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  <div class="openurl"><a href="http://worldcatlibraries.org/registry/gateway?sid=FIZ-Karlsruhe%3AZMATH&amp;genre=article&amp;aulast=Faltings&amp;atitle=Stable+%3Cspan%3E%3Cmath+xmlns%3D%27http%3A%2F%2Fwww.w3.org%2F1998%2FMath%2FMathML%27%3E%3Cmi%3EG%3C%2Fmi%3E%3C%2Fmath%3E%3C%2Fspan%3E-bundles+and+projective+connections.&amp;title=Journal+of+Algebraic+Geometry&amp;stitle=J.+Algebr.+Geom.&amp;issn=1056-3911&amp;volume=2&amp;issue=3&amp;spage=507&amp;date=1993" onclick="window.open('http://worldcatlibraries.org/registry/gateway?sid=FIZ-Karlsruhe%3AZMATH&amp;genre=article&amp;aulast=Faltings&amp;atitle=Stable+%3Cspan%3E%3Cmath+xmlns%3D%27http%3A%2F%2Fwww.w3.org%2F1998%2FMath%2FMathML%27%3E%3Cmi%3EG%3C%2Fmi%3E%3C%2Fmath%3E%3C%2Fspan%3E-bundles+and+projective+connections.&amp;title=Journal+of+Algebraic+Geometry&amp;stitle=J.+Algebr.+Geom.&amp;issn=1056-3911&amp;volume=2&amp;issue=3&amp;spage=507&amp;date=1993','openurl','width=800,height=600,menubar,scrollbars');return false" title="WorldCat.org"><img src="images/worldcat.gif" alt="WorldCat.org" title="WorldCat.org" /></a></div>

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  <a href="search/?q=an%3A0790.14019">Zbl 0790.14019</a><br />                    <a class="meta bold" href="search/?q=ai:faltings.gerd">Faltings, Gerd</a>            </div>
<div>
  <strong>Stable <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>G</mi></math></span>-bundles and projective connections.<span class="normal"> (English)</span></strong>
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<div>
                                          
            <a href="journals/?q=an:00001863">J. Algebr. Geom.</a>
             2, No.3, 507-568 (1993).
                              </div>


  <div class="review">
    <p>This paper gives a self-contained, detailed account of the construction and compactification of the moduli space of Higgs bundle on (families of) curves. It is divided into five parts: I. The theorem of the cube; II. <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>G</mi></math></span>-bundles; III. Abelianisation; IV. Projective connections; V. Infinitesimal parabolic structure.</p> <p>Part I starts with a theorem on the determinant of the cohomology of coherent sheaves on a curve. It is shown that the theorem of the cube follows from this result. A second application is at the basis of the construction, via theta-functions, of global sections of determinant bundles on the moduli space of Higgs bundles. More precisely, let <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>S</mi></math></span> be a noetherian base scheme for the family of curves <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><mi>&#x3C0;</mi><mo>:</mo><mi>C</mi><mo>&#x02192;</mo><mi>S</mi></mrow></math></span>, with <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>&#x3C0;</mi></math></span> proper, all fibers of dimension <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><mo>&#x02264;</mo><mn>1</mn></mrow></math></span>, and such that <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><msub><mi>&#x3C0;</mi> <mo>*</mo> </msub><mrow><mo>(</mo><msub><mi>&#x1D4AA;</mi> <mi>C</mi> </msub><mo>)</mo></mrow><mo>=</mo><msub><mi>&#x1D4AA;</mi> <mi>S</mi> </msub></mrow></math></span>. A Higgs bundle on <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>C</mi></math></span> is a vector bundle <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>&#x2131;</mi></math></span> together with a section <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>&#x3B8;</mi></math></span> of <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><mtext>&#x393;</mtext><mo>(</mo><mi>C</mi><mo>,</mo><mi>&#x2130;</mi><mi>n</mi><mi>d</mi><mrow><mo>(</mo><mi>&#x2131;</mi><mo>)</mo></mrow><mo>&#x02297;</mo><msub><mi>&#x3C9;</mi> <mi>C</mi> </msub><mo>)</mo></mrow></math></span>. The coefficients of the characteristic polynomial of <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>&#x3B8;</mi></math></span> define global