Advances in Condensed Matter Physics

Advances in Condensed Matter Physics / 2008 / Article

Research Article | Open Access

Volume 2008 |Article ID 941372 | https://doi.org/10.1155/2008/941372

V. A. Kulbachinskii, B. M. Bulychev, V. G. Kytin, A. V. Krechetov, E. A. Konstantinova, R. A. Lunin, "Superconductivity, Electron Paramagnetic Resonance, and Raman Scattering Studies of Heterofullerides with Cs and Mg", Advances in Condensed Matter Physics, vol. 2008, Article ID 941372, 6 pages, 2008. https://doi.org/10.1155/2008/941372

Superconductivity, Electron Paramagnetic Resonance, and Raman Scattering Studies of Heterofullerides with Cs and Mg

Academic Editor: Victor Moshchalkov
Received09 Jun 2008
Accepted23 Oct 2008
Published21 Dec 2008

Abstract

In the present study, the results of investigation of physical properties of heterofullerides (A=K, Rb, Cs, M=Be, Mg, Ca, Al, Fe, Tl, ); as well as , , and are described. All of the fullerides were synthesized by the exchange reactions of alkaline fullerides with anhydrous metal halides. Superconductivity was found in and .

1. Introduction

It is well known that critical temperature of superconducting transition () of alkali-intercalated fullerides depends on the crystalline lattice parameter [1]. The value of increases with the increase in some interval of the lattice parameter a. Thus one can expect that heterofullerides with Cs may possess higher values because of larger a values, compared to fullerides with K and Rb. Fulleride , synthesized by standard gaseous method, has primitive cubic lattice and is not a superconductor. Under high pressure, is a superconductor with  K in FCC lattice as well as and . The efforts to synthesize fullerides with composition from to in a solvent (toluol) give amorphous or polymerized non-superconducting substances [2]. It is worth to note that for and fullerides, both methods produce superconductors with the same .

We showed that exchange reaction of homofullerides of K and Rb with anhydrous group 8–10 metal halides rear earth metal halides in tetrahydrofuran substitute a part of alkali metal to Ln or Fe with surviving of superconductivity [3, 4]. The open question is as follows: are these substances superconductors themselves or they are partly defected fullerides and ? To check the effectiveness of exchange reaction, we tried to synthesize by the same method the heterofullerides with Cs. The Cs fullerides under normal conditions are non-superconductors, that is why the observation of superconductivity when some atoms of Cs replaced by metal of will be an evidence of superconducting properties of heterofullerides with other not alkali metals.

2. Experimental

Toluene and tetrahydrofuran (THF) were cleared and absolutized by standard techniques. Anhydrous metal chlorides were also obtained by standard techniques; chlorides of beryllium, aluminum, and iron were synthesized by chlorination of metal by dry chlorine; chlorides of magnesium, calcium, barium, and strontium were received by thermal drying of hydrated salts with ammonium chloride in vacuum; thallium chloride was commercially available. Potassium, rubidium, and caesium fullerides were synthesized by reaction of fullerite with the stehiometric quantity of metal in the environment of toluene at 120–130 by a method described in [5].

Synthesis of the initial of alkali metal fullerides, partial removal of toluene, blending of fulleride suspension with suspension of heterometal halogenide in THF, drying of products of reaction, and their packaging in ampoules for definition of temperature of superconducting transition were carried out in vacuum in the full glass facilities equipment. In more detail, the technique is described in [4, 5]. The exchange reactions are writing as where A—K, Rb, Cs; M—Be, Mg, Ca; —Al, Fe; —Tl.

The measurements of RFA were carried out with Guinier G670 HUBER. The sample of fulleride was located in a thin-walled glass capillary which was brazed in vacuum. NMR spectra are measured by Bruker AC-200 under the one-pulse program with duration of excitation impulse 4 microseconds. Intervals between impulses was 2 seconds. For measurements of Raman spectra Perkin-Elmer Raman spectrometer with He-Ne, the laser with wavelengths of 632.7 nanometers was used. Measurements of EPR spectra were carried out on EPR spectrometer Bruker (model Elexsys 500) in the X-range with flow cryostat in temperature interval of 105–300 K. The values of g-factors were calculated based on reference line of ions in MgO .

Temperatures of superconducting transitions of fullerides were defined by standard low-frequency induction method by measuring the temperature dependence of a magnetic susceptibility in temperature interval .

3. Results and Discussion

3.1. Superconductivity

Fullerides and have superconducting transition temperature higher than others. For , the value of  = 21.7 K is the highest for fullerides with K. Fullerides with composition (M—metal, ) are non-superconductors. We found that of fullerides with composition is lower than that of (excluding , with  =21.7 K). Moreover, there is a correlation between lattice constant of these fullerides and their , namely, lattice constant of fullerides (excluding ) is smaller than lattice constant of due to smaller radii of ion substituting ion .

Superconductivity of triple heterofullerides at  = 26.4 K, at  = 21.7 K, and a heterofulleride at  = 27.2 K was discovered by investigation of temperature dependence of magnetic susceptibility. Temperature dependencies of magnetic susceptibility of these compounds are plotted in Figure 1. It should be mentioned that and transfer to superconducting state at temperatures higher than values of our previously investigated heterofullerides, synthesized by the same method. The  = 24.5 K of was maximal, that was achieved previously [4, 6]. The fulleride possesses the highest  = 21.7 K among all synthesized in the present study of heterofullerides with potassium. This confirms the suggestion that the increase of the value is due to the increase of the lattice constant caused by substitution of K and Rb by Cs. has maximal value of compared to among all superconducting heterofullerides with potassium. The same is for (). Such appreciable increase of the parameter a of FCC 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 . In Table 1, parameters of two superconducting fullerides with Cs are shown together with and for comparison.


