Superhard Superconductive Composite Materials Obtained by High-Pressure-High-Temperature Sintering

1. Introduction

Superhard superconducting materials are of considerable interest for the creation of high pressure devices for investigating electrical and superconducting properties of various materials. The superconducting composites consisting of superconductors and superhard materials that are in thermal and electrical contacts may satisfy very conflicting requirements imposed on superconducting materials for special research cryogenic technique, wear-resistive parts of superconductor devices, superconducting micro-electro-mechanical systems (MEMS), etc. The design of materials combining such properties as superconductivity, superhardness, and high strength is an interesting task for both scientific and applied reasons. Superconducting composites may be used for the production of large superconducting magnetic systems (Gurevich et al., 1987).

The discovery of superconductivity in heavily boron-doped diamonds (Ekimov et al., 2004; Sidorov et al., 2005) has attracted much attention. Superconducting diamonds are the hardest known superconductors. The potential applications of superconducting diamonds are broad, ranging from anvils in research high-pressure apparatus to supecronducting MEMS. However, the highest value of the superconductivity onset temperature in boron-doped diamonds was found just about 7 K in thin CVD-grown films (Takano et al., 2004) and at about 4 K in bulk diamonds grown at high-pressure and high-temperature (Ekimov et al., 2004; Sidorov et al., 2005). In these pioneering works bulk polycrystalline diamonds with micron grainsize have been synthesized from graphite and B₄C composition (Ekimov et al., 2004) and graphite with 4 wt% amorphous boron (Sidorov et al., 2005). The synthesis have been carried out at 8-9 GPa pressure and 2500-2800 K temperature in both cases. Later Dubrovinskaya et al., 2006, carried out synthesis of graphite with B₄C composition at much higher pressure value 20 GPa but the same temperature of 2700K and found the superconducting state transition at lower temperature 2.4 - 1.4 K in the obtained doped polycrystalline diamonds. Due to the sharpening of the temperature interval of the superconductivity transition in magnetic field they suggested that superconductivity could arise from filaments of zero-resistant material. An alternative method for the creation of composite diamond superconductors was suggested by one of the authors of the present article, G. Dubitsky, who used sintering of diamond powders with molybdenum to fabricate special research high-pressure anvils with T_C= 10 K (Narozhnyi et al., 1988). Such a unique high-strength superconducting anvils for research high-pressure apparatus were employed for investigations of the pressure effect up to 22 GPa on the superconductor transition temperatures in the metallic high-pressure phase of GaP. Modern technologies for large-scale industrial powder diamonds and cubic boron nitride manufacturing provide an easy opportunity to produce a wide range of superhard sintered superconductors with various mechanical and electronic properties.

By sintering diamond micropowders with metal powders (Nb, Mo) and using metal-coated diamond micropowders at high static pressure and temperature we obtained superhard superconductors with T_Csubstantially higher than in boron-doped diamonds (Dubitsky et al., 2005, 2006). Interacting with diamond, Nb and Mo metals form carbides bonding diamond crystallites into a united compact material having relatively high critical temperatures of the transition to the superconducting state.

The alternative route is the sintering of superconductor powders with superhard fullerites - new carbon materials produced from C₆₀ and C₇₀ fullerenes (Blank et al., 1998, 2006). Under high pressure and temperature treatment soft C₆₀ and C₇₀ powders transform into fullerene polymers and other carbon structures with various hardness including superhard and even superior to diamond. There are known many alkali metal-fullerene superconductors with relatively high T_Cup to about 30K (Holczer & Whetten, 1993, Kulbachinskii, 2004, Kulbachinskii et al., 2008). However alkali metal-fullerenes react with oxygen when exposed to air. Sintering with inert superhard materials may protect such compounds from oxidation and provide superconducting properties of such superhard composites.

The highest critical temperature of superconductor transition among known "regular" superconductors has magnesium diboride MgB₂ with T_C= 39K. The superconductor composites based on MgB₂ and superhard materials are promising materials as well (Kulbachinskii et al., 2010).

Using high-pressure-high-temperature sintering method we manufactured the following composite superhard superconducting materials: diamond-Nb, diamond-Mo, diamond-MgB₂, cubic boron nitride-MgB₂, fullerite C₆₀- MgB₂, diamond-Ti₃₄Nb₆₆, diamond-Nb₃Sn, what will be described in this chapter.

