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LATTICE SUSY joel.giedt, simon.catterall, raghav.govind.jha, - PowerPoint PPT Presentation

LATTICE SUSY joel.giedt, simon.catterall, raghav.govind.jha, david.schaich DESPERATELY SEEKING SUSY (ELISE TOO) WILSON FERMION N=4 Can impose SO(4), gauge invariance 8-dimensional parameter space to fine-tune in Notice rescaling of fields


  1. LATTICE SUSY joel.giedt, simon.catterall, raghav.govind.jha, david.schaich

  2. DESPERATELY SEEKING SUSY (ELISE TOO…)

  3. WILSON FERMION N=4 Can impose SO(4), gauge invariance 8-dimensional parameter space to fine-tune in Notice rescaling of fields exploited for first three terms---we do that in our twisted theory too.

  4. The twisted, Q invariant lattice action takes the form Observes the notion that anything correct should be simple. Four terms --- will result in four coefficients to fine tune.

  5. WHAT’S THE DIFFERENCE? Of course we have to say how the derivatives are implemented:

  6. SCALAR SUPERSYMMETRY The supersymmetry transformation is:

  7. BIANCHI IDENTITY FOR Q CLOSED TERM then algebra

  8. PRIMITIVE VECTORS

  9. TRUNCATION Hence we can consistently truncate to SL(N,C). All we lose is the U(1) gauge invariance, if we do it right. The surviving gauge group is SU(N). This is very helpful because the U(1) modes (scalar and gauge) are a royal pain.

  10. Q RESTORATION

  11. 3D HOLOGRAPHY

  12. CONCLUSIONS Lattice formulation with very little fine-tuning, due to symmetries BPS solitons under study Understanding of renormalization Highly optimized code with good scaling SL(N,C) truncation Adequate computing resources Lower-dimensional finite T/gauge-gravity duality Operator dimensions

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