• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
  • 同族专利
  • 引用文献
  • 法律状态
  • 优先权
    • 专利摘要:
    In a method for controlling a motor vehicle headlight, the motor vehicle headlight at least comprising a laser diode (1) and a light conversion element (8) associated with the laser diode (1), areas of the light conversion element (8) corresponding to different regions of the light image (11 ') being separated by a light beam (8). 2) of the laser diode (1) can be illuminated periodically and with different intensity, wherein the illumination intensity in the regions of the light conversion element (8) corresponding to the different regions of the light image (11 ') is determined both by the relative illumination duration of the different regions and by different light intensities The laser diode (1) is set in the regions of the light conversion element (8) corresponding to the different regions of the light image (11 ') in regions in which the light beam (2) has an angular velocity below a defined value for the angular velocity is moved, only turning off and turning on the laser diode (1) and are set above a defined value for the angular velocity different light intensities of the laser diode (1). The motor vehicle headlight according to the invention has an arithmetic unit (4) for carrying out the method according to the invention.
    公开号:AT517957A4
    申请号:T51093/2015
    申请日:2015-12-22
    公开日:2017-06-15
    发明作者:Mitterlehner Thomas；Koller Jan；Weber Emanuel；Schantl Patrik
    申请人:Zkw Group Gmbh；
    IPC主号:
    专利说明:

    Method for controlling a motor vehicle headlight
    The invention relates to a method for controlling a motor vehicle headlamp, the motor vehicle headlamp comprising at least a laser diode and a light conversion element associated with the laser diode, wherein corresponding regions of the light conversion element of a light beam of the laser diode periodically and with different intensity can be illuminated in different areas of the light image, wherein the illumination intensity in the the regions of the light conversion element corresponding to different regions of the light image are set simultaneously by both the relative illumination duration of the different regions and by different light intensities of the laser diode in the regions of the light conversion element corresponding to the different regions of the light image and the relative illumination duration in the different regions of the light image corresponding areas of the light conversion element s different Quick pivoting of the light beam is achieved. Furthermore, the invention relates to a motor vehicle headlamp with at least one adjustable in light intensity laser diode, the laser beam is steerable to a light conversion element to generate a luminous image on this, which is projected via an imaging system as a light image on the road, and a deflection mirror of the light scanner accordingly fixed control characteristics in at least one coordinate direction is pivotable, as well as with a laser driver and a computing unit associated therewith.
    Various types of vehicle headlamps are known in the prior art, with headlamps having discharge lamps and halogen light sources being used predominantly in recent years. For energy saving reasons and to further reduce the footprint of vehicle headlights, the use of Laserdio is increasingly being tested as semiconductor lasers, since they are advantageous in this regard. In order to make the laser light usable for a vehicle headlight, a light conversion element, a so-called phosphor converter, is irradiated with a laser diode, which is thereby excited to emit visible light. The phosphorus converter can be opaque in this case, in which case the laser light is directed onto the emission side of the phosphorus converter. Alternatively, the light conversion element may be transmissive
    Be type in which the laser beam is directed to the back of the phosphor converter and emitted on the other side, the emission side, as converted light.
    In so-called static systems, the laser beam is directed immovably to the phosphorus converter. In contrast, in the so-called dynamic system, the laser beam or the laser beams, which are used to excite the phosphorus converter, moved by means of oscillating mirrors on the phosphorus converter, so that the eye creates a light image, which is the outer shape of the phosphor Converter or the illuminated by the laser beam areas of the light conversion element corresponds. The laser beam thus sweeps over the light conversion element, which emits light in the visible range in the currently irradiated area, wherein due to the relatively high scanning speed of the laser beam, the human eye perceives a continuous glow and no flicker or flicker is recognizable. The light of the light conversion element is emitted by reflectors and / or lens systems in front of the vehicle. As a result, certain light functions or precise light-dark boundaries of the light functions such as high beam, low beam and the like can be achieved.
    For the realization of complex light images and in particular for the realization of dynamic light functions such as, for example, adaptive high beam, the light image is constructed from a plurality of different discrete areas, so-called pixels, in which different illumination intensities can be realized. The different illumination intensities result from differently intense illumination or irradiation of the light conversion element in the different regions of the light conversion element corresponding to the pixels of the light image, the pixels of the light conversion element, said reflectors and / or lens systems serving to correspondingly focus the different discrete regions of the light conversion element in the area in front of the vehicle.
