CN104774013B - Y2O3:Eu3+ illuminant doped MgB2 superconductor with high critical transition temperature - Google Patents

Y2O3:Eu3+ illuminant doped MgB2 superconductor with high critical transition temperature Download PDF

Info

Publication number
CN104774013B
CN104774013B CN201510121032.1A CN201510121032A CN104774013B CN 104774013 B CN104774013 B CN 104774013B CN 201510121032 A CN201510121032 A CN 201510121032A CN 104774013 B CN104774013 B CN 104774013B
Authority
CN
China
Prior art keywords
superconductor
mgb
illuminator
transition temperature
doping
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
CN201510121032.1A
Other languages
Chinese (zh)
Other versions
CN104774013A (en
Inventor
赵晓鹏
张志伟
陶硕
陈国维
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.)
Northwestern Polytechnical University
Original Assignee
Northwestern Polytechnical University
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 Northwestern Polytechnical University filed Critical Northwestern Polytechnical University
Priority to CN201510121032.1A priority Critical patent/CN104774013B/en
Publication of CN104774013A publication Critical patent/CN104774013A/en
Application granted granted Critical
Publication of CN104774013B publication Critical patent/CN104774013B/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Abstract

The invention relates to an Y2O3:Eu3+ illuminant doped MgB2 superconductor with a high critical transition temperature. The Y2O3:Eu3+ illuminant is used to change the MgB2 superconductor transition temperature. The hydrothermal method is adopted to prepare an Y2O3:Eu3+ nano rod, and a solid doping method is utilized to prepare the Y2O3:Eu3+ illuminant doped MgB2 superconductor. In the hydrothermal method, the mole ratio of Y to Eu is 0.95:0.05; in the prepared Y2O3:Eu3+ illuminant doped MgB2 superconductor, the atomic ratio of Mg and B is 1.2:2, and the Y2O3:Eu3+ illuminant accounts for 4 to 8% of the total weight of the MgB2 superconductor. In the absence of an external magnetic field, when the Y2O3:Eu3+ illuminant accounts for 8% of the total weight of the MgB2 superconductor, the Tc (37.4 K) of the doped MgB2 superconductor is higher than that (Tc=37 K) of the pure MgB2.

