We discuss the impact of various tool design perspectives on defect detection sensitivity for dark-field-based extreme ultraviolet (EUV) actinic blank inspection. We consider the impact of pixel size, EUV source type, and photon collection efficiency on critical defect signal-to-noise ratio (SNR) performance. The results show that as the pixel size approaches the target defect image size, defect SNR increases, and that pixel size also determines the dominant noise source in the inspection system. Moreover, the choice of the EUV source affects the optimal numerical aperture (NA) and illumination settings. For plasma-discharged sources, more photons provided by larger partial coherent illumination can improve the defect SNR, while coherent illumination is needed to get a higher defect SNR for synchrotron-based source. In the end, we show that simply increasing the photon collection efficiency by using high-NA optics or increasing the source power cannot always improve the defect SNR. In a speckle-noise dominated situation, larger outer NA includes more noise than defect signal, thus resulting in a lower SNR. The impact of source power also saturates at a certain level as the system becomes speckle-noise limited compared to photon-noise limited.
Mask 3D (M3D) effects remain a significant challenge affecting EUV lithography (EUVL) imaging performance due to the comparable sizes of the mask and the EUV wavelength. Pre-compensation with the insertion of sub-resolution assist features (SRAFs) has been proposed as a solution to compensate M3D effects and improve the process window for advanced technology nodes. In this paper, we discuss the possible positive impact of SRAFs on Bossung tilt, and provide physical insight into the optical mechanisms at play enabling M3D effect mitigation. In particular, we consider an example isolated 2-bar (CD = 16 nm) pattern imaged under delta function dipole illumination. We compare the scattered order distribution and Bossung tilt with and without SRAFs. The results show that SRAFs actually introduce stronger effective single pole aberrations in the imaging process. However, the opposite impacts on Bossung tilt from each pole results in an overall improvement for dipole illumination. Reduced Bossung tilt and a 21% improvement of the overlapping process window are achieved by the insertion of asymmetric SRAFs into the 2-bar mask design.
In this paper, we discuss the impact of various tool design perspectives on defect detection sensitivity for dark-field based EUV actinic blank inspection. We consider the impact from optical resolution (pixel size), EUV source type, and photon collection efficiency on critical defect SNR performance. The results show that as the pixel size approaches the target defect image size, defect SNR increases, and that pixel size also determines the dominant noise source in the inspection system. Moreover, the choice of the EUV source affects the optimal NA and illumination settings. For plasma-discharged sources, more photons provided by larger partial coherent illumination can improve the defect SNR, while coherent illumination is needed to get a higher defect SNR for synchrotron-based source. In the end, we show that simply increasing the photon collection efficiency by using high NA optics or increasing the source power cannot always improve the defect SNR. In a speckle noise dominated situation, larger outer NA includes more noise than defect signal, thus results in a lower SNR. The impact of source power also saturates at certain level as the system becomes speckle noise limited compared to photon noise limited.
We discuss the impact of various noise sources and the optical design in bright field extreme ultraviolet (EUV) actinic inspection of mask features for defects in the patterned absorber. It is shown that an optimum pixel size is needed to maximize the defect signal-to-noise ratio (SNR) to balance the trade-off in increasing signal strength with shot noise from defect signal and the background pattern intensity (mask layout image) and speckle noise from the mask blank roughness. Moreover, we consider defocus showing that the EUV mask phase effect has an asymmetric impact on pattern defect SNR’s through-focus behavior. The impact of defocus limits inspection performance based on defect SNR. Using critical defect sizes in a case study, we show the defect SNR performance of the limiting case and discuss the possibility of utilizing a nominal defocus in the inspection system to leverage the phase effect of EUV mask absorber to improve the defect SNR. A 50% improvement in defect SNR is shown to be possible by introducing a −50 nm nominal defocus into the bright field inspection system.
