MATRIX LIGHTING DEVICE WITH TIME OF FLIGHT ESTIMATION
20210253019 · 2021-08-19
Assignee
Inventors
Cpc classification
B60Q1/0023
PERFORMING OPERATIONS; TRANSPORTING
F21S41/663
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F21S41/153
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F21V23/0471
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F21Y2115/10
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
International classification
B60Q1/00
PERFORMING OPERATIONS; TRANSPORTING
F21S41/153
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F21S41/663
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F21V23/04
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
Abstract
The invention proposes a lighting device for a motor vehicle comprising a matrix light source that performs a lighting function within the motor vehicle. The same source is used, together with a photodiode, to estimate the time of flight of captured light pulses initially generated by the matrix source. It becomes possible to detect objects and/or gestures using light in the visible spectrum, and without having to use specific pulse sources dedicated for this purpose.
Claims
1. A lighting device for a motor vehicle comprising a matrix light source having a plurality of electroluminescent semiconductor element-based elementary light sources, the matrix light source being intended to perform at least one lighting function of the motor vehicle, characterized in that the matrix light source is voltage-driven by a supply circuit and comprises a substrate (112) in which a plurality of switch elements are integrated, each switch element being intended to selectively connect at least one elementary source to the supply circuit, the device comprises a detector intended to detect a light signal emitted by one of the elementary light sources and reflected from an object and in that the device comprises a processing unit operationally connected to the switch elements and intended to control the state thereof, and to process a signal detected by the detector, and in that the processing unit is able to generate a delayed copy, delayed by a duration T, of a detected light signal, emitted by the matrix light source and reflected by said object, and a time-of-flight measurement unit configured so as to calculate the time of flight of the emitted light signal between the object and the matrix source so as to be able to estimate the distance to the object.
2. The device as claimed in claim 1, wherein the detector comprises at least one photodiode.
3. The device as claimed in claim 1, wherein the processing unit is configured so as to estimate the distance between the photodiode and said object, using the signal detected by said photodiode.
4. The device as claimed in claim 1, wherein the processing unit comprises a delay line, involved in a constant-fraction discriminator circuit, for generating a delayed copy of a detected light signal, emitted by the matrix source and reflected by said object, and a time-of-flight measurement unit configured so as, on the basis of the signal generated by the constant-fraction discriminator circuit, to determine the time of flight of the emitted light signal between the object and the matrix source.
5. The device as claimed in claim 1, wherein the switch element is connected in series with an elementary light source.
6. The device as claimed in claim 1, wherein the switch element comprises an N-channel MOS metal-oxide gate field-effect transistor whose state is controlled by way of a signal applied to its gate.
7. The device as claimed in claim 1, wherein the thickness of the substrate is between 100 and 800 microns.
8. The device as claimed in claim 1, wherein said supply circuit is integrated into said substrate.
9. The device as claimed in claim 1, wherein the internal series resistances of each of the elementary light sources are identical and between 1 and 100 ohms.
10. The device as claimed in claim 1, wherein the matrix light source comprises a monolithic component in which the semiconductor layers of the elementary light sources are arranged on a common substrate.
11. The device as claimed in claim 1, wherein the luminescent semiconductor element-based elementary sources comprise sources emitting in the blue spectrum, corresponding to wavelengths of between 400 and 490 nm.
12. The device as claimed in claim 1, wherein said light signals comprise pulses having a rise time of less than 20 ns.
13. A method for detecting an object by way of a device as claimed in claim 1, wherein the method comprises the following steps: supplying electricity to the matrix light source, using a control unit to sequentially control the switch elements of each elementary light source, so as to emit a sequence of light signals, each signal being emitted from the location of one of the elementary light sources; using the detector to sequentially detect the light signal respectively reflected by an object; for each emitted light signal, recording an item of data in a memory element, the item of data indicating whether or not an object has been detected at the location illuminated by the corresponding light signal.
14. The method as claimed in claim 13, wherein for each emitted light signal, the processing unit records an item of data additionally indicating an estimate of the distance D between the object detected or not detected at the corresponding location and the detector.
15. The device as claimed in claim 2, wherein the processing unit is configured so as to estimate the distance between the photodiode and said object, using the signal detected by said photodiode.
