JM3 Letters

Observation of negative mask error enhancement factor due to mask transmission resonance

[+] Author Affiliations
Vicky Philipsen, Peter De Bisschop, Kei Mesuda

IMEC, Kapeldreef 75, B-3001 Leuven, Belgium

J. Micro/Nanolith. MEMS MOEMS. 7(2), 020501 (June 26, 2008). doi:10.1117/1.2938993
History: Received December 17, 2007; Revised March 05, 2008; Accepted March 07, 2008; Published June 26, 2008
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* On assignment from Dai Nippon Printing

We report on the observation of mask transmission resonances in line/space gratings on bilayer mask stacks, both experimentally and in rigorous electromagnetic field (EMF) lithographic simulations. The mask transmission resonances manifest themselves as a local enhancement in the dose-to-size curve through mask linewidth for a given pitch targeted to a fixed wafer CD. We relate this finding to a local transmission loss of the propagating diffraction orders. We investigate both by experiments and by simulations the dependency of this mask transmission resonance on various lithographic conditions such as mask material, grating pitch, and incidence angle and polarization state of the incoming light. The resonant-type anomaly has a large impact on the mask error enhancement factor (MEEF) behavior of these bilayer mask stacks. The dependence of the MEEF as a function of mask linewidth shows strong variations and even negative MEEF values around the position of this resonance, which stem from the local dose-to-size enhancement. More precisely, the behavior of the MEEF can be well predicted by the differential of the dose-to-size curve.

Figures in this Article

Starting from a range of mask linewidths for a given pitch, we determine, for each mask linewidth, the exposure dose needed to print the line/space grating to a fixed target CD, i.e., the dose to size. In general, the dose-to-size curve is expected to increase monotonically as the mask linewidth increases. However, we have detected a local enhancement in such a dose-to-size curve for a bilayer attenuated phase shift mask (att.PSM). The experiment is conducted with a mask consisting of a 34-nm-thick Ta layer with a 113-nm-thick SiON phase-shift layer on top—referred to as TaSiON 1% att.PSM—containing a y-oriented grating of 360-nm pitch. (All dimensions at mask level.) The grating is exposed at NA 1.20 using cQuad 20deg (opening angle) 0.96/0.8 (outer/inner sigma) xy-polarized illumination. The wafer target is a 45-nm CD at 90-nm pitch. For these settings, the mask transmission resonance occurs as a sharp peak on top of the smoothly increasing dose-to-size curve between 40- and 50-nm mask linewidth (at 1×), as presented in Fig. 1. This resonant-type anomaly is well predicted by rigorous electromagnetic field (EMF) lithographic simulators, and is thus fully described by the Maxwell equations. The experimental observation of this anomaly validates in fact the predictive power of lithographic simulators for the imaging performance of even this type of exotic mask stacks.

Graphic Jump LocationF1 :

Observation of a mask transmission resonance (indicated by an arrow) through mask linewidth at pitch 90nm (at 1×) for TaSiON 1% att.PSM using NA 1.20 cQuad 20deg 0.96/0.8 (outer/inner sigma) xy-polarized illumination. Right axis: experimental dose-to-size curve. Left axis: simulated amplitudes of the propagating diffraction orders for the x-oriented poles using y-polarization.

Simulations reveal this resonance effect already in the off-axis diffraction spectrum as a local transmission loss in the propagating diffraction orders (see Fig. 1). Both zeroth and first diffraction orders exhibit a dip in their amplitude leading to an increase of the required dose.

Because of its substantial impact on the dose-to-size behavior, we have examined the dependency of the mask transmission resonance on various mask and lithographic settings.

First, we observe multiple mask transmission resonances through mask linewidth for a large pitch range. Figure 2 compares the dose-to-size curves from simulation to those from experimental printing evaluation for a pitch range of 88nm to 130nm targeted to a 45-nm wafer CD. Resonances around mask linewidths 30nm, 45nm, and 62nm become apparent. The pitch influences only the magnitude of the resonance.

Graphic Jump LocationF2 :

Top: simulated dose-to-size curves through mask linewidth for a pitch range of 90nm to 130nm. Bottom: corresponding experimental printing results for a pitch range of 88nm to 130nm. Results for TaSiON 1% att.PSM using NA 1.20 x-oriented dipole 0.96/0.8 sigma outer-inner y-polarized illumination.

