CN204758926U - Expand and restraint collimation optical system - Google Patents
Expand and restraint collimation optical system Download PDFInfo
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- CN204758926U CN204758926U CN201520468124.2U CN201520468124U CN204758926U CN 204758926 U CN204758926 U CN 204758926U CN 201520468124 U CN201520468124 U CN 201520468124U CN 204758926 U CN204758926 U CN 204758926U
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- collimation
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Abstract
The utility model discloses an expand and restraint collimation optical system and preparation method. Optical system include that preceding group transmission is expanded and restraint collimation group and expand with back group reflection and restraint collimation group, press the light incidence orientation, the transmission is expanded and is restrainted collimation group including a biconcave burden mirror, a biconvex direct position of telescope and two curved month direct position of telescopes, the curved phototropic incident direction of camber of two curved month direct position of telescopes, the reflection is expanded bundle collimation group and including two paraboloidal mirrors that have the same focus position, is small -bore paraboloidal mirror and heavy -calibre paraboloidal mirror in proper order, and the shape of face of heavy -calibre paraboloidal mirror is the off -axis concave surface. The utility model provides an expand the collimation system of restrainting, can expand and restraint for the arbitrary laser wavelength of broadband within range or white light laser provide the collimation, and not need any removal compensating unit. Its compact structure, it is small, expand and restraint that the multiplying power is big, the collimation performance is high, can be used to fields such as holographic imaging, optical test, laser radar.
Description
Technical field
The utility model relates to a kind of broadband high magnification beam spread collimation optical system of compact.
Background technology
In many application scenarios such as optical detection, spectral calibration, laser radar, security protections, need to carry out to light beam the very small angles transmitting that shaping realizes light beam, thus realize long range propagation or the optimum coupling of light beam.The system beam-expanding collimation of current optics can be divided into two types, and a kind of is laser beam application and development for single wave band, and the beam-expanding collimation system of its correspondence has transmission-type, reflective and both combining form; Another is for laser application under multiple wavelength, and this structure is in the constant situation of maintenance optical component parameter, and the spacing changing eyepiece and object lens adapts to different wavelength.Last type, because being only suitable for single wavelength, is easy to the requirement of satisfied large multiplying power or conversion multiplying power; A rear type, for the laser instrument of multiple wavelength, its large multiplying power expands and is not easy to realize, change eyepiece and object lens spacing is needed to adapt to, namely the pitch requirements under different optical maser wavelength can be met by the special adjusting mechanism of design or the way that adds spacer ring, as document " Design of Transmitting Beam Expander for Different Waves " (the infrared and laser of J., vol37, No.7) adopt complicated transmissive design realize three wavelength beam-expanding collimation.When adjusting object lens and width between eyepiece, the spacing accuracy of system, the depth of parallelism and right alignment etc. can bring error, impact collimation performance.And along with the application of continuous or white light laser and some particular application thereof, need the beam spread collimation optical system be suitable for the laser beam of continuous wavelength in broadband scope, the way of this change spacing just cannot meet.
Summary of the invention
The deficiency that the utility model exists for prior art, a kind of broadband high magnification beam spread collimation optical system is provided, this optical system is applicable to the laser instrument of multiple wavelength, and need not mobile eyeglass thus adjustment lenticular spacing adapts to the beam-expanding collimation of different wave length, have outside high-quality collimation performance, and high optical transmittance can be realized, for a kind of without the compact broadband high magnification beam spread collimation optical system of distance adjustor.