    In principle, in order to achieve different illumination intensities in the light conversion element, two possibilities are available. On the one hand, the light intensity of the laser diode can be adjusted differently depending on the pixel which, due to the current position of the oscillating deflection mirror, is currently being irradiated or irradiated with the light of the laser diode. In this method, usually only a few steps of the light intensity of the laser diode control technology provided. For example, the laser diode may be operated at 0%, 50% or 100% of the maximum light intensity of the laser diode, depending on its position. In most cases, however, a much higher number of different levels of brightness in the photo is needed to meet the requirements of modern automotive technology. For example, 256 brightness levels are desirable, for which 256 brightness levels of the laser diode would have to be adjustable in this first possibility, but this is not practical in practice because of the control engineering complexity associated with an increasing number of possible brightness levels of the laser diode and due to increasing power losses. This can already be achieved with two brightness levels of the laser diode according to the second possibility, provided that it is possible to set the relative illumination duration of the light conversion element by the laser beam in the different regions or pixels of the light conversion element in, for example, 256 steps. This can be done on the one hand by light pulses of the laser diode when sweeping the pixel, so that the pixel, for example. Only half of the time is irradiated (resulting in 50% luminous intensity perceptible by the human eye) or the scanning period of the laser beam is small enough, i. The scanning frequency of the laser beam is chosen to be high enough to be able to adjust the different relative irradiation time in the individual pixels due to the large number of repetitions of the sweeping. The said plurality of repetitions of the sweep or said high sampling frequency refers to a minimum frequency or basic period of the light image structure which also applies to pixels with the lowest brightness level, which then results if the corresponding pixel is also at a multiple sampling frequency of the laser beam other pixels are irradiated with only one light pulse, it must be ensured to ensure a uniform, flicker-free light image to the human eye. For example, such fundamental period is 1/200 second, in which case the minimum frequency is 200 Hz (Hertz). Doubling the sampling frequency in this case means that all the pixels can be irradiated at a frequency of 400 Hz, i. the laser beam can within the basic period of 1/200 sec. paint over each pixel twice. If the pixel is also illuminated twice, resulting in 100% brightness, the pixel is illuminated only once, resulting in 50% brightness. In other words, in addition to the possibility of not illuminating the pixel at all (the pixel remains dark), two levels of relative illumination duration are possible.
    To achieve the stated high number of brightness levels, both methods have their limitations, since, firstly, when dimming a laser diode, i. When setting a plurality of different light outputs to relatively high power losses and thus to large heat generation, as already stated above. On the other hand, it is not possible to generate laser pulses sufficiently short and accurate in order to achieve the stated high number of brightness levels exclusively on the basis of the relative illumination duration. Furthermore, repeating the sweep in a period can not be multiplied indefinitely because here the deflection systems, usually the already mentioned oscillating mirror would reach its mechanical limits. Another possibility of setting the relative illumination duration is to achieve a different speed pivoting of the light beam in the corresponding areas of the light image portions of the light conversion element by the light beam of the laser diode is pivoted at different speeds, resulting in a different residence time of the light spot of the laser beam results in the individual areas. Where the light distribution should be bright, the laser spot is moved at a slower speed than where the light distribution is supposed to be relatively dark. This type of adjustment of the relative illumination duration of the individual pixels is the subject of the present invention, since at high scanning speeds the demands on the switching frequency of the laser diode are increased by a multiple. On the other hand, a pure switching of the laser diode, in terms of switching on and off of the laser diode due to higher efficiency at low scan speeds, and thus low switching frequency, preferred. It is only at higher scanning speeds or switching frequencies that better properties with regard to the electromagnetic shielding of corresponding circuits make it advantageous to set different light intensities of the laser diode in the sense of dimming the laser diode.
    The present invention is therefore based on the object as far as possible to eliminate the disadvantages of said switching modes of the laser diode as a function of the speed of pivoting of the light beam of the laser diode.
