[go: up one dir, main page]

CN1269755C - bismuth-doped germanium-based optical glass and preparation method thereof - Google Patents

bismuth-doped germanium-based optical glass and preparation method thereof Download PDF

Info

Publication number
CN1269755C
CN1269755C CN 200410054216 CN200410054216A CN1269755C CN 1269755 C CN1269755 C CN 1269755C CN 200410054216 CN200410054216 CN 200410054216 CN 200410054216 A CN200410054216 A CN 200410054216A CN 1269755 C CN1269755 C CN 1269755C
Authority
CN
China
Prior art keywords
glass
fluorescence
bismuth
hours
optical glass
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Fee Related
Application number
CN 200410054216
Other languages
Chinese (zh)
Other versions
CN1587142A (en
Inventor
彭明营
孟宪赓
邱建荣
陈丹平
姜雄伟
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Shanghai Institute of Optics and Fine Mechanics of CAS
Original Assignee
Shanghai Institute of Optics and Fine Mechanics of CAS
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Shanghai Institute of Optics and Fine Mechanics of CAS filed Critical Shanghai Institute of Optics and Fine Mechanics of CAS
Priority to CN 200410054216 priority Critical patent/CN1269755C/en
Publication of CN1587142A publication Critical patent/CN1587142A/en
Application granted granted Critical
Publication of CN1269755C publication Critical patent/CN1269755C/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Images

Classifications

    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03CCHEMICAL COMPOSITION OF GLASSES, GLAZES OR VITREOUS ENAMELS; SURFACE TREATMENT OF GLASS; SURFACE TREATMENT OF FIBRES OR FILAMENTS MADE FROM GLASS, MINERALS OR SLAGS; JOINING GLASS TO GLASS OR OTHER MATERIALS
    • C03C3/00Glass compositions
    • C03C3/12Silica-free oxide glass compositions
    • C03C3/253Silica-free oxide glass compositions containing germanium

Landscapes

  • Chemical & Material Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • General Chemical & Material Sciences (AREA)
  • Geochemistry & Mineralogy (AREA)
  • Materials Engineering (AREA)
  • Organic Chemistry (AREA)
  • Glass Compositions (AREA)

Abstract

一种掺铋锗基光学玻璃及其制备方法,该玻璃各组成及其摩尔百分比:GeO290~99.98mol%;M=Al2O3,Ta2O5,Ga2O3或B2O3为0.01~9mol%;Bi2O3为0.01~5mol%。该玻璃的吸收光谱覆盖从可见到近红外区域,荧光光谱的中心波长位于1300nm左右,荧光寿命大于200μs,荧光半高宽大于200nm,可以用532nm,632.5nm以及808nm的激光进行泵浦。这些光学玻璃有望用于超宽带光放大器,高功率激光器,可调谐激光器等技术领域。

Figure 200410054216

A bismuth-doped germanium-based optical glass and a preparation method thereof, wherein the components and molar percentages of the glass are as follows: GeO 2 90-99.98 mol%; M=Al 2 O 3 , Ta 2 O 5 , Ga 2 O 3 or B 2 O 3 0.01-9 mol%; Bi 2 O 3 0.01-5 mol%. The absorption spectrum of the glass covers the visible to near-infrared region, the central wavelength of the fluorescence spectrum is about 1300 nm, the fluorescence lifetime is greater than 200 μs, the fluorescence half-width is greater than 200 nm, and it can be pumped by 532 nm, 632.5 nm and 808 nm lasers. These optical glasses are expected to be used in the technical fields of ultra-wideband optical amplifiers, high-power lasers, tunable lasers, etc.