In this paper, we discuss the impact of various noise sources and optical design on defect sensitivity for bright field EUV
actinic pattern inspection. The result shows that an optimum pixel size is needed to maximize the defect signal to noise
ratio (SNR) to balance the impact of increasing signal strength and photon shot noise from defect signal and the
background pattern intensity (mask layout image) and speckle noise from the mask blank roughness. Moreover, we
consider defocus showing that the EUV mask phase effect has an asymmetric impact on pattern defect SNR’s throughfocus.
The impact of defocus limits inspection performance based on defect SNR. Using critical defect sizes in a case
study, we show the defect SNR performance of the limiting case and discuss the possibility to utilize the phase effect of
EUV mask absorber to improve the defect SNR by introducing a nominal defocus into the inspection system. A 50%
improvement on SNR is achieved by introducing a -50 nm nominal defocus into the bright field inspection system to
operate at a higher defect SNR region.
The SHARP high-numerical aperture actinic reticle review project is a synchrotron-based, extreme ultraviolet (EUV) microscope dedicated to photomask research. SHARP emulates the illumination and imaging conditions of current EUV lithography scanners and those several generations into the future. An anamorphic imaging optic with increased mask-side numerical aperture (NA) in the horizontal and increased demagnification in the vertical direction has been proposed to overcome limitations of current multilayer coatings and extend EUV lithography beyond 0.33 NA. Zoneplate lenses with an anamorphic 4×/8× NA of 0.55 are fabricated and installed in the SHARP microscope to emulate anamorphic imaging. SHARP’s Fourier synthesis illuminator with a range of angles exceeding the collected solid angle of the newly designed elliptical zoneplates can produce arbitrary angular source spectra matched to anamorphic imaging. A target with anamorphic dense features down to 50-nm critical dimension is fabricated using 40 nm of nickel as the absorber. In a demonstration experiment, anamorphic imaging at 0.55 4×/8× NA and 6 deg central ray angle (CRA) is compared with conventional imaging at 0.5 4× NA and 8 deg CRA. A significant contrast loss in horizontal features is observed in the conventional images. The anamorphic images show the same image quality in the horizontal and vertical directions.
In this paper, we discuss the impact of optimized pupil engineering and photon noise on native defect sensitivity in EUV actinic blank inspection. Native defects include phase-dominated defects, absorber defects, and defects with a combination of phase and absorption behavior. First, we extend the idea of the Zernike phase contrast (ZPC) method and study the impact of optimum phase shift in the pupil plane on native defect sensitivity, showing a 23% signal-to-noise ratio (SNR) enhancement compare to bright field (BF) for a phase defect with 20% absorption. We also describe the possibility to increase target defect SNR on target defect sizes at the price of losing the sensitivity on smaller (non-critical) defects. Moreover, we show the advantage of the optimized phase contrast (OZPC) method over BF EUV actinic blank inspection. A single focus scan from OZPC has better inspection efficiency over BF. Second, we make a detailed comparison between the phase contrast with apodization (AZPC) method and dark field (DF) method based on defect sensitivity in the presence of both photon shot noise and camera noise. Performance is compared for a variety of photon levels, mask roughness conditions, and combinations of defect phase and absorption.
The SHARP High numerical aperture Actinic Reticle review Project is a synchrotron-based, extreme ultraviolet (EUV) microscope dedicated to photomask research. SHARP emulates the illumination and imaging conditions of current EUV lithography scanners and several generations into the future. An anamorphic imaging optic with increased mask side-NA in the horizontal and increased demagnification in the vertical direction has been proposed to overcome limitations of current multilayer coatings and extend EUV lithography beyond 0.33 NA.1 Zoneplate lenses with an anamorphic 4x/8x NA of 0.55 are fabricated and installed in the SHARP microscope to emulate anamorphic imaging. SHARP’s Fourier synthesis illuminator with a range of angles exceeding the collected solid angle of the newly designed elliptical zoneplates can produce arbitrary angular source spectra, matched to anamorphic imaging. A target with anamorphic dense features down to 50-nm critical dimension is fabricated using 40-nm of nickel as the absorber. In a demonstration experiment anamorphic imaging at 0.55 4x/8xNA and 6° central ray angle is compared to conventional imaging at 0.5 4xNA and 8° central ray angle. A significant contrast loss in horizontal features is observed in the conventional images. The anamorphic images show the same image quality in the horizontal and vertical directions.
