euv maskless lithography j. vac. sci. technol. b 30, 051606 (2012); 9/25/20121k. johnson...

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EUV Maskless Lithography J. Vac. Sci. Technol. B 30, 051606 (2012); http://dx.doi.org/10.1116/1.4752112 9/25/2012 1 K. Johnson [email protected]

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Page 1: EUV Maskless Lithography J. Vac. Sci. Technol. B 30, 051606 (2012);  9/25/20121K. Johnson kjinnovation@earthlink.net

K. Johnson [email protected] 1

EUV Maskless Lithography

J. Vac. Sci. Technol. B 30, 051606 (2012); http://dx.doi.org/10.1116/1.4752112

9/25/2012

Page 2: EUV Maskless Lithography J. Vac. Sci. Technol. B 30, 051606 (2012);  9/25/20121K. Johnson kjinnovation@earthlink.net

K. Johnson [email protected] 2

EUV Maskless Lithography

Concept:• -Scanned-spot array (e.g., 4000-by-4000 array over

10 mm square image field, 2.5 μm spacing)• Spots can be either individually modulated (with an

SLM) or source-modulated (for printing periodic patterns).

9/25/2012

Performance capability (based on JVST-B paper):• ~20 nm print resolution (13.5-nm wavelength, 0.3 NA, EUV source ~40 μm

diameter with 1 steradian collection per image field)• ~30 (300-mm) wafers per hour, with 500 kHz EUV source (“… Using a 10 μm nozzle tin

droplets as small as 17 μm in diameter at a 550 kHz repetition rate have been demonstrated. …” Brandt et al., Ref. 25)

Advantages:• Maskless• Eliminates coherent proximity effects• Comparatively simple optics (e.g., only 2 projection mirrors)• Comparatively moderate EUV power requirement

Page 3: EUV Maskless Lithography J. Vac. Sci. Technol. B 30, 051606 (2012);  9/25/20121K. Johnson kjinnovation@earthlink.net

K. Johnson [email protected] 39/25/2012

Projection Optics

• Two-mirror, flat-image Schwarzschild system• 10-mm square image field• 10-X reduction• 0.3 NA (obscuration: 0.12-NA)

M1

M2

objectsurface

object spot array

detail view 1

Schematic:

Effect of central obscuration on focused image spot:

unobscured

obscured

(Side lobe has relatively minimal effect because image spots do not overlap.)

side lobe

Page 4: EUV Maskless Lithography J. Vac. Sci. Technol. B 30, 051606 (2012);  9/25/20121K. Johnson kjinnovation@earthlink.net

K. Johnson [email protected] 49/25/2012

objectsurface

L0

L1

EUV illumination

microchannelarray

virtualobject spot

L2

aperture

intermediatefocus

Schematic(detail view 1)

detail view 2

Spot-Generation Optics

• Phase-Fresnel microlens arrays (L1 & L2) in achromatic configuration (L0 beam shaper optional)

• Transmittance (including lenses, substrates, fill factor losses) about 20%; no spectral narrowing.

• Can accommodate SLM shutters at intermediate foci.

mm

Microlens Fresnel zone structure at edge of object field

Page 5: EUV Maskless Lithography J. Vac. Sci. Technol. B 30, 051606 (2012);  9/25/20121K. Johnson kjinnovation@earthlink.net

K. Johnson [email protected] 59/25/2012

Microlens Structure

• Stepped Fresnel profile: 8 bilayers of Mo (20 nm) / Ru (2 nm etch stop) on thin Si substrate

• Minimum Fresnel zone width: 0.9 μm• Deposition tolerances: about 26X less stringent than EUV reflection optics• Axial lens positioning tolerance (focus): about 100X less stringent than

EUV reflection optics• Patterning/alignment tolerances: about 10 nm (comparable to EUV

photomasks)

Microlens profile (detail view 2)

Page 6: EUV Maskless Lithography J. Vac. Sci. Technol. B 30, 051606 (2012);  9/25/20121K. Johnson kjinnovation@earthlink.net

K. Johnson [email protected] 69/25/2012

Aberration Compensation

• Microlens design completely eliminates geometric aberration (including image distortion and image field curvature).

• Microlens doublet configuration substantially eliminates chromatic aberration.

Image of object point (at field edge), no aberration correction:

With aberration correction (at 3 wavelengths: 13.4, 13.5, 13.6 nm):

nm nm

Page 7: EUV Maskless Lithography J. Vac. Sci. Technol. B 30, 051606 (2012);  9/25/20121K. Johnson kjinnovation@earthlink.net

K. Johnson [email protected] 79/25/2012

EUV Source and Collection Optics

• Power requirement: modest due to comparatively low throughput (e.g., 30 wph) and few near-normal-incidence mirrors.

• Source size requirement: The scan spots are demagnified images of the source; should be within the diffraction limit. (1 steradian collected from a 40-μm source could be partitioned, e.g., into a 4000-by-4000 array of spots with 1-steradian convergence cones and 10-nm geometric spot size).

• Rep rate requirement: Printing throughput is proportional to the rep rate and number of spots (e.g., with a 500 kHz rep rate, 16 million spots, and 10-nm grid step, the scan rate would be 8 cm2/sec).

• Source power sharing: The source size (area) can be N times larger, and the rep rate N times smaller, if N print units are supplied from a single source. (Throughput per source will be the same as N=1.)

• The microlens design can correct moderate imperfections in the collection optics :

– Non-ideal beam shape.– Nonuniform source magnification across microlens array.– Nonuniform radiant intensity across microlens array.

Page 8: EUV Maskless Lithography J. Vac. Sci. Technol. B 30, 051606 (2012);  9/25/20121K. Johnson kjinnovation@earthlink.net

K. Johnson [email protected] 89/25/2012

EUV Maskless Lithography Development Tasks• Develop system design outline based on realistic, practical source

characteristics:– Source size? (limits print resolution)– Rep rate? (limits printing throughput)– Power? (comparatively moderate power requirement)

• Develop detailed, full-system optical design; simulate lithography performance.

• Evaluate microlens/microchannel fabrication methods.• Evaluate SLM feasibility.• Economic modeling.• Proof-of-concept prototype (e.g., using the CXRO’s MET tool)• Productization options:

– Source-modulated (alternative to interference lithography, GRATE for HVM)– Full image modulation with SLM (alternative to maskless e-beam, e.g., REBL,

MAPPER)– BEUV (Maskless capability and simplified projection optics could facilitate accelerated

development of 6.x-nm lithography.)