• Journal of the Korean Institute of Telematics and Electronics D
• /
• v.36D no.4
• /
• pp.56-62
• /
• 1999

In this study, (Ba, Sr)$TiO_3$ thin films were etched with $Cl_2$/Ar gas mixing ratio in an inductively coupled plasma (ICP) by varying the etching parameter such as rf power, dc bias voltage, and chamber pressure. The etch rate was 56 nm/min under $Cl_2$/($Cl_2$+Ar) gas mixing ratio of 0.2, rf power of 600 W, dc bias voltage of 250 V, and chamber pressure of 5 mTorr. At this time, the selectivity of BST to Pt, $SiO_2$ was respectively 0.52, 0.43. The surface reaction of the etched (Ba, Sr)$TiO_3$ thin films was investigated with X-ray photoelectron spectroscopy (XPS). Ba is removed by chemical reaction between Sr and Cl to remove Sr. Ti is removed by chemical reaction such as $TiCl_4$ with ease. The results of secondary ion mass spectrometer (SIMS) analysis compared with the results of XPS analysis and the results were the same.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
• /
• 2005.11a
• /
• pp.68-69
• /
• 2005

BTO ($BaTiO_3$) thin film is one of the high dielectric materials for high-density dynamic random access memories (DRAMs) due to its relatively high dielectric constant. It is generally known that BTO film is difficult to be etched by plasma etching, but high etch rate with good selectivity to pattern mask was required. The problem of sidewall angle also still remained to be solved in plasma etching of BTO thin film. In this study, we first examined the patterning possibility of BTO film by chemical mechanical polishing (CMP) process instead of plasma etching. The sputtered BTO film on TEOS film as a stopper layer was polished by CMP process with the self-developed $BaTiO_3$- and $TiO_2$-mixed abrasives slurries (MAS), respectively. The removal rate of BTO thin film using the$ BaTiO_3$-mixed abrasive slurry ($BaTiO_3$-MAS) was higher than that using the $TiO_2$-mixed abrasive slurry ($TiO_2$-MAS) in the same concentrations. The maximum removal rate of BTO thin film was 848 nm/min with an addition of $BaTiO_3$ abrasive at the concentration of 3 wt%. The sufficient within-wafer non-uniformity (WIWNU%)below 5% was obtained in each abrasive at all concentrations. The surface morphology of polished BTO thin film was investigated by atomic force microscopy (AFM).

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
• /
• 2006.05a
• /
• pp.101-102
• /
• 2006

BTO ($BaTiO_3$) thin film is one of the high dielectric materials for high-density dynamic random access memories (DRAMs) due to its relatively high dielectric constant, It is generally known that BTO film is difficult to be etched by plasma etching, but high etch rate with good selectivity to pattern mask was required. The problem of sidewall angle also still remained to be solved in plasma etching of BTO thin film. In this study, we first examined the patterning possibility of BTO film by chemical mechanical polishing (CMP) process instead of plasma etching. The sputtered BTO film on TEOS film as a stopper layer was polished by CMP process with the sell-developed $BaTiO_3$- and $TiO_2$-mixed abrasives slurries (MAS). respectively. The removal rate of BTO thin film using the $BaTiO_3$-mixed abrasive slurry ($BaTiO_3$-MAS) was higher than that using the $TiO_2$-mixed abrasive slurry ($TiO_2$-MAS) in the same concentrations. The maximum removal rate of BTO thin film was 848 nm/min with an addition of $BaTiO_3$ abrasive at the concentration of 3 wt%.

