JP2014085519A - Laser light source device and laser projector using laser light source device - Google Patents

Abstract

PROBLEM TO BE SOLVED: To provide a laser light source device capable of enhancing the stability of outgoing beam from a laser light source device using a wavelength conversion element and a small laser projector using the laser light source device.SOLUTION: A laser light source device comprises: a laser element 10; a wavelength conversion element 20 which converts the wavelength of a laser light from the laser element 10; a control circuit 50 which controls the drive of the laser element 10; a detection element 40 which detects outgoing beam from the wavelength conversion element 20. The control circuit 50 includes an oscillation changeover circuit 51 which switches an oscillation state of the laser element 10, while the oscillation changeover circuit 51 switches the laser element 10 to pulse oscillation and continuous oscillation. The detection element 40 detects a conversion wave of the laser light when the laser element 10 is oscillated in pulsed mode, and detects a fundamental wave of the laser light when the laser element 10 is oscillated in continuous mode. The control circuit 50, based on detection information of the fundamental wave and the conversion wave from the detection element 40, controls the drive of the laser element 10.

Description

  The present invention relates to a laser light source device using a wavelength conversion element and a laser projector using the laser light source device.

  Short wavelength laser light sources such as green and blue have been widely developed in fields such as laser projectors and high-density optical storage devices. This short-wavelength laser light source has a method called SHG (Second Harmonic Generation), and uses a wavelength conversion element that converts infrared light of a fundamental wave oscillated by a semiconductor laser into a second harmonic. ing.

  The wavelength conversion element used in this SHG type laser light source device has an optical waveguide whose main component is LN (lithium niobate: LiNbO3), which is a ferroelectric single crystal material, and receives infrared light from the laser element. Incident light is converted into a second harmonic by an optical waveguide, and converted light of green light or blue light is emitted. However, the wavelength conversion element has temperature dependency, and there is a problem that the intensity and wavelength of the converted light fluctuate due to ambient temperature changes.

  In order to solve such a problem, a tunable laser diode is used as a basic light source, a first detection means for detecting the light quantity of the fundamental wave, and a second detector for detecting the light quantity of the converted wave from the wavelength conversion element. There is a proposal of providing two detection means as detection means, controlling the power of the laser element in accordance with the light amount of the fundamental wave, and controlling the wavelength of the laser element in accordance with the light amount of the converted wave (for example, see Patent Document 1). .

  As another proposal, a tunable semiconductor laser is used as a basic light source, and a first detection means for detecting a fundamental wave and a second detection means for detecting a converted wave (second harmonic) are provided. The intensity of the fundamental wave is detected by the control so that the fundamental wave always has a constant output, and the second detection means transmits the converted wave output through the interference filter and enters the output of the second detection means. Accordingly, there is a proposal to stabilize the fluctuation of the wavelength by controlling the injection current to the phase control region of the wavelength tunable semiconductor laser (see, for example, Patent Document 2).

Japanese Patent Laid-Open No. 4-13118 (page 128, FIG. 1) JP-A-6-175175 (5 pages, FIG. 8)

  However, it can be assumed that the conventional laser light source device is a pulse wave whose fundamental wave is output in a pulse form, but the pulse wave has a wide wavelength distribution, so it is difficult to detect with high accuracy and maintains stable oscillation with little fluctuation. It was difficult to do.

  An object of the present invention is to provide a laser light source device that solves the above-described problems and realizes improved stability of emitted light of a laser light source device using a wavelength conversion element, and a laser projector using the laser light source device. It is.

In order to solve the above-described problems, the laser light source device of the present invention and the laser projector using the laser light source device adopt the following configurations.

  The laser light source device of the present invention is a laser light source device having a laser element and a wavelength conversion element that converts and emits the wavelength of the laser light from the laser element, a control unit that controls driving of the laser element, and a wavelength Detecting means for detecting light emitted from the conversion element, the control means includes an oscillation state switching means for switching the oscillation state of the laser element, and the oscillation state switching means continuously changes the oscillation state of the laser element to pulse oscillation. When the laser element is in a pulse oscillation state, the detection means detects a converted wave of the laser beam, and when the laser element is in a continuous oscillation state, the detection means detects the fundamental wave of the laser beam. The detection and control means controls the driving of the laser element based on the detection information of the fundamental wave and the detection information of the converted wave from the detection means.

  The detecting means detects both the converted wave and the fundamental wave with a single detecting element.

  A laser projector according to the present invention includes a laser light source device according to the present invention, a control unit that controls the laser light source device, a scanning unit that scans laser light from the laser light source device horizontally or vertically, and scanning of the laser light. And a shielding unit that shields light whose ratio of the scanning angle to the maximum scanning angle is equal to or greater than a predetermined ratio, and the control unit detects a converted wave from the laser light source device during the horizontal scanning period, and performs vertical scanning. Control is performed so as to detect a fundamental wave from the laser light source device during the period.

  Further, the control means detects the converted wave during the horizontal scanning period while the laser light is shielded by the shielding portion.

  In the laser light source device of the present invention, the fundamental wave can be detected by a continuous wave having a narrow wavelength distribution and a peak wavelength output sufficiently large for detection. It is possible to realize a laser light source device that corrects fluctuations in incident light with high accuracy. Further, by switching between pulse oscillation and continuous oscillation of the laser element, it becomes possible to detect the converted wave and the fundamental wave of the laser beam with one detection element, and it is possible to provide a laser light source device with a minimum configuration including peripheral components.

  In addition, by detecting the conversion wave and fundamental wave separately, it is possible to grasp the deterioration characteristics of the laser element due to changes over time, and the laser that drives the laser element finely and maintains stable oscillation with little fluctuation. A light source device can be provided.

  In addition, the laser projector of the present invention detects a converted wave during a period in which the laser beam is shielded by the shielding portion by horizontal scanning, and detects a fundamental wave during a vertical scanning period of the laser light. As a result, the display image is not adversely affected when the converted wave and the fundamental wave are detected. In addition, since the converted wave and the fundamental wave are separately detected and the change due to the time-dependent change of the laser element and the temperature characteristic is corrected, it is possible to provide a laser projector that always displays a stable and beautiful image.

