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of the very forward region of a detector at ILC, with LumiCal placed $\\mathrm{2500 \\: mm}$ from the IP.","label":"fig_1","source":"arxiv","key":"5d6af67b88276a187d4ca71c7a5ab2e2","url":"https://inspirehep.net/files/5d6af67b88276a187d4ca71c7a5ab2e2"},{"filename":"lumi_H20-staged-dBS-new.png","material":"preprint","caption":"Integrated luminosity vs. ILC running time in the H-20 operating scenario.","label":"fig_2","source":"arxiv","key":"db45f0d69a2f14e02f73c04247011814","url":"https://inspirehep.net/files/db45f0d69a2f14e02f73c04247011814"},{"filename":"DeltaRin_Zpole_lin.png","material":"preprint","caption":"(a) Impact of uncertainty $\\Delta r_{in}$ of LumiCal FV inner radius on Bhabha counting, at 91.2 GeV; (b) The same at 250 GeV, 500 GeV and 1 TeV center-of-mass energies for AS1 event selection (Section \\ref{sec:sec2.2}).","label":"fig3","source":"arxiv","key":"8c9ea36efad5bac63add25d0b460acc7","url":"https://inspirehep.net/files/8c9ea36efad5bac63add25d0b460acc7"},{"filename":"DeltaRin_ILC_3_AS1_lin.png","material":"preprint","caption":"(a) Impact of uncertainty $\\Delta r_{in}$ of LumiCal FV inner radius on Bhabha counting, at 91.2 GeV; (b) The same at 250 GeV, 500 GeV and 1 TeV center-of-mass energies for AS1 event selection (Section \\ref{sec:sec2.2}).","label":"fig3","source":"arxiv","key":"c45f63d77fd8048e95488ec055fa99e3","url":"https://inspirehep.net/files/c45f63d77fd8048e95488ec055fa99e3"},{"filename":"DeltaRout_Zpole_S-AS1_lin.png","material":"preprint","caption":"(a) Impact of uncertainty $\\Delta r_{out}$ of LumiCal FV outer radius on Bhabha counting, at 91.2 GeV; (b) The same at 250 GeV, 500 GeV and 1 TeV center-of-mass energies for AS1 event selection (Section \\ref{sec:sec2.2}).","label":"fig4","source":"arxiv","key":"84c124ce1bc21f04e30cb5bc38918ed6","url":"https://inspirehep.net/files/84c124ce1bc21f04e30cb5bc38918ed6"},{"filename":"DeltaRout_ILC_3_AS1_5x_lin.png","material":"preprint","caption":"(a) Impact of uncertainty $\\Delta r_{out}$ of LumiCal FV outer radius on Bhabha counting, at 91.2 GeV; (b) The same at 250 GeV, 500 GeV and 1 TeV center-of-mass energies for AS1 event selection (Section \\ref{sec:sec2.2}).","label":"fig4","source":"arxiv","key":"1d12c6f806089b960c83649af1fad3b8","url":"https://inspirehep.net/files/1d12c6f806089b960c83649af1fad3b8"},{"filename":"sigmaR_Zpole_lin.png","material":"preprint","caption":"(a) Impact of the uncertainty $\\sigma_{r}$ of measured shower radial position with respect to the true Bhabha position, at 91.2 GeV; (b) The same at 250 GeV, 500 GeV and 1 TeV center-of-mass energies for AS1 event selection (Section \\ref{sec:sec2.2}).","label":"fig5","source":"arxiv","key":"efe82e2273fbeb5da495534215e57f9a","url":"https://inspirehep.net/files/efe82e2273fbeb5da495534215e57f9a"},{"filename":"sigmaR_ILC_3_AS1_5x_lin.png","material":"preprint","caption":"(a) Impact of the uncertainty $\\sigma_{r}$ of measured shower radial position with respect to the true Bhabha position, at 91.2 GeV; (b) The same at 250 GeV, 500 GeV and 1 TeV center-of-mass energies for AS1 event selection (Section \\ref{sec:sec2.2}).","label":"fig5","source":"arxiv","key":"d2e5a5107fc0babcf887343555bdc140","url":"https://inspirehep.net/files/d2e5a5107fc0babcf887343555bdc140"},{"filename":"DeltaL_Zpole_lin.png","material":"preprint","caption":"(a) Impact of uncertainty of the longitudinal distance $\\Delta l$  between left and right halves of LumiCal, at 91.2 GeV;  (b) The same at 250 GeV, 500 GeV and 1 TeV center-of-mass energies for AS1 event selection (Section \\ref{sec:sec2.2}).","label":"fig6","source":"arxiv","key":"6c97c729d35dcc23650b8e603e9891e2","url":"https://inspirehep.net/files/6c97c729d35dcc23650b8e603e9891e2"},{"filename":"DeltaL_ILC_3_AS1_lin.png","material":"preprint","caption":"(a) Impact of uncertainty of the longitudinal distance $\\Delta l$  between left and right halves of LumiCal, at 91.2 GeV;  (b) The same at 250 GeV, 500 GeV and 1 TeV center-of-mass energies for AS1 event selection (Section \\ref{sec:sec2.2}).","label":"fig6","source":"arxiv","key":"10e5f752c5f3b44fae899e3dbbe3ff47","url":"https://inspirehep.net/files/10e5f752c5f3b44fae899e3dbbe3ff47"},{"filename":"sigmaX_Zpole_5x_lin.png","material":"preprint","caption":"(a) Impact of radial fluctuations $\\sigma_{x_{IP}}$ of LumiCal with respect to the IP, at 91.2 GeV; (b) The same at 250 GeV, 500 GeV and 1 TeV center-of-mass energies for AS1 event selection (Section \\ref{sec:sec2.2}).","label":"fig7","source":"arxiv","key":"a1ab9b2da7c77ef8d76694ec07799552","url":"https://inspirehep.net/files/a1ab9b2da7c77ef8d76694ec07799552"},{"filename":"sigmaX_ILC_3_AS1_5x_lin.png","material":"preprint","caption":"(a) Impact of radial fluctuations $\\sigma_{x_{IP}}$ of LumiCal with respect to the IP, at 91.2 GeV; (b) The same at 250 GeV, 500 GeV and 1 TeV center-of-mass energies for AS1 event selection (Section \\ref{sec:sec2.2}).","label":"fig7","source":"arxiv","key":"e3ed6f3a19323405ff7632c513ce6803","url":"https://inspirehep.net/files/e3ed6f3a19323405ff7632c513ce6803"},{"filename":"sigmaZ_Zpole_5x_lin.png","material":"preprint","caption":"(a) Impact of axial fluctuations $\\sigma_{z_{IP}}$ of LumiCal with respect to the IP, at 91.2 GeV; (b) The same at 250 GeV, 500 GeV and 1 TeV center-of-mass  energies for AS1 event selection (Section \\ref{sec:sec2.2}).","label":"fig8","source":"arxiv","key":"d70a9628c3f7cdb60ed514e09acbd717","url":"https://inspirehep.net/files/d70a9628c3f7cdb60ed514e09acbd717"},{"filename":"sigmaZ_ILC_3_AS1_5x_lin.png","material":"preprint","caption":"(a) Impact of axial fluctuations $\\sigma_{z_{IP}}$ of LumiCal with respect to the IP, at 91.2 GeV; (b) The same at 250 GeV, 500 GeV and 1 TeV center-of-mass  energies for AS1 event selection (Section \\ref{sec:sec2.2}).","label":"fig8","source":"arxiv","key":"c5ffab1951b0a4751e7a575f39efa071","url":"https://inspirehep.net/files/c5ffab1951b0a4751e7a575f39efa071"},{"filename":"tilt_Zpole_line.png","material":"preprint","caption":"(a) Impact of rotation of LumiCal arms around the y-axis for a certain angle $\\mathrm{\\Delta \\varphi}$ (tilt), at 91.2 GeV; (b) The same at 250 GeV, 500 GeV and 1 TeV center-of-mass energies for AS1 event selection (Section \\ref{sec:sec2.2}).","label":"fig9","source":"arxiv","key":"671dc9aefd0cd03ec31d19293fa5951a","url":"https://inspirehep.net/files/671dc9aefd0cd03ec31d19293fa5951a"},{"filename":"tilt_ILC_3_AS1_lin.png","material":"preprint","caption":"(a) Impact of rotation of LumiCal arms around the y-axis for a certain angle $\\mathrm{\\Delta \\varphi}$ (tilt), at 91.2 GeV; (b) The same at 250 GeV, 500 GeV and 1 TeV center-of-mass energies for AS1 event selection (Section \\ref{sec:sec2.2}).","label":"fig9","source":"arxiv","key":"9a8df7e4b94918c66c0f805601ddb153","url":"https://inspirehep.net/files/9a8df7e4b94918c66c0f805601ddb153"},{"filename":"DeltaX_Zpole_lin.png","material":"preprint","caption":"(a) Impact of radial displacements $\\Delta_{x_{IP}}$ of the interaction point with respect to LumiCal, at 91.2 GeV;  (b) The same at 250 GeV, 500 GeV and 1 TeV center-of-mass energies for AS1 event selection (Section \\ref{sec:sec2.2}).","label":"fig10","source":"arxiv","key":"de51deb916934731a9fccfd03e976710","url":"https://inspirehep.net/files/de51deb916934731a9fccfd03e976710"},{"filename":"DeltaX_ILC_3_AS1_lin.png","material":"preprint","caption":"(a) Impact