BCl3/N2 Plasma for Advanced non-Si Gate Patterning

2006 ◽  
Vol 913 ◽  
Author(s):  
Denis Shamiryan ◽  
Vasile Paraschiv ◽  
Salvador Eslava-Fernandez ◽  
Marc Demand ◽  
Mikhail Baklanov ◽  
...  

AbstractAs conventional materials in CMOS manufacturing, Si as a gate material and SiO2 as a gate dielectric, approach their performance limit, the search for new materials becomes key point. Patterning of the new stacks containing these materials require both new plasma etch chemistries and new approaches.We propose a BCl3/N2 based plasma mixture for the advanced gate patterning (in this case pure Ge gates and TaN metal gates). There are three reasons to select this combination:a) The gas mixture generates Cl* species able to etch a diversity of materials, b) it is selective towards Si due to formation of passivating Si-B bonds and c) it improves profile control possibly by formation of a passivating BN-like film on feature side walls. It was found that BCl3 in presence of N2 results in a film deposition if no bias is applied to the substrate (i.e. there is no ion bombardment). The film is hexagonal BN-like since the characteristic peaks corresponding to the in-plane B-N and out-of-plane B-N-B bonds were found in FTIR spectra. The composition of the film surface as found by XPS is B, N and O (as no O2 is present in the plasma it may be a result of oxidation in the atmosphere), the amount of Cl is approx. 1%. The film is soluble in water that makes its removal easy. The deposition rate can be as high as 300 nm/min depending on plasma power, pressure, flow rates and BCl3 to N2 ratio.We propose to use the BCl3/N2 mixture to etch materials too sensitive to Cl-based plasma. Pure BCl3 plasma might distort gate profiles, as materials are etched in a lateral direction as well, this is the case, e.g. for pure Ge gates. Addition of small amount of nitrogen (5% to 10%) to the BCl3 plasma preserves the vertical profile, apparently by the formation of a passivating BN-like layer on the vertical surfaces where there is no ion bombardment. Too high nitrogen concentration results in positively sloped gate profile or even in the etch stop that could be attributed to the too high deposition rate that exceeds the etch rate. All experiments have been performed in Lam Versys 2300 etch chamber.

2018 ◽  
Vol 781 ◽  
pp. 8-13 ◽  
Author(s):  
Mariya Makarova ◽  
Konstantin Moiseev ◽  
Alexander Nazarenko ◽  
Petr Luchnikov ◽  
Galina Dalskaya ◽  
...  

Technological features of obtaining of tin films in a vacuum by liquid-phase target magnetron sputtering were reviewed. With high deposition rate the white color tin coating with amorphous structure is formed on the substrate. X-ray microanalysis of the obtained tin films showed the presence of micro-and nanoparticles of an impurity of the crucible material in the structure of the films. The use of the tantalum crucible with liquid-phase target magnetron sputtering with deposition rate of 3.2 μm / min allows obtaining ultra-pure, continuous, homogeneous tin film on a stationary substrate without impurity material of the crucible.


1990 ◽  
Vol 182 ◽  
Author(s):  
Shih-Chang Chen ◽  
Akihiro Sakamoto ◽  
Hiroyuki Tamura ◽  
Masaki Yoshimaru ◽  
Masayoshi Ino

AbstractTitanium silicide (TiSix), used as polycide gate consists of TiSi1.1 and amorphous silicon (a—Si), was deposited by Plasma Enhanced Chemical Vapor Deposition method (PE—CVD). The effect of a—Si layer in PE—CVD Ti polycide gate dielectrics has been studied. In order to evaluate the a—Si layer effect, three types of samples were prepared on gate SiO2 film with following structures: a) a—Si / TiSil.1 / a—Si / phosphorus (P) doped poly—Si, b) a—Si / TiSi1.1 / non—doped poly—Si / P doped poly—Si and c) a—Si / TiSi1.1 / P doped poly—Si, respectively. Furthermore, in order to avoid the influence of native oxide existence at the interface, the pre—cleaning treatment was performed in—situ on the poly—Si film surface before TiSi1.1 film deposition. The gate dielectric strengths of these samples indicate that the gate dielectric degradation in PE—CVD Ti polycide gate is greatly dependent on Si under layer crystallization. It is effective using a—Si film as the under layer in decreasing the gate dielectric degradation. This is due to the Ti oxide interlayer, formed at the interface of TiSi2.0 and poly—Si films, whichrestrains the TiSix local penetration.


