y = V_H / w and J_x = I / (w·t), where w is the sample width and t is its thickness along the field direction — the width w cancels out, leaving the practical working formula: R_H = V_H·t / (I·B). From R_H you can also recover the carrier concentration directly: n = 1 / (R_H·e), where e = 1.602 × 10⁻¹⁹ C is the elementary charge.
Working with units and sign convention
- Keep every quantity in consistent SI units before computing by hand: volts (V), amps (A), tesla (T), and meters (m). This calculator converts your chosen units for you.
- Common conversions: 1 mT = 0.001 T, 1 gauss (G) = 10⁻⁴ T, and 1 mA = 0.001 A.
- The Hall voltage's sign matters — enter it as measured (positive or negative). A positive R_H points to holes (p-type); a negative R_H points to electrons (n-type).
Practical limits and assumptions
This single-carrier formula assumes one dominant charge carrier type, a uniform current density, and a thin, geometrically uniform sample with ohmic (non-rectifying) contacts. Real semiconductors can have both electron and hole populations contributing simultaneously, which biases the simple R_H = 1/(nq) result — this is usually handled with a two-carrier model or a Hall scattering factor correction. R_H can also vary with temperature and with the strength of the applied magnetic field, so measurements are typically reported alongside the temperature and field at which they were taken.