• International Journal of Internet, Broadcasting and Communication
• /
• 제12권2호
• /
• pp.30-36
• /
• 2020

We demonstrated a successful fabrication of 4" Gallium Nitride (GaN)/Diamond High Electron Mobility Transistors (HEMTs) incorporated with Inner Slot Via Hole process. We made in manufacturing technology of 4" GaN/Diamond HEMT wafers in a compound semiconductor foundry since reported [1]. Wafer thickness uniformity and wafer flatness of starting GaN/Diamond wafers have improved greatly, which contributed to improved processing yield. By optimizing Laser drilling techniques, we successfully demonstrated a through-substrate-via process, which is last hurdle in GaN/Diamond manufacturing technology. To fully exploit Diamond's superior thermal property for GaN HEMT devices, we include Aluminum Nitride (AlN) barrier in epitaxial layer structure, in addition to conventional Aluminum Gallium Nitride (AlGaN) barrier layer. The current collapse revealed very stable up to Vds = 90 V. The trapping behaviors were measured Emission Microscope (EMMI). The traps are located in interface between Silicon Nitride (SiN) passivation layer and GaN cap layer.

• 한국표면공학회지
• /
• 제31권1호
• /
• pp.54-62
• /
• 1998

In this study, the behaviorof ion nitriding of AISI 304 stainless steel was investigated using plasma ion nitriding system. The characteristics of ion nitriding, and their micsoctrucyures, and physical properties were investigated as a function of process parmeteds. important conclusions can be summarzied as follows. Firstly, it was found that growth of nitride layer in ion nitriding are mainly affected by N2 partial pressures and nitriding temperatures for AISI 304 stainless steel. The $N_2$<\TEX> partial pressure plays on important role in ion nitriding since it determiness the incoming flux of nitrogen species onto specimen surface. Nitriding thmprrature is also important besauseit determines the diffusion rates of nitrogen through nitride layers. While both parameters affects the characteristics rateding are controlled by nitridingen diffusion nitration profiles of N and alloying elements such as Cr and Ni are observed through niride layers. Secondly, nitride layer consists of the upper white laywe having various nitride phases and the underneath diffusion layers. The thickness of white layer increases with $N_2$<\TEX> partial pressures and nitriding temperatures. The thinkness of diffusion layer is increasting nitriding temperatures. Finally, nitriding of stainless steels steel show slighly low their corrsionce prorerties. However, passivation properties, which is normally observed in stainless steels, were still observed aftre ion nitriding.

• 전자공학회논문지D
• /
• 제36D권10호
• /
• pp.9-16
• /
• 1999

Flash EEPROM 셀에서 기존의 ONO 구조의 IPD를 사용하면 peripheral MOSFET의 게이트 산화막을 성장할 때에 사용되는 세정 공정을 인하여 ONO 막의 상층 산화막이 식각되어 전하 보존 특성이 크게 열화되었으나 IPD 공정에 ONON 막을 사용하면 그 세정 공정시에 상층 질화막이 상층 산호막이 식각되는 것을 방지시켜 줌으로 전하보존 특성이 크게 개선되었다. ONON IPD 막을 갖고 있는 Flash EEPROM 셀의 전화 보존 특성의 모델링을 위하여 여기서는 굽는(bake) 동안의 전하 손실로 인한 문턱전압 감소의 실험식으로 ${\Delta}V_t\; = \;{\beta}t^me^{-ea/kT}$을 사용하였으며, 측정 결과 ${\beta}$=184.7, m=0.224, Ea=0.31 eV의 값을 얻었다. 이러한 0.31 eV의 활성화 에너지 값은 굽기로 인한 문턱전압의 감소가 층간 질화막 내에서의 트립된 전자들의 이동에 의한 것임을 암시하고 있다. 한편, 그 모델을 사용한 전사 모사의 결과는 굽기의 thermal budget이 낮은 경우에 실험치와 잘 일치하였으나, 반면에 높은 경우에는 측정치가 전사 모사의 결과보다 훨씬 더 크게 나타났다. 이는 thermal budge가 높은 경우에는 프로그램시에 층간 질화막 내에 트립되어 누설전류의 흐름을 차단해 주었던 전자들이 빠져나감으로 인하여 터널링에 의한 누설전류가 발생하였기 때문으로 보여졌다. 이러한 누설전류의 발생을 차단하기 위해서는 ONON 막 중에서 층간 질화막의 두께는 가능한 얇게 하고 상층 산화막의 두께는 가능한 두껍게 하는 것이 요구된다.

• ETRI Journal
• /
• 제34권6호
• /
• pp.962-965
• /
• 2012

In this letter, we propose a new RESURF stepped oxide (RSO) process to make a semi-superjunction (semi-SJ) trench double-diffused MOSFET (TDMOS). In this new process, the thick single insulation layer ($SiO_2$) of a conventional device is replaced by a multilayered insulator ($SiO_2/SiN_x/TEOS$) to improve the process and electrical properties. To compare the electrical properties of the conventional RSO TDMOS to those of the proposed TDMOS, that is, the nitride_RSO TDMOS, simulation studies are performed using a TCAD simulator. The nitride_RSO TDMOS has superior properties compared to those of the RSO TDMOS, in terms of drain current and on-resistance, owing to a high nitride permittivity. Moreover, variations in the electrical properties of the nitride_RSO TDMOS are investigated using various devices, pitch sizes, and thicknesses of the insulator. Along with an increase of the device pitch size and the thickness of the insulator, the breakdown voltage slowly improves due to a vertical field plate effect; however, the drain current and on-resistance degenerate, owing to a shrinking of the drift width. The nitride_RSO TDMOS is successfully fabricated, and the blocking voltage and specific on-resistance are 108 V and $1.1m{\Omega}cm^2$, respectively.