2. Experimental section

Experimental samples of the target materials were obtained by treatment at high static pressures and temperatures. The experiments were carried out using modified “anvils with cavity”-type high-pressure apparatus (Blank et al., 2007). Pressure value was calibrated by electrical resistance jumps in reference metals Ba (5.5 GPa), Bi (2.5, 2.7, 7.7 GPa), Pb (13 GPa) and ZnSe (13.7 GPa) at known phase transitions. The temperature graduation of the chambers was performed using Pt/Pt-10%Rh and W/Re thermocouples. The initial components were placed into a tantalum-foil shell of 0.1 mm thickness. Samples were heated by ac current through a graphite heater with a tantalum shell as a part of the sample system. The materials have been obtained at pressures in the range of 7.7 - 12.5 GPa and temperatures of 1373 - 2173 K. The heating time was 60 – 90 s. The samples were quenched under high pressure with a rate of 200 K per second. After pressure release the samples were extracted from the high-pressure cell. Small cylinder-shaped samples with a diameter of 4.5 mm and a height of 3.5 mm were obtained. The parallelepiped samples 3.9×2.51×1.54 mm³ size were made by laser cutting and polishing. The examples of optical images of polished surfaces for 2 different samples are presented in Fig. 1.

Figure 1.

The examples of images of the polished surfaces of diamond-Nb sample (a) and micro-nanodiamod-NbTi sample (b).

The pictures show grains of superhard compound like diamonds and superconducting compounds like metal alloys in between the grains. The X-ray diffraction analysis revealed formation of metal carbides on the boundaries of diamond micro- and nanocrystals and nanocarbon phases originated from C₆₀ fullerene in the samples synthesized with C₆₀ powder. The carbide phases provide strong chemical bonding of superconductor matrix with superhard carbon grains, thus the target composites possess very high strength.

We investigated the phase content of the samples by the powder X-ray diffraction method using an ARL X’TRA diffractometer with Si-Li semiconductor detector and Cu Kα radiation (λ = 0.1541 nm) source. The electrical resistance of the resulting samples was measured by the conventional four probe method. Electrical contacts were made using conducting silver paste. The temperature dependence of the resistance was measured in the interval 1.7 < T < 300 K. We applied the magnetic field up to 5T to determine the effect of magnetic field on the superconductivity transition temperature.

The Vickers microhardness was measured using PMT-3 device at an indenter load of 5.5 N. Sound velocities in 3 samples were measured using a wide-field pulse scanning acoustical microscope (WFPAM) in reflection mode (time-of-flight method) at a driving frequency of 50 MHz. The mean diameter of the acoustic beam in the specimen was about 0.1 mm. This experimental procedure was described in detail in (Prokhorov et al., 1999).

3. Superhard material-superconductive metal-systems

3.1. Diamond-niobium system

Synthetic diamond powder with 80 – 100 µm crystallites covered with a niobium film by vacuum sputtering was used as the initial material. The total amount of niobium in the initial material was 24 wt %. The experiments were carried out at a pressure of 7.7 GPa and a temperature of 1973 K for 60 s. The diffraction patterns exhibited peaks associated with diamond and NbC monocarbide (Fig. 2 ). A small fraction of NbO₂, practically traces, was also found. The NbC monocarbide synthesized at the boundaries of the crystallites had a face-centered cubic lattice with the cubic parameter a₀= 0.447 nm. This value is consistent with the data obtained for NbC by another method (Toth, 1971).

Figure 2.

X-ray diffraction pattern of sintered diamond-niobium sample. Diffraction reflections of NbC, diamond and NbO₂ are denoted.

The critical temperature of the transition to the superconducting state in all the measurements was fixed at the onset of the transition. According to an analysis of the temperature dependence of the resistance, the critical temperature of the transition of the synthesized samples to the superconducting state was equal to T_C≈ 12.6 K (Fig. 3a), which is characteristic of a NbC compound with almost full carbon positions (Karimov & Utkina, 1990; Shabanova et al., 1996; Krasnosvobodtsev et al., 1995). Carbon deficient NbC_1−x having lower T_Cor superconductivity was entirely absent. The characteristic feature of the synthesized samples is a quite narrow superconducting transition, ∆T≈ 1.5 K. The measured dependence of the resistance of a sample on the external magnetic field (Fig. 3b) is characteristic of NbC carbide. The value of the second critical field H_C2 = 1.25 T (at T= 4.2 K) is consistent with H_C2for NbC films obtained by the laser-evaporation method (Shabanova et al., 1996). Thus, one may conclude that crystallites NbC with an almost perfect crystal structure were formed on the surface of the sintered diamond and a low concentration of defects has place in NbC which reduces the temperature of the superconducting transition (Pickett et al., 1986). An insignificant admixture of NbO₂ had no effect on the critical temperature of samples.

