Synthesis of novel superhard materials under ultrahigh pressure
固体超强酸催化α-蒎烯合成龙脑的研究
固体超强酸催化α-蒎烯合成龙脑的研究下载提示:该文档是本店铺精心编制而成的,希望大家下载后,能够帮助大家解决实际问题。
文档下载后可定制修改,请根据实际需要进行调整和使用,谢谢!本店铺为大家提供各种类型的实用资料,如教育随笔、日记赏析、句子摘抄、古诗大全、经典美文、话题作文、工作总结、词语解析、文案摘录、其他资料等等,想了解不同资料格式和写法,敬请关注!Download tips: This document is carefully compiled by this editor. I hope that after you download it, it can help you solve practical problems. The document can be customized and modified after downloading, please adjust and use it according to actual needs, thank you! In addition, this shop provides you with various types of practical materials, such as educational essays, diary appreciation, sentence excerpts, ancient poems, classic articles, topic composition, work summary, word parsing, copy excerpts, other materials and so on, want to know different data formats and writing methods, please pay attention!固体超强酸催化α-蒎烯合成龙脑的研究引言龙脑是一种广泛应用于药物、香料和化妆品等领域的重要化合物,其合成一直是有机化学领域的研究热点之一。
芳肼衍生物的合成与精制研究
化学杂交剂(Chemical hybridizing agent)是制备优良、高产杂交种子,提高粮食产量的重要方法之一。化学杂交剂育种的关键问题是要有去雄率高但又不影响雌性器官的优良化学杂交剂。哒嗪酮衍生物的合成及其在生物活性方面的研究和应用是近年的研究热点。在一些活性化合物的母体结构中引入其它活性基团,利用基团之间相互影响找到生物活性更佳的新型优良化学杂交剂是研究的一个重要方向。将具有广泛生物活性的噻二唑和吡唑酮基团引入到哒嗪酮环上,修饰该类化合物的结构,以期得到去雄活性好的先导化合物。
重氮化时所用的酸,从反应速度来说,以盐酸和氢溴酸最快,硫酸和硝酸较慢,但在置换反应中,仍以用硫酸为好。芳环上若有推电子基团,也会使反应加快。氨基的邻位若有取代基团,会产生位阻效应。
重氮盐多半易溶于水,只有少数杂酸盐和复盐不溶。这些不溶于水的重氮盐,往往比较稳定。它们中常见的有,氟硼酸盐、氟磷酸盐、1,5-萘二磺酸盐、氯化锌复盐、氯化汞复盐等。这些重氮盐在有机上合成都有广泛的应用。
常州大学
硕士学位论文
开题报告
课题名称芳肼衍生物的合成与精制研究
学 号__091012223___
姓 名___吴有才____
研究方向__有机合成___
二级学科__有机合成___
一级学科__有机化学___
学 院_石油化工学院
2010年11月16日
二 选题依据
1.课题的背景和研究依据
芳香杂环化合物的种类多,数量大,在自然界分布广泛,许多天然杂环化合物在动、植物体内起着重要的生理作用,例如,植物中的叶绿素,动物血液中的血红素,中草药中的有效成分生物碱及部分苷类,部分抗生素和维生素,组成蛋白质的某些氨基酸和核苷酸的碱基等都含有杂环的结构。因此,芳香杂环化合物在有机化合物尤其是有机药物中占有重要的地位。
Annu.Rev.Mater.Res.31_1_2001
Annu.Rev.Mater.Res.2001.31:1–23Copyright c2001by Annual Reviews.All rights reserved S YNTHESIS AND D ESIGN OF S UPERHARDM ATERIALSJ Haines,JM L´e ger,and G BocquillonLaboratoire de Physico-Chimie des Mat´e riaux,Centre National de la Recherche Scientifique,1place Aristide Briand,92190Meudon,France;e-mail:haines@cnrs-bellevue.fr;leger@cnrs-bellevue.frKey Words diamond,cubic boron nitride,carbon nitride,high pressure,stishovite s Abstract The synthesis of the two currently used superhard materials,diamond and cubic boron nitride,is briefly described with indications of the factors influencing the quality of the crystals obtained.The physics of hardness is discussed and the importance of covalent bonding and fixed atomic positions in the crystal structure,which determine high hardness values,is outlined.The materials investigated to date are described and new potentially superhard materials are presented.No material that is thermodynamically stable under ambient conditions and composed of light (small)atoms will have a hardness greater than that of diamond.Materials with hardness values similar to that of cubic boron nitride (cBN)can be obtained.However,increasing the capabilities of the high-pressure devices could lead to the production of better quality cBN compacts without binders.INTRODUCTIONDiamond has always fascinated humans.It is the hardest substance known,based on its ability to scratch any other material.Its optical properties,with the highest refraction index known,have made it the most prized stone in jewelry.Furthermore,diamond exhibits high thermal conductivity,which is nearly five times that of the best metallic thermal conductors (copper or silver)at room temperature and,at the same time,is an excellent electrical insulator,even at high temperature.In industry,the hardness of diamond makes it an irreplaceable material for grinding tools,and diamond is used on a large scale for drilling rocks for oil wells,cutting concrete,polishing stones,machining,and honing.The diamonds used for industry are now mostly man-made because their cutting edges are much sharper than those of natural diamonds,which have been eroded by geological time.The synthesis of diamond has been a goal of science from Moissant at the end of the nineteenth century to the successful synthesis under high pressures in 1955(1).However,diamond has a major drawback in that it reacts with iron and cannot be used for machining steel.This has prompted the synthesis of a second superhard0084-6600/01/0801-0001$14.001A n n u . R e v . M a t e r . R e s . 2001.31:1-23. D o w n l o a d e d f r o m a r j o u r n a l s .a n n u a l r e v i e w s .o r gb y C h i n e s e Ac ade m y of S c i e n c e s - L i b r a r y o n 05/16/09. F o r p e r s o n a l u s e o n l y .2HAINESL ´EGERBOCQUILLONmaterial,cubic boron nitride (cBN),whose structure is derived from that of dia-mond with half the carbon atoms being replaced by boron and the other half by nitrogen atoms.The resulting compound is half as hard as diamond,but it does not react with iron and can be used for machining steel.Cubic boron nitride does not exist in nature and is prepared under high-pressure high-temperature conditions,as is synthetic diamond.However,its synthesis is more difficult,and it has not been possible to prepare large crystals.Industry is thus looking for new superhard ma-terials that will need to be much harder than present ceramics (Si 3N 4,Al 2O 3,TiC).Hardness is a quality less well defined than many other physical properties.Hardness was first defined as the ability of one material to scratch another;this corresponds to the Mohs scale.This scale is highly nonlinear (talc =1,diamond =10);however,this definition of hardness is not reliable because materials of similar hardness can scratch each other and the resulting value depends on the specific details of the contact between the two materials.It is well known (2)that at room temperature copper can scratch magnesium oxide and at high temperatures cBN can scratch diamond (principle of soft indenter).Another,more accurate,way of defining and measuring hardness is by the indentation of the material by a hard indenter.According to the nature and shape of the indenter,different scales are used:Brinell,Rockwell,Vickers,and Knoop.The last two are the most frequently used.The indenter is made of a pyramidal-shaped diamond with a square base (Vickers),or elongated lozenge (Knoop).The hardness is deduced from the size of the indentation produced using a defined load;the unit is the same as that for pressure,the gigapascal (GPa).Superhard materials are defined as having a hardness of above 40GPa.The hardness of diamond is 90GPa;the second hardest material is cBN,with a hardness of 50GPa.The design of new materials with a hardness comparable to diamond is a great challenge to scientists.We first describe the current status of the two known super-hard materials,diamond and cBN.We then describe the search for new bulk super-hard materials,discuss the possibility of making materials harder than diamond,and comment on the new potentially superhard materials and their preparation.DIAMOND AND CUBIC BORON NITRIDE DiamondThe synthesis of diamond is performed under high pressure (5.5–6GPa)and high temperature (1500–1900K).Carbon,usually in the form of graphite,and a transi-tion metal,e.g.iron,cobalt,nickel,or alloys of these metals [called solvent-catalyst (SC)],are treated under high-pressure high-temperature conditions;upon heating,graphite dissolves in the metal and if the pressure and temperature conditions are in the thermodynamic stability field of diamond,carbon can crystallize as dia-mond because the solubility of diamond in the molten metal is less than that of graphite.Some details about the synthesis and qualities of diamond obtained by this spontaneous nucleation method are given below,but we do not describe the growthA n n u . R e v . M a t e r . R e s . 2001.31:1-23. D o w n l o a d e d f r o m a r j o u r n a l s .a n n u a l r e v i e w s .o r gb y C h i n e s e Ac ade m y of S c i e n c e s - L i b r a r y o n 05/16/09. F o r p e r s o n a l u s e o n l y .SUPERHARD MATERIALS 3of single-crystal diamond under high pressure,which is necessary in order to ob-tain large single crystals with dimensions greater than 1mm.Crystals of this size are expensive and represent only a very minor proportion of the diamonds used for machining;they are principally used for their thermal properties.It is well known that making diamonds is relatively straightforward,but control-ling the quality of the diamonds produced is much more difficult.Improvements in the method of synthesis since 1955have greatly extended the size range and the mechanical properties and purity of the synthetic diamond crystals.Depending on the exact pressure (P )and temperature (T )of synthesis,the form and the nature of the carbon,the metal solvent used,the time (t )of synthesis,and the pathways in P-T-t space,diamond crystals (3,4)varying greatly in shape (5),size,and fri-ability are produced.These three characteristics are used to classify diamonds;the required properties differ depending on the industrial application.Friability is related to impact strength.It is the most important mechanical property for the practical use of superhard materials,and low friability is required in order for tools to have a long lifetime.In commercial literature,the various types of diamonds are classed as a function of their uses,which depend mainly on their friabilities,but the numerical values are not given,so it is difficult to compare the qualities of diamonds from various sources.The friability,which is defined by the percentage of diamonds destroyed in a specific grinding process,is obtained by subjecting a defined quantity of diamonds to repeated impacts by grinding in a ball-mill or by the action of a load falling on them.The friability values depend strongly on the experimental conditions used,and only values for crystals measured under the same conditions can be compared.The effect of various synthesis parameters on their quality can be evaluated by considering the total mass of diamond obtained in one experiment,the distribution size of these diamonds,and the friability of the diamonds of a defined size.A first parameter is the source of the carbon.Most carbon-based substance can be used to make diamonds (6),but the nature of the carbon source has an effect on the quantity and the quality of synthetic diamonds.The best carbon source for diamond synthesis is graphite,and its characteristics are important.The effect of the density,gas permeability,and purity of graphite on the diamond yield have been investigated using cobalt as the SC (7).Variations of the density and gas permeability have no effect on the diamond yield,but carbon purity is important.The main impurity in synthetic graphite is CaO.If good quality diamonds are required,the calcium content should be kept below 1000ppm in order to avoid excessive nucleation on the calcium oxide particles.A second factor that alters the quality of diamonds is the nature of the SC.The friability and the size distribution are better with CoFe (alloy of cobalt with a small quantity of iron)than with invar,an iron-nickel alloy (Table 1:Ia,Ib;Figure 1a ).Another parameter is how the mixture of carbon and SC is prepared.When fine or coarse powders of intimately mixed graphite and SC are used,a high yield of diamonds with high friabilities is obtained (8).These diamonds are very small,A n n u . R e v . M a t e r . R e s . 