Anomalous prompt photon production in hadronic collisions at low-\(x_T\)
We investigate the discrepancy that exists at low-\(x_T=2p_T/\sqrt{s}\) between the next--to--leading order QCD calculations of prompt photon production and the measured cross section. The central values of the measured cross section are of order 100\% larger than QCD predictions in this region. It...
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description | We investigate the discrepancy that exists at low-\(x_T=2p_T/\sqrt{s}\) between the next--to--leading order QCD calculations of prompt photon production and the measured cross section. The central values of the measured cross section are of order 100\% larger than QCD predictions in this region. It has been suggested that the bremsstrahlung contribution may account for this discrepancy. The quark fragmentation function \(D_{\gamma/q}(z)\) has not been measured and an exactly known asymptotic form is normally used in calculations. We examine the effect of much larger fragmentation functions on the QCD predictions. After illustrating the effect of the large fragmentation functions in some detail for recent CDF data at \(\sqrt{s}\)=1.8~TeV, we perform a \(\chi^2\) fit to 8 prompt photon data sets ranging in CMS energy from 24~GeV to 1.8~TeV. While a large fragmentation function normalization may prove to play an important role in resolving the discrepancy, the present theoretical and experimental uncertainties prevent any definite normalization value from being determined. |
doi_str_mv | 10.48550/arxiv.9211233 |
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The central values of the measured cross section are of order 100\% larger than QCD predictions in this region. It has been suggested that the bremsstrahlung contribution may account for this discrepancy. The quark fragmentation function \(D_{\gamma/q}(z)\) has not been measured and an exactly known asymptotic form is normally used in calculations. We examine the effect of much larger fragmentation functions on the QCD predictions. After illustrating the effect of the large fragmentation functions in some detail for recent CDF data at \(\sqrt{s}\)=1.8~TeV, we perform a \(\chi^2\) fit to 8 prompt photon data sets ranging in CMS energy from 24~GeV to 1.8~TeV. While a large fragmentation function normalization may prove to play an important role in resolving the discrepancy, the present theoretical and experimental uncertainties prevent any definite normalization value from being determined.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.9211233</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Asymptotic methods ; Bremsstrahlung ; Cross-sections ; Fragmentation ; Mathematical analysis</subject><ispartof>arXiv.org, 1992-11</ispartof><rights>1992. This work is published under https://arxiv.org/licenses/assumed-1991-2003/license.html (the “License”). 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The quark fragmentation function \(D_{\gamma/q}(z)\) has not been measured and an exactly known asymptotic form is normally used in calculations. We examine the effect of much larger fragmentation functions on the QCD predictions. After illustrating the effect of the large fragmentation functions in some detail for recent CDF data at \(\sqrt{s}\)=1.8~TeV, we perform a \(\chi^2\) fit to 8 prompt photon data sets ranging in CMS energy from 24~GeV to 1.8~TeV. 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The central values of the measured cross section are of order 100\% larger than QCD predictions in this region. It has been suggested that the bremsstrahlung contribution may account for this discrepancy. The quark fragmentation function \(D_{\gamma/q}(z)\) has not been measured and an exactly known asymptotic form is normally used in calculations. We examine the effect of much larger fragmentation functions on the QCD predictions. After illustrating the effect of the large fragmentation functions in some detail for recent CDF data at \(\sqrt{s}\)=1.8~TeV, we perform a \(\chi^2\) fit to 8 prompt photon data sets ranging in CMS energy from 24~GeV to 1.8~TeV. While a large fragmentation function normalization may prove to play an important role in resolving the discrepancy, the present theoretical and experimental uncertainties prevent any definite normalization value from being determined.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.9211233</doi><oa>free_for_read</oa></addata></record> |
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subjects | Asymptotic methods Bremsstrahlung Cross-sections Fragmentation Mathematical analysis |
title | Anomalous prompt photon production in hadronic collisions at low-\(x_T\) |
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