Autonomous, self-driving, and semi-autonomous automobiles use a combination of different sensors and technologies such as radar, image-recognition cameras, and sonar for detection and location of surrounding objects. These sensors enable a host of improvements in driver safety including collision warning, automatic-emergency braking, lane-departure warning, lane-keeping assistance, adaptive cruise control, and piloted driving. Among these sensor technologies, light detection and ranging (LiDAR) systems take a critical role, enabling real-time, high-resolution 3D mapping of the surrounding environment.
Most current LiDAR systems used for autonomous vehicles today utilize a small number of lasers, combined with some method of mechanically scanning the environment. Some state-of-the-art LiDAR systems use two-dimensional Vertical Cavity Surface Emitting Lasers (VCSEL) arrays as the illumination source. It is highly desirable for future autonomous cars to utilize solid-state semiconductor-based LiDAR systems with high reliability and wide environmental operating ranges. These systems are advantageous because they have no moving parts and can be highly reliable. However, currently state-of-the-art LiDAR systems have many practical limitations.
The present teaching, in accordance with preferred and exemplary embodiments, together with further advantages thereof, is more particularly described in the following detailed description, taken in conjunction with the accompanying drawings. The skilled person in the art will understand that the drawings, described below, are for illustration purposes only. The drawings are not necessarily to scale; emphasis instead generally being placed upon illustrating principles of the teaching. The drawings are not intended to limit the scope of the Applicant's teaching in any way.
Emitting Laser array for a LiDAR system according to the present teaching.
The present teaching will now be described in more detail with reference to exemplary embodiments thereof as shown in the accompanying drawings. While the present teaching is described in conjunction with various embodiments and examples, it is not intended that the present teaching be limited to such embodiments. On the contrary, the present teaching encompasses various alternatives, modifications and equivalents, as will be appreciated by those of skill in the art. Those of ordinary skill in the art having access to the teaching herein will recognize additional implementations, modifications, and embodiments, as well as other fields of use, which are within the scope of the present disclosure as described herein.
Reference in the specification to “one embodiment” or “an embodiment” means that a particular feature, structure, or characteristic described in connection with the embodiment is included in at least one embodiment of the teaching. The appearances of the phrase “in one embodiment” in various places in the specification are not necessarily all referring to the same embodiment.
It should be understood that the individual steps of the method of the present teaching can be performed in any order and/or simultaneously as long as the teaching remains operable. Furthermore, it should be understood that the apparatus and method of the present teaching can include any number or all of the described embodiments as long as the teaching remains operable.
The present teaching relates to Light Detection and Ranging (LiDAR), which is a remote sensing method that uses laser light to measure distances (ranges) to objects. Autonomous vehicles make use of LiDAR systems to generate a highly accurate 3D map of the surrounding environment with fine resolution. The systems and methods described herein are directed towards providing a solid-state, pulsed time-of-flight (TOF) LiDAR system with high levels of reliability, while also maintaining long measurement range as well as low cost.
In addition, the systems and methods described herein that provide solid-state pulsed TOF LiDAR are also configured to maintain Class 1 eye safety. A Class 1 eye safety rating means the system is safe under all conditions of normal use. To maintain Class 1 eye safety, the laser optical energy or laser optical power cannot exceed a maximum permissible exposure (MPE) level as defined by U.S. and international safety standards. However, the measurement range of a LiDAR system is strongly dependent on the maximum transmitted optical pulse energy or power level. Therefore, it is desirable for automotive LiDAR systems to intentionally operate as close to the Class 1 MPE limit as feasible. Hence, the configuration and layout of the two-dimensional VCSEL array is critical to achieving optimal performance.
Individual lasers in two-dimensional VCSEL array are activated in predetermined sequences to illuminate different points or regions of interest to be measured by the LiDAR system. The resolution and/or field-of-view (FOV) of the system is determined by which lasers are activated in the two-dimensional VCSEL array. It follows then for systems with fine resolution and/or large field-of-view, the number of lasers is very large, and can be in the hundreds or even many thousands of individual lasers. Individually driving very large numbers of lasers in a two-dimensional VCSEL array with separate laser drivers makes the resulting LiDAR transmitter system relatively large, complex and costly.
