Loading src/modules/ElectricFieldReader/README.md +2 −2 Original line number Diff line number Diff line Loading @@ -22,7 +22,7 @@ The reader provides the following models for electric fields: The sign of depletion voltage is always ignored. If the sensor is depleted from the implant side, the absolute value of the electric field is calculated using the formula ```math E(z) = \|frac{U_{bias}| - |U_{depl}|}{d} + 2 \frac{|U_{depl}|}{d}\left( 1- \frac{z}{d} \right), E(z) = \frac{|U_{bias}| - |U_{depl}|}{d} + 2 \frac{|U_{depl}|}{d}\left( 1- \frac{z}{d} \right), ``` where d is the thickness of the sensor, and $`U_{depl}`$, $`U_{bias}`$ are the depletion and bias voltages, respectively. In case of a depletion from the back side, the absolute value of the electric field is calculated as Loading Loading
src/modules/ElectricFieldReader/README.md +2 −2 Original line number Diff line number Diff line Loading @@ -22,7 +22,7 @@ The reader provides the following models for electric fields: The sign of depletion voltage is always ignored. If the sensor is depleted from the implant side, the absolute value of the electric field is calculated using the formula ```math E(z) = \|frac{U_{bias}| - |U_{depl}|}{d} + 2 \frac{|U_{depl}|}{d}\left( 1- \frac{z}{d} \right), E(z) = \frac{|U_{bias}| - |U_{depl}|}{d} + 2 \frac{|U_{depl}|}{d}\left( 1- \frac{z}{d} \right), ``` where d is the thickness of the sensor, and $`U_{depl}`$, $`U_{bias}`$ are the depletion and bias voltages, respectively. In case of a depletion from the back side, the absolute value of the electric field is calculated as Loading
