Lecture 14 Advanced Photolithography

Transcription

1 Lecture 14 Advanced Photolithography Chapter 14 Wolf and Tauber 1/74

2 Announcements Term Paper: You are expected to produce a 4-5 page term paper on a selected topic (from a list). Term paper contributes 25% of course grade. You should have all been assigned your first-choice topic. The term paper should be handed in at the start of class on Tuesday 21 st November. Details / regulations are on the course website. The term paper will be returned to you in class on Thursday 30 th November. 2/74

3 Useful Links UT-Austin: Review Article on Immersion Lithography: Review Article on Extreme ultraviolet lithography: Review Article on Electron-Beam Lithography: Review Article on Nanoimprint Lithography: 3/74

4 Lecture 14 Review of Lecture 13 Improving Resolution of Optical Lithography. Extreme UV-Lithography. Electron Beam Lithography. Nanoimprint Lithography. 4/74

5 Review of Optical Photolithography 5/74

6 Apply The Photolithography Process Apply photoresist. Expose photoresist through a patterned mask or reticle. Develop PR by immersing it in a solvent which preferentially dissolves the PR of higher solubility. Process the exposed part of the wafer. Strip away the remaining photoresist. Inspect pattern. PR Substrate Mask Strip Etch Develop Expose 6/74

7 Photoresist Deposition Industrially this is done with robotic arms and automated dispensers: Extremely uniform films can be deposited using spin coating (rms roughness ~ Å s) 7/74

8 Exposure Techniques Three approaches are typically taken to exposure: Contact Printing Mask Defects Bowing of mask 1:1 Printing Proximity Printing 2-4 μm resolution Mask space ( 25 mm) Mask lens 2-5 X reduction Printing System Magn. Resolution (μm) Use Contact Research Proximity Low Cost Projection Mainstream VLSI Projection Printing 8/74

9 Fraunhofer Diffraction The resolution in Fraunhofer diffraction is defined by the Rayleigh criterion. Rayleigh Criterion: when the peak of one projection lands on the first zero of the other: 9/74

10 Modulation Transfer Function Intensity at Mask 1 Intensity on wafer 1 I Max I Min 0 Position 0 Position We define MTF: MTF = I max I min I max + I min MTF is defined between 0 (small features) and 1 (large features). Generally, MTF needs to be > 0.5 for the resist to resolve features. 10/74

11 Improving Resolution of Optical Lithography 11/74

12 Optical Lithography State of the Art as of 2009: Half-pitch (half of distance between elements) 12/74

13 Optical Lithography State of the Art as of 2009: 13/74

14 Optical Lithography The next generation of lithography will likely achieved via one of the following approaches: Extreme ultraviolet (EUV) lithography. Electron beam lithography (EPL). Nanoimprint Imprint lithography (NIL). λ ~ nm. However, because of existing infrastructure, it is likely that 193nm-based optical technology will be extended as far as possible. There are a number of techniques that optical lithography can be improved. 14/74

15 Optical Proximity Correction Optical Proximity Correction (OPC): Clever mask engineering based on software algorithms can compensate some of this error. This requires sophisticated computer modeling. 15/74

16 OPC Examples 16/74

17 Phase Shift Masks Until now we talked just about intensity (I) on the light on the mask or wafer. But the wave has an a amplitude, E, which can be negative, positive (or complex). E x, t = A cos kx ωt θ The intensity is the square of the amplitude I = E 2 17/74

18 Phase Shift Masks Masks can be manufactured (albeit expensively) to shift the phase of the light: Mask Amplitude At Wafer 180 o phase shift Intensity 18/74

19 Multilayer Resist Processing Multilayer resists are a way to address depth of focus and modulation issues. E.g. bilayer: Layer to be processed (e.g. etched) Contrast enhancement layer ( nm) Conventional photoresist Substrate The Contrast enhancement layer is photo-bleachable layer, and will change its optical transmittance on exposure to light. Poly(methyl methacrylate) (PMMA) is often employed here: 19/74

20 Multilayer Resist Processing Conventional photoresist Contrast enhancement layer Mask lens Exposed regions become transparent to UV light The top layer (e.g. PMMA) now acts as a contact mask. Without the problems due to metal contamination. 20/74

