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<titleInfo><title>Second order semiclassics with self generated magnetic fields</title></titleInfo>


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<name type="personal">
  <namePart type="given">László</namePart>
  <namePart type="family">Erdös</namePart>
  <role><roleTerm type="text">author</roleTerm> </role><identifier type="local">4DBD5372-F248-11E8-B48F-1D18A9856A87</identifier><description xsi:type="identifierDefinition" type="orcid">0000-0001-5366-9603</description></name>
<name type="personal">
  <namePart type="given">Søren</namePart>
  <namePart type="family">Fournais</namePart>
  <role><roleTerm type="text">author</roleTerm> </role></name>
<name type="personal">
  <namePart type="given">Jan</namePart>
  <namePart type="family">Solovej</namePart>
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<abstract lang="eng">We consider the semiclassical asymptotics of the sum of negative eigenvalues of the three-dimensional Pauli operator with an external potential and a self-generated magnetic field B. We also add the field energy β ∫ B 2 and we minimize over all magnetic fields. The parameter β effectively determines the strength of the field. We consider the weak field regime with βh 2 ≥ const &amp;gt; 0, where h is the semiclassical parameter. For smooth potentials we prove that the semiclassical asymptotics of the total energy is given by the non-magnetic Weyl term to leading order with an error bound that is smaller by a factor h 1+e{open}, i. e. the subleading term vanishes. However for potentials with a Coulomb singularity, the subleading term does not vanish due to the non-semiclassical effect of the singularity. Combined with a multiscale technique, this refined estimate is used in the companion paper (Erdo{double acute}s et al. in Scott correction for large molecules with a self-generated magnetic field, Preprint, 2011) to prove the second order Scott correction to the ground state energy of large atoms and molecules.</abstract>

<originInfo><publisher>Birkhäuser</publisher><dateIssued encoding="w3cdtf">2012</dateIssued>
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<relatedItem type="host"><titleInfo><title>Annales Henri Poincare</title></titleInfo><identifier type="doi">10.1007/s00023-011-0150-z</identifier>
<part><detail type="volume"><number>13</number></detail><detail type="issue"><number>4</number></detail><extent unit="pages">671 - 730</extent>
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<short>L. Erdös, S. Fournais, J. Solovej, Annales Henri Poincare 13 (2012) 671–730.</short>
<apa>Erdös, L., Fournais, S., &amp;#38; Solovej, J. (2012). Second order semiclassics with self generated magnetic fields. &lt;i&gt;Annales Henri Poincare&lt;/i&gt;. Birkhäuser. &lt;a href=&quot;https://doi.org/10.1007/s00023-011-0150-z&quot;&gt;https://doi.org/10.1007/s00023-011-0150-z&lt;/a&gt;</apa>
<ama>Erdös L, Fournais S, Solovej J. Second order semiclassics with self generated magnetic fields. &lt;i&gt;Annales Henri Poincare&lt;/i&gt;. 2012;13(4):671-730. doi:&lt;a href=&quot;https://doi.org/10.1007/s00023-011-0150-z&quot;&gt;10.1007/s00023-011-0150-z&lt;/a&gt;</ama>
<mla>Erdös, László, et al. “Second Order Semiclassics with Self Generated Magnetic Fields.” &lt;i&gt;Annales Henri Poincare&lt;/i&gt;, vol. 13, no. 4, Birkhäuser, 2012, pp. 671–730, doi:&lt;a href=&quot;https://doi.org/10.1007/s00023-011-0150-z&quot;&gt;10.1007/s00023-011-0150-z&lt;/a&gt;.</mla>
<ista>Erdös L, Fournais S, Solovej J. 2012. Second order semiclassics with self generated magnetic fields. Annales Henri Poincare. 13(4), 671–730.</ista>
<ieee>L. Erdös, S. Fournais, and J. Solovej, “Second order semiclassics with self generated magnetic fields,” &lt;i&gt;Annales Henri Poincare&lt;/i&gt;, vol. 13, no. 4. Birkhäuser, pp. 671–730, 2012.</ieee>
<chicago>Erdös, László, Søren Fournais, and Jan Solovej. “Second Order Semiclassics with Self Generated Magnetic Fields.” &lt;i&gt;Annales Henri Poincare&lt;/i&gt;. Birkhäuser, 2012. &lt;a href=&quot;https://doi.org/10.1007/s00023-011-0150-z&quot;&gt;https://doi.org/10.1007/s00023-011-0150-z&lt;/a&gt;.</chicago>
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