Heteroepitaxial Growth of Cubic AlN Thin Films on Sapphire and The Application to Underlayers for Single Crystalline Diamond Growth   

 

Hexagonal AlN (α-AlN) is a wide-gap III-V compound semiconductor possessing high thermal conductivity, chemical and thermal stability, and acoustical properties. Thus, it is a promising material for applications in optoelectronic and high-temperature microelectronics devices. On the other hand, few studies have reported on metastable cubic AlN (β-AlN). The physical properties of the cubic AlN might be different from those of α-AlN. β-AlN is expected to possess higher ballistic electron velocities, thermal conductivity, and acoustic velocity than α-AlN due to its higher crystallographic symmetry. This is interesting from the physical as well as practical viewpoints.
     β-AlN has two types of structures—the NaCl type with a lattice constant of 4.045 Å, and the zincblende type with lattice constants of 7.9131, and 4.38 Å. Two different lattice constants have been reported for the zincblende type. The epitaxial growths of zincblende-type β-AlN on Si(111), Si(001), and MgO(001) have been reported. For sapphire (0001), the epitaxial growth of β-AlN with the following relationship is expected: β-AlN(111) //sapphire(0001)[010] with lattice mismatches of 20% for the NaCl type and 17 and 30% for the zincblende types with the lattice constants of 7.913 and 4.38 Å respectively.

     We have been interested in heteroepitaxial growth of diamond on widely-usable single crystalline substrates such as MgO and sapphire. β-AlN possesses a similar crystalline structure, and it is a new candidate for an underlayer for heteroepitaxial growth of diamond thin films in my opinion. At first we will make an effort to grow β-AlN thin films heteroepitaxially on sapphire, and after that we are going to challenge to grow diamond thin films heteroepitaxially on the single crystalline β-AlN thin films.    

Our recent reports

 

"Synchrotron X-ray Diffraction Study of Single-Phase β-AlN Thin Film Heteroepitaxially Grown on a Sapphire(0001) Substrate by Pulsed Laser Deposition"

Kazushi Sumitani , Ryota Ohtani, Tomohiro Yoshida, You Nakagawa, Satoshi Mohri, and Tsuyoshi Yoshitake

Jpn. J. Appl. Phys. Vol. 49, No. 2 (2010) 020212.

 

β-AlN films grown on sapphire (0001) substrates by pulsed laser deposition were crystallographically evaluated by X-ray diffraction using synchrotron radiation at the SAGA Light Source. A θ–2θ measurement suggested that single-phase β-AlN was grown. From measurements of β-AlN 1-11 diffraction spots, it was found that β-AlN with a lattice constant of 7.90 ± 0.06 Å was heteroepitaxially grown on the substrate with a relationship of β-AlN(111)[1-21] ǁ Al2O3(0001)[11-20]. The film was composed of highly-oriented β-AlN crystallites with an average diameter of
about 100 Å.

 

 
 

Diffraction profile of the θ-2θ measurement. The peaks attributable to the film are indicated by the arrows. The sharp peaks at 2θ = 33.3 and 69.9 are 0006 and 00012 Bragg peaks from the sapphire substrate.

X-ray intensities related to AlN 1-11 diffraction spots as a
function of φ.

 

 

"Growth of metastable β-AlN by pulsed laser deposition"

Tsuyoshi YOSHITAKE , Satoshi MOHRI, Takeshi HARA, and Kunihito NAGAYAMA

Jpn. J. Appl. Phys. Vol. 47, No. 5 (2008) pp. 3600-3602.

 

Aluminum nitride (AlN) thin films were prepared on sapphire (0001) in ambient nitrogen by pulsed laser deposition using a sintered AlN target, and the film structure was evaluated by X-ray diffraction and scanning electron microscopy. The central area of the film was partially studded with cubic AlN (β-AlN) crystallites with obvious facets. This area was located on the normal of the irradiation spot on the target, and it corresponded to the region on the film where the highly energetic and dense species were deposited. A nonequilibrium condition and large supply of nitrogen are both important factors for the growth of metastable β-AlN.

 

 
 

XRD patterns of the films deposited at different nitrogen pressures.

SEM images of the film deposited at a nitrogen pressure of 40-50 mTorr.