Figure 200410054216

Description

Mix bismuth germanium base optical glass and preparation method thereof
Technical field
The present invention relates to opticglass, particularly a kind of bismuth germanium base optical glass and preparation method thereof of mixing, this glass can be sent out near infrared communication band fluorescence, has long fluorescence lifetime, wide gain bandwidth is suitable as gain media and is applied to optical amplifier and/or laser apparatus.
Background technology
March 4 in 1998 order, the quiet patent (special permission discloses flat 11-29334) that waits the people to apply for being entitled as " mixing bismuth silica glass, optical fiber and image intensifer manufacture method " of the liana of Mitsubishi Cable Ind Ltd.They utilize the zeolite of bismuth exchange as dispersion medium, and comprehensive sol-gel method and high-temperature melting method have prepared and mixed the bismuth silica glass, draw out corresponding optical fiber, realized the light amplification at 1.3 μ m places under the 0.81 μ m pumping.The photoluminescence peak of this glass is positioned near the 1130nm, and maximum fluorescence halfwidth is 250nm, and maximum fluorescence lifetime is 650 μ s, and stimulated emission cross section is approximately 1.0 * 10 -20Cm 2.2001 on February 22,, liana is quiet to wait the people to apply for being entitled as " optical fiber and image intensifer " (the open 2002-252397 of special permission) again, and its basic glass consists of: Al 2O 3-SiO 2-Bi 2O 3, under 1750 ℃, found, draw out corresponding optical fiber, realized the light amplification at 1.3 μ m places under the 0.8 μ m pumping.
December 13 calendar year 2001, on June 18th, 2002, on December 25th, 2002, this positive first-class of the bank of Nippon Sheet Glass Co Ltd has applied for being entitled as the patent (special permission open 2003-183047,2004-20994,2003-283028) of " red glass and transparent glass-ceramics thereof ", " light amplification glass optical fiber ", " infrared lumious material and optical amplification medium " continuously, and its basic glass consists of A 2O-BO-Al 2O 3-SiO 2-Bi 2O 3(A=basic metal; The B=alkaline-earth metal).Corresponding product presents red or red-brown; Red glass its color after crystallization is handled does not have obvious change, but character such as its thermotolerance and physical strength obviously strengthen; Pumping wavelength pumping with being positioned at 400~850nm zone can access the fluorescence that highest peak is positioned at 1000~1600nm interval, and can realize the light amplification of wavelength between 1000~1400nm; Bismuth oxide, aluminum oxide and silicon-dioxide etc. are the necessary basal component of this luminescent material of preparation.
Be developed into erbium-doped fiber amplifier (EDFA) from the end of the eighties to the beginning of the nineties, and begin to be applied to have promoted opticfiber communication and developed since the opticfiber communication cable of 1.55mm frequency range, and technological development and the commercialization of present EDFA are the most ripe to full optical transmission direction; The EDFA fiber amplifier has been abandoned traditional photoelectricity light data-transmission mode, and directly optical signal is amplified, thereby effectively overcome the electronic bottleneck problem in the original transmission mode, this image intensifer also has in real time simultaneously, high gain, broadband, online, lower noise, low-loss full optical amplification function, is requisite Primary Component in the opticfiber communication cable of new generation; Because this technology has not only solved the restriction of decay to optical-fiber network transfer rate and distance, the more important thing is that it has started the wavelength-division multiplex of 1550nm frequency range, thereby ultra-high speed, vast capacity, over distance wavelength-division multiplex (WDM), dense wave division multipurpose (DWDM), full light transmission, soliton transmission etc. will be become a reality, and be epoch-making milestones on the opticfiber communication development history.At present widely used is that its operation window of C-band EDFA is at 1530~1565nm, it is minimum to have fibre loss, output rating is big, gain is high,, amplification characteristic low with polarization irrelevant, noise figure has nothing to do with systematic bits rate and data layout, and amplify a series of characteristics such as multichannel wavelength signals simultaneously, in long-distance optical communication system, obtained using widely.Its deficiency is that the gain bandwidth of C-Band EDFA has only 35nm, only covers the part of quartzy single-mode fiber low loss window, has restricted the intrinsic wavelength channel number that can hold of optical fiber; Yet along with developing rapidly and the quickening of IT application process of Internet technology, require the transmission capacity of ferry optical transmission system constantly to enlarge, and will enlarge transmission capacity, mainly contain three kinds of solution routes at present: (1) increases the transfer rate of each wavelength; (2) reduce channel separation; (3) increase total transmission bandwidth.For first kind of way, will bring new dispersion compensation problem if speed is brought