From imaging algorithms to quantum methods Seminar

Europe/Warsaw
https://cern.zoom.us/j/66151941204?pwd=n7upvvZYibexBhbtyn5kvTpy36L0Wo.1 (Zoom)

https://cern.zoom.us/j/66151941204?pwd=n7upvvZYibexBhbtyn5kvTpy36L0Wo.1

Zoom

Konrad Klimaszewski (NCBJ), Wojciech Krzemien (NCBJ)

#Title: Bayesian fitting in positronium lifetime imaging
#presenter: Roman Y. Shopa
#date: 16.06 2025

#Participants: 

Wojciech Krzemien (WK),  Lech Raczyński(LR),  Roman Shopa (RS), Wojciech Wiślicki (WW), Michał Mazurek (MM), Mateusz Bała (MB), Konrad Klimaszewski (KK), Krzysztof Nawrocki (KN)

 

#Questions/Remarks

WW: What does the pathway mean?
RS: It is just a type of decay: para-, ortho- etc.

WK: Is the sampling from the prior distribution?
RS: Yes

WK: Which posterior sampling method do you use underneath?
RS: Hamiltonian MC implementation

WK: Can you give the intuition on how this convergence works?e.g. In which direction is the next parameter chosen?
RS: I would need to read a bit more.

KK: Does your result already include the MCMC or Non-U-turn?
RS: Yes

MM: What are those vertical lines on p.13? E.g. red line at -10 ns?
RS: The line on the left probably limits the spectrum region, as for the red one - I hardly see it, but the slide is from J.Qi's presentation, so I have little idea.

LR: It is not obvious why the Bayesian method works worse in the log scale and better in the linear scale.

WW: Dependence of priors is visible, then it is worrying. If it is really a Markov chain, then it cannot depend on priors. It comes from the Markov theorem.
So either there is some numerical problem, or it is not a truly Markov chain.

LR: Markov process, by definition, depends only on the previous step. The method should not be sensitive to any starting points. This is guaranteed mathematically.

RS: Hamiltonian Monte Carlo introduces momentum variables for each parameter, treating the sampling process as a particle movement. It simulates the particle’s trajectory guided by the gradient of the log-posterior, proportional to the likelihood x prior.

MM: Would Bayesian neural networks be helpful in this case?
RS: Not sure, worth checking, but impractical for PLI where there are many spectra for many voxels... Bayesian fitting itself is a good alternative to least-squares, which struggles with overfitting and is sensitive to the initial guess.

KK: Do you observe a problem with initialisation for Bayesian fitting?
RS: I observe a dependence on priors. If I start with the prior far away from the assumed truth then it can not converge correctly.

KK: How fast is the convergence?
RS: Very slow, even in multi-thread mode. It requires many iterations/Markov chains, each processed slower than least-squares minimisation. Also, the R package 'brms' requires C++ compilation each time I adjust the prior. It is impractical for multi-voxel PLI.

There are minutes attached to this event. Show them.
    • 10:00 11:00
      Bayesian fitting in positronium lifetime imaging 1h

      The analysis of positronium (Ps) annihilation lifetime spectra requires multi-component modelling, constituted by exponentially modified Gaussian functions. A direct curve fitting is an ill-posed problem and needs either deconvolution or multi-stage constrained minimisation. In Ps lifetime imaging (PLI), a technique that targets local Ps lifetime distribution, an additional challenge emerges – the low number of counts per spectrum.

      In this talk, we review the application of non-linear Bayesian fitting in PLI, based on the prior knowledge about the parameters of the Ps lifetime model. The available software implementations shall be compared, with the preliminary results for the simulated data.

      Speaker: Roman Shopa (National Centre for Nuclear Research)
    • 11:00 11:30
      Discussion 30m
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