• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
  • 同族专利
  • 引用文献
  • 法律状态
  • 优先权
    • 专利摘要:
    - The active element plate (1) for laser source comprises at least one input surface (5) of a pumping beam, a first portion (2) rod-shaped elongated along a longitudinal axis (4) which includes a first doped matrix (2a) capable of absorbing the pump beam to amplify longitudinally propagating laser radiation, a second portion (3) at least partially covering the first portion (2), the second portion (3) including a second doped matrix (3a, 3b) capable of absorbing the laser radiation and being transparent to the pump beam.
    公开号:FR3066330A1
    申请号:FR1700512
    申请日:2017-05-12
    公开日:2018-11-16
    发明作者:David Sabourdy；Jean-Eucher Montagne；Alexandre Martins-Santana；Guy Nguyen
    申请人:Compagnie Industriel des Lasers CILAS SA；
    IPC主号:
    专利说明:

    TECHNICAL AREA
    The present invention relates to the field of plates (or "slab" in English) of active element for laser source as well as a laser source comprising such a plate.
    STATE OF THE ART
    A laser source generally comprises a resonant cavity in which an amplifying medium is located. The excitation of the amplifying medium (or active medium) is obtained by a pumping beam emitted by a pumping source. The pumping beam allows a population inversion favoring a stimulated emission generating the laser radiation.
    The compactness of a laser source is an important issue when this source equips a device that must be compact. The dimensions of the laser source can be a major drawback when the device is portable.
    In addition, when the device is subjected to temperature variations, it is important that the laser source is not very sensitive to these variations. In the case of solid lasers pumped by diode, this last point can be critical taking into account that the central wavelength of the standard laser diodes derives from approximately 0.25 nm / ° C. Depending on the profile of the absorption spectrum of the doping ions considered, the laser energy can then be affected.
    For example, there are lasers pumped by diodes called athermal lasers.
    In general, the principle of these sources is based on a longitudinal pumping of doped amplifier bars. The pump is then guided in the bar so that the absorption length varies according to the operating temperature and the associated absorption coefficient. Generally, the pumping beam comes from a stack of diodes and then collected by an optical device to be injected at the input of the amplifier bar.
    For example, in the case of the longitudinal pumping of an Nd doped YAG crystal bar of length 80 mm, necessary to absorb at least 90% of the pumping beam, the total length of the pumping and amplifier bar assembly may reach 130 mm.
    In this configuration, a significant part of the cavity length is dictated by the dimensions of the active medium and of its associated pumping source generating the pumping beam.
    Although this type of solution works satisfactorily, a more compact and efficient solution would be preferable.
    STATEMENT OF THE INVENTION
    The object of the present invention is to overcome this drawback by proposing a solution which makes it possible to obtain a laser source of small dimensions, little sensitive to changes in temperature. To this end, the invention relates to an active element plate for a laser source.
    According to the invention, the active element plate comprises: - at least one entry surface of a pumping beam, - a first part in the form of a bar elongated along a longitudinal axis which includes a first doped matrix capable of absorbing the pumping beam to amplify longitudinally propagating laser radiation, - a second part covering at least partially the first part, the second part including a second doped matrix capable of absorbing the laser radiation and of being transparent to the pumping beam .
    Thus, thanks to the matrix of the second part capable of absorbing laser radiation, it is possible to reduce the parasitic emission modes while limiting the losses.
    According to one feature, the first doped matrix has a refractive index substantially equal to the refractive index of the second doped matrix.
    According to one feature, the first doped matrix and the second doped matrix have refractive indices greater than a refractive index of a medium in which the plate is likely to be used.
    According to a variant, the first doped matrix has a doping concentration which evolves along the longitudinal axis so that the doping concentration at a first end of the first part close to the entry surface (s) is less important than the doping concentration at a second end furthest from the entry surface (s).
    According to another variant, the first doped matrix has a doping concentration which changes radially so that the doping concentration in a central zone of the first part parallel to the longitudinal axis is greater than the doping concentration in a zone further from the central area.