21 Multilayer Resist Processing Bilayer resists cannot measurably improve resolution. Image on PMMA remains limited by projection printing. Contrast enhancement can improve modulation: Intensity on PMMA 1 I Max Intensity on Wafer 1 I Min 0 Position 0 Position 21/74

22 Multilayer Resist Processing Example of results: Advantages of bilayer processing: Better modulation. Disadvantages of bilayer processing: Increased complexity (cost). 22/74

23 Multilayer Resist Processing Another example is self-aligned sidewall patterning: Reactive ion etch 23/74

24 Multilayer Resist Processing Advantages of self-aligned sidewall patterning: Low cost. High resolution. Disadvantages of self-aligned sidewall patterning: Every feature will have the same linewidth Will create loops. 24/74

25 Multilayer Resist Processing There are many approaches to multi-layer patterning: 25/74

26 Immersion Lithography Recall that for projection printing the resolution is quantified via the Rayleigh Criterion: f = Focal length R = k 1 λ f d d = Lens diameter k 1 is an experimental parameter associated with the system and resist (0.6 <k 1 < 0.8). Alternatively: NA = d f = nsinα α = maximum half angle of incident light: Numerical aperture R = k 1λ NA n = index of refraction (1 in air). α = Maximum half-angle 26/74

27 Immersion Lithography The resolution (Rayleigh Criterion) is inversely proportional to the numerical aperture: R 1 NA NA = nsinα R 1 n So can we increase the refractive index of the medium to improve the resolution? This would be equivalent to reducing the wavelength. This is the approach taken in immersion lithography. 27/74

28 Immersion Lithography The wafer is direction in contact with liquid, which is directly in contact with lens. 28/74

29 Immersion Lithography The basic operation is shown below: Refractive index of air Refractive index of lens n g Refractive index of fluid n 0 Refractive index of resist n f n r The maximum resolution for a system is determined by the lowest refractive index in the glass/fluid/resist stack. Often this is the fluid. 29/74

30 Immersion Lithography If the fluid does have the lowest refractive index, the resolution and depth of focus are given by: R = k 1λ NA = k 1λ n f sinα δ = k 2λ NA 2 = k 2 λ n f sinα 2 Or more generally: R = k 1λ nsinα δ = k 2λ nsinα 2 Where: Refractive index of lens Refractive index of fluid n = Min(n g, n f, n r ) Refractive index of resist 30/74

31 Immersion Lithography Some refractive indices: Material Use Refractive Index SiO 2 Oxide (to etch) 1.56 CaF 2 Lens (for UV) 1.51 Water Immersion Fluid Various Resists Resist ~ /74

32 Example The best conditions for conventional lithography are typically around the following: k 1 = 0.3. sinα = 0.9. λ = 193 nm (ArF). What improvement in resolution would we expect when employing water-based immersion lithography. First determine resolution with standard lithography: R = k 1λ nsinα = = 64 nm Refractive index of air 32/74

33 Example If we use immersion lithography, then we first determine the minimum refractive index: Below the resist is not considered Material Use Refractive Index SiO 2 Oxide (to etch) 1.56 CaF 2 Lens (for UV) 1.51 Water Immersion Fluid Various Resists Resist ~1.70 n = Min(n g, n f, n r ) n = Min(1.51, 1.435,1.70) n = We then proceed as before: 33/74

34 Example All other conditions are the same: k 1 = 0.3. sinα = 0.9. λ = 193 nm (ArF). R = k 1λ nsinα = = 45 nm Refractive index of water This gets us down to 45nm feature size. But for VLSI we now need 22nm (or lower)! 34/74

35 Going Below 45nm We are limited by the minimum refractive index. So we need to increase the refractive of all components together. However we also need the materials to be transparent to UV light (193 nm). Candidate lenses: Material Use Refractive Index CaF 2 Lens 1.51 BaLiF 3 Lens 1.64 Lu 3 Al 5 O 12 - LuAG Lens 2.1 Mg 3 AlSi 3 O 12 Pyrope Lens 2.0 So, we can find lenses which will not be the limiting factor. 35/74