It is a schematic block diagram of the laser light source apparatus concerning 1st Embodiment. It is typical sectional drawing explaining the structure and operation | movement of a laser element containing the saturable absorber of 1st Embodiment. It is a spectrum figure of the typical laser beam explaining switching operation of the fundamental wave and conversion wave of the laser light source device concerning a 1st embodiment. 5 is a flowchart and a lookup table for explaining a fundamental wave correcting operation of the laser light source device according to the first embodiment. It is a flowchart explaining the conversion wave correction | amendment operation | movement of the laser light source apparatus concerning 1st Embodiment. It is a partial block diagram of the laser light source apparatus of the modification of 1st Embodiment. It is a schematic block diagram of the laser projector concerning 2nd Embodiment. It is explanatory drawing explaining the locus | trajectory of the laser beam projected by the MEMS mirror of the laser projector concerning 2nd Embodiment. 10 is a timing chart for explaining operations of detecting a converted wave and a fundamental wave of a laser beam of a laser projector according to a second embodiment.

Hereinafter, embodiments of the present invention will be described in detail with reference to the drawings.
[Features of each embodiment]
A feature of the first embodiment is a laser light source device including a laser element including a saturable absorber, a wavelength conversion element, a reflection element, and one or two detection elements. A feature of the second embodiment is a MEMS (Micro Electro Mechanical Systems) mirror type laser projector using the laser light source device of the first embodiment.

[Description of Configuration of Laser Light Source Device of First Embodiment: FIG. 1]
The configuration of the laser light source device of the first embodiment will be described with reference to FIG. In FIG. 1, a laser light source device 1 includes a laser element 10, a wavelength conversion element (hereinafter abbreviated as SHG element) 20, and an FBG (Fiber Bragg Grating) type reflection element (hereinafter abbreviated as FBG element) which is a reflection element. ) 30, a detection element (hereinafter abbreviated as PD) 40 as detection means, and a control circuit 50 as control means.

  The laser element 10 includes a saturable absorber (hereinafter abbreviated as SA) 12 together with a laser diode (hereinafter abbreviated as LD) 11. A common electrode of the LD 11 and SA 12 is a cathode electrode 10a and is connected to 0V. The LD electrode 11a, which is a terminal of the LD 11, is connected to a drive current control circuit of the control circuit 50 described later, and is supplied with a drive current Id. Further, the SA electrode 12a, which is a terminal of the SA12, is connected to an oscillation switching circuit of the control circuit 50 described later, and a bias voltage Vb is applied thereto.

  The laser element 10 emits a fundamental wave mode for emitting a fundamental wave laser beam LS1 (hereinafter abbreviated as a fundamental wave LS1) that is a continuous wave and a pulse wave LS2 that oscillates in a pulsed manner by switching the bias voltage Vb. It has two modes, the pulse wave mode to The operation of the laser element 10 will be described later.

  As described above, the SHG element 20 is an optical element that converts laser light of a specific wavelength into a second harmonic, and the SHG element 20 is emitted from the laser element 10 in the fundamental wave mode of the laser element 10. The fundamental wave LS1 is transmitted as it is. In the pulse wave mode, the SHG element 20 transmits part of the pulse wave LS2 emitted from the laser element 10. The SHG element 20 is configured to perform wavelength conversion and emit a second harmonic of the reflected wave when a selective reflected wave from the FBG element 30 described later is incident.

The FBG element 30 is an optical element that reflects only a laser beam having a specific wavelength among incident laser beams as a reflected wave. When the fundamental wave LS1 is transmitted from the SHG element 20 in the fundamental wave mode, the FBG element 30 is reflected. Since the reflected wavelength does not match the wavelength of the fundamental wave LS1, the fundamental wave LS1 is transmitted as it is, and the fundamental wave LS1 is emitted from the FBG element 30 to the outside as the emitted light LS5.

  Further, when the pulse wave LS2 is transmitted from the SHG element 20 in the pulse wave mode, the FBG element 30 has a wide wavelength distribution of the pulse wave LS2 and includes the reflected wavelength component of the FBG element 30. The reflected wave LS3 is fed back to the SHG element 20 side.

  When the SHG element 20 receives the reflected wave LS3 fed back, as described above, a part of the reflected wave LS3 is wavelength-converted internally, but the conversion efficiency depends on the amplitude of the incident wave of the SHG element 20, and this Since the amplitude of the reflected wave is small at the time, most of the reflected wave LS3 returns to the laser element 10. The reflected wave LS3 returned to the laser element 10 is amplified by the wavelength component selected by the FBG element 30 in the gain region of the laser element 10 (not shown), and is subjected to pulse modulation by the saturable absorber portion. It is reflected by the mirror at the end face of and is amplified again in the gain region. As a result, the pulse wave LS2, which has been pulsed and has a high peak value, includes many reflected wavelength components selected by the FBG element 30 and is also coincident with the converted wavelength of the SHG element 20, and is therefore wavelength-converted with high efficiency. The converted wave LS4, which is the second harmonic of the reflected wave LS3, is emitted toward the FBG element 30. The FBG element 30 receives and transmits the converted wave LS4 and emits the converted wave LS4 as outgoing light LS5.

  That is, the laser light source device 1 emits the fundamental wave LS1 as the emitted light LS5 and emits the pulse wave LS2 from the laser element 10 in the fundamental wave mode in which the continuous wave fundamental wave LS1 is emitted from the laser element 10. In the pulse wave mode, the converted wave LS4 is emitted as the emitted light LS5. Details of the fundamental wave LS1, the pulse wave LS2, the reflected wave LS3, and the converted wave LS4 will be described with reference to FIG.

  Further, the PD 40 receives the detection light LS6 reflected by a part of the outgoing light LS5 by the mirror 41, outputs a detection signal K0 corresponding to the light intensity of the detection light LS6, and inputs the detection signal K0 to the control circuit 50.

  The control circuit 50 corrects an oscillation switching circuit 51 serving as an oscillation state switching means for switching the oscillation of the laser element 10, a drive current control circuit 52 that outputs a drive current Id of the LD 11 of the laser element 10, and a deterioration characteristic of the LD 11. And a lookup table 53. The oscillation switching circuit 51 applies a bias voltage Vb to the SA electrode 12a of the laser element 10 described above. The drive current control circuit 52 outputs the drive current Id to the LD electrode 11a of the laser element 10 described above. Further, the control circuit 50 receives a control signal C1 from the external input 2 of the laser light source device 1, and the oscillation switching circuit 51 and the drive current control circuit 52 operate based on the control signal C1, so that the laser element 10 Driven.