2001.31:1-23. D o w n l o a d e d f r o m a r j o u r n a l s .a n n u a l r e v i e w s .o r g b y C h i n e s e A c a d e m y o f S c i e n c e s - L i b r a r y o n 05/16/09. F o r p e r s o n a l u s e o n l y .4HAINESL ´EGERBOCQUILLONTABLE 1Friabilities of some diamonds as a function of the details of the synthesis process fora selected size of 200–250µmSDA a MBS a 100+70Ia Ib IIa IIb IIc IIIa IIIb Synthesis CoFeInvar 1C-2SC 1C-1SC 2C-2SC Cycle A Cycle B detail stacking stacking stacking Friability 74121395053637250(%)aThe SDA 100+is among De Beers best diamond with a very high strength that is recommended for sawing the hardest stones and cast refractories.MBS 70is in the middle of General Electric’s range of diamonds for sawing and drilling.Other diamonds were obtained in the laboratory using a belt–type apparatus with a working chamber of 40mm diameter.(C,graphite;SC,solvent-catalyst.)with metal inclusions,and they are linked together with numerous cavities filled with SC.A favorable geometry in order to obtain well-formed diamonds is to stack disks of graphite and SC.The effect of local concentration has been exam-ined by changing the stacking of these disks (Table 1:IIa,IIb,IIc;Figure 1b ).The method of stacking modifies the local oversaturation of dissolved carbon and thus the local spontaneous diamond germination.For the synthesis of dia-mond,the heating current goes directly through the graphite-SC mixture.Because the electrical resistivity of the graphite is much greater than that of the SC,the temperature of the graphite is raised by the Joule effect,whereas that of the SC increases mainly because of thermal conduction.Upon increasing the thickness of the SC disk,the local thermal gradient increases and the dissolved atoms of carbon cannot move as easily;the local carbon oversaturation then enhances the spontaneous diamond germination.This enables one to work at lower tempera-tures and pressures,which results in slower growth and therefore better quality diamonds.Another important factor for the yield and the quality of the diamonds is the pathway followed in P-T-t space.The results of two cycles with the same final pressure and temperature are shown.In cycle A (Figure 1d ),the graphite-SC mixture reaches the eutectic melting temperature while it is still far from the equilibrium line between diamond and graphite;as a result spontaneous nucleation is very high and the seeds grow very quickly.These two effects explain the high yield and the poor quality and small size and high friability of the diamonds compared with those obtained in cycle B (Figure 1d ;see Table 1IIIa and IIIb and Figure 1c ).Large crystals (over 400µm)of good quality are obtained when the degree of spontaneous nucleation is limited.The pathway in P-T-t space must then remain near the graphite-diamond phase boundary (Figure 1d ),and the time of the treatment must be extended in the final P-T-t conditions.Usually,friability increases with the size of the diamonds.Nucleation takes place at the beginning of the synthesis when the carbon oversaturation is important,and the carbon in solution is then absorbed by the existing nuclei,which grow larger.A n n u . R e v . M a t e r . R e s . 2001.31:1-23. D o w n l o a d e d f r o m a r j o u r n a l s .a n n u a l r e v i e w s .o r g b y C h i n e s e A c a d e m y o f S c i e n c e s - L i b r a r y o n 05/16/09. F o r p e r s o n a l u s e o n l y .SUPERHARD MATERIALS5Figure 1Size distribution of diamonds in one laboratory run for different synthesis pro-cesses;effects of (panel a )the nature of the metal,(panel b )the stacking of graphite and metal disks,(panel c )the P-T pathway.(Panel d )P-T pathways for synthesis.1:graphite-diamond boundary and 2:melting temperature of the carbon-eutectic.The diamond synthesis occurs between the boundaries 1and 2.The growth time is about the same for all the crystals,thus those that can grow more quickly owing to a greater local thermal gradient become the largest.Owing to their rapid growth rate,they trap more impurities and have more defects,and therefore their friability is higher.Similarly,friability increases with the diamond yield.The diamonds produced by the spontaneous nucleation method range in size up to 800–1000µm.The best conditions for diamond synthesis correspond to a compromise between the quantity and the quality of the diamonds.A n n u . R e v . M a t e r . R e s . 2001.31:1-23. D o w n l o a d e d f r o m a r j o u r n a l s .a n n u a l r e v i e w s .o r g b y C h i n e s e A c a d e m y o f S c i e n c e s - L i b r a r y o n 05/16/09. F o r p e r s o n a l u s e o n l y .6HAINESL ´EGERBOCQUILLONCubic Boron NitrideCubic boron nitride (cBN)is the second hardest material.The synthesis of cBN isperformed in the same pressure range as that for diamond,but at higher tempera-tures,i.e.above 1950K.The general process is the same;dissolution of hexagonal boron nitride (hBN)in a solvent-catalyst (SC),followed by spontaneous nucle-ation of cBN.However,the synthesis is much more complicated.The usual SCs are alkali or alkaline-earth metals and their nitrides (9):Mg,Ca,Li 3N,Mg 3N 2,and Ca 3N 2.All these SCs are hygroscopic,and water or oxygen are poisons for the synthesis.Thus great care must be taken,which requires dehydration of the materials and preparation in glove boxes,to avoid the presence of water in the high-pressure cell.Furthermore,the above compounds react first with hBN to form inter-mediate compounds,Li 3BN 2,Mg 3B 2N 4,or Ca 3B 2N 4,which become the true SC.These compounds and the hBN source are electrical insulators,thus an internal furnace must be used,which makes fabrication of the high pressure cell more complicated and reduces the available volume for the samples.In addition,the chemical reaction involved is complicated by this intermediate step,and in gen-eral the yield of cBN is lower than for diamond.Work is in progress to determine in situ which intermediate compounds are involved in the synthesis process.The crystals of cBN obtained from these processes are of lower quality (Figure 2)and size than for diamond.Depending on the exact conditions,orange-yellow or dark crystals are obtained;the color difference comes from a defect or an excess of boron (less than 1%);the dark crystals,which have an excess of born,are harder.As in the synthesis of diamond,the initial forms of the SC source,hBN,play important roles,but the number of parameters is larger.For the source of BN,it is better to use pressed pellets of hBN powder rather than sintered hBN products,as the latter contain additives (oxides);a very fine powder yields a better reactivity.Doping of Li,Ca,or Mg nitrides with Al,B,Ti,or Si induces a change in the morphology and color of cBN crystals,which are dark instead of orange,are larger (500µm),have better shapes and,in addition,gives a higher yield (10).Use of supercritical fluids enables cBN to be synthesized at lower pressures and temperatures (2GPa,800K),but the resulting crystal size is small (11).Diamond and cBN crystals are produced on a large scale,and the main problem is how to use them for making viable tools for industry.Different compacts of these materials are made (12)for various pacts of diamonds are made using cobalt as the SC.The mixture is treated under high-pressure high-temperature conditions,at which superficial graphitization of the diamonds takes place,and then under the P-T-t diamond synthesis conditions so as to transform the graphite into diamond and induce intergranular growth of diamonds.The diamond compacts produced in this way still contain some cobalt as a binder,but their hardness is close to that of single-crystal pacts of cBN cannot be made in the same way because the SCs are compounds that decompose in air.Sintering without binders (13)is possible at higher pressures of about 7.5–8GPa and temperatures higher than 2200K,but these conditions are currently outside the range of thoseA n n u . R e v . M a t e r . R e s . 2001.31:1-23. D o w n l o a d e d f r o m a r j o u r n a l s .a n n u a l r e v i e w s .o r g b y C h i n e s e A c a d e m y o f S c i e n c e s - L i b r a r y o n 05/16/09. F o r p e r s o n a l u s e o n l y.SUPERHARD MATERIALS7Figure 2SEM photographs of diamond (top )and cBN (bottom )crystals of different qualities depending on the synthesis conditions (the long vertical bar corresponds to a distance of 100µm).Top left :good quality mid-sized diamonds of cubo-octahedral shape with well-defined faces and sharp edges;top right :lower quality diamonds;bottom left :orange cBN crystals;bottom right :very large black cBN crystals of better shapes.A n n u . R e v . M a t e r . R e s . 2001.31:1-23. D o w n l o a d e d f r o m a r j o u r n a l s .a n n u a l r e v i e w s .o r g b y C h i n e s e A c a d e m y o f S c i e n c e s - L i b r a r y o n 05/16/09. F o r p e r s o n a l u s e o n l y .8HAINESL ´EGERBOCQUILLONused in industrial pacts of cBN with TiC or TaN binders are ofmarkedly lower hardness because there is no direct bonding between the superhard crystals,in contrast to diamond compacts.In addition,they are expensive,and this has motivated the search for other superhard materials.SEARCH FOR NEW SUPERHARD MATERIALSOne approach for increasing hardness of known materials is to manipulate the nanostructure.For instance,the effect of particle size on the hardness of materials has been investigated.It is well known that high-purity metals have very low shear strengths;this arises from the low energy required for nucleation and motion of dislocations in metals.The introduction of barriers by the addition of impurities or grain size effects may thus enhance the hardness of the starting phase.In this case,intragranular and intergranular mechanisms are activated and compete with each other.As each mechanism has a different dependency on grain size,there can be a maximum in hardness as the function of the grain size.This effect of increasing the hardness with respect to the single-crystal value does not exist in the case of ceramic materials.In alumina,which has been thoroughly studied,the hardness (14)of fine-grained compacts is at most the hardness of the single crystal.When considering superhard materials,any hardness enhancement would have to come from the intergranular material,which would be by definition of lower hard-ness.In the case of thin films,it has been reported that it is possible to increase the hardness by repeating a layered structure of two materials with nanometer scale dimensions,which are deposited onto a surface (15).This effect arises from the repulsive barrier to the movement of dislocations across the interface between the two materials and is only valid in one direction for nanometer scale defor-mations.This could be suitable for coatings,but having bulk superhard materials would further enhance the unidirectional hardness of such coatings.In addition,hardness in these cases is determined from tests at a nanometer scale with very small loads,and results vary critically (up to a factor of three)with the nature of the substrate and the theoretical models necessary to estimate quantitatively the substrate’s influence (16).We now discuss the search for bulk superhard materials.Physics of HardnessThere is a direct relation between bulk modulus and hardness for nonmetallic ma-terials (Figure 3)(17–24),and here we discuss the fundamental physical properties upon which hardness depends.Hardness is deduced from the size of the inden-tation after an indenter has deformed a material.This process infers that many phenomena are involved.Hardness is related to the elastic and plastic properties of a material.The size of the permanent deformation produced depends on the resistance to the volume compression produced by the pressure created by the indenter,the resistance to shear deformation,and the resistance to the creation and motion of dislocations.These various types of resistance to deformation indicateA n n u . R e v . M a t e r . R e s . 