Material Properties of GaAs-on-Si and Fabrication of Digital Integrated Circuits

1988 ◽  
Vol 116 ◽  
Author(s):  
N. Clhand ◽  
F. Ren ◽  
S. N. G. Chu ◽  
A. M. Sergent ◽  
T. Boone ◽  
...  

AbstractWe have found that the surface morphology of GaAs grown on Si by MBE is smoother at lower growth temperatures (<500° C), but that the crystalline properties improve at higher growth temperatures (575-600°C). After thermal annealing at 850°C for 15 rai the TEM plan-views indicate that the dislocation density on the surface is reduced by a factor of 4 only. However, the TEM cross-sections indicate a much larger reduction of dislocations in highly dislocated regions near the GaAs/Si interface. Dislocations which are loops or tangles tend to shrink and clean up after annealing leaving a larger volume of GaAs free from, or with fewer, dislocations. The density of electron deep levels reduces with increasing thickness. Electron traps M1, M3 and M4 are not seen when a high purity As is used. For high device performance, the GaAs buffer layer thickness should be at least 2 µm. Although the wafer warpage increases from 7 µm to 52 µm as the GaAs thickness increases from 1.2 µm to 4.2 µm on 7.5 cm wafers, the wafers are as fiat as the original Si wafers under vacuum clamping. Wafer warpage reduced significantly when GaAs was grown selectively through a Si shadow mask. For 1 µm gate MESFET's, σvT was 65 mV on a 3.5 × 3 cm2 wafer area with gmax = 153 mS/ram. A minimum propagation delay of 52 ps/stage at a power dissipation of 1.3 mW/gate was measured for the 19 stage DCFL ring oscillators with 40= yield. Conductivity of the Si substrate and GaAs buffer layer posed no problem in channel isolation. The divide-by-two circuits performed the frequency dividing operation up to 1.8 GHz. The study shows that GaAs-on-Si has a great potential for digital IC's.

2015 ◽  
Vol 24 (07) ◽  
pp. 1550094 ◽  
Author(s):  
Jizhong Shen ◽  
Liang Geng ◽  
Xuexiang Wu

Flip-flop is an important unit in digital integrated circuits, whose characteristics have a deep impact on the performance of the circuits. To reduce the power dissipation of flip-flops, clock triggering edge control technique is proposed, which is feasible to block one or two triggering edges of a clock cycle if they are redundant in dual-edge pulse-triggered flip-flops (DEPFFs). Based on this technique, redundant pulses can be suppressed when the input stays unchanged, and all the redundant triggerings are eliminated to reduce redundant transitions at the internal nodes of the flip-flop, so the power dissipation can be decreased. Then a novel DEPFF based on clock triggering edge control (DEPFF-CEC) technique is proposed. Based on the SMIC 65-nm technology, the post layout simulation results show that the proposed DEPFF-CEC gains an improvement of 8.03–39.83% in terms of power dissipation when the input switching activity is 10%, as compared with its counterparts. Thus, it is suitable for energy-efficient designs whose input data switching activity is low.


1987 ◽  
Vol 91 ◽  
Author(s):  
R.M. Lum ◽  
J.K. Klingert ◽  
B.A. Davidson ◽  
M.G. Lamont

ABSTRACTIn the direct growth of GaAs on Si by MOCVD the overall quality of the heteroepitaxial film is controlled to a large extent by the growth parameters of the initial GaAs buffer layer. We have investigated the structural properties of this layer using Rutherford Backscattering Spectrometry (RBS) and X-ray double crystal diffractometry. The crystallinity of the buffer layer was observed to improve with increasing layer thickness in the range 10–100nm, and then to rapidly degrade for thicker layers. High temperature (750°C) annealing of the buffer layers resulted in considerable reordering of all but the thicker (>200 nm) layers. Alteration of the usual GaAs/Si growth sequence to include an in-situ anneal of the buffer layer after growth interruption yielded GaAs films with improved structural, optical and electrical properties.


