CR004 $pp \to B \bar{B} \to tW/bZ/bH + X$
Pair production of custodial charge -1/3 bottom partner B Status REVIEWED VERIFIED High Code: NO Priority Medium
PDG / equivalent values
| Observable | Value | Year | Experiment / source | Provenance |
|---|---|---|---|---|
| $m_B$ lower limit from pp $ \to $ B $\bar{B}$, B(B $ \to $ H b)=1 | m_B > 1570 GeV 95% CL (lower_limit) | 2025 | CMS | source ↑ |
| $m_B$ lower limit from pp $ \to $ B $\bar{B}$, B(B $ \to $ Z b)=1 | m_B > 1540 GeV 95% CL (lower_limit) | 2025 | CMS | source ↑ |
| $m_B$ lower limit from pp $ \to $ B $\bar{B}$, B(B $ \to $ W t)=1 | m_B > 1560 GeV 95% CL (lower_limit) | 2025 | CMS | source ↑ |
Why this constrains the RS scan
In custodial RS and composite-Higgs language, the \(B\) state is a physical
fermion resonance, not the KK gluon itself. A direct \(B\bar B\) search
therefore constrains \(m_B\) under a specified custodial multiplet and decay
pattern; it becomes a constraint on \(M_{\mathrm{KK}}\) only after choosing
the model relation between the light bottom partner and the gauge/fermion
KK scale. Pair production is comparatively robust because it is QCD driven,
but the mass exclusion still depends on the signal width, the allowed
decays, and the branching fractions into \(tW\), \(bZ\), and \(bH\).
For the RS scan in this repo, CR004 is a cross-check rather
than the leading bound. The this repository quark-scan methodology note reports
\(M_{\mathrm{KK}}^{\min}(p50,g_\ast=3)=47.26~\mathrm{TeV}\) from the
low-energy flavor scan, with \(127.13~\mathrm{TeV}\) at \(95\%\) acceptance.
That scale is far above the present direct \(B\)-partner reach near
\(1.5~\mathrm{TeV}\). The collider entry is still useful for non-anarchic
RS variants, custodial spectra where fermion partners sit well below the
gauge KK scale, or benchmark points tuned to evade the low-energy flavor
envelope.
What's changed since the original paper
The pre-LHC RS-motivated baseline is Contino--Servant arXiv:0801.1679, which
emphasized same-sign dileptons from \(B,T_{5/3}\to Wt\) in custodial
top-partner spectra. Post-2010 LHC work turned that benchmark strategy into
broad branching-fraction searches: ATLAS arXiv:1808.02343 combined 13 TeV
searches across the \(T\) and \(B\) decay simplex; CMS arXiv:2008.09835 made
fully hadronic \(bH/bZ\) final states competitive with leptonic channels;
CMS arXiv:2209.07327 used single-lepton, same-sign dilepton, and multilepton
categories and drives the PDG \(B\to Wt\) corner; and ATLAS arXiv:2210.15413
plus arXiv:2212.05263 are full-Run-2 \(Z+\)third-generation and
high-\(E_T^{\rm miss}\) cross-checks. The current CMS arXiv:2402.13808
result added a \(0\ell/2\ell\) combination with HEPData exclusion contours
over the \(bH\), \(bZ\), and \(tW\) branching simplex. The CMS
arXiv:2405.17605 review is used as Run-2 synthesis, not as a new measured
limit.
Validity and model dependence
The quoted limits are valid as direct LHC mass-exclusion statements for
prompt, narrow enough, pair-produced \(B\) quarks with the stated branching
assumptions. They are not inclusive limits on every custodial-RS bottom
partner. A broad resonance, nonstandard cascade decays, additional nearly
degenerate partners, altered \(B\)-tag/Higgs/Z acceptances, or branching
fractions spread across several modes can move the bound. A single
production bound can reach higher masses, but it is controlled by
electroweak mixing/coupling choices and is therefore not the canonical CR004
pair-production observable.
Code coverage in this repo
NO. The required code-coverage grep over
quarkConstraints/,
qcd/, flavorConstraints/, neutrinos/,
yukawa/, warpConfig/, solvers/,
scanParams/, and tests/ found no direct collider
constraint, VLQ object, branching-simplex filter, or ATLAS/CMS/HEPData limit
ingestion. The collider/VLQ query returned only
tests/test\_alpha\_s.py:88 and tests/test\_alpha\_s.py:89,
a \(\alpha_s\) CMS/RunDec example, not an LHC search. Nearby evidence is
flavor-only: scanParams/scan.py:399 computes \(M_{\mathrm{KK}}\) for
a scan row and scanParams/scan.py:523 applies the \(\mu\to e\gamma\)
check, while quarkConstraints/scan.py:359 maps
\(\Lambda_{\rm IR}\) to \(M_{\mathrm{KK}}\) and
quarkConstraints/scan.py:377 evaluates \(\Delta F=2\) constraints.Implementation difficulty
HIGH. A faithful implementation needs external LHC likelihoods or
a reinterpretation chain such as CheckMATE, MadAnalysis5, or SModelS, plus
signal generation for the custodial spectrum, widths, branching fractions,
detector acceptances, and correlations across final states. A simple
hard-coded mass veto would be easy but would be misleading for RS scans
because \(m_B/M_{\mathrm{KK}}\), widths, and \(B\to tW,bZ,bH\) fractions are
model dependent.
Reason: A faithful constraint needs LHC likelihoods or reinterpretation tooling, signal generation for RS custodial spectra, widths, branching fractions, detector acceptances, and correlated final-state combinations. A hard mass cut would be model-dependent and misleading.
Key references
PDG2025\_BPrimeListing;
ContinoServant2008\_TopPartners;
ATLAS2018\_VLQCombination;
CMS2020\_BVLQFullyHadronic;
CMS2023\_VLQLeptonic;
ATLAS2023\_ZThirdGen;
ATLAS2023\_METPartners;
CMS2024\_BVLQDilepHad;
HEPData2024\_BVLQContours;
CMS2025\_VLQReview.