The technical scheme realizing the utility model object is to provide a kind of beam spread collimation optical system, and it comprises transmission beam-expanding collimation group and reflection beam-expanding collimation group; By light direction, described transmission beam-expanding collimation group comprise bear that mirror and one piece of biconvex telescope direct form by one piece of concave-concave expand grouping, the collimation grouping be made up of first piece of bent moon telescope direct and second piece of bent moon telescope direct, the curvature of first piece and second piece bent moon telescope direct all bends towards light direction; The combined focal length expanding grouping is negative value, the combined focal length of collimation grouping be on the occasion of the multiplying power of, transmission beam-expanding collimation group be the focal length that divides into groups of collimation and the absolute value of ratio of focal length expanding grouping; Described reflection beam-expanding collimation group comprises the paraboloidal mirror that two pieces have same focal point position, be followed successively by small-bore paraboloidal mirror and heavy caliber paraboloidal mirror, the face shape of heavy caliber paraboloidal mirror is from axle concave surface, and the beam-expanding collimation multiplying power of reflection beam-expanding collimation group is the ratio of the vertex curvature radius of heavy caliber paraboloidal mirror and the vertex curvature radius of small-bore paraboloidal mirror.
In the utility model, the multiplying power of transmission beam-expanding collimation group is 2x ~ 10x; The multiplying power of reflection beam-expanding collimation group is 8x ~ 30x.
The optical system that the utility model provides is made up of transmission beam-expanding collimation group and reflection beam-expanding collimation group, and its principle is as follows:
The little multiplying power that transmission beam-expanding collimation group realizes light expands, and adopts biconcave mirror-biconvex and meniscus lens-meniscus lens to form.Smaller owing to expanding, aberration is mainly spherical aberration and aberration.Spherical aberration correction is realized, by the chromatic aberration correction selecting suitable glass material combination to realize broadband wavelength by optimizing face shape.Reflection expands group and is made up of two panels off-axis parabolic mirror, adopts oval concentric structure, realizes expanding of the large multiplying power of low-angle.Through the light that transmission beam-expanding collimation group exports, after inciding small-bore off axis paraboloidal mirror, reflex to bigbore off axis paraboloidal mirror and realize expanding of larger ratio.
The transmission beam-expanding collimation group of the utility model beam spread collimation optical system adopts four lens to form, the beam-expanding collimation that whole realization is less than less than 10 times.Front two panels forms mirror and expands grouping, and first mirror is concave-concave pattern, adopts the material that dispersion is relatively high, refractive index is relatively high; Second mirror is biconvex pattern, and adopt the material of low-refraction and low dispersion, their combined focal length is negative; Rear two panels forms collimation grouping, two panels is bent moon telescope direct pattern, its curvature all bends towards light beam incident direction, selecting of two eyeglasses is contrary with selecting of two panels above, namely first bent moon telescope direct selects the material of low-refraction and low dispersion, and second bent moon telescope direct selects the material that dispersion is relatively high, refractive index is relatively high.The selection of initial focal length and material is determined by following formula (1), (2) and (3):
；
Wherein,
for the beam-expanding collimation multiplying power of the beams extended by lens collimation group,
for expanding the focal length of grouping,
for the focal length of collimation grouping,
with
be respectively and expand focal length and the material Abbe number thereof that concave-concave in grouping bears mirror,
with
be respectively the focal length and material Abbe number thereof that expand biconvex telescope direct mirror in grouping.Equally, the Material selec-tion of the eyeglass in collimation grouping also obtains by formula (1), (2) and (3).
Penetrate the employing of beam-expanding collimation group after in the utility model with two paraboloidal mirrors of focal position, more than 10x beam-expanding collimation can be realized.By paraboloidal mirror, light path is turned back from axle, optical system structure length can be reduced.One of them focus of two paraboloidal mirrors, in same position, forms oval concentric structure, recoverable other several aberrations except the curvature of field, as spherical aberration, and coma, astigmatism etc.Small-bore paraboloidal mirror and heavy caliber paraboloidal mirror have identical focal position, and namely the ellipse on two sides is concentric structure.Its vertex curvature ratio is the beam-expanding collimation ratio of this group
, i.e. formula (4):
（4）；
Wherein,
for the vertex curvature radius of small-bore paraboloidal mirror,
for the vertex curvature radius of heavy caliber paraboloidal mirror.After current transmission beam-expanding collimation and back reflection beam-expanding collimation group combine, the beam-expanding collimation multiplying power of formation is than being formula (5):
（5）；
The beam-expanding collimation multiplying power more than more than 30 times can be formed thus, even can reach the beam-expanding collimation ratio of more than 200 times.By mutually compensating the aberration of correct residual after both combinations, the residue high-order spherical aberration as front transmission group can correct in reflection group, and the residual field curvature in reflection group can compensate in transmission group.Due to turning back light path from axle of adopting, can reduction system volume, and transmission beam-expanding collimation group can placed from shaft space, make transmission beam-expanding collimation group not need to take unnecessary space, thus make system compacter.