• Transactions on Electrical and Electronic Materials
• /
• v.5 no.6
• /
• pp.223-226
• /
• 2004

The PZT thin films are one of well-known materials that has been widely studied for ferroelectric random access memory (FRAM). We etched the PZT thin films by $CF_{4}/(Cl_{2}+Ar)$ plasma and investigated improvement in etching damage by $O_{2}$ annealing. The maximum etch rate of the PZT thin films was 157 nrn/min and that the selectivity of the PZT thin films to Pt was 3.1 when $CF_{4}(30{\%})$ was added to a $Cl_{2}(80{\%})/Ar(20{\%})$ gas mixing ratio. To improve the ferroelectric properties of PZT thin films after etching, the samples were annealed for 10 min at various temperatures in $O_{2}$ atmosphere. After $O_{2}$ annealing, the remanent polarization of the asdeposited films was $34.6{\mu}/cm^{2}$ and the sample annealed at 650, 550, and $450^{\circ}C$ was 32.8, 22.3, and $18.6{\mu}/cm^{2}$, respectively. PZT thin films with $O_{2}$ annealing at $450^{\circ}C$ retained $77{\%}$ of their original polarization at 106 cycles. Also as the annealing temperature increased, the fatigue properties improved. And the leakage current was decreased gradually and almost recovered to the as-deposited value after the annealing at $450^{\circ}C$.

• Journal of the Korean Institute of Electrical and Electronic Material Engineers
• /
• v.18 no.5
• /
• pp.389-395
• /
• 2005

The etching technology of the high aspect ratio contact(HARC) is necessary at the critical contact processes of semiconductor devices. Etching the $SiO_{2}$ contact hole with the sub-micron design rule in manufacturing VLSI devices, the unexpected phenomenon of 'profile tilting' or 'bottom distortion' is often observed. This makes a short circuit between neighboring contact holes, which causes to drop seriously the device yield. As the aspect ratio of contact holes increases, the high C/F ratio gases, $C_{4}F_{6}$, $C_{4}F_{8}$ and $C_{5}F_{8}$, become widely used in order to minimize the mask layer loss during the etching process. These gases provide abundant fluorocarbon polymer as well as high selectivity to the mask layer, and the polymer with high sticking yield accumulates at the top-wall of the contact hole. During the etch process, many electrons are accumulated around the asymmetric hole mouth to distort the electric field, and this distorts the ion trajectory arriving at the hole bottom. These ions with the distorted trajectory induce the deformation of the hole bottom, which is called 'profile tilting' or 'bottom distortion'. To prevent this phenomenon, three methods are suggested here. 1) Using lower C/F ratio gases, $CF_{4}$ or $C_{3}F_{8}$, the amount of the Polymer at the hole mouth is reduced to minimize the asymmetry of the hole top. 2) The number of the neighboring holes with equal distance is maximized to get the more symmetry of the oxygen distribution around the hole. 3) The dual frequency plasma source is used to release the excessive charge build-up at the hole mouth. From the suggested methods, we have obtained the nearly circular hole bottom, which Implies that the ion trajectory Incident on the hole bottom is symmetry.

• Proceedings of the Materials Research Society of Korea Conference
• /
• 2009.05a
• /
• pp.26.2-26.2
• /
• 2009