    According to one embodiment, the first part in the form of an elongated bar has a square cross section, the second part comprising two portions of rectangular cross sections between which the first part is sandwiched.
    According to another embodiment, the first part in the form of an elongated bar has a circular cross section, the second part comprising two portions of semi-annular cross section conforming to the shape of the first part sandwiched between the two portions of the second part.
    According to another embodiment, the second part has a thickness greater than the thickness of the first part.
    According to one configuration, the second part comprises two entry surfaces of the pumping beam arranged symmetrically with respect to the longitudinal axis at a first end of the plate, the two entry surfaces being inclined with respect to the longitudinal axis.
    According to another configuration, the second part comprises four entry surfaces of the pumping beam, two entry surfaces of the pumping beam being arranged symmetrically with respect to the longitudinal axis at a first end of the plate and two surfaces of inlet of the pumping beam being arranged symmetrically with respect to the longitudinal axis at a second end of the plate, the four inlet surfaces being inclined with respect to the longitudinal axis.
    According to one embodiment, the plate also comprises at least a third portion in the form of a bar elongated along the longitudinal axis which includes a third doped matrix capable of absorbing the pumping beam to amplify laser radiation propagating longitudinally.
    For example, the first doped matrix comprises a garnet of yttrium-aluminum doped with neodymium.
    In addition, the second doped matrix includes a samarium-doped crystal. The invention also relates to a laser source comprising: - an active element plate for a laser source, - at least one pumping source capable of emitting a pumping beam penetrating into the active element plate,
    According to the invention, the active element plate is an active element plate of the type of that specified above.
    According to one feature, the pumping source or sources comprise at least one laser diode.
    BRIEF DESCRIPTION OF THE FIGURES The invention, with its characteristics and advantages, will emerge more clearly on reading the description made with reference to the appended drawings in which: - Figure 1 represents an active element plate according to one embodiment; - Figure 2 shows an active element plate according to another embodiment, - Figure 3a shows a view of the active element plate in a direction parallel to the longitudinal axis according to an embodiment, - Figure 3b shows a view of the active element plate in a direction perpendicular to the longitudinal axis, - Figure 3c shows a view of the active element plate in a direction parallel to the longitudinal axis according to another embodiment , - Figure 4 shows a part of an active element plate according to one embodiment.
    DETAILED DESCRIPTION
    The remainder of the description will refer to the figures cited above. The invention relates to an active element plate 1 for a laser source. In the following description, the active element plate 1 can also be called plate 1.
    The active element plate 1 comprises: - at least one entry surface 5 of a pumping beam, - a first part 2 in the form of a bar which is elongated along a longitudinal axis 4. This first part 2 includes a first doped matrix 2a capable of absorbing the pumping beam to amplify a laser radiation propagating along the longitudinal axis 4, - a second part 3 covering at least partially the first part, the second part including a second doped matrix 3a, 3b susceptible absorb laser radiation and be transparent to the pumping beam.
    Thus, the pumping beam emitted by a pumping source 6 specified below can penetrate into the first doped matrix 2a through the second doped matrix 3a, 3b which is transparent to the pumping beam. The pumping beam having entered the first doped matrix 2a can then be absorbed by the first doped matrix 2a. The first doped matrix 2a can then emit and amplify the laser radiation which propagates longitudinally at the bar (that is to say substantially along the longitudinal axis 4). The second doped matrix 3a, 3b is capable of absorbing laser radiation in order to limit the appearance of amplified spontaneous emissions (ASE) and parasitic emission modes.
    Preferably, the absorption rate by the second doped matrix 3a, 3b is greater than 80%.
    Advantageously, the first matrix 2a is doped with luminescent ions such as the neodymium ion (Nd), the ytterbium ion (Yb), I erbium ion (Er), the thulium ion (Tm), the holmium ion ( Ho) or any other luminescent ion.
    According to one embodiment, the first doped matrix 2a and the second doped matrix 3a, 3b have refractive indices greater than a refractive index of a medium in which the plate 1 is capable of being used. This jump in index between the two doped matrices 2a and 3a, 3b and the medium in which the plate 1 is likely to be used allows the confinement of the pumping beam in the plate 1.
