TY - GEN
T1 - The effect of object shape and laser beam shape on LIDAR system resolution
AU - Cheng, Hongchang
AU - Wang, Jingyi
AU - Ke, Jun
N1 - Publisher Copyright:
© 2016 SPIE.
PY - 2016
Y1 - 2016
N2 - In a LIDAR system, a pulsed laser beam is propagated to a scene, and then reflected back by objects. Ideally if the beam diameter and the pulse width are close to zero, then the reflected beam in time domain is similar to a delta function, which can accurately locate an object's position. However, in a practical system, the beam has finite size. Therefore, even if the pulse width is small, an object shape will make the reflected beam stretched along the time axis, then affect system resolution. In this paper, we assume the beam with Gaussian shape. The beam can be formulated as a delta function convolved with a shape function, such as a rectangular function, in time domain. Then the reflected beam can be defined as a system response function convolved with the shape function. We use symmetric objects to analyze the reflected beam. Corn, sphere, and cylinder objects are used to find a LIDAR system's response function. The case for large beam size is discussed. We assume the beam shape is similar to a plane wave. With this assumption, we get the simplified LIDAR system response functions for the three kinds of objects. Then we use tiny spheres to emulate an arbitrary object, and study its effect to the returned beam.
AB - In a LIDAR system, a pulsed laser beam is propagated to a scene, and then reflected back by objects. Ideally if the beam diameter and the pulse width are close to zero, then the reflected beam in time domain is similar to a delta function, which can accurately locate an object's position. However, in a practical system, the beam has finite size. Therefore, even if the pulse width is small, an object shape will make the reflected beam stretched along the time axis, then affect system resolution. In this paper, we assume the beam with Gaussian shape. The beam can be formulated as a delta function convolved with a shape function, such as a rectangular function, in time domain. Then the reflected beam can be defined as a system response function convolved with the shape function. We use symmetric objects to analyze the reflected beam. Corn, sphere, and cylinder objects are used to find a LIDAR system's response function. The case for large beam size is discussed. We assume the beam shape is similar to a plane wave. With this assumption, we get the simplified LIDAR system response functions for the three kinds of objects. Then we use tiny spheres to emulate an arbitrary object, and study its effect to the returned beam.
KW - Gaussian pulse
KW - LIDAR
KW - Plane pulse
KW - Response function
UR - http://www.scopus.com/inward/record.url?scp=84982285476&partnerID=8YFLogxK
U2 - 10.1117/12.2225197
DO - 10.1117/12.2225197
M3 - Conference contribution
AN - SCOPUS:84982285476
T3 - Proceedings of SPIE - The International Society for Optical Engineering
BT - Three-Dimensional Imaging, Visualization, and Display 2016
A2 - Javidi, Bahram
A2 - Son, Jung-Young
PB - SPIE
T2 - Three-Dimensional Imaging, Visualization, and Display 2016 Conference
Y2 - 18 April 2016 through 20 April 2016
ER -