In the world of sphere packing, thereβs been debate about whether order or a dash of chaos will give the best results. A recent proof marks a win for order. www.quantamagazine.org/new-sphere-p...
07.07.2025 14:27 β π 23 π 6 π¬ 0 π 0@alexxthiery.bsky.social
Associate Prof. in ML & Statistics at NUS πΈπ¬ MonteCarlo methods, probabilistic models, Inverse Problems, Optimization https://alexxthiery.github.io/
In the world of sphere packing, thereβs been debate about whether order or a dash of chaos will give the best results. A recent proof marks a win for order. www.quantamagazine.org/new-sphere-p...
07.07.2025 14:27 β π 23 π 6 π¬ 0 π 0And a recent very well written review of NS:
"Nested sampling for physical scientists"
arxiv.org/abs/2205.15570
Nested Sampling is extremely popular in some communities, and there are often claims that it helps mitigate "phase transition" issues that can often affect standard geometric "tempering" methods (although I do not understand that well enough yet...) It's great to see explicit connections with SMC!
23.06.2025 11:29 β π 0 π 0 π¬ 1 π 0"Unbiased and Consistent Nested Sampling via Sequential Monte Carlo"
by Robert Salomone, Leah F. South, Christopher Drovandi, Dirk P. Kroese, Adam M. Johansen
arxiv.org/abs/1805.03924
"A simpler nested sampling identity"
Interesting blogpost on nested sampling & SMC by Nicolas Chopin
statisfaction-blog.github.io/posts/04-06-...
See you in πΈπ¬
15.06.2025 11:46 β π 2 π 0 π¬ 0 π 0My bad, this wasn't clear. It's in the space of all probability densities
13.06.2025 18:29 β π 0 π 0 π¬ 0 π 0Motivated by the reading of this nice article:
"Sequential Monte Carlo approximations of Wasserstein--Fisher--Rao gradient flows"
by Francesca R. Crucinio, Sahani Pathiraja
arxiv.org/abs/2506.05905
And here is how the geodesic path looks like (again under the Fisher-Rao metric)
13.06.2025 16:30 β π 6 π 0 π¬ 1 π 0Here's how the gradient flow for minimizing KL(pi, target) looks under the Fisher-Rao metric. I thought some probability mass would be disappearing on the left and appearing on the right (i.e. teleportation), like a geodesic under the same metric, but I was very wrong... What's the right intuition?
13.06.2025 16:29 β π 23 π 6 π¬ 4 π 0Once you have tried symplectic integrators, you never go back.
07.06.2025 21:34 β π 46 π 3 π¬ 6 π 0The full (?) program of talks etc. for BayesComp seems to be online now (bayescomp2025.sg#programme), and looks pretty exciting - I will need to set aside some time to carve out my own schedule!
01.06.2025 12:03 β π 26 π 3 π¬ 0 π 0Once the prompt is public, I do not think it will provide much signal (but it could potentially slightly help some the papers make sure their writing style align well with the conference expectations)
17.05.2025 09:17 β π 1 π 0 π¬ 1 π 0How to implement this in practice, make the "review" prompt public in advance?
17.05.2025 08:57 β π 1 π 0 π¬ 1 π 0<proud advisor>
Hot off the arXiv! 𦬠"Appa: Bending Weather Dynamics with Latent Diffusion Models for Global Data Assimilation" π Appa is our novel 1.5B-parameter probabilistic weather model that unifies reanalysis, filtering, and forecasting in a single framework. A thread π§΅
These sparse Gaussian Processes have been around longer than some grad students, but still fun to code! (and today was my first time coding one...)
19.04.2025 15:18 β π 8 π 1 π¬ 0 π 0Today, re-reading a classic.. the 1953 paper that started it all
11.04.2025 09:00 β π 9 π 0 π¬ 0 π 0Is it based on the last year's preprint by Huhtikuun Typerys?
01.04.2025 13:19 β π 2 π 0 π¬ 1 π 0extracted from:
"Upper Bounds for the Connective Constant of Self-Avoiding Walks" by Sven Erick Alm
www.cambridge.org/core/journal...
Cute way to upper bound the connective constant of Z^d. For some length L, enumerate {w_1, w_2, ... , w_N} the Self-Avoiding-Walks of size L. An upper bound is given by the largest eigenvalue of the NxN matrix where M_{i,j}=1 iff there is a SAW of size (L+1) that starts with w_i and ends with w_j.
01.04.2025 09:42 β π 1 π 0 π¬ 1 π 0Ah, but this paper seems to be confident that the conjecture is wrong, based on extensive simulations for estimating the connective constant up to 12 decimals (at which point there is a departure from the conjectured value). Still open though π
arxiv.org/pdf/1607.02984
Conjecture dates from 1992:
"Algebraic Techniques for Enumerating Self-Avoiding Walks on the Square Lattice"
arxiv.org/abs/hep-lat/...
"While we consider it would be fortuitous if this were the true value of the critical point, it nevertheless provides a useful mnemonic" π
Approximating N(L), the number of Self-Avoiding-Walks in Z^2 of length L, is an assignment in my Simulation course this year. The connective constant is:
C = \lim N(L)^1/L ~ 2.638..
Still open-problem to this day: is it true that 1/C equals the zero of the polynomial P(x)=581*x^4 + 7*x^2 - 13 π±
That's interesting that it seems like very little is known about the asymptotic of the second largest increasing subsequence (and no fast method to compute it)
30.03.2025 07:23 β π 3 π 0 π¬ 0 π 0This fast way of finding the LIS is neat! Just tried to reproduce your nice plot without leaving the phone π
chatgpt.com/share/67e8ec...
Sequential Monte Carlo (aka. Particle Socialism?):
"why send one explorer when you can send a whole army of clueless one"
Next week is the MCMC chapter of my simulation course. Asked chatgpt to come up with a funny drawing:
29.03.2025 08:08 β π 38 π 5 π¬ 3 π 2I already advertised for this document when I posted it on arXiv, and later when it was published.
This week, with the agreement of the publisher, I uploaded the published version on arXiv.
Less typos, more references and additional sections including PAC-Bayes Bernstein.
arxiv.org/abs/2110.11216
Are you at AAAI in Philadelphia and interested about #tensor-factorizations or #circuits or even both?
Then join us today at our tutorial: "From tensor factorizations to circuits (and back!)"
Details and materials here
april-tools.github.io/aaai25-tf-pc...
Time 4:15pm - 6:00pm, Room 117
New video! Terence Tao on how we measure the cosmos: youtu.be/YdOXS_9_P4U
08.02.2025 13:46 β π 445 π 81 π¬ 23 π 24