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Electroweak and Flavor Dynamics at Hadron Colliders
High Energy Physics - Phenomenology · Submitted 8 May 1996
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We catalog the principal signatures of electroweak and flavor dynamics at $\pbarp$ and $pp$ colliders for use at the 1996 Snowmass Workshop on New Directions in High Energy Physics.
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The abstract, sentence by sentence
We catalog the principal signatures of electroweak and flavor dynamics at $\pbarp$ and $pp$ colliders for use at the 1996 Snowmass Workshop on New Directions in High Energy Physics. The framework for dynamical symmetry breaking we assume is technicolor, with a walking coupling $\atc$, and extended technicolor. The reactions discussed occur mainly at subprocess energies $\rshat \simle 1\,\tev$. They include production of color-singlet and octet technirhos and their decay into pairs of technipions, longitudinal weak bosons, or jets. Technipions, in turn, decay predominantly into heavy fermions. Many of these signatures are also expected to occur in topcolor-assisted technicolor. Several particles specific to this new scenario are discussed. Additional signatures of flavor dynamics, associated with quark and lepton substructure, may be sought in excess production rates for high $E_T$ and invariant mass dijets and dileptons. An important feature of these processes is that they exhibit fairly central angular and rapidity distributions.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We catalog the principal signatures of electroweak and flavor dynamics at $\pbarp$ and $pp$ colliders for use at the 1996 Snowmass Workshop on New Directions in High Energy Physics. | contribution 0.97 | 0.85 | 0.08 | asserted 0.95 |
| s1 | The framework for dynamical symmetry breaking we assume is technicolor, with a walking coupling $\atc$, and extended technicolor. | method 0.94 | 0.16 | 0.05 | asserted 0.96 |
| s2 | The reactions discussed occur mainly at subprocess energies $\rshat \simle 1\,\tev$. | method 0.51 | 0.20 | 0.03 | asserted 0.98 |
| s3 | They include production of color-singlet and octet technirhos and their decay into pairs of technipions, longitudinal weak bosons, or jets. | contribution 0.89 | 0.19 | 0.07 | asserted 0.98 |
| s4 | Technipions, in turn, decay predominantly into heavy fermions. | background 0.29 | 0.14 | 0.04 | asserted 0.98 |
| s5 | Many of these signatures are also expected to occur in topcolor-assisted technicolor. | interpretation 0.66 | 0.20 | 0.07 | hedged possibility 0.85 |
| s6 | Several particles specific to this new scenario are discussed. | contribution 0.99 | 0.45 | 0.04 | asserted 0.88 |
| s7 | Additional signatures of flavor dynamics, associated with quark and lepton substructure, may be sought in excess production rates for high $E_T$ and invariant mass dijets and dileptons. | future work 0.48 | 0.08 | 0.07 | hedged possibility 1.00 |
| s8 | An important feature of these processes is that they exhibit fairly central angular and rapidity distributions. | result 0.83 | 0.29 | 0.07 | asserted 0.96 |
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Original abstract
We catalog the principal signatures of electroweak and flavor dynamics at $\pbarp$ and $pp$ colliders for use at the 1996 Snowmass Workshop on New Directions in High Energy Physics. The framework for dynamical symmetry breaking we assume is technicolor, with a walking coupling $\atc$, and extended technicolor. The reactions discussed occur mainly at subprocess energies $\rshat \simle 1\,\tev$. They include production of color-singlet and octet technirhos and their decay into pairs of technipions, longitudinal weak bosons, or jets. Technipions, in turn, decay predominantly into heavy fermions. Many of these signatures are also expected to occur in topcolor-assisted technicolor. Several particles specific to this new scenario are discussed. Additional signatures of flavor dynamics, associated with quark and lepton substructure, may be sought in excess production rates for high $E_T$ and invariant mass dijets and dileptons. An important feature of these processes is that they exhibit fairly central angular and rapidity distributions.
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References
How the literature uses it
13 arXiv papers cite this in 21 sentences
Papers citing it · 10 sentences without a confident label
Uses its method or tool 2 papers
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The new physics cross sections are computed using the matrix elements from Refs. [ref] .
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Hypothetically, quarks could be made of other particles, as assumed in the quark compositeness model in Ref. [ref] .
Measurement of dijet angular distributions at sqrt{s}=1.96TeV and searches for quark compositeness and extra spatial dimensions · Introduction · 0.99
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Dijet resonances from theories such as Technicolor [ref] , Grand Unified Theory [ref] , Superstrings [ref] , Compositeness [ref] , Extra Dimensions [ref] and Extra Color [ref] [ref] , and Contact Interactions [ref] [ref] [Both ATLAS and CMS use the CI lagrangian term: L$_qqqq$ = A (g$^2/$2$Λ^2_LL$) (q̄$_Lγ^μ$q$_L$)(q̄$_Lγ_μ$q$_L$) where $Λ$ is the contact interaction scale, g$^2$ is by convention 4$πα_s$ and with A = +1 (destructive interference sign). ] (CI) are signals of New Physics (NP) which can be discovered with dijet events, thanks to the deviations they produce in the basic SM distributions.
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Interactions at an energy scale much lower than the mass of the mediating particle can be modeled by contact interactions (CI) [ref] governed by a single mass scale conventionally denoted by $Λ$.
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