CN108840564A - The phosphate laser neodymium glass of luminescence effect - Google Patents
The phosphate laser neodymium glass of luminescence effect Download PDFInfo
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- CN108840564A CN108840564A CN201811022539.1A CN201811022539A CN108840564A CN 108840564 A CN108840564 A CN 108840564A CN 201811022539 A CN201811022539 A CN 201811022539A CN 108840564 A CN108840564 A CN 108840564A
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- neodymium glass
- luminescence effect
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Abstract
The present invention provides a kind of phosphate laser neodymium glass with luminescence effect, and molar percentage composition includes：P2O550-70mol%；Al2O33-25mol%；MO 5-25mol%, R2O 10-20mol%；R2O30.5-5mol%, wherein the MO is one of BaO, MgO, ZnO or a variety of；R2O is Li2O、Na2O、K2One of O or a variety of；R2O3For B2O3、Sb2O3、Nd2O3One of or it is a variety of.The present invention realizes that thermo-optical coeffecient ds/dT close to 0, reduces nonlinear refractive index n by reasonably selecting to each component and its content2, increase neodymium glass stimulated emission cross section, can satisfy the needs of device of high power laser.
Description
The application is for application No. is 201410781664.6, and the applying date is on December 16th, 2014, entitled " no heat
The divisional application of the application for a patent for invention of the phosphate laser neodymium glass of luminous effect ".
Technical field
The present invention relates to a kind of phosphate laser neodymium glass, more particularly to a kind of swashing suitable for device of high power laser
Light glass, stimulated emission cross section is high, second nonlinear refractive index is low, luminescence effect.
Background technique
The elimination of thermal-optical distortion is one of the major subjects of superlaser glass development.Luminescence effect glass refers to light path
The glass that length does not vary with temperature, i.e. thermo-optical coeffecient ds/dT are close to 0.Generally for making laser generation that optical pumping be repeated
When Pu, the temperature of glass is increased, and optical path length will change.Since glass heating temperature is unevenly distributed, to be formed
The optical path length variation of gradient causes wavefront deformation, the i.e. distortion of generation photo-thermal.With the continuous expansion of device of high power laser scale
Greatly, the continuous improvement of laser output energy, after per surface area laser energy density reaches certain magnitude, the heat of laser glass
Luminous effect must draw attention.
A possibility that optical path-length shifts as caused by temperature change are smaller, i.e., ds/dT is smaller, generate photo-thermal distortion is got over
It is small.Phosphate laser neodymium glass is mainly used as the operation material of laser amplifier in device of high power laser, in order to realize height
Gain, it is desirable that the stimulated emission cross section of neodymium glass is as big as possible, nonlinear refractive index n2It is low as far as possible, but can not ignore simultaneously
The influence of glass thermo-optic effect.For that purpose it is necessary to which the composition of reasonable component design, is obtaining big stimulated emission cross section, low second order
Nonlinear refractive index, and while realize high-gain, it should minimize or eliminate the thermo-optic effect of neodymium glass.
Existing phosphate laser neodymium glass domestic at present, as N31 glass (N31 laser neodymium glass acceptance report, 1998 12
Month), although stimulated emission cross section is higher by (3.9 × 10-20cm2), but its thermo-optical coeffecient (dS/dT=14 × 10-7/ K) it is larger, no
It is able to satisfy requirement of the following device of high power laser to laser glass low-heat luminous effect.
United States Patent (USP) US 4108673, US 5526369, US5032315 individually disclose a kind of phosphate laser neodymium glass
Glass, but height is all not belonging to by emission cross section, the phosphate laser neodymium glass of low second nonlinear refractive index, luminescence effect.
Summary of the invention
Technical problem to be solved by the invention is to provide a kind of phosphate laser neodymium glass with luminescence effect, can
To meet the needs of device of high power laser.
The present invention solves solution used by technical problem：The phosphate laser neodymium glass of luminescence effect,
Molar percentage forms：P2O550-70mol%；Al2O33-25mol%；MO 5-25mol%, R2O 10-20mol%；
R2O30.5-5mol%, wherein the MO is one of BaO, MgO, ZnO or a variety of；R2O is Li2O、Na2O、K2One in O
Kind is a variety of；R2O3For B2O3、Sb2O3、Nd2O3One of or it is a variety of.