    According to a variant, the first doped matrix 2a has a doping concentration which evolves along the longitudinal axis 4. The doping concentration evolves so that it is less significant at a first end 11 of the first part 2 close to the entry surface (s) 5 as that located at a second end 12 furthest from the entry surface (s) 5.
    According to another variant, the first doped matrix 2a has a doping concentration which evolves radially so that the doping concentration in a central zone of the first part 2 parallel to the longitudinal axis 4 is greater than the doping concentration in region furthest from the central region.
    Whether radially or along the longitudinal axis, the doping concentration can change continuously. The doping concentration can also evolve discreetly in steps or by concentration jump.
    The two variants of doping concentration evolution can be combined.
    According to one embodiment, the first part 2 is sandwiched by the second part 3. The second part 3 thus comprises two portions 3a, 3b between which the first part 2 is inserted.
    According to a preferred embodiment, the first part 2 in the form of an elongated bar has a cross section of square or rectangular shape. The second part 3 comprises two portions 3a, 3b of rectangular sections. The first part 2 is sandwiched between the two portions 3a, 3b. Without limitation, the square section of the first part 2 has a side S1 between 2 mm and 8 mm, preferably a side of 3.5 mm.
    According to another embodiment, the elongated bar-shaped part has a cross section of circular shape. The second part 3 comprises two portions 3a, 3b of semi-annular cross section. The first part 2 is sandwiched between the two portions 3a, 3b of the second part 3 so that the convex circular side of each portion 3a, 3b follows the circular shape of the first part 2. In a nonlimiting manner, the section transverse circular shape of the first part 2 has a diameter between 2 mm and 8 mm, preferably a diameter of 4 mm.
    According to another embodiment (FIG. 3c), the second part 3 has a thickness E greater than the thickness of the first part 2.
    In a nonlimiting manner, the section of square shape or of circular shape of the first part 2 has a side S1 of dimension equal to 3.5 mm while the second part 3 has a thickness E of dimension equal to 5 mm.
    Advantageously, the first part 2 is arranged in the second part 3 in an opposite manner as illustrated in FIG. 3c.
    Advantageously, two opposite surfaces corresponding to the surfaces comprising the junction between parts 2 and 3 and having the largest dimensions are covered with a reflective layer, called the guide layer 7, as shown in FIG. 3. This guide layer 7 allows to keep the pumping beam confined in the first part 2 and the second part 3. In a nonlimiting manner, the guide layer 7 has a refractive index lower than the refractive index of the first doped matrix 2a and of the second doped matrix 3a, 3b. Preferably, the guide layer 7 has a refractive index of 1.45. The guide layer 7 can be applied to said surfaces by thin layer deposition techniques, for example.
    Advantageously, these surfaces can be used to interface the plate 1 with heat sinks in order to thermalize the amplifying medium.
    Without limitation, for a bi-wavelength pumping beam emitting at 801 nm and 806 nm, the plate 1, the second part 2 of which comprises an Nd doped YAG crystal, has a length L in a range from from 45 mm to 65 mm, preferably 60 mm. This length L can allow more than 80% of the pumping beam to be absorbed in the first doped matrix 2a over an operating temperature range around 100 ° C.
    In a first preferred embodiment, as shown in FIG. 1, the second part 3a, 3b comprises at least one entry surface 5 of the pumping beam at the first end 11 of the plate 1. Preferably, the second part 3a, 3b comprises at least two entry surfaces 5. The two entry surfaces 5 are arranged symmetrically with respect to the longitudinal axis 4. They are further inclined with respect to this longitudinal axis 4. The angle of inclination a is such that the pumping beam entering the plate 1 is guided by total internal reflection and performs at least a double pass in the first part 2. The pumping beam is thus trapped in the plate 1 and is absorbed by the first doped matrix 2a of the first part 2 during its propagation.