36 Going Below 45nm Immersion Liquid: 36/74

37 Summary of Immersion Liquids Nonspecific IFs Region of interest 37/74

38 Going Below 45nm The difficulty is finding the appropriate immersion fluid (IF). The best we have so far is decalin: This has a refractive index of n = R = 37nm. This is the so-called 2 nd generation IF. 38/74

39 3 rd Generation The current target with immersion lithography is 32 nm. Lens: LuAG (n = 2.1) Resist: n = 1.8. Immersion Fluid: n = 1.9. No candidate material has been for this high refractive index fluid yet. 39/74

40 Extreme UV-Lithography 40/74

41 Extreme UV Lithography (EUV) Sometimes called deep UV Lithography (DUV). As before the resolution is determined by the Rayleigh Criterion: f = Focal length d = Lens diameter R = k 1 λ f d = k 1λ NA = k 1λ nsinα The approach is to reduce wavelength. For ArF lasers λ = 193 nm. We aim for λ = 13.4 nm. Currently in development for VLSI. Numerical aperture 41/74

42 Difficulties: Photoresist: 42/74

43 Difficulties: Lenses: 43/74

44 Difficulties: Even air: 44/74

45 So we Cannot Use Lenses So we cannot use optical lenses. Mirrors have to be employed: Also need a vacuum, to avoid absorption in chamber. 45/74

46 So we Cannot Use Lenses Multilayer high/low index mirrors used to focus light (50 double layer Mo(2.7nm)/Si(4.0nm)). Mask formed by applying absorber to multilayer mirror. 46/74

47 EUV Source The EUV source must provide sufficient power at the desired wavelength to yield an adequate wafer throughput for a lithography tool. Producing ~10nm radiation is not trivial. Options include: Laser-produced-plasma (LPP). Synchrotron radiation. High-harmonic generation with femtosecond laser pulses. X-Ray lasers. Electron beam driven radiation devices Most are not capable to W of EUV source power at acceptable manufacturing costs. 47/74

48 EUV Source The EUV source must provide sufficient power at the desired wavelength to yield an adequate wafer throughput for a lithography tool. Producing ~10nm radiation is not trivial. Options include: Laser-produced-plasma (LPP). Synchrotron radiation. High-harmonic generation with femtosecond laser pulses. X-Ray lasers. Electron beam driven radiation devices Most are not capable to W of EUV source power at acceptable manufacturing costs. 48/74

49 EUV Source Laser-produced-plasma (LPP) turns out to be the most promising source. The LPP sources are formed by focusing a pulsed (optical) laser beam onto a solid, liquid, or gas target to produce a bright spark which has broad emission from the visible to the EUV. The LPP produces a point-like source converting 0.8% - 3.8% of the incident laser power into EUV light in the required spectral bandwidth. High-repetition-rate (3 khz) pulsed laser drivers that deliver 1500 W average power to create the Xe plasma are actively being developed commercially. 49/74

50 Optics Again, because of the extreme wavelength, the choice of mirror requires careful consideration. The materials must be chosen to be highly reflective at the chosen wavelength. Bilayer Mo/Si and Mo/Be are currently most promising. Mirrors must also be extremely flat. Rms roughness λ. Typically total sum of roughness ~ 10 Å E.g. 4 mirrors 2.5Å rms roughness per mirror. 50/74

51 Masks Masking is in theory relatively straight-forward, since most solids absorb at ~13nm. Mask formed by applying absorber to multilayer mirror. Typically Al, Ti, on the mirror surface. Patterned with e-beam lithography. The challenge for EUV mask blank fabrication is defect reduction. 51/74

52 Resists There is strong attenuation of 13.4 nm in all organic resist materials. The absorption is atomic (not by the bonds), and will not convert the materials predictably. The radiation will not penetrate through a thick photoresist. Resist must also be stable in a vacuum. Organic resist can also collapse at small linewidths: Pattern collapse on a 70 nm pitch with dose of 1.65 nc/cm 52/74

53 Resists Inorganic resists are candidates E.g. HfSOx. Advantages of inorganic resists: High etch resistance. Thin layers minimize pattern collapse. High resolution and low line edge roughness. 21 nm Residual material Patterned HfSOx 50 nm 53/74

