Rotatable prisms for controlling dispersion magnitude and orientation and methods of use
Systems and methods for dispersing an optical beam are disclosed. In one implementation, an optical system includes a first double Amici prism and a second double Amici prism. The first and second double Amici prisms are aligned along an optical axis of the system and configured to transmit the optical beam. At least one of the first and second double Amici prisms is rotatable relative to the other around the optical axis. Advantageously, the disclosed systems and methods allow for efficient and versatile adjustment of the magnitude and/or orientation of the dispersion of the optical beam.
1. An optical system for dispersing an optical beam, comprising:
a first double Amici prism; and
a second double Amici prism;
wherein the first and second double Amici prisms are aligned along an optical axis of the optical system and configured to transmit the optical beam;
wherein at least one of the first and second double Amici prisms is rotatable relative to the other around the optical axis;
wherein each of the first and second double Amici prisms comprises a first element, a second element, and a third element;
wherein the third element is arranged between the first element and the second element;
wherein each of the first element and the second element is made of a first glass having a first index of refraction, and the third element is made of a second glass having a second index of refraction that is different from the first index of refraction; and
wherein an input optical axis and an output optical axis of a predetermined wavelength of the optical beam are collinear.
2. The system of claim 1 , wherein the first and second double Amici prisms are independently rotatable around the optical axis.
3. The system of claim 1 , wherein at least one of the first and second double Amici prisms is rotatable relative to the other around the optical axis by a rotational angle ranging from 0° to 180°.
4. The system of claim 3 , wherein a magnitude of the dispersion of the optical beam varies with the rotational angle.
5. The system of claim 4 , wherein the optical beam is dispersed to a maximum magnitude when the rotational angle is 0°.
6. The system of claim 4 , wherein the optical beam is dispersed to a minimum magnitude when the rotational angle is 180°.
7. The system of claim 1 , wherein the first double Amici prism and the second double Amici prism are identical.
8. The system of claim 1 , wherein an orientation of the dispersion of the optical beam is determined by rotational angles of both of the first and second double Amici prisms around the optical axis.
9. The system of claim 1 , further comprising a first lens configured to collimate the optical beam before the dispersion and a second lens configured to focus the optical beam after the dispersion.
10. The system of claim 1 , wherein each of the first and second double Amici prisms comprises a first face through which the optical beam enters and a second face through which the optical beam exits, and each of the first face and the second face is oriented at a non-perpendicular angle with respect to the optical axis.
11. A method for dispersing an optical beam, comprising:
receiving the optical beam;
transmitting the optical beam through a first double Amici prism and a second double Amici prism, the first and second double Amici prisms being aligned along an optical axis; and
dispersing the optical beam to a predetermined magnitude by rotating at least one of the first and second double Amici prisms relative to the other around the optical axis;
wherein each of the first and second double Amici prisms comprises a first element, a second element, and a third element;
wherein the third element is arranged between the first element and the second element;
wherein each of the first element and the second element is made of a first glass having a first index of refraction, and the third element is made of a second glass having a second index of refraction that is different from the first index of refraction; and
wherein an input optical axis and an output optical axis of a predetermined wavelength of the optical beam are collinear.
12. The method of claim 11 , wherein the first and second double Amici prisms are independently rotatable around the optical axis.
13. The method of claim 11 , further comprising varying the predetermined magnitude by adjusting a rotational angle between the first and second double Amici prisms around the optical axis to a degree ranging from 0° to 180°.
14. The method of claim 13 , further comprising dispersing the optical beam to a maximum magnitude when the rotational angle is 0°.
15. The method of claim 13 , further comprising dispersing the optical beam to a minimum magnitude when the rotational angle is 180°.
16. The method of claim 11 , wherein the first double Amici prism and the second double Amici prism are identical.
17. The method of claim 11 , further comprising adjusting an orientation of the dispersion of the optical beam by rotating both of the first and second double Amici prisms around the optical axis.
18. The method of claim 11 , further comprising
collimating, using a first lens, the optical beam before the dispersion; and
focusing, using a second lens, the optical beam after the dispersion.
19. The method of claim 11 , wherein each of the first and second double Amici prisms comprises a first face through which the optical beam enters and a second face through which the optical beam exits, and each of the first face and the second face is oriented at a non-perpendicular angle with respect to the optical axis.
20. A method for configuring a hyperspectral imaging system, comprising:
receiving an optical beam;
transmitting the optical beam through a set of optical elements aligned along an optical axis, the set of optical elements comprising:
a first double Amici prism;
a second double Amici prism; and
at least one lens; and
dispersing the optical beam to a predetermined magnitude by rotating at least one of the first and second double Amici prisms relative to the other around the optical axis;
wherein each of the first and second double Amici prisms comprises a first element, a second element, and a third element;
wherein the third element is arranged between the first element and the second element;
wherein each of the first element and the second element is made of a first glass having a first index of refraction, and the third element is made of a second glass having a second index of refraction that is different from the first index of refraction; and
wherein an input optical axis and an output optical axis of a predetermined wavelength of the optical beam are collinear.