of radial displacements $\\Delta_{x_{IP}}$ of the interaction point with respect to LumiCal, at 91.2 GeV;  (b) The same at 250 GeV, 500 GeV and 1 TeV center-of-mass energies for AS1 event selection (Section \\ref{sec:sec2.2}).","label":"fig10","source":"arxiv","key":"51b813b36725f57e914e49113e341962","url":"https://inspirehep.net/files/51b813b36725f57e914e49113e341962"},{"filename":"DeltaZ_Zpole_lin.png","material":"preprint","caption":"(a) Impact of axial displacements $\\Delta z_{IP}$ of the interaction point with respect to LumiCal, at 91.2 GeV; (b) The same at 250 GeV, 500 GeV and 1 TeV center-of-mass energies for AS1 event selection (Section \\ref{sec:sec2.2}).","label":"fig11","source":"arxiv","key":"8f4bfe42bcfc0113b11654b987d000b7","url":"https://inspirehep.net/files/8f4bfe42bcfc0113b11654b987d000b7"},{"filename":"DeltaZ_ILC_3_AS1_lin.png","material":"preprint","caption":"(a) Impact of axial displacements $\\Delta z_{IP}$ of the interaction point with respect to LumiCal, at 91.2 GeV; (b) The same at 250 GeV, 500 GeV and 1 TeV center-of-mass energies for AS1 event selection (Section \\ref{sec:sec2.2}).","label":"fig11","source":"arxiv","key":"23415ce3f30b12acd3308f83286388dc","url":"https://inspirehep.net/files/23415ce3f30b12acd3308f83286388dc"},{"filename":"sigmabetaZ_Zpole_lin.png","material":"preprint","caption":"(a) Impact of the half-width $\\sigma_{E_{BS}}$ of the Gaussian beam energy spread at 91.2 GeV as a source of longitudinal boost $\\beta_z$ of the final state; (b) The same at 250 GeV, 500 GeV and 1 TeV center-of-mass energies for AS1 event selection (Section \\ref{sec:sec2.2}).","label":"fig12","source":"arxiv","key":"5564f1a54a7bbaa543dbd3839a742209","url":"https://inspirehep.net/files/5564f1a54a7bbaa543dbd3839a742209"},{"filename":"sigmabetaZ_ILC_3_AS_lin.png","material":"preprint","caption":"(a) Impact of the half-width $\\sigma_{E_{BS}}$ of the Gaussian beam energy spread at 91.2 GeV as a source of longitudinal boost $\\beta_z$ of the final state; (b) The same at 250 GeV, 500 GeV and 1 TeV center-of-mass energies for AS1 event selection (Section \\ref{sec:sec2.2}).","label":"fig12","source":"arxiv","key":"6f1accf1de9911f021a3ebabe367ca48","url":"https://inspirehep.net/files/6f1accf1de9911f021a3ebabe367ca48"},{"filename":"betaZ_Zpole_lin.png","material":"preprint","caption":"(a) Impact of the difference in energy $\\Delta E$ between the colliding beams at 91.2 GeV, producing the longitudinal boost $\\beta_z$; (b) The same at 250 GeV, 500 GeV and 1 TeV center-of-mass energies for AS1 event selection (Section \\ref{sec:sec2.2}).","label":"fig13","source":"arxiv","key":"c4500c6392db759825cf06d867e02e61","url":"https://inspirehep.net/files/c4500c6392db759825cf06d867e02e61"},{"filename":"BetaZ_ILC_3_AS1_lin.png","material":"preprint","caption":"(a) Impact of the difference in energy $\\Delta E$ between the colliding beams at 91.2 GeV, producing the longitudinal boost $\\beta_z$; (b) The same at 250 GeV, 500 GeV and 1 TeV center-of-mass energies for AS1 event selection (Section \\ref{sec:sec2.2}).","label":"fig13","source":"arxiv","key":"7a10742a7913c3ea31fcce4062a94fe8","url":"https://inspirehep.net/files/7a10742a7913c3ea31fcce4062a94fe8"}],"inspire_categories":[{"term":"Experiment-HEP","source":"arxiv"},{"term":"Instrumentation","source":"arxiv"}],"first_author":{"emails":["i.smiljanic@vin.bg.ac.rs"],"affiliations_identifiers":[{"schema":"ROR","value":"https://ror.org/02qsmb048"}],"full_name":"Smiljanić, Ivan","ids":[{"schema":"ORCID","value":"0000-0003-3626-158X"},{"schema":"INSPIRE BAI","value":"I.Smiljanic.1"}],"last_name":"Smiljanić","first_name":"Ivan","recid":1046635},"control_number":2804229,"dois":[{"source":"Oxford