The microhardness values varied in the range of 35 –95 GPa depending on the actual place of indentation (Dubitski et al., 2005, 2006). According to (Toth, 1971), the Vickers microhardness of NbC is approximately equal to 17 GPa. This value is significantly lower than the results obtained in our work for microdomains enriched in NbC The hardness of

Figure 3.

Temperature (a) and magnetic field (b) dependences of the resistance for the sample obtained in the diamond-niobium system.

	P; g cm^-3	VL; km s^-1	VT; km s^-1	E; GPa	B; GPa	G; GPa	σ
Diamond-Nb	4.1± 0.1	12.1± 0.5	6.9± 0.25	490± 95	340± 30	195± 14	0.26± 0.04
Polycrystalline; diamond "carbonado"	3.74± 0.05	16± 0.5	9.6± 0.3	850± 120	490± 30	340± 24	0.22± 0.04

Table 1.

Diamond-Nb density ρ, longitudinal and transverse sound velocities V_L, V_T, Young modulus E, bulk and shear elastic modules B, Gand the Poisson ratio σ. Data for polycrystalline sintered diamond "carbonado" type are given for reference.

such microdomains is high apparently due to the effect of the of diamond crystallites, which have much higher hardness (100 – 150 GPa along different faces, depending on the quality of the crystals). The velocities of sound and the elastic modules are 30 – 40% less than in pure bulk polycrystalline diamond (Table 1). Nevertheless they are comparable with the values for the next very strong superhard material: cubic boron nitride (c-BN).

3.2. C₆₀-diamond-niobium system

High-pressure - high-temperature treatment of C₆₀ and C₇₀ fullerenes leads to polymerization and transformation into new metastable carbon structures (Blank et al., 1998, 2006). Among various polymeric forms, the 3D-polymeric ones are the hardest

Figure 4.

The X-ray diffraction pattern (a) and the temperature dependence of the resistance (b) for the sample obtained in the C₆₀- diamond-niobium system.

(Blank et al., 1998). The density of superhard (H_v > 50 GPa) and ultrahard (H_v > 120 GPa) forms ranges from 2.5 to 3.3 g cm⁻³, intermediate between the densities of graphite and diamond. Mechanical, electrical and other properties of such materials strongly depend on their particular crystalline or disordered structure. A set of metal-C₆₀ compounds are superconducting with T_C= 2 – 34 K (Holczer & Whetten, 1993). However the conventional fullerene superconductors are not hard and chemically reactive; they oxidize in air. We investigated the synthesis of composite superconductors on the basis of a 50%–50% mixture of C₆₀ powder with niobium coated diamond powder (Dubitsky et al., 2006) as described in the part above. Sintering was carried out at a pressure of 12.5 GPa and temperature 1650 K. The XRD analysis (Fig. 4a) showed formation of a disordered superhard component on the basis of C₆₀ (broad diffraction peak) and niobium monocarbide with diamond crystals. The microhardness values of this composite material was 45 – 95 GPa. It is superconducting below 10.5 K (Fig. 4b).

3.3. Diamond-molybdenum system

In this system, a synthetic-diamond powder with a granularity of 40 – 100 µm and a molybdenum powder with a particle size of 1 – 5 µm were used as the initial materials consisting of 60 wt % of diamond and 40 wt % of molybdenum. A compact material was obtained by holding at a pressure of 7.7 GPa and a temperature of 2173 K for 90 s. The phase content of the samples was determined by the same method as for the diamond-Nb system. The following phases were identified in the samples: the diamond, the α-MoC phase with a cubic lattice with the parameter a₀ = 0.427 nm (B1 type), the η-MoC hexagonal phase with the lattice parameters a₀= 0.300 and c₀= 1.452 nm, and traces of the hexagonal γ-MoC phase (WC type) with the parameters a₀= 0.290 and c₀= 0.282 nm. The lattice parameters that were determined for molybdenum-carbon compounds are consistent with the data published by (Toth, 1971). The Vickers microhardness of the samples varies in the range of 27 – 83 GPa.