[Description of Internal Configuration of Laser Element 10 of First Embodiment: FIG. 2]
Next, although it is a publicly known technique, a schematic configuration inside the laser element 10 used in the first embodiment will be described with reference to FIG. The laser element 10 includes a semiconductor crystal layer, and includes an LD 11 serving as a gain region and an SA 12 including a saturable absorber portion. A cathode electrode 10a is formed on the common surface of the LD 11 and the SA 12, and the common electrode of the LD 11 and the SA 12 is connected to 0V as described above. On the other hand, the LD electrode 11a is formed on the opposing surface on the LD11 side, and the drive current Id is supplied as described above. Further, the SA electrode 12a is formed on the opposite surface on the SA12 side, and the bias voltage Vb is applied as described above.

An n-type semiconductor layer 10n is formed in the vicinity of the cathode electrode 10a, and a p-type semiconductor layer 10p is formed in the vicinity of the LD electrode 11a and the SA electrode 12a. The n-type semiconductor layer 10n and the p-type semiconductor layer are formed. An active layer 10d is formed between 10p. An SA layer 12b is formed in the vicinity of the active layer 10d on the SA12 side. Further, an HR coat 10e that functions as a reflection mirror for the fundamental wave is formed on the left end face of the SA12 drawing, and an AR coat 10f for the fundamental wave is formed on the right end face of the LD11 drawing.

[Description of Operation of Laser Element 10 of First Embodiment: FIG. 2]
Next, a schematic operation of the laser element 10 will be described with reference to FIG. In FIG. 2, when the laser element 10 is oscillated in the fundamental wave mode, the cathode electrode 10a is connected to 0V (GND), a bias voltage Vb of 0V is applied to the SA electrode 12a, and a predetermined drive current Id is applied to the LD electrode 11a. Supply. In this fundamental wave mode, the LD 11 oscillates the fundamental wave LS1 having a predetermined wavelength by the drive current Id. However, since the SA electrode 12a is 0 V, the SA 12 always functions as a transparent body. As a result, the fundamental wave LS1 is generated as a continuous wave in the active layer 10d, reflects the HR coat 10e, and is emitted to the outside from the surface of the AR coat 10f.

  Further, when the laser element 10 is oscillated in the pulse wave mode, the cathode electrode 10a is connected to 0V, the reverse bias voltage Vb of about −2V is applied to the SA electrode 12a as an example, and the LD electrode 11a is driven to a predetermined level. A current Id is supplied. In this pulse wave mode, when a reverse bias voltage is applied to SA12, SA12 functions as an absorber for laser light having a low light intensity, and functions as a transparent body for laser light having a high light intensity.

  As a result, the oscillation of the LD 11 becomes a pulse oscillation (self-excited oscillation) in a pulse shape, and the pulse wave LS2 reflects the HR coat 10e and is emitted to the outside from the surface of the AR coat 10f. Thus, the laser element 10 can switch the emitted light to the fundamental wave LS1 and the pulse wave LS2 which are continuous waves by switching the bias voltage Vb applied to the SA electrode 12a.

[Description of switching operation of fundamental wave and converted wave of laser light source device of first embodiment: FIGS. 1 and 3]
Next, details of the switching operation between the fundamental wave and the converted wave of the laser light source device 1 will be described with reference to FIGS. FIG. 3 schematically shows the spectrum of the laser beam, where the horizontal axis represents the wavelength of the laser beam and the vertical axis represents the emission level (light intensity) of the laser beam.

  In FIG. 1, when the bias voltage Vb to the laser element 10 is 0 V, the laser light generated by the laser element 10 becomes a continuous fundamental wave LS1 and enters the SHG element 20 as described above. As shown in FIG. 3, the spectrum of the fundamental wave LS1 has a high emission level at the wavelength W1 that is the center of the fundamental wave LS1, and it can be understood that the spectrum is very small in a region outside the wavelength W1. That is, the fundamental wave LS1 has most of the components of the wavelength W1, and the other wavelength components are small. This is because the fundamental wave LS1 is a continuous wave close to a sine wave.

  Here, the fundamental wave LS1 is transmitted through the SHG element 20 and the FBG element 30, but as shown in FIG. 3, if the wavelength of the reflected wave LS3 reflected by the FBG element 30 is W3, the fundamental wave LS1 is Since the component of the wavelength W3 of the reflected wave LS3 is very small, the reflected wave LS3 hardly occurs, the fundamental wave LS1 is not drawn into the wavelength W3 of the reflected wave LS3, and the SHG element 20 and the FBG element 30 are No effect on the fundamental wave LS1. As a result, the fundamental wave LS1 passes through the SHG element 20 and the FBG element 30 as they are and is emitted as the outgoing light LS5. That is, when the bias voltage Vb to the laser element 10 is 0V, the fundamental wave LS1 is emitted from the emitted light LS5.

Therefore, the fundamental wave LS1 is merely transmitted through the SHG element 20 and the FBG element 30, and is not affected by the temperature characteristics of the SHG element 20 and the FBG element 30. That is, when a bias voltage Vb of 0 V is applied to the laser element 10, the emitted fundamental wave LS1 is emitted as the emitted light LS5 without being affected by the characteristics of the SHG element 20 and the FBG element 30, so that the laser The emission level of the emitted light LS5 from the light source device 1 is a value that depends only on the emission characteristics of the laser element 10.

  Therefore, in the fundamental wave mode of the laser element 10, the value of the detection signal K0 obtained by detecting the light intensity of the detection light LS6 obtained by reflecting a part of the emitted light LS5 by the mirror 41 by the PD 40 is the laser element 10 alone. When the laser element 10 is deteriorated due to a change over time and the output level is lowered, the change in the output level can be reliably grasped by the detection signal K0. As a result, the control circuit 50 adjusts the drive current Id so that the value of the detection signal K0 is constant, thereby correcting the emission variation of the laser element 10 and keeping the emitted light LS5 constant.

  On the other hand, when the bias voltage Vb to the laser element 10 is about −2 V, as described above, the laser light generated by the laser element 10 becomes the pulse wave LS2 and enters the SHG element 20, and the SHG element 20 The pulse wave LS2 is transmitted and incident on the FBG element 30. As shown in FIG. 3, the spectrum of the pulse wave LS2 has the highest emission level at the center wavelength W2 of the pulse wave LS2, but it can be understood that there are a wide range of regions having a high emission level even outside the wavelength W2. . That is, the pulse wave LS2 has a wide wavelength distribution and has many wavelength components from a short wavelength to a long wavelength. This is because the pulse wave LS2 is a laser beam that repeatedly turns on and off in a pulsed manner at high speed.