Further, further include：Nb2O50-0.5mol%；Sb2O30-1mol%.
Further, wherein BaO 5-20mol%；MgO 0-5mol%.
Further, wherein B2O30-2mol%.
Further, wherein Al2O35-15mol%.
Further, wherein MO 10-20mol%.
Further, wherein BaO 9-17mol%.
Further, the second nonlinear refractive index n of glass2It is 1.05~1.14 (10-13esu)。
Further, the stimulated emission cross section σ of glass is 3.9~4.4 (10-20cm2)。
Further, (20-60 DEG C) of the thermo-optical coeffecient ds/dT of glass is 0.1~3 (10-7/K)。
The beneficial effects of the invention are as follows：The present invention passes through the phosphate glass that refractive index temperature coefficient is small, the coefficient of expansion is big
The component and its content of glass are reasonably selected, and realize thermo-optical coeffecient ds/dT close to 0；By reducing phosphate laser neodymium glass
The linear refractive index of glass and dispersion reach and reduce nonlinear refractive index n2Purpose；It can be improved neodymium ion transmitting by increasing
If the dry ingredients in section, increase neodymium glass stimulated emission cross section, reach material comprehensive performance most preferably, can satisfy high power and swash
The needs of electro-optical device.
Detailed description of the invention
Fig. 1 is the fluorescent spectrum curve of the glass of the embodiment of the present invention 6.
Specific embodiment
The technology of the present invention route is that the phosphate glass small by refractive index temperature coefficient, the coefficient of expansion is big is selected
It selects, realizes ds/dT close to 0；Simultaneously by reducing linear refractive index and the dispersion of phosphate laser neodymium glass, it is non-to reach reduction
Linear refractive index n2Purpose；If commonly can be improved the dry ingredients of neodymium ion emission cross section by increasing, increase neodymium glass
Stimulated emission cross section makes material comprehensive performance reach best.
The temperature coefficient of optical path length is：
In formula (1), (n-1) and coefficient of expansion α are positive number, and refractive index will increase ordinary glass material when temperature is raised
Greatly.By (1) formula as it can be seen that make ds/dT close to 0, dn/dT must just be made to become negative, this be thermal refractive index coefficient with
The relations problems of the coefficient of expansion make refractive index temperature by the adjustment to phosphate glass thermal refractive index coefficient, the coefficient of expansion
The negative value of coefficient increases to offset the optical path length that glass is generated by expanded by heating, to eliminate the thermo-optic effect of glass, i.e.,
Realize that thermo-optical coeffecient ds/dT is reduced to close to 0.
The molar percentage of the phosphate laser neodymium glass of luminescence effect of the invention forms：P2O550-
70mol%；Al2O33-25mol%；MO 5-25mol%, R2O 10-20mol%；R2O30.5-5mol%.
Wherein, above-mentioned MO is one of BaO, MgO, ZnO or a variety of；R2O is Li2O、Na2O、K2One of O or more
Kind；R2O3For B2O3、Sb2O3、Nd2O3One of or it is a variety of.
Wherein, above-mentioned BaO 5-20mol%；MgO 0-5mol%；Nb2O50-0.5mol%；B2O30-2mol%；
Sb2O30-1mol%.
Preferably, Al2O35-15mol%；MO 10-20mol%, BaO 9-17mol%.
In above-mentioned composition, monovalence alkali metal oxide Li2O、Na2O、K2MgO in O and alkaline earth oxide can drop
The refractive index and dispersion of hypophosphate laser neodymium glass, so that reaching reduces nonlinear refractive index n2Purpose.In addition, inventor
By the study found that alkali metal oxide and alkaline earth oxide are to raising neodymium glass stimulated emission in phosphate glass
The sequence of section from small to large is respectively Li2O→Na2O→K2O, MgO → CaO → SrO → BaO is adjusted according to this rule is appropriate
Whole each oxide ratios, in unobvious raising nonlinear refractive index n2Under the premise of, suitably increase K2The content ratio of O component,
And more BaO content is introduced, to improve the stimulated emission cross section of neodymium glass.
