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RESEARCH REPORT |
1 The University of Texas Health Science Center at San Antonio, Department of Restorative Dentistry, Division of Biomaterials, MSC 7890, 7703 Floyd Curl Drive, San Antonio, TX 78229-3900;
2 Kyungpook National University, College of Dentistry and Institute of Biomaterials Research and Development, Department of Dental Biomaterials, 2-101 Dongin Dong, Jung-Gu, Daegu 700-422, Korea;
3 The University of Texas at San Antonio, College of Engineering, 6900 N. Loop 1604, San Antonio, TX 78249-0619; and
4 The University of Texas Health Science Center at San Antonio, Center for Clinical Bioengineering, Department of Restorative Dentistry, Division of Biomaterials, MSC 7890, 7703 Floyd Curl Drive, San Antonio, TX 78229-3900;
*corresponding author, ong{at}uthscsa.edu
| ABSTRACT |
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KEY WORDS: calcium phosphate coating heat treatment x-ray diffraction crystallinity Fourier transform infrared spectroscopy
| INTRODUCTION |
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In addition to the coating process, extensive in vitro and in vivo research also suggested that CaP coatings are essential for early bone performance when compared with Ti implants (Overgaard et al., 1997, 1999; Ong et al., 1998, 2002; Ferraz et al., 1999; Blokhuis et al., 2000; Moroni et al., 2002; ter Brugge and Jansen, 2002). The presence of water vapor during heat treatment has been reported to affect the crystallinity of plasma-sprayed HA coatings (Cao et al., 1996; Chen et al., 1997; Tong et al., 1997). In our attempt to control the crystallinity of sputtered CaP coatings in this study, we evaluated the effects of heat treatment time and the presence of water vapor during heat treatment on the crystallinity of CaP coatings.
| MATERIALS & METHODS |
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Sputter Coating
Sputtering was performed with the use of a CMS-18 radiofrequency magnetron sputtering system (Kurt J. Lesker Company, Clairton, PA, USA) and a 4-inch-diameter sintered HA target (0.25 inches thick) bonded to a copper backing (Target Materials, Inc., Dayton, OH, USA). The base pressure in the sputtering chamber was
5 x 10-6 torr. Sputtering was accomplished with the use of a process pressure of 1.0
1.5 mbar and a power of 200 W for 7 hrs at a coating rate of 60 nm per hour. Fig. 1
displays a representative fracture surface morphology of as-sputtered CaP coatings on a slide glass substrate. The dense and continuous as-sputtered coating was observed to consist of nano-particles of approximately 5 nm in diameter and in the range of 50 to 100 nm in diameter in the subsurface and surface, respectively.
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X-ray diffraction
A D8 Advanced x-ray diffractometer (Bruker, Madison, WI, USA), equipped with a single Gobel mirror to yield a diffracted parallel beam while removing the Kß radiation, was used to characterize the structure of coatings. Using a grazing incidence attachment, a 0.35° soller slit, and a LiF (100) flat crystal monochromator to improve resolution and peak-to-background ratios, we analyzed triplicate coatings using Cu K
radiation at 40 KV and 30 mA. Triplicate coatings per treatment group were scanned from 25° to 35° 2
at a scan rate of 0.1° per min. Crystalline peak area in the 25° to 35° range was calculated, and we quantified the percent crystallinity of the coatings by correlating the crystalline peak area to the known HA crystallinity standard curve, derived by mixing various ratios of 100% crystalline and amorphous commercial HA powder (Hitemco Medical Applications, Inc., Bethpage, NY, USA).(AQ) Percent crystallinity of the coating was analyzed by ANOVA, and differences were considered significant if P < 0.05.
Fourier Transform Infrared (FTIR) Spectroscopy
Structural and molecular composition of coatings and sputtering target were evaluated by means of a model 550 Magna-IRTM FTIR (Thermo Nicolet, Madison, WI, USA). Using a resolution of 1 cm-1 and a scan number of 32, we analyzed triplicate coatings per treatment group from 400 cm-1 to 4000 cm-1. Control Ti disks were used for background collection. For the CaP coatings, data collection was performed with the use of a 80° grazing angle accessory.
| RESULTS |
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). As-sputtered coatings were observed to be amorphous, whereas heat-treated coatings were observed to exhibit an increase in coating crystallinity. Coatings after 1 hr of post-deposition heat treatment in the presence and absence of water vapor were observed to exhibit only one small crystalline peak at 32.9° (2
). The most intense peaks for CaP coatings after 2 hrs and 4 hrs of heat treatment in the presence of water vapor were observed to be at 32.9° (2
) and 25.9° (2
), respectively.
