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DTSTART:20200308T030000
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DTSTART:20191103T010000
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BEGIN:VEVENT
DTSTAMP:20191205T190552Z
UID:5A9A6617-89E9-488F-A6AC-9216B6176490
DTSTART;TZID=US/Eastern:20191204T153000
DTEND;TZID=US/Eastern:20191204T163000
DESCRIPTION:The most fundamental plasma is the quantum vacuum\, but it rema
 ins largely inaccessible to experiments because of the energy scales invol
 ved. The minimum temperature required to “ionize” the vacuum is equiva
 lent to the mass of an electron-positron pair\, 1 MeV\, or about 1010K. On
 e way to imagine creating an e+e- plasma out of “nothing” is through t
 unnel ionization of the vacuum by a laser\; but simple scaling shows that 
 the intensity required to reach the tunneling threshold must be more than 
 1029 W/cm2\, which has been called the “Schwinger threshold”. This tal
 k will introduce the experimental methods we will use to reach this regime
 \, and what we might expect to find.\n\nCo-sponsored by: MIPSE\n\nSpeaker(
 s): Prof. Philip Bucksbaum\, \n\nRoom: 1005\, Bldg: EECS\, 1301 Beal Ave\,
  Ann Arbor\, Michigan\, United States\, 48109
LOCATION:Room: 1005\, Bldg: EECS\, 1301 Beal Ave\, Ann Arbor\, Michigan\, U
 nited States\, 48109
ORGANIZER:jordann@umich.edu
SEQUENCE:1
SUMMARY:The Schwinger Plasma: An Experimental Program to Study the Plasmas 
 That Exist Inside the Vacuum
URL;VALUE=URI:https://events.vtools.ieee.org/m/209871
X-ALT-DESC:Description: &lt;br /&gt;&lt;p&gt;&lt;span style=&quot;color: #333333\; font-family:
  &#39;IBM Plex Sans Condensed&#39;\; font-size: 17.6px\; font-style: normal\; font
 -variant-ligatures: normal\; font-variant-caps: normal\; font-weight: 400\
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 ;&quot;&gt;The most fundamental plasma is the quantum vacuum\, but it remains larg
 ely inaccessible to experiments because of the energy scales involved. The
  minimum temperature required to &amp;ldquo\;ionize&amp;rdquo\; the vacuum is equi
 valent to the mass of an electron-positron pair\, 1 MeV\, or about 1010K. 
 One way to imagine creating an e+e- plasma out of &amp;ldquo\;nothing&amp;rdquo\; 
 is through tunnel ionization of the vacuum by a laser\; but simple scaling
  shows that the intensity required to reach the tunneling threshold must b
 e more than 1029 W/cm2\, which has been called the &amp;ldquo\;Schwinger thres
 hold&amp;rdquo\;. This talk will introduce the experimental methods we will us
 e to reach this regime\, and what we might expect to find.&lt;/span&gt;&lt;/p&gt;
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