2015
DOI: 10.1587/transele.e98.c.382
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Room Temperature Atomic Layer Deposition of Gallium Oxide Investigated by IR Absorption Spectroscopy

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Cited by 12 publications
(16 citation statements)
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“…The O 1s core level spectrum is well fitted with two major components at binding energies (BEs) of 530.5 and 531.6 eV for in situ Ar annealed and 530.8 and 532.1 eV for 200 W as-deposited samples. The lower BEs at 530.5 and 530.8 eV for both samples (Figure b,e) match well with the lattice oxide (in the form of O–Ga bonding state) in the Ga 2 O 3 films. ,, , Aside from this, some prior studies have attributed the additional O peaks that appear at slightly higher BEs such as 531.3 and 531.1 eV to oxygen vacancies, 532.7, 532.3, 532.0, 533.3, and 532.8 eV to hydroxyl (−OH) types of bonding state, and 533.2, 532.8, and 531.6 eV to the carbonyl type of bonding structure (in the form OC). Similar features are also seen here for these PEALD grown Ga 2 O 3 films: the subpeak at 531.6 eV for in situ Ar annealing sample (Figure b) can be assigned to oxygen vacancies, whereas the subpeak at 532.1 eV for the 200 W as-deposited film can be attributed to hydroxyl (−OH) and/or carbonyl (OC) bonding states.…”
Section: Results and Discussionsupporting
confidence: 76%
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“…The O 1s core level spectrum is well fitted with two major components at binding energies (BEs) of 530.5 and 531.6 eV for in situ Ar annealed and 530.8 and 532.1 eV for 200 W as-deposited samples. The lower BEs at 530.5 and 530.8 eV for both samples (Figure b,e) match well with the lattice oxide (in the form of O–Ga bonding state) in the Ga 2 O 3 films. ,, , Aside from this, some prior studies have attributed the additional O peaks that appear at slightly higher BEs such as 531.3 and 531.1 eV to oxygen vacancies, 532.7, 532.3, 532.0, 533.3, and 532.8 eV to hydroxyl (−OH) types of bonding state, and 533.2, 532.8, and 531.6 eV to the carbonyl type of bonding structure (in the form OC). Similar features are also seen here for these PEALD grown Ga 2 O 3 films: the subpeak at 531.6 eV for in situ Ar annealing sample (Figure b) can be assigned to oxygen vacancies, whereas the subpeak at 532.1 eV for the 200 W as-deposited film can be attributed to hydroxyl (−OH) and/or carbonyl (OC) bonding states.…”
Section: Results and Discussionsupporting
confidence: 76%
“…We propose two possible reasons behind this: (i) In our recent AlN growth efforts with the same PEALD system, we have observed that such abrupt thickness gains (kinks) arise due to plasma-induced artifacts at elevated rf powers (≥75 W). , (ii) As the rate of post-plasma thickness gains at 100 and 200 W (Figure a) appears to be more gradual rather than abrupt jumps as was the case in our previous works, , it might be that the possible ligand redeposition process still remains active slightly into early stages of the purge, whereafter it stops as no new energetic plasma species are generated and the plasma-generated (ligand) byproducts are fully pumped out. Although, there are almost no prior in-depth studies on real-time in situ dynamic growth monitoring , of ALD grown Ga 2 O 3 , in a relatively recent work, similar film thickness gains during post-plasma purge periods were observed where the authors have attributed it to the potentially trapped Ga precursor in the delivery line getting adsorbed even before their next precursor was pulsed …”
Section: Results and Discussionmentioning
confidence: 92%
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“…There are only a few literature reports of gallium oxide grown by ALD. , They mostly result in amorphous films that require high-temperature annealing to crystallize. However, there are very few reports ,,,,, of ALD growth of crystalline gallium oxide.…”
Section: Introductionmentioning
confidence: 99%