One feature of the present teaching is the use of matrix-addressing in LiDAR transmitters using two-dimensional VCSEL arrays to reduce the physical size, complexity and cost of the LiDAR transmitter. Using matrix-addressing of the two-dimensional VCSEL array according to the present teaching is desirable because it provides the ability to activate individual lasers without needing an individual laser driver per each laser. With matrix-addressing, the number of laser drivers scales on the order of N+M instead of scaling on order of N*M, where N and M are integer numbers of shared anode and cathode electrical contacts, respectively.
In various embodiments of the LiDAR systems according to the present teaching, the geometry of the two-dimensional VCSEL array and the particular layout of the individual lasers can be improved or optimized based on numerous design constraints including the desired optical output power for each laser, the laser optical efficiency, the maximum laser bias current, the desired size of the individual and total optical emission areas, eye safety power limitations, inductance/impedance of the electrical circuit, RF pulse characteristics, as well as other physical, optical and electrical design constraints. Thus, the present teaching relates, at least in part, to various configurations for matrix-addressable VCSEL arrays specifically configured for solid-state LiDAR system that addresses at least some of these constraints. For example, one aspect of the present teaching is that the matrix-addressable vertical cavity surface emitting laser can be configured so that at least one of the rows of vertical cavity surface emitting lasers has anode connections that allow activating a portion of the vertical cavity surface emitting lasers in the at least one row of vertical cavity surface emitting lasers with a particular bias current so that Class 1 eye safety is maintained if vertical cavity surface emitting lasers in that portion of the row of vertical cavity surface emitting lasers are activated and Class 1 eye safety is exceeded if the entire at least one row of vertical cavity surface emitting lasers is activated. Also, the plurality of vertical cavity surface emitting lasers can each be configured with the common cathode electrical connection on one side of the die with anode connections that allow activating a portion of the vertical cavity surface emitting lasers in a row of vertical cavity surface emitting lasers with a particular bias current so that Class 1 eye safety is maintained if vertical cavity surface emitting lasers in that portion of the row of vertical cavity surface emitting lasers are activated and Class 1 eye safety is exceeded if that entire row of vertical cavity surface emitting lasers is activated.
Wire bonds or other electrical contacts are made between the anodes and cathodes of the lasers and the driver circuit. The physical size of the electrical contact area can be a limiting factor in some designs. A typical contact can be on the order of 250 microns in the widest dimension. Because of the fast rise/fall times involved in pulse operation of state-of-the art LiDAR systems, it is often desirable to have a large electrical contact pad with multiple wire bonds and/or gold ribbon in order to minimize the undesirable inductance of the wire bond and the associated impedance. Larger cross-section wires and/or multiple bonds also result in higher electrical current carrying capacity, which is highly desirable.
The electrical contacts 106 to the VCSEL array 100 at the top and bottom of the matrix-addressable VCSEL array 100 are electrical contacts to the laser anodes, which are p-type semiconductor electrical contact. The electrical contact 108 to the left and right of the matrix-addressable VCSEL array 100 are electrical contacts to the laser cathodes of the matrix, which are the n-type electrical contacts. By appropriately biasing the electrical contacts 106, 108 of each row/column, the individual lasers within the matrix are activated. A controller or processor typically instructs an electrical bias circuit to bias particular row/column locations within the matrix in a predetermined sequence according to the desired operation while simultaneously maintaining eye-safety constraints. In this known VCSEL configuration shown in
In this example array 100, the individually-addressable laser element has sixteen emitters 102 that share a common anode 106 and cathode 108 electrode. The array of the groups of sixteen emitters 102 has a pitch in the vertical dimension that is equal to the pitch of the electrodes 108. The array of groups of sixteen emitters 102 has a pitch in the horizontal dimension that is equal to the pitch of the anode electrodes 106. Thus, the size of an addressable laser element that includes the sixteen emitters is the pitch of the anode emitters times the pitch of the cathode emitters. Because the contact electrode size needs to be large as described herein, new connection approaches are needed so the physical size of the group of laser emitters that is commonly addressed by a contact electrode can be physically smaller than the contact electrode size and/or the spacing between electrodes (pitch).
