Indian Journal of Engineering & Materials Sciences Vol. 11, August 2004, pp. 353-357 Preparation and characterization of vacuum deposited magnetic polyaniline thin films† Prafull Mathura, S C K Misraa, Ram Kishoreb, U C Upretib & J L Pandeya a Engineering Materials Division, bMaterials Characterization Division National Physical Laboratory, New Delhi 110 012, India Received 24 January 2003; accepted 20 October 2003 Vacuum deposited polyaniline thin films have been found to exhibit excellent magneto-optic properties. The vacuum deposited thin films of doped polyaniline have been prepared on various substrates and their optical, electrical and magnetic characterization carried out. The thin films prepared on different substrate show a variety of surface topography and magnetic domains in crystalline phase. The crystallinity is induced by the influence of substrate on which the film is deposited. This technology establishes the feasibility of preparation of high-density disc storage magnetic recording media using vacuum deposited thin films. The advantage of these films is their magnetization at lower magnetic fields. IPC Code: Int. Cl.7 H01F 10/26 During the last few decades there is remarkable growth of interest in development of magnetic thin films for industrial and technological applications particularly as recording media. The microminiaturization has led to the development of computer equipment, surgical tools and communications pipelines shrink ever smaller, the next step in engineering is to merge biological and mechanical molecules and compounds into really, small machines. This may happen in many different ways like collection of information by fastest methods and efficient and compact storing of the information in smallest space. This can be done by miniaturizing the magnetic storage devices. Such devices can be prepared by using nano-technology using dimensions and tolerances in the range of 0.1-100 nm. This also accelerates the need of miniaturization of magnetoopto-electronic devices. This is made possible by using nano-crystalline polymeric thin films magnetic devices. The magnetic polymeric thin films have several advantages over conventional inorganic ones like ease of fabrication, low temperature processing and a very flexible metrology for preparation of film with desired properties. These films are used for magnetic gyrator for phase shifters, insulators and amplifiers, magnetic memory devices disc storage, _______________ Presented at International Workshop on Recent Advances in Nanotechnology of Magnetic Fluids, held at National Physical Laboratory, New Delhi, during 22-24 January 2003. magnetic tapes and sheets and cards. It is therefore, essential to study the magnetic properties and the details of feasibility of preparation of nano-crystalline magnetic polyaniline thin films. There have been studies on determination of magnetic susceptibility and polyaniline and its blends as in the past few years as the polymeric magnetic materials have become increasingly important in the area of information storage and magnetic recording1-8. The thin film magnetic configuration depends on various experimental factors like deposition, size, shape, structure, substrate, processing, contamination and so on. Magnetic metal doped polyaniline is emerging as a new materials for preparation of magnetic thin film for recording media. Vacuum deposited thin films are the best and preferred media for use as magnetic films. The magnetic polyaniline structure remains unchanged after vacuum evaporation due to polymerization and conjugation of the chains broken during the evaporation9-11. It has been established that polyaniline has a magnetic behaviour arising from its electronic and lattice contributions and gives rise to reasonable magnetic susceptibility, which varies with temperature. Polyaniline possesses diamagnetic susceptibility indicating the existence of free electron spins. Adding various dopants so as to enhance the magnetization of polyaniline further can modify the density of states of free electrons. This magnetic polyaniline has a potential of being used as active magnetic device in the form of powder, pellets or thin 354 INDIAN J ENG. MATER. SCI., AUGUST 2004 films. The films can be prepared by various methods for many applications. We have devised a completely dry process to prepare polyaniline thin films by vacuum evaporation of polyaniline powder onto suitable substrate. These films can be made magnetic by suitably doping the polyaniline powder during the synthesis. The preparation and study of magnetic polyaniline vacuum deposited thin films for use in magnetic data storage applications has been reported. Experimental Procedure Preparation of un-doped and Fe-doped polyaniline nano-crystalline films was done in two steps. First, preparation of polymer and preparation of polymeric magnetic film on a substrate and second, preparation of nano-crystalline polymeric thin films on suitable substrates. A copolymer of aniline and formaldehyde was prepared by dissolving 10.5 g of aniline in 12.5 mL of 10 M hydrochloric acid diluted with 11 mL distilled water. 