The Al of proper content is introduced in inventive formulation2O3, make glass that there are better processing characteristics.Meanwhile Al2O3
Introducing improve the coefficient of expansion α of glass to a certain extent.Pass through Al2O3With the adjustment of BaO content, make glass expansion coefficient α
Match with thermal refractive index coefficient, to achieve the purpose that reduce thermo-optical coeffecient.
The preparation method of the phosphate laser neodymium glass of above-mentioned luminescence effect, includes the following steps：
1. selected glass formula, weighs each raw material；
2. raw material is sufficiently mixed uniformly, mixture is formed；
3. silicon carbide smelting furnace is warming up to 1300-1400 DEG C, 20-25Kg/h is divided to be homogeneously added into the mixture
In silicification hopper in silicon carbide smelting furnace；
4. being passed through O in the silicification hopper2+SOC12Mixed gas, throughput are 1-2L/ minutes；
5. glass metal is injected platinum crucible after stopping ventilation, glass metal is clarified 3-4 hours at 1350-1450 DEG C；
6. being carried out mechanical stirring 6-10 hours at 1250-1350 DEG C to glass metal；
It is formed 7. glass metal obtained is poured into graphite jig, the cooling phosphorus that thermo-optic effect of the invention is made of annealing
Hydrochlorate laser neodymium glass.
The test method of the indices of glass of the present invention is as follows：
1) nonlinear refractive index n2Test method
The second nonlinear refractive index n of glass2It is expressed with following formula：
In formula, ndFor refractive index of the glass at 587.6nm wavelength, υ is the Abbe number of glass, and calculation formula is：
nF、nCRespectively refractive index of the glass at 486.1nm and 656.3nm wavelength.nd、nF、nCBy GMR-1D precision
Angular instrument is tested to obtain.
By test, the nonlinear refractive index n of glass of the present invention2It is 1.05~1.14 (10-13esu)。
2) test method of the stimulated emission cross section σ of glass
The stimulated emission cross section of glass is calculated by Judd-Ofelt model.In Judd-Ofelt theory, it is stimulated
Penetrate section σ and radiative transistion probability A [(4F3/2)；(4F11/2)] relationship be：
Wherein, λpIt is wavelength of the fluorescence peak, λeffIt is the effective line width of wavelength of the fluorescence peak, i.e.,
λeff=∫ I (λ) d λ/I1053
By test, the stimulated emission cross section σ of glass of the present invention is 3.9~4.4 (10-20cm2)。
3) test method of thermo-optical coeffecient ds/dT
The test of thermo-optical coeffecient ds/dT is obtained by following expression measuring and calculation：
In formula, n is the refractive index of glass, and dn/dT is the thermal refractive index coefficient of glass, by GMR-1D precision goniometer
Test obtains.
α is the thermal expansion coefficient of glass, is tested using DIL-402C thermal dilatometer.
By test, (20-60 DEG C) of thermo-optical coeffecient ds/dT of glass of the present invention is 0.1~3 (10-7/K)。
10 embodiments of the invention are shown in Table 1.Molar percentage composition, the non-linear folding of glass are given in table 1
Penetrate rate n2(10-13Esu), the stimulated emission cross section σ (10 of glass-20cm2) and thermo-optical coeffecient ds/dT.
Table 1
Fig. 1 be glass of the present invention by the glass processing of above-described embodiment 6 at the sample of 1mm thickness, then use Fluorescence Spectrometer
Its fluorescence spectrum is measured, fluorescent spectrum curve needed for obtaining the stimulated emission cross section measuring and calculation of 6 glass of embodiment.
Claims (10)
1. the phosphate laser neodymium glass of luminescence effect, which is characterized in that its molar percentage, which forms, includes：P2O5 50-
70mol%；Al2O33-25mol%；MO 5-25mol%, R2O 10-20mol%；R2O30.5-5mol%, wherein the MO
For one of BaO, MgO, ZnO or a variety of；R2O is Li2O、Na2O、K2One of O or a variety of；R2O3For B2O3、Sb2O3、
Nd2O3One of or it is a variety of.