2001.31:1-23. D o w n l o a d e d f r o m a r j o u r n a l s .a n n u a l r e v i e w s .o r g b y C h i n e s e A c a d e m y o f S c i e n c e s - L i b r a r y o n 05/16/09. F o r p e r s o n a l u s e o n l y .SUPERHARD MATERIALS 9Figure 3Hardness as a function of the bulk modulus for selected materials (r-,rutile-type;c,cubic;m,monoclinic).WC and RuO 2do not fill all the requirements to be superhard (see text).which properties a material must have to exhibit the smallest indentation possible and consequently the highest hardness.There are three conditions that must be met in order for a material to be hard:The material must support the volume decrease created by the applied pressure,therefore it must have a high bulk modulus;the material must not deform in a direction different from the applied load,it must have a high shear modulus;the material must not deform plastically,the creation and motion of the dislocations must be as small as possible.These conditions give indications of which materials may be superhard.We first consider the two elastic properties,bulk modulus (B)and shear modulus (G),which are related by Poisson’s ratio (ν).We consider only isotropic materials;a superhard material should preferably be isotropic,otherwise it would deform preferentially in a given direction (the crystal structure of diamond is isotropic,but the mechanical properties of a single crystal are not fully isotropic because cleavage may occur).In the case of isotropic materials,G =(3/2)B (1−2ν)/(1+ν);In order for G to be high,νmust be small,and the above expression reduces thenA n n u . R e v . M a t e r . R e s . 2001.31:1-23. D o w n l o a d e d f r o m a r j o u r n a l s .a n n u a l r e v i e w s .o r g b y C h i n e s e A c a d e m y o f S c i e n c e s - L i b r a r y o n 05/16/09. F o r p e r s o n a l u s e o n l y .10HAINESL ´EGERBOCQUILLONto G =(3/2)B (1−3ν).The value of νis small for covalent materials (typicallyν=0.1),and there is little difference between G and B:G =1.1B.A typical value of νfor ionic materials is 0.25and G =0.6B;for metallic materials νis typically 0.33and G =0.4B;in the extreme case where νis 0.5,G is zero.The bulk and shear moduli can be obtained from elastic constants:B =(c 11+2c 12)/3,G =(c 11−c 12+3c 44)/5.Assuming isotropy c 11−c 12=2c 44,it follows that G =c 44;Actually G is always close to c 44.In order to have high values of B and G,then c 11and c 44must be high with c 12low.This is the opposite of the central forces model in which c 12=c 44(Cauchy relation).The two conditions,that νbe small and that central forces be absent,indicate that bonding must be highly directional and that covalent bonding is the most suitable.This requirement for high bulk moduli and covalent or ionic bonding has been previously established (17–19,21–24)and theoretical calculations (19,25,26)over the last two decades have aimed at finding materials with high values of B (Figure 3).The bulk modulus was used primarily for the reason that it is cheaper to calculate considering the efficient use of computer time,and an effort was made to identify hypothetical materials with bulk moduli exceeding 250–300GPa.At the present time with the power of modern computers,elastic constants can be obtained theoretically and the shear modulus calculated (27).The requirement for having directional bonds arises from the relationship be-tween the shear modulus G and bond bending (28).Materials that exhibit lim-ited bond bending are those with directional bonds in a high symmetry,three-dimensional lattice,with fixed atomic positions.Covalent materials are much better candidates for high hardness than ionic compounds because electrostatic interac-tions are omnidirectional and yield low bond-bending force constants,which result in low shear moduli.The ratio of bond-bending to bond-stretching force constants decreases linearly from about 0.3for a covalent material to essentially zero for a purely ionic compound (29,30).The result of this is that the bulk modulus has very little dependence on ionicity,whereas the shear modulus will exhibit a relative de-crease by a factor of more than three owing entirely to the change in bond character.Thus for a given value of the bulk modulus,an ionic compound will have a lower shear modulus than a covalent material and consequently a lower hardness.There is an added enhancement in the case of first row atoms because s-p hybridization is much more complete than for heavier atoms.The electronic structure also plays an important role in the strength of the bonds.In transition metal carbonitrides,for example,which have the rock-salt structure,the hardness and c 44go through a maximum for a valence electron concentration of about 8.4per unit cell (31).The exact nature of the crystal and electronic structures is thus important for determin-ing the shear modulus,whereas the bulk modulus depends mainly on the molar volume and is less directly related to fine details of the structure.This difference is due to the fact that the bulk modulus is related to the stretching of bonds,which are governed by central forces.Materials with high bulk moduli will thus be based on densely packed three-dimensional networks,and examples can be found among covalent,ionic,and metallic materials.In ionic compounds,the overall structure isA n n u . R e v . M a t e r . R e s . 2001.31:1-23. D o w n l o a d e d f r o m a r j o u r n a l s .a n n u a l r e v i e w s .o r g b y C h i n e s e A c a d e m y o f S c i e n c e s - L i b r a r y o n 05/16/09. F o r p e r s o n a l u s e o n l y .principally defined by the anion sublattice,with the cations occupying interstitial sites,and compounds with high bulk moduli will thus have dense anion packing with short anion-anion distances.The shear modulus,which is related to bond bending,depends on the nature of the bond and decreases dramatically as a func-tion of ionicity.In order for the compound to have a high shear modulus and high hardness (Figure 4),directional (covalent)bonding and a rigid structural topology are necessary in addition to a high bulk modulus.A superhard material will have a high bulk modulus and a three-dimensional isotropic structure with fixed atomic positions and covalent or partially covalent ionic bonds.Hardness also depends strongly on plastic deformation,which is related to the creation and motion of dislocations.This is not controlled by the shear modulus but by the shear strength τ,which varies as much as a factor of 10for different materials with similar shear moduli.It has been theoretically shown that τ/G is of the order of 0.03–0.04for a face-centered cubic metal,0.02for a layer structure such as graphite,0.15for an ionic compound such as sodium chloride,and 0.25for a purely covalent material such as diamond (32).Detailed calculationsmustFigure 4Hardness as a function of the shear modulus for selected materials (r-,rutile-type;c,cubic).A n n u . R e v . M a t e r . R e s . 2001.31:1-23. D o w n l o a d e d f r o m a r j o u r n a l s .a n n u a l r e v i e w s .o r g b y C h i n e s e A c a d e m y o f S c i e n c e s - L i b r a r y o n 05/16/09. F o r p e r s o n a l u s e o n l y .。
含有萘酰亚胺的菁染料太阳能电池敏化剂的合成
含有萘酰亚胺的菁染料太阳能电池敏化剂的合成詹文海 花建丽 金樱华 武文俊 田禾*(华东理工大学精细化工研究所结构可控先进功能材料及其制备教育部重点实验室 上海 200237)摘 要 通过Click反应把萘酰亚胺化合物连接到含有醛基的吲哚上,再通过醛基和吲哚碘盐的Knoevenagel缩合反应合成出带有萘酰亚胺部分的菁染料,用NMR、MS、元素分析、UV_Vis等方法对其结构和性能进行了表征和测试。
关键词 菁染料 萘酰亚胺 太阳能电池敏化染料 合成Synthesis of Novel Naphthalimide_containing Cyanine Dye Utilized as Solar Cell SensitizerZhan Wenhai,Hua Jianli,Jin Yinghua,Wu Wenjun,Tian He*(Laboratory for Advanced Materials and Institute of Fine Chemicals,East China University of Science&T echnology,Shanghai200237)Abstract Two novel cyanine dyes containing naphthali mide have been syn thesized by Knoevenagel condensation reaction between i ndole iodide and naphthali mide_indoles generated from naphthalimides and indole via Click reaction andcharacterized by NMR,MS,elemental analysis,UV_Vis absorption spectra etc.Key words Naphthalimide,Cyanine dye,Solar cell sensitizer,Synthesis目前,染料敏化太阳能电池的光电转换效率已经超过了10%,达到了实用的要求。
功能有机材料
2.2 Photochemical Syntheses
Vollhardt’s group adopted the cobalt-catalyzed photochemical cyclotrimerization of alkynes for the rapid construction of a novel class of helicenes
The challenge in this area is to obtain materials with inherently strong chiral properties at the macromolecular level, rather than derived from an aggregate or a supramolecular structure. Such inherently strong chiral properties, approaching or exceeding in magnitude their achiral counterparts, would facilitate exploration of chiral properties of single molecule devices and the design of novel chiral materials.
3. Conclusion
Introduction
Chirality is increasingly important in the design of organic π-conjugated materials. One of the aspects of the design involves optimization of achiral properties through the introduction of chirality. In this context, the inherent threedimensional character of chirality and the control of intermolecular interactions associated with diastereomeric recognition provide a versatile handle for the optimization of supramolecular structures, film morphology and liquid crystalline order of p-conjugated polymers and oligomers in three dimensions .