Compared with prior art, the beneficial effects of the utility model are:
1, the beam-expanding collimation system that provides of the utility model, does not need to arrange the large multiplying power beam-expanding collimation that element adjusting mechanism or aberration compensation parts just can realize broadband light beam.The implementation method decapacitation that the utility model proposes is applied in visible near-infrared wave band, at all the other wave bands, as ultraviolet, medium wave, long wave infrared region are suitable for too.
2, the powerful compact beam-expanding collimation system of broadband that provides of the utility model, can be any optical maser wavelength within the scope of broadband or white light laser provides beam-expanding collimation, and without any need for motion compensation parts, compact conformation, volume is little, expand that multiplying power is large, collimation performance is high, can be used for the aspects such as holographic imaging, optic test, laser radar.
Accompanying drawing explanation
The one that Fig. 1 provides for the utility model embodiment is for broadband high magnification beam spread collimation optical system structural representation;
Fig. 2 for the utility model embodiment provide a kind of for the wave front chart of broadband high magnification beam spread collimation optical system at 632.8nm place;
Fig. 3 for the utility model embodiment provide a kind of for the wave front chart of broadband high magnification beam spread collimation optical system at 1064nm place;
A kind of MTF curve map of outgoing beam after the imaging of 200mm perfect lens for broadband high magnification beam spread collimation optical system that Fig. 4 provides for the utility model embodiment;
The one that Fig. 5 provides for another embodiment of the utility model is for broadband high magnification beam spread collimation optical system structural representation;
In figure, 1, double-concave negative lens; 2, biconvex positive lens; 3, first piece of meniscus lens; 4, second piece of meniscus lens; 5, small-bore paraboloidal mirror; 6, heavy caliber paraboloidal mirror.
Embodiment
Below in conjunction with drawings and Examples, technical solutions of the utility model are further elaborated.
Embodiment 1:
The designing requirement of the present embodiment beam spread collimation optical system to be processed: incident beam is 1.5mm, dispersion angle is 22mrad, realize the beam-expanding collimation of 33x, after beam-expanding collimation, the emergent light angle of divergence is not more than 0.7mrad, and the wavelength coverage that can be suitable for is 488nm ~ 1064m.
See accompanying drawing 1, it is that the one that provides of the present embodiment is for broadband high magnification beam spread collimation optical system structural representation; It comprises transmission beam-expanding collimation group and reflection beam-expanding collimation group; Described transmission beam-expanding collimation group, by light direction, comprise bear that mirror 1 and one piece of biconvex telescope direct 2 form by one piece of concave-concave expand grouping, the collimation be made up of first piece of bent moon telescope direct 3 and second piece of bent moon telescope direct 4 divides into groups; The combined focal length expanding grouping is negative, and the curvature of two pieces of bent moon telescope directs bends towards light direction, and the combined focal length of collimation grouping just be, and the multiplying power of transmission beam-expanding collimation group is the focal length that divides into groups of collimation and the absolute value of ratio of focal length expanding grouping; Reflection beam-expanding collimation group comprises the paraboloidal mirror that two pieces have same focal point position, be followed successively by small-bore paraboloidal mirror 5 and heavy caliber paraboloidal mirror 6, the face shape of heavy caliber paraboloidal mirror is from axle concave surface, the face shape of small-bore paraboloidal mirror is from crown of roll face, and the beam-expanding collimation multiplying power of rear group is the ratio of the vertex curvature radius of heavy caliber paraboloidal mirror 6 and the vertex curvature radius of small-bore paraboloidal mirror 5.