  Here, as shown in FIG. 3, if the specific reflection wavelength reflected by the FBG element 30 is W3, the pulse wave LS2 has a wide wavelength distribution and includes many wavelength components of the reflection wavelength W3 of the FBG element 30. Therefore, the reflected wave LS3 is generated in the FBG element 30 so that the pulse wave LS2 is drawn into the reflected wavelength W3. The reflected wave LS3 travels in the direction returning to the SHG element 20 and is fed back to the laser element 10 (see FIG. 1). As a result, a feedback loop is formed among the laser element 10, the SHG element 20, and the FBG element 30, and the reflected wave LS3 locked at the reflection wavelength W3 of the FBG element 30 continuously oscillates. The reflected wave LS3 is a pulse wave whose wavelength is selected by the FBG element 30, and has a higher peak value than a continuous wave having the same average light intensity, and thus is higher than a continuous wave having the same average light intensity in the SHG element 20. Conversion efficiency can be obtained. For example, the wavelength W3 of the reflected wave LS3 is set to 1,064 nm.

  Here, assuming that the SHG element 20 located in the feedback loop is set so as to be phase-matched to 532 nm, which is a half wavelength of the wavelength W3 of the reflected wave LS3, the SHG element 20 has the reflected wave LS3. Is converted into a wavelength, and a converted wave LS4 having a wavelength W4 of 532 nm, which is a second harmonic, is emitted. As a result, the converted wave LS4 passes through the FBG element 30 and is emitted to the outside as outgoing light LS5. The 532 nm converted wave LS4 is green laser light (G light).

  That is, when a bias voltage Vb of about −2 V is applied to the laser element 10, the laser element 10 emits a pulse wave LS2, and the operation of the FBG element 30 and the SHG element 20 causes the emitted light LS5 to have a wavelength W4 of 532 nm. The converted wave LS4 is emitted. At this time, the output level of the output light LS5 varies depending on the temperature characteristics of the SHG element 20 and the FBG element 30. This is because the outgoing light LS5 is composed of a reflected wave LS3 from the FBG element 30 and a converted wave LS4 obtained by converting the wavelength of the reflected wave LS3 by the SHG element 20.

Therefore, in the pulse wave mode of the laser element 10, the value of the detection signal K0 obtained by detecting the light intensity of the detection light LS6 obtained by reflecting a part of the emitted light LS5 by the mirror 41 by the PD 40 is the same as that of the SHG element 20 and the FBG. The value depends on the temperature characteristics of the element 30 and the like. As a result, the control circuit 50 adjusts the drive current Id so that the value of the detection signal K0 becomes constant, thereby correcting the temperature characteristics of the SHG element 20 and the FBG element 30 and the like, and being stable without being affected by the environment. The laser beam can be emitted.

  As described above, the laser light source device of the present invention switches the emitted light from the laser element 10 to the fundamental wave LS1 and the pulse wave LS2 which are continuous waves by switching the bias voltage Vb applied to the laser element 10, and further, By the operations of the SHG element 20 and the FBG element 30, the emitted light LS5 can be switched to the fundamental wave LS1 and the converted wave LS4 which is the second harmonic.

[Description of fundamental wave correction by fundamental wave detection of laser light source device of first embodiment: FIGS. 1 and 4]
Next, the operation of correcting the fluctuation (deterioration) of the emission level of the laser element 10 by detecting the light intensity of the fundamental wave LS1 will be described with reference to the flowchart of FIG. 4 and a lookup table. The configuration of the laser light source device 1 is referred to FIG.

  In FIG. 4A, the oscillation switching circuit 51 of the control circuit 50 outputs a bias voltage Vb of 0V, and the drive current control circuit 52 outputs a drive current Idk having a predetermined value. A certain fundamental wave LS1 is emitted (step ST1). Accordingly, the laser light source device 1 emits the fundamental wave LS1 as the emitted light LS5.

  Next, the PD 40 receives the detection light LS6 and outputs a detection signal K0 corresponding to the light intensity of the fundamental wave LS1 (step ST2).

  Next, the control circuit 50 receives the detection signal K0 and determines whether the detection signal K0 is within a predetermined range (step ST3). If the detection signal K0 is within the predetermined range, the process proceeds to step ST4. If the detection signal K0 is outside the predetermined range, the process proceeds to step ST5.

  Next, if it is determined in step ST3 that the detection signal K0 is within a predetermined range, the drive current Id is not changed and the process proceeds to step ST6 with a predetermined constant value (step ST4).

  If it is determined in step ST3 that the detection signal K0 is out of the predetermined range, the lookup table 53 stored in advance is referred to determine the drive current Id corresponding to the detection signal K0 (step ST5).

  Next, the control circuit 50 outputs the determined drive current Id from the drive current control circuit 52, drives the LD 11, adjusts the light intensity of the fundamental wave LS1, and corrects the fluctuation (step ST6).

  FIG. 4B shows an example of the lookup table 53. The horizontal axis represents the detection signal K0 detected by the PD 40, and the vertical axis represents the drive current Id set corresponding to the detection signal K0. The set value of the drive current Id is non-linear with respect to the detection signal K0. When the detection signal K0 is small, the set value of the drive current Id is large, and when the detection signal K0 is large, the set value of the drive current Id is small. The control circuit 50 refers to the lookup table 53 based on the detection signal K0, so that even if the light intensity of the fundamental wave LS1 with respect to the driving current Id of the laser element 10 is nonlinear, the correction is performed by the lookup table 53. In addition, it is possible to emit the stable emission light LS5 with little fluctuation.

In this way, by using the lookup table 53, the nonlinearity is stored in the lookup table 53 regardless of the nonlinearity of the emission characteristics due to the temporal change of the laser element 10. LS5 can be corrected with high accuracy. In addition, since the fluctuation of the light intensity of the fundamental wave LS1 indicates the emission characteristic of the laser element 10 alone as described above, the light intensity of the fundamental wave LS1 is detected and influenced by the characteristics of other optical elements. Therefore, it is possible to provide a laser light source device that can perform highly accurate correction on the laser element 10 alone and emit laser light that is stable for a long period of time. The fundamental wave detection timing operation will be described in a second embodiment to be described later.

[Conversion Wave Correction Explanation by Conversion Wave Detection of Laser Light Source Device of First Embodiment: FIGS. 1 and 5]
Next, an operation for correcting fluctuation due to temperature characteristics of the SHG element 20 and the FBG element 30 by detecting the light intensity of the converted wave LS4 will be described with reference to the flowchart of FIG. The configuration of the laser light source device 1 is referred to FIG.

