Pith Number

pith:K45SMCLF

pith:2026:K45SMCLFBNHFY4ZIOJ55QRLBMR

not attested not anchored not stored refs resolved

Predicting Three Generations of Fermions: Discovery Prospects of the Bilepton Model

Ahmed Hammad, Andreas Crivellin, Paul H. Frampton

Doubly charged bileptons can be discovered at the HL-LHC in four-lepton events up to 2.5 TeV heavy quark masses or 2 TeV bilepton masses.

arxiv:2605.15286 v1 · 2026-05-14 · hep-ph · hep-ex

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\usepackage{pith}
\pithnumber{K45SMCLFBNHFY4ZIOJ55QRLBMR}

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Record completeness

1 Bitcoin timestamp

2 Internet Archive

3 Author claim open · sign in to claim

4 Citations open

5 Replications open

✓ Portable graph bundle live · download bundle · merged state

The bundle contains the canonical record plus signed events. A mirror can host it anywhere and recompute the same current state with the deterministic merge algorithm.

Claims

C1strongest claim

Owing to the essentially background-free signature of four energetic leptons at the LHC, we show that Run-2 data allow a discovery only for m_D ≲ 1 TeV, whereas the HL-LHC can achieve a 5σ discovery up to m_D ≲ 2.5 TeV (nearly independently of m_Y) and/or for m_Y ≲ 2 TeV (even if D is heavy).

C2weakest assumption

The four-lepton final state is treated as essentially background-free and the production cross sections (both direct and via heavy-quark decays) are assumed to be accurately predicted by leading-order or next-to-leading-order calculations without large uncertainties from parton distributions or higher-order corrections.

C3one line summary

Bilepton Model predicts observable pairs of doubly-charged bileptons at HL-LHC up to m_D ~2.5 TeV or m_Y ~2 TeV through background-free four-lepton final states in two complementary channels.

References

36 extracted · 36 resolved · 19 Pith anchors

[1] Foundation of Machine Learning Physics 2000

[2] S. L. Glashow,Partial Symmetries of Weak Interactions,Nucl. Phys.22(1961) 579. [2]Particle Data Groupcollaboration, S. Navas et al., Review of particle physics,Phys. Rev. D110(2024) 030001. [3]Gargame 1961

[3] P. W. Higgs,Broken symmetries, massless particles and gauge fields,Phys. Lett.12(1964) 132 1964

[4] F. Englert and R. Brout,Broken Symmetry and the Mass of Gauge Vector Mesons,Phys. Rev. Lett.13 (1964) 321 1964

[5] Weinberg,A Model of Leptons,Phys 1967

Formal links

2 machine-checked theorem links

Receipt and verification

First computed	2026-05-20T00:00:50.700161Z
Builder	pith-number-builder-2026-05-17-v1
Signature	Pith Ed25519 (`pith-v1-2026-05`) · public key
Schema	pith-number/v1.0

Canonical hash

573b2609650b4e5c7328727bd845616477dc759f6458ccf8c6cf2f3c54fff06b

Aliases

arxiv: 2605.15286 · arxiv_version: 2605.15286v1 · doi: 10.48550/arxiv.2605.15286 · pith_short_12: K45SMCLFBNHF · pith_short_16: K45SMCLFBNHFY4ZI · pith_short_8: K45SMCLF

Agent API

Resolver JSON Graph JSON Events JSON Schema Signing key

Verify this Pith Number yourself

curl -sH 'Accept: application/ld+json' https://pith.science/pith/K45SMCLFBNHFY4ZIOJ55QRLBMR \
  | jq -c '.canonical_record' \
  | python3 -c "import sys,json,hashlib; b=json.dumps(json.loads(sys.stdin.read()), sort_keys=True, separators=(',',':'), ensure_ascii=False).encode(); print(hashlib.sha256(b).hexdigest())"
# expect: 573b2609650b4e5c7328727bd845616477dc759f6458ccf8c6cf2f3c54fff06b

Canonical record JSON

{
  "metadata": {
    "abstract_canon_sha256": "bfe4695f9dc8620bb451449052fc963628e7e33eddbe097e348b9b5fa434acea",
    "cross_cats_sorted": [
      "hep-ex"
    ],
    "license": "http://creativecommons.org/licenses/by/4.0/",
    "primary_cat": "hep-ph",
    "submitted_at": "2026-05-14T18:01:06Z",
    "title_canon_sha256": "c52d29d9f543565e28c724669d1739cdc132d4750ecefd2f56d97ecc2ae85434"
  },
  "schema_version": "1.0",
  "source": {
    "id": "2605.15286",
    "kind": "arxiv",
    "version": 1
  }
}