Second, we have investigated the effect of the mask material and stack on the resonance at the same lithographic conditions as for the TaSiON 1% att.PSM. We did not find a resonance anomaly in the standard mask stacks Cr binary mask and MoSi 6% att.PSM. We also have looked into the behavior of two bilayer att.PSM versions with Ta as absorber, but SiO2 as transparent phase shifter. These masks have a Ta thickness of 20nm or 30nm with a corresponding SiO2 thickness of 145nm or 138nm, respectively, on top. Experimentally, we do not observe a resonance in these TaSiO2 att.PSM for pitch 90nm. This is an indication that the mask transmission resonance is not related to the Ta-metal absorber alone, but is more likely created by the mask stack configuration of a dielectric layer on top of the absorber. Indeed, if we perform by simulations a thickness variation of SiON or SiO2 on any absorber layer such as Ta, Cr, or even MoSi, we can find a thickness of the transparent layer that will generate a resonance around one or more specific mask linewidths. For example, at NA 1.2 using x-oriented dipole 40deg 0.96/0.8 (outer/inner sigma) with y-polarized illumination, a SiO2 thickness around 180nm on top of 19-nm-thick Ta layer produces a mask transmission resonance, while at 145-nm SiO2 thickness, no anomaly in the dose-to-size curve is seen [see Fig. 3].

Graphic Jump LocationF3 :

Impact of the dielectric layer thickness on the presence of a mask transmission resonance in the simulated dose-to-size curve using x-oriented dipole illumination, other settings as in Fig. 1. (a) For TaSiO2 att.PSM with 19-nm Ta-absorber using y-polarized light. (b) For TaSiON att.PSM with 34-nm Ta-absorber using x-polarized light.

Last, the magnitude of the mask transmission resonance depends on the NA, illuminator shape, and polarization state of the incoming light, but the resonant-type anomaly appears at all investigated settings. For both x- and y-polarized light, resonances occur, but at different parametric mask settings. Figure 3 illustrates that at the SiON thickness, where a resonance occurs for y-polarized light (cf. Fig. 1), no resonance is observed for x-polarized light. However, by increasing the SiON thickness, the mask transmission resonance starts emerging at the large linewidth side. As such, the mask configuration acts as a polarization-sensitive filter. These findings support the idea of an optical resonance induced by the transparent phase-shift layer of the mask grating. This phenomenon seems closely related to the waveguide-grating resonances described in Refs. 12. The resonances occur due to the coupling of the diffracted fields from the incoming light into the waveguide modes. In our case, the absorber grating creates the diffracted fields, and the waveguide is formed by the dielectric layer of higher refractive index between the quartz substrate and air of lower refractive index. For a certain mask linewidth, the dielectric cavity becomes a resonator for one polarization direction. Looking at the transmission of the EMF under off-axis incidence through the mask, as exemplified in Fig. 4 for TaSiON 1% att.PSM, we observe spots of higher intensities confined inside the SiON-cavity for the resonant mask linewidth using y-polarized illumination, in contrast to the nonresonant mask linewidth and in contrast to x-polarized illumination.

Graphic Jump LocationF4 :

Transmission of the EMFs under 15deg oblique incidence through the TaSiON 1% att.PSM mask unit cell of pitch 90nm (at 1×). The illumination is y-polarized in (a) and (b), x-polarized in (c). The mask linewidth (at 1×) is 35nm in (a) and 45nm in (b) and (c).

The sharp enhancement of the dose-to-size curve around the resonant mask linewidth will induce a variation in the mask error enhancement factor (MEEF) behavior. We even measure negative MEEF values caused by a mask transmission resonance (see Fig. 5). A negative MEEF seems counterintuitive since it implies that the printed wafer CD decreases with increasing mask linewidth at fixed exposure dose. Moreover, the correlation between the dose-to-size curve and MEEF behavior clearly indicates that the MEEF behavior can be well predicted by the differential of the dose-to-size curve through mask linewidth. This can be simply explained as follows. MEEF is defined as the derivative of the wafer CD through mask linewidth, orDisplay Formula

1MEEF=dCDdmLW,
with mLW=mask linewidth. Multiplying the right side of Eq. 1 by unity, or (dDosedDose) givesDisplay Formula
2MEEF=dDosedmLWdCDdDose.

Graphic Jump LocationF5 :

Settings identical to Fig. 1. Top: experimental dose-to-size curve; bottom: experimental MEEF curve and differential of the experimental dose-to-size curve.

