DEVICE FOR THE TWO-DIMENSIONALLY SCANNING BEAM DEFLECTION OF A LIGHT BEAM

Abstract

A device for two-dimensionally scanning beam deflection of a light beam has spectrally tunable light source that emits a light beam having a time-varying wavelength. The device further comprises a first optical component that produces a first beam deflection. The first beam deflection causes the light beam to be deflected wavelength-dependently in a first direction. A second optical component produces a second beam deflection which causes the light beam to be deflected in a second direction different to the first direction. The second optical component comprises a prism pair comprising two prisms that are rotatably arranged successively in a beam path of the light beam. The two prisms are configured to perform continuous counter-rotational movements.

Claims

1. A device for two-dimensionally scanning beam deflection of a light beam, comprising at least one spectrally tunable light source configured to emit a light beam having a time-varying wavelength; a first optical component configured to produce a first beam deflection, wherein the first beam deflection causes the light beam to be deflected wavelength-dependently in a first direction; and a second optical component configured to produce a second beam deflection, wherein the second beam deflection causes the light beam to be deflected in a second direction different to the first direction, wherein the second optical component comprises a prism pair comprising two prisms that are rotatably arranged successively in a beam path of the light beam, and wherein the two prisms are configured to perform continuous counter-rotational movements.

2. The device of claim 1, wherein the first optical component comprises a grating.

3. The device of claim 1, wherein the first optical component comprises a grating prism.

4. The device of claim 1, wherein the two prisms are achromatic prisms.

5. The device of claim 1, wherein the second direction is perpendicular to the first direction.

6. The device of claim 1, wherein the second optical component is arranged after the first optical component along a light propagation direction of the light beam.

7. The device of claim 1, wherein the spectrally tunable light source is configured to simultaneously emit a multiplicity of light beams each having a time-varying wavelength.

8. The device of claim 1, comprising a polarizer.

9. A LIDAR system for a scanning distance determination of an object, the system comprising a spectrally tunable light source configured to emit a light beam having a time-varying wavelength, an evaluation unit configured to determine a distance of the object on the basis of measurement signals originating from the light beam and reflected at the object and reference signals not reflected at the object; and the device of claim 1.

10. A device for two-dimensionally scanning beam deflection of a light beam, comprising at least one spectrally tunable light source configured to simultaneously emit a multiplicity of light beams each having a time-varying wavelength, a first optical component configured to produce a first beam deflection, wherein the first beam deflection causes the light beams to be deflected wavelength-dependently in a first direction; and a second optical component configured to produce a second beam deflection, wherein the second beam deflection causes the light beams to be deflected in a second direction different to the first direction, wherein the second optical component comprises a prism pair comprising two prisms that are rotatably arranged successively in a beam path of the light beam.

11. The device of claim 10, wherein the first optical component comprises a grating.

12. The device of claim 10, wherein the first optical component comprises a grating prism.

13. The device of claim 10, wherein the two prisms are achromatic prisms.

14. The device of claim 10, wherein the second direction is perpendicular to the first direction.

15. The device of claim 10, wherein the second optical component is arranged after the first optical component along a light propagation direction of the light beam.

16. The device of claim 10, comprising a polarizer.

17. A LIDAR system for a scanning distance determination of an object, the system comprising a spectrally tunable light source configured to emit a light beam having a time-varying wavelength, an evaluation unit configured to determine a distance of the object on the basis of measurement signals originating from the light beam and reflected at the object and reference signals not reflected at the object; and the device of claim 10.

18. A device for two-dimensionally scanning beam deflection of a light beam, comprising at least one spectrally tunable light source configured to emit a light beam having a time-varying wavelength; a first optical component configured to produce a first beam deflection, wherein the first beam deflection causes the light beam to be deflected wavelength-dependently in a first direction; and a second optical component configured to produce a second beam deflection, wherein the second beam deflection causes the light beam to be deflected in a second direction different to the first direction, wherein the second optical component comprises a prism pair comprising two achromatic prisms that are rotatably arranged successively in a beam path of the light beam.

19. The device of claim 18, wherein the first optical component comprises a grating.

20. The device of claim 18, wherein the first optical component comprises a grating prism.

21. The device of claim 18, wherein the second direction is perpendicular to the first direction.

22. The device of claim 18, wherein the second optical component is arranged after the first optical component along a light propagation direction of the light beam.