  In FIG. 5, the oscillation switching circuit 51 of the control circuit 50 outputs a bias voltage Vb of −2V, the drive current control circuit 52 outputs a drive current Idh of a predetermined value, and the pulse wave LS2 is output from the laser element 10. The light is emitted (step ST10). Thereby, the laser light source device 1 emits the converted wave LS4 as the emitted light LS5.

  Next, the PD 40 receives the detection light LS6 and outputs a detection signal K0 corresponding to the light intensity of the converted wave LS4 (step ST11). At this time, a part of the fundamental wave that has not been reflected by the FBG element 30 enters the PD 40 at the same time, but most of the fundamental wave becomes the converted wave LS4. Therefore, even if the PD 40 has no wavelength selectivity, the emitted light LS5 is converted into the converted wave. It can be regarded as LS4.

  Next, the control circuit 50 receives the detection signal K0 and determines whether the detection signal K0 is within a predetermined range (step ST12). If the detection signal K0 is within the predetermined range, the process proceeds to step ST13. If the detection signal K0 is out of the predetermined range, the process proceeds to step ST14.

  Next, if it is determined in step ST12 that the detection signal K0 is within a predetermined range, the driving current Id is set to a predetermined constant value without changing, and the process proceeds to step ST17 (step ST13).

  If it is determined in step ST12 that the detection signal K0 is outside the predetermined range, it is determined whether or not the detection signal K0 is in a decreasing direction (step ST14). If the detection signal K0 is in the decreasing direction (positive determination), the process proceeds to step ST15. If the detection signal K0 is in the increasing direction (negative determination), the process proceeds to step ST16.

  Next, if the determination in step ST14 is affirmative, the drive current Id is increased by a predetermined amount and the process proceeds to step ST17 (step ST15).

  If step ST14 is negative, the drive current Id is decreased by a predetermined amount and the process proceeds to step ST17 (step ST16).

  Next, the control circuit 50 outputs the drive current Id determined in each of steps ST13, ST15, and ST16 from the drive current control circuit 52, drives the LD 11, and sets the light intensity of the emitted light LS5 that is the converted wave LS4. Adjustment is made to correct the fluctuation (step ST17). In this way, even if the emitted light LS5 fluctuates due to the temperature characteristics of the SHG element 20 or the FBG element 30, the drive current Id can be adjusted according to the detection signal K0 from the PD 40, so that the fluctuation of the emitted light LS5 is corrected. Thus, it is possible to emit the stable emission light LS5 with little fluctuation. The converted wave detection timing operation will be described in a second embodiment to be described later.

  As described above, according to the laser light source device of the present invention, by detecting the fundamental wave and the converted wave separately, the influence of the characteristics of the SHG element 20 and the FBG element 30 is removed, and the laser element 10 itself is removed. The emission characteristics can be grasped. As a result, the emission level of the emitted light can be obtained by separately performing the control for correcting the deterioration characteristics due to the time-dependent change of the laser element 10 and the control for correcting the fluctuation due to the temperature characteristics by the SHG element 20 and the FBG element 30. It is possible to provide a high-performance laser light source device that emits a stable laser beam for a long period of time by finely adjusting.

  In addition, since the fundamental wave can be detected with a continuous wave having a narrow wavelength distribution and a peak wavelength that is sufficiently large for detection, the fundamental wave can be easily detected, and the fundamental wave emission level is increased. Since it can be detected with high accuracy, it is possible to realize a laser light source device that corrects fluctuations of emitted light with high accuracy.

  Further, by selecting continuous oscillation or pulse oscillation by the bias voltage Vb applied to the laser element 10, the emitted light can be switched between the fundamental wave and the converted wave. Thereby, it is also possible to constitute one detection element for detecting the emitted light LS5 as in this embodiment.

  Although the laser light source device shown as the first embodiment has been described as a light source device that emits green (G) laser light, the color of the emitted laser light is not limited to green, and blue (B), Or red (R) may be sufficient. That is, by changing the reflection wavelength W3 of the FBG element 30 and the phase matching wavelength of the SHG element 20 (that is, the wavelength W4 of the converted wave LS4), a laser light source device that stably emits various wavelengths can be realized.

[Description of Configuration of Laser Light Source Device of Modified Example of First Embodiment: FIG. 6]
Next, a configuration of a laser light source device which is a modification of the first embodiment will be described with reference to FIG. This modification is characterized in that a plurality of detection elements for detecting the laser beam, specifically two elements, are configured. Except for the two detection elements and their peripheral configuration, the first embodiment described above is used. Since it is the same as the configuration (see FIG. 1), FIG. 6 shows only the two detection elements and the surrounding configuration, and the same elements as those in FIG.

  In FIG. 6, the emitted light LS5 emitted from the FBG element 30 of the laser light source device 1 ′ according to the modification of the first embodiment is incident on the mirror 41, and the mirror 41 transmits most of the emitted light LS5. In addition to being emitted to the outside, a part of the emitted light LS5 is reflected and emitted as detection light LS6. Here, reference numerals 42 and 43 denote two detection elements (hereinafter abbreviated as PD42 and PD43).

  The PDs 42 and 43 are arranged so that the detection light LS6 from the mirror 41 is incident substantially uniformly, and output the detection signals K1 and K2 corresponding to the light intensity of the detection light LS6 and input them to the control circuit 50. To do. Here, as an example, a filter 42a that transmits only the wavelength W1 of the fundamental wave LS1 (see FIG. 3) is attached to the entrance of the PD 42, and the wavelength W4 of the converted wave LS4 (see FIG. 3) is attached to the entrance of the PD 43. The filter 43a which transmits only the reference) is mounted.

  With this configuration, when the laser light source device 1 ′ is in the fundamental wave mode, as described above, since the emitted light LS5 is the fundamental wave LS1, the PD 42 receives the fundamental wave LS1 that has passed through the filter 42a, and the fundamental wave LS1 enters. A detection signal K1 corresponding to the light intensity of LS1 is output and input to the control circuit 50. When the laser light source device 1 ′ is in the converted wave mode, the outgoing light LS5 is the converted wave LS4. Therefore, the PD 43 enters the converted wave LS4 that has passed through the filter 43a and corresponds to the light intensity of the converted wave LS4. The detection signal K2 is output and input to the control circuit 50.

