Software R&D Working Meeting Minutes
2021-09-22
Introduction
- IRIS-HEP fellowships can be granted to very early career people, even undergraduates. Very useful way to attract talent to our field.
- ACAT “results” will be known in advance of needing to submit CHEP abstracts (ACAT is 29 November - 3 December).
- There is also an ML4Sim seminar on Thurdsay 30 September: https://indico.cern.ch/event/1073290/.
Faster Simulation
- Different calorimeter materials, but is it a different geometry?
- Not geometry per-se, but material in this case (slides 8, 12). leading to very different energy deposition profile.
- But meta-learning model does really use different geometries (from GDML, slide 14)
- How do the hits/energy deposits come in?
- Via the Geant4 hits, mapped to the geometry
- What about “invisible” energy (e.g., using Geant4 tracks)?
- No, not training with this, only using EM energy deposits at the moment
- If there’s a new geometry can we try this? New detector concepts.
- What about multi-dimensional metrics (beyond energy and energy per layer)
- It’s the next step, but E and E_layer have to first be correct, so that’s where we started
- How do you represent the different geometries?
- Using a tokenisation of the GDML features (slide 38)
- These become the conditioning “hash”
- But that does not encode any simlarities between any geometries
- However, this does not encode everything, so we are investigating passing relevant parameters (layers, thickness, material, etc.)
- Slide 8 geometry, is the particle always incident at (0, 0, 0)?
- Yes, it is at the moment
- Open question as to if the training will scale to this being a new input parameter
- Maybe scaling is better with the ‘learning to learn’ approach?
- Response from cells can be very sensitive to impact position?
- Can use a higher granularity approach, with voxelisation finer than cells (although that’s not done right now)
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