12 mL of 25% formaldehyde solution was added to this solution, followed by addition of ferric chloride in a predetermined quality. The resultant solution was stirred for 60 min and poured into 200 mL of 5-10% NaOH solution. The precipitate obtained was filtered, washed and dried. This powder was used for preparation of polymeric films by evaporation on glass substrate under a vacuum of 10-6 mm Hg. The accurate temperature for evaporation of polyaniline powder was determined by carrying out DTA of Fe-doped polyaniline powder so as to ensure a perfect homogeneous Fe-doped uniform polyaniline thin film and also to determine the polyaniline evaporation temperature (Fig. 1). The optical characterization of vacuum deposited magnetic polyaniline thin films was carried out using Hitachi UV-3400 spectrophotometer, Mössbauer spectro-scopy, surface topography, X-ray diffraction analysis, electron spin resonance and Fig. 1⎯DTA (differential thermal analysis) of magnetic Fe-doped polyaniline electrically detected magnetic resonance were carried out. Since the thickness of the vacuum deposited films is of the order 1000Å, it was required to carry out measurements at low fields. To study the magnetic properties of a material it is essential to magnetize the polymeric thin film specimen12-14. This was done by placing the specimen film in a uniform magnetic field. The lines of magnetic flux around the film form a closed path. The cycle of magnetization of the film consisted of magnetizing and demagnetizing the specimen. For demagnetization a small steady current is passed through the solenoid in series with the specimen film. The direction of current is now reversed to complete the magnetization-demagnetization cycle. Results and Discussion Fig. 1 shows the differential thermal analysis (DTA) of polyaniline nano-crystalline magnetic thin film doped with Fe, indicating the temperature of evaporation around 288°C and at this temperature the whole of Fe-doped polyaniline nano-crystalline magnetic thin film converts into a thin film comparing of nano-crystalline composites of polyaniline nanocrystalline magnetic thin film and Fe-crystallites. This process of evaporation re-polymerization of the nano crystalline domain rich polymeric thin films. Fig. 2 shows UV-visible spectra of undoped and doped polyaniline. This spectrum shows the effect of addition of Fe on the optical characteristics. The addition of Fe in polyaniline nanocrystalline magnetic thin film induces the formation of nano-composite complex of Fe with polyaniline nano-crystalline host. Fig. 2⎯UV visible spectra of un-doped and doped polyaniline MATHUR et al.: VACUUM DEPOSITED MAGNETIC POLYANILINE THIN FILMS 355 Fig. 3⎯EDAX of polyaniline thin films Fig. 5⎯Electron diffraction of Fe-doped polyaniline nanocrystalline magnetic thin films Fig. 4⎯Surface topography of (a) un-doped and (b) doped polyaniline nano-crystalline magnetic thin films From Fig. 2, it can be seen that doping of polyaniline with Fe has remarkable effect on optical absorption spectra and position of the optical absorption peak. Doping of polyaniline thin film by Fe also induces crystallinity in the films, which is a direct evidence of magnetizable nano-crystalline domains. Fig. 3 shows the EDAX of polyaniline thin films indicating the semi-amorphous and crystalline peaks of Fe doped polyaniline nano-crystalline magnetic thin film. The surface topography of undoped and doped polyaniline nano-crystalline magnetic thin film is shown in Figs 4a and 4b. It is observed those magnetizable crystalline domains are formed after annealing of the Fe-doped thin films (Fig. 4b). The crystallinity of the Fe-doped polyaniline nano-crystalline magnetic thin film is shown in Fig. 5 (electron diffraction). These thin films are highly magnetic as shown by the B-H curve compared to a steel substrate Fig. 6. The