阅读说明：本技术 光参量振荡器 (Optical parametric oscillator ) 是由 约翰·乔治·德什·奥努瓦 本杰明·希曼斯基 于 2019-02-27 设计创作，主要内容包括：本发明涉及双谐振光参量振荡器(1),包括具有二阶光学非线性并置于能反射泵浦波(2)的光腔(6)中的扇出晶体(5,55,105),晶体(5,55,105)包括光轴穿过的入射面(59)和出射面(60)、上面(57)和下面(58)。根据本发明的光参量振荡器(1)的主要特征为晶体(105)具有极性反转线(106)的网,极性反转线(106)分开且靠近地始于与晶体(105)上面(57)平行的上虚拟直线(61)并分开且彼此远离地结束于与晶体(105)下面(58)平行的下虚拟直线(63)或晶体入射面(59),且两相继线(106)彼此形成恒定角度,网从起始于晶体(105)出射面(60)并通过从出射面(60)发散而朝下虚拟直线(63)延伸的第一线(108)开始,所有其它线从第一线(108)向晶体(105)入射面(59)逐渐且单调倾斜。(The invention relates to a dual-resonant optical parametric oscillator (1) comprising a fan-out crystal (5, 55, 105) having a second order optical nonlinearity and arranged in an optical cavity (6) capable of reflecting a pump wave (2), the crystal (5, 55, 105) comprising an entrance face (59) and an exit face (60) through which an optical axis passes, an upper face (57) and a lower face (58). The main feature of the optical parametric oscillator (1) according to the invention is that the crystal (105) has a network of lines of polarity inversion (106), the lines of polarity inversion (106) starting separately and closely from an upper virtual straight line (61) parallel to the upper face (57) of the crystal (105) and ending separately and far away from each other at a lower virtual straight line (63) or at the crystal entrance face (59) parallel to the lower face (58) of the crystal (105), and the two successive lines (106) forming a constant angle with each other, the network starting from a first line (108) starting at the crystal (105) exit face (60) and extending towards the lower virtual straight line (63) by diverging from the exit face (60), all other lines being gradually and monotonically inclined from the first line (108) towards the crystal (105) entrance face (59).)

1. An optical parametric oscillator (1) of the double resonance type, comprising a crystal (5, 55, 105) of the fan-out type, said crystal (5, 55, 105) having a second order optical nonlinearity and being placed in an optical cavity (6) capable of reflecting a pump wave (2), said crystal (5, 55, 105) comprising an entrance face (59) and an exit face (60), an upper face (57) and a lower face (58), with an optical axis passing through said entrance face (59) and said exit face (60), characterized in that said crystal (105) comprises a grid of lines of polarity inversion (106), said lines of polarity inversion (106) starting separately and with a narrow spacing from an upper virtual straight line (61) parallel to said upper face (57) of said crystal (105) and ending separately and with a wide spacing from a lower virtual straight line (63) parallel to said lower face (58) of said crystal (105) or ending at said entrance face (59) of said crystal (105), and two successive lines (106) forming a constant angle between each other, the grid starting from a first line (108), the first line (108) starting from the exit face (60) of the crystal (105) and extending towards the lower virtual straight line (63) while diverging from the exit face (60), all the other lines being progressively and monotonically inclined from the first line (108) towards the entrance face (59) of the crystal (105).

2. An optical parametric oscillator according to claim 1, characterized in that the four faces (57, 58, 59, 60) of the crystal (105) are planar.

3. An optical parametric oscillator according to any of claims 1 and 2, characterized in that the upper face (57) and the lower face (58) are parallel and the entrance face (59) and the exit face (60) are parallel.

4. An optical parametric oscillator according to any one of claims 1 to 3, characterized in that the polarity-reversal line (106) is located immediately after the first line (108) and the first line (108) also ends at the lower virtual straight line (63), and the following lines (106) all end at the entrance face (59).

5. An optical parametric oscillator according to any of claims 1 to 4, characterized in that the constant angle of tilt between two consecutive lines (106) is about 0.1 mrad.

