Abstract:Direct bonding may provide a cheap and reliable alternative to the use of adhesives. While direct bonding of two silicon surfaces is well documented, not much is known about direct bonding between silicon nitride and glass. This is unfortunate since silicon nitride is extensively used as an anti-reflection coating in the PV industry, often in contact with a shielding layer made of glass. A series of bonding experiments between glass and SiN was performed. The highest bonding quality, manifested by the highest … Show more
“…While the O 2 plasma activation resulted on average in lower contact angles compared to the HCl activation, some batches approached 90°indicating that in principle, plasma activation can achieve a sufficiently high hydroxy density on the surface. [47] In agreement with activation in a N 2 plasma reported to be better, [47] we measured a significantly higher contact angle of 82:5 � 2:2°(N ¼ 432) with less variability when using the N 2 plasma (see Table 4 for significance values). Yet, both O 2 and N 2 plasmas do not contain any hydrogen species for direct surface hydroxylation.…”
Section: Optimized Plasma Surface Activation In the Presence Of Hydro...supporting
confidence: 85%
“…As a control, we plotted the results of the HCl and O 2 plasma activations of Figure 2A (note the zoom‐in of the y ‐axis). While the O 2 plasma activation resulted on average in lower contact angles compared to the HCl activation, some batches approached 90° indicating that in principle, plasma activation can achieve a sufficiently high hydroxy density on the surface [47] . In agreement with activation in a N 2 plasma reported to be better, [47] we measured a significantly higher contact angle of ° ( ) with less variability when using the N 2 plasma (see Table 4 for significance values).…”
Section: Resultsmentioning
confidence: 98%
“…Yet, both O 2 and N 2 plasmas do not contain any hydrogen species for direct surface hydroxylation. Instead, it is assumed that the exposure of the freshly plasma‐activated, reactive surfaces to ambient air results in surface‐silanol formation [47] . Thus, we tested whether an air plasma with its natural water content would be more effective.…”
Single-molecule assays often require functionalized surfaces. One approach for microtubule assays renders surfaces hydrophobic and uses amphiphilic blocking agents. However, the optimal hydrophobicity is unclear, protocols take long, produce toxic waste, and are susceptible to failure. Our method uses plasma activation with hydrocarbons for hexamethyldisilazane (HMDS) silanization in the gas phase. We measured the surface hydrophobicity, its effect on how well microtubule filaments were bound to the surface, and the number of nonspecific interactions with kinesin motor proteins. Additionally, we tested and discuss the use of different silanes and activation methods. We found that even weakly hydrophobic surfaces were optimal. Our environmentally friendly method significanty reduced the overall preparation effort and resulted in reproducible, high-quality surfaces with low variability. We expect the method to be applicable to a wide range of other single-molecule assays.
“…While the O 2 plasma activation resulted on average in lower contact angles compared to the HCl activation, some batches approached 90°indicating that in principle, plasma activation can achieve a sufficiently high hydroxy density on the surface. [47] In agreement with activation in a N 2 plasma reported to be better, [47] we measured a significantly higher contact angle of 82:5 � 2:2°(N ¼ 432) with less variability when using the N 2 plasma (see Table 4 for significance values). Yet, both O 2 and N 2 plasmas do not contain any hydrogen species for direct surface hydroxylation.…”
Section: Optimized Plasma Surface Activation In the Presence Of Hydro...supporting
confidence: 85%
“…As a control, we plotted the results of the HCl and O 2 plasma activations of Figure 2A (note the zoom‐in of the y ‐axis). While the O 2 plasma activation resulted on average in lower contact angles compared to the HCl activation, some batches approached 90° indicating that in principle, plasma activation can achieve a sufficiently high hydroxy density on the surface [47] . In agreement with activation in a N 2 plasma reported to be better, [47] we measured a significantly higher contact angle of ° ( ) with less variability when using the N 2 plasma (see Table 4 for significance values).…”
Section: Resultsmentioning
confidence: 98%
“…Yet, both O 2 and N 2 plasmas do not contain any hydrogen species for direct surface hydroxylation. Instead, it is assumed that the exposure of the freshly plasma‐activated, reactive surfaces to ambient air results in surface‐silanol formation [47] . Thus, we tested whether an air plasma with its natural water content would be more effective.…”
Single-molecule assays often require functionalized surfaces. One approach for microtubule assays renders surfaces hydrophobic and uses amphiphilic blocking agents. However, the optimal hydrophobicity is unclear, protocols take long, produce toxic waste, and are susceptible to failure. Our method uses plasma activation with hydrocarbons for hexamethyldisilazane (HMDS) silanization in the gas phase. We measured the surface hydrophobicity, its effect on how well microtubule filaments were bound to the surface, and the number of nonspecific interactions with kinesin motor proteins. Additionally, we tested and discuss the use of different silanes and activation methods. We found that even weakly hydrophobic surfaces were optimal. Our environmentally friendly method significanty reduced the overall preparation effort and resulted in reproducible, high-quality surfaces with low variability. We expect the method to be applicable to a wide range of other single-molecule assays.