Figure 5.

Temperature dependence of the resistance for the sample obtained in the diamond-molybdenum system.

The composites obtained in the reaction of diamonds with molybdenum are superconductors with characteristic features. First, the onset of the transition to the superconducting state is T_C= 9.3 K, which is slightly lower than the T_Cvalues for molybdenum carbide obtained by sintering powders of molybdenum and graphite (Willens et al., 1967). Second, the transition width T≈ 5 K is larger than that for the diamond-niobium system. Fig. 5 shows the temperature dependence of the resistance of these composites.

4. Superhard material-MgB₂-systems

4.1. Diamond-MgB₂ and cubic boron nitride-MgB₂-systems

Magnesium diboride, whose superconductivity was discovered 10 years ago (Nagamatsu et al., 2001; Zenitani & Akimitsu, 2003) has much higher critical temperature T_C= 39 K than niobium carbide and molybdenum carbide. Many investigations were devoted to the effect of the conditions of MgB₂ producing and treatement at high pressures and temperatures on the superconducting properties with various dopants (Jung et al., 2001; Prikhna et al., 2002; Pachla et al., 2003; Tampieri et al., 2004; Toulemonde et al., 2003; Zhao et al., 2003; Dou et al., 2003). It is of interest to obtain a superconducting composite material in which diamond or cubic boron nitride are used as the superhard components and MgB₂ is used as the superconducting component.

As the initial material, we used industrial MgB₂ powders in which the content of the basic product was equal to 98.5%. The particle size was reduced to 5 – 10 µm by additional powdering. The prepared mixtures consisted of 80 wt % of the superhard component and 20 wt % of MgB₂. The granularity of the diamond and cubic boron nitride powders was equal to 40 – 100 and 28 – 40 µm, respectively. The assembly of the high-pressure cells and the experimental procedure were the same as those used for the diamond-molybdenum system. In one of the experiments, a niobium-coated diamond powder was used. The samples were obtained by sintering at a pressure of 7.7 GPa and a temperature of 1373 K for 60 s.

Using XRD analysis, diamond, MgB₂ and MgO were identified in the system diamond-MgB₂ after the synthesis.

The temperature dependence of the resistance of the samples shows that the temperature of the transition to the superconducting state is T_C≈ 37 K (Fig. 6), which is close to the value known for MgB₂ (Nagamatsu et al., 2001). This closeness indicates that MgB₂ has a key role in the superconductivity of these composite materials, and the matrix consisting of cubic boron nitride or diamond changes Tcinsignificantly, while the hardness of such superconducting material is much higher than the one of compacted MgB₂.

The microhardness of the samples indicates that the composite matrix (consisting of cubic boron nitride or diamond) occupying the major part of the body of the samples has a

	,; g cm-3	VL,; km/s	VT,; km/s	E,; GPa	B,; GPa	G,; GPa		Hv,
Diamond- MgB2	3.40.1	5.60.3	3,30.15	9020	574	353	0.230.04	2578
cBN -MgB2	3.30.1	6.00.3	3.70.15	11025	607	454	0.190.04	2457

Table 2.

Diamond- MgB₂ and cBN-MgB₂ composites density ρ, longitudinal and transverse sound velocities V_L, V_T, Young modulus E, bulk and shear elastic modules B, Gand Poisson ratio σand the Vickers microhardnes H_v.

Figure 6.

Temperature dependence of the resistance (a) and transition range (b) for the composite samples obtained in the systems (1) cubic boron nitride-MgB₂,T_C= 36.1 K, (2) diamond-MgB₂,T_C= 36.9 K, (3) MgB₂,T_C= 37 K, and (4) diamond-niobium-MgB₂,T_C= 37.5 K.

microhardness of 57 – 95 GPa. Such microhardness values are characteristic for superhard compact polycrystalline materials based on cubic boron nitride and diamond that are used to produce various abrasive and cutting tools (Shul’zhenko et al., 1987). The specific gravity and velocities of longitudinal and transverse sound waves were measured and elastic modules evaluated (Table 2). Though the elastic modules are not very high, such materials have good potential for applications.