6. An optical parametric oscillator according to any of claims 1 to 5, characterized in that the crystal (105) is made of lithium niobate.

7. The optical parametric oscillator according to any one of claims 1 to 6, wherein the grating comprises an original line (109) placed before the first line (108), and the original line (109) starts at the exit face (60) and ends at the lower virtual straight line (63) below the upper virtual straight line (61).

8. An optical parametric oscillator according to any one of claims 1 to 7, wherein the first line (108) is inclined at an angle greater than or equal to the constant angle with respect to the exit face (60) so as to separate two successive lines (106).

9. A crystal for manufacturing an optical parametric oscillator according to any one of claims 1 to 8, the crystal (5, 55, 105) comprising an entrance face (59) and an exit face (60), an upper face (57) and a lower face (58), an optical axis passing through the entrance face (59) and the exit face (60), characterized in that the crystal (105) comprises a grid of polarity-reversing lines (106), the polarity-reversing lines (106) starting separately and in a narrowly spaced manner from an upper virtual straight line (61) parallel to the upper face (57) of the crystal (105) and ending separately and in a widely spaced manner from a lower virtual straight line (63) parallel to the lower face (58) of the crystal (105) or ending at the entrance face (59), and two successive lines (106) forming a constant angle between each other, the grid starting from a first line (108), the first line (108) starts at the exit face (60) of the crystal (105) and extends towards the lower virtual straight line (63) while diverging from the exit face (60), all other lines being gradually and monotonically inclined from the first line (108) towards the entrance face (59) of the crystal (105).

Technical Field

The present invention relates to an optical parametric oscillator.

Background

An Optical Parametric Oscillator (OPO) is a frequency converter that operates from an angular frequency ofThe laser wave (pump wave) generates angular frequencies of

Andtwo new waves called "signal wave" and "idler wave", so that

Parametric frequency conversion is obtained by propagating a pump wave through a second-order optically nonlinear component, typically a crystal. If a physical parameter of the crystal is modified, such as the temperature, the angle with respect to the pump radiation or even the periodicity of the ferroelectric domains (e.g. periodic domain inversion in the case of crystals such as lithium niobate) the values can be adjusted within a very wide rangeAnd

thus, OPO is a coherent light source that can be tuned over a very wide and much wider spectral range than lasers. This important feature opens up many fields of application for OPO, such as spectroscopic analysis of gases.

Disclosure of Invention

The optical parametric oscillator according to the present invention is a cavity-in-line optical parametric oscillator (NesCOPO), i.e. based on the OPO of two separate resonant cavities, each of which exhibits resonance at one of the wavelengths generated by second order parametric conversion. This OPO is a double resonance type with double pass of the pump wave.

European patent application EP2503387 describes a NesCOPO parametric oscillator that employs a continuously variable pitch lithium niobate fan-out crystal. The disadvantages of such an oscillator are: including crystals whose ferromagnetic domains are not optimally oriented, which results in a wave number that the source cannot emit without changing parameters (e.g., the temperature of the crystal).

The optical parametric oscillator according to the invention comprises a crystal whose ferromagnetic pattern has been optimized to provide for the adoption of the entire desired wavelength range without having to modify certain crystal-related parameters, such as temperature.

The terms "upper", "lower", "front" and "rear" must be interpreted as if the crystal were placed in an operational position in the optical cavity of the optical parametric oscillator.

An object of the present invention is an optical parametric oscillator of a double resonance type, which includes a fan-out type crystal having second-order optical nonlinearity and disposed in an optical cavity capable of reflecting a pump wave, the crystal including an incident surface and an exit surface, an upper surface and a lower surface, and an optical axis passing through the incident surface and the exit surface.

The optical parametric oscillator according to the present invention is mainly characterized in that the crystal comprises a grid of polarity-inverted lines, the polarity-inverted lines starting separately and at narrow intervals from an upper virtual straight line parallel to the upper face of the crystal and ending separately and at wide intervals from a lower virtual straight line parallel to the lower face of the crystal or from the entrance face of the crystal, two successive lines forming a constant angle between each other, the grid starting from a first line, the first line starting from the exit face of the crystal and extending towards a lower virtual straight line while diverging from the exit face, all other lines being gradually and monotonically inclined from the first line towards the entrance face of the crystal.