“…54 Thus, domains are formed on the Si 3 N 4 surface to form SiO 2 networks, which have a higher affinity to form silanol groups on the surface after plasma activation. 55,56 The SiO 2 domains saturated with silanol groups have a lower positive surface charge than the Si 3 N 4 surface, as shown by surface charge measurements after plasma activation, because SiO 2 forms also under normal ambient condition silanol dangling bonds. 57 Thus, the total positive charge at the Si 3 N 4 surface is lowered in comparison to the untreated one.…”
Controlling
the doping level in graphene during integration into
silicon CMOS compatible devices is an open challenge. In general,
the doping level in graphene is influenced via substrate interactions,
metal contacts, and encapsulation layers. Here, we demonstrate a method
to control the Fermi level in graphene through transfer onto ionic-doped
oxide surfaces. The substrates were prepared to this end by diffusion
of ammonia and aluminum on the oxide surface, which induces positive
(NSiO+) and negative (AlSiO–) charges
on the oxide layer. Van der Pauw measurements show that the charge
neutrality or Dirac voltage in graphene can be shifted from about
−60 V (n = −8.62 × 1012 cm–2) on standard SiO2 to about 13
V (n = 2.17 × 1012 cm–2) on negatively doped SiO2 layers by manipulating the
surface charge. Hall measurements show that the electron mobility
in graphene transferred on an as-grown oxide surface is higher than
for graphene on a doped oxide because of additional scattering centers.
Transfer line method measurements show that the contact resistance
between graphene and nickel electrodes varies in average from 683.3
Ω·μm on SiO2 to 1046.6 Ω·μm
on negatively doped SiO2 and that it depends on both the
substrate surface charge and on graphene sheet resistance. Ionic-doped
oxide surfaces are generally temperature-stable with respect to front-
and back-end-of-the-line semiconductor manufacturing. The method presented
here allows adjustments of the surface charge density of the substrate,
and thus in graphene, which cannot be realized by organic or metallic
functionalization. Therefore, the method may be suitable for engineering
graphene-based devices and circuits, in particular, for applications
that require complementary devices or a specific position of the Fermi
level in graphene, for example, to adjust contact resistivity, sheet
resistance, or sensor sensitivity.
“…PI reaches a certain degree of curing after pre-baking (Figure 7b). Combining the above discussion and analysis of the bonding surface and the bonding interface, as well as the previously published reports [32][33][34][35], we can get the effect of O2 plasma on the surface of the PI film: (1) removing surface contaminants; (2) increasing the number of -OH (hydroxyl) groups pre unit area on the surface; (3) changing the surface structure and improving the diffusion capacity of water and gas on the surface. The experimental results show that the PI film becomes smoother and exhibits more significant hydrophilicity after O2 plasma treatment (Figure 7c).…”
In situ measurements of sensing signals in space platforms requires that the micro-electro-mechanical system (MEMS) sensors be located directly at the point to be measured and in contact with the subject to be measured. Traditional radiation-tolerant silicon-based MEMS sensors cannot acquire spatial signals directly. Compared to silicon-based structures, LiNbO3 single crystalline has wide application prospects in the aerospace field owing to its excellent corrosion resistance, low-temperature resistance and radiation resistance. In our work, 4-inch LiNbO3 and LiNbO3/Cr/Au wafers are fabricated to silicon substrate by means of a polyimide bonding method, respectively. The low-temperature bonding process (≤100 °C) is also useful for heterostructure to avoid wafer fragmentation results from a coefficient of thermal expansion (CTE) mismatch. The hydrophilic polyimide surfaces result from the increasing of -OH groups were acquired based on contact angle and X-ray photoelectron spectroscopy characterizations. A tight and defect-free bonding interface was confirmed by scanning electron microscopy. More importantly, benefiting from low-temperature tolerance and radiation-hardened properties of polyimide material, the bonding strength of the heterostructure based on oxygen plasma activation achieved 6.582 MPa and 3.339 MPa corresponding to room temperature and ultra-low temperature (≈ −263.15 °C), which meets the bonding strength requirements of aerospace applications.
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