이 논문은 반응성 $BCl_3$ 플라즈마로 GaAs의 건식 식각을 진행한 후 그 결과에 대하여 연구 분석 한 것이다. 이 때 사용한 식각 공정 변수는 $BCl_3$ 플라즈마에서의 가스유량, 공정 압력과 RIE 척 파워의 변화이다. 먼저 공정 압력을 75 mTorr 고정시킨 후 $BCl_3$ 유량을 변화 (2.5~10 sccm)해서 실험하였다. 또한 BCl3의 유량을 5 sccm으로 고정시킨 후 공정압력을 변화(47~180 mTorr)해서 식각 실험을 실시하였다. 마지막으로 47 mTorr와 100 mTorr 의 각각의 공정압력에서 RF 척 파워를 변화시켜 (50~200 W) 실험하였다. GaAs 플라즈마 식각이 끝난 후 표면단차 측정기 (Surface profiler)를 사용하여 표면의 단차와 거칠기를 분석하였다. 그 후 그 결과를 이용하여 식각율 (Etch rate), 식각 표면 거칠기 (RMS roughness), 식각 선택비 (Selectivity) 등의 식각 특성평가를 하였다. 또한 식각 공정 중에 샘플 척에 발생하는 자기 바이어스와 $BCl_3$ 플라즈마 가스를 광학 발광 분석기 (Optical Emission Spectroscopy)를 이용하여 플라즈마의 상태를 실시간으로 분석하였다. 이 실험 결과에 따르면 공정 압력의 증가는 샘플 척의 자기 바이어스의 값을 감소시켰다. $BCl_3$ 압력 변화에 의한 GaAs의 식각 결과를 정리하면 5 sccm의 $BCl_3$ 가스유량과 RF 척 파워를 100 W로 고정시켰을 때 식각율은 47 mTorr에서 가장 높았으며, 그 값은 $0.42{\mu}m/min$ 이었다. GaAs의 식각 속도는 공정압력이 증가할수록 감소하였으며 180 mTorr에서는 식각율이 $0.03{\mu}m/min$로 거의 식각되지 않았다. 또한 공정압력을 75 mTorr, RF 척 파워를 100 W로 고정시키고, $BCl_3$ 가스유량을 2.5 sccm에서 10 sccm까지 변화시켰을 때, 10 sccm 의 $BCl_3$ 가스유량에서 가장 높은 식각율인 $0.87{\mu}m/min$이 측정되었다. 압력에 따른 GaAs의 식각 후 표면 거칠기는 최대 2 nm 정도로 비교적 매끈하였으며, 거의 식각되지 않은 180mTorr의 조건에서는 약 1 nm로 낮아졌다. 본 실험 조건에서 GaAs의 감광제에 대한 식각 선택비는 최대 약 3:1 이내였다.

• Proceedings of the Materials Research Society of Korea Conference
• /
• 2009.05a
• /
• pp.39.1-39.1
• /
• 2009

본 실험은 연성과 광 투명도가 뛰어난 아크릴 (PMMA) 과 폴리카보네이트 (Polycabonate) 기판의 축전 결합형 플라즈마 (CCP) 건식 식각 연구에 관한 것이다. 특히 식각 반응기 내부의 압력 변화에 따른 두 기판의 건식 식각 특성 분석에 초점을 맞추었다. 실험에 사용된 기판은 두께 1mm의 아크릴 (PMMA) 과 폴리카보네이트 (Polycabonate)를 $1.5\times1.5\;cm^2$로 절단하여 Photo-lithography 공정을 통하여 감광제 (Photo-resist)로 패턴하였다. 식각 반응기 내부에 패턴 된 아크릴(PMMA) 과 폴리카보네이트 (Polycabonate)를 넣은 후 반응기 내부 진공 상태로 만들었다. 그 후 5 sccm $O_2$ 가스를 유량조절기 (Mass flow controller)를 통하여 식각 반응기 내부로 유입하여 실험을 하였다. 이때 식각 공정 변수는 식각 반응기 내부 압력과 샘플 척 파워이다. 특성평가 항목은 식각 후 기판 (Substrate)의 식각율 (Etch rate), 식각 선택비 (Selectivity) 그리고 기판 표면 거칠기 (RMS roughness)이다. 실험 결과는 표면 단차 분석기(Surface profiler)를 이용하여 기판 (Substrate)의 표면을 분석 하였다. 또한 OES (Optical Emission Spectroscopy) 를 이용하여 식각 중 내부 플라즈마의 상태를 분석하였다. 본 실험 결과에 따르면 5 sccm $O_2$ 가스와 100 W 척 파워를 고정한 후 반응기 내부의 압력을 25 mTorr에서 180 mTorr까지 변화시켜 실험한 결과 40 mTorr의 반응기 내부 압력에서 실험 자료 중 가장 높은 식각율로 아크릴 (PMMA)은 $0.46\;{\mu}m/min$, 폴리카보네이트 (Polycabonate)는 $0.28\;{\mu}m/min$의 결과를 얻었다. 또한 이 자료를 바탕으로 5 sccm $O_2$ 가스와 반응기 내부 압력을 40 mTorr로 고정시키고 RIE 척 파워를 25 W에서 150 W로 증가시켰을 때 아크릴 (PMMA)의 식각율은 $0.15\;{\mu}m/min$에서 $0.72\;{\mu}m/min$까지 증가하였고, 폴리카보네이트 (Polycabonate) 의 식각율은 $0.1\;{\mu}m/min$에서 $0.36\;{\mu}m/min$까지 증가하였다.