  The control circuit 50 inputs the detection signal K1 in the fundamental wave mode, determines the drive current Id according to the detection signal K1 and corrects the deterioration characteristics due to the time-dependent change of the laser element 10 as in the flowchart of FIG. To stabilize the fluctuation of the emitted light LS5. Further, the control circuit 50 receives the detection signal K2 in the converted wave mode, determines the drive current Id according to the detection signal K2, as in the flowchart of FIG. 5, and the temperature characteristics of the SHG element 20 and the FBG element 30. The fluctuation of the output light LS5 is stabilized by correcting the fluctuation due to the above.

As described above, the laser light source device 1 ′ according to the modification of the first embodiment requires two detection elements PD42 and PD43 for detecting laser light. Since the fundamental wave LS1 and the converted wave LS4 are detected individually and independently, more accurate detection is possible, and a laser light source device that finely and accurately corrects the emission level of the emitted light LS5 can be provided.

[Description of Configuration of Laser Projector of Second Embodiment: FIG. 7]
Next, as a second embodiment, a schematic configuration of a laser projector using the laser light source device of the first embodiment of the present invention will be described with reference to FIG. In FIG. 7, a laser projector 100 transmits the laser light source device 1 according to the first embodiment, a control unit 110 as a control unit that controls the laser light source device 1, and light emitted from the laser light source device 1 to a collimator lens 120. Scanning means 140 for scanning the laser light 121 collected by the collimator lens 120 horizontally or vertically, a scanning driver 150 for driving the scanning means 140, and a scanning region of the laser light 121 scanned by the scanning means 140 It is comprised from the shielding part 160 which light-shields the circumference | surroundings.

  In addition, when the laser projector 100 displays a color image, the laser light source device 1 is configured by three units that emit laser beams of three types of RGB wavelengths, not shown, and the respective RGB laser beams are synthesized. Is incident on the optical fiber 130. Note that the laser light 121 emitted from the optical fiber 130 corresponds to the emitted light LS5 of the first embodiment. Reference numeral 170 denotes a screen. The display area 171 is irradiated with the laser light 121 that passes through the opening 161 of the shielding part 160 to form an image as the projection spot 122.

  The control unit 110 receives a video signal V1 from the outside, and controls a light intensity of each laser beam of the three laser light source devices 1 that respectively emit RGB laser beams according to the video signal V1, A scan control signal C2 for controlling the scan driver 150 is output.

  The scanning means 140 uses a MEMS mirror 141 and can be swung in the horizontal direction (hereinafter referred to as the X direction) and the vertical direction (hereinafter referred to as the Y direction) by the scanning driver 150. Resonantly driven at 20 KHz, the scanning angle in the X direction changes sinusoidally with respect to time. In the Y direction, it is driven at 60 Hz by a sawtooth forced drive, and its scanning angle is displaced in a sawtooth manner.

  Therefore, the laser beam 121 repeatedly scans one line of the image to be displayed in the X direction at a high speed, and scans one screen of the image to be displayed in the Y direction at a low speed. The driving method of the scanning unit 140 includes an electrostatic method, an electromagnetic method, a piezo method, and the like, and may be a combination of different methods such as horizontal scanning and vertical scanning.

  That is, the laser beam 121 is a sinusoidal wave from the first X-line scan in the uppermost X direction to the last one-line scan in the X direction at the bottom by the scanning angle displacement of the scanning unit 140 in the X and Y directions. An image is formed on a screen basis by repeating the operation of moving in the Y direction while drawing and returning to the top one-line scanning in the first X direction.

[Explanation of Laser Light Scanning by Laser Projector of Second Embodiment: FIG. 8]
Next, the locus of laser light projected by scanning by the laser projector 100 of the second embodiment will be described with reference to FIG. The configuration of the laser projector 100 is referred to FIG.

In FIG. 8, the projection spot 122 of the laser beam scans in the direction of the arrow H1 by the swing of the MEMS mirror 141 in the XY directions, and forms a locus L indicated by a dotted line and a solid line. Here, the locus L of the projection spot 122 is shielded when the peripheral portion 162 of the shielding portion 160 is scanned (the locus indicated by the dotted line), and is scanned when the opening portion 161 of the shielding portion 160 is scanned (the solid line). The trajectory shown) reaches the display area 171 (see FIG. 7) of the screen 170 and displays an image.

  That is, the locus L of the projected spot 122 by scanning moves as a sine wave indicated by a dotted line in the peripheral portion 162 with the point P1 in FIG. 8 as the starting point, and from the point P2 of the opening portion 161 of the shielding portion 160 to the opening portion 161. For example, the trajectories La1 and La2 form sinusoidal trajectories as shown by solid lines, and the trajectories in the peripheral portion 162 are trajectories Lb1 and Lb2 are sinusoidal waves as shown by dotted lines, for example. Each of these trajectories is periodically repeated, and the scanning in the opening 161 is finished at the point P3, and the trajectory indicated by the dotted line is drawn by the peripheral portion 162 and reaches the lowermost point P4.

  And it passes along the locus | trajectory Lc1 and Lc2 which are shown with the rough dotted line along the locus | trajectory of the sine wave of the upward return, and returns to the upper starting point P1. With this operation, drawing of one screen is completed. By repeating the above operation, the locus L of the projection spot 122 scans within the opening 161 of the shielding part 160, so that a continuous image can be displayed on the display area 171 of the screen 170. In FIG. 8, for the sake of easy understanding, the number of scans is reduced, but the actual number of scans in the Y direction is about 600 as an example.

  Here, the scanning angle of the MEMS mirror 141 corresponds to the maximum scanning amplitude α1 of the MEMS mirror 141 in the X direction of the locus L of the projection spot 122 in the X direction, and corresponds to the maximum scanning amplitude B1 of the Y direction in the Y direction. This corresponds to the maximum scanning angle β1 (not shown).

  Further, the opening 161 of the shielding part 160 is formed by the X-direction display width A2 and the Y-direction display width B2, and this area displays and forms an image on the display area 171 of the screen 170 (see FIG. 7). Then, the X direction display width A2 of the opening 161 and the X direction display scanning angle α2 of the MEMS mirror 141 match, and the Y direction display width B2 and the Y direction display scanning angle β2 (not shown) match.

  That is, since the scanning angle of the laser beam 121 in the X direction changes in a sine wave shape, light in a region where the scanning speed near the maximum scanning angle α1 in the X direction is close to zero, for example, light in the traces Lb1 and Lb2 indicated by dotted lines Is shielded by the peripheral part 162 of the shielding part 160, the projection spot 122 does not reach the screen 170, and no image is displayed. Further, light in a region where the change in scanning speed within the X-direction display scanning angle α2 is small, for example, light in the traces La1 and La2 indicated by solid lines is configured to display an image in the display region 171 of the screen 170. .