    In a second embodiment, as shown in FIG. 2, the second part 3 comprises four entry surfaces 5 for the pumping beam. Two inlet surfaces 5 of the pumping beam are arranged symmetrically with respect to the longitudinal axis 4 at the first end 11 of the plate 1. Two other inlet surfaces 5 of the pumping beam are arranged symmetrically with respect to the longitudinal axis 4 at the second end 12 of the plate 1. The four entry surfaces 5 are inclined relative to the longitudinal axis 4. According to a preferred variant, the angle of inclination a of two entry surfaces at a first end 11 of the plate 1 is equal to the angle of inclination a of the two input surfaces 5 to the second end 12 of the plate 1. According to another variant, the angle of inclination a of two surfaces entry 5 at the first end 11 of the plate 1 is different from the angle of inclination a of the two entry surfaces 5 at the second end 12 of the plate 1. According to a preferred variant, the inclination angles its has 5 entry surfaces of one end are equal. According to another variant, the angles of inclination at the entry surfaces 5 of one end are not equal.
    Without limitation, the angle of inclination a is in a range from 35 ° to 45 °, preferably 40 °. This angle can be valid in the case of a YAG plate 1, the second part 3 of which is in contact with a medium with a refractive index substantially equal to 1.
    Without limitation, the dimensions of each entry surface 5 have a width substantially equal to the thickness E of the plate 1 (FIGS. 3a and 3b) and a length D lying in a range from 5 mm to 12 mm, preferably 6 mm (Figures 1 and 3b), depending on the type of diodes used. In order to optimize the absorption of the pumping beam in the first doped matrix 2a, a length D of 5 mm is preferred. The length D depends on the size of the pumping source. For example, for a given pumping source dimension, the length D of the inlet surface 5 corresponds to the dimension of the pumping source increased by 1 mm.
    According to one feature, the first doped matrix 2a comprises a garnet of yttrium-aluminum doped with neodymium.
    Without limitation, the first doped matrix 2a has a doping with neodymium ions of between 0.1% and 1%, preferably 0.5%.
    According to another particular feature, the second doped matrix 3a, 3b comprises a crystal doped with samarium. This doping in the samarium makes it possible to effectively control parasitic emissions such as amplified spontaneous emissions.
    Without limitation, the second matrix 3a, 3b is doped with samarium at a rate between 1% and 15%, preferably 5%. A doping at 5% generates an absorption greater than 2 cm'1 at 1064 nm and no absorption on the band from 750 nm to 850 nm.
    With a plate 1 having a first doped matrix 2a comprising a yttrium-aluminum garnet doped with neodymium and a second doped matrix 3a, 3b comprising a crystal doped with samarium, it is possible to obtain a beam absorption rate of pumping by the first doped matrix 2a of around 77% at a temperature of -30 ° C, a rate of around 90% at a temperature of 20 ° C and a rate of around 87% at 70 ° C.
    Due to the transverse component of the pumping beam, the ion doping is preferably adjusted so that the gain integrated over the length of the bar has a homogeneous distribution and does not have an overcurrent on the edges of the bar. The distribution can be adjusted using a multi-wavelength pumping beam.
    According to one embodiment, the parts 2, 3 of the plate 1 are produced by a ceramic process.
    According to another embodiment, the parts 2, 3 of the plate 1 are made from single crystals. In this latter embodiment, the first part 2 must adhere to the second part 3 with the risk that a certain amount of micro-defects is present per unit of surface at the interfaces.
    According to one embodiment (FIG. 4), the plate 1 also comprises at least a third part 7 in the form of a bar elongated along the longitudinal axis 4 which includes a third doped matrix 7a capable of absorbing the pumping beam to amplify longitudinally propagating laser radiation. Preferably, the third part is the same type as the first part 2 with a third doped matrix 7a and 7b in the same way as the first doped matrix 2a. This forms a plate comprising a set of several amplifying media separated by one or more doped or undoped zones.
    The plate 1 as described above can be integrated into a laser source.
    Thus, the laser source (not shown) comprises: - an active element plate 1 for laser source of the type described above, - at least one pumping source 6 capable of emitting a pumping beam penetrating into the active element plate 1.
