AVS 62nd International Symposium & Exhibition | |
Plasma Science and Technology | Thursday Sessions |
Session PS-ThP |
Session: | Plasma Science and Technology Poster Session |
Presenter: | Takeshi Kitajima, National Defense Academy of Japan |
Authors: | T. Kitajima, National Defense Academy of Japan T. Nakano, National Defense Academy of Japan |
Correspondent: | Click to Email |
Hexagonal Boron Nitride (h-BN) is interested because of its similar 2 dimensional crystal feature to Graphene.
The stack of h-BN with Graphene has less lattice mismatch compared to the other dielectric materials.
Mechanical exfoliation and stacking of h-BN with Graphene is examined and presented a novel transistor characteristics1. Chemical vapor deposition schemes are desired for the future mass production of the devices.
CVD growth of h-BN film on Cu or Ni is shown by several groups using Borazine as the source of BN under high temperature atomospheric conditions2.
In this study, we introduced a new plasma induced chemical transport technique3 of Borazine to the growth of h-BN for expanding the process window.
The experimental apparatus of the plasma chemical transport consists of the growth chamber and the plasma chamber (Fig.1). The growth chamber has a manipulator with a Mo sample heater. The plasma chamber has inner type 9 turn coil for inductive coupling of 100 MHz RF power. On the side of the coil, Borazine powder is placed to be vaporized by the hydrogen plasma exposure. The pressure of the plasma is 30 Pa. The Borazine vapor and the hydrogen radicals are transported to the growth chamber through 2 mm orifice which suppresses the ion exposure to the sample surface. The growth temperature ranges 560C to 1000C.
The optical microscope image of the film (Fig.2) shows the BN related clusters are locally produced on 560C sample while 1000C sample shows many graphene patches generated from excess carbons from the plasma source. The atomic concentration of the sample (Fig.3) shows the B and N concentration is highest (16 and 12 %) at 560C, and decreases to 3 and 2 % at 730C. Therefore, BN precursors can deposit on Cu surface only at lower sample temperature. This is also confirmed by the Atomic Force Microscope image of the sample (Fig.4). The image shows the 560C sample is covered with BN related polymer islands about a few tens of nm in width. The islands disappear as the growth temperature increases and the terrace of the Cu is emphasized.
The results show that BN growth on Cu with low pressure plasma induced chemical transport of Borazine is only possible at relatively low sample temperature. The 2 dimensional BN film growth is required to start from the BN polymer growth at lower temperature. We expect the BN polymer should be annealed at higher temperature around 1000C and be converted to 2 dimensional atomic layer.
1. I. Meric, et.al.IEDM, (2010) 23.2
2. S. Yumeng, et.al. Nano Letters 10, 4134 (2010)
3. H. Ohmi et al., J. Appl. Phys. 102, 023302 (2007)