Simultaneous QE scanning system and methods for photovoltaic devices
View Patent ↗Methods for simultaneously making quantum efficiency measurements at multiple points in a photovoltaic cell are provided. A light beam (e.g., monochromatic light) can be directed to a first beam splitter, where it is split into a first reflected portion and a first passthrough portion such that the first reflected portion is directed to a first point on the photovoltaic cell. The first reflected portion can then be chopped at a first frequency between the first beam splitter and the first point. The first passthrough portion of the light beam can be reflected at a second beam splitter to a second point on the photovoltaic cell. The second reflected portion can then be chopped at a second frequency between the second beam splitter and the second point. Finally, the quantum efficiency can be calculated at both the first point and the second point. Systems are also generally provided for simultaneously making quantum efficiency measurements at multiple points in a photovoltaic cell.
1. A method of simultaneously making quantum efficiency measurements at multiple points in a photovoltaic cell, comprising:
directing a light beam to a first beam splitter, wherein the light beam defines a monochromatic light;
splitting the light beam at the first beam splitter into a first reflected portion and a first passthrough portion, wherein the first reflected portion is directed to a first point on the photovoltaic cell;
chopping the first reflected portion at a first frequency between the first beam splitter and the first point;
reflecting the first passthrough portion of the light beam at a second beam splitter to a second point on the photovoltaic cell;
chopping the second reflected portion at a second frequency between the second beam splitter and the second point, wherein the first frequency is different than the second frequency; and,
calculating the quantum efficiency at both the first point and the second point.
2. The method of claim 1 , wherein the first frequency and the second frequency do not have a common multiple.
3. The method of claim 1 , wherein the second beam splitter reflects the first passthrough portion of the light beam to the second point on the photovoltaic cell and allows a second passthrough portion of the light beam to pass through the second beam splitter.
4. The method of claim 3 , further comprising:
reflecting the second passthrough portion of the light beam at a third beam splitter to a third point on the photovoltaic cell;
chopping the third reflected portion at a third frequency between the third beam splitter and the third point; and,
calculating the quantum efficiency at the first point, the second point, and the third point.
5. The method of claim 4 , wherein the third frequency is different than both the first frequency and the second frequency.
6. The method of claim 4 , wherein the third beam splitter reflects the second passthrough portion of the light beam to the third point on the photovoltaic cell and allows a third passthrough portion of the light beam to pass through the third beam splitter.
7. The method of claim 6 , further comprising:
reflecting the third passthrough portion of the light beam at a fourth beam splitter to a fourth point on the photovoltaic cell;
chopping the fourth reflected portion at a fourth frequency between the fourth beam splitter and the fourth point; and,
calculating the quantum efficiency at the first point, the second point, the third point, and the fourth point.
8. The method of claim 7 , wherein the fourth frequency is different than the first frequency, the second frequency, and the third frequency.