The present embodiment prepares the concrete steps process flow diagram of broadband high magnification beam spread collimation optical system, and step is as follows:
1, according to the designing requirement of beam spread collimation optical system to be processed, as volume, wavelength coverage, beam-expanding collimation multiplying power or input, output angle etc., distribute the beam-expanding collimation multiplying power between transmission beam-expanding collimation group and reflection beam-expanding collimation group, what make front transmission beam-expanding collimation group expands multiplying power between 2x ~ 10x, make the multiplying power of back reflection beam-expanding collimation group at more than 8x, reach required beam-expanding collimation multiplying power.
2, the selection of initial focal length and material is determined by following formula (1), (2) and (3):
；
Wherein,
for the beam-expanding collimation multiplying power of the beams extended by lens collimation group,
for expanding the focal length of grouping,
for the focal length of collimation grouping,
with
be respectively and expand focal length and the material Abbe number thereof that concave-concave in grouping bears mirror,
with
be respectively the focal length and material Abbe number thereof that expand biconvex telescope direct mirror in grouping.Equally, the Material selec-tion of the eyeglass in collimation grouping also obtains by formula (1), (2) and (3).
The expand collimation that grouping and rear two mirrors form of optical simulation software Zemax or CodeV to two mirrors compositions before in the beams extended by lens collimation group is utilized to divide into groups to carry out chromatic aberration correction respectively, spherical aberration optimization, focal length are chosen, and then combination expands grouping and collimates grouping and carries out comprehensive aberration correction.
3, to curvature, the spacing of back reflection beam-expanding collimation group or carry out preferably from axle amount; The vertex curvature ratio of two pieces of paraboloidal mirrors is the beam-expanding collimation ratio of this group
, i.e. formula (4):
（4）；
Wherein,
for the vertex curvature radius of small-bore paraboloidal mirror,
for the vertex curvature radius of heavy caliber paraboloidal mirror.
4, combine transmission beam-expanding collimation group and spread collimation group with reflection, after current transmission beam-expanding collimation and back reflection beam-expanding collimation group combine, the beam-expanding collimation multiplying power of formation is than being formula (5):
（5）；
To aberration and the collimation performance global optimization of system, obtain the parameters of system.
Judge whether the result obtained meets the demands, if because catoptron difficulty of processing is large or volume size restriction can not reach expection requirement, then adjust two groups of multiplying powers by the method for step 1, return step 2 and re-start design again, with the horizontal and vertical size of balanced system; Otherwise, perform step 5.
5, can meet in the situation such as beam-expanding collimation performance and processing technology requirement, carry out the processing of system, assembling and test, obtain a kind of beam spread collimation optical system.
By above-mentioned implementation step, the design parameter obtained is as shown in table 1.
Table 1
。
In embodiment of the present utility model, transmission beam-expanding collimation group be placed in reflection beam-expanding collimation group from axle inclined reflection leaving space position, make whole system volume compacter, whole optical system length is 85mm, and width is 65mm.
Lens before in the present embodiment in transmission beam-expanding collimation group, negative mirror 1 is front, and positive biconvex mirror 2 is rear, and negative mirror 1 and positive biconvex mirror 2 form negative mirror group.Negative mirror 1 adopts the flint glass ZF2 of high dispersion high index of refraction, and positive biconvex mirror 2 adopts the crown glass K9 of the low dispersion of low-refraction.Mirror 3 and mirror 4 form telescope direct group, and all adopt positive bent moon form, curvature bends towards light incident direction, and two mirrors adopt K9 and ZF2 respectively.