    To achieve this object, the method according to the invention is developed on the basis of a method of the type mentioned in that in areas where the light beam is moved at an angular velocity below a defined value for the angular velocity, only turning off and turning on the laser diode takes place and above a defined value for the angular velocity different light intensities of the laser diode can be set. In order to obtain a large number of brightness levels, according to the present invention, the effects of controlling the illumination intensity by controlling the relative illumination duration are combined with those of controlling the illumination intensity by controlling the light levels of the laser diode. Each halving of the sampling period leads to a doubling of the brightness levels which can be represented solely by the achievable different relative illumination duration of the regions of the light conversion element corresponding to the different regions of the light image, as well as any doubling of the number of adjustable light intensities of the laser diode to a doubling of the achievable ones Brightness levels leads. In this way, the disadvantages of the two types of generation of different brightness levels mentioned can be kept low. Table 1 shows how each doubling of the sampling frequency relative to the fundamental period brings about a doubling of the displayable brightness levels.
    Table. 1
    In principle, the light beam of the laser diode can be guided along any desired pattern over the light conversion element. According to a preferred variant of the present invention, however, the procedure is such that the light conversion element is illuminated by the light beam of the laser diode along lines and / or columns, whereby an efficient light guide is achieved which allows the highest possible scanning speeds.
    Preferably, the light beam is moved back and forth along the rows and / or columns, so that no idling of the deflection mirror is necessary to return to the starting point after passing through a period. When the light beam is moved back and forth, the peripheral pixels may be illuminated very briefly in succession when the light beam is reversed, but subsequently only with a long time interval until the light beam has traveled to the other edge and back again. In order to take this circumstance into account and to avoid extreme cases, it may therefore be preferred that light pulses required to obtain the relative illumination duration are emitted in a pixel not in succession but distributed over a basic period.
    Preferably, the procedure is such that the light beam of the laser diode is directed by means of a movable deflection mirror on the light conversion element, although any other form of deflection of the light beam of the laser diode, such as. With the aid of movable prisms is conceivable.
    In particular, the deflection mirror is part of a MEMS micro-scanner, as corresponds to a preferred embodiment of the present invention. MEMS micro-scanners are characterized by the precise realizability of high sampling frequencies, which in connection with the present invention is advantageous for achieving a plurality of brightness levels.
    Alternatively, however, the deflection mirror may be driven electromagnetically, as corresponds to a preferred embodiment of the present invention.
    According to a preferred embodiment of the present invention, at least three light intensities, in particular 100%, 50% and 0% of the maximum light intensity of the laser diode are adjustable on the laser diode.
    In the method according to the invention, the procedure is preferably such that the defined value for the angular velocity is between 4000 ° / sec. and 8000 ° / sec., in particular between 5000 ° / sec. and 7000 ° / sec., in particular 6000 ° / sec. is selected. In particular, the value of 6000 ° / sec. has been found to be relevant in practice since, starting from this value, the problems of electromagnetic shielding in the control of the laser diode for generating the fast high-speed pulses corresponding to the fast scan speed compared to the higher-frequency range setting of different luminous intensities, i. Dimming the laser diode, take over.
    Starting from a motor vehicle headlight of the type mentioned at the beginning, the motor vehicle headlight according to the invention is characterized in that the arithmetic unit is set up to carry out the method just described.
    The inventive method will be explained with reference to the figures in the drawing. In this show
    1 shows the essential components of a motor vehicle headlight for applying the method according to the invention,
    2 shows an illustration of a method for controlling a motor vehicle headlight, in which the illumination intensity is set by changing the intensity of the laser diode,
    3a-3b are illustrations of non-inventive methods in which the illumination intensity is set by the relative illumination duration of the different regions;
    4 shows an illustration of the differently fast pivoting of the light beam, and FIG. 5 shows an example of defined values in which, according to the invention, the modulation mode of the laser diode changes.
    With reference to Fig. 1, an embodiment of the invention will now be explained in more detail. In particular, the important parts for a headlight according to the invention are shown, it being understood that a motor vehicle headlamp contains many other parts that allow its meaningful use in a motor vehicle, in particular a car or motorcycle. The lighting starting point of the headlamp is a laser diode 1, which emits a laser beam 2, and which is associated with a laser driver 3, said driver 3 for power supply and for monitoring the laser emission or e.g. is used for temperature control and is also set up to modulate the intensity of the emitted laser beam. By "modulating" in the context of the present invention is meant that the intensity of the laser diode can be changed, whether continuous or pulsed, in the sense of switching on and off. It is essential that the light output can be changed, depending on the angular position at which a later described in more detail mirror is. In addition, there is the possibility of switching on and off for a certain time. An example of a dynamic driving concept for forming an image by a scanning laser beam is described, for example, in Applicant's document AT 514633. The drive signal of the laser diode 1 is denoted by Us.