• 반도체디스플레이기술학회지
• /
• 제18권4호
• /
• pp.134-137
• /
• 2019

In this paper, the data retention characteristics were analyzed to find out the thickness effect on the trap energy distribution of silicon nitride in the silicon-oxide-nitride-oxide-silicon (SONOS) flash memory devices. The nitride films were prepared by low pressure chemical vapor deposition (LPCVD). The flat band voltage shift in the programmed device was measured at the elevated temperatures to observe the thermal excitation of electrons from the nitride traps in the retention mode. The trap energy distribution was extracted using the charge decay rates and the experimental results show that the portion of the shallow interface trap in the total nitride trap amount including interface and bulk trap increases as the nitride thickness decreases.

• Journal of Advanced Marine Engineering and Technology
• /
• 제24권3호
• /
• pp.43-51
• /
• 2000

The effect of time, temperature and gas composition on the case hardened thickness, hardness and nitride formation in the surface of ductile cast iron(GCD400) have been studied by micro-pulse plasma technique. Typically, external compound layer and internal diffusion layer which is much thicker than compound layer was observed in the nitride hardening of ductile cast iron. The relative amount kind of phases formed in the nitrided hardening changed with the change of nitriding conditions. Generally, only nitride phases such as $\gamma^'$($Fe_4N$), or $\varepsilon$($Fe_{2-3}N$) phases were detected in compound layer by XRD analysis. The thickness of compound layer increased with the increase of nitrogen content in the gas composition. The optimum nitriding temperature was obtained at $520^{\circ}C$. The nitrided hardening thickness parabolically with nitriding time(t) and thus, the case hardened layer(d) fits well with the typical parabolic equation ; d=kt. The material constant k for GCD400 nitrided at $520^{\circ}C$ was $0.04919\times10^3{\mu}m.hr^{-1/2}$.

• 한국전기전자재료학회논문지
• /
• 제17권3호
• /
• pp.283-288
• /
• 2004

We have fabricated MIM capacitors for MMIC applications, with capacitances as high as 600pF/$\textrm{mm}^2$ and excellent electrical properties of the insulator layer. Silicon nitride thin film is the desirable material for MMIC capacitor fabrication. Standard MIM capacitance in MMIC is 300pF/$\textrm{mm}^2$ with an insulator layer thickness of more than 2000$\AA$. However, capacitors with thin insulator layers have breakdown voltages as low as 20V. We have deposited insulator layers by PECVD in our MIM structure with an air bridge between the top metal and the contact pad. The PECVD process was optimized for fabricating the desired capacitors to be used in MMIC. Silicon nitride(Si$_{x}$N$_{y}$) thin films of about 1000$\AA$ thick show capacitances of about 600pF/$\textrm{mm}^2$, and breakdown voltages above 70V at 100nA.A.A.

• 대한기계학회:학술대회논문집
• /
• 대한기계학회 2007년도 춘계학술대회B
• /
• pp.2032-2037
• /
• 2007

Numerical analysis was conducted to investigate the atomic layer deposition(ALD) of silicon nitride using silane and ammonia as precursors. The present study simulated the surface reactions for as-deposited $Si_3N_4$ as well as the kinetics for the reactions of $SiH_4$ and $NH_3$on the semiconductor wafer. The present numerical results showed that the ALD process is dependent on the activation constant. It was also shown that the low activation constant leads to the self-limiting reaction required for the ALD process. The inlet and wafer temperatures were 473 K and 823 K, respectively. The system pressure is 2 Torr.

• 한국공작기계학회:학술대회논문집
• /
• 한국공작기계학회 1999년도 추계학술대회 논문집 - 한국공작기계학회
• /
• pp.197-203
• /
• 1999

Stainless steels in general has passive film having strong corrosion resistance on surface. Therefore it must be necessarily removed by etching in mixing solution of sulfuric and chloric acid before Nitriding treatment. But in the ion nitriding, nitride layer was easily formed because passive film was removed without difficult by sputtering effect. The removal extent of these passive films was greatly effected by gas mixing ratios and pressure and holding times of pre sputtering factors in pre sputtering stage. As a results of experiment it has been known that pre sputtering pressure and holding time was not nearly effective on the formation behavior of nitride layer. But when A/H2 gas mixing ratios was 1/2 (vol%) was the most effective of the all pre sputtering conditions. It was resulted from the combination of mechanical reaction byArgon bombardment and chemical reaction by reduction of hydrogen on the passive film.

• 한국전기전자재료학회논문지
• /
• 제18권11호
• /
• pp.1056-1060
• /
• 2005

We investigated the fabrication and characteristics of the nitride-based spin-polarized LEDs with room-temperature ferromagnetic (Ga,Mn)N layer as a spin injection source. The (Ga,Mn)N thin films having room-temperature ferromagnetic ordering were found to exhibit the negative MR and anomalous Hall resistance up to room temperature, revealing the existence of spin-polarized electrons in (Ga,Mn)N films at room temperature. The electrical characteristics in the spin LEDs did not degraded in spite of the insertion of the (Ga,Mn)N layer into the LED structure. In EL spectra of the spin LEDs, it is confirmed that the devices produce intense EL emission at 7 K as well as room temperature. These results are expected to open up new opportunities to realize room-temperature operating semiconductor spintronic devices.