up to 10Gbit/s, moreover present electronic system also exists what is called " electronic bottleneck " effect problem.If second kind of way is reduced to 50GHz or 25GHz will bring four-wave mixing non-linear effects such as (FWM) to system with sitgnal distancel from 100GHz, and requires system to adopt Wavelength stabilized technology.The EDFA that studies new fiber amplifier such as L-band is increase total transmission bandwidth a kind of, and it expands to L-band 1570~1605nm with the EDFA operation wavelength by C-band 1530~1560nm, makes the gain amplifier spectrum of EDFA expand one times.Although the wavelength of L-band EDFA has covered the afterbody of EDF gain spectral, but still can compare favourably with advanced in performance C-band EDFA product: for example both basic structure is similar, and the design and fabrication technology of most of C-band EDFA still can be applicable to L-band EDFA development; L-band EDFA has less radiation and the absorption and the lower average counter-rotating factor, and the gain fluctuation coefficient is much smaller than C-band EDFA, and existence brings the passive fiber loss bigger because the EDF of L-band EDFA is long, amplifies the big slightly deficiency that waits of noise.Though EDFA can make bandwidth increase to some extent from C-Band to the L-Band development, but be based on rare earth ion as the optical amplifier of activator because the restriction of the luminosity of himself, very difficult acquisition has bigger gain bandwidth, the luminescent material of shorter wavelength region (for example 1500nm or shorter).
The Raman amplifier can provide gain in big bandwidth range, the highest bandwidth that 300nm is provided of this amplification, but this needs higher drawing power (for length less than the optical fiber of 100m greater than 1 watt), thus communication system is had higher requirement.
As the active ions of crystalline host material, (1000~1500nm) can send the fluorescence with big bandwidth to transition metal, such as the sapphire (Ti:Al of Doped with Titanium in the near-infrared region for they for a long time 2O 3) can provide optical gain, Cr for another example at 650-1100nm 4+Ion is as the crystallo-luminescence material of activator, 1988, people such as V.Petricevic obtained the output of 1167~1345nm tunable laser, same year in mixing the forsterite of chromium, people such as Angert have also realized 1350~1500 interval tunable Cr at YAG:Cr among the Ca 4+Laser output.Owing to have suitable wavelength region and bandwidth, so the material of doped transition metal ions just can be used for communication field.But, because general transmission medium all is the glass optical fiber material, therefore crystalline material is docked in the communication system with regard to difficult, so very natural people just expect transition metal ion is mixed in the glass host material, above-mentioned like this butt joint problem just can be readily solved.2000, SetsuhisaTanabe and Xian Feng were with Cr 4+Mix in the aluminate glass, obtained the fluorescence that is positioned at 1.3 μ m 2003 that bandwidth surpasses 200nm, Fujimoto and Nakatsuka realized mixing the light amplification of bismuth silica glass at 1.3 μ m.
The melt temperature of silica glass is higher, even if report fusion under 1760 ℃ high temperature in the document still has a large amount of bubbles and exists.
Summary of the invention
The objective of the invention is for the higher shortcoming of the melt temperature that overcomes above-mentioned silica glass, a kind of bismuth germanium base optical glass and preparation method thereof of mixing is provided, this glass melting temperature is obviously much lower, thereby eliminate influence of air bubbles will easier realization, and has an optical property of the ultra broadband that can cover whole communication band, be expected at ultra broadband optics amplifier, superpower laser, technical fields such as tunable laser are applied.
Technology of the present invention solves that to put case as follows:
A kind of bismuth germanium base optical glass of mixing, each is composed as follows to it is characterized in that this glass:
Form mol%
GeO 2 90~99.98;
M=Al 2O 3, Ta 2O 5, Ga 2O 3Or B 2O 30.01~9;
Bi 2O 3 0.01~5。
The described preparation method who mixes bismuth germanium base optical glass comprises the following steps:
1. selected glass is formed and content mol%, and each raw material by the certain total amount of this proportioning weighing grinds half an hour in agate mortar;
2. then 500 ℃ of following pre-burnings 7 hours, take out grinding after, again 1550 ℃ of fusions 2 hours;
3. melt is poured over fast on the stainless steel plate and with another block plate and flattens, and transfers in the annealing furnace, naturally cools to room temperature with stove in annealing under 500 ℃ after 7 hours, and taking-up promptly gets this and mixes bismuth germanium base optical glass.
In this glass ingredient, GeO 2Be glass network former, Bi 2O 3Provide the raw material of light emitting ionic, can form the luminescence center relevant with bismuth, M is that glass network is modified body, the viscosity of reduction glass melting liquid that can be suitable, be beneficial to from crucible and pour out, be again the essential composition that this glass can produce fluorescence, also can disperse luminescence center to a certain extent simultaneously, play the effect of dispersion agent.
