Recent progress in source development for extreme UV lithography

The continuation of Moore's law for semiconductor fabrication envisages the introduction of extreme ultraviolet lithography (EUVL) based on a source wavelength of 13.5 nm for high-volume manufacturing within the next few years. While exposure tools have already been developed and the feasibility of the technology well demonstrated, the key source requirement in terms of power output remains to be achieved. Currently, sources based on laser-produced plasmas from tin droplet targets appear to be the most promising and are being deployed in manufacturing tools. Progress in CO2 laser design aimed at increasing conversion efficiency to close to 5% should make possible the attainment of greater than 200 W of in-band optical power. Recently, research has commenced on the development of sources operating at a wavelength near 6.7 nm for beyond 13.5 nm lithography and gadolinium has been identified as the fuel of choice. The results of these experiments are described and show many similarities to the behavior of tin plasmas as essentially the same atomic and plasma processes are involved, albeit at an electron temperature close to a factor of three higher.

[1]  Tamotsu Abe,et al.  Development of laser-produced plasma-based EUV light source technology for HVM EUV lithography , 2012, Advanced Lithography.

[2]  Paul Sheridan,et al.  Robust liquid metal collector mirror for EUV and soft x-ray plasma sources , 2010, Optical Engineering + Applications.

[3]  S S Churilov,et al.  Analysis of the spectra of In XII–XIV and Sn XIII–XV in the far-VUV region , 2006 .

[4]  Klapisch,et al.  Interpretation of the quasicontinuum band emitted by highly ionized rare-earth elements in the 70-100-Å range. , 1987, Physical review. A, General physics.

[5]  Farrokh Najmabadi,et al.  Interaction of a $\hbox{CO}_{2}$ Laser Pulse With Tin-Based Plasma for an Extreme Ultraviolet Lithography Source , 2010, IEEE Transactions on Plasma Science.

[6]  S. S. Harilal,et al.  Efficient laser-produced plasma extreme ultraviolet sources using grooved Sn targets , 2010 .

[7]  Toyohiko Yatagai,et al.  Rare-earth plasma extreme ultraviolet sources at 6.5―6.7 nm , 2010 .

[8]  A. Cummings,et al.  13.5 nm extreme ultraviolet emission from tin based laser produced plasma sources , 2006 .

[9]  Chihiro Suzuki,et al.  Tungsten spectra recorded at the LHD and comparison with calculations , 2010 .

[10]  Chihiro Suzuki,et al.  Analysis of EUV spectra of Sn XIX–XXII observed in low-density plasmas in the Large Helical Device , 2010 .

[11]  G. Tonon,et al.  X‐ray emission in laser‐produced plasmas , 1973 .

[12]  Franck Gilleron,et al.  Modeling of EUV emission from xenon and tin plasma sources for nanolithography , 2006 .

[13]  Jack Sugar,et al.  Spectra of Ag i isoelectronic sequence observed from Er 21+ to Au 32+ , 1993 .

[14]  Chihiro Suzuki,et al.  Transitions and the effects of configuration interaction in the spectra of Sn XV –Sn XVIII , 2009 .

[15]  Toyohiko Yatagai,et al.  Systematic investigation of self-absorption and conversion efficiency of 6.7 nm extreme ultraviolet sources , 2010 .

[16]  Bowen Li,et al.  Extreme ultraviolet source at 6.7 nm based on a low-density plasma , 2011 .

[17]  Mark S. Tillack,et al.  Two dimensional expansion effects on angular distribution of 13.5nm in-band extreme ultraviolet emission from laser-produced Sn plasma , 2008 .

[18]  Mark S. Tillack,et al.  Optimization of the size ratio of Sn sphere and laser focal spot for an extreme ultraviolet light source , 2008 .

[19]  Hiroaki Nishimura,et al.  4d-4f unresolved transition arrays of xenon and tin ions in charge exchange collisions , 2007 .

[20]  A. Cummings,et al.  Simplified modeling of 13.5 nm unresolved transition array emission of a Sn plasma and comparison with experiment , 2005 .

[21]  S S Churilov,et al.  EUV spectra of Gd and Tb ions excited in laser-produced and vacuum spark plasmas , 2009 .