手性超材料研究进展
手性超材料研究进展钟柯松2111409023 物理1. 引言超材料是有特殊电磁性质的人造结构性材料,其中一个典型的性质就是负折射率。
第一种负折射率材料1两个部分组成:一个是连续的金属线,它来实现负介电常数2,另一个是开环谐振器,来实现负的磁导率3。
在同时实现复介电常数和负磁导率的时候,负折射率就是实现了。
后来,人们大多数以这个原则4-5来设计负折射率材料。
虽然负磁导率在微波段很容易实现,但是在光频区域却极其困难7,8。
与此同时,Pendry9,Tretyakov10,11和Monzon12等人从理论上提出了另一种利用手性实现负折射率的途径。
而手性材料层作为完美透镜也从理论上实现了9-13。
在这些报告中,Pendry提出了一种3D螺旋线结构来实现负折射率的手性超材料9。
Tretyakov 等人则在理论上研究了在手性和偶极粒子手性复合材料中得到负折射率的可能性11。
理论表明,负折射率是可以在以3D螺旋对称为晶格的金属球超材料中可以得到14。
同时也表明,周期上的手性散射是3D和各向同性负折射率的原因15。
实际上,Bose曾经在1898年利用螺旋结构研究了平面偏振电磁波的旋转16。
Lindman也是研究微波段人造手性介质的先驱17。
最近,Zhang 等人在实验上实现了一个3D手性超材料在THz波段的负折射率18。
Wang等人则在微波段同时实现了3D手性超材料的负折射率和巨大的光学活性和圆二色性19,20。
但是,这些提到的3D手性超材料都很难构建。
同时,平面手型超材料显示了光学活性也被报道了21-24。
这里需要指出的是,平面手性结构是正真的3D手性结构是不同的。
Arnaut和Davis第一次把平面手性结构引入到了电磁波的研究中25,26。
一个结构如果被定义为手性结构,那么它应该是在任何平面是没有镜面对称的,然而,一个平面结构被认为是手性的,则它是不能和它在该平面上的镜像重叠的,除非它不在这个平面上。
实际上,一个平面手性结构还是和镜像镜面对称的。
超硬碳化物的第一性原理设计
Ultrastiff carbides uncovered in first principlesChen Zhouwen 1,Gu Mingxia 1,Sun Changqing 1,Zhang Xinyu 2,Liu Riping 2 1. School of Electrical and Electronic Engineering,Nanyang Technological University,Singapore(639798)2. Key Laboratory of Metastable Materials Science & Technology,Yanshan University,Qinhuangdao (066004)E-mail:ecqsun@.sg,riping@AbstractWe have computationally designed ultraincompressible materials namely rhenium carbide in the WC and NiAs structure with a very high shear modulus. The corresponding calculated bulk modulus is comparable with that of diamond. Especially for the WC typed rhenium carbide (ReC), the incompressibility along the c-axis is demonstrated to exceed the linear incompressibility of diamond. The unique mechanical properties would make it suitable for applications under extreme conditions.Keywords:superhard materials,first prnciple caculations1. IntroductionSearching for hard materials are all along the aspiration of science and engineering studies. Nowadays, this exploration mainly focus on the following aspects: compounds composed of light elements as boron, carbon, nitrogen and oxygen (B-C-N-O systems) such as cubic BN, B4C, B6O,C3N4, cubic BC2N1. The intrinsically strong and directional covalent bonds of the light elements would lead to tight, three-dimensional networks with extreme resistance to external shear; Noble metal diborides OsB22,3 and ReB21; Noble metal dinitrides such as PtN24,5, OsN2 and IrN25,6; Transition metal oxides cotunnite TiO27; Noble monocarbide like OsC8 and PtC9. However, no prominent mechanical properties have yet been found in these noble metal monocarbides even that the exact structures are still not well resolved10,11. Transition metal carbides are known for their very high melting temperature, extreme hardness that can be used in cutting tools, dental drills, rock drills in mining, and abrasives like HfC, WC and TaC. For designing superhard monocarbide materials, we combine three influential factors: high valence electron density, low bond ionicity and small bond volume that have been demonstrated to be effective both in experimental l,12 and theoretical13 approaches. Among the transition metals, osmium has the highest valence electron density3 (0.572 electrons/Å3). Experiment has provided evidence for a synthesis of osmium carbide at zero pressure by Kempter and Nadler forty six years ago7, and it was assumed to be in the WC structure. However, OsC in the postulated WC structure was theoretically demonstrated to be electronically and mechanically unstable10 subsequently although another density functional calculation suggests that OsC of WC structure type possess a high bulk modulus14. The conclusive determination of exact crystal structures of OsC may be difficult due to miscellaneous phases in the Os-C system similar to the case of binary borides of ruthenium, osmium and iridium intermediate phases15. Similar to Os, Re has a high valence electron density (0.476 electrons/Å3), being second to Os. The bond volume for the corresponding carbide may be expected to be reduced due to the lanthanide contraction (the ionic radii of the elements decrease with increasing atomic number). In addition, strong covalent bonds could also be achieved due to hybridizing between metal d and nonmetal 2p electrons12. Previous studies have proposed other two possible structures for the synthesized noble metal carbide compound PtC, with Ref.16 suggesting a zincblende structure to be mechanically stable, while Fan et. al10 proposed PtC to have a rock-salt structure, which was also suggested as an alternative in the originalexperimental paper, since the corresponding bulk modulus is more comparable to the experimental data 8. In addition, a closely related structure to WC is the NiAs type which is also considered in this work. Therefore four candidate structures are chosen for ReC in namely rock-salt, zincblende, WC and NiAs types.2. Theoretical approachesTo identify the equilibrium structure, we performed first-principles calculations based on a plane wave basis set, by expanding the electron wavefunctions up to a kinetic energy cut-off of 500 eV with periodic boundary conditions. The ultrasoft pseudopotential 17 wad used for the electron-ion interaction, and the generalized gradient approximation (GGA) of Perdew et al.18 for the electron-electron exchange and correlation. Such a scheme has been demonstrated to be very good in providing accurate and reliable predictions of structural and mechanical properties of transition metal compounds system 19. Integrations in the Brillouin zone are performed using special k points generated with 10×10×10, 10×10×4, 9×9×9 and 9×9×9 mesh parameters grid for WC, NiAs, zincblende and rocksalt typed structures of ReC. The cell parameters a and c in the hexagonal structures are varied until the minimal enthalpy H = E +PV is achieved under the restriction of the given symmetry. During the subsequent geometrical optimization, all forces on atoms are converged to less than 0.001eV/Å, and the total stress tensor is reduced to the order of 0.01 GPa. Among the considered polymorphs, ReC in the WC type is energetically the most stable polymorph with the NiAs structure type close in enthalpy as a metastable phase. The relative stability order is WC type>NiAs type>zincblende>rocksalt for ReC, resulted from the computed enthalpy differences -0.71, -0.62 and -0.2 eV/atom respectively with respect to the rocksalt ReC. In the following parts, we refer to the WC and NiAs phases within the hexagonal symmetry. Structures shown in Fig. 1 are optimized geometries, which show no imaginary phonon modes, indicating their thermodynamic stability. The optimizedstructures expand the original Re lattice laterally only by 3.7% and 3.8% upon incorporation of carbon for WC- and NiAs-type, which is less than that of ReB 2 with 5%1, resulting in the shorter and therefore stronger metal-metal bonds.3. Results and discussionThe five independent elastic stiffness constants ij C are evaluated by computing the stress tensor i σ generated by forcing strain j ε to the optimized unit cell with four different magnitudes, =ε-0.003, -0.001, 0.001 and 0.003. Table 1 lists the structural parameters and elastic properties data for WC- and NiAs-ReC. We note that our calculation of the data for WC in GGA approximation is in good agreement with the experimental results except for the bulk modulus. However, the general trend should bemaintained and reflected in the calculated results. The obtained elastic stiffness constants satisfy the Born stability criteria for a hexagonal crystal 20, suggesting an elastic stability of these two structure types of ReC. It is also confirmed that OsC in the WC type is mechanically unstable according to our calculations. This may not be surprising when considering the fact that for dinitrides and diborides of the noble metals in the same period(PtN 2, OsN 2 and IrN 2 with pyrite, marcasite and a lower symmetry structures 21,22,23; OsB 2 and ReB 2 were confirmed in an orthorhombic and hexagonal lattice respectively 1,2, but these structures can be correlated by distortion). The bulk and shear moduli are computed in terms of elastic constants obtained based on the Voigt scheme. The result predicted an extraordinary high bulk modulus of 440 GPa(diamond 443 GPa in this work) and an extreme incompressibility along the c -axis with 33C =1123 GPa (diamond 11C =1092 GPa) for WC-ReC, consistent with the very low c/a ratio of 0.977 compared to ideal value of1.633. WC-ReC also possesses a high shear modulus of 223 GPa. While for NiAs-ReC, the bulk modulus isalso very high(422 GPa, close to that of diamond), associated with a shear modulus 274 GPa slightly smaller than that of WC. As was demonstrated in Ref. 13 the dependence of hardness on bulk or shear modulus is notmonotonic, and thus a quantitative estimate is essential. We can obtain the predicted Vickers hardness using the semiempirical relation 13,24 3/5)/(b Vv P H ∝for binary covalent