16. The device as claimed in claim 2, wherein the processing unit comprises a delay line, involved in a constant-fraction discriminator circuit, for generating a delayed copy of a detected light signal, emitted by the matrix source and reflected by said object, and a time-of-flight measurement unit configured so as, on the basis of the signal generated by the constant-fraction discriminator circuit, to determine the time of flight of the emitted light signal between the object and the matrix source.
17. The device as claimed in claim 2, wherein the switch clement is connected in series with an elementary light source.
18. The device as claimed in claim 2, wherein the switch element comprises an N-channel MOS metal-oxide gate field-effect transistor whose state is controlled by way of a signal applied to its gate.
19. The device as claimed in claim 2, wherein the thickness of the substrate is between 100 and 800 microns.
20. The device as claimed in claim 2, wherein said supply circuit is integrated into said substrate.
Description
[0028] Other features and advantages of the present invention will be better understood with the aid of the description of the examples and of the drawings, in which:
[0029]
[0030]
[0031] Unless specified otherwise, technical features that are described in detail for one given embodiment may be combined with the technical features that are described in the context of other embodiments described by way of example and without limitation. Similar reference numerals will be used to describe similar concepts across various embodiments of the invention. For example, the references 100 and 200 denote two embodiments of a device according to the invention.
[0032] The description focuses on the technical elements that are required to understand the invention. Other elements that are well known in the field of lighting devices for motor vehicles and that are not linked directly to the invention will be omitted for the sake of clarity. For example, a lighting device generally comprises an optical system as well as supports for keeping the various components in place, without such details being mentioned explicitly in this description.
[0033] The illustration of
[0034] To create the white light for a lighting function from blue light, use is typically made of a layer of yellow phosphorus or of a quantum dot converter. However, this white light typically has a delay greater than 20 ns, thereby making it unsuitable for the object detection function. The detection system therefore mainly uses blue rays that have not been converted into white light. It is typically estimated that around ⅓ to ½ of the photons from the light source are not converted by the layer of phosphorus.
[0035] The voltage source 130 is produced for example by way of a converter circuit that converts an input voltage Vcc supplied by a battery internal to the motor vehicle into a voltage V suitable for supplying the matrix light source 110. Such converter circuits are known in the art, and their operation will not be described in detail in the context of the present invention.
[0036] The matrix light source 110 is preferably a monolithic component in which the semiconductor layers of the elementary light sources 120 are arranged on a common substrate 112. The matrix light source 110 preferably comprises a parallel assembly of a plurality of branches, each branch comprising electroluminescent semiconductor light sources 120.
[0037] By way of example and without limitation, the matrix light source 110 comprises, along the thickness of the substrate and starting at the end opposite the location of the elementary sources 10, a first electrically conductive layer deposited on an electrically insulating substrate. This is followed by an n-doped semiconductor layer whose thickness is between 0.1 and 2 μm. This thickness is much smaller than that of known light-emitting diodes, for which the corresponding layer has a thickness of the order of 1 to 2 μm. The following layer is the active quantum well layer having a thickness of around 30 nm, followed by an electron-blocking layer, and finally a p-doped semiconductor layer, the latter having a thickness of around 300 nm. Preferably, the first layer is an (Al)GaN: Si layer, the second layer is an n-GaN: Si layer, and the active layer comprises quantum wells made of InGaN alternating with barriers made of GaN. The blocking layer is preferably made of AlGaN:Mg and the p-doped layer is preferably made of p-GaN:Mg. n-doped gallium nitride has a resistivity of 0.0005 ohm/cm, whereas p-doped gallium nitride has a resistivity of 1 ohm/cm. The thicknesses of the proposed layers make it possible in particular to increase the internal series resistance of the elementary source, while at the same time significantly reducing its manufacturing time, as the n-doped layer is not as thick in comparison with known LEDs and requires a shorter deposition time. By way of example, a time of 5 hours is typically required for MOCVD depositions for a standard-configuration LED with 2 μm of n layer, and this time may be reduced by 50% if the thickness of the n layer is reduced to 0.2 μm.