In other words, a first line of the grid starts at and diverges from the exit face of the crystal, and all other lines are inclined from this first line towards the entrance face of the crystal in a manner that increasingly diverges from the exit face. The first line is the only one starting from the exit face, all other lines of the grid being away from the exit face. In other words, the grid of lines gives the impression that it rotates from the exit face of the crystal towards the entrance face of the crystal, starting with the first line having only one point of contact with the exit face of the crystal. It is noted that all lines of the grid start from the upper virtual straight line, including the first polarity-reversing line.

Advantageously, the four faces of the crystal are planar.

Preferably, the upper and lower faces are parallel, and the entrance face and the exit face are parallel. In this way, the crystal is parallelepiped-shaped with a small thickness.

Preferably, the polarity-reversing line is located immediately after the first line and the first line also ends at the lower virtual straight line, and the subsequent lines all end at the incident surface. The expression "end at the entrance face" must be understood to mean "present at the entrance face".

Advantageously, the constant angle of inclination between two successive wires is about 0.1 mrad. The expression "about 0.1 mrad" means equal to 0.1mrad +/-0.05 mrad.

Preferably, the crystal is made of lithium niobate. This material is particularly, but not exclusively, suitable for an optical parametric oscillator according to the invention.

Preferably, the grid comprises an original line placed before the first line, said original line starting from the exit face below the upper virtual straight line and ending at the lower virtual straight line.

Advantageously, the first line is inclined at an angle greater than or equal to a constant angle with respect to the exit face, so as to separate two successive lines. The angle of inclination is preferably between 1 and 2 times the constant angle of inclination between two successive lines of the grid.

Another object of the present invention is a crystal for manufacturing an optical parametric oscillator according to the present invention, the crystal comprising an entrance face and an exit face, an upper face and a lower face, an optical axis passing through the entrance face and the exit face.

The crystal according to the invention is primarily characterized in that it comprises a grid of lines of polarity inversion starting at narrowly spaced intervals from an upper virtual straight line parallel to the upper face of the crystal and ending at widely spaced intervals at a lower virtual straight line parallel to the lower face of the crystal or at the entrance face of the crystal, two successive lines forming a constant angle between each other, the grid starting from a first line starting at the exit face of the crystal and extending towards the lower virtual straight line, all other lines being gradually and monotonically inclined from the first line towards the entrance face of the crystal.

The optical parametric oscillator according to the present invention has the following advantages: each wavenumber in a given wavelength range can be obtained, eliminating the unusable area observed with the existing optical parametric vibrators. This achievement is obtained with a specific design of the polarity inversion line of the grid, thus allowing to avoid the need to set the crystal temperature.

Drawings

A detailed description of an optical parametric oscillator according to the present invention is given below with reference to the following drawings:

figure 1 is a schematic diagram of a prior art optical parametric oscillator,

figure 2 is a front view of a fan-out crystal used in a prior art optical parametric oscillator,

FIG. 3 is a graph showing an example of the achievable wavenumber as a function of the position of the crystal of FIG. 2 in the optical cavity in a prior art OPO,

FIG. 4 is a front view of a fan-out crystal according to the invention,

fig. 5 is a graph showing an example of the achievable wavenumber as a function of the position of the crystal of fig. 4 in the optical cavity.

Detailed Description

In the remainder of the description, the terms "OPO" and "optical parametric oscillator" are equivalent.

Referring to fig. 1, an optical parametric oscillator 1 is a system that allows a pump wave 2 generated by a laser beam to be converted into two waves, a "signal" wave 3 and an "idler" wave 4, by a nonlinear crystal 5 (which may be made of lithium niobate, for example). The crystal 5 is placed in an optical cavity 6 defined by a first mirror M1 and a second mirror M3. The two mirrors M1 and M3 are mounted on the piezoelectric element 7 so as to allow the optical cavity 6 to be tuned. In the example shown in fig. 1, the crystal 5 includes a third mirror M2. The pump wave 2 is converted within a crystal 5 placed in an optical cavity 6. In the context of an OPO 1 according to the invention, the crystal 5 is Periodically Poled Lithium Niobate (PPLN).