  Note that the ratio of the X-direction display scanning angle α2 to the X-direction maximum scanning angle α1 can be set at a predetermined ratio. For example, the ratio of the display scanning angle α2 to the maximum scanning angle α1 may be set to 0.75 or more. desirable.

  Here, the laser projector according to the second embodiment is characterized by the time during which the locus L of the projection spot 122 is shielded at both ends of the peripheral portion 162 of the shielding portion 160, that is, the locus described above. By effectively utilizing the time during which the portion indicated by the dotted lines of Lb1 and Lb2 is scanned (the time in the vicinity of the maximum scanning angle α1) and the blanking period in which the locus L returns from the point P4 to the point P1, This is to detect the fundamental wave.

[Explanation of Detection Timing of Laser Light by Laser Projector of Second Embodiment: FIG. 9]
Next, the detection timing of the converted wave and the fundamental wave of the laser beam of the laser projector according to the second embodiment will be described with reference to FIG. The laser projector 100 uses three laser light source devices 1 that respectively emit R light, G light, and B laser light. Here, for ease of explanation, one laser light source is used. The apparatus will be described as an example.

  FIG. 9A is a graph showing the temporal change of the luminance signal, taking as an example an image in which the upper part of the display area 171 of the screen 170 (see FIG. 7) is dark and becomes brighter toward the lower part in the drawing for one screen. The vertical axis represents the luminance Q by the laser beam 121, and the horizontal axis is the time axis t. Note that the horizontal axis of all the following graphs is the time axis t. Here, the luminance Q rises linearly based on the luminance signal.

  FIG. 9B shows a temporal change in control of the drive current Id (see FIG. 1) to the LD 11 based on the luminance signal, and the vertical axis is a graph of the drive current Id. This drive current Id is drive currents Id1, Id2,... Id9 for obtaining luminances Q1, Q2,... Q9, Q10 based on luminance signals in one scanning display periods Ta1, Ta2,. , Id10 flows, and the driving current for display is controlled not to flow during one scanning blanking periods Tb1, Tb2,.

  FIG. 9C shows a temporal change of the scanning angle in the X direction of the MEMS mirror 141 for scanning the laser beam 121 in the X direction, and the vertical axis is a graph of the scanning angle α.

  FIG. 9D shows a temporal change in the scanning angle in the Y direction of the MEMS mirror 141 for scanning the laser beam 121 in the Y direction, and the vertical axis is a graph of the scanning angle β.

  FIG. 9E shows the bias voltage Vb applied to the SA 12 of the laser element 10. FIG. 9F shows the timing for detecting the converted wave, and FIG. 9G shows the timing for detecting the fundamental wave.

  Hereinafter, in contrast to the points P1, P2, P3, and P4 of the locus L of the projection spot 122 in FIG. 8, in FIG. 9, the scanning angles α and β of the MEMS mirror 141, the drive current Id, the luminance Q, the bias voltage Vb, The detection timing of the converted wave LS4 and the fundamental wave LS1 will be described along the time axis.

  First, the relationship between the point P and the time axis t will be described with reference to FIGS. 8 and 9D. Times t1, t2, t3, t4, and t5 = t1 on the time axis t are one-screen drawing periods F for displaying one screen, and points P1, P2, P3, P4, P5 = It is configured that the displacement in the Y direction of P1 is periodically repeated in a sawtooth shape, and one screen is formed in one cycle.

  Points P1 to P2 at times t1 to t2 are an upper blanking period TB1 in which the laser beam 121 is shielded at the upper part of the peripheral part 162 of the shield part 160. Points P2 to P3 at times t2 to t3 are one-screen display periods TS in which the projection spot 122 is transmitted through the opening 161 of the shielding part 160 and can be displayed on the display area 171 of the screen 170. Points P3 to P4 at times t3 to t4 are a lower blanking period TB2 in which the laser beam 121 is shielded below the peripheral portion 162 of the shield 160, and points P4 to P5 at times t4 to t5 (t1) ( P1) is a return blanking period TB3 for returning the projected spot 122 scanned downward again upward.

The return blanking period TB3 is a period during which the projection spot 122 is transmitted through the opening 161 (see rough dotted lines Lc1 and Lc2 in FIG. 8). Regarding the Y-direction scanning angle, the Y-direction maximum scanning angle β1 corresponds to the maximum Y-direction scanning amplitude B1 from the point P1 to the point P4 shown in FIG. 8, and the Y-direction display scanning angle β2 is shown in FIG. This corresponds to the Y-direction display width B2 from the point P2 to the point P3 shown.

  Further, in FIG. 9C, the scanning angle α in the X direction is periodically changed in a sine wave shape, and is constituted by, for example, a sine wave having a period of time t1 to t2. An interval that is half of the period corresponds to one scanning period Ts1. The one scanning period Ts1 is composed of one scanning display period Ta1 and one scanning blanking period Tb1, and the next one scanning period Ts2 is composed of one scanning display period Ta2 and one scanning blanking period Tb2. At the end of the screen display period TS, a one-scan blanking period Tb9 and a one-scan display period Ta10 are reached. Accordingly, one scanning period Ts1 and the next one scanning period Ts2 constitute one cycle of a sine wave, and scanning in the X direction is formed by repeating this.

  The one-scan display periods Ta1 and Ta2 and the one-scan blanking periods Tb1 and Tb2 project a locus La1 (solid line), Lb1 (dotted line), La2 (solid line), and Lb2 (dotted line), which are part of the locus L in FIG. One screen is formed by repeating this corresponding to the period during which the spot 122 passes. Regarding the X direction scanning angle, the X direction maximum scanning angle α1 in FIG. 9C corresponds to the X direction maximum scanning amplitude A1 shown in FIG. 8, and the X direction display scanning angle α2 in FIG. This corresponds to the indicated X-direction display width A2.

  Next, in FIG. 9E, the bias voltage Vb applied to SA12 of the laser element 10 becomes 0 V in the return blanking period TB3, and the upper blanking period TB1, the one-screen display period TS, and the lower blanking period TB2 The oscillation switching circuit 51 (see FIG. 1) of the control circuit 50 controls so that the voltage becomes about −2V. By this control, as described above, the emitted light LS5 becomes the continuous fundamental wave LS1 when the bias voltage Vb is 0V, and the emitted light LS5 becomes the converted wave LS4 when the bias voltage Vb is about −2V. That is, the fundamental wave LS1 is emitted during the return blanking period TB3, and the converted wave LS4 is emitted during the other periods.

