February 27, 2023 to March 3, 2023
Institute for Advanced Study of the Technische Universität München
Europe/Berlin timezone

Contribution List

70 out of 70 displayed
  1. 2/27/23, 8:30 AM
  2. Nora Brambilla
    2/27/23, 9:10 AM
  3. Maria-Paola Lombardo
    2/27/23, 9:25 AM
  4. Daniel Hackett
    2/27/23, 9:55 AM
  5. David Albandea
    2/27/23, 10:20 AM
  6. Lingxiao Wang
    2/27/23, 11:15 AM
  7. Elia Cellini
    2/27/23, 11:40 AM
  8. Chair: Sinead Ryan, Members: Simone Bacchio, Daniel Hackett, Maria Paola Lombardo, Alberto Ramos
    2/27/23, 12:00 PM
  9. Sven Krippendorf
    2/27/23, 2:30 PM
  10. Rasmus Orsoe
    2/27/23, 2:50 PM
  11. Vincent Stimper
    2/27/23, 3:10 PM
  12. Chair: Lukas Heinrich
    2/27/23, 3:30 PM
  13. Gurtej Kanwar
    2/27/23, 4:30 PM
  14. Yukari Yamauchi
    2/27/23, 4:50 PM
  15. Marcel Rodekamp
    2/27/23, 5:10 PM
  16. Chair: Will Detmold, Members: Gurtej Kanwar, Andrei Alexandru (The George Washington University), Thomas Luu, Yukari Yamauchi
    2/27/23, 5:30 PM

    1) Is there a way to determine the maximum improvement in <sign> or in S-to-N that is achievable through contour deformations and related
    approaches?

    2) How can ML be targeted towards such a maximal improvement?

    3) Are there features of specific observables that make contour
    deformation particularly effective or ineffective?

    4) How do contour deformations for one observable/theory...

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  17. Frank Pollmann
    2/28/23, 9:50 AM
  18. Alberto Ramos
    2/28/23, 10:20 AM
  19. Jacob Finkenrath
    2/28/23, 11:15 AM
  20. Tomasz Stebel
    2/28/23, 11:40 AM
  21. Jeanne Trinquier
    2/28/23, 12:00 PM
  22. Chair: Phiala Shanahan, Members: Fernando Romero Lopez, Jacob Finkenrath, Jeanne Trinquier
    2/28/23, 12:20 PM

    • Temperature check: for each panelist, in 2-5 words, how optimistic or pessimistic do you feel about the utility of ML in accelerating lattice field generation in your context.
    • What are the most application-specific features of the LQCD gauge field generation problem i.e., in what important ways is it different from applications in other areas of physics, and how does that impact the way...

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  23. Andrei Alexandru
    2/28/23, 2:30 PM
  24. Marius Neumann
    2/28/23, 2:50 PM
  25. Francesco Di Renzo
    2/28/23, 3:10 PM
  26. Chair: Maria Paola Lombardo
    2/28/23, 3:30 PM

    Panel discussion addressing the three main questions:

    --Where do we stand with the identification of phases with ML?
    Do you feel ML could become competitive with standard techniques for the quantitative studies of known phase transitions i.e. order of the transition at large Nf, chiral limit, etc.

    --Which are your views on the need/concrete possibility of identifying hypothesised, not...

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  27. Gert Aarts
    2/28/23, 4:30 PM
  28. Julian Urban
    2/28/23, 4:40 PM
  29. Kai Zhou, Lingxiao Wang
    2/28/23, 5:10 PM
  30. Alexander Rothkopf
    2/28/23, 5:40 PM
  31. Chair: Gert Aarts
    2/28/23, 5:50 PM
  32. Sylvia Kortüm
    3/1/23, 8:45 AM
  33. Simone Bacchio
    3/1/23, 9:00 AM
  34. Aleksas Mazeliauskas
    3/1/23, 9:40 AM
  35. Marina Marinkovic
    3/1/23, 10:10 AM
  36. Fernando Romero-Lopez
    3/1/23, 11:10 AM
  37. Chair: Nora Brambilla, Members: Marina Marinkovic, Phiala Shanahan, William Detmold, Aleksas Mazeliauskas
    3/1/23, 11:40 AM

    --what can EFTs do for ML4LATTICE?
    --what ML4LATTICE could do for EFTs?

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  38. Michael Albergo
    3/1/23, 2:30 PM
  39. A. Ramos
    3/1/23, 3:00 PM
  40. Miles Cranmer
    3/1/23, 3:25 PM
  41. Chair: Phiala Shanahan, Members: Michael Albergo, Andrei Alexandru, Miles Cranmer
    3/1/23, 3:55 PM

    • What does it mean to have an ML-accelerated algorithm that is “exact”?
    Discuss the distinction between exact algs, interpretable algs, and algs that allow error propagation.
    • What are the differences between in-principle and in-practice exactness? Are they important?
    • In what applications (both in LQFT and drawing parallels to other ares in physics) is it important to guarantee...

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  42. Phiala Shanahan
    3/1/23, 6:00 PM
  43. Lukas Heinrich
    3/2/23, 9:30 AM
  44. Alexander Rothkopf
    3/2/23, 10:00 AM
  45. Julien Frison
    3/2/23, 10:30 AM
  46. Sebastian Wetzel
    3/2/23, 11:15 AM
  47. Nicholas Gao
    3/2/23, 11:35 AM
  48. Chair: Alexander Rothkopf, Members: Sebastian Wetzel, Matteo Favoni, Fernando Romero Lopez, Miles Cranmer
    3/2/23, 12:00 PM
    1. Alexander Rothkopf: Setting the stage – ML for physics interpretation
    2. Sebastian Wetzel: ML for identifying order parameters & effective d.o.f. in the context of phase transitions
    3. Matteo Favoni: ML for identifying defects and effective d.o.f. in the context of confinement
    4. Fernando Romero Lopez: ML for extraction of emergent d.o.f. in the context of scattering resonance
    5. Miles...
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  49. Matteo Favoni
    3/2/23, 2:30 PM
  50. Daniel Hackett
    3/2/23, 2:50 PM
  51. Chair: Phiala Shanahan, Members: Gurtej Kanwar, Christoph Lehner, Matteo Favoni
    3/2/23, 3:05 PM

    • There is ongoing debate in the ML community about the value of trying to incorporate domain knowledge into architectures vs using computational brute force. What guides your intuition for the value of building symmetry-equivariant architectures? In your experience when is symmetry-equivariance valuable and when is it not?
    • What makes gauge equivariance in particular challenging from a...

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  52. Gert Aarts
    3/3/23, 9:00 AM
  53. Gabor Papp
    3/3/23, 9:30 AM
  54. Jian Liang
    3/3/23, 10:00 AM
  55. Kai Zhou
    3/3/23, 10:30 AM
  56. Alessandro De Santis
    3/3/23, 11:30 AM
  57. Chair: Andreas Kronfeld
    3/3/23, 12:00 PM
  58. Abdulhakim Alnuqayqdan
    3/3/23, 2:00 PM
  59. Thomas Luu
    3/3/23, 2:25 PM
  60. Christoph Lehner
    3/3/23, 2:50 PM
  61. Luigi Scorzato
    3/3/23, 3:40 PM
  62. Andreas Athenodorou
    3/3/23, 4:10 PM
  63. Nakul Aggarwal
    3/3/23, 4:40 PM
  64. Nora Brambilla
    3/3/23, 5:00 PM
  65. Alberto Ramos
  66. Ankur Singha
  67. Daniel Schuh
  68. Phiala Shanahan
  69. Gitta Kutyniok
  70. Julian Mayer-Steudte