2011 ◽  
Vol 1339 ◽  
Author(s):  
E.V. Johnson ◽  
S. Pouliquen ◽  
P.A. Delattre ◽  
J.P. Booth

ABSTRACTThe use of Voltage Waveform Tailoring (VWT) – that is the use of non-sinusoidal waveforms with a period equivalent to RF frequencies – is shown to be effective in modifying the electric field distribution in a parallel plate, capacitively coupled laboratory plasma deposition reactor, and thus in changing the growth mode of silicon thin films from amorphous to nanocrystalline. The use of the VWT technique allows one to decouple the power injected into the plasma from the ion-bombardment energy at the film surface without changing any other deposition parameters, such as pressure or gas mixture. Material results are presented for an H2/SiH4 gas composition. A “peaks” type waveform increases the ion-bombardment energy at the RF electrode and reduces it at the substrate, resulting in more nanocrystalline growth. The use of a “valleys”-type waveform has the opposite effect, and results in more amorphous growth. We show the dependence of the process on silane dilution and pressure, including results on changes to the deposition rate when changing the excitation voltage waveform.


Coatings ◽  
2020 ◽  
Vol 10 (4) ◽  
pp. 331
Author(s):  
Chang Weon Song ◽  
Dae Seung Cho ◽  
Jae Myung Lee ◽  
Pung Keun Song

Diamond coating using hot-filament chemical vapor deposition (HFCVD) is now widely used in many fields. The quality of the diamond film and many factors determine the success of the coating, such as temperature, time, and pressure during coating. The purpose of this study was to produce coated boron-doped diamond (BDD) films by doping boron in the diamond film and to assess them through comparative analysis with foreign acid BDD, which is widely used as a water-treatment electrode in the present industry. The bending of the titanium substrate due to the high temperature during the diamond deposition was avoided by adding an intermediate layer with a columnar structure to niobium film. The filament temperature and pressure were determined through preliminary experiments, and BDD films were coated. The BDD film deposition rate was confirmed to be 100 nm/h, and the potential window increased with increasing thickness. The electrochemical activation and catalytic performance were confirmed according to the surface characteristics. Although the high deposition rate of the BDD coating is also an important factor, it was confirmed that conducting coating so that amorphous carbonization does not occur by controlling the temperature during coating can improve the electrochemical properties of BDD film.


1990 ◽  
Vol 181 ◽  
Author(s):  
Shih-Chang Chen ◽  
Akihiro Sakamoto ◽  
Hiroyuki Tamura ◽  
Masaki Yoshimaru ◽  
Masayoshi Ino

ABSTRACTTitanium silicide (TiSix), used as polycide gate consists of TiSi1.1 and amorphous silicon (a-Si), was deposited by Plasma Enhanced Chemical Vapor Deposition method (PE-CVD). The effect of a-Si layer in PE-CVD Ti polycide gate dielectrics has been studied. In order to evaluate the a-Si layer effect, three types of samples were prepared on gate SiO2 film with following structures : a) a-Si / TiSi-1.1 / a-Si / phosphorus (P) doped poly-Si, b) a-Si / TiSi-1.1 / non-doped poly-Si / P doped poly-Si and c) a-Si / TiSi1.1 / P doped poly-Si, respectively. Furthermore, in order to avoid the influence of native oxide existence at the interface, the pre-cleaning treatment was performed in-situ on the poly-Si film surface before TiSi1.1 film deposition. The gate dielectric strengths of these samples indicate that the gate dielectric degradation in PE-CVD Ti polycide gate is greatly dependent on Si under layer crystallization. It is effective using a-Si film as the under layer in decreasing the gate dielectric degradation . This is due to the Ti oxide interlayer, formed at the interface of TiSi2.0 and poly-Si films, which restrains the TiSix local penetration.


