1) In this part, it'll be talked about 2 properties that precise physical definitions of those don't matter. One of them is 'color' and the other one is 'hardness'. It happens to be an empirical fact that the color and hardness of properties of particles can assume only 2 possible values: white/black and hard/soft. No experiment has shown that there are any other values other than these.
We can build a color box such that if the particle that enters the entrance of the box is measured white, it'll go through one aperture and if the particle is measured black, it'll go through the other one. If the particle is measured black/white in a color box, it'll be measured black/white in a second color box and so on. These are also valid for a hardness box.
One might be curious about the possibility of relation of these properties with each other. One relation might be correlation and we can check if there is a correlation between the properties with our boxes. If we check, we see that there is no such correlation. For example, if we put bunch of white particles into the hardness box, statistically half of them will be measured hard and the other half will be measured soft. This is valid if the particles were black or if the particles were hard/soft and put into a color box.
Now suppose a particle goes through 3 boxes such that 2 of them are color and one of them is a hardness box. The boxes will be replaced such that a particle firstly goes through the color box firstly, then a hardness box, and again goes through another color box lastly. Of course for every outcome, there must be more than 3 boxes(7 boxes). I drew the experiment
so if the measurement done in a hardness box doesn't have an impact on the color of the particle, we expect that 1, 4, 7, 8 baskets will be empty because the measured color in the last box is different from the measured color in the first box. Statistically, in each of 2,3,5,6 boxes there will be %25 of the particles. However, it is not what happens, actually we see that in each of every box there are %12.5 of the particles. It shows that the measurement done in a hardness box does have an impact on the color of the particles. This means the half of the particles measured black in the first box will be measured white and other half will be measured black. So we know half of the black particles changes their color, this fact raises the question 'what determines the half of the black particles changed their color and the other half don't?". This question seems to have no answer because, as I understand, there is no physical difference between the black particles that were measured white in the first box and the black particles that were measured black in the first box. Another question raises 'May there be a hardness box such that changed the color property of the particles or changed statistically different from we showed here?'. Hardness box can be built in a number of entire ways and all of them will produce the same statistics.
Note: Albert says it's striking that we can't even change the statistics one millionth of one percentage point away, but how can we say such a absolute thing when we talk about statistics?
Since the one information about one property disrupts the other property, we can't say something like "the particle X is now black and soft". It's called uncertainty principle, some properties that act like the hardness and color are called 'incompatible'.
Now suppose an experiment such as
Mirrors in the experiment only there to change the direction of the particles that come out of hardness box but the mirrors or anything between the boxes does not change anything else. If we sent white particles to the hardness box, the half of them will take the path s and the other half will take the path h and also if we sent hard particles to the hardness box, it will take h path and if we measure its color at 'h and s, the half of them will be measured white and other half will be measured black. The interesting happens as follows, suppose we sent again white particles to the hardness box . We know the one half will take h path and other one will take s path. If we measure their color before reaching the black box, it will be 50-50 black and white in each path as we do in the previous experiment which we used 7 boxes. However, if we measure the color of the particles. However, if we measure color of the particles at 'h and s', all of them will be measured white. Suppose now we have a wall which we can put in the middle of paths. If we put the wall into the path, which means we block soft particles, only the half of the particles at 'h and s' will be white. If we put the wall in to the h path, which means we block hard particles, again only the half of the particles at 'h and s' will be measured white. However, if we don't block the particles, all of them will be measured white. If we ask ourselves "when there is no block in paths, which path particles we measure white all of them at 'h and s'?". It can't be h or s paths because when we measure the particles at h or s, their color will be 50-50 black/white. Can it be both paths? Well, if we sent particles one by one and measure their paths for each particle, we find half of the particles take path h and the other half take s but not both. The answer is superposition, which something we don't understand. We know, by the experiment, the particles come out of hardness box as hard/soft only if they're hard/soft particles when they enter the box. When a white particle goes into the hard box, it comes out of neither hard aperture nor soft aperture nor both neither. So saying a particle is white must be the same thing as saying the particle is the superposition of hard and soft. Remember that the knowing or blocking the path of individual photons change their probability of position on the screen.
Note: It seems if we don't know what kind of hardness the individual particles have(or measured last time), the measurement of hardness doesn't have an impact on the color of the particles.
Note 2: The properties act like hardness/color seem are not absolute property but depend on the measurement.
Note 3: David Albert asks which path white particles take, but another question also comes to my mind "What happened to the black ones?".
Chapter 2: Mathematical Formalism