4.2. Polymerized fullerite C₆₀-MgB₂- system

We synthesized and investigated a set of composite materials obtained from MgB₂ superconductor and C₆₀ fullerite mixed in various bulk ratios (Kulbachinskii et al., 2010). The same commercial MgB₂ powder with 98.5% of MgB₂ and commercial C₆₀ powder with 99,8% C₆₀ and the rest 0,2% of other carbon components were used as the initial compounds for the synthesis. The superconducting superhard composite possesses superconductivity due to MgB₂ fraction and superhardness due to polymerized C₆₀ part (Blank et al., 1998).

Figure 7.

Diffraction data composites MgB₂:C₆₀. Parameters of synthesis are shown at figures.

The particle size was reduced to 5–10 µm by additional powdering. We prepared polycrystalline composite MgB₂:C₆₀ with different wt. content of C₆₀ up to 60%. The samples of the materials were obtained at high static pressures 7.7 GPa and temperatures 1273 - 1373 K. The Vickers microhardness values of composites MgB₂-C₆₀ were in the range of 18 – 59 GPa. The lowest value has been measured at the local point with dominating MgB₂ grains and the highest ones at the point with dominating superhard compound. According to (Prikhna et al., 2002), the Vickers microhardness H_Vof MgB₂ with 2 wt. % of Ta synthesized at T_s=1073 K and P = 2 GPa was approximately equal to 12.8 GPa. In samples of composites

Figure 8.

a) Temperature dependence of resistivity for composites with different content MgB₂:С₆₀: 1 – 80:20; 2 – 40:60; 3 – 50:50 wt%; b) logarithm of the relative change of the resistivity versus T^-1/4.

MgB₂:C₆₀ we identified MgB₂, MgO and superhard 3D-polymerized C₆₀. MgO was revealed in the initial magnesium diboride, its content increased with the increasing of sintering temperature. In Fig. 7 diffraction data are shown for two samples with different MgB₂:C₆₀ ratio.

It was found that up to 20 wt. % C₆₀ the composite MgB₂:С₆₀ is a superconductor. The superconducting transition temperature of composite MgB₂:С₆₀ – 80%:20% is Т_C=39,2 К, that is the same as for host MgB₂ (Т_C≈ 39 К (Nagamatsu et al., 2001) ). In Fig. 8 we plotted temperature dependences of resistivity for composites with different С₆₀ content.

The resistivity of the superconducting composite MgB₂:С₆₀-80%:20% increases near the transition to the superconducting state (39<T<80 K). It is not typical for the host MgB₂. We suppose that in this temperature range C₆₀ clusters play a significant role in the temperature dependence of the resistivity. For clusters of C₆₀ the resistivity increases when temperature decreases (Buga et al., 2000, 2005).

When the content of C₆₀ increases above 20 wt. %, the superconductivity disappears and the temperature dependence of the resistivity changes. Mott variable range hopping conductivity was observed, following the law:

$$\sigma ={\sigma }_0\text{exp}\left\{-{\left({\text{T}}_0/\text{T}\right)}^{\text{1}/\text{4}}\right\}$$E1

Fig. 8b. shows the relative change of resistivity in logarithmic scale on T^-1/4. The linear dependence is clearly visible in the temperature range 4.2- 60 K. When the content of С₆₀ is >60 wt. % the resistivity slowly increases with the temperature decrease as it is shown in Fig. 8 for sample MgB₂:С₆₀-40%:60%. This takes place because the main superhard carbon component which appeared after C₆₀ transformation has graphite-like cross-linked layered structure with semimetallic type of conductivity (Buga et al., 2000).

Figure 9.

The crystal structure of MgB₂. Axes of hexagonal unit cellaandcare designated.

MgB₂ has hexagonal crystal structure ((Nagamatsu et al., 2001). This structure (Fig. 9) consists from a sequence of hexagonal closed packed layers of Mg and graphite-like layers of B. In such structure atoms of Mg have ionic bonding with atoms of B. Inside the boron layer B atoms have covalent 2D bonding.

The critical field value B_c^cfor magnetic field parallel to caxis is about 3–4 T down to T = 0 K (Lyard et al., 2002). The value of in plane critical magnetic field B_c^abin the abplane is significantly higher and reaches 15–20 Т at T=0 K. The anisotropy coefficient is equal B_c^ab/B_c^c= 4–5. In the superconducting composite MgB₂:С₆₀-80%:20% we measured superconducting transition at different magnetic fields. (Fig. 10a). Using these data the temperature dependence of the critical magnetic field B_cwas plotted in Fig. 10b. The temperature dependence of B_cis close to the same dependence in the initial MgB₂ (Lyard et al., 2002; Buzea & Yamashita, 2001). Thus composite with 20 wt. % of C₆₀ has the same superconducting parameters as host MgB₂.