    In a preferred embodiment, the pumping source or sources 6 comprise at least one laser diode. Preferably, the pumping source or sources 6 comprise at least one stack of diodes. Preferably, the input surfaces 5 have dimensions adjusted to the surface of the diode stacks.
    Different stacking of diodes can be envisaged, such as 10 mm, 5 mm or 3 mm strips.
    Preferably, the laser source comprises two stacks of diodes composed of a plurality of strips 5 mm wide. This leads to a potential peak power of several kilowatts. In a nonlimiting manner, these bars are multi-wavelength. For example, they can be bi-wavelength at 801 nm and 806 nm or tri-wavelength at 793 nm, 807 nm and 809 nm. In addition, the gap between each strip of a diode stack can have an available value of between 150 μm and 1.6 mm depending on the need and the manufacturers.
    Advantageously, the emitting surfaces of the pumping sources are positioned at a distance D1 from each input surface 5 of the second part 3. In a nonlimiting manner, the distance D1 is substantially equal to 500 μm.
    Thus, without limitation, the laser source may have a length of up to approximately 73 mm; which gives a gain in length of 1.78 compared to the laser sources of so-called athermal designators.
    The present description details various embodiments with reference to figures and / or technical characteristics. Those skilled in the art will understand that the various technical characteristics of the various modes can be combined with one another to obtain other embodiments, unless the reverse is explicitly mentioned or these technical characteristics are incompatible. Likewise, a technical characteristic of an embodiment can be isolated from the other technical characteristics of this embodiment unless the reverse is mentioned. In this description, many specific details are provided by way of illustration and in no way limitative, so as to detail the invention precisely. Those skilled in the art will however understand that the invention can be carried out in the absence of one or more of these specific details or with variants. On other occasions, certain aspects are not detailed so as to avoid obscuring and weighing down the present description and the person skilled in the art will understand that various and varied means may be used and that the invention is not limited only to the examples described.
    It should be obvious to those skilled in the art that the present invention allows embodiments in many other specific forms without departing from the scope of the invention as claimed. Therefore, the present embodiments should be considered by way of illustration, but may be modified in the field defined by the scope of the appended claims, and the invention should not be limited to the details given above.
    权利要求:
    Claims (15)
    [1" id="c-fr-0001]
    1. Active element plate for laser source, characterized in that it comprises: - at least one entry surface (5) of a pumping beam, - a first part (2) in the form of an elongated bar according to a longitudinal axis (4) which includes a first doped matrix (2a) capable of absorbing the pumping beam to amplify longitudinally propagating laser radiation, a second part (3) at least partially covering the first part (2), the second part (3) including a second doped matrix (3a, 3b) capable of absorbing the laser radiation and of being transparent to the pumping beam.
    [2" id="c-fr-0002]
    2. Plate according to claim 1, characterized in that the first doped matrix (2a) has a refractive index substantially equal to the refractive index of the second doped matrix (3a, 3b).
    [3" id="c-fr-0003]
    3. Plate according to any one of claims 1 or 2, characterized in that the first doped matrix (2a) and the second doped matrix (3a, 3b) have refractive indices greater than a refractive index of a medium in which the plate (1) can be used.
    [4" id="c-fr-0004]
    4. Plate according to any one of claims 1 to 3, characterized in that the first doped matrix (2a) has a doping concentration which evolves along the longitudinal axis (4) so that the doping concentration at a first end (11) of the first part (2) close to the entry surface (s) (5) is less important than the doping concentration at a second end (12) furthest from the surface (s) entrance (5).
    [5" id="c-fr-0005]
    5. Plate according to any one of claims 1 to 4, characterized in that the first doped matrix (2a) has a doping concentration which changes radially so that the doping concentration in a central area of the first part (2 ) parallel to the longitudinal axis (4) is greater than the doping concentration in a zone furthest from the central zone.
    [6" id="c-fr-0006]
    6. Plate according to any one of claims 1 to 5, characterized in that the first part (2) in the form of an elongated bar has a square cross section, the second part (3) comprising two portions of rectangular cross sections between which the first part (2) is sandwiched.