This glass sample is because of Bi 2O 3Concentration different and present pink, purplish red or reddish-brown; All samples are all transparent and do not have bubble and exist.Test shows: different luminosity and the fluorescence lifetimes of forming glass are different, wavelength be respectively 532,632.5 and the pumping of 808nm light source under, all samples all can produce fluorescence halfwidth (FWHM) greater than 200nm, fluorescence lifetime is greater than the fluorescence that is positioned at 1000~1700nm of 200 μ s.
Description of drawings
Fig. 1 is glass 96GeO of the present invention 23Al 2O 31.0Bi 2O 3Absorption spectrum
Fig. 2 is glass 96GeO of the present invention 23Al 2O 31.0Bi 2O 3Fluorescence spectrum under different pumping wavelengths
Fig. 3 is glass 96GeO of the present invention 23Ta 2O 51.0Bi 2O 3Absorption spectrum
Fig. 4 glass 96GeO of the present invention 23Ta 2O 51.0Bi 2O 3Fluorescence spectrum under different pumping wavelengths
Fig. 5 is glass 96GeO of the present invention 23Ga 2O 31.0Bi 2O 3Absorption spectrum
Fig. 6 glass 96GeO of the present invention 23Ga 2O 31.0Bi 2O 3Fluorescence spectrum under different pumping wavelengths
Fig. 7 is glass 96GeO of the present invention 23B 2O 31.0Bi 2O 3Absorption spectrum
Fig. 8 glass 96GeO of the present invention 23B 2O 31.0Bi 2O 3Fluorescence spectrum under different pumping wavelengths
Embodiment
The invention will be further described below in conjunction with embodiment and accompanying drawing, but should not limit protection scope of the present invention with this.
Table 1, table 2, table 3 and table 4 have been listed M=Al in the glass composition of the present invention respectively 2O 3, Ta 2O 5, Ga 2O 3, B 2O 3Composition and the molar percentage thereof of four groups of embodiment, the color of corresponding glass, fluorescence position and halfwidth thereof, the test result of fluorescence lifetime, wherein embodiment 1,4,21,24,31,34,41 and 44 is Comparative Examples.
Embodiment group 1
The preparation method is as follows: the batching of pressing the about 20g of proportioning weighing of table 1, in agate mortar, grind half an hour, then 500 ℃ of following pre-burnings 7 hours, after taking out grinding, again in 1550 ℃ of fusions 2 hours, so that thoroughly eliminate bubble, melt is poured over fast on the stainless steel plate and with another block plate and flattens, transfer in the annealing furnace and naturally cool to room temperature with stove after 7 hours, take out and promptly get sample in annealing under 500 ℃.Glass sample is because of Bi 2O 3Concentration different and present pink, purplish red or reddish-brown; All samples are all transparent and do not have bubble and exist.Sample cuts into 10 * 10 * 1mm 3, the polishing back is for the usefulness of test.Table 1 has listed file names with the luminosity and the fluorescence lifetime of the glass of these compositions.As seen from the table, corresponding 99GeO 21.0Bi 2O 3The glass of forming, promptly Comparative Examples 1, no matter is the laser pumping of 532nm, and still 632.5 and the pumping of 808nm is neither can produce fluorescence, only just can produce fluorescence later on mixing aluminum oxide, the adding of visible aluminum oxide is to produce the fluorescence essential condition; The centre wavelength of fluorescence is with Bi 2O 3The increase gradually of concentration, clocklike move to long wave; Fluorescence has dependency to pumping wavelength.Fig. 1 is for consisting of 96GeO 23Al 2O 31.0Bi 2O 3Absorption spectrum, by 500,700,800 and four absorption bands of 1000nm form, cover from seeing the zone of infrared broadness like this, this makes it the easier pumping source that searches out coupling, the absorption spectrum of the glass of other compositions with it with.Fig. 2 is for consisting of 96GeO 23Al 2O 31.0Bi 2O 3The fluorescence spectrum under different pumping wavelengths, present the characteristics of ultra broadband, and disclose and can but can find its pumping source in 450~1000nm interval, also the glassy phase of composition is seemingly therewith for the glass of other compositions.
Embodiment group 2
Press the batching of the proportioning weighing 20g of table 2, in agate mortar, grind half an hour, then 500 ℃ of following pre-burnings 7 hours, after taking out grinding, again in 1550 ℃ of fusions 2 hours, so that thoroughly eliminate bubble, melt is poured over fast on the stainless steel plate and with another block plate and flattens, transfer in the annealing furnace and naturally cool to room temperature with stove after 7 hours, take out and promptly get sample in annealing under 500 ℃.Glass sample is because of Bi 2O 3Concentration different and present pink, purplish red or reddish-brown; All samples are all transparent and do not have bubble and exist.Sample cuts into 10 * 10 * 1mm 3, the polishing back is for the usefulness of test.Table 2 has listed file names with the luminosity and the fluorescence lifetime of the glass of these compositions.As seen from the table, corresponding 99GeO 21.0Bi 2O 3The glass of forming, promptly Comparative Examples 21, no matter are the laser pumpings of 532nm, and still 632.5 and the pumping of 808nm is neither can