sections <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><msub><mi>f</mi> <mi>i</mi> </msub><mo>&#x02208;</mo><mtext>&#x393;</mtext><mrow><mo>(</mo><mi>C</mi><mo>,</mo><msup><mi>&#x3C9;</mi> <mi>i</mi> </msup><mo>)</mo></mrow></mrow></math></span>, and the affine space classifying such sections is called the characteristic variety <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><mi>&#x1D49E;</mi><mi>h</mi><mi>a</mi><mi>r</mi></mrow></math></span> (it depends on <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><mtext>rk</mtext><mo>(</mo><mi>&#x2131;</mi><mo>)</mo><mo>)</mo></mrow></math></span>, and <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>&#x2131;</mi></math></span> defines a point <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><mtext>char</mtext><mo>(</mo><mi>&#x2131;</mi><mo>)</mo></mrow></math></span> in <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><mi>&#x1D49E;</mi><mi>h</mi><mi>a</mi><mi>r</mi></mrow></math></span>. Such a Higgs bundle will often be denoted <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><mo>(</mo><mi>&#x2131;</mi><mo>,</mo><mi>&#x3B8;</mi><mo>)</mo></mrow></math></span>. One has the notion of (semi)-stability for Higgs bundles, and any semistable Higgs bundle admits a Jordan- Hölder (JH) filtration by subbundles with stable quotieents of constant ratio degree/rank. The isomorphism classes and multiplicities of these stable components are independent of the filtration. Two semi-stable Higgs bundles are called JH-equivalent if these coincide. A result on JH- equivalence is derived and used to show that the theta-functions separate points in the moduli space of Higgs bundles. The moduli-space of stable Higgs bundles of given rank and degree is constructed as an algebraic space <span><math xmlns='http://www.w3.org/1998/Math/MathML'><msubsup><mrow><mi>&#x2133;</mi></mrow> <mi>&#x3B8;</mi> <mn>0</mn> </msubsup></math></span>. Then <span><math xmlns='http://www.w3.org/1998/Math/MathML'><msubsup><mi>&#x2133;</mi> <mi>&#x3B8;</mi> <mn>0</mn> </msubsup></math></span> embeds as an open subscheme into the onrmalization <span><math xmlns='http://www.w3.org/1998/Math/MathML'><msub><mi>&#x2133;</mi> <mi>&#x3B8;</mi> </msub></math></span> of <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><msup><mi>&#x2119;</mi> <mi>N</mi> </msup><mo>&#xD7;</mo><mi>&#x1D49E;</mi><mi>h</mi><mi>a</mi><mi>r</mi></mrow></math></span> (for suitable <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><mi>N</mi><mo>)</mo></mrow></math></span> in <span><math xmlns='http://www.w3.org/1998/Math/MathML'><msubsup><mrow><mi>&#x2133;</mi></mrow> <mi>&#x3B8;</mi> <mn>0</mn> </msubsup></math></span>.</p> <p>In part II one considers a reductive connected algebraic group <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>&#x1D4A2;</mi></math></span> over a smooth projective connected curve <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>C</mi></math></span> over a field <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>k</mi></math></span>. A <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>&#x1D4A2;</mi></math></span>-torsor <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>P</mi></math></span> on <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>C</mi></math></span>, together with an element</p> <div><math mode='display' xmlns='http://www.w3.org/1998/Math/MathML'><mrow><mi>&#x3B8;</mi><mo>&#x02208;</mo><mtext>&#x393;</mtext><mo>(</mo><mi>C</mi><mo>,</mo><mtext>Lie</mtext><mrow><mo>(</mo><msub><mi>&#x1D4A2;</mi> <mi>P</mi> </msub><mo>)</mo></mrow><mo>&#xD7;</mo><msub><mi>&#x3C9;</mi> <mi>C</mi> </msub><mo>)</mo></mrow></math></div> <p>is called semistable if <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><mo>(</mo><mtext>Lie</mtext><mrow><mo>(</mo><msub><mi>&#x1D4A2;</mi> <mi>P</mi> </msub><mo>)</mo></mrow></mrow></math></span>, ad<span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><mo>(</mo><mi>&#x3B8;</mi><mo>)</mo><mo>)</mo></mrow></math></span> is a semistable Higgs bundle of degree zero. One also has the