54 Electron Beam Lithography 54/74

55 Electron Beam Lithography As with EUV lithography, the purpose of e - beam lithography is to reduce the wavelength on the incident particles. λ < 1Å. So diffraction is no longer a problem. Pattern direct written into resist by scanning e-beam. Essentially is just like an SEM: On-off capability. Pixilation. Accurate Positioning. 55/74

56 Research e-beam Lithography Often a modified SEM is employed. When imaging you can damage the material being imaged when using high energies. 1nm spot size. 10nm resolution is routinely achieved. A computer is used to design patterns. PMMA is often used as a resist. 3-5 nm 56/74

57 Sources Low energy: thermionic source (heated filament). Tungsten. Lanthanum hexaboride (LaB 6 ). High energy: field-emission source. These are reasonably complex, but basically electrons are pulled off of metal by a very large electric field. Require a high vacuum and are difficult to fabricate. 57/74

58 Electron Wavelength For low velocity electrons the wavelength would be given by the de Broglie Equation: λ = h 2m 0 ev Where: λ = Electron wavelength. h = Planck Constant. e = Charge on electron. V = Accelerating voltage. m 0 = Rest mass of electron. 58/74

59 Electron Wavelength However, at high voltages we are accelerating electrons to appreciable percentages of the speed of light. So instead we must use the relativistic equation for wavelength: Where: λ = h 2m 0 ev c = Speed of light in vacuum ev 2m 0 c 2 Relativistic correction 59/74

60 Example If we accelerate electrons with a 200kV source, what is the difference in wavelength calculated with and without considering special relativity? Start with our non-relativistic equation: λ nr = h 2m 0 ev nr for nonrelativistic V = 200 kv is the only parameter not a fundamental constant: λ nr = λ nr = m λ nr = 2.74pm V = 200 kv 60/74

61 Example Now consider relativistic equation: r for relativistic λ r = λ r = 1 + h 2m 0 ev λ r = λ nr ev 2m 0 c ev 2m 0 c λ r = /1.09 λ r = m λ r = 2.51pm 61/74

62 Example So the results are: λ nr = 2.74pm λ r = 2.51pm Hence the effect of relativity is non-negligible at these high energies. 62/74

63 Electron Column After electrons are accelerated they are directed using electromagnetic lenses. Beam blanker is used to divert the electron beam from the optical axis of the column thus preventing electrons from reaching the sample surface. Ability to focus the electron beam limits the resolution. Sample stage is moved mechanically. 63/74

64 e-beam Lithography for VLSI Advantages: No mask needed computer controlled electro-magnetic lenses define features. Extremely accurate layer registration. Diffraction effects are not a factor. Resolution is good (3-10nm in lab). Disadvantages: Extremely slow throughput (50 slower than optical lithography!). Expensive, and expensive facilities. 64/74

65 Nanoimprint Lithography 65/74

66 Nano-Imprint Lithography Nano-Imprint Lithography (NIL) is a very simple concept: A hard mold that contains nanoscale surface-relief features is pressed into a polymeric material cast on a substrate. This creates a thickness contrast in the polymeric material. A thin residual layer of polymeric material is intentionally left underneath the mold protrusions. This acts as a cushioning layer that prevents direct impact of the hard mold on the substrate. 66/74

67 Nano-Imprint Lithography It s very easy to achieve high-resolution using NIL: 67/74

68 Step-and-Flash Imprint A variation is called step and flash imprint lithography (SFIL). Uses a transparent mold and UV-curable precursor liquid to define the pattern. Can be carried out at room temperature. 68/74

69 Mold Fabrication The mold is fabricated using a combination of reactive ion etching and lift-off. The mold is formed of a hard material (such as SiO 2 ). 69/74

70 Nano-Imprint Lithography Advantages: Low cost of ownership (COO). High precision. Complex patterns are possible. Disadvantages: Reproducibility is low. Contamination (contact with resist). Not industrially scaled (although system do exist). 70/74

71 Adhesion Lithography One example of very low-resolution features. Employ self-assembled monolayers (SAMs): ~nm Can be applied onto the surface of metals. Self-assemble into monolayers. 71/74

72 Adhesion Lithography 72/74

73 Adhesion Lithography 73/74

74 Adhesion Lithography 74/74