• Journal of the Korean Vacuum Society
• /
• v.7 no.4
• /
• pp.374-380
• /
• 1998

Radical and ion densities in a $CF_4$plasma have been calculated as a function of input power density, gas pressure and feed gas flow rate using simple 0 dimensional global model. Fluorine atom is found to be the most abundant neutral particle. Highly fragmented species such as CF and $CF^+$ become dominant neutral and ionic radical at the high power condition. As the pressure increase, ion density increases but ionization rate decreases due to the decrease in electron temperature. The fractional dissociation of $CF_4$feed gas decreases with pressure after increasing at the low pressure range. Electron density and temperature are almost independent of flow rate within calculation conditions studied. The fractional dissociation of $CF_4$monotonically decreases with flow rate, which results in increase in $CF_3$and decrease in CF density. The calculation results show that the $SiO_2$etch selectivity improvement correlates to the increase in the relative density of fluorocarbon ion and neutral radicals which has high C/F ratio.

• Journal of Sensor Science and Technology
• /
• v.8 no.3
• /
• pp.291-297
• /
• 1999

The plasma etching of tungsten thin films has been studied with $SF_6$ gas in RIE system. The etch rate of ${\alpha}$-phase W film with $SF_6$ gas plasma has been showed to depend strongly on process parameters ($SF_6$, $SF_6-N_2$ gas). Effect of $N_2$ addition and etching selectivity between W film and photoresist have also been studied in detail. Etching profiles between W film and photoresist were investigated by SEM. The compounds on W surface after $SF_6-N_2$ gas plasma treatment were examined by XPS and the concentration of F ions was detected by OES during plasma on.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
• /
• 2007.06a
• /
• pp.85-85
• /
• 2007

최근 귀금속중의 하나인 Ruthenium(Ru)은 높은 일함수, 누설전류에 대한 높은 저항성등의 톡성으로 인해 캐패시터의 하부전극으로 각광받고 있다. 하부전극으로 증착된 Ru은 일반적으로 각 캐패시터의 분리와 평탄화를 위해 건식식각이 이루어진다. 하지만, 건식식각 공정중 유독한 $RUO_4$ 가스가 발생할 수 있으며, 불균일한 캐패시터 표면을 유발할 수 있다. 이러한 문제점들을 해결하기 위해 CMP 공정이 필요하게 되었다. 하지만, Ru은 화학적으로 매우 안정하기 때문에 Ru CMP 슬러리에 대한 연구가 필요하게 되었으며, 이에 대한 연구가 활발히 진행되고 있다. 본 연구에서는 Ru CMP 공정에서 Chemical A가 에칭제 및 산화제로 사용된 슬러리의 pH 변화와 pH 적정제에 따른 영향을 살펴보았다. Ru wafer를 이용하여 static etch rate, passivation film thickness와 wettability를 pH와 pH 적정제에 따라 비교해 보았다. 또한, pH 적정제로 $NH_4OH$와 TMAH를 이용하여 pH별 슬러리를 제작하고 CMP 공정을 실시하여 Ru의 removal rate을 측정하였다. $NH_4OH$와 TMAH의 경우 각각 130. 100 nm/min의 연마율이 측정된 pH 6에서 가장 높은 연마률을 보였으며, TMAH의 경우가 pH 전 구간에서 $NH_4OH$에 비해 낮은 연마율이 측정되었다. TEOS 에 대한 Ru의 선택비를 측정해 본 결과, $NH_4OH$의 경우 pH 8~9. TMAH의 경우 pH 6~7에서 높은 selectivity를 얻을 수 있었다.