Description

A kind of Y with high critical transition temperature2O3:Eu3+Illuminator doping MgB2Superconductor
Technical field
The present invention relates to a kind of improve MgB2The method of superconductor transition temperature, make use of Y2O3:Eu3+Illuminator is to MgB2 The impact of superconductor transition temperature.
Background technology
Intermetallic compound Mg B is found that in calendar year 2001, Akimitsu of Japan et al.2With superconducting characteristic, pass through The high-pressure sinter of 196MPa obtains its critical-temperature for 39K.Binary metal boride MgB2The discovery of superconducting characteristic, causes this Very big concern of the researcher in field to fundamental research and the application of superconductor.MgB2With of a relatively high stagnation temperature Degree (the close 40K of its transition temperature), larger superconduction correlation length, high critical current density and wider energy gap etc. are excellent Point, therefore it has huge application potential in terms of superconductive device.MgB2Simple structure, it is easy to make and process, it has Far above the critical-temperature of cryogenic superconductor, and not there are problems that the Weak link for being difficult to overcome in high-temperature superconductor, therefore, MgB2 Development and application to superconductor technology brings new opportunity.Additionally, MgB2Itself belongs to type, with dual intensity Gap, superconducting mechanism is unique, for the basic research of superconductivity theory has very big impetus.Therefore, MgB2Superconductor without It is of great significance by all having to basic research or application study.
Y2O3:Eu3+Illuminator has good luminescent properties, in atmosphere with preferable stability, will not be as sulfuration Thing dangerous property like that.MgB2Belong to the typical material of BCS theory category, be the type of standard, simple structure is made Valency is cheap, it is easy to synthesize.But MgB2Superconducting critical transition temperature it is not high limit its application, it is desirable to by adulterate come Improve its superconducting transition temperature.But substantial amounts of result of study shows, many chemical dopings all cause MgB2The T of superconductorcDrop It is low.Because MgB2The impurity of material is not easily accomplished very much, and most atoms cannot adulterate and enter MgB2Lattice in.Separately On the one hand, chemical doping can affect the physical propertys such as carrier concentration, lattice paprmeter and crystallization degree.For example, Al and C mixes Miscellaneous, they instead of respectively MgB2In Mg and B atoms, significantly reduce MgB2Tc.The present invention is from luminous to suiperconducting transition The impact of temperature is started with, and has prepared a kind of Y2O3:Eu3+The MgB of illuminator doping2Superconductor, by the doping reality of different proportion The contrast tested, draws a kind of Y with high critical transition temperature2O3:Eu3+Illuminator doping MgB2Superconductor.
The content of the invention
In view of the above circumstances, it is an object of the invention to prepare a kind of Y2O3:Eu3+The MgB of illuminator doping2Superconductor, The superconductor has high critical transition temperature, and makes easy.
The present invention prepares Y using hydro-thermal method2O3:Eu3+Nanometer rods, solid phase doping methods prepare Y2O3:Eu3+Illuminator doping MgB2Superconductor.As described below:
(1) a kind of Y with high critical transition temperature2O3:Eu3+The MgB of illuminator doping2Superconductor, wherein Y2O3:Eu3+ Illuminator nanometer rods are distributed in MgB2In superconductor sintered body;Y2O3:Eu3+Illuminator nanometer rods are distributed in MgB2Superconductor crystal grain Boundary;
(2) according to the MgB of the high critical transition temperature of above-mentioned (1)2Superconductor, wherein, hydro-thermal method prepares Y2O3:Eu3+Nanometer During rod, the mol ratio of Y and Eu is 0.95: 0.05;When in Y2O3:Eu3+The MgB of illuminator doping2Contain in superconductor sintered body The atomic ratio of Mg and B is 1.2: 2, wherein Y2O3:Eu3+Mass fraction shared by illuminator is 4%~8%;
(3) according to above-mentioned (1) or the MgB of the high critical transition temperature of (2)2Superconductor, works as Y2O3:Eu3+Shared by illuminator MgB2When superconductor mass fraction is 8%, under conditions of without external magnetic field, pure MgB2Tc=37K, Y2O3:Eu3+Illuminator The MgB of doping2The T of superconductorc=37.4K.
Description of the drawings
Fig. 1 .a hydro-thermal methods prepare Y2O3The flow chart of nanometer rods
Fig. 1 .b hydro-thermal methods prepare Y2O3:Eu3+The flow chart of nanometer rods
Fig. 2 Y2O3:Eu3+The SEM figures of illuminator
Fig. 3 Y2O3:Eu3+The MgB of illuminator doping2The SEM figures of superconductor
The Y of Fig. 4 .a embodiments one2O3And Y2O3:Eu3+The MgB of illuminator doping2Superconductor XRD
The Y of Fig. 4 .b embodiments one2O3And Y2O3:Eu3+The MgB of illuminator doping2Superconductor low-temperature resistance figure
The Y of Fig. 5 .a embodiments two2O3And Y2O3:Eu3+The MgB of illuminator doping2Superconductor XRD
The Y of Fig. 5 .b embodiments two2O3And Y2O3:Eu3+The MgB of illuminator doping2Superconductor low-temperature resistance figure
The Y of Fig. 6 .a embodiments three2O3And Y2O3:Eu3+The MgB of illuminator doping2Superconductor XRD
The Y of Fig. 6 .b embodiments three2O3And Y2O3:Eu3+The MgB of illuminator doping2Superconductor low-temperature resistance figure
Specific embodiment
The present invention prepares Y using hydro-thermal method2O3:Eu3+Nanometer rods, solid phase doping methods prepare Y2O3:Eu3+Illuminator doping MgB2Superconductor.Concrete preparation process is as follows:
(1) Y of 0.306g is weighed2O3With the Eu of 0.025g2O3, the mol ratio of Y and Eu is dissolving at 0.95: 0.05,50 DEG C In excess nitric acid, Y (NO are obtained3)3With Eu (NO3)3Mixed solution, mixed solution is heated to into 80 DEG C, be evaporated, removed Amount nitric acid, obtains white crystal, deionized water dissolving.The NaOH solution of addition 1M is in above-mentioned solution.Obtain PH=13.5 Precipitated liquid, move to reactor, 2h is incubated at 180 DEG C, room temperature is naturally cooled to afterwards.The solution in reactor is taken out, is washed, Alcohol is washed, and each three times, is precipitated liquid A, and A is dried into a few hours acquisition Y at 90 DEG C2O3:Eu3+Rod precursor B.By B at 800 DEG C Calcining obtains Y in 2 hours2O3:Eu3+Nanometer rods.If being added without Eu in above-mentioned preparation process2O3, can finally prepare Y2O3Receive Rice rod.Preparation flow figure is as shown in Figure 1.
(2) in glove box, in molar ratio magnesium powder and boron powder are weighed at 1.2: 2, is fully ground after mixing, place into compressing tablet Compressing tablet is carried out in mould.During tube type vacuum stove is put into after compression molding, under flowing Ar atmosphere, 5 DEG C/min of heating rate exists respectively 640 DEG C and 800 DEG C are incubated 1 hour, so as to obtain MgB2Sample.Weigh magnesium powder 0.22g, boron powder 0.18g, respectively with respective quality The Y of fraction2O3、Y2O3:Eu3+Mixed grinding, compressing tablet prepare corresponding doped samples according to above-mentioned sintering process.
The present invention's realizes process and material property by embodiment and description of the drawings:
Embodiment one:
(1) hydro-thermal method prepares Y2O3And Y2O3:Eu3+Nanometer rods:Preparation flow figure is as shown in Figure 1.
(2) solid phase doping methods prepare pure MgB2、Y2O3And Y2O3:Eu3+The MgB of illuminator doping2(mass fraction is superconductor 4%).
(3) material phase analysis are carried out to sample using Dutch PANalytical company X ' Pert MPD PRO types X-ray diffractometers;Profit With the liquid helium cryogenic system of Advanced Research Systems companies of the U.S., sample resistance is measured using four probe method The curve for varying with temperature:As shown in Figure 4.Can see from Fig. 4 .a, Y2O3And Y2O3:Eu3+The MgB of illuminator doping2It is super The principal phase of conductor sample is MgB2, also have the Y that some are remained in addition2O3Phase, the source of impurities phase MgO is probably 1. gloves 2. tableting processes or sample are shifted from glove box to vacuum tube furnace for the trace oxygen in high-purity argon in case process of lapping During to have touched the vacuum of a small amount of oxygen 3. vacuum tube furnace be not to contain micro oxygen in very high 4. Ar gas.From figure Can see in 4.b, doping causes the T of samplecReduce, and Y2O3:Eu3+The T of nanometer rods doped samplescThan Y2O3Receive The T of rice rod doped samplescIt is low.
Embodiment two:
(1) hydro-thermal method prepares Y2O3And Y2O3:Eu3+Nanometer rods:Preparation flow figure is as shown in Figure 1.
(2) solid phase doping methods prepare pure MgB2、Y2O3And Y2O3:Eu3+The MgB of illuminator doping2(mass fraction is superconductor 6%).
(3) material phase analysis are carried out to sample using Dutch PANalytical company X ' Pert MPD PRO types X-ray diffractometers;Profit With the liquid helium cryogenic system of Advanced Research Systems companies of the U.S., sample resistance is measured using four probe method The curve for varying with temperature:As shown in Figure 5.Can see from Fig. 5 .a, Y2O3And Y2O3:Eu3+The MgB of illuminator doping2Superconduction The principal phase of body sample is MgB2, also have the Y that some are remained in addition2O3Phase, institute in the source such as embodiment one of impurities phase MgO State.Can see from Fig. 5 .b, doping causes the T of samplecReduce, and Y2O3:Eu3+The T of nanometer rods doped samplescWill Compare Y2O3The T of nanometer rods doped samplescIt is low, and comparison diagram 4.b it is found that doping amount it is more, the T of samplecIt is lower.
Embodiment three:
(1) hydro-thermal method prepares Y2O3And Y2O3:Eu3+Nanometer rods:Preparation flow figure is as shown in Figure 1.
(2) solid phase doping methods prepare pure MgB2、Y2O3And Y2O3:Eu3+The MgB of illuminator doping2Superconductor (mass fraction For 8%).
(3) material phase analysis are carried out to sample using Dutch PANalytical company X ' Pert MPD PRO types X-ray diffractometers;Profit With the liquid helium cryogenic system of Advanced Research Systems companies of the U.S., sample resistance is measured using four probe method The curve for varying with temperature:As shown in Figure 6.Can see from Fig. 6 .a, Y2O3And Y2O3:Eu3+The MgB of illuminator doping2Superconduction The principal phase of body sample is MgB2, also have the Y that some are remained in addition2O3Phase, institute in the source such as embodiment one of impurities phase MgO State.Can see from Fig. 6 .b, Y2O3The T of nanometer rods doped samplescThan pure MgB2TcIt is low, but Y2O3:Eu3+Illuminator is mixed Miscellaneous MgB2The T of superconductor samplecPure MgB is exceeded2Tc, this just prepares a kind of Y with high critical transition temperature2O3:Eu3+ Illuminator doping MgB2Superconductor.
The preferred embodiments of the present invention are the foregoing is only, when the scope that the present invention is implemented can not be limited with this, i.e., Generally the simple equivalence changes made according to the claims in the present invention and description of the invention content and modification, all should still belong to the present invention In the range of patent is covered.

