I guess mine was too bad, or too hidden :(.
The numbers remind me of a story I saw a while ago (not sure if it really happened): Some students released three pigs at a university, and had them labeled as "1", "2" and "4". The search for pig "3" took quite some time!Problem 4 needs some love. I'll assume that a detection has the same probability for all x between 1 and 20, otherwise we have insufficient information to start working on it. As we do not know the total number of particles, the distribution in the interval is the only thing we can use. We expect an exponential distribution, this is invariant under shifts, so for simplicity subtract 1 from all measured values and the range, we measure from 0 to 19. Unfortunately, within the small experimental sample, the best fit is a flat distribution. Looking at the data, this is not surprising as we have 4 out of 6 decays in the second half. We cannot set an upper limit on λ. For each event, we can calculate a likelihood:
$$L(x)=\frac {e^{-x/\lambda}} { \lambda \left(1-e^{-19/\lambda}\right) }$$
Calculate the product of all 6 events for a total likelihood, and take the negative logarithm of it for a nice scaling.
In images, first the distribution for this dataset, then the distribution for a "more normal" dataset, with more events for small x:
Given data, red line at the limit for λ->infinity.
Example data with a more usual distribution, red line at the limit for λ->infinity again.
A particle physicist would now probably look for the range where the negative log likelihood is not larger than ##\chi_2^{-1}(0.05)/2=1.92## above the minimum, which leads to ##\lambda > 4.0## at 95% confidence level.