Composition (K)a (Å) (Å)

18.514.3110(5)1.33
27.214.448(6)(+3e) 0.95
(+1e) 1.47
21.714.424(14)(+3e) 0.95
(+1e) 1.47
26.414.673(17)(+3e) 0.95
(+1e) 1.47

3.2. X-Ray Data

According to RFA, data majority of heterofullerides with Cs are amorphous. All attempts to synthesize caesium heterofullerides by interaction of homofullerides with chlorides of beryllium, magnesium, calcium, barium, aluminum, and iron on (1) and (3) lead to non-superconducting X-ray amorphous samples (Figure 2). One can see only wide peak (halo) at and peaks identified as crystalline CsCl in X-ray spectrum. As in NMR spectra of these samples, there is no resonance at 170–200 ppm, which is common for all homo- and heterofullerides with FCC lattice with freely rotating anion . We assume that caesium fullerides are not simply amorphous, but polymeric substances.

The results of interaction of with TlCl, according to (4), do not give any new information. But in reaction of thallium chloride with alkali metal heterofullerides, according to (4), obtained heterofullerides are crystalline substances (Figure 3) and superconductors.

3.3. Raman Scattering

The results of measurement and investigation of Raman scattering of fullerides , , (M=Ca, Ba) showed that these fullerides are most likely not crystalline. This is testified by the absence of nearly all characteristic fullerene phonon modes (Figure 4). The lines in Raman spectra are strongly shifted and extended compared to the lines of pure fullerite. Thus one cannot definitely identify presented lines and estimate the charge state of molecule in these compounds.

The absence of the majority of oscillatory modes observed in spectrum specifies polymerization (more rigid fixing of molecules ).

On the basis of X-ray and Raman spectra, one can conclude that fullerides and heterofullerides of caesium are polymers. This fact can explain the absence of superconductivity in these compounds because polymerization suppresses the phonon modes of molecules that mediate electron-electron attraction [7]. Besides, polymerization may cause transition to the dielectric state.

3.4. Electron Paramagnetic Resonance

In EPR spectrum of , there are two lines, the second one has higher g-factor and is much wider than the main line. Parameters of this line are shown in Table 2. Intensity of this line decreases as temperature decreases and it is not visible for . The most probably explanation of the drastically decrease of the intensity is due to transition of paramagnetic centers to the different spin states. The nature of these centers at the moment is unknown.


Composition Hpp and -factorT (K)
297200120

2.0010 0.0003
Hpp (Oe)4.85.47.3

Hpp (Oe)3.34.47.2

(wide line) 2.23352.2785
Hpp (Oe)248221

Hpp (Oe)3.72.72.1

Hpp (Oe)52.41.8

The analysis of electron paramagnetic resonance (EPR) spectra and their temperature dependence revealed the presence of at least two different types of paramagnetic centers, that is, two lines of different widths, in superconducting fullerides (A=K, Rb, M=Be, Mg)—Figure 5.

Temperature dependence of paramagnetic susceptibility (double-integrated EPR signal) of narrow line is described by Curie-Weiss law Figure 6. Therefore, the appropriate paramagnetic centers obey Bolzman statistics and probably are due to electron-charged defects like –O or –O– [8, 9]. Temperature dependence of parameters of broad line (second type of centers) is weak. This points out to the Fermi statistics of the centers of the second type, presumably they are conduction electrons [10, 11].

At the same time, EPR spectra of non-superconducting fullerides with the composition (), can be described by anisotropic signal of only one type of paramagnetic signals with Bolzman statistics, that is, defects with odd electron charge. This follows from temperature dependence of lineshape and paramagnetic susceptibility, calculated by double integration of EPR spectra. In the investigated temperature range (105 K–300 K), paramagnetic susceptibility can be well fitted by Curie-Weiss law. The extraction of the signal from conducting electrons with temperature-independent paramagnetic susceptibility for ERP spectra of these fullerides is not possible, indicating that the density of electrons is low. This fact is confirmed by the absence of superconducting transition in this fullerides.

In Figure 7, we plotted ERR spectra for fulleride. The width of the line increases while the amplitude decreases when temperature decreases, notification of ferromagnetic resonance. Some parameters of EPR signals for non-superconducting fullerides are listed in Table 2.

4. Conclusions

Exchange reactions of caesium fullerides with anhydrous metal chlorides lead to polymeric and non-superconducting phases. The exception is ternary fullerides with supposed composition of with  = 26.4 K and with  = 21.7 K. As it is known for alkali metal fullerides, depends linear on the lattice parameter a and the same linear law was found for synthesized superconducting heterofullerides.

The EPR spectra of non-superconducting fullerides with the composition (), can be described by anisotropic signal, that originate from one type of paramagnetic centers with Bolzman statistics. Most likely, these centers are odd-charged defects –O or –O–. The results of measurement and investigation of Raman scattering of fullerides , , (M=Ca, Ba) showed that these fullerides are polymers. This fact simultaneously with absence of conduction electrons can explain the non-superconducting character of these compounds because polymerization suppresses the phonon modes of molecules that mediate electron-electron attraction.

Acknowledgment

The work was supported by RFBR, Grant no. 08-03-00237-a. The measurements of EPR and Raman spectra were carried out on the equipment of the Center of Users' Facilities of Moscow State University.

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Copyright © 2008 V. A. Kulbachinskii et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.


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