    The laser driver 3 in turn receives signals from a central processing unit 4, which sensor signals sl, si, sn can be supplied. These signals can on the one hand, for example, switching commands for switching from high beam to low beam or on the other hand, signals that are taken, for example, from sensors Sl ... Sn, such as cameras, which capture the lighting conditions, environmental conditions and / or objects on the road. Also, the signals may originate from vehicle-vehicle communication information. The arithmetic unit 4 drawn here schematically as a block can be contained completely or partially in the headlight and serves in particular also for carrying out the method of the invention described below.
    The laser diode 1 emits, for example, blue or UV light, wherein the laser diode is followed by a collimator optics 5 and a focusing optics 6. The design of the optics depends, inter alia, on the type, number and spatial placement of the laser diodes used, on the required beam quality and on the desired laser spot size at the light conversion element.
    The focused or shaped laser beam 2 'arrives at a light scanner 7 and is reflected by a deflection mirror 10 onto a light conversion element 8, which in the present example is designed as a light-emitting surface and which is used, for example. has a phosphor for light conversion in a known manner. For example, the phosphor converts blue or UV light into "white" light. By "phosphorus" in the context of the present invention is generally understood a substance or mixture of substances which converts light of one wavelength into light of another wavelength or of a wavelength mixture, in particular "white" light, which is termed "wavelength conversion". is subsumed.
    One uses luminescent dyes, wherein the output wavelength is generally shorter and thus more energetic than the emitted wavelength mixture. The desired white light impression is created by additive color mixing. In this case, "white light" is understood as meaning light of such a spectral composition which causes the color impression "white" in humans. Of course, the term "light" is not limited to radiation visible to the human eye. For example, optoceramics are suitable for the light conversion element, these are transparent ceramics, such as YAG: Ce (an yttrium-aluminum garnet doped with cerium).
    It should be noted at this point that in the drawing the light conversion element 8 is shown as a phosphor surface on which the scanning laser beam 2 or scanning laser beams produce an image projected from this side of the phosphor. However, it is also possible to use a translucent phosphor in which the laser beam 2, coming from the side facing away from the projection lens, produces an image, but the emission side is located on the side of the light conversion element facing the projection lens. Thus, both reflective and transmissive beam paths are possible, and ultimately a mixture of reflective and transmissive beam paths is not excluded.
    The deflecting mirror 10 oscillating about two axes in the present example is controlled by a mirror drive 9 with the aid of driver signals ax, ay and e.g. deflected in two mutually orthogonal directions x, y. The mirror drive 9 is also controlled by the arithmetic unit 4 in order to be able to set the oscillation amplitudes of the deflection mirror 10 as well as its instantaneous angular velocity, wherein asymmetrical oscillation about the respective axis can also be adjustable. The control of deflecting mirrors is known and can be done in many ways, e.g. electrostatic or electrodynamic. In proven embodiments of the invention, the deflection mirror 10 pivots in the x-direction about a first axis of rotation lOx and in the y-direction about a second axis of rotation lOy and its maximum deflection leads, depending on its activation, to deflections in the resulting luminous image of, for example, +/- 35 ° in the x-direction and -12 ° to + 6 ° in the y-direction, where the mirror deflections are the halves of these values.
    The position of the deflecting mirror 10 is expediently confirmed by means of a position signal pr to the mirror drive 9 and / or to the arithmetic unit 4. It should be noted that other beam deflecting means, such as e.g. movable prisms can be used, although the use of a deflecting mirror is preferred.
    The laser beam 6 thus scans across the light conversion element 8, which is generally flat, but need not be flat, and produces a luminous image 11 with a predetermined light distribution. This light image 11 is now projected onto the roadway 13 with an imaging system 12 as a light image 11 '. In this case, the laser diode is pulsed or driven continuously at high frequency, so that according to the position of the deflecting mirror 10 arbitrary light distributions are not only adjustable - for example, high beam / low beam - but also quickly changeable, if this requires a special terrain or road situation, such as pedestrians or oncoming vehicles are detected by one or more of the sensors Sl ... Sn and accordingly a change in the geometry and / or intensity of the light image 11 'of the road illumination is desired. The imaging system 12 is shown here in simplified form as a lens.