notion of stable <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>P</mi></math></span>. The main result on semistable pairs <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><mo>(</mo><mi>P</mi><mo>,</mo><mi>&#x3B8;</mi><mo>)</mo></mrow></math></span> is the following semistable reduction theorem: If <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>V</mi></math></span> is a complete discrete valuation ring with fraction field <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>K</mi></math></span>, <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><mi>C</mi><mo>&#x02192;</mo><mi>V</mi></mrow></math></span> a smooth projective curve, <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><mo>(</mo><msub><mi>P</mi> <mi>K</mi> </msub><mo>,</mo><msub><mi>&#x3B8;</mi> <mi>K</mi> </msub><mo>)</mo></mrow></math></span> a semistable pair (associated with a connected reductive group <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>&#x1D4A2;</mi></math></span> over <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><mi>C</mi><mo>)</mo></mrow></math></span> whose characteristic is integral over <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>V</mi></math></span>, then there exists a finite extension <span><math xmlns='http://www.w3.org/1998/Math/MathML'><msup><mi>V</mi> <mo>&#x27;</mo> </msup></math></span> of <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>V</mi></math></span> such that the base extension of <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><mo>(</mo><msub><mi>P</mi> <mi>K</mi> </msub><mo>,</mo><msub><mi>&#x3B8;</mi> <mi>K</mi> </msub><mo>)</mo></mrow></math></span> extends to a semistable pair on <span><math xmlns='http://www.w3.org/1998/Math/MathML'><msub><mi>C</mi> <msup><mi>V</mi> <mo>&#x27;</mo> </msup> </msub></math></span>. Furthermore, if the special fiber of this extension is stable, then any other semistable extension is isomorphic to it. For stable <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><mo>(</mo><mi>P</mi><mo>,</mo><mi>&#x3B8;</mi><mo>)</mo></mrow></math></span> one is led to construct an algebraic moduli stack <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><msubsup><mrow><mi>&#x2133;</mi></mrow> <mi>&#x3B8;</mi> <mn>0</mn> </msubsup><mrow><mo>(</mo><mi>&#x1D4A2;</mi><mo>)</mo></mrow></mrow></math></span> and the coarse moduli space <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><msubsup><mi>M</mi> <mi>&#x3B8;</mi> <mn>0</mn> </msubsup><mrow><mo>(</mo><mi>&#x1D4A2;</mi><mo>)</mo></mrow></mrow></math></span> which is shown to be quasi-projective of explicitly calculated relative dimension over a suitable base. As before one defines a <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><msub><mi>M</mi> <mi>&#x3B8;</mi> </msub><mrow><mo>(</mo><mi>&#x1D4A2;</mi><mo>)</mo></mrow></mrow></math></span> as the normalisation of a <span><math xmlns='http://www.w3.org/1998/Math/MathML'><msup><mi>&#x2119;</mi> <mi>N</mi> </msup></math></span> in <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><msubsup><mi>M</mi> <mi>&#x3B8;</mi> <mn>0</mn> </msubsup><mrow><mo>(</mo><mi>&#x1D4A2;</mi><mo>)</mo></mrow></mrow></math></span>. Then <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><msub><mi>M</mi> <mi>&#x3B8;</mi> </msub><mrow><mo>(</mo><mi>&#x1D4A2;</mi><mo>)</mo></mrow></mrow></math></span> is projective over <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><mi>&#x1D49E;</mi><mi>h</mi><mi>a</mi><mi>r</mi></mrow></math></span> and contains <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><msubsup><mi>M</mi> <mi>&#x3B8;</mi> <mn>0</mn> </msubsup><mrow><mo>(</mo><mi>&#x1D4A2;</mi><mo>)</mo></mrow></mrow></math></span> as an open subscheme. Then, for example, if <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>C</mi></math></span> has genus <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><mo>&gt;</mo><mn>2</mn></mrow></math></span>, the boundary <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><msub><mi>M</mi> <mi>&#x3B8;</mi> </msub><mrow><mo>(</mo><mi>&#x1D4A2;</mi><mo>)</mo></mrow><mo>-</mo><msubsup><mi>M</mi> <mi>&#x3B8;</mi> <mn>0</mn> </msubsup><mrow><mo>(</mo><mi>&#x1D4A2;</mi><mo>)</mo></mrow></mrow></math></span> has codimension <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><mo>&#x2265;</mo><mn>4</mn></mrow></math></span>. Many other results are derived.