The architecture of the OPO 1 according to the invention is also referred to by the abbreviation NesCOPO (nested cavity) optical parametric oscillator). The pump wave 2 has an incident component 8 originating from the first mirror M1 and a reflected component 9 obtained after reflection of said incident wave 8 from the second mirror M3 of the optical cavity 6. As an illustrative and non-limiting example, the wavelength of the pump wave 2 is 1 μm, the wavelength of the signal wave 3 is in the range of 1.4 μm to 1.6 μm, and the wavelength of the idler wave 4 is in the range of 3.2 μm to 4.2 μm.

The OPO 1 according to the present invention utilizes a non-linear frequency conversion within a crystal 5 placed in an optical cavity 6. The OPO 1 is a double resonance type having double pass (incident component 8 and reflected component 9) of the pump wave 2.

Referring to fig. 2, a conventional fan-out crystal 55 has a grid of polarity-reversal lines 56, these polarity-reversal lines 56 allowing a continuous change in the generated wavelength to be obtained by moving the crystal 55 within the optical cavity 6. Such a crystal 55 has, schematically, a parallelepiped shape and has:

-an upper face 57 of the plane surface,

a planar lower face 58, which is parallel to the upper face 57,

a planar entrance face 59, through which entrance face 59 the pump wave 2 passing through the first mirror M1 will enter the crystal 55,

a planar exit face 60, which is parallel to the entrance face 59,

two rectangular and parallel side faces 61, each delimited by an upper face 57, a lower face 58, an entrance face 59 and an exit face 60.

Such a crystal 55 may for example have a length L of 10mm, a width L of 5mm and a thickness of 1 mm. These dimensions show examples of OPOs suitable according to the invention, but these are non-limiting.

The polarity inversion lines 56 are organized within the crystal 55 such that they begin at an upper virtual straight line 61 parallel to the upper wall 57 and located near the upper wall 57. These lines 56 start separately and in narrowly spaced manner on said straight line 61 and over the entire width of the crystal 55. The centre line 62 starts from the middle of the upper straight line 61 and extends parallel to the entrance face 59 or the exit face 60 towards a lower virtual straight line 63, which lower virtual straight line 63 is parallel to the upper virtual straight line 61 and located near the lower face 58 of the crystal 55. Some of the lines 56 on the upper virtual straight line 61 on one side of the centre line 62 extend towards the lower virtual straight line 63, those lines being the lines closest to said centre line 62, while the other lines extend towards the exit face 60, those lines being the lines furthest from said centre line 62. Some of the lines 56 on the other side of the centre line 62 on the upper virtual straight line 61 extend towards the lower virtual straight line 63, those lines being the lines closest to said centre line 62, while the other lines extend towards the entrance face 59, those lines being the lines furthest away from said centre line 62. Two successive lines 56 of the grid diverge from each other as they extend from a position on an upper virtual straight line 61 towards a lower virtual straight line 63 or towards the entrance face 59 or the exit face 60. In this way, two successive lines of polarity inversion 56 form a constant angle therebetween, which is preferably equal to 0.1 mrad.

In summary, the grid of lines 56 has an axis of symmetry represented by a centerline 62, some of the lines 56 (those lines lying on one side of the centerline 62) having a tendency to extend toward the entrance face 59, and the remaining lines of the lines 56 (those lines lying on the other side of the centerline 56) having a tendency to extend toward the exit face 60.

The pump wave 2 (the beam size of which may be, for example, about 100 μm) reaches the entrance face 59 and passes through the crystal 55 to exit the crystal 55 via the exit face 60. The crystal 55 can be translated along the longitudinal axis of said crystal 55 within the optical cavity 6 in order to vary the parameters of the conversion and obtain a given wavenumber.