produce fluorescence, only just can produce fluorescence later on mixing tantalum oxide, the adding of visible tantalum oxide is to produce the fluorescence essential condition; The centre wavelength of fluorescence is with Bi 2O 3The increase gradually of concentration, clocklike move to the long wave direction; Fluorescence has dependency to pumping wavelength.Fig. 3 is for consisting of 96GeO 23Ta 2O 51.0Bi 2O 3Absorption spectrum, by 508,712,800 and four absorption bands of 1000nm form, cover from seeing the zone of infrared broadness like this, this makes it the easier pumping source that searches out coupling, the absorption spectrum of the glass of other compositions with it with.Fig. 4 is for consisting of 96GeO 23Ta 2O 51.0Bi 2O 3The fluorescence spectrum under different pumping wavelengths, present the characteristics of ultra broadband, and disclose and can all can find its pumping source in 450~1000nm interval, also the glassy phase of composition is seemingly therewith for the glass of other compositions.
Embodiment group 3
Press the batching of the proportioning weighing 20g of table 3, in agate mortar, grind half an hour, then 500 ℃ of following pre-burnings 7 hours, after taking out grinding, again in 1550 ℃ of fusions 2 hours, so that thoroughly eliminate bubble, melt is poured over fast on the stainless steel plate and with another block plate and flattens, transfer in the annealing furnace and naturally cool to room temperature with stove after 7 hours, take out and promptly get sample in annealing under 500 ℃.Glass sample is because of Bi 2O 3Concentration different and present pink, purplish red or reddish-brown; All samples are all transparent and do not have bubble and exist.Sample cuts into 10 * 10 * 1mm 3, the polishing back is for the usefulness of test.Table 3 has listed file names with the luminosity and the fluorescence lifetime of the glass of these compositions.As seen from the table, corresponding 99GeO 21.0Bi 2O 3The glass of forming, promptly Comparative Examples 31, no matter are the laser pumpings of 532nm, and still 632.5 and the pumping of 808nm is neither can produce fluorescence, only just can produce fluorescence later on mixing gallium oxide, the adding of visible gallium oxide is to produce the fluorescence essential condition; The centre wavelength of fluorescence is with Bi 2O 3The increase gradually of concentration, clocklike move to the long wave direction; Fluorescence has dependency to pumping wavelength.Fig. 5 is for consisting of 96GeO 23Ga 2O 31.0Bi 2O 3Absorption spectrum, by 501,708,800 and four absorption bands of 1000nm form, cover from seeing the zone of infrared broadness like this, this makes it the easier pumping source that searches out coupling, the absorption spectrum of the glass of other compositions with it with.Fig. 6 is for consisting of 96GeO 23Ga 2O 31.0Bi 2O 3The fluorescence spectrum under different pumping wavelengths, present the characteristics of ultra broadband, and disclose and can all can find its pumping source in 450~1000nm interval, also the glassy phase of composition is seemingly therewith for the glass of other compositions.
Embodiment group 4
Press the batching of the proportioning weighing 20g of table 4, in agate mortar, grind half an hour, then 500 ℃ of following pre-burnings 7 hours, after taking out grinding, again in 1550 ℃ of fusions 2 hours, so that thoroughly eliminate bubble, melt is poured over fast on the stainless steel plate and with another block plate and flattens, transfer in the annealing furnace and naturally cool to room temperature with stove after 7 hours, take out and promptly get sample in annealing under 500 ℃.Glass sample is because of Bi 2O 3Concentration different and present pink, purplish red or reddish-brown; All samples are all transparent and do not have bubble and exist.Sample cuts into 10 * 10 * 1mm 3, the polishing back is for the usefulness of test.Table 4 has listed file names with the luminosity and the fluorescence lifetime of the glass of these compositions.As seen from the table, corresponding 99GeO 21.0Bi 2O 3The glass of forming, promptly Comparative Examples 41, no matter are the laser pumpings of 532nm, and still 632.5 and the pumping of 808nm is neither can produce fluorescence, only just can produce fluorescence later on mixing boron oxide, the adding of visible boron oxide is to produce the fluorescence essential condition; The centre wavelength of fluorescence is with Bi 2O 3The increase gradually of concentration, clocklike move to the long wave direction; Fluorescence has dependency to pumping wavelength.Fig. 7 is for consisting of 96GeO 23B 2O 31.0Bi 2O 3Absorption spectrum, by 508,705,800 and four absorption bands of 1000nm form, cover from seeing the zone of infrared broadness like this, this makes it the easier pumping source that searches out coupling, the absorption spectrum of the glass of other compositions with it with.Fig. 8 is for consisting of 96GeO 23B 2O 31.0Bi 2O 3The fluorescence spectrum under different pumping wavelengths, present the characteristics of ultra broadband, and disclose and can but can find its pumping source in 450~1000nm interval, also the glassy phase of composition is seemingly therewith for the glass of other compositions.
Table 1
Table 1
Table 2
Table 3
Table 4
*Semiconductor laser diode pumping with 808nm.