1991 ◽  
Vol 30 (Part 2, No. 3B) ◽  
pp. L447-L450 ◽  
Author(s):  
Akihiro Hashimoto ◽  
Naoharu Sugiyama ◽  
Masao Tamura

1993 ◽  
Vol 325 ◽  
Author(s):  
Sahn Nahm ◽  
Hee-Tae Lee ◽  
Sang-Gi Kim ◽  
Kyoung-Ik Cho

AbstractFor the GaAs buffer layer deposited on Si substrate at 80°C and annealed at 300°C for 10 min, the size of most GaAs islands was observed as ∼ 10 nm but large islands (∼ 40 nm) were also seen. According to the calculation of spacing of moire fringes, large GaAs islands are considered to be rotated about 4 ° with respect to the Si substrate normal. However, for the main GaAs film overgrown on the GaAs buffer layer at 580 °C, moire fringes with the spacing of 5 nm (GaAs film without rotation) completely covered the surface of Si substrate. Misfit dislocations and stacking faults were already formed at the growth stage of buffer layer. Stacking faults and misfit dislocations consisting of Lomer and 60 ° dislocations were observed in GaAs films grown at 580 °C. However, after rapid thermal annealing at 900 °C for 10 sec, only Lomer dislocations with 1/2[110] and 1/2[-110] Burgers vectors were observed.


1991 ◽  
Vol 241 ◽  
Author(s):  
J. M. Ballingall ◽  
Pin Ho ◽  
R. P. Smith ◽  
S. Wang ◽  
G. Tessmer ◽  
...  

ABSTRACTMBE GaAs grown at low temperature (300°C) is evaluated for its suitability as a buffer layer for microwave power FETs. Hall effect and capacitance-voltage (C-V) measurements show that low temperature (LT) buffers may have strong deleterious effects on the electronic quality of FET active layers unless they are heat-treated in-situ at 600'C and topped with a thin (∼0. lμm) 600°C GaAs buffer prior to growth of the FET active layer. The voltage isolation properties of the LT buffers are found to be thermally stable to rapid thermal anneals up to 870°C for 10 seconds.Transmission electron microscopy (TEM) cross-sections were examined on FET layers with LT buffer layers which ranged in thickness from 0.1μm to 1.0μm. The TEM reveals a high density (∼1017 cm−3) of small (<100Å) arsenic precipitates in all of the buffer layers studied. In cases where the LT buffer is not heat treated and topped with a thin 600°C GaAs buffer layer, dislocations and arsenic precipitates extend from the buffer layer into the FET active layer. Their presence in the active layer correlates with the degradation in electronic properties observed with Hall effect and CV. Microwave power FETs were measured at DC and 5 GHz. DC and RF results for devices with LT buffer layers are comparable to devices with conventional buffer layers.


1991 ◽  
Vol 107 (1-4) ◽  
pp. 473-478 ◽  
Author(s):  
K. Fujita ◽  
Y. Shiba ◽  
K. Asai

2004 ◽  
Vol 829 ◽  
Author(s):  
Shigeya Naritsuka ◽  
Koji Saitoh ◽  
Toshiyuki Kondo ◽  
Takahiro Maruyama

ABSTRACTBeam induced lateral epitaxy (BILE) on truncated ridges was applied to the heteroepitaxial growth of GaAs on a Si substrate. A GaAs buffer layer was formed on the Si substrate, and then this GaAs/Si template was used as a substrate for the BILE process. As a result, overgrown regions of GaAs of widths as large as 6.5 μm were grown laterally from the sides of the truncated ridges. The growth regions had a flat, smooth top surface consisting of a (111) facet. Although stacking faults from the GaAs/Si template remained in the growth region, which are unfavorable for device applications, the lateral grown region has no dislocations. Thus, the BILE method is useful for reducing dislocations in heteroepitaxy.


2011 ◽  
Vol 1288 ◽  
Author(s):  
Céline Durand ◽  
Bernadette Domengès ◽  
Philippe Le Duc

ABSTRACTMicrostructural characterization (Focused Ion Beam and Transmission Electron Microscopy imaging) was performed on cross-sections of contacts in thick Electro Chemical Deposition copper metallization of System In Package Integrated Circuits. It was shown that the lower growth rate of ECD-Cu in the AlSiCu – barrier Ti – PVD-Cu – ECD-Cu layer stacking is related to a local higher resistivity induced by the presence of a great number of almost planar grain boundaries in the PVD-Cu layer, which are perpendicular to the growth axis. This morphology is a consequence of the almost heteroepitaxial growth of Ti layer on AlSiCu layer.


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