crystals by scaling calculated quantities and experimental 7 =V H 30 GPa for WC. P is the Mulliken bond overlap population that can be derived from first-principles computations. It is a measure of the spatial charge density between bonding atoms which combines the effects of bond ionicity and valence electrons density. b v is the average bond volume, which can be obtained by the ratio between the cell volume and the containing bond number. Defining the ratio WC C q q q R /)(Re =of any property q , our calculations give =)(P R 0.42/0.38=1.105, and =)(b v R 3.267/3.448=0.948, which finally produces a total enhancement factor of 1.21 and a hardness 36 GPa for WC-ReC. Application of the same method produces 38 GPa for NiAs-ReC, making it a potential superhard material considering the estimated error. Obviously, the higher hardness originatesfrom higher valence electron density increasing the covalent nature and the smaller bond volume compared to WC. It is essential to get valuable insight into the bonding character of the different phases from theelectronic structure. The density of states (DOS) shown in Fig. 2 elucidate that WC- and NiAs-ReC have close similarity to a certain extent. They can be characterized for both being metallic and exhibiting a finite density of states N (E F ) at the Fermi level. A higher N (E F ) value for NiAs-ReC than for WC-ReC indicates its less stability of the former, consistent with the energy calculation results. For both phases, the DOS around the Fermi level come predominantly from d orbits of Re. There is a deep valley called pseudogap near the Fermi level (E F ), which results from the strong hybridization and leads to a separation between the bonding states(occupied) and anti-bonding (unoccupied) states. The presence of a pseudogap indicates a strong covalent bonding in WC- and NiAs-ReC, resulting in a high bulk modulus.5. ConclusionThis compound should be accessible in synthesis from the arc-melting method without using extreme pressure for producing this hard material, similar to the process for the ReB 2 preparation 1. These two types of ReC phases maybe the hardest binary metal carbide so far discovered, which are harder than the known carbides such as WC and TaC. The low incompressibility comparable to diamond and even higher uniaxial Young’s modulus may allow to replace diamond in some applications like cutting processes.6. AcknowledgementThis work was financially supported by NSFC (Grant No. 50325103) and SKPBRC (Grant No.2005CB724400).Reference1 H.-Y. Chung, M. B. Weinberger, J. B. Levine, A. Kavner, J. M. Yang, S. H. Tolbert, and R. B. Kaner, Science 316, 436 (2007).2 R. B. Kaner, J. J. Gilman, and S. H. Tolbert, Science 308, 1268 (2005).3 R. W. Cumberland, M. B. Weinberger, J. J. Gilman, S. M. Clark, S. H. Tolbert, and R. B. Kaner, J. Am. Chem. Soc. 127, 7264 (2005).4 E. Gregoryanz, C. Sanloup, M. Somayazulu, J. Badro, G. Fiquet, H.-K. Mao, and R. J. Hemley, Nat. Mater. 3, 294 (2004).5 J. C. Crowhurst, A. F. Goncharov, B. Sadigh, C. L. Evans, P. G. Morrall, J. L. Ferreira, and A. J. Nelson, Science 311, 1275 (2006).6 A. F. Young, C. Sanloup, E. Gregoryanz, S. Scandolo, R. J. Hemley, and H.-K Mao,Phys. Rev. Lett. 96, 155501 (2006).7 L. S. Dubrovinsky, N. A. Dubrovinskaia, V. Swamy, J. Muscat, N. M. Harrison, R. Ahuja, B. Holm, and B. Johansson, Nature 410, 653 (2001).8 C.P. Kempter, J. Chem. Phys.41, 1515 (1964).9 S. Ono, T. Kikegawa, and Y. Ohishi, Solid State Commun. 133, 55 (2005).10 M. Zemzemi, M. Hebbache, D. Zivkovic, and L. Stuparevic, See:/s_mrs/sec_subscribe.asp?CID=7587&DID=191586&action=detail.11 C. Z. Fan, S. Y. Zeng, Z. J. Zan, R. P. Liu, W. Q. Wang, P. Zhang, and Y. G. Yao, Appl. Phys. Lett. 89, 071913 (2006).12 S. H. Jhi, J. Ihm, S. G. Louie, and M. L. Cohen, Nature 399, 132 (1999).13 F. M. Gao, J. L. He, E. D. Wu, S. M. Liu, D. L. Yu, D. C. Li, S. Y. Zhang, and Y. J. Tian, Phys. Rev. Lett. 91, 015502 (2003).14 J.-C. Zheng, Phys. Rev. B 72, 052105 (2005).15 B. Aronsson, E. Stenberg, and J. Åselius, Nature 195, 377 (1962).16 L. Y. Li, W. Yu, and C. Q. Jin, J. Phys.: Condens. Matter 17, 5965 (2005).17 D. Vanderbilt, Phys. Rev.B 41, 7892-7895 (1990).18 J. P. Perdew, K. Burke, and M. Ernzerhof, Phys. Rev. Lett.77, 3865-3868 (1996).19 H. Y. Gou, L. Hou, J. W. Zhang, H. Li, G. F. Sun and F. M. Gao, Appl. Phys. Lett. 88, 221904 (2006).20 X. F. Hao, Y. H. Xu, Z. J. Wu, D. F. Zhou, X. J. Liu, X. Q. Cao, and J. Meng, Phys. Rev. B 74, 224112 (2006).21 R. Yu, Q. Zhan, and L. C. De Jonghe, Angew Chem Int Ed Engl. 46, 1136 (2007).22 Z. W. Chen, X. J. Guo, Z. Y. Liu, M. Z. Ma, Q. Jing, G. Li, X. Y. Zhang, L. X. Li, Q. Wang, Y. J. Tian, and R. P. Liu, Phys. Rev. B75, 054103 (2007).23 J. A. Montoya, A. D. Hernandez, C. Sanloup, E. Gregoryanz, and S. Scandolo, Appl. Phys. Lett.90, 011909 (2007).24 F. M.Gao, Phys. Rev. B73, 132104 (2006).25 See: /7108831.htmlTable I. Structure associated parameters of ReC in the WC- and NiAs-type at zero pressure, compared to the theoretical and experimental results for WC, where z refers to the number of formula units in a conventional cell. Also shown are elastic properties including elastic constants, bulk modulus and shear modulus.WC ReCCal.WC-type NiAs-type Exp.ThisCrystal system HexagonalSpace group P-6m2 (no.187) P63mmc(no.194)Cell parametersa (Ǻ) 2.87a 2.906 2.850 2.853c (Ǻ) 2.85a 2.828 2.786 5.593z 1 2V (Ǻ3) 20.33 20.69 19.60 39.42Elastic stiff constants (GPa)726796C11 721993C33 9631123195284C44 302229242C12 219192225C13 160Bulk and shear modulus(GPa)B 421b 386 440 422G 282c 285 223 274a from ref. 25.b from ref. 7.c from ref. 24.Figure CaptionsFigure 1. Ultra-incompressible and hard material created by combining high valence density metal rhenium and small radius atom carbon with covalent bonding in WC-type (a) and NiAs-type (b) structures. WC-type ReC unit cell is doubled along c axis for clear comparison. Rhenium and carbon are represented by blue and red spheres.zero energy and marked by the vertical lines.。
纳米孪晶金刚石--比天然金刚石硬度高1倍
synthesized from C60, amorphous carbon and glassy carbon, but Knoop hardness decreases significantly to 70286 GPa (ref. 6). The observed hardness deficiency seems to originate from intergranular fracturing along poorly sintered grain boundaries, rather than the reverse Hall2 Petch effect resulting from grain-boundary sliding6. Technically, the synthesis of well-sintered nanograined diamond while maintaining a smaller grain size remains a challenge.
超硬材料
Superhard Materials
In thinking about new ultrahard materials, it is useful to consider the types of structural changes that a material can undergo under load. These changes can be divided into elastic (reversible) and plastic (irreversible) deformations. A material is considered stiff if it is difficult to compress elastically. Such a material has a large bulk modulus (it is resistant to volume compression) and/or Young’s modulus (it is resistant to linear compression). Elastic deformation in a direction different from that of the applied load results in shape rather than volume changes; these motions are measured by the shear modulus. In all elastic distortions, the basic relations between atoms do not chthese ideas in mind, efforts to design superhard materials can be divided into two main approaches. In the first, light elements, including boron, carbon, nitrogen, and/or oxygen, are combined to form short covalent bonds. In the second, elements with very high densities of valence electrons are included to ensure that the materials resist being squeezed together.
含荧光基团透明质酸衍生物的合成及其荧光性能
变 化 其 荧 光 强 度 变 化 趋 势 不 明显 ,较 为 稳 定 ,随 温 度 的 变 化 其 荧 光 强 度 基 本 保 持 稳 定 。为 以 后探 索 具 有 药 物 载 体 透 明 质 酸 在 机
体 内 的作 用 机 理 及 其 靶 向作 用 提 供 良好 的实 验 基 础 。 关键 词 :透 明质 酸 ;7 - 羟基一 4 一 甲基 香 豆 素 ;荧 光 性 能 中 图分 类 号 :TQ 2 0 1 文 献 标 识 码 :A d o i :1 0 . 3 9 6 9 / j . i s s n . 2 0 9 5 —0 4 1 1 . 2 0 1 3 . 0 4 . 0 1 2
Vo1 . 25 No. 4 0c t . 2 O1 3
文章 编 号 :2 0 9 5 —0 4 1 I( 2 0 1 3 )0 4— 0 0 5 7— 0 4
含 荧 光 基 团透 明质 酸 衍 生物 的合 成 及 其荧 光 性 能
周 维杰 ,席 海 涛 孙 小 强
,
( 常州大学 石油化工学 院 , 江苏 常州 2 1 3 1 6 4 )
t a l b a s e s f o r t h e me c h a n i s m o f a c t i o n o f h y a l u r o n i c a c i d a s a d r u g c a r r i e r i n h u ma n b o d y a s we l l a s i t s t a r —
第2 5卷 第 4期
2 0 1 3年 1 0月
常 州 大学 学报 ( 自然科 学版 )
J o u r n a l o f C h a n g z h o u Un i v e r s i t y( Na t u r a l S c i e n c e Ed i t i o n )
superhard material(超硬材料)
Ⅰb diamond
In 1966, Dupont synthetized diamond by explosion method . In1970, Wentorf synthetized large particles of diamond by artificial growth successfully which size is 6mm, weight 1carat. In 1972, Artificial polycrystalline diamond synthetized. In 1980s, the thin film of synthetic diamond researched successfully.