Claims (3)

1. a kind of Y with high critical transition temperature2O3:Eu3+Illuminator doping MgB2Superconductor, is primarily characterized in that hydro-thermal Method prepares Y2O3:Eu3+The mol ratio of nanometer rods, wherein Y and Eu is 0.95: 0.05;Solid phase doping methods prepare Y2O3:Eu3+Illuminator Doping MgB2Superconductor, wherein raw material Mg and B atomic ratios are 1.2: 2, Y2O3:Eu3+Superconductor mass fraction is shared by illuminator 4%~8%.
2. the as described in claim 1 MgB of high critical transition temperature2Superconductor, it is characterised in that Y2O3:Eu3+Illuminator is received Rice rod is distributed in MgB2At superconductor grain boundary.
3. the as described in claim 1 MgB of high critical transition temperature2Superconductor, it is characterised in that preparation technology includes following Step:
(1) Y of 0.306g is weighed2O3With the Eu of 0.025g2O3, it is dissolved at 50 DEG C in excess nitric acid, mixed solution is heated to 80 DEG C, it is evaporated, removes excess nitric acid, obtain white crystal, deionized water dissolving adds the NaOH solution of 1M to above-mentioned solution In;The precipitated liquid of PH=13.5 is obtained, reactor is moved to, 2h is incubated at 180 DEG C, room temperature is naturally cooled to afterwards;Take out reaction Solution in kettle, washing, alcohol is washed, and each three times, is precipitated liquid A, and A is dried into a few hours acquisition Y at 90 DEG C2O3:Eu3+Before rod Drive body B;B is obtained into Y in 2 hours in 800 DEG C of calcinings2O3:Eu3+Nanometer rods;
(2) in glove box, in molar ratio magnesium powder 0.22g, boron powder 0.18g, Y with respective quality fraction are weighed at 1.2: 22O3: Eu3+It is fully ground after mixing, places into and carry out in compression mold compressing tablet;During tube type vacuum stove is put into after compression molding, flow Ar Under atmosphere, 5 DEG C/min of heating rate is incubated 1 hour, so as to obtain Y at 640 DEG C and 800 DEG C respectively2O3:Eu3+Illuminator adulterates MgB2Superconductor sample.
CN201510121032.1A 2015-03-13 2015-03-13 Y2O3:Eu3+ illuminant doped MgB2 superconductor with high critical transition temperature Expired - Fee Related CN104774013B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201510121032.1A CN104774013B (en) 2015-03-13 2015-03-13 Y2O3:Eu3+ illuminant doped MgB2 superconductor with high critical transition temperature

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201510121032.1A CN104774013B (en) 2015-03-13 2015-03-13 Y2O3:Eu3+ illuminant doped MgB2 superconductor with high critical transition temperature