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| DISCUSSION |
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In the process of sputtering CaP coatings, plasma argon ions were produced with the use of working gas argon and were accelerated by electromagnetic field to bombard the HA target surface. It was reported that surface calcium and phosphorus atoms were bombarded off the target and initially deposited on substrates as CaP islands (Ong et al., 1991). The formation of these initial islands during sputtering had been attributed to the use of hollow cathode sources and the use of substrate rotation (Thornton and Hedgcoth, 1975). Over continuous sputtering time, CaP islands combined and formed the integrated CaP coating. The as-sputtered coatings were observed to be amorphous, indicating that the sputtering process resulted in a loss of the apatite-type structure found on the HA target. As observed in this study, heat treatments allowed CaP coatings to crystallize, forming an apatite-type structure. However, changes in the most intense peak between heat-treated CaP coatings and HA target suggested differences in structural orientation of the crystals. Poorly crystalline CaP coatings were observed after a 400°C heat treatment for 1 hr, as indicated by a peak at 32.9° (2
). This initial peak formation for poorly crystalline CaP coatings suggested that crystal growth initially began at the [300] crystal plane. The most intense peak remained at 32.9° (2
) after a two-hour heat treatment in the presence of water vapor. It was suggested from these observations that the [300] crystal plane was the preferred growth crystal plane for the initial CaP coatings heat-treated at 400°C.
In the absence of water vapor, crystallinity of the coatings increased with increasing heating time. The amorphous-to-crystalline transformation of CaP coatings at such a low temperature was suggested to be attributed to the nanostructure of as-sputtered coatings (Stupp and Braun, 1997). The presence of nanostructure in as-sputtered coatings was confirmed by SEM, showing a very dense coating consisting of nano-particles within the coatings. Similar to the parameters used for producing amorphous as-sputtered coatings, other reports have also indicated that nano-structural HA could be synthesized in ambient temperature and pressure (Stupp and Braun, 1997).
Using identical heating time, we observed coatings heated in the presence of water vapor to have a significantly higher degree of crystallinity compared with coatings heated without water vapor. This suggested that the presence of water vapor during heat treatments plays an important role in increasing CaP crystallinity. In addition, this observation was in concurrence with other reports indicating a significant increase in the crystallinity of plasma-sprayed HA coatings after heating in the presence of water vapor, as compared with HA coatings heated in air (Cao et al., 1996; Chen et al., 1997; Tong et al., 1997).
FTIR analysis of the HA target indicated the presence of OH peaks at 3572 cm-1 and PO4 peaks at 1084 cm-1, 964 cm-1, 617 cm-1, 585 cm-1, and 458 cm-1. Additional peaks observed on the HA target were 656 cm-1, 1176 cm-1, and 3647 cm-1 (Arends et al., 1987; Koutsopoulos 2002). As suggested by other investigators, the 1176 cm-1 peak was assigned to the presence of other CaP compounds and amorphous CaP, and the 3647 cm-1 peak was assigned to water molecules which replaced the OH groups bonded to Ca ions (Joris and Amberg, 1971).
An OH peak at 3572 cm-1 was observed for CaP coatings heat-treated for 2 and 4 hrs in the presence and absence of water vapor. It was reported that the OH group variation indicated different degrees of dehydroxylation as a result of HA decomposition during the coating or treatment process (Berry and Baddiel, 1976). As a result of decomposition, it was reported that HA converted to oxyhydroxyapatite, with the formula Ca10(PO4)6(OH)2-2xOx
x (
= vacancy, x < 1) (Berry and Baddiel, 1976; Tsui et al., 1998).
The PO4 peaks at 547 cm-1 and 458 cm-1 were observed in as-sputtered coatings and CaP coatings heat-treated for 1 hr in the presence and absence of water vapor. Increasing the heating time to 2 hrs in the absence of water vapor resulted in an additional PO4 peak at 573 cm-1. For coatings heat-treated for 2 hrs in the presence of water vapor and 4 hrs in the presence and absence of water vapor, additional PO4 peaks at 1084 cm-1, 964 cm-1, 617 cm-1, and 585 cm-1 were observed. The increasing number of PO4 peaks observed as a result of increasing heat treatment time or the presence and absence of water vapor was consistent with the increasing degree of coating crystallinity.
In addition to OH and PO4 peaks, other peaks at 3365 cm-1, 3735 cm-1, 1253 cm-1, 1158 cm-1, 915 cm-1, and 812 cm-1 were also observed for all CaP coatings. The peaks at 3365 cm-1 and 3735 cm-1 were suggested to be attributed to adsorbed water molecules (Joris and Amberg, 1971; Koutsopoulos, 2002), whereas the peaks at 1253 cm-1, 1158 cm-1, 915 cm-1, and 812 cm-1 were assigned to the presence of other CaP compounds, such as oxyhydroxyapatite and amorphous CaP (Tsui et al., 1998; Koutsopoulos, 2002).
| ACKNOWLEDGMENTS |
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Received February 24, 2003; Last revision July 22, 2003; Accepted July 25, 2003
| REFERENCES |
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