The wafer CD variation through exposure dose is assumed to correspond to a first-order function for small dose variation based on simulations and experiments specific to this study, in other words, (dCDdDose) is a constant, and Eq. 2 results in the proportionalityDisplay Formula

3MEEFdDosedmLW.
More precisely, when the dose-to-size curve decreases with increasing mask linewidth, a negative MEEF is measured, which is consistent with the negative slope of the dose-to-size curve around these mask linewidths. Figure 5 is an experimental proof of the relationship Eq. 3 between dose to size and MEEF for the specific conditions of this study, showing a MEEF oscillation from +25 to 10 over only a 2-nm mask linewidth increase at 1×. The occurrence of strong varying MEEF within the current limits of mask linewidth uniformity is of course an undesirable imaging effect, as it will give rise to uncontrollable CD variations at fixed exposure dose. On the other hand, understanding the mechanism of the mask transmission resonance can offer the possibility to explore potential imaging applications.

In this letter, we have demonstrated the existence of mask transmission resonances under specific lithographic conditions of mask stack, line/space grating, and illumination. Experimental investigations have revealed the presence of such mask transmission resonance as an irregularity in the dose-to-size behavior through mask linewidth. As a consequence, even negative MEEF values were reported. Furthermore, we have argued that the differential of the dose-to-size curve through mask linewidth corresponds to the MEEF. In addition, the agreement between our experimental and simulated results confirms the validity of mask 3-D simulations for the conditions of this study.

We conclude this letter with a two-part remark: First, caution is required when exploring alternative mask stacks for improving imaging to exclude uncontrollable and thus unwanted optical anomalies. Second, the awareness of these optical effects could possibly translate into a controllable and thus beneficial impact on imaging. However, the implementation has yet to be proven viable.

Magnusson  R., and Wang  S. S., “ New principle for optical filters. ,” Appl. Phys. Lett..  0003-6951 61, (9 ), 1022–1024  ((1992)).
Bao  G., and Huang  K., “ Optimal design of guided-mode grating resonance filters. ,” IEEE Photonics Technol. Lett..  1041-1135 16, (1 ), 141–143  ((2004)).
© 2008 Society of Photo-Optical Instrumentation Engineers

Citation

Vicky Philipsen ; Peter De Bisschop and Kei Mesuda
"Observation of negative mask error enhancement factor due to mask transmission resonance", J. Micro/Nanolith. MEMS MOEMS. 7(2), 020501 (June 26, 2008). ; http://dx.doi.org/10.1117/1.2938993


Figures

Graphic Jump LocationF4 :

Transmission of the EMFs under 15deg oblique incidence through the TaSiON 1% att.PSM mask unit cell of pitch 90nm (at 1×). The illumination is y-polarized in (a) and (b), x-polarized in (c). The mask linewidth (at 1×) is 35nm in (a) and 45nm in (b) and (c).

Graphic Jump LocationF5 :

Settings identical to Fig. 1. Top: experimental dose-to-size curve; bottom: experimental MEEF curve and differential of the experimental dose-to-size curve.

Graphic Jump LocationF3 :

Impact of the dielectric layer thickness on the presence of a mask transmission resonance in the simulated dose-to-size curve using x-oriented dipole illumination, other settings as in Fig. 1. (a) For TaSiO2 att.PSM with 19-nm Ta-absorber using y-polarized light. (b) For TaSiON att.PSM with 34-nm Ta-absorber using x-polarized light.

Graphic Jump LocationF2 :

Top: simulated dose-to-size curves through mask linewidth for a pitch range of 90nm to 130nm. Bottom: corresponding experimental printing results for a pitch range of 88nm to 130nm. Results for TaSiON 1% att.PSM using NA 1.20 x-oriented dipole 0.96/0.8 sigma outer-inner y-polarized illumination.

Graphic Jump LocationF1 :

Observation of a mask transmission resonance (indicated by an arrow) through mask linewidth at pitch 90nm (at 1×) for TaSiON 1% att.PSM using NA 1.20 cQuad 20deg 0.96/0.8 (outer/inner sigma) xy-polarized illumination. Right axis: experimental dose-to-size curve. Left axis: simulated amplitudes of the propagating diffraction orders for the x-oriented poles using y-polarization.

Tables

References

Magnusson  R., and Wang  S. S., “ New principle for optical filters. ,” Appl. Phys. Lett..  0003-6951 61, (9 ), 1022–1024  ((1992)).
Bao  G., and Huang  K., “ Optimal design of guided-mode grating resonance filters. ,” IEEE Photonics Technol. Lett..  1041-1135 16, (1 ), 141–143  ((2004)).

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