Presentation Slides Flashcards
1
Q
01 : Title Slide
A
- Using tensor networks to represent scattering amplitudes
- Not a computing project, just the mathematical representation
- Aim is to contruct an accurate & flexible self-contained system
2
Q
02 : What is tensor notation
A
- Tensor notation = diagramatic tensor algebra (Boolean metaphor)
- Shapes represent tensors, legs represent indices
- Connected legs represent contracted indices
3
Q
03 : Penrose Graphical Notation
A
- Roger Penrose developed this for general relativity
- Here’s some examples (Bianchi identity)
- Emphisis on readablity to humans
4
Q
04 : Quantum Tensor Applications
A
- Tensor networks approximate quantum simulations (degrees of freedom)
- Ground-state Hamiltonian sweeping (red tensors are varied)
- PEPS Hilbert space for lattice gauge theory (virtual legs dimensions = entanglement between regions)
5
Q
05 : My approach to Feynman Diagrams
A
- It was decided to try & apply tensor notation to matrix elements (not Lagrangians)
- Aim is to improve the computability of scattering amplitude construction
- Feynman diagrams are good, but don’t scale well
6
Q
06 : Why Feynman diagrams don’t scale
A
- You need a huge number of diagrams
- The matrix elements become incredibly large
- My aim is to contruct amplitudes without needing to refer to mathematics
7
Q
07 : Particle Network Basics
A
- Explain the different means for each symbol
- Explain the original factorised space (which way lines contract)
- Show the modern layout with Feynman diagram
8
Q
08 : Electromagnetic Interactions
A
- Lines = quantum numbers. We only need spin & momentum lines.
- Differing vertex & propagator regions
- The effective field operator for Fermi interactions
9
Q
09 : Strong & Weak Interactions
A
- Strong & weak add new quantum number lines
- Strong : Gell-mann matrices
- Weak : PL/PR, mixing matrices & massive boson propagators
10
Q
10 : Necessary vs Aesthetic
A
- Middle of the road between Penrose & computers, more towards computers
- Constants have been absorbed into tensors
- Weak propagator was designed by necessity from the lines of contractions
11
Q
11 : Direct construction of process
A
- Main purpose = build networks without graphs
- Turn final states spinor into fermion propagator
- Add vertex terms, then new decay channel
12
Q
12 : Missing Vertices
A
- Missing Higgs & boson-boson coupling
- Need to do loop corrections & renormalisations
- Fully expect all of this to be done in next semester
13
Q
13 : Beyond the standard model
A
- Quantum gravity (problems with renormalisation)
- GUT theories: new field & bosons to explore
- Super-symmetry offers a huge number of new particles
14
Q
14 : Conclusion
A
- Aid computation of scattering amplitudes
- Aid comprhension of QFT processes
- Critical evaluation : have you succeeded in either?