We evaluate the performance of several phase retrieval algorithms using through-focus aerial image measurements of patterned EUV photomasks. Patterns present a challenge for phase retrieval algorithms due to the high- contrast and strong diffraction they produce. For this study, we look at the ability to correctly recover phase for line-space patterns on an EUV mask with a TaN absorber and for an etched EUV multilayer phase shift mask. The recovered phase and amplitude extracted from measurements taken using the SHARP EUV microscope at Lawrence Berkeley National Laboratory is compared to rigorous, 3D electromagnetic simulations. The impact of uncertainty in background intensity, coherence, and focus on the recovered field is evaluated to see if the algorithms respond differently.
In this paper, we present a detail study of the impact of material-induced phase effect on the EUV mask absorber defect through-focus behavior. Illumination, material properties, and defect size are shown to have different impacts on the behavior. Also, we study the possibility of using alternative absorber materials to reduce the phase effects on the defect. Based on the mask near field distribution, energy confinement and phase accumulation can be reduced with new absorber materials. The defect sensitivity is reduced and the peak signal position is closer to the best focus due to less material-induced phase. Moreover, the novel pupil engineering method can utilize the phase induced by the material to improve the defect sensitivity of absorber defect by adding lens phase shifts in the pupil plane. At least 29% enhancement of the absorber defect signal at focus can be achieved by optimum lens phase shifts.
In this paper, we present an experimental verification of Zernike phase contrast enhanced EUV multilayer (ML) blank defect detection using the SHARP EUV microscope. A programmed defect as small as 0.35 nm in height is detected at focus with signal to noise ratio (SNR) up to 8. Also, a direct comparison of the through-focus image behavior between bright field and Zernike phase contrast for ML defects ranging from 40 nm to 75 nm in width on the substrate is presented. Results show the advantages of using the Zernike phase contrast method even for defects with both phase and absorption components including a native defect. The impact of pupil apodization combined with Zernike phase contrast is also demonstrated, showing improved SNR is due to the stronger reduction of roughness dependent noise than defect signal, confirming our previous simulation results. Finally we directly compare Zernike phase contrast, dark field and bright field microscopes.
Extreme Ultraviolet (EUV) Lithography mask defects were examined on the actinic mask imaging system, SHARP, at Lawrence Berkeley National Laboratory. A quantitative phase retrieval algorithm based on the Weak Object Transfer Function was applied to the measured through-focus aerial images to examine the amplitude and phase of the defects. The accuracy of the algorithm was demonstrated by comparing the results of measurements using a phase contrast zone plate and a standard zone plate. Using partially coherent illumination to measure frequencies that would otherwise fall outside the numerical aperture (NA), it was shown that some defects are smaller than the conventional resolution of the microscope. Programmed defects of various sizes were measured and shown to have both an amplitude and a phase component that the algorithm is able to recover.
The authors are expanding the capabilities of the SHARP microscope by implementing complementary imaging modes. SHARP (the SEMATECH High-NA Actinic Reticle Review Project) is an actinic, synchrotron-based microscope dedicated to extreme ultraviolet photomask research. SHARP’s programmable Fourier synthesis illuminator and its use of Fresnel zoneplate lenses as imaging optics provide a versatile framework, facilitating the implementation of diverse modes beyond conventional imaging. In addition to SHARP’s set of standard zoneplates, we have created more than 100 zoneplates for complementary imaging modes, all designed to extract additional information from photomasks, to improve navigation, and to enhance defect detection. More than 50 new zoneplates are installed in the tool; the remaining lenses are currently in production. We discuss the design and fabrication of zoneplates for complementary imaging modes and present image data, obtained using Zernike phase contrast and different implementations of differential interference contrast (DIC). First results show that Zernike phase contrast can significantly increase the signal from phase defects in SHARP image data, thus improving the sensitivity of the microscope. DIC is effective on a variety of features, including phase defects and intensity speckle from substrate and multilayer roughness. The additional imaging modes are now available to users of the SHARP microscope.
