No confinement without Coulomb confinement

Daniel Zwanziger

    Research output: Contribution to journalArticle

    Abstract

    Confinement is most commonly characterized by the behavior of VD(R), the gauge-invariant potential energy between an external quark-pair at separation R in the representation D of the gauge structure group SU(N). The bound implies that if the potential between external quarks in the fundamental representation increases linearly at large R, VF(R)∼σR, where σ is the standard string tension.

    Original languageEnglish (US)
    JournalPhysical Review Letters
    Volume90
    Issue number10
    StatePublished - Mar 14 2003

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    quarks
    strings
    potential energy

    ASJC Scopus subject areas

    • Physics and Astronomy(all)

    Cite this

    No confinement without Coulomb confinement. / Zwanziger, Daniel.

    In: Physical Review Letters, Vol. 90, No. 10, 14.03.2003.

    Research output: Contribution to journalArticle

    Zwanziger, Daniel. / No confinement without Coulomb confinement. In: Physical Review Letters. 2003 ; Vol. 90, No. 10.
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