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
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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
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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
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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)
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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
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6
Q

06 : Why Feynman diagrams don’t scale

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  • 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
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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
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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
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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
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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
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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
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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
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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
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14
Q

14 : Conclusion

A
  • Aid computation of scattering amplitudes
  • Aid comprhension of QFT processes
  • Critical evaluation : have you succeeded in either?
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