The role of Un-Balanced Magnetron sputtering on the characteristics of Tin dioxide thin-film
Sputtering was first introduced in 1852 and was used by a person named Groe. He could using an electrical discharge deposited the metal film on a cold cathode. At first, sputtering was used for deposition of the refractory metals film, whose deposition was not possible by thermal evaporation, but gradually, using radio frequency waves (RF), the possibility of dielectric films was also provided by the Suturing deposition method.
Spotting is in fact the process of transferring the momentum of the particles (usually the ions of neutral gases) to the surface of the target. Parameters such as energy, angles and masses of the incident particles, as well as the binding energy between atoms, affect its efficiency. The contacting ions with the target surface are either absorbed by or reflected. As the energy increases, ions penetrate into the target material atomic network and begin to degrade the surface. When the amount of energy reaches the threshold, the atoms begin to drop off the surface.
The minimum energy required to throw an atom from the target material’s surface is the amount of energy that it refers to as primary energy. Usually, the initial energy value is about 3 to 4 times greater than the binding energy between the surface target atoms.
By creating the potential difference between the cathode (where the target material is placed) and the anode (which is actually the wall of the chamber and the substrate attached to the electrically ground), the neutral gas in the chamber (i.e. argon) is ionized and the plasma is ignited.
The generated ions accelerate towards the cathode, which is located at a negative potential. If the energy transferred from the incident ions to the surface of the target material (which is located in the cathode) is greater than the initial energy, the removed atoms collide with other atoms and the energy is cascaded. The atoms removed from the material’s surface after a few collisions, reach the substrate with their remaining energy.
If the sputtering process uses a magnetic field to control the motion of the electrons, then it is called Magnetron Spattering. This field is created by magnets with different shape and sizes placed behind the cathode. By this magnetic field, secondary electrons can be trapped near the surface of the target material which causes ionization of argon atoms prior to re-absorption. This causes the formation of plasma at lower pressures and plasma stability.
The use of Magnetron Sputtering is done in two ways that relates to the configuration of the magnets. The usual balanced magnetron sputtering and another is un-balanced magnetron sputtering. In an unbalanced Magnetron sputtering, the plasma is also pulled up into the substrate, and argon ions also bombard the growing thin film.
Magnetron sputtering devices use a bipolar structure to trap electrons around the cathode. Bipolar not only allow for low discharge (less than 10-2 mbar) of, but also improve the rate of excitation and ionization. This dipole is created using rows of permanent magnets. The placement of magnets is such that the S-N-S or N-S-N combinations are formed and the central magnetism (internal) has the opposite polarity of the two other rows. Usually, external magnets are mounted on iron rings. If all the magnets have the same power, all the field lines out of the external magnets pass through the central magnet. This configuration, called “Balanced Magnetron Sputtering” which in that the electrons cannot escape from the magnetic field, and as a result, the plasma remains only around the cathode [1, 2].
On the other hand, if only the center magnets are week, all the magnetic field lines will not be caught up by center magnet and the shape of the resultant magnetic field will change allowing some of the electrons from plasma to escape easily towards the substrate, and this condition of magnetron arrangement is called unbalanced magnetron sputtering. The presence of electrons around the substrate leads to the ionization of neutral gas atoms and the penetration of plasma into this region. High-energy ions bombarded the substrate, which increases the quality of the growing thin film.
Indian researchers have succeeded in improving the optical, electrical, and structural properties of tin dioxide thin-film by investigation the effect of using un-balanced magnetron sputtering on the properties of tin dioxide thin film.
Tin dioxide (SnO2), has received significant attention due to its potential utility in various practical applications such as conductive electrodes and transparent coatings, heterojunction solar cells, optoelectronic devices, gas sensors, and thin film transistors, etc. . Since the characteristics of the thin films depend on the conditions of the deposition and deposition methods, a lot of studies have been done on the deposition of the material, so that it can be used optimally.
Studies of this research group have been done on a thin film of tin dioxide deposited on a silicon substrate using an unbalanced RF Magnetron Sputtering method.
According to the results of these studies, the crystallographic structure of the deposited thin-film tend to have random orientation with intense (110), (101), (211) peaks and a very low intensity (200) and (111) peaks. As the power increased to 200W the films showed a dominant (101) orientation in comparison to other peaks, indicating that it is possible to obtain highly oriented SnO2 thin films simply by tailoring the applied RF power
The XRD results confirm that the thin film deposited by the un-balanced Magnetron sputtering method in terms of crystalline properties in all RF power range has a better quality than the thin film deposited by the conventional balanced Magnetron Sputtering method. This effect is due to the re-crystallization of the thin film during the ion bombardment.
The C-V curves shows that the hysteresis effect for thin films deposited by the both balanced and un-balanced Magnetron Sputtering at the frequency of 1 MHz in all applied power range. In the C-V curve of the thin film deposited by the balanced Magnetron Sputtering, the hysteresis effect reduces by increasing the applied power. On the other hand, for the thin film deposited by the un-balanced Magnetron sputtering, the effect of hysteresis increases with the increase of applied power. In this case there is a counter clockwise shift of C-V curve with a huge flat band shift of about 3 V for the films deposited at 250 W, indicating that it can act as electron trapping and de-trapping memory device.
The overall observed C-V behavior in both UBM and BM sputtering can be attributed to the formation/curing of different traps in the growing films during the physical bombardment of growing film by energetic.
To find out more about the results of this research, see the link below.
- B. Window, N. Savvides, J. Vac. Sci. Technol. A 4 (1986) 196.
- Gauri Shanker, P. Prathap, K.M.K. Srivatsa, Preetam Singh- Effect of balanced and unbalanced magnetron sputtering processes on the properties of SnO2 thin films, Current Applied Physics, 19 (2019) 697–703.
- A.M. Gheidari, E.A. Soleimani, M. Mansorhoseini, S. Mohajerzadeh, N. Madani W. Shams-Kolahi, Mater. Res. Bull. 40 (2005) 1303.