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X-WR-CALNAME;VALUE=TEXT:Online: Seminar, Leonard Gross (Cornell University), Equivalence of Helicity and Euclidean Self-Duality for Gauge Fields
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SUMMARY:Online: Seminar, Leonard Gross (Cornell University), Equivalence of Helicity and Euclidean Self-Duality for Gauge Fields
DESCRIPTION:<p>	<drupal-media data-entity-type="media" data-entity-uuid="3a46dae3-6319-4238-9c74-27ddafedc14d" alt="Leonard Gross" data-view-mode="hwp_small"></drupal-media></p><p>	<strong>Location: </strong>Zoom https://harvard.zoom.us/j/779283357 </p><p>	<strong>Time: </strong>Tuesday, April 7, 2020, 10:00 AM (Eastern US), 16:00 (Central Europe), 22:00 (China)</p><p>	<strong>Title:</strong> Equivalence of Helicity and Euclidean Self-Duality for Gauge Fields</p><p>	<strong>Abstract:</strong> Circularly polarized light (i.e. helicity) is a concept defined in terms of plane wave expansions of solutions to Maxwell's equations.  We wish to find  an analogous concept for classical and quantized Yang-Mills fields. Since the classical (hyperbolic) Yang-Mills equation is a non-linear equation, a gauge invariant  plane wave expansion does not exist.  We will first show, in electromagnetism,  an equivalence between the usual plane wave characterization  of helicity and a characterization in terms of (anti-)self duality of a gauge potential on a half space of Euclidean <span class="math-tex">\(\mathbb R^4\)</span>. The transition from Minkowski space to Euclidean space is implemented by the Maxwell-Poisson equation. We will then replace the Maxwell-Poisson equation by the Yang-Mills-Poisson equation to find a decomposition of the Yang-Mills configuration space into submanifolds arguably corresponding to positive and negative helicity. This is a report on the paper [1].</p><p>	<strong>References</strong><br>[1] https://doi.org/10.1016/j.nuclphysb.2019.114685</p><p>	<strong>Additional Ways to Join</strong><br>Join by telephone (use any number to dial in)<br>        +1 929 436 2866<br>        +1 312 626 6799<br>        +1 669 900 6833<br>        +1 253 215 8782<br>        +1 301 715 8592<br>        +1 346 248 7799<br>        +41 43 210 70 42<br>        +41 43 210 71 08<br>        +41 22 591 00 05<br>        +41 22 591 01 56<br>        +41 31 528 09 88<br>        +31 20 794 6520<br>        +31 20 794 7345<br>        +31 20 241 0288<br>        +31 20 794 0854<br>        +31 20 794 6519<br>        +65 3165 1065<br>        +65 3158 7288<br>        +33 1 7095 0350<br>        +33 7 5678 4048<br>        +33 1 7037 2246<br>        +33 1 7037 9729<br>        +33 1 7095 0103<br>        +49 30 5679 5800<br>        +49 695 050 2596<br>        +49 69 7104 9922<br>        +45 32 72 80 11<br>        +45 89 88 37 88<br>        +45 32 70 12 06<br>        +45 32 71 31 57<br>        +45 32 72 80 10<br>        400 669 9381 China Toll-free<br>        400 616 8835 China Toll-free<br>        0 800 561 252 Switzerland Toll-free<br>        0 800 002 622 Switzerland Toll-free<br>        0 800 220 0040 Netherlands Toll-free<br>        0 800 022 1954 Netherlands Toll-free<br>        800 852 6054 Singapore Toll-free<br>        800 101 3814 Singapore Toll-free<br>        0 805 082 588 France Toll-free<br>        0 800 940 415 France Toll-free<br>        0 800 1800 150 Germany Toll-free<br>        0 800 000 6954 Germany Toll-free<br>        80 82 02 88 Denmark Toll-free<br>        80 71 12 51 Denmark Toll-free</p><p>	International numbers available: https://harvard.zoom.us/u/aclg6kOggb</p><p>	One tap mobile: +19294362866,,779283357# US (New York)<br>    <br>Join by SIP conference room system<br>Meeting ID: 779 283 357<br>779283357@zoomcrc.com</p>
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DTSTART:20200407T140000Z
DTEND:20200407T140000Z
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