Claims (2)

1、一种掺铋锗基光学玻璃,其特征在于该玻璃各组成如下:1. A bismuth-doped germanium-based optical glass, characterized in that each composition of the glass is as follows: 组成                                              摩尔百分比Composition Mole Percentage GeO2                                             90~99.98;GeO 2 90~99.98; M=Al2O3,Ta2O5,Ga2O3或B2O3        0.01~9;M=Al 2 O 3 , Ta 2 O 5 , Ga 2 O 3 or B 2 O 3 0.01~9; Bi2O3                                           0.01~5。Bi 2 O 3 0.01-5. 2、根据权利要求1所述的掺铋锗基光学玻璃的制备方法,其特征在于该方法包括下列步骤:2. The method for preparing bismuth-germanium-doped optical glass according to claim 1, characterized in that the method comprises the following steps: ①选定玻璃组成和含量mol%,按该配比称量一定总量的各原料,在玛瑙研钵中研磨半小时;① select the glass composition and content mol%, weigh a certain amount of each raw material according to the proportion, and grind it in an agate mortar for half an hour; ②然后在500℃下预烧7小时,拿出研磨后,再在1550℃熔融2小时;② Then pre-fire at 500°C for 7 hours, take it out and grind it, and then melt it at 1550°C for 2 hours; ③熔体快速倾倒在一不锈钢板上并用另一块钢板压平,转移到退火炉中,在500℃下退火7小时后,随炉自然冷却到室温,取出即得该掺铋锗基光学玻璃。③The melt is quickly poured on a stainless steel plate and flattened with another steel plate, transferred to an annealing furnace, annealed at 500°C for 7 hours, cooled naturally to room temperature with the furnace, and taken out to obtain the bismuth-germanium-doped optical glass.
CN 200410054216 2004-09-02 2004-09-02 bismuth-doped germanium-based optical glass and preparation method thereof Expired - Fee Related CN1269755C (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN 200410054216 CN1269755C (en) 2004-09-02 2004-09-02 bismuth-doped germanium-based optical glass and preparation method thereof

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN 200410054216 CN1269755C (en) 2004-09-02 2004-09-02 bismuth-doped germanium-based optical glass and preparation method thereof

Publications (2)

Publication Number Publication Date
CN1587142A CN1587142A (en) 2005-03-02
CN1269755C true CN1269755C (en) 2006-08-16

Family

ID=34603084

Family Applications (1)

Application Number Title Priority Date Filing Date
CN 200410054216 Expired - Fee Related CN1269755C (en) 2004-09-02 2004-09-02 bismuth-doped germanium-based optical glass and preparation method thereof

Country Status (1)

Country Link
CN (1) CN1269755C (en)