Figure 10.

Temperature dependence resistance of R for MgB₂:С₆₀ - 80:20 wt. % at different magnetic field (a), and temperature dependence of critical magnetic fieldB_c(b) that is similar to that of the initial MgB₂.

4.3. Superconductivity of heterofullerides

Recently a method has been developed for synthesizing superconducting heterofullerides of the Fe and Cu groups with the composition K₂MC₆₀ (Bulychev et al., 2004). For example, Fig. 11a shows the temperature dependence of the magnetic susceptibilityfor fullerides with M=Fe, Ni, Cu. Also shown in Fig. 11a is the (T) curve for the well-known superconductor K₃C₆₀ for comparison. Superconducting heterofullerides of composition K₂MC₆₀ have lower superconducting transition temperatures T_cthan K₃C₆₀, and the crystal lattice constant a of

Figure 11.

Temperature dependence of the magnetic susceptibility x of fullerides of composition K₂MC₆₀ (M = Fe, Ni, Cu) and K₃C₆₀ for comparison (upper) and compounds RbCsTlC₆₀, KCsTlC₆₀, Rb₂TlC₆₀ (down).

the heterofullerides studied is smaller than that of K₃C₆₀, apparently because substitution of the potassium ion by an ion of smaller diameter decreases the lattice constant. Thus there is a correlation between the superconducting transition temperature and the crystal lattice constant: a decrease of a leads to a decrease of T_c.

Fullerides RbCsTlC₆₀ and Rb₂TlC₆₀ have superconducting transition temperature T_c= 26.4 K, and 27.2 K respectively. For KCsTlC₆₀, the value of T_c= 21.7 K is the highest for fullerides with potassium atoms. Temperature dependences of the magnetic susceptibility of these compounds are plotted in Figure 11b. The fulleride KCsTlC₆₀ possesses the highest T_c= 21.7 K among all synthesized in the present study of heterofullerides with potassium. This confirms the suggestion that the increase of the T_cvalue is due to the increase of the lattice constant caused by substitution of K and Rb by Cs. KCsTlC₆₀ has maximal value of a (a = 1.442 nm compared to K₃C₆₀ a = 1.431 nm) among all superconducting heterofullerides with potassium. The same is for RbCsTlC₆₀ (a = 1.467 nm, Rb₂BeC₆₀ a = 1.445 nm). Such appreciable increase of the parameter a of face-centred cubic lattice is quite naturally and also is one more proof of intercalation of atoms of bigger sizes in fulleride structure. There were no superconducting transitions in heterofullerides with more than one Cs atom per fullerene C₆₀. It is of substantial interest to investigate sintering of such compounds with superhard materials like diamond and сBN to learn if superhard compounds protect superconducting metal-fullerene compound against oxydation and provide high mechanical properties of the composite.

5. Ti₃₄Nb₆₆- and Nb₃Sn-diamond micropowder-systems

5.1. Ti₃₄Nb₆₆-diamond system

The NbTi alloy is a superconductor which has one of the best strength and high critical magnetic field. A set of new composite materials were synthesized from Ti₃₄Nb₆₆ and Nb₃Sn superconductors mixed with microcrystalline diamond and nanodiamond powders in various bulk ratios. The particle size of superconductors was reduced to 5–10 µm by powdering.

The initial Ti₃₄Nb₆₆ alloy (Fig. 12) has a body-centered cubic crystal structure with I m͞ 3 m space group and the unit cell parameter а = 0.328 nm. The superconducting temperature T_C= 9.85 К is known for this alloy.

The crystal structure of Nb₃₄Ti₆₆ is a homogeneous solid solution with statistical distribution of elements in a unit cell. Figure 13 shows diffractograms of samples obtained after sintering of the mixture of diamond powder and superconductor under pressure of 7.7 GPa at temperatures 1373 K and 1623 K. The lower diffractogram No. 4 (Fig. 13a) was obtained from the initial alloy, the next one (No. 3) of the sample obtained after sintering at 1373 K. No reflections of TiC or NbC appeared at this synthesis temperature.

