Kinematics path method for laser-induced breakdown spectroscopy
A method for compositional analysis includes providing a sample having a surface and determining with a controller a plurality of equidistant positions along an oscillatory path along the surface. The oscillatory path is sinusoid in at least one orthogonal dimension within a plane approximately parallel to the surface. The method further includes, for each equidistant position of the plurality of equidistant position, moving an ablation point along the oscillatory path to the each equidistant position, pulsing an energy source to provide an electromagnetic energy beam to ablate material at the ablation point, and collecting an emission spectrum with a spectrographic instrument in response to pulsing the energy source. The method also includes analyzing the emission spectrum to determine a composition at the surface.
1. A method for compositional analysis, the method comprising:
providing a sample having a surface;
determining with a controller a plurality of equidistant positions along an oscillatory path along the surface, the oscillatory path being sinusoid in at least one orthogonal dimension within a plane approximately parallel to the surface, wherein an amplitude of the oscillatory path in the at least one orthogonal dimension is a function of position in another orthogonal dimension;
for each equidistant position of the plurality of equidistant positions:
moving an ablation point along the oscillatory path to each of the plurality of equidistant position;
pulsing an energy source to provide an electromagnetic energy beam to ablate material at the ablation point; and
collecting an emission spectrum with a spectrographic instrument in response to pulsing the energy source; and
analyzing the emission spectrum to determine a composition at the surface.
2. The method of claim 1 , wherein moving the ablation point includes moving the sample using a translation plate.
3. The method of claim 1 , wherein moving the ablation point includes positioning mirrors.
4. The method of claim 1 , wherein the plurality of equidistant positions are linearly equidistant along the oscillatory path.
5. The method of claim 1 , wherein the plurality of equidistant positions are curvilinearly equidistant along the oscillatory path.
6. The method of claim 1 , wherein, in the another orthogonal dimension within the plane, the oscillatory path varies in proportion to time.
7. The method of claim 1 , wherein, in the another orthogonal dimension within the plane, the oscillatory path is sinusoidal.
8. The method of claim 1 , wherein the oscillatory path is continuously differentiable.
9. The method of claim 1 , wherein, in the at least one orthogonal dimension within the plane, the oscillatory path varies as one of a sine or cosine function of time and, in the another orthogonal dimension within the plane, the oscillatory path varies as the other of the sine or cosine function of time.
10. The method of claim 7 , wherein, in the at least one orthogonal dimension within the plane, the oscillatory path varies with a first periodicity and, in the another orthogonal dimension within the plane, the oscillatory path varies with a second periodicity, wherein the first periodicity is an integer multiple of the second periodicity.
11. The method of claim 10 , wherein the integer multiple is in a range of 1 to 100.
12. The method of claim 11 , wherein the integer multiple is in a range of 2 to 20.
13. The method of claim 1 , wherein analyzing the emission spectrum includes averaging the composition for each equidistant position of the plurality of equidistant positions.
14. The method of claim 1 , further comprising selecting a test area on the surface of the sample, the oscillatory path being within the test area.
15. The method of claim 14 , further comprising determining a center line of the test area and determining a width of the center line, the center line extending in the another orthogonal dimensions within the plane.
16. The method of claim 15 , further comprising, with the controller:
determining a distance in the at least one orthogonal dimension from the center line to an edge of the test area at a peak of a sinusoidal oscillation; and
adjusting an amplitude of the sinusoidal oscillation based on the distance.
17. A system for laser-induced breakdown spectroscopy comprising:
a table to receive a sample;
a laser source to provide a laser beam;
a mirror system to direct the laser beam to a surface of the sample, the laser beam to ablate a portion of the sample at an ablation point and to initiate a plasma that emits an emission spectrum;
a spectrographic instrument to receive the spectrum; and
a controller in communication with the mirror system, the controller to determine a plurality of equidistant positions along an oscillatory path along the surface, the oscillatory path being sinusoid in at least one orthogonal dimension within a plane approximately parallel to the surface, wherein an amplitude of the oscillatory path in the at least one orthogonal dimension is a function of position in another orthogonal dimension, the controller to control the mirror system to move the ablation point along the oscillatory path to each equidistant position.
18. The system of claim 17 , wherein the controller is in communication with the laser source, the controller to direct the laser to pulse the laser beam.
19. The method of claim 1 , wherein, in the at least one orthogonal dimension within the plane, the oscillatory path varies with a first periodicity and, in the another orthogonal dimension within the plane, the oscillatory path varies with a second periodicity, wherein the first periodicity is different from the second periodicity.
20. The system of claim 17 , wherein, in the at least one orthogonal dimension within the plane, the oscillatory path varies with a first periodicity and, in the another orthogonal dimension within the plane, the oscillatory path varies with a second periodicity, wherein the first periodicity is different from the second periodicity.