  With this control, when a predetermined drive current Id flows to the LD 11 during the one-screen display period TS, a converted wave LS4 corresponding to the magnitude of the drive current Id is emitted, and the laser beam 121 is displayed to display an image on the screen 170. I can do it. If the wavelength of the converted wave LS4 is G light of 532 nm as described above, a green image is displayed on the screen 170. Even if the drive current Id flows during the return blanking period TB3, the laser light source device 1 emits the fundamental wave LS1 of infrared light, so that the projection spot 122 passes through the opening 161 as the trajectories Lc1 and Lc2. However, it is not visible on the screen 170.

  Further, in FIG. 9F, the timing Th for detecting the emission level of the converted wave LS4 is, for example, the projection spot 122 as the shielding portion 160 in the one-screen display period TS in which the converted wave LS4 is emitted. This is performed in the period of the locus Lb1 when the peripheral portion 162 is scanned, that is, in one scanning blanking period Tb1. During this timing Th, the drive current Idh (see FIG. 9B) is supplied to the laser element 10, and the PD 40 detects the emission level of the emitted light LS5 at that time. Thereby, the control circuit 50 of the laser light source device 1 can grasp the emission level of the converted wave LS4 and acquire data for correcting the converted wave LS4. That is, the conversion wave correction operation described in FIG. 5 of the first embodiment is performed at the detection timing Th of the conversion wave LS4.

  Further, when the drive current Idh is supplied to the laser element 10, the converted light LS4 is emitted from the laser light source device 1. As described above, the projection spot 122 shields the detection timing Th of the converted wave LS4. Since this is performed during one scanning blanking period Tb1 in which the peripheral portion 162 of 160 is scanned, the converted wave LS4 is shielded by the shielding portion 160 and is not seen on the screen 170 and does not affect the display image.

  In FIG. 9F, the detection timing of the converted wave LS4 is shown as only once (that is, Tb1) in the one-screen display period TS. However, the detection timing Th is not limited to this. There may be a plurality of times in one repeated blanking period Tb. Conversely, the detection of the converted wave LS4 may be performed at a certain interval instead of every time of one screen display period TS.

  In FIG. 9G, timing Tk for detecting the emission level of the fundamental wave LS1 is performed in a predetermined period in the return blanking period TB3. During this timing Tk, the drive current Idk (see FIG. 9B) is supplied to the laser element 10, and the PD 40 detects the emission level of the emission light LS5 at that time. Thereby, the control circuit 50 of the laser light source device 1 can grasp the emission level of the fundamental wave LS1 and acquire data for correcting the fundamental wave LS1. That is, at the detection timing Tk of the fundamental wave LS1, the fundamental wave correction operation described in FIG. 4 of the first embodiment is performed.

  Even if the drive current Idk for detecting the fundamental wave is supplied to the laser element 10 during the return blanking period TB3, as described above, the fundamental wave LS1 with weak infrared light is emitted from the laser light source device 1. Therefore, it is not visible on the screen 170 and does not affect the display image.

  As described above, the laser projector according to the second embodiment detects the converted wave LS4 during the one scanning blanking period Tb in which the laser light from the laser light source device 1 is shielded by the shielding unit 160 by horizontal scanning. In addition, the fundamental wave is detected during the return blanking period TB3 of the vertical scanning of the laser light from the laser light source device 1. As a result, the emitted light by each detection current does not affect the display image, and the converted wave and the fundamental wave can be detected individually. Thereby, it is possible to provide a small laser projector that always corrects the variation of the emitted light due to the temporal change of each optical element, temperature characteristics, etc., and displays a stable and beautiful image.

  Note that the configuration diagrams, flowcharts, and the like shown in the embodiments of the present invention are not limited thereto, and may be arbitrarily changed as long as they satisfy the gist of the present invention. Further, the scanning means of the laser projector of the second embodiment is exemplified as the MEMS mirror system, but the scanning means system is not limited, and the present invention is applicable to any scanning means. The

1, 1 'laser light source device 10 laser element 11 LD (laser diode)
12 SA (saturable absorber)
20 SHG element (wavelength conversion element)
30 FBG element (FBG type reflective element)
40, 42, 43 PD (detection element)
DESCRIPTION OF SYMBOLS 41 Mirror 42a, 43a Filter 50 Control circuit 51 Oscillation switching circuit 52 Drive current control circuit 53 Look-up table 100 Laser projector 110 Control part 120 Collimator lens 121 Laser light 122 Projection spot 130 Optical fiber 140 Scan means 141 MEMS mirror 150 Scan driver 160 shielding part 161 opening part 162 peripheral part 170 screen 171 display area LS1 fundamental wave (fundamental laser beam)
LS2 pulse wave LS3 reflected wave LS4 converted wave LS5 outgoing light LS6 detection light Id drive current Vb bias voltage C1 control signal C2 scanning control signal K0, K1, K2 detection signal

Claims (4)

A laser element;
A wavelength conversion element that converts the wavelength of the laser light from the laser element and emits it;
In a laser light source device having
Control means for controlling the driving of the laser element;
Detecting means for detecting light emitted from the wavelength conversion element,
The control means includes an oscillation state switching means for switching an oscillation state of the laser element,
The oscillation state switching means switches the oscillation state of the laser element between pulse oscillation and continuous oscillation,
The detection means detects a converted wave of the laser beam when the laser element is in a pulse oscillation state, and detects a fundamental wave of the laser beam when the laser element is in a continuous oscillation state. ,
The laser light source apparatus, wherein the control means controls driving of the laser element based on detection information of the fundamental wave and detection information of the converted wave from the detection means.   The laser light source device according to claim 1, wherein the detection unit detects both the converted wave and the fundamental wave by a single detection element. The laser light source device according to claim 1 or 2,
Control means for controlling the laser light source device;
Scanning means for horizontally or vertically scanning laser light from the laser light source device;
A shielding unit that shields light of which the ratio of the scanning angle by the scanning unit to the maximum scanning angle is a predetermined ratio or more of the laser light;
The control means detects the converted wave from the laser light source device during a horizontal scanning period,
A laser projector characterized by performing control so as to detect a fundamental wave from the laser light source device during a vertical scanning period. 4. The laser projector according to claim 3, wherein the control unit detects the converted wave while the laser beam is shielded by the shielding unit during the horizontal scanning period. 5.

Images