After in the present embodiment, the catoptron 5 of group adopts convex paraboloid face shape, is 6mm from axle amount, and parabolic lens 4 is sampled concave paraboloid face shape, is 40mm from axle amount, and two focal positions of throwing face mirrors overlap.
According to current process, the utility model give beam spread collimation optical system can through more than 90% at 488nm ~ 1064nm wave band, dispersion angle is the incident beam of 22mrad, and the angle of divergence obtaining outgoing beam after collimator and extender is less than 0.7mrad, expands multiplying power at 33x.
See accompanying drawing 2, give the present embodiment disperses visual field wave front chart at 632.8nm place central vision and edge, wherein, (a) figure is PV value, and (b) figure is RMS value; Can be seen by figure, when 0 visual field, PV value is 0.093 wavelength, and RMS value is 0.02 wavelength, and when peripheral field, PV value is 0.086 wavelength, and RMS value is 0.020 wavelength.
See accompanying drawing 3, give the present embodiment disperses visual field wave front chart at 1064nm place central vision and edge, wherein, (a) figure is PV value, and (b) figure is RMS value; Can be seen by figure, when 0 visual field, PV value is 0.078 wavelength, and RMS value is 0.14 wavelength, and when peripheral field, PV value is 0.091 wavelength, and RMS value is 0.015 wavelength.
See accompanying drawing 4, it is modulation transfer function (MTF) curve after the beam-expanding collimation system focal imaging that adopts 200mm perfect lens and provide the present embodiment.As shown in Figure 5, through optical system beam-expanding collimation of the present utility model under the incidence of the 22mrad angle of divergence, again through desirable lens imaging, close to diffraction limit under the MTF obtained, can illustrate that beam spread collimation optical system of the present utility model has and good expand parasexuality energy.
Embodiment 2
See accompanying drawing 5, the one that the present embodiment provides is for broadband high magnification beam spread collimation optical system structural representation; The present embodiment adopts the transmission identical with embodiment 1 to spread collimation group, have employed small-bore concave surface paraboloidal mirror in reflection beam-expanding collimation group.
Small-bore concave paraboloid mirror 5 in the present embodiment, its vertex curvature is the same with the vertex curvature numerical values recited of the convex parabolic lens in embodiment 1, and symbol is contrary, in namely the radius-of-curvature of element in table 15 being changed into-20.1.Owing to using little concave paraboloid mirror can form middle real focus, thus make entire system length, and what formed when using the small-bore convex surface paraboloidal mirror in embodiment 1 is virtual focus, length can shorten.Small-bore concave paraboloid mirror in the present embodiment is in use, also contrary with the small-bore convex paraboloid mirror in embodiment 1 from direction of principal axis, namely from axle amount be-6mm.
In the present embodiment, after inciding the light beam of small-sized recessed catoptron, can first pool a bit, this point be the common focus of paraboloidal mirror 5 and paraboloidal mirror 6.Beam divergence after convergence incides on bigbore parabola and realizes collimation.
The performance index of the beam-expanding collimation system that the present embodiment relates to are consistent with embodiment 1.
Beam-expanding collimation system of the present utility model does not need to arrange the large multiplying power beam-expanding collimation that element adjusting mechanism or aberration compensation parts just can realize broadband light beam.The implementation method decapacitation that the utility model proposes is applied in visible near-infrared wave band, at all the other wave bands, as ultraviolet, medium wave, long wave infrared region are suitable for too.