In 1954, the diamond Synthetized firstly. In 1962, Decarli and Jamieson first synthetized diamond by explosion method under 30 Gpa shock pressure . In 1962, Bundy measured the triple point of diamond, graphite, liquid phase is 4100 k, 12.5 GPa in the condition of 1962 ~ 4000 k and the static pressure of over 12 GPa that different catalyst of graphite change to diamond directly.
Fe70Ni30粉末触媒中Ⅱa型金刚石大单晶的高温高压合成
第47卷第5期人工晶体学报Vol.47 No.5 2018 年5 月_________________________JOURNAL OF SYNTHETIC CRYSTALS________________________May,2018Fe7()Ni3()粉末触媒中Ila型金刚石大单晶的局温局压合成李勇1,賡江河2,陈宁3,佘彦超1,宋谋胜1,宋坤1(1.铜仁学院物理与电子工程系,铜仁554300 ;2.湖南科技大学物理与电子科学学院,湘潭411201;3.吉林大学超硬材料国家重点实验室,长春130012)摘要:在6.5GPa高压条件下,使用FeT O Ni%粉末触媒研究了I la型金刚石大单晶的合成。
实验结果表明,若不对晶 种表面进行保护,高温高压条件下金刚石晶种将发生碳化,致使难以合成出金刚石。
当合成腔体中除氮剂Ti/Cu添加量达到2. 2wt%时,所合成的金刚石大单晶呈现为无色透明,利用傅里叶显微红外光谱仪(FTIR)对所合成的金 刚石大单晶进行了测试,所合成的晶体中不含有氮杂质。
然而,FTIR测试结果表明所合成的I la型金刚石大单晶中有碳-氢基团的存在,其对应的FTIR特征吸收峰分别位于2850 cnT1和2920 cnT1处。
此外,所合成的I la型金刚 石大单晶的Raman特征峰位于1132. 13 cm_1处,且其结晶度非常高。
关键词:高温高压;Ila型金刚石;Fe7Q Ni3Q粉末触媒中图分类号:0781 文献标识码:A 文章编号:1000-985X( 2018) 05-1055-05 Synthesis of Ila Type Diamond Single Crystal in Fe70Ni30 Powder Catalyst under High Temperature and High Pressure LI Yong1,LIAO Jiang-he2,CHEN Ning3,SHE Yan-chao1,SONG Mou-sheng1,SONG Kun1(1. Department of Physics and E lectrical Engineering, Tongren U niversity, Tongren 554300, C hin a;2. School of Physics and E lectronics, Hunan U niversity of Science and Technology, Xiangtan 411201, C hin a;3. State Key Laboratory of Superhard M aterials, J ilin U niversity, Changchun 130012, C hina)Abstract:The synthesis of Ila type diamond single crystal was investigated at pressure of 6. 5 GPa by temperature gradient growth method, employing Fe70Ni30powders as catalyst. The experimental results show that the growth of diamond crystal can not run if the diamond seed is not protected during the synthesis process under high pressure and high temperature ( HPHT) , because of the carbonization of diamond seed crystal at HPHT conditions. The synthesized diamond exhibited colorless when the addition content of the nitrogen getter Ti/Cu achieve 2.2wt% in the synthesis system. It was characterized by FTIR and the result displayed that nitrogen was inexistence in the colorless diamond, indicating that it belongs to Ila type diamond. However, the C-H groups were noticed in the FTIR spectra and the corresponding absorption peaks located at 2850 cm -1 and 2920 cm-1, respectively. Furthermore, the Raman peak of the obtained Ila type diamond located at 1132. 13 cm-1 and the crystallization was perfect.Key w ords:high temperature and high pressure; Ila type diamond; Fe70Ni30 powders catalyst基金项目:国家自然科学基金(11604246);贵州省教育厅创新群体重大研究项目(KY字[2017 ] 053);贵州省科技厅基金项目([2018 ] 1163);吉林大学超硬材料国家重点实验室开放课题(201610);全国大学生创新创业项目(2016106677)作者简介:李勇(1981-),男,山东省人,博士,教授。
超硬材料工艺流程
超硬材料工艺流程In the production of superhard materials, the technological process is crucial for achieving the desired properties of the materials. 超硬材料的生产中,工艺流程对于实现材料所需的性能至关重要。
The first step in the process is the selection of raw materials. Raw materials for superhard materials may include diamonds, cubic boron nitride, and other materials with exceptional hardness. 工艺流程中的第一步是选择原材料。
超硬材料的原材料可能包括钻石、立方氮化硼和其他硬度异常高的材料。
Once the raw materials are selected, they undergo a thorough inspection and testing process to ensure their quality and suitability for the production of superhard materials. 一旦选择了原材料,它们就要经过彻底的检验和测试过程,以确保它们的质量和适用性,以用于超硬材料的生产。
The next step involves the shaping of the raw materials into the desired form. This may involve processes such as cutting, grinding, and polishing to achieve the precise dimensions and surface finishrequired for superhard materials. 接下来的步骤涉及将原材料成型为所需的形式。
h-BN掺杂对金刚石晶体结构的影响
h-BN掺杂对金刚石晶体结构的影响李沛航;崔梦男;万玉春【摘要】报道了在Fe70Ni30合金触媒和石墨系体中,掺杂六角立方氮化硼(h-BN)和硼(B)生长金刚石单晶的过程.研究发现,h-BN和B掺杂对于金刚石生长条件及形貌等具有较大的影响,其中h-BN掺杂生长金刚石的最低生长压力达到了6.2 GPa,同时晶体呈绿色条状.说明h-BN和B在金刚石晶体生长以及取代碳原子进入晶格时起到了不同的作用.通过X射线衍射及光电子能谱等表征手段,分析了硼氮对金刚石晶体结构的影响,以及硼氮在金刚石中的化学环境及成键方式.在此基础上阐述了硼氮掺杂的形成机制.%In this work, we report the growth process of single crystal diamond by doping boron (B) and hexagonal boron nitride (h-BN) in the system of Fe70Ni30 alloy catalyst and graphite. The doping of B and h-BN has signifi-cant effect on the growth condition and morphology of diamonds. The lowest growth pressure of h-BN doped diamond is 6.2Gpa and the crystals have a green strip morphology. This results indicates that B and h-BN have different effects on the diamond growth and have different ways to replace carbon atoms. We analyze the effect of doping B and N at-oms on the structure of diamond,and the chemical environment of B and N atoms in diamond by using X-ray diffrac-tion and photoelectron spectroscopy. The mechanism of B and N doped diamond is also demonstrated.【期刊名称】《长春理工大学学报(自然科学版)》【年(卷),期】2015(038)005【总页数】4页(P72-75)【关键词】h-BN;金刚石;成键方式;高温高压【作者】李沛航;崔梦男;万玉春【作者单位】长春理工大学材料科学与工程学院,长春 130022;长春理工大学材料科学与工程学院,长春 130022;长春理工大学材料科学与工程学院,长春 130022【正文语种】中文【中图分类】TP391.41自20世纪50年代人们利用静高温高压方法合成出金刚石和立方氮化硼以来,金刚石和立方氮化硼作为超硬材料已得到了深入的研究和广泛的应用。
模具超硬刀具材料高硼化钨的结构研究
模具超硬刀具材料高硼化钨的结构研究*秦 平1,高振帮2,欧阳玲玉1,龙永莲1,王浦舟1(1.江西应用技术职业学院,江西赣州 341000;2.天地上海采掘装备科技有限公司,上海 201400)【摘要】为研究模具超硬刀具材料高硼化钨的结构,基于WB 3-hP16结构,以及调整钨、硼原子对Wyckoff 2b 和2c 位置的占据成分,建立可能存在的结构体系,运用第一性原理计算,得出高硼化钨的稳定结构应为WB 3.86,其中三角硼群的占据1/4的Wyckoff 2b 位置,并且计算分析其力学性质,其具有最高的硬度值(42.24GPa ),并且其硬度、体变模量、剪切模量和杨氏模量都与其实验更为接近。
另外还研究了其微观特性,其费米能位于其最低点,得出结论:高硼化钨的结构为WB 3.86结构,为实际合成高硼化钨提供理论依据以及合成配比,更有利于超硬刀具材料高硼化钨的有效合成。
关键词:高硼化钨,第一性原理,力学性质,微观特性中图分类号:TG162;TG659 文献标识码:B DOI :10.13596/ki.44-1542/th.2024.03.022Study on the Structure of Tungsten High-Boride as Die & Mold Superhard Tool MaterialQin Ping 1, Gao Zhenbang 2, Ouyang Lingyu 1, Long Yonglian 1, Wang Puzhou 1(1.Jiangxi College of Applied Technology ,Ganzhou ,Jiangxi 341000,CHN ;2.Tiandi Shanghai Equipment for Excavation Science and Technology Co., Ltd., Shanghai 201400,CHN )【Abstract 】 In order to study the structure of tungsten high-boride as a superhard tool material for die & mold, this article is based on the WB 3-hP16 structure and adjusts the composition of tungstenand boron atoms occupying Wyckoff 2b and 2c positions, establishing a possible structural system. Using first principles calculations, the stable structure of high boronized tungsten should be WB 3.86, with the triangular boron group occupying 1/4 of Wyckoff 2b positions. And through calculation and analysis of its mechanical properties, it has the highest hardness value (42.24 GPa), and its hardness, bulk modulus, shear modulus, and Young's modulus are closer to their experimental values. In addition, its microscopic characteristics were also studied, and its Fermi energy was located at its lowest point, which led us to conclude that the structure of high boron tungsten is WB 3.86. Provide theoretical basis and synthesis ratio for the actual synthesis of tungsten high-boride, which is more conducive to the effective synthesis of superhard tool material high boron tungsten.Key words : tungsten high- boride ; first principles ; mechanical properties ; microscopic properties* 项目支持:江西省教育厅科学技术研究项目支持(项目编号:Gjj2205005)1 引言随着模具精度的要求不断提高,对于材料的性能要求也越来越高[1]。
超硬材料具有高硬度
超硬材料具有高硬度、高强度、高熔点和耐腐蚀等优良的力学性能,因而在工程机械、切削加工、矿物开采、耐磨涂层和航天材料等各种工业中被广泛应用,甚至直接决定着刀刃具行业发展水平的高低。
周所周知,金刚石和立方氮化硼分别是世界上现有的第一、第二硬的材料[1],然而,在高温下金刚石易于同二价金属(如铁)发生化学反应,不能作为各类钢材切削工具,大大限制了它在切削刀具中的使用。
立方氮化硼虽具有很强热与化学的稳定性,非常适合于硬、韧和难于常规切削的金属材料的加工,但它的合成需要高温和高压的极端条件,使成本变得非常昂贵。
目前,使用最多的两种刀具材料是高速钢和硬质合金,分别约占刀具总量的30%~40%和50%~60%。
与金刚石相比,它们的硬度偏低,因而这些刀具寿命短,造成机械加工成本高。
而且,当前切削技术的快速发展,已经进入了现代切削技术新阶段,刀具材料成为制造业开发新产品和新工艺,应用新材料的基础工艺和建立创新体系的关键因素之一。
随着科学技术迅速发展,各种难于加工材料不断涌现,现有的超硬材料难以满足制造业的需要,迫切需要寻找新的稳定热性质和化学性质的超硬材料。
因此,理论上设计和实验中合成超硬材料成为国际研究的前沿热点[2]。
为了能设计和合成新的超硬材料,一方面可以利用硼、碳、氮和氧等小原子元素,仿照金刚石的结构,形成三维立体强共价键化合物,设计和合成超硬材料。
另一方面,最近Science、JACS报道[3-5],过渡金属元素的硼、碳、氮、氧等化合物可能提供了一条新的设计与合成超硬材料途径。
过渡金属元素都具有d电子,因而具有高的价电子浓度,致使它们具有极大的体变模量,极强的抵抗弹性变形能力,超低的不可压缩性能。
可是,从化学成键角度来说,这些价电子大都形成的是金属键,不能有效地阻止晶格位错地产生和运动,致使纯过渡金属往往呈现很低的硬度。
要使它们从超低压缩性材料变成超硬材料,需要把各个方向均匀的金属键变成有方向性的共价键,因此,把硼、碳、氮、氧等小的原子掺入到过渡金属的晶格中,使其引入共价键,再设计理想的晶格结构,就能增强了它们抵抗塑性变形的能力,大大提高它们的硬度,例如RuO2[6]、WC[7]、和Co6W6C[8]等都是这类硬性材料。
银纳米颗粒的合成与表面增强拉曼光谱
银纳米颗粒的合成与表面增强拉曼光谱
银纳米颗粒的合成与表面增强拉曼光谱
采用传统水热法制备出尺寸单一的银纳米颗粒,其反应机理基于相转移和相分离机制.银纳米颗粒的乙醇溶液通过甩胶处理涂抹在清洗后的硅片表面.Rhodamine 6G分子被用为检测分子,发现该材料为具有表面增强拉曼散射活性的衬底材料,其较大的增强因子可归结为金属颗粒耦合增强机制.
作者:沈剑沧 SHEN Jian-cang 作者单位:南京大学,物理学系,固体微结构物理国家重点实验室,江苏,南京,210093 刊名:兰州大学学报(自然科学版)ISTIC PKU 英文刊名:JOURNAL OF LANZHOU UNIVERSITY(NATURAL SCIENCES)年,卷(期):2007 43(5) 分类号: O657.3 关键词:银纳米颗粒水热法表面增强拉曼光谱。
二硫化钼的合成
Nano sphere MoS2 synthesized with lowconcentration high-ionic surfactant PEG-2000
assist
Conclusion
Hybrid
Modification
Reference
1. X Fan, P Xu, YC Li, D Zhou, Y Sun, et al. Controlled Exfoliation of MoS2 Crystals into Trilayer Nanosheets [J]. J. Am. Chem. Soc. 2016, 138, 5143−5149.
Introduction
The structure of transistor with 1-nanometer gate length
Introduction
Properties Crystal structure
Density Appearance
Hardness
Structure
Graphite
8. B Cabane,R Duplessix. Organization of surfactant micelles adsorbed on a polymer molecule in water : a neutron scattering study [J]. J. Physique 43 (1982) 1529-1542 .