degree of magnetization is quite high. It can be observed that due to specimen being thin film (1000 Å) sufficient magnetization is achieved at low magnetic fields. The same is confirmed by Fig. 7 showing ESR and EDMR signal from Fe-doped polyaniline nano-crystalline magnetic thin film. This signal also induces the EDMR signal that may be fitted with a Lorentzian. While the ESR signal is asymmetric as can be seen in Fig. 7, the asymmetry in the line shape can have different origins, possibly due to distribution of gfactor or spin diffusion related to a diverse conduction mechanism in polyaniline magnetic thin films due to polarons and bi-polarons. This may also give rise to typical ESR lineshapes coming from structure of guest host matrix structure arising out of Fe/ 356 INDIAN J ENG. MATER. SCI., AUGUST 2004 Fig 6⎯B-H curve of polyaniline thin films Fig. 8⎯The Mössbauer spectroscopic analysis of Fe-doped polyaniline thin films linearity in polyaniline thin films as reported earlier9. From these results it can be concluded that the spectra show presence of dopant in polyaniline thin films which further reveal complete homogenization and paramagnetic behaviour of the film. The Mössbauer spectroscopic analysis of Fe-doped polyaniline thin films were carried out and Mössbauer parameters were calculated from the graph which showed isomeric shift 0.355 mm/s with respect to ∝Fe, quadrupole splitting 0.693 mm/s and linewidth 0.505 mm/s (Fig. 8). 11 Fig. 7⎯ESR and EDMR of Fe doped polyaniline nano-crystalline magnetic thin film polyaniline complexes in otherwise semiconducting polyaniline base. EDMR signal is enhancing, i.e., Δ σ > 0, as expected for conduction in polyaniline. The EDMR signals come from the peculiarities of the process of polaron hopping via paramagnetic sites. If we assume that in a magnetic polymeric thin films, the paramagnetic states are polarons and bi-polarons, there are various types of hopping processes associated with the various energy levels occupied by the charged defects in polyaniline thin films, giving rise to the observed signals having a broad component. It is observed that for homogeneous resonance lines the linewidth of ESR/EDMR signals is inversely proportional to the spin-spin relaxation time. Thus, for the broader component the relaxation time is most probably shorter than for the narrower line. For electric fields higher than 200 V/cm the conductivity is found to increase exponentially with the electric field, which is direct evidence of non- Conclusions The feasibility of preparation of vacuum deposited magnetic nano-crystalline polyaniline thin films for device applications has been established. The optical absorption, ESR/EDMR study indicates the presence of free charge carrier in the magnetic thin films. The ESR studies and SEM study are indicative of presence of magnetizable domains in the thin films. These domains can be magnetized at low fields as indicated by B-H curve. It can be concluded that vacuum deposited polyaniline thin films hold potential for being used as active magnetic devices for a wide variety of applications including storage media, magnetic bubble memory, switching and monitoring of very small magnetic fields like those in biological specimen. Acknowledgements The authors are grateful to Prof. Vikram Kumar, Director, NPL, New Delhi for his interest in this work. MATHUR et al.: VACUUM DEPOSITED MAGNETIC POLYANILINE THIN FILMS References 1 Kahol P K, Guan H & McCormick B J, Phys Rev B, 44. (1991) 10393. 2 Ragunathan A, Kahol PK, Ho J C Chen Y Y ChaoY D, Lin Y S & Wessling B, Phys Rev B, 58 (1998) R15 955. 3 Karol P K, Phys Rev B, 62 (2000) 13803. 4 Bertram H N & Aias R, J Appl Phys, 71(7) (1992) 3439. 5 Sanders I L, Howard J K, Lambert S E & Yogi T, J Appl Phys, 65 (1989) 1234. 6 Lacroix J C, Kanazawa K K & Diaz A, J Electrochem Soc, 136 (1989) 308. 7 Tuyen Le T T, Potje Kamloth K & Liess D H, Thin Solid Films, 2492 (1997) 293. 357 8 Misra S C K, Pant R P, Pandey J L & Kumar N, J Magn Magn Mater, 252 (2002) 20. 9 Gupta R, Misra S C K & Chandra S, Appl Phys Lett, 58 (1) (1991) 51. 10 Misra S C K & Chandra S, Indian J Chem, 33 (1994) 583. 11 Pandey S S, Misra S C K, Malhotra B D & Chandra S, J Appl Pol Sci, 44 (1992) 911. 12 Wang Z H, Scherrer E M, MacDiarmid A G & Epstein A J, Phys Rev B, 45(1992) 4190. 13 Long S M, Sun Y, MacDiarmid A G & Epstein A J, Phys Rev Lett, 72 (1994) 3210. 14 Misra S C K & Chandra S, Indian J Pure & Appl Phys, 36 (1998) 391.
© Copyright 2026 Paperzz