University Press","value":"10.1093/ptep/ptaf015"}],"document_type":["article"],"texkeys":["Smiljanic:2024twn"],"abstracts":[{"source":"Oxford University Press","value":"Precision measurement of the integrated luminosity L at future Higgs factories, including the International Linear Collider (ILC), is of crucial importance for the cross-section measurements, and in particular for the line-shape measurements at the Z-pole. Since there is no up-to-date estimate of the integrated luminosity uncertainties arising from metrology effects at ILC, here we review the metrology requirements for the targeted precision of L at foreseen ILC center-of-mass energies: 91.2 GeV, 250 GeV, 500 GeV and 1 TeV, using small-angle Bhabha scattering.","abstract_source_suggest":{"input":"Oxford University Press"}},{"source":"arXiv","value":"Precision measurement of the integrated luminosity $\\mathcal{L}$ at future Higgs factories, including ILC, is of crucial importance for the cross-section measurements, and in particular for the line-shape measurements at the Z-pole. Since there is no up-to-date estimate of the integrated luminosity uncertainties arising from metrology effects at ILC, here we review the metrology requirements for the targeted precision of $\\mathcal{L}$ at foreseen ILC center-of-mass energies: 91.2 GeV, 250 GeV, 500 GeV and 1 TeV, using small-angle Bhabha scattering.","abstract_source_suggest":{"input":"arXiv"}}],"primary_arxiv_category":["hep-ex"],"titles":[{"source":"Oxford University Press","title":"Metrology Requirements for the Integrated Luminosity Measurement Using Small-Angle Bhabha Scattering at ILC"},{"source":"arXiv","title":"Metrology requirements for the integrated luminosity measurement using small angle Bhabha scattering at ILC"},{"source":"arXiv","title":"Metrology requirements for the integrated luminosity measurement at ILC"}],"imprints":[{"date":"2025-01-25"}],"curated":false},"links":{"bibtex":"https://inspirehep.net/api/literature/2804229?format=bibtex","latex-eu":"https://inspirehep.net/api/literature/2804229?format=latex-eu","latex-us":"https://inspirehep.net/api/literature/2804229?format=latex-us","json":"https://inspirehep.net/api/literature/2804229?format=json","json-expanded":"https://inspirehep.net/api/literature/2804229?format=json-expanded","cv":"https://inspirehep.net/api/literature/2804229?format=cv","citations":"https://inspirehep.net/api/literature/?q=refersto%3Arecid%3A2804229"},"created":"2024-07-04T04:17:52.519351+00:00","id":"2804229","updated":"2025-03-10T05:27:27.794414+00:00"}],"total":13},"links":{"self":"https://inspirehep.net/api/literature/?q=title%20%22Bhabha%20scattering%22%20and%20title%20luminosity&size=10&page=1","next":"https://inspirehep.net/api/literature/?q=title%20%22Bhabha%20scattering%22%20and%20title%20luminosity&size=10&page=2","bibtex":"https://inspirehep.net/api/literature/?q=title%20%22Bhabha%20scattering%22%20and%20title%20luminosity&size=10&page=1&format=bibtex","latex-eu":"https://inspirehep.net/api/literature/?q=title%20%22Bhabha%20scattering%22%20and%20title%20luminosity&size=10&page=1&format=latex-eu","latex-us":"https://inspirehep.net/api/literature/?q=title%20%22Bhabha%20scattering%22%20and%20title%20luminosity&size=10&page=1&format=latex-us","json":"https://inspirehep.net/api/literature/?q=title%20%22Bhabha%20scattering%22%20and%20title%20luminosity&size=10&page=1&format=json","json-expanded":"https://inspirehep.net/api/literature/?q=title%20%22Bhabha%20scattering%22%20and%20title%20luminosity&size=10&page=1&format=json-expanded","cv":"https://inspirehep.net/api/literature/?q=title%20%22Bhabha%20scattering%22%20and%20title%20luminosity&size=10&page=1&format=cv"}}