Supporting Information
Laser induced synthesis
The flow chart of laser induced synthesis method
Laser induced synthesis
电负性在化学中的应用[总结]
附件1:学年论文(设计)学院* * * * 学院专业应用化学年级* * 级应用化学班姓名* * *论文(设计)题目电负性在化学中的应用指导教师****职称教授成绩2010年6月2日目录摘要: (1)关键词 (1)Abstract (1)Keywords (1)引言 (1)1.电负性理论的发展 (2)1.1元素电负性的发展及应用 (2)1.2离子电负性的发展及应用 (2)1.3键电负性的发展及应用 (2)2周期表中电负性的递变规律 (3)3.电负性的运用 (3)3.1电负性可用来判断元素、化学键类型 (3)3.2电负性可判断金属性和非金属性强弱 (3)4电负性效应对脂肪胺核磁共振谱化学位移的影响 (4)4.2 部分净电荷 (4)5结语 (4)参考文献: (5)电负性在化学中的应用学生姓名:* * * 学号:* * * * * *化学化工学院应用化学专业指导教师:* * * 职称:副教授摘要:本文主要讨论元素电负性理论的发展和应用,及元素周期表中电负性的变化规律。
同时讨论了运用元素的电负性判断元素类型,以及元素的价态、物质的晶型、化合物的键型,总结了元素电负性理论对化学领域几个方面的贡献。
关键词:电负性;应用;元素类型;价态;晶型;键型Abstract: This article main discussion element negativity theory development and application, and in the periodic table negativity change rule.Simultaneously discussed the utilization element negativity judgment element type, as well as the element valent state, the material crystal, the compound key, summarized the element negativity theory to chemistry domain several aspect contributions.Keywords: Electronegativity;Application; element type; V alence; crystalline; key-type;引言元素的电负性是指元素在形成的化学物质中将电子吸引向自己的本领。
材料硬度与键合性质关系分析
。
键体积 v ( ) 2. 836 10. 011 3. 457 5. 842 6. 813 5. 280 2. 952 5. 124 5. 708
μ b 3
体弹模量 B( GPa) 443 , 419 82. 7 421 [7] , 391 169 [7] 128 221[7] 401 368[7] , 203[6] 210[6] 358 , 344 305[7] , 310 496[6] 437[6]
-1 -7 式的特殊 K 点方法,倒空间的间隔小于 0. 04 ,自洽计算的 收 敛精 度 设 为 5. 0 × 10 eV / atom 。 对多种 晶 。 体结构和电子结构的计算结 果 如 表 1 , 并 结 合 imu nek 小 组 的 理论 硬 度 计 算 模 型 获 得 了 相 应 的 理论 硬 度 值。
。
2. 1 imunek 理论小组的理论硬度计算模型的一个改进 Mulliken 重叠布居值可表明原子在成键过程 中 转 移 ( 或产 生 偏 移 ) 的 电 子 数 目 情况, 据 此可 用 来 确 定 参 。 与成键原子的化合价态。这相对于 imunek 理论小组用 估 算 的 方法 来 确 定 元 素 化 合 价 要 更 加 合 理 和 准确。 如 4] 中,计算 ReB2 晶体的理论硬度时,Re 的 Mulliken 重叠布居计算值为 P v = 0. 66 ,就可以清楚 知 道 文献 [ Re 原子在与 B 原子形成 Re - B 键的过程中转移 走 了 0. 66 个 电 子, 成 键 化 合 价 就 为 6. 34 , 也就 不 用 再 为 Re 的化合价取值为 6 或 7 为难了。因而采用 Mulliken 布居值表征化合物中元素的化合价将使计算结果更加可信。 2. 2 材料的弹性参数与硬度之间的关系 将表 1 中各晶体的弹性参数与实验硬度作图,如图 1 所示。 从 图 中 可 以 看 出 各 晶 体 的 硬 度 与 剪 切 模 量或 者弹性模量之间没有一一对应的关系。如 WC 具有比 Cubic - BN 更高体弹模量 B 及相当剪切模量 G 值,但其 硬度却仅为后者的一半左右,同时 ReB2 具有 与 Cubic - BN 相 当 剪 切 模 量 G 值 但 硬 度 却 比 后者 小 很 多。 故 具 有高的体弹模量和剪切模量特征的材料不一定是高硬度材料。但 从 另 外 一 个方面 来 看, 具 有 较 高 硬 度 的材 料 却大多具有高体弹模量和剪切模量特征; 低硬度材料的体弹模量 和 剪 切 模 量 也 都较 低, 因 而 可 以 将 高体 弹 模 量和剪切模量特征作为高硬度材料筛选的充分而非必要条件,而最 后 能 否 成 为 超 硬 材 料 则 可 以 通 过 实 验验 证 36
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Review Condensed Matter PhysicsSynthesis of novel superhard materials under ultrahigh pressureChao Xu •Duanwei He •Haikuo Wang •Wendan Wang •Mingjun Tang •Pei WangReceived:28January 2014/Accepted:14May 2014ÓScience China Press and Springer-Verlag Berlin Heidelberg 2014Abstract Superhard materials are solids whose Vickers hardness is beyond 40GPa.They have wide applications in industry such as cutting and polishing tools,wear-resistant coatings.Most preparations of superhard materials are conducted under extreme pressure and temperature condi-tions,not only for scientific investigations,but also for the practical applications.In this paper,we would introduce the recent progress on the design and preparations of novel superhard materials,mainly on nanopolycrystalline dia-mond,B–C–N superhard solid solutions,and cubic-Si 3N 4/diamond nanocomposites prepared under ultrahigh pres-sure and high temperature (HPHT),using multi-anvil apparatus based on the hinged-type cubic press.Bulk materials of all these superhard phases have been suc-cessfully synthesized and are systematically tested.We emphasize that ultra-HPHT method plays an important role in the scientific research and industrial production of su-perhard materials.It provides the driving forces for the light elements forming novel superhard phases as well as the way for sintering high-density nanosuperhard materials.Keywords High pressure ÁSuperhard material ÁNanopolycrystalline diamond ÁB–C–N material ÁSi–C–N composites1IntroductionSuperhard materials are solids whose Vickers hardness is beyond 40GPa.Their synthesis is motivated by a need for robust,chemically diverse materials for industrial appli-cations,ranging from cutting and polishing tools to wear-resistant coatings [1–3].As the hardest known material,diamond and related products have been widely used to fulfill many of these needs.However,diamond also has limitations.For example,it is not effective for cutting steel and related materials due to a chemical reaction with iron.Thus,there is a great desire for new materials that can be used in place of diamond.Cubic boron nitride (cBN),currently the second hardest material in industry,can be used to cut ferrous metals.Yet,it does not exist in the nature and must be synthesized under extreme pressure and temperature conditions,making it quite expensive.There-fore,synthesis of novel superhard phases is not only for scientific investigations,but also for the practical applica-tions [1,3–10].Researchers find that superhard materials are commonly composed of boron,carbon,nitrogen,and oxygen.These light elements can form three-dimensional covalent bonds or networks,which can sustain large shear stress [1,3,6,8,11].By enhancing the large intrinsic strength,people could obtain intrinsically superhard materials.Up to now,most of the superhard materials,for example,diamond [9],cBN [10],B 6O [8],B–C–N [3],B–C materials [7],are synthe-sized under high-pressure and high-temperature (HPHT)conditions.Thus,high-pressure method provides an effective way to achieve novel superhard materials.In this paper,we would introduce the recent research progress on some new superhard materials,such as nanopolycrystalline diamond (NPD)[12],B–C–N superhard solid solutions [13],and Si–C–N composites [14],prepared underSPECIAL TOPIC:High Pressure PhysicsC.Xu ÁD.He (&)ÁH.Wang ÁW.Wang ÁM.Tang ÁP.Wang Institute of Atomic and Molecular Physics,Sichuan University,Chengdu 610065,Chinae-mail:duanweihe@Chin.Sci.Bull. DOI 10.1007//scpultrahigh pressure above 18GPa and high temperature up to 2,500°C using two-stage multi-anvil technologies based on the hinged-type cubic press.2Two-stage multi-anvil technologies based on the hinged-type cubic pressThe development of two-stage multi-anvil technologies and the achievement of extreme P –T conditions are the keys to the synthesis of novel superhard materials.In the high-pressure field,various types of two-stage multi-anvil appa-ratus have been developed,for example Walker-type and Kawai-type multi-anvil apparatus [9,10].Though they are widely used in the high-pressure laboratories,the equipment installations as well as the operation costs are very high.More importantly,their particular framework prevents them from being combined with advanced in situ detection tech-nologies.Therefore,there is a trend for researchers to develop new types of two-stage multi-anvil apparatus based on other frameworks.Based on the hinged-type cubic press,which is widely used in the superhard materials factories,we have successfully developed a two-stage multi-anvil appa-ratus as shown in Fig.1[15].Eight tungsten carbide (WC)anvils (18mm 918mm)with different truncation edge length (8,6,4mm)were used to generate pressure,and the semi-sintered magnesia (MgO)was processed into octahe-dral of different length (14,12,10mm)and then used as the pressure medium.These high-pressure assemblies are com-monly represented as 14/8,12/6,and 10/4assembly.Pyro-phyllite closely surrounds the octahedral as the gasket.Metals with high melting points (for example,molybdenum (Mo),tantalum (Ta),and rhenium (Re))are usually pro-cessed into tubes for heating,and zirconium dioxide (ZrO 2)is used as the thermal insulator [12].The pressure in the sample assembly can be calibrated based on the well-known phase transitions of materials like Bi [16],ZnTe [17],and ZnS [18]at room temperature,while temperature in the sample assembly can be measured directly using a B-type or W-Re-type thermocouple,with a precision of about ±10°C.When the needed experimental temperatures were higher than 2,100°C,temperatures could be estimated according to the electric power–temperature relationship,which might result in ±50°C errors.After years of development,the upper pressure limits of 14/8,12/6,and 10/4are about 16,19,and 22GPa,respectively,and the highest temperature can reach 2,500°C.Figure 1shows the whole structures and operation process of the two-stage multi-anvil apparatus based on the hinged-type DS698MN cubic ing this apparatus,we have synthesized some new superhard materials,such as NPD [12],B–C–N superhard solid solu-tions [13],and Si–C–N composites [14].3Synthesis of novel superhard materials 3.1NPDNPD,regarded as a new generation of high-performance superhard material,refers to the diamond products pre-pared through direct converting of graphite intodiamondFig.1(Color online)The structure and operation process of a two-stage multi-anvil apparatus based on the hinged-type DS698MN cubic pressChin.Sci.Bull.under static high pressure without any catalysts[9,19]. This type of product has a high-purity nanopolycrystalline body with strong and direct bonding offine diamond par-ticles in nanometer level.It not only has good perfor-mances that a natural single crystal diamond has,like high density,high hardness,and transparency,but also has better physical and chemical properties than those of single crystal and traditional polycrystalline diamond products. For example,NPD has higher thermal stability,higher fracture toughness,and better wear resistance[20–22].In the meantime,NPD is composed of nanoparticles,so it is isotropic,and can be arbitrarily processed into various shapes[23].Therefore,NPD has a broad application prospects in thefields of industrial applications and sci-entific research[24–26].In order to synthesize NPD samples,high-purity well-crystallized graphite(99.9995%,Alfa Aesar,USA),with crystalline size of5–20l m,was used as the starting material.In addition,some of the graphite was pretreated by high-energy ball-milling for34h in the argon gas atmosphere.In order to remove the absorbed substances such as harmful gases and water,all the powders were also processed in vacuum with the pressure of about 2.5910-3Pa and the temperature of about1,000°C. After these procedures,the powders were packed into the sample assembly immediately and put into the high-pres-sure apparatus[12].Figure2a shows the optical images of the NPD sample we have prepared under HPHT conditions of about 16GPa,2,300°C[12].It is about1.5mm in both diameter and height,and has a dark gray color.A high-quality X-ray diffraction(XRD)data of the as-synthesized sample were collected as can be seen in Fig.2b.By comparing the d-spacing data of the diffraction rings with the database,we found that the main diffraction peaksfit well with cubic diamond’s(111),(220),(311),and(400)diffraction peaks, indicating that the major phase of the as-synthesized sample was cubic diamond.Besides,two weak diffraction peaks were also found to be the(002)and(004)peaks of hexagonal diamond phase.Because of the ultrahigh tem-perature conditions,the package