    [7" id="c-fr-0007]
    7. Plate according to any one of claims 1 to 6, characterized in that the first part (2) in the form of an elongated bar has a circular cross section, the second part (3) comprising two portions (3a, 3b) of semi-annular cross section conforming to the shape of the first part (2) sandwiched between the two portions (3a, 3b) of the second part (3).
    [8" id="c-fr-0008]
    8. Plate according to any one of claims 1 to 7, characterized in that the second part (3) has a thickness (E) greater than the thickness of the first part (2).
    [9" id="c-fr-0009]
    9. Plate according to any one of claims 1 to 8, characterized in that the second part (3) comprises two surfaces (5) for entering the pumping beam arranged symmetrically with respect to the longitudinal axis (4) at a first end (11) of the plate (1), the two inlet surfaces (5) being inclined relative to the longitudinal axis (4).
    [10" id="c-fr-0010]
    10. Plate according to any one of claims 1 to 9, characterized in that the second part (3) comprises four inlet surfaces (5) of the pumping beam, two inlet surfaces (5) of the pumping beam being arranged symmetrically with respect to the longitudinal axis (4) at a first end (11) of the plate (1) and two inlet surfaces (5) of the pumping beam being arranged symmetrically with respect to the longitudinal axis ( 4) at a second end (12) of the plate (1), the four inlet surfaces (5) being inclined relative to the longitudinal axis (4).
    [11" id="c-fr-0011]
    11. Plate according to any one of claims 1 to 10, characterized in that it further comprises at least a third part (7) in the form of a bar elongated along the longitudinal axis (4) which includes a third doped matrix (7a, 7b) capable of absorbing the pumping beam to amplify longitudinally propagating laser radiation
    [12" id="c-fr-0012]
    12. Plate according to any one of claims 1 to 11, characterized in that the first doped matrix (2a) comprises a yttrium-aluminum garnet doped with neodymium.
    [13" id="c-fr-0013]
    13. Plate according to any one of claims 1 to 12, characterized in that the second doped matrix (3a, 3b) comprises a crystal doped with samarium.
    [14" id="c-fr-0014]
    14. Laser source comprising: - an active element plate (1) for a laser source, - at least one pumping source (6) capable of emitting a pumping beam penetrating into the active element plate (1), characterized in that the active element plate (1) is an active element plate of the type of that specified under any one of claims 1 to 13.
    [15" id="c-fr-0015]
    15. Laser source according to claim 14, characterized in that the pumping source or sources (6) comprise at least one laser diode.
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    同族专利:
    公开号 | 公开日
    US20180331487A1|2018-11-15|
    US10367325B2|2019-07-30|
    FR3066330B1|2019-09-13|
    EP3402015A1|2018-11-14|
    EP3402015B1|2021-01-06|
    CN108879299A|2018-11-23|
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    法律状态:
    2018-05-28| PLFP| Fee payment|Year of fee payment: 2 |
    2018-11-16| PLSC| Search report ready|Effective date: 20181116 |
    2019-05-31| PLFP| Fee payment|Year of fee payment: 3 |
    2020-05-30| PLFP| Fee payment|Year of fee payment: 4 |
    2021-05-31| PLFP| Fee payment|Year of fee payment: 5 |
    优先权:
    申请号 | 申请日 | 专利标题
    FR1700512A|FR3066330B1|2017-05-12|2017-05-12|ACTIVE ELEMENT PLATE FOR LASER SOURCE AND LASER SOURCE COMPRISING SUCH A PLATE|
    FR1700512|2017-05-12|FR1700512A| FR3066330B1|2017-05-12|2017-05-12|ACTIVE ELEMENT PLATE FOR LASER SOURCE AND LASER SOURCE COMPRISING SUCH A PLATE|
    EP18290047.2A| EP3402015B1|2017-05-12|2018-05-07|Active element plate for laser source and laser source comprising such a plate|
    US15/976,032| US10367325B2|2017-05-12|2018-05-10|Active element slab for a laser source|
    CN201810448580.9A| CN108879299A|2017-05-12|2018-05-11|Active component lath for laser source|
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