Abstract:Hybrid metal−organic cluster resist materials, also termed as organo-inorganics, demonstrate their potential for use in next-generation lithography owing to their ability for patterning down to ∼10 nm or below. High-resolution resist patterning is integrally associated with the compatibility of the resist and irradiation of the exposure source. Helium ion beam lithography (HIBL) is an emerging approach for the realization of sub-10 nm patterns at considerably lower line edge/width roughness (LER/ LWR) and high… Show more
“…For the current research, we have fixed 500 nm square boxes with a base dose of 100 μC/cm 2 . 29 Apart from the variable dose, the beam energy was also varied to analyze the energy dispersion inside the 40 nm-thick 3b. The beam energies (E Beam ) were 1, 2, 5, 10, and 20 keV.…”
Given the current need for resist
materials for patterning transistors
with ultralow nodes, there has been a quest for developing resists
with improved performance for nanoscale patterning with good contrast.
The present work demonstrates polymeric resists (MAPDST-TIPMA) developed
through the integration of a radiation-sensitive monomer (MAPDST)
with an organoiodine functionality (TIPMA) for sub-16 nm patterning
using electron-beam and helium ion beam lithography. The structural
integrity was established by several spectroscopic techniques particularly
NMR, FTIR, XPS, and GPC. These polymeric resists possess weight-average
molecular weight (M
w) in the range of
10000–12000 with low PDI. While the resists 3a and 3b were synthesized with feed ratios of 80:20 and
70:30 of the monomers MAPDST and TIPMA, respectively, the actual microstructure
compositions were calculated, using XPS and GPC data, to be ∼94:6
and 91:9, respectively. The present resists have the potential for
patterning 16 nm line/space features when exposed to e-beam. Also,
15 nm features were successfully patterned using MAPDST-TIPMA resists.
The line edge roughness (LER) and line width roughness (LWR) of the
20 nm L/3S features were calculated to be 2.48 and 3.6 nm, respectively.
Moreover, complex nanofeatures of different shapes were successfully
patterned using 3b. A critical analysis of nanofeatures
using AFM revealed that the patterns are very well developed with
a sharp wall profile. The normalized resist thickness (NRT) curve
was established to evaluate the sensitivity of the present resist
which was calculated to be 341 μC/cm2 at 20 keV.
The nature and slope of the NRT curve indicated that MAPDST-TIPMA
is a negative tone resist with good contrast. Finally, the resist
was found to be highly sensitive to He+ beam (sensitivity
∼6.21 μC/cm2) resulting in 20 nm L/S as well
as 15 nm features with a good wall profile.
“…For the current research, we have fixed 500 nm square boxes with a base dose of 100 μC/cm 2 . 29 Apart from the variable dose, the beam energy was also varied to analyze the energy dispersion inside the 40 nm-thick 3b. The beam energies (E Beam ) were 1, 2, 5, 10, and 20 keV.…”
Given the current need for resist
materials for patterning transistors
with ultralow nodes, there has been a quest for developing resists
with improved performance for nanoscale patterning with good contrast.
The present work demonstrates polymeric resists (MAPDST-TIPMA) developed
through the integration of a radiation-sensitive monomer (MAPDST)
with an organoiodine functionality (TIPMA) for sub-16 nm patterning
using electron-beam and helium ion beam lithography. The structural
integrity was established by several spectroscopic techniques particularly
NMR, FTIR, XPS, and GPC. These polymeric resists possess weight-average
molecular weight (M
w) in the range of
10000–12000 with low PDI. While the resists 3a and 3b were synthesized with feed ratios of 80:20 and
70:30 of the monomers MAPDST and TIPMA, respectively, the actual microstructure
compositions were calculated, using XPS and GPC data, to be ∼94:6
and 91:9, respectively. The present resists have the potential for
patterning 16 nm line/space features when exposed to e-beam. Also,
15 nm features were successfully patterned using MAPDST-TIPMA resists.
The line edge roughness (LER) and line width roughness (LWR) of the
20 nm L/3S features were calculated to be 2.48 and 3.6 nm, respectively.