material(tantalum)reac-ted with the carbon source and thus generated a small amount of Ta–C compounds,as shown in the XRD pattern. By further increasing the temperature to about2,500°C, the hexagonal diamond would not appear in the sample, suggesting that the crystalline graphite can be completely converted to cubic diamond at this P–T condition[12].In comparison,we also synthesized NPD samples using the ball-milled graphite as the starting material.The results showed that even at2,100°C,the milled graphite could completely be converted into cubic diamond.Therefore, high-energy ball-milling pretreatment provides an effective way to lower the needed temperature for the NPD preparations under high pressure and can greatly reduce the NPD synthesis costs in the practical applications[12].Figure2c shows the scanning electron microscope(SEM) image of the polished sample that was prepared under P–T conditions of about16GPa,2,300°C using the ball-mil-led graphite as the raw material.We found that the NPD was fully dense,with grain sizes below100nm,which was consistence with the average crystalline sizes estimated according to the Scherer’s formula.We also tested the Vickers hardness of the well-sintered NPD samples through Vickers indentation method.In the hardness tests procedure, loading forces of0.5,1,3,5,and10kg could be chosen,and indentations for each loading force were repeated in three different areas of the polished surface,with the maintaining duration of15s.As is known,the obtained hardness values depend on the loading ually,the larger the loading force is,the lower for the hardness value is.By drawing the hardness-loading curves,scientists found that as the loading force increases,the hardness would decrease,butfinally tended to afixed value.Then,such asymptotic value of hardness versus load curve was regarded as the credible hardness of the material[27].When the load was0.5and 1kg,the indentations were too small to be detected.By further increasing the loading force,the indenter broke[12]. Thus,we believe that our NPD samples are ultrahard. Recently,we have developed a new method to synthesize NPD samples by direct sintering nanodiamond powders under HPHT.Figure2d shows the hardness test results of the NPD samples synthesized by direct sintering method.As shown in thefigure,when the load forces were0.5and1kg, almost no observable indentations were detected.With fur-ther increasing the loads to3kg,a small indentation could be clearly detected,and the hardness was found beyond 100GPa.By further increasing the loading force to5kg, and even to10kg,we got the asymptotic value of about 86GPa.Therefore,direct sintering nanodiamond powder under HPHT is also an effective method to synthesize ul-trahard NPD.3.2B–C–N superhard solid solutionsBoth diamond and cBN have disadvantages in practical applications.For diamond,it would become unstable in the oxygen-enriched environment around900K.Worse still, diamond would react with the ferrous alloys in the high-speed machining process.For cBN,though it possesses better chemical inertness,its hardness is only half of that of diamond.Thus,in order to obtain an ideal superhard material which could possess the advantages of both dia-mond and cBN,scientists were trying to search for some novel superhard phases,namely diamond–cBN alloy or B–C–N solid solutions[1].Theoretical studies suggest that high-pressure dense B–C–N ternary phases are excellentChin.Sci.Bull.alternative materials with ideal thermal stability and chemical inertness.More importantly,they have hardness much higher than cBN.Therefore,these B–C–N ternary phases would not only resist oxidation and graphitization in the extremely harsh working environment,but also keep stable during the hardened-steel cuttings [3,28].Because of technological importance,researchers are trying to prepare superhard B–C–N phases by sintering various starting materials under HPHT conditions [3,13,28–30].In our research [13],mixture of diamond and cBN,as well as mixture of graphite and hBN,was chosen as the raw materials.In the first set of experimental runs,diamond (Alfa,99.99%,0.5–1.5l m)and cBN powder (Alfa,99.99%,80nm–2l m)were first intensively mixed and pretreated in the vacuum.After packaged by the capsule and set into the high-pressure sample assembly,they were compressed to about 18and 20GPa,and heated to 2,000and 2,200K for 5min.We also pretreated the graphite and hBN through high-energy ball-milling process and finally got the amorphous mixture of the carbon and BN.Fig-ure 3a shows the sample prepared at 20GPa and 2,200K from such amorphous mixture.It was clear that the as-synthesized sample was a well-shaped transparent cylinder,with the height of about 1.5mm and diameter of about 1.2mm.The XRD patterns of samples prepared at various P –T conditions were shown in Fig.3b [13].For the sample prepared at the pressure of 18GPa and temperature of 2,000K,the XRD pattern showed visible bifurcations at the (111),(220),and (311)diffraction peaks.Meanwhile,we can see that there is an obviously broadened diffractionpeak in the d -spacing range from 3.8to 4.7A˚.By further increasing the pressure up to about 20GPa and the tem-perature to 2,200K,we got the sample as shown in Fig.3a,and the XRD data of the BC 4N sample show no peak splitting (Fig.3b).It is worth noting that,comparing with the diffraction data of our raw materials,the obvious (200)diffraction peak as well as other two new weak diffraction peaks were detected,indicating a new single crystalline phase was synthesized.This also indicates that the diamond and cBN grains started to react with each other at 18GPa and 2,000K,while at the P –T conditions of 20GPaandFig.2(Color online)a NPD sample prepared at 16GPa,2,300°C,b XRD of NPD prepared at 16GPa and 2,300°C,c SEM image of the NPD prepared at 16GPa and 2,300°C,d Vickers hardness of NPD sample synthesized at 18GPa,2,300°CChin.Sci.Bull.2,200K,the reaction occurred completely.According to the full width at half height of the XRD peaks,we could also find that,when the starting materials were not fully reacted with each other at 18GPa and 2,000K,the width of half height of the diffraction peaks had little change.However,when the reaction fully happened at 20GPa and 2,200K,the XRD peaks of the sample were obviously broadened,indicating the decreasing of the grain size.According to transmission electron microscope (TEM)observations and the Scherer’s formula,we estimated the average crystalline size of the synthesized sample to be about 40nm,which clearly proved that diamond or other carbon could react with BN above the P –T conditions of about 18GPa and 2,000K [13].The well-sintered BC 4N cylinder has a diameter above 1mm and thus was big enough for its hardness test.In our indentation experiments,when the applied loading force was less than 3kg,no observable indentations could be detected,indicating its superhard nature.Further increasing the loading force up to 5kg,a typical Vickers indentation was observed.By measuring the diagonal of the indenta-tions,and computing according to the Vickers hardness formula,we finally got the average hardness of 85±4GPa,very close to the hardness of diamond (75–100GPa).Our experimental hardness also agreed very well with the predicted hardness of 84.3GPa [31].3.3Si–C–N nanocompositesOne of the most famous superhard materials in the theo-retical prediction was carbon nitride (b -C 3N 4),whose hardness was predicted to be as large as that of diamond [32,33].Scientists have been trying to synthesize this potential superhard material,but as far as we know,no clear proof of successful preparation of carbon nitride was obtained.With a similar chemical formula of carbon nitride,cubic spinel Si 3N 4was synthesized by Zerr et al.[34].In the meantime,spinel nitrides,whose Si atoms are substituted by B,C,O,have been intensively studied theoretically [35–37].Though some of these novel superhard phases have been success-fully prepared,most of them are not.As a potential super-hard material with a predicted hardness of about 52GPa,spinel CSi 2N 4has not yet been prepared successfully [38].Thus,our initial purpose was trying to preparing spinel C 3N 4and CSi 2N 4through HPHT method [14].In our experiment [14],h-Si 3N 4(99.9%,1l m,Alfa Aesar),graphite (99.9995%,5–20l m,Alfa Aesar),or diamond powders were selected as the starting materials and were first intensively mixed in a Si 3N 4/C molar ratio of 1:6.Since the high-energy ball-milling process was usually applied in the mechanochemistry,enhancing the homoge-neity as well as the reactivity of the starting materials,we also treated our raw materials through the high-energy ball-milling process within nitrogen atmosphere for 26h.After that,it was treated under HPHT conditions.Figure 4a shows the C–Si–N sample prepared under the P –T conditions of 18GPa/2,000°C,with h-Si 3N 4/diamond mixture as the starting materials [14].From the figure,we can see that the sample has yellow–green color and shaped into a regular cylinder with a height of 2mm and a diameter of 1.2mm.XRD of the sample was tested as shown in Fig.4b.It was clear that the main phases of the sample were cubic Si 3N 4and diamond.There are weak peaks of Al 2O 3due to the Al 2O 3capsule.This indicated that both h-Si 3N 4and graphite were directly transformed into the cubic structure.However,no evidence was found for the formation of the new C–Si–N compound undersuchFig.3(Color online)a BC 4N sample prepared from a ball-milled amorphous mixture of the graphite and hBN at 20GPa and 2,200K,with height of 1.5mm and diameter of 1.2mm,b XRD patterns of the samples are (I)prepared from the mixture of diamond and cBN at 18GPa and 2,000K;(II)synthesized at 20GPa and 2,200K with a ball-milled mixture of the graphite and hBN;(III)prepared from the mixture of diamond and cBN at 20GPa and 2,200K.The top right inset is the XRD pattern for the starting mixture of diamond and cBN [13]Chin.Sci.Bull.P –T condition.We further checked the sample by TEM as shown in Fig.5and found that the crystalline size of c-Si 3N 4/diamond sample is about 20nm [14].Vickers hardness test was performed as well.When the loading force was about 1kg,the measured Vickers hardness was about 41.0GPa,significantly greater than that of the pure c-Si 3N 4(about 31GPa).More importantly,by sintering composites with nanodiamond,we can not only enhance the toughness of c-Si 3N 4samples greatly,but also got a well-sintered bulk c-Si 3N 4/diamond nanocomposite [14].4ConclusionsIn this paper,we introduced the recent progress on the synthesis of novel superhard materials,such as NPD,B–C–N superhard solid solutions,and Si–C–N nanocomposites under ultra-HPHT using multi-anvil apparatus based on the hinged-type cubic press.Bulk materials were successfully synthesized and superhard.We emphasize that ultra-HPHT method plays an important role in the scientific research and industrial production in the field of novel superhard materials.It provides not only the driving forces for the light elements forming 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