For example, in the VCSEL configuration shown in
In various embodiments of the present teaching, more individually addressed emitters (lasers 204) are achieved per unit area with more control because each row of emitters has a cathode contact on only one side of the die 202. A row is referred to herein generally as a group of lasers that are individually addressable. For example, in the configuration shown in
The increased number of lasers in a given array size that are individually controlled is achievable because each row of emitters has a cathode contact on only one side of the die 202. That is, by having at least some adjacent rows, e.g. a top row and a bottom row, of emitters connected to a cathode electrode such that the top row is connected on one side of the array and the bottom row is connected on the other side of the array, the two rows become individually addressable. Since a row refers to a group of lasers that are individually addressable, these rows may have a vertical extent of one, two or more lasers, depending on the configuration. Importantly, the pitch of an individually addressable row is not necessarily the same as the pitch of the cathodes, and in particular, the individually addressable rows are more closely spaced than the cathode electrodes.
The electrical contact arrangement described in connection with
Thus, the electrode configuration described in connection with
The optical pitch in the vertical dimension can be expressed as the distance between rows of lasers arrays, for example, the distance between the first row 306 and the second row 310. The optical pitch in the horizontal dimension can be expressed by the distance between columns of the laser arrays, for example, the distance between the first column 322 and the second column 324. Thus, for the configuration described in connection with
In the configuration of
This improvement in the state-of-the art is achieved by connecting both the rows (cathode connections) and the columns (anode connections) on only one side of a die, as opposed to both sides. Thus, in the example embodiment described in connection with
In one embodiment of the present teaching, different pitch ratios can be used along either or both of the vertical or horizontal direction to achieve desired independent control over portions of the entire laser array. For example, lower resolutions (larger groups of individually addressable emitters) can be used on the edges of the overall array and higher resolution (smaller groups of individually addressable emitters) can be used near the center of the overall array. An almost unlimited number of different patterns can be realized based on the size, position, and connection pattern of the electrodes in combination with the individual emitter size and position with respect to the electrodes to which they are connected.
One feature of the present teaching is that the single ended contact configuration can be applied to both anode and cathode electrodes.
One skilled in the art will appreciate that there are numerous other VCSEL array configurations according to the present teaching where, for example, each row of emitters has a cathode contact on only one side of the die and that these configurations can be chosen to achieve various cost and/or performance objectives, such as achieving higher resolution and/or greater field-of-view at particular price points.
Also, it should be understood that the anode driver and the cathode driver design can impact the overall design of the laser array. The two types of drivers often have different costs to implement and these costs often drive the overall design. One feature of the present teaching is that the ability to provide a single-ended electrode for either the laser cathodes or the laser anodes allows the laser array optical and electrical pitch and the driver type to be optimized separately for various cost and/or performance metrics. As just one example, if a VCSEL array has a shape of N*M, where N is not equal to M, one skilled in the art will know how to select the lowest cost driver to drive the larger number of contacts.
While the Applicant's teaching is described in conjunction with various embodiments, it is not intended that the Applicant's teaching be limited to such embodiments. On the contrary, the Applicant's teaching encompasses various alternatives, modifications, and equivalents, as will be appreciated by those of skill in the art, which may be made therein without departing from the spirit and scope of the teaching.
The present application is a non-provisional application of U.S. Provisional Patent Application Ser. No. 62/965,161 entitled “Matrix-Addressable VCSEL for Solid-State LiDAR” filed on Jan. 23, 2020. The entire content of U.S. Provisional Patent Application Ser. No. 62/965,161 is herein incorporated by reference.
Number | Date | Country | |
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62965161 | Jan 2020 | US |