ABSTRACT
This work presents the morphologic and structural study of nanolaminated Ti/TiN multilayers using high-resolution scanning electron microscopy (HR-SEM), coupled to x-ray reflectometry (XRR). The multilayers have been deposited by reactive rf-sputtering on silicon substrates. For large period thickness (lambda=40 nm, 10 periods), in XRR, the low number of interfaces makes the interference less structured. An experimental pattern with broad and weakly intense Braggs peaks is obtained, but is difficult to simulate. On the other hand, HR-SEM observation of cross sections gives excellent pictures of the multilayer, so that precise measurements of the thickness can be achieved: a 42 nm thick period is observed, formed with 17 nm of Ti and with 25 nm of TiN. For small (Ti+TiN) period thickness (lambda=2.5 nm, 120 periods), the XRR pattern exhibits intense and narrow Bragg peaks: the number of interfaces is sufficient to structure the interference and an intense signal is obtained. The best fit of simulation is obtained for a 2.6 nm thin period, made of 0.9 nm of Ti and 1.7 nm of TiN. No laminated structure has been observed by cross-section HR-SEM observation because its resolution (around 2 nm at 10 kV) is larger than the layer thickness in a period. High-resolution SEM and XRR are thus two complementary techniques for the routine characterization of multilayers.
ABSTRACT
W/Mg2Si multilayers for soft x-ray optics above the MgKα and MgLα lines have been deposited by RF sputtering. Their structural characteristics have been deduced from in situ kinetic ellipsometry, ex situ grazing x-ray reflection measurements, and high-resolution electron microscopy. Their soft x-ray performances have been measured by synchrotron radiation around the MgKα and MgLα lines and related to the structural characteristics. For short wavelengths, first Bragg peak reflectivities as high as 31% have been measured for multilayers with double period equal to 84 Å. For samples with smaller layer thicknesses, these performances decrease due to finite interdiffusion at the interfaces. Nevertheless, well-defined Bragg peaks are observed even when the double period is as low as 44 Å. Near the MgLα line, more than 20% reflectivity at the first Bragg peak has been measured at normal incidence. At the same wavelength the selectivity is two times higher than that of conventional systems such as Mo/Si.
