Abstract:Commercial EUV lithographic systems require multilayers with higher reflectance and better stability then that published to date. Interface-engineered MoISi multilayers with 70% reflectance at 13.5 nm wavelength (peak width of 0.545 nm) and 71% at 12.7 nm wavelength (peak width of 0.49 nm) were developed. These results were achieved with 50 bilayers. These new multilayers consist of Mo and Si layers separated by thin boron carbide layers. Depositing boron carbide on interfaces leads to reduction in silicide fo… Show more
“…The mirror is assumed to have a ruthenium surface because in EUV lithography this metal is often applied as a capping layer ͑thick-ness Ϸ1.5 nm͒ to provide a barrier against oxidation of the underlying Mo/ Si stacks. 15 The EUV radiation is partially reflected by the mirror with a reflection coefficient of R ml = 68%, which is typical for Mo/ Si multilayer mirrors. 1,16 The remaining 32% of the radiation is absorbed and is converted primarily to heat.…”
Future generation lithography tools will use extreme ultraviolet radiation to enable the printing of sub-50 nanometer features on silicon wafers. The extreme ultraviolet radiation, coming from a pulsed discharge, photoionizes the low pressure background gas in the tool. A weakly ionized plasma is formed, which will be in contact with the optical components of the lithography device. In the plasma sheath region ions will be accelerated towards the surfaces of multilayer mirrors. A self-consistent kinetic particle-in-cell model has been applied to describe a radiation driven plasma. The simulations predict the plasma parameters and notably the energy at which ions impact on the plasma boundaries. We have studied the influence of photoelectron emission from the mirror on the sheath dynamics and on the ion impact energy. Furthermore, the ion impact energy distribution has been convoluted with the formula of Yamamura and Tawara [At. Data Nucl. Data Tables 62, 149 (1996)] for the sputter yield to obtain the rate of physical sputtering. The model predicts that the sputter rate is dominated by the presence of doubly ionized argon ions.
“…The mirror is assumed to have a ruthenium surface because in EUV lithography this metal is often applied as a capping layer ͑thick-ness Ϸ1.5 nm͒ to provide a barrier against oxidation of the underlying Mo/ Si stacks. 15 The EUV radiation is partially reflected by the mirror with a reflection coefficient of R ml = 68%, which is typical for Mo/ Si multilayer mirrors. 1,16 The remaining 32% of the radiation is absorbed and is converted primarily to heat.…”
Future generation lithography tools will use extreme ultraviolet radiation to enable the printing of sub-50 nanometer features on silicon wafers. The extreme ultraviolet radiation, coming from a pulsed discharge, photoionizes the low pressure background gas in the tool. A weakly ionized plasma is formed, which will be in contact with the optical components of the lithography device. In the plasma sheath region ions will be accelerated towards the surfaces of multilayer mirrors. A self-consistent kinetic particle-in-cell model has been applied to describe a radiation driven plasma. The simulations predict the plasma parameters and notably the energy at which ions impact on the plasma boundaries. We have studied the influence of photoelectron emission from the mirror on the sheath dynamics and on the ion impact energy. Furthermore, the ion impact energy distribution has been convoluted with the formula of Yamamura and Tawara [At. Data Nucl. Data Tables 62, 149 (1996)] for the sputter yield to obtain the rate of physical sputtering. The model predicts that the sputter rate is dominated by the presence of doubly ionized argon ions.
“…The high-reflectance Mo/Si multilayer used in the EUVL system consists of polycrystalline Mo and amorphous Si layers that are separated by an interfacial region [4,5]. In order to obtain high reflectivity, a minimal thickness of Mo/Si interface is required because the intermixing region tends to reduce reflectivity [6].…”
The energetics and the electronic structure of the Si/Mo(110) surface have been investigated using density functional theory calculations based on the generalized gradient approximation. The calculated potential energy surface for a single Si adatom reveals that a hollow site is favored for the adsorption of Si on Mo(110). The energy barrier for hopping between the hollow sites is located at the bridge site and is found to be 0.64 eV. The electron density plot indicates that four Mo-Si covalent bonds were formed around the Si atom at the hollow site. According to the surface formation energy for different Si coverage, 1 ML Si/Mo(110)− p(1 × 1) is energetically favorable for a Si-rich environment. For the Si-poor case, the clean Mo(110) surface is the most stable structure.
“…A suitable replacement to these lens systems has been found in molybdenum silicon (Mo/Si) multilayer mirror systems. Due to their reflectivity (∼ 70%) at 13.5 nm [1], this means that source designers must optimise the EUV flux emitted by the source in this range, as it can be reflected 9, 11 or 13 times in the lithography process. Laser produced plasmas (LPPs) can be made to significantly emit at the appropriate wavelengths [2,3].…”
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