The Simplest little Higgs

By M. Schmaltz. 2004

174 citations recorded by the source corpus.

We show that the SU(3) little Higgs model has a region of parameter space in which electroweak symmetry breaking is natural and in which corrections to precision electroweak observables are sufficiently small. The model is anomaly free, generates a Higgs mass near 150 GeV, and predicts new gauge bosons and fermions at 1 TeV.

Subfields: Artificial Intelligence, Atmospheric Science, Nuclear and High Energy Physics

View Paper: https://www.semanticscholar.org/paper/8312b8deaf631bd3ed660f0d96c73efb899b8e70

How researchers see this paper

The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.

In Artificial Intelligence

1. David Tucker-Smith
2. I. Low
3. M. Schmaltz
4. A. Falkowski
5. Hsin-Chia Cheng
6. T. Volansky
7. E. Kuflik
8. Dean Carmi

In Atmospheric Science

1. David Tucker-Smith
2. I. Low
3. Dean Carmi
4. E. Kuflik
5. A. Falkowski
6. T. Volansky

In Nuclear and High Energy Physics

1. I. Low
2. David Tucker-Smith
3. M. Schmaltz
4. Hsin-Chia Cheng
5. A. Falkowski
6. T. Volansky
7. E. Kuflik
8. Lian-tao Wang

Citations in the corpus

• A Quirky Little Higgs Model (2008, background): “From the model building perspective, one sees that if we want the quadratic divergence from the top quark to be cancelled by a spin-1/2 partners as in the Little Higgs mechanism, then the new particles are not necessarily colored as in the original little Higgs model [6, 7].”
• Interpreting LHC Higgs results from natural new physics perspective (2012, methodology): “in the Simplest Little Higgs model with an [SU(3)/SU(2)]2 coset structure [60–65] when taking the limit f2 f1.”
• LITTLE HIGGS THEORIES (2005, methodology): “The explicit model we are going to construct in this section is the “simplest little Higgs” [19, 20, 30].”
• A pseudoscalar decaying to photon pairs in the early LHC Run 2 data (2015, background): “Other coset spaces can have additional singlets, an example (that suffers custodial breaking and hence is tuned) is SU(3)×U(1)X / SU(2)L×U(1)Y [42, 43].”
• T parity and the littlest Higgs (2004, background): “There are many variants of the little Higgs models [13]–[18], as well as some examples of UV extensions above 10TeV [19, 20], and extensive phenomenological studies have been performed [21]– [29].”