The next two samples were sintered at 1623 K. The diffractogram No. 2 corresponds to the sample Nb₃₄Ti₆₆ (50%) mixed with 45% diamond micropowder covered by Nb and 5% of nanodiamond is added in this composition. The diffractogram No. 1 corresponds to the sample Nb₃₄Ti₆₆ (50%) mixed with 50% diamond micropowder. We will discuss in detail the difference of diffraction patterns of these samples and how it may affect on the superconductive transition temperature.

At the dffractograms of samples No. 1 and 2 the diffraction peaks from Nb₃₄ Ti₆₆ alloy are easy visible because they have maximal amplitude. They are slightly shifted one to another and the shift is larger at wide angles (2θ ∼ 90 ÷ 100⁰). A cubic unit cell parameter of Тi₃₄Nb₆₆

Figure 12.

The crystal structure of Nb₃₄Ti₆₆ alloy. Nb and Ti atoms have no determined positions.

alloy calculated with the wide angles (see fig. 13) а=0.329 nm of sample No. 1 is slightly less than а = 0.330 nm of sample No. 2. The intensities of the main peaks are different in these two samples. The intensities of TiC and NbC peaks are different in these samples as well. In sample No. 1 the intensity of TiC-reflections is higher than NbC-reflections while in sample No 2 the intensity of NbC-reflections is higher than TiC-reflections. As for example, at 2θ = 70÷75⁰ and 85÷90⁰ regions (Fig. 13b) NbC-reflections of diffractogram No. 1 disappear. The additional Nb covering diamond crystals in sample No. 2 leads to higher quantity of NbC in this sample. Apparently, 5% of nanodiamond in sample No. 2 increases a separation of Nb. Taking into account that the atomic radius of Ti (0.146 nm) is higher than the atomic radius of Nb (0.145 nm) and that the intensities of NbC – reflections increased, we suppose that the concentration of Nb in sample No. 1 is higher than in sample No. 2. That is why the cubic parameter is smaller. This leads to higher Т_Cin sample No 1 than in sample No. 2 (Fig. 14).

The appearance of NbC and TiC evidences partial decomposition of Nb₃₄Ti₆₆ alloy during the synthesis. Carbides were synthesized under high pressure 7.7 GPa without melting of metals though temperature of synthesis 1625 K is less than the necessary for direct synthesis of carbides. Their melting temperatures exceed 2000 K. The large part of carbon (50%) in samples promotes formation of carbides. However, the content of carbides is not sufficient to rise the T_Cvalue up to 12.6 K known for NbC carbide.

Table 3 shows the Vickers microhardness of Ti₃₄Nb₆₆ –diamond composite samples No's 1 and 2. The value of microhardness has a wide range as well as in the other composites: the lowest value of hardness has been measured for the Ti-Nb-alloy located in superconductive channels (35 GPa in sample No. 1 and 42 GPa in sample No. 2) and the highest ones in superhard matrix (93-98 GPa). We suppose that the higher hardness of channels (42 GPa) in sample No. 2 has place due to nanodiamond fraction in this sample.

No. 1: 50% Ti₃₄Nb₆₆ + 50% diamond micropowder, T_C=8.9 K;

No. 2: 50% Ti₃₄Nb₆₆ + 45% diamond micropowder covered by metallic Nb + 5% nanodiamond, T_C=6 K.

Figure 13.

a) Diffractograms of (Ti₃₄Nb₆₆ + diamond micropowder) samples sintered at high pressure 7.7 GPa and high temperature 1373 K and 1623 K. The composition of samples: 1) 50% Ti₃₄Nb₆₆ + 50% diamond micropowder, T=1623 K; 2) 50% Ti₃₄Nb₆₆ + 45% diamond micropowder covered by Nb + 5% nanodiamonds, T=1623 K; 3) 50% Ti₃₄Nb₆₆ + 50% diamond micropowder, T = 1373 K; 4) initial Ti₃₄Nb₆₆ alloy.

(b) X-ray diffractograms of samples No's. 1 and 2._. D – diffractional reflections of diamond, NbC and TiC – diffractional reflections from Nb and Ti carbides. TiNb and the wide angles of 2θ⁰ are denoted for Ti₃₄Nb₆₆ reflections.

Figure 14.

Temperature dependence of resistance in two superhard composites sintered at T = 1623 K and P =7.7 GPa.

Sample; No.	Composite	Component ratio, wt.%	Vickers microhardness,; GPa	Tc, K
1	Ti34Nb66 –diamond micropowder	50:50	35-93	8.9
2	Ti34Nb66 –(diamond micropowder covered by Nb + 5% nanodiamond)	50:50 (45:5)	42-98	6

Table 3.