Publications (2)

Publication Number Publication Date
CN104774013A CN104774013A (en) 2015-07-15
CN104774013B true CN104774013B (en) 2017-04-19

Family

ID=53615823

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201510121032.1A Expired - Fee Related CN104774013B (en) 2015-03-13 2015-03-13 Y2O3:Eu3+ illuminant doped MgB2 superconductor with high critical transition temperature

Country Status (1)

Country Link
CN (1) CN104774013B (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN105788752B (en) * 2016-04-05 2018-04-13 西北工业大学 The MgB that electroluminescent excitation critical transition temperature improves2Base super conductor and preparation method thereof
CN108383531B (en) * 2018-05-15 2021-02-19 西北工业大学 MgB doped with topological luminophores in heterogeneous phase2Base superconductor and method for producing same
CN109942290A (en) * 2019-03-12 2019-06-28 西北工业大学 Bi (the Pb)-Sr-Ca-Cu-O of the topological heterogeneous phase doping of illuminator is super structure superconductor and preparation method thereof

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101295563B (en) * 2008-06-27 2010-12-08 北京工业大学 Production method of MgB2 block material doped with organic matter

Also Published As

Publication number Publication date
CN104774013A (en) 2015-07-15

Similar Documents

Publication Publication Date Title
Tang et al. Superconductivity in quasi-one-dimensional Cs 2 Cr 3 As 3 with large interchain distance
Zhao et al. High critical current density of MgB 2 bulk superconductor doped with Ti and sintered at ambient pressure
Ren et al. Superconductivity in the iron-based F-doped layered quaternary compound Nd [O1− x Fx] FeAs
Wu et al. Transport properties and superconductivity in Ba1-xMxFe2As2 (M= La and K) with double FeAs layers
CN103420675B (en) A kind of Nd 2-xce xcuO 4-δthe low temperature preparation method of superconducting nano porcelain powder
CN104774013B (en) Y2O3:Eu3+ illuminant doped MgB2 superconductor with high critical transition temperature
Shirage et al. Superconductivity at 43 K at ambient pressure in the iron-based layered compound La 1− x Y x FeAsO y
CN1929044B (en) MgB2 superconductive material containing Si element and C element and its preparing method
Long et al. Flipping of antiferromagnetic to superconducting states in pressurized quasi-one-dimensional manganese-based compounds
Xu et al. Microstructure and superconducting properties of nanocarbon-doped internal Mg diffusion-processed MgB2 wires fabricated using different boron powders
CN101295563B (en) Production method of MgB2 block material doped with organic matter
CN101224897A (en) Cu doped MgB2 superconductor and low-temperature rapid preparation method
CN102074309B (en) Method for preparing magnesium diboride composite superconducting material
CN105788752B (en) The MgB that electroluminescent excitation critical transition temperature improves2Base super conductor and preparation method thereof
CN102122549B (en) Application of glucose in preparation of magnesium diboride-doped superconducting material
Rodgers et al. Suppression of the superconducting transition of R FeAsO 1− x F x (R= Tb, Dy, and Ho)
Lu et al. Formation and texture of Bi-2223 phase during sintering in high magnetic fields
Cheng et al. The isotope effect of boron on the carbon doping and critical current density of Mg 11 B 2 superconductors
CN101608340B (en) Iron-based high-temperature superconductive crystal and preparation method thereof
CN102531610B (en) Glycine-doped MgB2 superconductor with high critical current density and preparation method thereof
Luo et al. Microstructure and superconducting properties of MgB2 bulks prepared from Mg+ B+ Mg (BH4) 2 composites
Wang et al. Superconducting properties of “111” type LiFeAs iron arsenide single crystals
CN101314544A (en) Method for quickly producing MgB2 cryogenic conductor at low-temperature
Qasim et al. Role of Co nanoparticles in CuTl-1223 superconductor
CN102982889B (en) MgB 2superconducting line and manufacture method thereof

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
EXSB Decision made by sipo to initiate substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant
CF01 Termination of patent right due to non-payment of annual fee
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20170419

Termination date: 20180313