Claims (2)
1. a beam spread collimation optical system, is characterized in that: it comprises transmission beam-expanding collimation group and reflection beam-expanding collimation group; By light direction, described transmission beam-expanding collimation group comprise bear that mirror (1) and one piece of biconvex telescope direct (2) form by one piece of concave-concave expand grouping, the collimation grouping be made up of first piece of bent moon telescope direct (3) and second piece of bent moon telescope direct (4), the curvature of first piece and second piece bent moon telescope direct all bends towards light direction; The combined focal length expanding grouping is negative value, the combined focal length of collimation grouping be on the occasion of the multiplying power of, transmission beam-expanding collimation group be the focal length that divides into groups of collimation and the absolute value of ratio of focal length expanding grouping; Described reflection beam-expanding collimation group comprises the paraboloidal mirror that two pieces have same focal point position, be followed successively by small-bore paraboloidal mirror (5) and heavy caliber paraboloidal mirror (6), the face shape of heavy caliber paraboloidal mirror is from axle concave surface, and the beam-expanding collimation multiplying power of reflection beam-expanding collimation group is the ratio of the vertex curvature radius of heavy caliber paraboloidal mirror (6) and the vertex curvature radius of small-bore paraboloidal mirror (5).
2. a kind of beam spread collimation optical system according to claim 1, is characterized in that: the multiplying power of transmission beam-expanding collimation group is 2x ~ 10x; The multiplying power of reflection beam-expanding collimation group is 8x ~ 30x.
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| CN201520468124.2U CN204758926U (en) | 2015-07-02 | 2015-07-02 | Expand and restraint collimation optical system |
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Cited By (6)
| Publication number | Priority date | Publication date | Assignee | Title |
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| CN104977720A (en) * | 2015-07-02 | 2015-10-14 | 苏州大学 | Beam-expanding collimating optical system and preparation method thereof |
| CN105449507A (en) * | 2016-01-06 | 2016-03-30 | 中国科学院上海光学精密机械研究所 | Compensation device and method for pulse-front distortion in femtosecond laser pulse amplification system |
| CN106017360A (en) * | 2016-08-07 | 2016-10-12 | 哈尔滨工业大学 | Portable array zero setting high-frequency-response large-working-distance auto-collimation device and method |
| CN109804287A (en) * | 2016-08-17 | 2019-05-24 | 纳米精密产品股份有限公司 | Optical connector ferrule component with the bireflectance surface for beam spread and the extension light beam connector including it |
| CN110824680A (en) * | 2019-11-28 | 2020-02-21 | 合肥工业大学 | Beam expanding device of catadioptric interferometer |
| CN115597483A (en) * | 2022-09-30 | 2023-01-13 | 南京理工大学（Cn） | Interferometer beam expanding and collimating device |
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2015
- 2015-07-02 CN CN201520468124.2U patent/CN204758926U/en not_active Withdrawn - After Issue
Cited By (8)
| Publication number | Priority date | Publication date | Assignee | Title |
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| CN104977720A (en) * | 2015-07-02 | 2015-10-14 | 苏州大学 | Beam-expanding collimating optical system and preparation method thereof |
| CN105449507A (en) * | 2016-01-06 | 2016-03-30 | 中国科学院上海光学精密机械研究所 | Compensation device and method for pulse-front distortion in femtosecond laser pulse amplification system |
| CN105449507B (en) * | 2016-01-06 | 2018-07-13 | 中国科学院上海光学精密机械研究所 | It is a kind of to be used for the compensation device and compensation method that pulse front edge distorts in femto-second laser pulse amplification system |
| CN106017360A (en) * | 2016-08-07 | 2016-10-12 | 哈尔滨工业大学 | Portable array zero setting high-frequency-response large-working-distance auto-collimation device and method |
| CN109804287A (en) * | 2016-08-17 | 2019-05-24 | 纳米精密产品股份有限公司 | Optical connector ferrule component with the bireflectance surface for beam spread and the extension light beam connector including it |
| CN110824680A (en) * | 2019-11-28 | 2020-02-21 | 合肥工业大学 | Beam expanding device of catadioptric interferometer |
| CN115597483A (en) * | 2022-09-30 | 2023-01-13 | 南京理工大学（Cn） | Interferometer beam expanding and collimating device |
| CN115597483B (en) * | 2022-09-30 | 2024-02-06 | 南京理工大学 | Interferometer beam expansion collimation device |
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