This page contains topics that are good to know if you want to contribute to this project.
The Rayleigh criterion is a measure of the limit at which two points of light can be distinguished as separate. It states that two points are resolvable when the principal diffraction maximum of one image coincides with the first minimum of the other. In simpler terms, it defines the smallest angular separation at which two light sources appear distinctly separate rather than as a single blurred point. This criterion helps in understanding the resolving power of optical instruments. When the Rayleigh criterion is expressed in terms of the numerical aperture, the equation becomes:
d=NA0.61λ
where:
d is the minimum resolvable spot size,
λ\lambda is the wavelength of light,
NA is the numerical aperture of the lens.
For blu-ray the wavelength is 405nm and the NA is 0.85 resulting in a spot size of 290nm.
Video explanation of resolution in optics (relevant info starts at 27:15 but the entire video is a great introduction to optics) https://www.youtube.com/watch?v=sTa-Hn_eisw
The minimum feature size in transistors, often referred to as the "technology node" or "process node," represents the smallest dimension of a transistor on a semiconductor chip. This size is measured in nanometers (nm) and dictates how densely transistors can be packed on a chip, which in turn influences the chip's performance, power consumption, and overall size.
1968
20,000 nm
100 nm
20,000 nm
1971
10,000 nm
100 nm
10,000 nm
1974
6,000 nm
100 nm
6,000 nm
1977
3,000 nm
100 nm
3,000 nm
1981
1,500 nm
100 nm
1,500 nm
1984
1,000 nm
100 nm
1,000 nm
1987
800 nm
100 nm
800 nm
1990
600 nm
100 nm
600 nm
1993
350 nm
100 nm
350 nm
1996
250 nm
100 nm
250 nm
1999
180 nm
100 nm
180 nm
2001
130 nm
100 nm
130 nm
2003
90 nm
100 nm
90 nm
2005
65 nm
100 nm
65 nm
2007
45 nm
100 nm
45 nm
2009
32 nm
100 nm
32 nm
2010
28 nm
100 nm
28 nm
2012
22 nm
100 nm
22 nm
2014
14 nm
100 nm
14 nm
2016
10 nm
100 nm
10 nm
2018
7 nm
100 nm
7 nm
2020
5 nm
100 nm
5 nm
2022
3 nm
100 nm
3 nm
Note: It is recommended to keep the cover layer, whose thickness depends on the operation wavelength, in front of the OPU objective lens to guarantee optimal laser focusing. Microscopy cover glasses provide a similar refractive index (1.47 to 1.5) as the cover layer or one can simply use the disc hard-coat polycarbonate cover layer. Furthermore, the cover layer can be used for sealing microfluidic channels. OPU-based imaging or sensing through different media, such as liquid or gas, demands the optimization of the distance between the cover layer and measurement target
Optical pickups focus on disc using the so called astigmatic method. This method is based on the deformation of the roundness of the laser beam when it is unfocused. The pickup has a series of lenses that lead the reflected ray to a photodiode array which generates four signals (A,B,C,D). Using them it is possible to deduct if the laser is unfocused and move the lens to focus it correctly.
Once you know the A,B,C,D signal pins, implementing the auto-focus algorithm is easy: just add A+C and subtract B+D from the result. The pickup returns those signals in the form of minimum current variations that depend on the laser light received by each photodiode. The photodiodes are arranged in a square (see following figure).
As you can see, it is possible to infer the focus level checking if the result is less than 0 (too close) equal to zero (focused) or greater than zero (too far) and with this information move the lens until the laser is focused.
http://www.diyouware.com/node/161 https://pmc.ncbi.nlm.nih.gov/articles/PMC6066758/
The minimum needed step size can be determined by the perimeter of the writing area and the minimum spot size
For the largest radius (58mm) the perimeter is 364mm
For the smallest radius (23mm) the perimeter is 144mm
From there number of steps is calculated by:
Assuming a 290nm spot size:
For the largest radius (58mm) the number of steps is 1.256M
For the smallest radius (23mm) the number of steps is 498k
The planned approach for repeatability is closed loop control. Since the blu-ray system works on reading concentric circles each disc will have a pattern written along the ring perimeter that identifies what is the current ring radius. It will also be used to help identify the start position on the perimeter.
Since this project plans to use a blu-ray drive, the working area is basically the entire readable area of a disc (including table of contents).
The start of the writing area for a disc is 46mm in diameter or 23mm in radius.
The end of the writing area for a disc is 116mm in diameter or 58mm in radius.
Therefore the writing radius is about 35mm.
5x Symmetrical dies can fit on a disc assuming 30mm x 30mm (900mm^2)
4x Asymmetrical dies can fit on a disc assuming 25mm x 50mm ( 1,250mm^2 )
To calculate how fast the disc needs to spin we first need to know how fast the spot we need to image is moving. the speed is dependent on how far we are from the center of the disc.
If we assume a random rotational speed in revolutions per minute (rpm), we can use the following steps to calculate how fast the imaging spot is moving:
Convert rpm to revolutions per nano-second (rpns):
Calculate the linear speed in nano-meters per nano-second (nm/ns):
Assuming the disc is spinning at 500rpm:
The smallest inner radius of the disc (23mm) is moving at roughly 1.24nm/ns
The largest outer radius of the disc (58mm) is moving at roughly 3.03nm/ns
http://educypedia.karadimov.info/library/general_bluraydiscformat-15263.pdf
https://blog.ligos.net/images/The-Reliability-Of-Optical-Disks/White_Paper_BD-RE_5th_20180216.pdf
This is a 3 part video series where Doctor Volt dissects a Blu-ray player to figure out how to make a laser scanning microscope out of it.
https://www.youtube.com/watch?v=liGuhbFh4IQ
https://www.youtube.com/watch?v=Hkialty_8K4&t=267s
https://backend.orbit.dtu.dk/ws/files/239879723/SSDM2020_Abstract_Edwin.pdf
#Paper
#Video
https://www.youtube.com/watch?v=Fw8r5FBaPTI&t=1281s
https://www.youtube.com/watch?v=5bqujaldaCQ
STED Microscopy https://www.youtube.com/watch?v=1pgpzHao1c0
Two-beam OBL utilizes a doughnut-shaped inhibition beam to inhibit the photopolymerization triggered by the writing beam at the doughnut ring leading to reduced feature size and improved resolution https://www.nature.com/articles/ncomms3061
Super-resolved critical dimensions in far-field I-line photolithography https://www.spiedigitallibrary.org/journals/journal-of-micro-nanolithography-mems-and-moems/volume-18/issue-1/013505/Super-resolved-critical-dimensions-in-far-field-I-line-photolithography/10.1117/1.JMM.18.1.013505.short
perimeter=2∗π∗radius
steps=minspotsizeperimeter
rpns=60∗109rpm
Linearspeed(nm/ns)=radius(nm)×2×π×rpns
Possible STED Architecture Diagram of BSM. The fluorescence signal passes through multimode fiber B7 and is collimated by collimator lens B8 and narrowband emission filter B9. D1, laser diode; D2, beam splitter; D3, collimator lens; D4, dichroic filter; D5, photodiode; D6, objective lens (NA: 0.6); D7, Al-coated address pattern; B1, blue laser diode; B2, B3, beam splitters; B4, collimator lens; B5, dichroic filter; B6, 4.34 mm focal lens; B10, objective lens (NA: 0.85); B11, lens holder. B12, cover glass; B13, collimator astigmatic plate; B14, photodetector. (https://pmc.ncbi.nlm.nih.gov/articles/PMC6066758/)