Now, referring to fig. 3, with such a fan-out crystal 55, the conversion conditions within the NesCOPO generally only allow certain wavelength ranges 64 to be obtained, separated by ranges 65 that are not available, since the holes in the graph indicate the various positions of the crystal 55 in the optical cavity 6. In particular, the crystal 55 can be translated within the optical cavity 6 along an axis parallel to the longitudinal axis of said crystal 55, so as to obtain all the possible wavelengths within a given range. However, the available regions do not overlap, and the occurrence of unachievable wave numbers is observed. This is a result of the relative phase conditions between the three waves (pump, signal, idler), which is important to consider in NesCOPO.

There are currently methods of avoiding these holes 65, but they are either very expensive, not industrially applicable, or slow.

The OPO according to the invention comprises a crystal 105, the polarity-reversal line 106 of which is organized in the crystal 105 in the following way: such that they allow all wavelengths to be obtained when the crystal 105 is translated along the longitudinal axis of the crystal 105 within the optical cavity 6.

Referring to fig. 4, the crystal 105 of the OPO according to the present invention is different from the above-described crystal only in the arrangement of the polarity inversion line 106 within the crystal 105. Specifically, the polarity-reversing lines 106 are organized within the crystal 105 such that they begin at an upper virtual straight line 61 parallel to the upper wall 57 and located near the upper wall 57. These lines 106 start separately and in narrowly spaced manner on said straight line 61 and over the entire width of the crystal 105. Each polarity reversal line 106 of the grid of crystals 105 of the OPO according to the present invention is obtained by rotating in a clockwise direction by a constant angle of between 1 ° and 10 ° around the intersection of each polarity reversal line with the upper virtual straight line 61, starting from each polarity reversal line 56 of the grid of crystals 55 described above. In this manner, each polarity inversion line 106 of crystal 105 according to the present invention is pivoted at an angle of between 1 ° and 10 ° from its position in prior crystal 55 shown in fig. 2 toward entrance face 59. For a crystal having a length of 10mm, a width of 5mm and a thickness of 1mm, the angle is preferably equal to 2.8 °.

In other words, the grid of lines of polarity inversion 106 starts from a first line 108, which first line 108 starts at the exit face 60 of the crystal 105 at the upper virtual straight line 61 and extends towards the above-mentioned lower virtual straight line 63, all other lines being gradually and monotonically inclined from said first line 108 towards the entrance face 59. Two successive lines 106 diverge from each other as they extend from a position on upper virtual straight line 61 toward lower virtual straight line 63 or toward incident surface 59. In this way, two successive lines of polarity inversion 106 form a constant angle between each other, preferably equal to 0.1mrad, as in the prior art crystal 55 described above. The line 106 immediately after the first line 108 extends to the lower virtual straight line 63, while the other lines appear on the entrance face 59 of the crystal 105.

The grid further comprises an original line 109 placed between the first line 108 and the exit face 60, which original line 109 starts at the exit face 60 below the starting point of the first line 108 on said exit face 60 and ends on the lower virtual straight line 63. The original line 109 is shorter than the first line 108.

In summary, in the crystal 105 according to the present invention, all the polarity inversion lines 106 are inclined in the same direction and on the same side (toward the incident surface 59) with respect to the axis extending along the exit surface 60. In the conventional crystal 55, they are inclined symmetrically on both sides of the axis with respect to the central axis parallel to the incident surface 59 or the exit surface 60 and in two opposite directions (toward the incident surface 59 and the exit surface 60).

A typical period of the pattern in the PPLN crystal 105 is 30 μm.

Referring to fig. 5, the OPO according to the invention allows to obtain all wavelengths within a given range by translating the crystal 105 along an axis parallel to the exit face 60 or the entrance face 59. Specifically, various experiments have shown that each wave number can be reached by using a PPLN crystal 105 with a new grid of polarity inversion lines 106 as described above. Looking at location 120 in crystal 105 where the phase matching condition is completely non-constructive, the desired wavelength can still be obtained due to the overlap of available areas 121.