Using Light to Make Processors with Features Smaller than It's Wavelength?

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Photolithography allows for the creation of processor features smaller than the wavelength of light, such as using 200nm light to produce 65nm features. This is achieved through techniques like phase masks and near-field contact mode, which manipulate light's behavior beyond traditional ray optics. Numerical aperture relates to the lens's ability to collect light, impacting diffraction and spot size; a larger lens reduces diffraction effects. At sub-wavelength scales, traditional optics assumptions break down, necessitating a return to full-wave electromagnetic solutions to Maxwell's equations. Understanding these principles is crucial for advancing photolithography technologies.
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I've been reading up on photolithography trying to understand how processors with sub-wavelength features can be made through photolithography, but I just don't get it.

Can someone please help me by explaining in a conceptual way how light with a wavelength of, say, 200nm can be used to make a processor with 65nm features? Even with a large lens used to focus the light, you still can't make a point smaller than the wavelength of the light being focused, right?

Thank you so much!

Also, what is meant by numerical aperture in regards to a lens? Wikipedia didn't help me understand this.
 
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The photolithography guys use a lot of tricks- using a phase mask (as opposed to intensity masks) is one technology, near-field contact mode is another. There are more exotic technologies under development. The mechanisms by which these technologies work are quite complex.

Loosely speaking, numerical aperture is a relationship between the focal length and diameter of a lens. Recall that diffraction occurs as a result of limiting the spatial extent of a wavefront. Collecting more of the wavefront (by increasing the diameter of the lens) means that diffraction effects are reduced, leading to a smaller spot size.
 
Basically, use a big lens, plus some other tricks, for projection lithography. There is nothing limiting a focal spot size to the dimension of a wavelength, though in practice it becomes increasingly challenging to do this.
 
When you go to sizes smaller then a light beam's wavelength, the electromagnetic fields of the light do not just disappear and become unusable. Rather, at sub-wavelength sizes, our neat intuitive picture of light being a bundle of rays traveling in straight lines and bouncing off things like billiard balls breaks down. For example, the air molecules in the sky are sub-wavelength to most of sunlight's spectrum, yet we have no problem seeing the blue sky. All that is required at sub-wavelength sizes is to return to full-wave electromagnetic solutions to Maxwell's equations and avoid assumptions or mental constructs from the world of optics (easy to do in principle, hard to do practice). When you go sub-wavelength, you have to really know what the electromagnetic fields are doing (typically using numerical em codes), and not just ray-trace.
 
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