Families Citing this family (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102701589A (en) * 2012-06-27 2012-10-03 华南理工大学 Red germanate glass and preparation method thereof
CN102730970A (en) * 2012-06-27 2012-10-17 华南理工大学 Red silicate glass and preparation method thereof
CN103086601B (en) * 2012-12-13 2015-06-03 昆明理工大学 Bismuth-doped germinate ultra wideband optical glass and preparation method thereof
FR3002530A1 (en) * 2013-02-28 2014-08-29 Centre Nat Rech Scient GLASSES AND VITROCERAMICS TRANSPARENT NANOSTRUCTURES IN VISIBLE AND INFRARED
CN103214183B (en) * 2013-03-28 2016-12-28 华南理工大学 A kind of lower conversion glass substrate and preparation method thereof and the application in CdTe solaode
CN105068178B (en) * 2015-07-17 2018-02-27 华南理工大学 A kind of near-infrared luminous bismuth doping multicomponent optical fiber and preparation method
CN108233165B (en) * 2018-01-22 2020-03-17 暨南大学 Near-infrared bismuth-tantalum double-doped laser crystal facing 0.95-1.65 micron all-solid-state laser
CN110752283A (en) * 2019-10-12 2020-02-04 华南理工大学 A broadband near-infrared LED device
CN114477764B (en) * 2022-01-26 2023-04-21 华南理工大学 Bismuth-thulium co-doped gain glass with high-efficiency broadband and preparation method thereof
CN116354598A (en) * 2023-03-01 2023-06-30 华南理工大学 A bismuth-gallium co-doped gain fiber used as a gain medium and its preparation method

Also Published As

Publication number Publication date
CN1587142A (en) 2005-03-02

Similar Documents

Publication Publication Date Title
Chen et al. Thermal stability and spectroscopic properties of Er3+-doped niobium tellurite glasses for broadband amplifiers
EP1285891B1 (en) Tellurite glass, optical amplifier and light source
Lakshmi et al. Structural, optical and NIR studies of Er3+ ions doped bismuth boro tellurite glasses for luminescence materials applications
El-Mallawany et al. Study of luminescence properties of Er3+-ions in new tellurite glasses
US6356699B1 (en) Rare earth doped optical glasses
US6589895B2 (en) Thulium-doped germanate glass composition and device for optical amplification
JP2002510595A (en) Antimony oxide glass with optical activity
Marcondes et al. Thermal and spectroscopic properties studies of Er3+-doped and Er3+/Yb3+-codoped niobium germanate glasses for optical applications
CN1269755C (en) bismuth-doped germanium-based optical glass and preparation method thereof
US5378664A (en) Optical fiber amplifier and a glass therefor
Zheng et al. The 1.53 μm spectroscopic properties and thermal stability in Er3+/Ce3+ codoped TeO2–WO3–Na2O–Nb2O5 glasses
Lakshminarayana et al. NIR luminescence from Er–Yb, Bi–Yb and Bi–Nd codoped germanate glasses for optical amplification
Lakshminarayana et al. Fluorescence features of Tm3+-doped multicomponent borosilicate and borotellurite glasses for blue laser and S-band optical amplifier applications
Ding et al. Pr3+/Tm3+/Er3+ tri-doped tellurite glass with ultra-broadband luminescence in the optical communication band
Shen et al. Broadband and flat near-infrared emission from Er3+/Tm3+ codoped tellurite glass for amplifier applications
Tikhomirov et al. Er3+ doped ultra-transparent oxy-fluoride glass-ceramics for application in the 1.54 μm telecommunication window
Petit et al. Effect of the introduction of Na2B4O7 on erbium luminescence in tellurite glasses
Li et al. Optical properties of Er3+ in MoO3–Bi2O3–TeO2 glasses
CN101168473B (en) Ytterbium nickel co-doped transparent silicate glass-ceramics and preparation method thereof
Xu et al. Effect of SiO2 content on the thermal stability and spectroscopic properties of Er3+/Yb3+ co-doped tellurite borate glasses
CN101182121B (en) Bismuth-nickel co-doped transparent silicate glass-ceramics and preparation method thereof
Chung et al. Selenide glass optical fiber doped with Pr3+ for U‐band optical amplifier
CN100513339C (en) Rare earth doped gallium germanium bismuth lead luminous glass material and its preparation method and uses
Duan et al. Effect of CdF2 addition on thermal stability and upconversion luminescence properties in Tm3+–Yb3+ codoped oxyfluoride silicate glasses
Gao et al. Study of luminescence properties of novel Er3+ single-doped and Er3+/Yb3+ co-doped tellurite glasses

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C14 Grant of patent or utility model
GR01 Patent grant
C17 Cessation of patent right
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20060816

Termination date: 20120902