Among the different types of lidar
systems available, the focus of this paper is primarily on the narrow-pulsed ToF
method. There are two types of beam steering in lidar systems:
- Mechanical lidar uses
high-grade optics and a rotating assembly to create a wide (typically
360-degree) FOV. The mechanical aspect provides a high signal-to-noise ratio
(SNR) over a wide FOV, but results in a bulky implementation (although size has
also been shrinking).
- Solid-state lidar has no
spinning mechanical components and a reduced FOV; thus, it costs less. Using
multiple channels at the front, rear and sides of a vehicle and fusing their
data creates an FOV that rivals mechanical lidar.
Solid-state lidars have multiple
implementation methods, including:
- Microelectromechanical systems
(MEMS) lidar. A MEMS lidar system uses tiny mirrors whose tilt angle
varies when applying a stimulus such as a voltage. In effect, the MEMS
substitutes mechanical scanning hardware with an electromechanical equivalent.
The receiver light collection aperture that determines the receive SNR is
typically quite small (a few millimeters) for MEMS. To move the laser beam in
multiple dimensions requires cascading multiple mirrors. This alignment process
is not trivial, and once installed, it is susceptible to shocks and vibrations
typically encountered in moving vehicles. Another potential pitfall with a MEMS-
based system is that automotive specifications start at –40°C, which can be
challenging for a MEMS device.
- Flash lidar. Flash lidar
operation is very similar to that of a standard digital camera using an optical
flash. In flash lidar, a single large-area laser pulse illuminates the
environment in front of it, while a focal plane array of photo detectors placed
in proximity to the laser captures the back-scattered light. The detector
captures the image distance, location and reflected intensity. Since this method
captures the entire scene in a single image compared to the mechanical laser
scanning method, the data capture rate is much faster. In addition, since the
entire image is captured in a single flash, this method is more immune to
vibration effects that could distort the image. A downside to this method is the
presence of retroreflectors in the real-world environment. Retroreflectors
reflect most of the light and back-scatter very little, in effect blinding the
entire sensor and rendering it useless. Another disadvantage to this method is
the very high peak laser power needed to illuminate the entire scene and see far
enough. To comply with eye safety requirements, flash lidar is primarily used in
short- to medium-range detection systems.
- Optical phase array (OPA).
The OPA principle is similar to phased-array radar. In an OPA system, an optical
phase modulator controls the speed of light passing through the lens.
Controlling the speed of light enables control of the optical wave-front shape,
as shown in Figure 2. The top beam is not delayed, while the middle and bottom beams are delayed
by increasing amounts. This phenomenon effectively “steers” the laser beam to
point in different directions. Similar methods can also steer the back-scattered
light toward the sensor, thus eliminating mechanical moving parts.
- Frequency-modulated continuous
wave (FMCW) lidar. While the methods listed so far are based on the ToF
principle using narrow light pulses, FMCW lidar uses a coherent method,
producing brief chirps of frequency- modulated laser light. Measuring the phase
and frequency of the return chirp enables the system to use the Doppler
principle to measure both distance and velocity. The computational load and
optics are simpler with the FMCW method, although the chirp generation adds
complexity. The laser power required for FMCW systems is considerably lower than
what pulsed ToF systems require, making FMCW suitable for very long-range
sensing applications. They also perform well in adverse weather conditions such
as fog, rain and snow.