23. The device of claim 18, comprising a polarizer.

24. A LIDAR system for a scanning distance determination of an object, the system comprising a spectrally tunable light source configured to emit a light beam having a time-varying wavelength, an evaluation unit configured to determine a distance of the object on the basis of measurement signals originating from the light beam and reflected at the object and reference signals not reflected at the object; and the device of claim 18.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0033] Further features and advantages of the invention will become apparent from the fol-lowing description of exemplary embodiments with reference to the drawings, in which

[0034] FIGS. 1-4 show schematic representations to explain different embodiments of the invention; and

[0035] FIGS. 5a-5b show schematic representations to explain the structure and mode of action of a device for distance determination.

DETAILED DESCRIPTION OF EMBODIMENTS

[0036] The basic possible structure and the functionality of a device according to the invention for two-dimensionally scanning beam deflection will be described below with the aid of different embodiments with reference to the schematic drawings of FIG. 1-4.

[0037] The device according to the invention has at least one light source, which is spectrally tunable (i.e. it is variable in terms of the wavelength of the emitted light), for emitting at least one light beam with a time-varying wavelength. In further embodiments, a plurality of light beams with a different wavelength or a different tuning range may also be provided for the purpose of time-parallelization of the scanning process, which may in turn be carried out by using a plurality of light sources or alternatively also by generating a frequency comb.

[0038] A common feature of the embodiments described below is that—for the two-dimensionally scanning beam deflection of at least one light beam with a time-varying wavelength produced respectively by a spectrally tunable light source—at least two separate optical components (respectively causing beam deflections in a mutually different direction) are used. In this case, one of these beam deflections takes place wavelength-dependently (for example via a grating or grating prism), the other of these beam deflections being caused by means of a prism pair consisting of prisms rotatably arranged successively in the beam path. In this case, a periodic variation of the deflection angle in the relevant direction—different to the beam deflection of the first optical component—is induced in the latter prism pair in particular by means of a continuous counter-rotational movement of the prisms, which does not require any acceleration or to and fro movement of the prisms, i.e. effectively a continuous rotational movement of the prisms is converted into a periodic scanning movement of the respective measurement beam.

[0039] FIG. 1a-1d and FIG. 2a-2d show schematic representations to explain a first embodiment. In this case, light of a spectrally tunable light source (not represented in FIG. 1-2) strikes first the first component, which is denoted by “110” and in the exemplary embodiment is configured as a (stationary) grating prism, and then the second component denoted by “120” and formed by the aforementioned prism pair.

[0040] The representations of FIG. 1a-1d respectively show the arrangement in plan view (i.e. in the x-z plane in the coordinate system indicated) and for different rotation angles of the counter-rotating prisms of the component 120, the position according to FIG. 1a corresponding to a rotation angle of 0°, the position according to FIG. 1b corresponding to a rotation angle of 90°, the position according to FIG. 1c corresponding to a rotation angle of 180° and the position according to FIG. 1d corresponding to a rotation angle of 270°. In this case, the counter-rotating prisms of the component 120 in the embodiment shown are rounded prisms.

[0041] FIG. 2a-2d show similar representations for the side view (i.e. in the y-z plane in the coordinate system indicated), again the position according to FIG. 2a corresponding to a rotation angle of 0°, the position according to FIG. 2b corresponding to a rotation angle of 90°, the position according to FIG. 2c corresponding to a rotation angle of 180° and the position according to FIG. 2d corresponding to a rotation angle of 270°.

[0042] The two-dimensional beam deflection is achieved during operation of the device of FIG. 1-2 on the one hand by the wavelength of the light source being tuned (which leads to the beam deflection schematically indicated in FIG. 2a-2d by means of the first component 110, or the grating prism, in the y-z plane) and on the other hand by a continuous counter-rotational movement of the two prisms of the second component 120 taking place (which leads to the beam deflection schematically indicated in FIG. 1a-1d in the x-z plane).

[0043] It is essential for the functional principle in this case that, in respect of the beam deflection taking place according to FIG. 1a-1d in the x-z plane, the first component 110, or the grating prism, does not itself cause any beam deflection, so that in this regard the beam deflection is based only on the second component 120 (i.e. the prism pair).

[0044] Conversely, for the beam deflection taking place according to FIG. 2a-2d in the y-z plane, which is caused as a result of the wavelength tuning by the first component 110, or the grating prism, the second component 120, or the prism pair, effectively appears essentially at any time as a plane plate (with a time-varying diameter because of the rotation) and therefore itself causes no beam deflection in the sense of a deflection angle in this direction, or in the y-z plane (possibly only a side offset of the ray bundle, which is generally noncritical but may also be corrected computationally, is caused).