    The term "roadway" is used here for a simplified representation, because of course it depends on the local conditions whether the photograph 11 'is actually located on the roadway or extends beyond it. "In principle, the image 11' corresponds to a projection onto a vertical one Area in accordance with the relevant standards relating to automotive lighting technology.
    In Fig. 2 and other figures, the lighting scheme is now shown on the light conversion element 8 simplified for only three pixels. In FIG. 2, the different regions or pixels of the light conversion element 8 corresponding to the different regions of the light image are periodically with a period duration of 1/200 sec. The laser diode is scanned for light intensity in the different pixels, i. within the period of 1/200 sec. is set differently, i. the illumination intensity in the different areas is set by different light intensity. In the example shown in FIG. 2, a luminous intensity of 25% of the maximum light intensity of the laser diode 1 in pixel 1, a luminous intensity of 100% of the maximum luminous intensity of the laser diode 1 in pixel 2 and a luminous intensity of 75% of the maximum luminous intensity of pixel 3 Laser diode 1 is set, which settings remain in the multiple, in this example, four times scanning the light conversion element 8. Overall, Pixel 1 results in 25% brightness, Pixel 2,100% brightness and Pixel 3 75% brightness.
    FIGS. 3a and 3b show various possibilities for setting the illumination intensity by the relative illumination duration of the different regions. In FIG. 3 a, the different regions or pixels of the light conversion element 8 corresponding to the different regions of the light image are also periodically also with a period duration of 1/200 sec. scanned, wherein the laser diode is adjustable only between 0% and 100% of the maximum light intensity of the laser diode. In order to achieve an illumination intensity corresponding to the example from FIG. 2, however, pixel 1 is irradiated only in 25% of the time in which the laser beam passes through pixel 1. Pixel 2 is irradiated for 100% of the turnaround time and pixel 3 for 75% of the turnaround time. This can be seen in FIG. 3 a because the light intensity drops to 0% of the maximum light intensity of the laser diode 1 after 25% of the passage from pixel 1, remains at 100%% of the maximum light intensity of the laser diode 1 during the passage of pixel 2 and at Pass from pixel 3 to 75% of the pass drops to 0% of the maximum intensity of laser diode 1. For the human eye, relative brightness impressions thus result in the individual pixels, which correspond to the said relative irradiation times. Such a method is called pulse width modulation.
    In Fig. 3b, the pixels are also irradiated in the extent of the relative irradiation times as in the example of Fig. 3a, however, the irradiation takes place here as a fourfold pulse width modulation, resulting in a more homogeneous light image. A period in which all pixels are traversed again measures 1/200 sec., With 4 identical passes being shown. For the human eye, therefore, the individual pixels again result in brightness impressions which correspond to the said relative irradiation times.
    In the diagram of FIG. 4 are Ver wren angle of the light beam 2 of the laser diode 1 is plotted on the ordinate against the angular velocity of the pivoting on the abscissa. It can be seen that in this example the angular velocity is about 1000 ° / sec. at 0 °, that is, when the light beam 2 of the laser diode 1 irradiates a portion of the light conversion means 8 located at the center of the corresponding light distribution 11 '. In contrast, the angular velocity at the edge of the light conversion means 8, which is irradiated in the present example at +/- 6 ° pivoting of the light beam 2 of the laser diode 1, or can be irradiated, up to 40 times higher (here about 36000 ° / sec .). Due to the large differences in speed, the different areas of the light conversion means are irradiated differently long and therefore different intensity, resulting in different relative
    Lighting duration of the different areas leads.
    In the diagram of FIG. 5 is symbolized that according to the present invention, a value for the angular velocity of the pivoting of the light beam 2 of the laser diode has been defined, from that of a pure switching on and off of the laser diode 1 to a more or less continuous control of the laser diode in the sense of setting different light intensities of the laser diode 1, ie is changed to a dimming of the laser diode in order to avoid the above-mentioned problems of modulation of the laser power by switching on and off of the laser diode 1 at high switching frequencies and yet a high resolution of the relative irradiation intensities of
    To achieve light conversion agent.
