{
  "abstract": "Magnetic dipole, $M1$, strengths were studied in semi-magic $^{50}$Ti up to the neutron-separation threshold by combining data from $(d,p)$ one-neutron transfer, $(γ,γ')$ real-photon scattering, $(e,e')$ inelastic scattering at extreme backward angles, and $(p,p')$ at $E_p = 210$ MeV and extreme forward angles. The combination of all probes provided unique access to the neutron spin-flip contribution and the possibility to evaluate its role in generating the spin-flip $M1$ strengths. The small contribution of the neutron $(1f_{7/2})^{-1}(1f_{5/2})^{+1}$ spin-flip transitions, which were probed with the $(d,p)$ reaction, to the overall strength in $^{50}$Ti questions the standard picture for the microscopic origin of spin-flip strength in the $fp$ shell. For $^{50}$Ti, this letter shows that $J^π = 1^+$ states with larger neutron $(1f_{7/2})^{-1}(1f_{5/2})^{+1}$ spectroscopic factors do not correspond to the ones with the largest $B(M1;0^+_1 \\rightarrow 1^+_i)$ strengths.",
  "abstract_shown": true,
  "affiliations": [],
  "article_type": "Journal reference: Phys. Rev. Lett. 136, 082502 (2026)",
  "arxiv": "2609.10843",
  "author_total": 17,
  "authors": [
    {
      "name": "B. Kelly"
    },
    {
      "name": "M. Spieker"
    },
    {
      "name": "U. Friman-Gayer"
    },
    {
      "name": "L. T. Baby"
    },
    {
      "name": "T. Beck"
    },
    {
      "name": "A. L. Conley"
    },
    {
      "name": "S. W. Finch"
    },
    {
      "name": "J. Isaak"
    },
    {
      "name": "Krishichayan"
    },
    {
      "name": "E. Litvinova"
    },
    {
      "name": "H. Pai"
    },
    {
      "name": "N. Pietralla"
    },
    {
      "name": "D. Savran"
    },
    {
      "name": "W. Tornow"
    },
    {
      "name": "N. Tsoneva"
    },
    {
      "name": "A. Volya"
    },
    {
      "name": "V. Werner"
    }
  ],
  "bibtex": "https://research.draconitic.com/paper/6fgttv1eg35jw.bib",
  "cited_by": 0,
  "doi": "10.48550/arxiv.2609.10843",
  "fulltext_url": null,
  "id": "6fgttv1eg35jw",
  "issns": [],
  "landing_url": "https://arxiv.org/abs/2609.10843",
  "language": null,
  "licence": "LicenseRef-arXiv-nonexclusive-1.0",
  "licence_label": "arXiv licence",
  "licence_source": "article",
  "licence_url": "http://arxiv.org/licenses/nonexclusive-distrib/1.0/",
  "metadata_licence": "CC0-1.0",
  "native_subjects": [
    [
      "arxiv",
      "nucl-ex"
    ],
    [
      "arxiv",
      "nucl-th"
    ]
  ],
  "openalex": null,
  "pdf_url": "https://arxiv.org/pdf/2609.10843",
  "pmcid": null,
  "pmid": null,
  "published": "2026-09-09",
  "publisher": null,
  "ris": "https://research.draconitic.com/paper/6fgttv1eg35jw.ris",
  "sources": [
    {
      "first_seen": "2026-10-30T12:20:26Z",
      "native_id": "2609.10843",
      "source": "arxiv",
      "url": "https://arxiv.org/abs/2609.10843"
    }
  ],
  "subjects": [
    {
      "field": "physics",
      "origin": "arxiv:nucl-ex",
      "subfield": "nuclear"
    }
  ],
  "title": "A detailed view at magnetic dipole strengths: The case of semi-magic $^{50}$Ti",
  "title_text": "A detailed view at magnetic dipole strengths: The case of semi-magic ^50Ti",
  "type": "preprint",
  "updated_at": "2026-10-30T12:20:26Z",
  "url": "https://research.draconitic.com/paper/6fgttv1eg35jw",
  "venue": "arXiv",
  "versions": [
    {
      "doi": "10.1103/82y9-svrd",
      "pid": null,
      "relation": "published-as",
      "title": null,
      "venue": null
    }
  ]
}