The authors are expanding the capabilities of the SHARP microscope by implementing complementary imaging modes.
SHARP (the SEMATECH High-NA Actinic Reticle review Project) is an actinic, synchrotron-based microscope
dedicated to extreme ultraviolet (EUV) photomask research. SHARP’s programmable Fourier Synthesis Illuminator and
its use of Fresnel zoneplate lenses as imaging optics provide a versatile framework, facilitating the implementation of
diverse modes beyond conventional imaging. In addition to SHARP’s set of standard zoneplates, we have created more
than 100 zoneplates for complementary imaging modes, all designed to extract additional information from photomasks,
improve navigation and enhance defect detection. More than 50 new zoneplates are installed in the tool; the remaining
lenses are currently in production. In this paper we discuss the design and fabrication of zoneplates for complementary
imaging modes and present image data, obtained using Zernike Phase Contrast and different implementations of
Differential Interference Contrast.
In this paper, we present a complete study on mask blank and patterned mask inspection utilizing the Zernike phase
contrast method. The Zernike phase contrast method provides in-focus inspection ability to study phase defects with
enhanced defect sensitivity. However, the 90 degree phase shift in the pupil will significantly reduce the amplitude
defect signal at focus. In order to detect both types of defects with a single scan, an optimized phase shift instead of 90
degree on the pupil plane is proposed to achieve an acceptable trade-off on their signal strengths. We can get a 70% of its
maximum signal strength at focus for both amplitude and phase defects with a 47 degree phase shift. For SNR, the tradeoff
between speckle noise and signal strength has to be considered. The SNR of phase and amplitude defects at focus can
both reach 11 with 13 degree phase shift and 50% apodization. Moreover, the simulation results on patterned mask
inspection of partially hidden phase defects with die-to-database inspection approach on the blank inspection tool show
that the improvement of the Zernike phase method is more limited. A 40% enhancement of peak signal strength can be
achieved with the Zernike phase contrast method when the defect is centered in the space, while the enhancement drops
to less than 10% when it is beneath the line.
In this paper, we address a new inspection method which provides in-focus inspection capability and higher defect sensitivity compared with conventional mask inspection methods. In the Zernike phase contrast microscope, an added phase shift to background wave combines with the phase of bump and pit defects to achieve higher contrast at focus. If we use a centralized apodization to half the lens radius to further reduce the intensity of the phase-shifted background wave, the signal strength can be improved up to 6-fold of its original value. Simulation results further show that this apodization for a typical EUV mask power spectral density results in the noise decreasing in absolute level similar to the clear field reference signal. Thus large improvements in signal to noise ratios are possible with the Zernike phase contrast microscope type systems for EUV mask inspection applications.
We investigated the phenomena of a metallic photonic crystal (MPC) immersed in liquid crystal. According to our
design, the photonic crystal has specific photonic band gap (PBG) and can be utilized as a filter. The device is filled with
nematic liquid crystal (NLC), MDA-00-3461. The refractive indices of NLC can be magnetically controlled by
reorienting the NLC molecules. Consequently, the corresponding PBG and the filtering performance of the device are
tunable. According to our experimental results, the low frequency boundary of PBG at 0.121 THz can be blue shifted by
6.17 GHz, and the high frequency boundary of PBG at 0.175 THz can be shifted to the blue by 11.04 GHz. As a tunable
THz filter, the peak transmittance at 0.187 THz can be blue shifted by 3.66 GHz.
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