    权利要求:
    Claims (10)
    [1]
    1. A method for controlling a motor vehicle headlight, the motor vehicle headlight comprising at least a laser diode (1) and a laser diode (1) associated light conversion element (8), wherein different areas of the light image (11 ') corresponding areas of the light conversion element (8) of a light beam ( 2) of the laser diode (1) can be illuminated periodically and with different intensity, wherein the illumination intensity in the regions of the light conversion element (8) corresponding to the different regions of the light image (11 ') is determined both by the relative illumination duration of the different regions and by different light intensities the laser diode (1) in the regions of the light conversion element (8) corresponding to the different regions of the light image (11 ') is set and the relative illumination duration by areas of the light k corresponding to the different regions of the light image (11') Onversionselements (8) different fast pivoting of the light beam is achieved, characterized in that in areas where the light beam (2) is moved at an angular velocity below a defined value for the angular velocity, only turning off and turning on the laser diode (1) takes place and different light intensities of the laser diode (1) are set above a defined value for the angular velocity.
    [2]
    2. The method according to claim 1, characterized in that the light conversion element (8) from the light beam (2) of the laser diode (1) along lines and / or columns is illuminated.
    [3]
    3. The method according to claim 2, characterized in that the light beam (2) along the rows and / or columns is moved back and forth.
    [4]
    4. The method according to claim 3, characterized in that to achieve the relative illumination time required light pulses in the different regions of the light image (11 ') corresponding areas of the light conversion element (8) are distributed distributed over a basic period.
    [5]
    5. The method according to any one of claims 1 to 4, characterized in that the light beam (2) of the laser diode (1) by means of a movable deflection mirror (10) is directed to the light conversion element (8).
    [6]
    6. The method according to claim 5, characterized in that the deflection mirror (10) is part of a MEMS micro-scanner.
    [7]
    7. The method according to claim 5, characterized in that the deflection mirror (10) is electromagnetically driven.
    [8]
    8. The method according to any one of claims 1 to 7, characterized in that at the laser diode (1) at least three different light intensities, in particular 100%, 50% and 0% of the maximum light intensity of the laser diode (1) are adjustable.
    [9]
    9. The method according to any one of claims 1 to 8, characterized in that the defined value for the angular velocity between 4000 ° / sec. and 8000 ° / sec., in particular between 5000 ° / sec. and 7000 ° / sec., in particular 6000 ° / sec. is selected.
    [10]
    10. Motor vehicle headlamp with at least one adjustable in terms of their light intensity laser diode (1), the laser beam (2) scanning a light conversion element (8) is steerable to generate at this a light image (7), which via an imaging system (12) as a light image (11 ') is projected onto the roadway, and a deflection mirror (10) of the light scanner according to fixed control characteristics in at least one coordinate direction is pivotable, and with a laser driver (3) and one of these associated computing unit (4), characterized in that the arithmetic unit (4) is set up to carry out the method according to one or more of the preceding claims.
    类似技术:
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    同族专利:
    公开号 | 公开日
    JP2019501066A|2019-01-17|
    JP6530565B2|2019-06-12|
    AT517957B1|2017-06-15|
    CN108391442B|2020-10-23|
    EP3394505B1|2021-05-26|
    CN108391442A|2018-08-10|
    KR102084566B1|2020-03-04|
    WO2017106894A1|2017-06-29|
    US20190011107A1|2019-01-10|
    KR20180094098A|2018-08-22|
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    法律状态:
    优先权:
    申请号 | 申请日 | 专利标题
    ATA51093/2015A|AT517957B1|2015-12-22|2015-12-22|Method for controlling a motor vehicle headlight|ATA51093/2015A| AT517957B1|2015-12-22|2015-12-22|Method for controlling a motor vehicle headlight|
    EP16822370.9A| EP3394505B1|2015-12-22|2016-12-19|Method for controlling a motor vehicle headlight|
    JP2018533050A| JP6530565B2|2015-12-22|2016-12-19|Method for controlling a car projector|
    CN201680075182.6A| CN108391442B|2015-12-22|2016-12-19|Method for controlling a motor vehicle headlight|
    KR1020187020910A| KR102084566B1|2015-12-22|2016-12-19|Vehicle Headlight Control Method|
    PCT/AT2016/060132| WO2017106894A1|2015-12-22|2016-12-19|Method for controlling a motor vehicle headlight|
    US16/064,252| US10801689B2|2015-12-22|2016-12-19|Method for controlling a motor vehicle headlight|
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