2. the phosphate laser neodymium glass of luminescence effect as described in claim 1, which is characterized in that further include：Nb2O5 0-
0.5mol%；Sb2O30-1mol%.
3. the phosphate laser neodymium glass of luminescence effect as described in claim 1, which is characterized in that wherein, BaO 5-
20mol%；MgO 0-5mol%.
4. the phosphate laser neodymium glass of luminescence effect as described in claim 1, which is characterized in that wherein, B2O3 0-
2mol%.
5. the phosphate laser neodymium glass of luminescence effect as described in claim 1, which is characterized in that wherein, Al2O3 5-
15mol%.
6. the phosphate laser neodymium glass of luminescence effect as described in claim 1, which is characterized in that wherein, MO 10-
20mol%.
7. the phosphate laser neodymium glass of luminescence effect as described in claim 1, which is characterized in that wherein, BaO 9-
17mol%.
8. the phosphate laser neodymium glass of luminescence effect as described in claim 1, which is characterized in that the second order non-linear of glass
Property refractive index n2It is 1.05~1.14 (10-13esu)。
9. the phosphate laser neodymium glass of luminescence effect as described in claim 1, which is characterized in that the stimulated emission of glass
Section σ is 3.9~4.4 (10-20cm2)。
10. the phosphate laser neodymium glass of luminescence effect as described in claim 1, which is characterized in that the hot spectrum of glass
(20-60 DEG C) of number ds/dT is 0.1~3 (10-7/K)。
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| CN201811022539.1A CN108840564B (en) | 2014-12-16 | 2014-12-16 | Phosphate laser neodymium glass without thermal effect |
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| CN201410781664.6A CN105753316B (en) | 2014-12-16 | 2014-12-16 | The phosphate laser neodymium glass of luminescence effect |
| CN201811022539.1A CN108840564B (en) | 2014-12-16 | 2014-12-16 | Phosphate laser neodymium glass without thermal effect |
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Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
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| CN113277731A (en) * | 2021-05-28 | 2021-08-20 | 成都光明光电有限责任公司 | Silver-containing nanoparticle laser glass and method for producing same |
| CN113461328A (en) * | 2021-06-28 | 2021-10-01 | 成都光明光电有限责任公司 | Phosphate laser neodymium glass and preparation method thereof |
| CN113636755A (en) * | 2021-06-28 | 2021-11-12 | 成都光明光电有限责任公司 | Phosphate laser glass and preparation method thereof |
| CN114634310A (en) * | 2022-03-09 | 2022-06-17 | 中国科学院上海光学精密机械研究所 | Phosphate laser neodymium glass and preparation method thereof |
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| CN109081579B (en) * | 2018-09-17 | 2021-07-27 | 成都光明光电有限责任公司 | Phosphate laser neodymium glass |
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| US4239645A (en) * | 1975-03-18 | 1980-12-16 | Hoya Glass Works, Ltd. | Phosphate base laser glasses |
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Cited By (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN113277731A (en) * | 2021-05-28 | 2021-08-20 | 成都光明光电有限责任公司 | Silver-containing nanoparticle laser glass and method for producing same |
| CN113277731B (en) * | 2021-05-28 | 2022-04-15 | 成都光明光电有限责任公司 | Silver-containing nanoparticle laser glass and method for producing same |
| CN113461328A (en) * | 2021-06-28 | 2021-10-01 | 成都光明光电有限责任公司 | Phosphate laser neodymium glass and preparation method thereof |
| CN113636755A (en) * | 2021-06-28 | 2021-11-12 | 成都光明光电有限责任公司 | Phosphate laser glass and preparation method thereof |
| CN113636755B (en) * | 2021-06-28 | 2022-06-03 | 成都光明光电有限责任公司 | Phosphate laser glass and preparation method thereof |
| CN114634310A (en) * | 2022-03-09 | 2022-06-17 | 中国科学院上海光学精密机械研究所 | Phosphate laser neodymium glass and preparation method thereof |
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| Publication number | Publication date |
|---|---|
| CN105753316A (en) | 2016-07-13 |
| CN108840564B (en) | 2021-07-27 |
| CN105753316B (en) | 2019-02-26 |
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