[0038] In order to achieve elementary light sources 120 having semiconductor layers having homogeneous thicknesses, the monolithic component 110 is preferably manufactured by depositing the layers homogeneously and uniformly over at least part of the surface of the substrate so as to cover it. The layers arc deposited for example using a metal oxide chemical vapor deposition (MOCVD) method. Such methods and reactors for implementing them are known for depositing semiconductor layers on a substrate, for example from patent documents WO 2010/072380 A1 or WO 01/46498 A1. Details on their implementation will therefore not be described in the context of the present invention. The layers thus formed are then pixelated. By way of example and without limitation, the layers are removed using known lithographic methods and by etching at the sites that subsequently correspond to the spaces between the elementary light sources 120 on the substrate. A plurality of several tens or hundreds or thousands of pixels 120 having a surface area smaller than one square millimeter for each individual pixel, and having a total surface area greater than 2 square millimeters, having semiconductor layers with homogeneous thicknesses, and therefore having homogeneous and high internal series resistances, are thus able to be produced on the substrate of a matrix light source 110. Generally speaking, the more the size of each LED pixel decreases, the more its series resistance increases, and the more this pixel is able to be driven by a voltage source. As an alternative, the substrate comprising the deposited layers covering at least part of the surface of the substrate is sawn or divided into elementary light sources, each of the elementary light sources having similar characteristics in terms of their internal series resistance.
[0039] The embodiment that has just been described is not limiting, and the invention pertains in the same way to types of semiconductor element-based elementary light sources involving other semiconductor layer configurations. In particular the substrates, the semiconductor materials of the layers, the layout of the layers, their thicknesses and any vias between the layers may be different from the example that has just been described, as long as the structure of the semiconductor layers is such that the internal series resistance of the elementary light source resulting therefrom is at least 1 ohm, and preferably at least 5 or 10 ohms, or else between 1 and 100 ohms.
[0040] Preferably, not only the switch elements 114 but also the supply circuit 130 may be integrated into the substrate 112 when the monolithic component 110 is manufactured.
[0041]
[0042] The profile of the light signal reflected by the object, for example a pulse having a rise time of the order of 1 to 20 ns, 242, is known to the processing means. In principle, the profile is similar to the pulse initially emitted by the matrix source. However, the amplitude of the detected pulse is in practice different from the amplitude of the emitted pulse. A version, delayed by a duration T, of the signal 242 is generated; this is the signal 242′. This is performed for example by way of a delay line 252. Corresponding electronic circuits are known in the art, and will not be described in the context of the present invention. The duration T, counted from the start of the emitted pulse, corresponds to a fraction of the maximum amplitude of the emitted pulse. T is chosen for example to correspond to an amplitude value of the pulse equivalent to 50% of its maximum amplitude. Other choices are possible. A differential amplifier circuit 253 uses, at input, the signal 242 received by the detector and possibly attenuated by a circuit, not illustrated, and the delayed signal 242′. The differential amplifier makes it possible to achieve bipolar shaping of the signal, the zero crossing of which does not depend on the amplitude of the detected signal. This makes it possible to obtain a signal whose timing does not depend on the amplitude of the detected signal. This type of circuit is known in the literature as a CFD “Constant Fraction Discriminator”.
[0043] The amplitude of the signal detected at the time that corresponds to the zero crossing of the signal from the CFD makes it possible to calculate the time of flight of the light pulse. Specifically, at this time, the amplitude of the detected signal has reached the fraction corresponding to the fraction determined by the duration T (for example 50%) of its maximum amplitude. It may then be concluded that the rising edge of the reflected signal has been successfully detected.
[0044] The measurement of the time of flight between the start of the rising edge of the emitted light pulse and the detection of the time at which the signal from the circuit crosses zero using a TAC (time-to-amplitude converter) and/or TDC (time-to-digital converter) device makes it possible to obtain the distance D between an object that reflected the light pulse and the source of the pulse. This makes it possible to detect an object located at the distance D. By using a plurality of signals from the pixelated light source, it is possible to implement detection with finer granularity, and it becomes possible to determine the exact distance at which the object is located. By using digitization of the amplitude corresponding to the time of flight, for example, it becomes possible to determine that the object is located between a distance D1 (corresponding to a signal delayed by a duration T1) and a distance D2 (corresponding to a signal delayed by a duration T2 slightly longer than T1), or the distance difference corresponds to the resolution of the amplitude/time conversion.
[0045] Other implementations of the processing unit 250 and of the delay line 252 and of the detection circuit may be contemplated as long as they make it possible to implement the functionality that has just been described without otherwise departing from the scope of the present invention.
[0046] In all of the embodiments, the plurality of elementary light sources 120 illustrated by
[0047] The scope of protection is defined by the following claims.