Moreover, complex nanofeatures of different shapes were successfully
patterned using 3b. A critical analysis of nanofeatures
using AFM revealed that the patterns are very well developed with
a sharp wall profile. The normalized resist thickness (NRT) curve
was established to evaluate the sensitivity of the present resist
which was calculated to be 341 μC/cm2 at 20 keV.
The nature and slope of the NRT curve indicated that MAPDST-TIPMA
is a negative tone resist with good contrast. Finally, the resist
was found to be highly sensitive to He+ beam (sensitivity
∼6.21 μC/cm2) resulting in 20 nm L/S as well
as 15 nm features with a good wall profile.
“…The first step‐1 weight loss is mainly attributed to the removal of solvents trapped in the material and the unbound moisture. [ 44 ] The second step‐2 of weight loss is unclear while the third step‐3 of weight loss is due to the loss of organic ligands attached in the Cu‐MOCs dielectric material. The total weight loss attributed to 73 wt% in Cu‐MOCs, thereby, leading to 27 wt% of dielectric material remains in the form of inorganic copper oxide counterparts.…”
The suitability of metal‐organic frameworks (MOFs) as functional materials for future electronic logic devices with desirable dielectric constant, bandgap, high‐quality interface, low leakage current, and better compatibility is still an open challenge. Owing to the synergistic complementary properties of MOFs systems, a low‐cost copper‐metal‐organic nanoclusters (Cu‐MOCs) has been synthesized comprising inorganic copper metal unit allied organic m‐toluic acid ligand by facile sol–gel strategy. It offers large‐area thin‐films uniformity, high dielectric constant (κ ≈ 5.49), improved interfacial properties, dynamic switching behavior with the stimuli field, and extends the realization of metal‐organic‐framework dielectric for scalable complementary‐metal‐oxide‐semiconductor (CMOS) logic applications over customary hybrid counterparts. Various techniques such as single crystal X‐ray diffraction, X‐ray photoelectron spectroscopy, thermogravimetric analysis, and energy dispersive X‐ray spectroscopy have been used to validate the Cu‐MOCs formulation. In particular, the fabricated Cu‐MOCs, metal–insulator–semiconductor structures exhibit promising dynamic switching behavior responsive to the applied field, hysteresis‐free capacitance–voltage characteristics, low interfacial trap density (≈1.4 × 1011 eV−1 cm−2), low effective oxide charges (≈1.1 × 1011 cm−2), and noteworthy small leakage current density (≈1.29 nA cm−2 @ 1 V) ever since in electrical analysis. Cost‐effective novel Cu‐MOCs successfully demonstrate high‐performance, reliable gate dielectrics for next‐generation CMOS logic devices.
“…Consequently, the spot size remains small for considerable distances above and below the focal plane, which allows for high‐resolution patterning even on tilted surfaces. [ 62 , 63 ]…”
Section: Established Fabrication Methodsmentioning
confidence: 99%
“…The degree of distortion is affected by the presence of nearby patterned features in the resist; distortions arising from scattering events are consequently known as “proximity effects.” Compared to electron beams, ion beams are far less susceptible to scattering and so exhibit much weaker proximity effects, making them a better choice for high density nanoscale patterning. [ 63 ]…”
Section: Established Fabrication Methodsmentioning
Metallic nanogaps with metal-metal separations of less than 10 nm have many applications in nanoscale photonics and electronics. However, their fabrication remains a considerable challenge, especially for applications that require patterning of nanoscale features over macroscopic length-scales. Here, some of the most promising techniques for nanogap fabrication are evaluated, covering established technologies such as photolithography, electron-beam lithography (EBL), and focused ion beam (FIB) milling, plus a number of newer methods that use novel electrochemical and mechanical means to effect the patterning. The physical principles behind each method are reviewed and their strengths and limitations for nanogap patterning in terms of resolution, fidelity, speed, ease of implementation, versatility, and scalability to large substrate sizes are discussed.
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