1989 ◽  
Vol 149 ◽  
Author(s):  
Y. H. Shing ◽  
C. L. Yang ◽  
C. E. Allevato ◽  
F. S. Pool

ABSTRACTAmorphous silicon (a-Si:H) and amorphous carbon (a-C:H) films have been deposited by electron cyclotron resonance (ECR) microwave plasma enhanced CVD. A high deposition rate of ˜ 25 Å/sec and a light-to-dark conductivity ratio of 1 × 105 for a- Si:H films have been achieved by the ECR process using a pure silane plasma. ECR microwave plasmas have been analyzed by in situ optical emission spectroscopy (OES) and have shown a strong H * emission at 434 nm indicating higher chemical reactivity than RF plasmas. The linear correlation between the film deposition rate and the SiH* emission intensity of ECR silane plasma suggests that SiH* species are related to the neutral radicals which are responsible for the a-Si:H film deposition. Hard and soft a-C:H films have been deposited by ECR with and without RF bias power, respectively. The RF bias to the substrate is found to play a critical role in determining the film structure and the carbon bonding configuration of ECR deposited a-C:H films. Raman spectra of these films indicate that ECR deposition conditions can be optimized to produce diamond films.


1999 ◽  
Vol 14 (4) ◽  
pp. 1204-1211 ◽  
Author(s):  
X. F. Zhang ◽  
H. H. Kung ◽  
S. R. Foltyn ◽  
Q. X. Jia ◽  
E. J. Peterson ◽  
...  

Two very different pulsed laser deposition rates, 192 and 6 Å/s, were used to produce 1 μm thick superconducting YBa2Cu3Ox (YBCO) films on (001) SrTiO3 single-crystal substrates at 790 °C. Transmission electron microscopy (TEM) was used to characterize and compare microstructures between the two films. It has been found that the high deposition rate led to a slight deviation from the expected epitaxial orientations, and extra stress was induced in the films by increased lattice mismatch between the films and the substrates. In addition, misoriented YBCO grains were formed in the high-rate films after a thickness of about 150 nm. Postannealing in oxygen had no visible influence on these defects, although superconducting properties were improved significantly. In contrast to the high-rate films, overall epitaxial orientations have been formed in the low-rate films, and no misoriented YBCO grains were found. However, variations in lattice parameters and columnar voids were observed, although their existence apparently does not have considerable influence on superconducting current density (Jc). Cation disorder was observed in both films. A two-step film growth mechanism is concluded which is responsible for the formation of some defects in the high-deposition rate films.


1999 ◽  
Vol 567 ◽  
Author(s):  
Renee Nieh ◽  
Wen-Jie Qi ◽  
Yongjoo Jeon ◽  
Byoung Hun Lee ◽  
Aaron Lucas ◽  
...  

ABSTRACTBa0.5Sr0.5TiO3 (BST) is one of the high-k candidates for replacing SiO2 as the gate dielectric in future generation devices. The biggest obstacle to scaling the equivalent oxide thickness (EOT) of BST is an interfacial layer, SixOy, which forms between BST and Si. Nitrogen (N2) implantation into the Si substrate has been proposed to reduce the growth of this interfacial layer. In this study, capacitors (Pt/BST/Si) were fabricated by depositing thin BST films (50Å) onto N2 implanted Si in order to evaluate the effects of implant dose and annealing conditions on EOT. It was found that N2 implantation reduced the EOT of RF magnetron sputtered and Metal Oxide Chemical Vapor Deposition (MOCVD) BST films by ∼20% and ∼33%, respectively. For sputtered BST, an implant dose of 1×1014cm−;2 provided sufficient nitrogen concentration without residual implant damage after annealing. X-ray photoelectron spectroscopy data confirmed that the reduction in EOT is due to a reduction in the interfacial layer growth. X-ray diffraction spectra revealed typical polycrystalline structure with (111) and (200) preferential orientations for both films. Leakage for these 50Å BST films is on the order of 10−8 to 10−5 A/cm2—lower than oxynitrides with comparable EOTs.


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