Guardado en:
| Autores principales: | , , |
|---|---|
| Formato: | Preprint |
| Publicado: |
2025
|
| Materias: | |
| Acceso en línea: | https://arxiv.org/abs/2506.01505 |
| Etiquetas: |
Agregar Etiqueta
Sin Etiquetas, Sea el primero en etiquetar este registro!
|
| _version_ | 1866910980611506176 |
|---|---|
| author | Murray, William O'Neill, Matt O'Gara, Finn |
| author_facet | Murray, William O'Neill, Matt O'Gara, Finn |
| contents | The cleanest way to discover a new particle is generally the "bump-hunt" methodology: looking for a localised excess in a mass (or related) distribution. However, if the mass of the particle being discovered is not known the procedure of quoting the most significant excess seen is "greedy", and random fluctuations from the background can be merged with the signal. This means that an observed 3σ evidence probably has the rate over-estimated by of order 10% and the mass uncertainty underestimated by more like 20%. If the width of the particle being discovered is also unknown, or the experimental resolution uncertain, the effect grows larger. In the context of LHC, the data-doubling period is now measured in years. If evidence for a genuine signal is obtained at the 3σ level, the true signal rate probably corresponds to a lower significance. The additional data required to produce a 5σ discovery may be hundreds of inverse femtobarn more than might be naively expected. |
| format | Preprint |
| id |
arxiv_https___arxiv_org_abs_2506_01505 |
| institution | arXiv |
| publishDate | 2025 |
| record_format | arxiv |
| spellingShingle | Biased rate estimates in bump-hunt searches Murray, William O'Neill, Matt O'Gara, Finn High Energy Physics - Phenomenology The cleanest way to discover a new particle is generally the "bump-hunt" methodology: looking for a localised excess in a mass (or related) distribution. However, if the mass of the particle being discovered is not known the procedure of quoting the most significant excess seen is "greedy", and random fluctuations from the background can be merged with the signal. This means that an observed 3σ evidence probably has the rate over-estimated by of order 10% and the mass uncertainty underestimated by more like 20%. If the width of the particle being discovered is also unknown, or the experimental resolution uncertain, the effect grows larger. In the context of LHC, the data-doubling period is now measured in years. If evidence for a genuine signal is obtained at the 3σ level, the true signal rate probably corresponds to a lower significance. The additional data required to produce a 5σ discovery may be hundreds of inverse femtobarn more than might be naively expected. |
| title | Biased rate estimates in bump-hunt searches |
| topic | High Energy Physics - Phenomenology |
| url | https://arxiv.org/abs/2506.01505 |