QCD Perturbation Theory: It's not what you were taught
Physical quantities in QCD do not depend upon $\alpha_s(Q)$. There is no way to measure $\alpha_s(Q)$ experimentally. If those statements sound shocking, please read on. They are actually well-known facts, though ones that are constantly being ignored in the QCD literature. Renormalized perturbation...
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creator | Stevenson, P. M |
description | Physical quantities in QCD do not depend upon $\alpha_s(Q)$. There is no way
to measure $\alpha_s(Q)$ experimentally. If those statements sound shocking,
please read on. They are actually well-known facts, though ones that are
constantly being ignored in the QCD literature. Renormalized perturbation
theory is not an ordinary power-series expansion; its renormalization-scheme
ambiguity is not merely a minor nuisance. Rather, it is a structure in which
invariance under redefinitions of the coupling is a fundamental symmetry -- a
symmetry that, like any other, deserves respect. I speak bluntly because
without a change in mindset perturbative QCD can never become a proper,
scientific enterprise. |
doi_str_mv | 10.48550/arxiv.2409.01228 |
format | Article |
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to measure $\alpha_s(Q)$ experimentally. If those statements sound shocking,
please read on. They are actually well-known facts, though ones that are
constantly being ignored in the QCD literature. Renormalized perturbation
theory is not an ordinary power-series expansion; its renormalization-scheme
ambiguity is not merely a minor nuisance. Rather, it is a structure in which
invariance under redefinitions of the coupling is a fundamental symmetry -- a
symmetry that, like any other, deserves respect. I speak bluntly because
without a change in mindset perturbative QCD can never become a proper,
scientific enterprise.</description><identifier>DOI: 10.48550/arxiv.2409.01228</identifier><language>eng</language><subject>Physics - High Energy Physics - Experiment ; Physics - High Energy Physics - Phenomenology ; Physics - High Energy Physics - Theory</subject><creationdate>2024-09</creationdate><rights>http://creativecommons.org/licenses/by/4.0</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,780,885</link.rule.ids><linktorsrc>$$Uhttps://arxiv.org/abs/2409.01228$$EView_record_in_Cornell_University$$FView_record_in_$$GCornell_University$$Hfree_for_read</linktorsrc><backlink>$$Uhttps://doi.org/10.48550/arXiv.2409.01228$$DView paper in arXiv$$Hfree_for_read</backlink></links><search><creatorcontrib>Stevenson, P. M</creatorcontrib><title>QCD Perturbation Theory: It's not what you were taught</title><description>Physical quantities in QCD do not depend upon $\alpha_s(Q)$. There is no way
to measure $\alpha_s(Q)$ experimentally. If those statements sound shocking,
please read on. They are actually well-known facts, though ones that are
constantly being ignored in the QCD literature. Renormalized perturbation
theory is not an ordinary power-series expansion; its renormalization-scheme
ambiguity is not merely a minor nuisance. Rather, it is a structure in which
invariance under redefinitions of the coupling is a fundamental symmetry -- a
symmetry that, like any other, deserves respect. I speak bluntly because
without a change in mindset perturbative QCD can never become a proper,
scientific enterprise.</description><subject>Physics - High Energy Physics - Experiment</subject><subject>Physics - High Energy Physics - Phenomenology</subject><subject>Physics - High Energy Physics - Theory</subject><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><sourceid>GOX</sourceid><recordid>eNpjYJA0NNAzsTA1NdBPLKrILNMzMjGw1DMwNDKy4GQwC3R2UQhILSopLUpKLMnMz1MIyUjNL6q0UvAsUS9WyMsvUSjPSCxRqMwvVShPLUpVKEksTc8o4WFgTUvMKU7lhdLcDPJuriHOHrpgG-ILijJzE4sq40E2xYNtMiasAgBE7zJD</recordid><startdate>20240902</startdate><enddate>20240902</enddate><creator>Stevenson, P. M</creator><scope>GOX</scope></search><sort><creationdate>20240902</creationdate><title>QCD Perturbation Theory: It's not what you were taught</title><author>Stevenson, P. M</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-arxiv_primary_2409_012283</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2024</creationdate><topic>Physics - High Energy Physics - Experiment</topic><topic>Physics - High Energy Physics - Phenomenology</topic><topic>Physics - High Energy Physics - Theory</topic><toplevel>online_resources</toplevel><creatorcontrib>Stevenson, P. M</creatorcontrib><collection>arXiv.org</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Stevenson, P. M</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>QCD Perturbation Theory: It's not what you were taught</atitle><date>2024-09-02</date><risdate>2024</risdate><abstract>Physical quantities in QCD do not depend upon $\alpha_s(Q)$. There is no way
to measure $\alpha_s(Q)$ experimentally. If those statements sound shocking,
please read on. They are actually well-known facts, though ones that are
constantly being ignored in the QCD literature. Renormalized perturbation
theory is not an ordinary power-series expansion; its renormalization-scheme
ambiguity is not merely a minor nuisance. Rather, it is a structure in which
invariance under redefinitions of the coupling is a fundamental symmetry -- a
symmetry that, like any other, deserves respect. I speak bluntly because
without a change in mindset perturbative QCD can never become a proper,
scientific enterprise.</abstract><doi>10.48550/arxiv.2409.01228</doi><oa>free_for_read</oa></addata></record> |
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subjects | Physics - High Energy Physics - Experiment Physics - High Energy Physics - Phenomenology Physics - High Energy Physics - Theory |
title | QCD Perturbation Theory: It's not what you were taught |
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