[0045] The order selected for the optical components 110, 120 in the embodiment of FIG. 1-2 is advantageous on the one hand insofar as the angles of incidence of the light existing for the first component 110, or the grating prism, remain unchanged independently of the rotation angle of the prisms, and on the other hand the lateral dimensions of the grating prism can also be minimized because of the placement at the light entry in the overall arrangement consisting of the first and second components.

[0046] The invention is not, however, restricted to the order described above. In this regard, FIG. 3a-3c and FIG. 4a-4c show similar representations of a further possible embodiment with a correspondingly interchanged order, so that light generated by the tunable light source and striking the arrangement in this case strikes first the second optical component 320 (i.e. the prism pair) and only then the first optical component 310 (or the grating prism).

[0047] The representations of FIG. 3a-3c respectively show the arrangement in plan view (i.e. in the x-z plane in the coordinate system indicated) and for different rotation angles of the counter-rotating prisms of the component 320, the position according to FIG. 3a corresponding to a rotation angle of 0°, the position according to FIG. 3b corresponding to a rotation angle of 90° and the position according to FIG. 3c corresponding to a rotation angle of 180°.

[0048] The prisms of the component 320 may (without the invention being restricted thereto) for example be made of borosilicate crown glass (for example the glass material commercially available under the designation BK7® from Schott). The wedge angle of the prism pair forming the component 320 is 10° in the exemplary embodiment, the resulting deflection angle varying between −17° and +17°. Furthermore, in the exemplary embodiment (but without the invention being restricted thereto), the first optical component 310, or the grating prism, is made of silicon (Si), the grating period being 413.2 nm (corresponding to a line density of 2420 lines/mm).

[0049] FIG. 4a-4c show similar representations for the side view (i.e. in the y-z plane in the coordinate system indicated), again the position according to FIG. 4a corresponding to a rotation angle of 0°, the position according to FIG. 4b corresponding to a rotation angle of 90° and the position according to FIG. 4c corresponding to a rotation angle of 180°.

[0050] The form of the first optical component 110 or 310 selected in the above-described embodiments of FIG. 1 to FIG. 4 as a (high-grade-dispersive) grating prism is particularly advantageous insofar as the tuning range, which is required for the two-dimensional scanning process, of the at least one light source may be relatively small. On the one hand, this takes account of the fact that the wavelength range usable to this extent in the region of a typical working wavelength of 1500 nm is relatively small with a view to the transmission properties to be ensured, and so an already significant variation of the deflection angle with a small wavelength change is desirable. In the aforementioned exemplary embodiment, the dispersion of the first optical component 310, or of the grating prism, gives a change in the deflection angle by about 0.30° for a wavelength change by 1 nm at a wavelength of 1530 nm, a change in the deflection angle by about 0.24° for a wavelength change by 1 nm at a wavelength of 1580 nm and a change in the deflection angle by about 0.21° for a wavelength change by 1 nm at a wavelength of 1625 nm.

[0051] On the other hand, with corresponding minimization of the tuning range of the light source because of the use of a high-grade-dispersive grating prism, the possibly undesired effect of a wavelength dependency of the beam deflection on sides of the second component 120 or 320, or of the prism pair, which would in principle lead to a trapezoidal image field, can be kept small.

[0052] In this case, a “high-grade-dispersive grating prism” is intended to mean a grating prism in which the change in the deflection angle when detuning the wavelength by 1 nm is at least 0.1°, in particular at least 0.2°, more particularly at least 0.3°.

[0053] In further embodiments, instead of a single grating, an arrangement of a plurality of gratings on sides of the first (i.e. “wavelength-dependently operating”) optical component may be used in order to increase the angle deflection or extend the achievable angle range of the angle deflection.

[0054] The two-dimensionally scanning beam deflection according to the invention may be used in an exemplary, advantageous application in a LIDAR system on the basis of the conventional structure described with the aid of FIG. 5a-5b (with corresponding configuration of the scanning device 55 with the arrangement according to the invention consisting of the first optical component and the second optical component).

[0055] The invention is not, however, restricted to this application, but may very generally be carried out advantageously in applications in which rapid two-dimensional beam deflection is desired.

[0056] Although the invention has been described with the aid of particular embodiments, many variations and alternative embodiments are available to the person skilled in the art, for example by combining and/or interchanging features of individual embodiments. Correspondingly, the person skilled in the art will understand that such variations and alternative embodiments are included by the present invention and the range of the invention is restricted only in the sense of the appended patent claims and their equivalents.