The Vickers microhardness and the temperature of superconductive transition T_Cof synthesized composite materials.

5.2. Nb₃Sn-diamod-system

An intermetallic Nb₃Sn compound crystallizes in cubic structure type A-15. Tin atoms are located in body-centered cubic positions, pairs of Nb atoms located on the cubic faces parallel to the coordinate axes (fig. 15). The unit cell contains 8 atoms: 2 Sn + 6Nb; the space group Pm3n, a_cub. = 0.529 nm. Nb-atoms generate cross-cut chains (fig. 15a). The interatomic distance for Nb-atoms in one chain is appreciably less than the distance in the different chains. The chains of Nb-atoms respond for the generation of quasi one-dimensional electronic spectrum of d-state in this structure.

Nb₃Sn was mixed with micropowdered synthetic diamond and sintered at P = 7.7 GPa, T=1623 K. The diffraction pattern in Fig. 16 shows that under high temperature and pressure Nb₃Sn partially decomposes to atoms of Nb and Sn. Metallic Nb creates NbC, while Sn in sample is in metallic state. It is worth to note that the temperature of synthesis 1623 K is much less than the melting temperature of Nb₃Sn (2400 K). It means that niobium carbide was synthesized in solid state without melting of metal. The content of metallic Sn is very

Figure 15.

The crystal structure of Nb₃Sn. a –Positions of atoms in the unit cell, b – chains of Nb-atoms. The coordinate axes are denoted in the b-part where two unit cell are painted.

small. Positions of diffractions peaks of Nb₃Sn correspond to the diffraction database (ICDD database PDF-2, card № 19-0875). Thus the decomposition of Nb₃Sn is insignificant in spite of high parameters of sintering. The composite Nb₃Sn with diamond powder is a superconductor with T_Cabout 15.5 K as it is shown in fig. 17. This value of T_Cis close to the T_Cof the initial Nb₃Sn.

Figure 16.

X-ray diffraction pattern of (50%Nb₃Sn + 50% micropowder diamond) sample sintered at P = 7.7 GPa, T = 1625 K; D – reflections of diamond, NbC – reflections of niobium carbide.

Figure 17.

Temperature dependence of resistance in different superhard composites: 1 – 50%Nb₃Sn + 50% micropowder diamond (T_C=15.6 K); 2 – 70%Nb₃Sn + 30% micropowder diamond (Т_C=15.5 K) and 3 – MgB₂+cBN (T_C=36.5 K) for comparison.

6. Conclusion

The superhard superconducting composites are the new large family of materials for cryogenic electro-mechanical tools and devices. We employed high-pressure-high-temperature technique for synthesis of various superconducting composites on the basis of the hardest known materials: diamond, cubic boron nitride, C₆₀-fullerites. The best traditional superconductor alloys and relatively new, like MgB₂ have been used for synthesis to provide a superconductivity of the target materials. The structure and properties of the synthesized composites have been investigated. The highest values of microhardness up to 98 GPa and the highest elastic moduli have been found in diamond-based composites. Among them diomond-niobium composite is the hardest and it possesses 12.5K superconductor transition temperature. The highest T_C= 37.5 K has diamond-niobium-MgB₂ composite. The composites of superhard materials with conventional superconductor alloys like Ti₃₄Nb₆₆ and Nb₃Sn also possess superconductivity with the critical temperature 8.9 - 15.6 K. The optimal ratio of superconductor to superhad compounds in composites varies in the range from 20:80 to 50:50 wt%. The pressure and temperature parameters of synthesis are rather high: P = 7.7 - 12.5 GPa ; T_s = 1373 - 2173 K at the heating time = 60 – 90 s. However it may be supposed that with the increase of the pressure and temperature of synthesis may be reduced substantially. The X-ray diffraction analysis revealed formation of metal carbides on the boundaries of diamond micro- and nanocrystals and nanocarbon phases originated from C₆₀ fullerene. The carbide phases provide strong chemical bonding of superconductor matrix with superhard carbon grains, thus the target composites possess very high strength. The obtained new composite materials can be successfully used in cryogenic electro-mechanical systems and in cryogenic research devices. The unique high-strength superconducting anvils for research pressure-induced apparatus were made and employed for investigations of the pressure effect up to 22 GPa on the superconductor transition temperatures in the metallic high-pressure phase of GaP.