[22]  Padraig Dunne,et al.  Angular emission and self-absorption studies of a tin laser produced plasma extreme ultraviolet source between 10 and 18 nm , 2008 .

[23]  S S Churilov,et al.  Analyses of the Sn IX–Sn XII spectra in the EUV region , 2006 .

[24]  Mark S. Tillack,et al.  Cavity formation in a liquid Sn droplet driven by laser ablation pressure for an extreme ultraviolet light source target , 2011 .

[25]  Toshihisa Tomie,et al.  Enhancement of EUV emission intensity from particles in a droplet by exploding the droplet , 2009 .

[26]  F de Gaufridy de Dortan,et al.  Influence of configuration interaction on satellite lines of xenon and tin in the EUV region , 2007 .

[27]  Deirdre Kilbane,et al.  Transition wavelengths and unresolved transition array statistics of ions with Z = 72–89 , 2011 .

[28]  Tatsuya Aota,et al.  Ultimate efficiency of extreme ultraviolet radiation from a laser-produced plasma. , 2005, Physical review letters.

[29]  Jack Sugar,et al.  Rh i isoelectronic sequence observed from Er 23+ to Pt 33+ , 1993 .

[30]  Jack Sugar,et al.  Observation of Pd-like resonance lines through Pt 32+ and Zn-like resonance lines of Er 38+ and Hf 42+ , 1993 .

[31]  Luke McKinney,et al.  Variable composition laser-produced Sn plasmas—a study of their time-independent ion distributions , 2004 .

[32]  E. Sokell,et al.  UTA versus line emission for EUVL: studies on xenon emission at the NIST EBIT , 2004 .

[33]  Sho Amano,et al.  Laser wavelength dependence of extreme ultraviolet light and particle emissions from laser-produced lithium plasmas , 2008 .

[34]  Johan Wallin,et al.  Status of the liquid-xenon-jet laser-plasma source for EUV lithography , 2002, SPIE Advanced Lithography.

[35]  Gerry O'Sullivan,et al.  Extreme ultraviolet emission spectra of Gd and Tb ions , 2010 .

[36]  A. Cummings,et al.  A spatio-temporal study of variable composition laser-produced Sn plasmas , 2006 .

[37]  R. D. Cowan,et al.  The Theory of Atomic Structure and Spectra , 1981 .

[38]  Gerry O'Sullivan,et al.  Ground-state configurations and unresolved transition arrays in extreme ultraviolet spectra of lanthanide ions , 2010 .

[39]  Judon Stoeldraijer,et al.  EUV lithography at chipmakers has started: performance validation of ASML's NXE:3100 , 2011, Advanced Lithography.

[40]  Hiroyuki Furukawa,et al.  Theoretical investigation of the spectrum and conversion efficiency of short wavelength extreme-ultraviolet light sources based on terbium plasmas , 2010 .

[41]  Kunioki Mima,et al.  Optimum laser pulse duration for efficient extreme ultraviolet light generation from laser-produced tin plasmas , 2006 .

[42]  G. O'Sullivan,et al.  Tunable narrowband soft x-ray source for projection lithography , 1994 .

[43]  D. Attwood Soft X-Rays and Extreme Ultraviolet Radiation , 1999 .

[44]  Katsunobu Nishihara,et al.  Optimization of Extreme Ultraviolet Emission from Laser-Produced Tin Plasmas Based on Radiation Hydrodynamics Simulations , 2008 .

[45]  Bruno M. La Fontaine,et al.  LPP source system development for HVM , 2011, Advanced Lithography.

[46]  Joseph Reader,et al.  High-resolution spectrum of xenon ions at 13.4 nm. , 2003, Optics letters.

[47]  Bowen Li,et al.  Gd plasma source modeling at 6.7 nm for future lithography , 2011 .

[48]  Kunioki Mima,et al.  Pure-tin microdroplets irradiated with double laser pulses for efficient and minimum-mass extreme-ultraviolet light source production , 2008 .

[49]  Georg Soumagne,et al.  Enhancement of extreme ultraviolet emission from a CO2 laser-produced Sn plasma using a cavity target , 2007 .

[50]  Hiroyuki Furukawa,et al.  Plasma physics and radiation hydrodynamics in developing an extreme ultraviolet light source for lithographya) , 2008 .