</p> <p>In part III the theory is extended to exceptional groups. As a corollary of the theory one obtains, with the notations above, that the set of connected components of the moduli space <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><msup><mrow><mi>&#x2133;</mi></mrow> <mn>0</mn> </msup><mrow><mo>(</mo><mi>&#x1D4A2;</mi><mo>)</mo></mrow></mrow></math></span> of stable (Higgs) <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>&#x1D4A2;</mi></math></span>-bundles coincides with that of <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><msubsup><mrow><mi>&#x2133;</mi></mrow> <mi>&#x3B8;</mi> <mn>0</mn> </msubsup><mrow><mo>(</mo><mi>&#x1D4A2;</mi><mo>)</mo></mrow></mrow></math></span>, <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><msub><mi>M</mi> <mi>&#x3B8;</mi> </msub><mrow><mo>(</mo><mi>&#x1D4A2;</mi><mo>)</mo></mrow></mrow></math></span> as well as that of a generic fiber of <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><msubsup><mrow><mi>&#x2133;</mi></mrow> <mi>&#x3B8;</mi> <mn>0</mn> </msubsup><mrow><mo>(</mo><mi>&#x1D4A2;</mi><mo>)</mo></mrow><mo>&#x02192;</mo><mi>&#x1D49E;</mi><mi>h</mi><mi>a</mi><mi>r</mi></mrow></math></span>, under the natural mappings. Among many other results, one application of abelianisation is given by another corollary: On each connected component of <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><msubsup><mrow><mi>&#x2133;</mi></mrow> <mi>&#x3B8;</mi> <mn>0</mn> </msubsup><mrow><mo>(</mo><mi>&#x1D4A2;</mi><mo>)</mo></mrow></mrow></math></span>, all global functions are obtained by pullback from <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><mi>&#x1D49E;</mi><mi>h</mi><mi>a</mi><mi>r</mi></mrow></math></span>.</p> <p>In part IV the accent is on <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><msup><mrow><mi>&#x2133;</mi></mrow> <mn>0</mn> </msup><mrow><mo>(</mo><mi>&#x1D4A2;</mi><mo>)</mo></mrow></mrow></math></span>, where <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>&#x1D4A2;</mi></math></span> is the twisted form of some semi-simple <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>G</mi></math></span>. The notion of <span><math xmlns='http://www.w3.org/1998/Math/MathML'><msub><mtext>&#x3a9;</mtext> <mi>C</mi> </msub></math></span>- connections <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>&#x02207;</mi></math></span> on <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>&#x1D4A2;</mi></math></span>-torsors <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>P</mi></math></span> is introduced. <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><msubsup><mrow><mi>&#x2133;</mi></mrow> <mi>&#x02207;</mi> <mn>0</mn> </msubsup><mrow><mo>(</mo><mi>&#x1D4A2;</mi><mo>)</mo></mrow></mrow></math></span> denotes the moduli stack of such pairs <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><mo>(</mo><mi>P</mi><mo>,</mo><mi>&#x02207;</mi><mo>)</mo></mrow></math></span> with <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>P</mi></math></span> stable. It is fibered over <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><msup><mrow><mi>&#x2133;</mi></mrow> <mn>0</mn> </msup><mrow><mo>(</mo><mi>&#x1D4A2;</mi><mo>)</mo></mrow></mrow></math></span>. Over <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>&#x2102;</mi></math></span>, <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><msubsup><mrow><mi>&#x2133;</mi></mrow> <mi>&#x02207;</mi> <mn>0</mn> </msubsup><mrow><mo>(</mo><mi>&#x1D4A2;</mi><mo>)</mo></mrow></mrow></math></span> classifies bundles with integrable connections, i.e. representations of <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><msub><mi>&#x3C0;</mi> <mn>1</mn> </msub><mrow><mo>(</mo><mi>C</mi><mo>)</mo></mrow></mrow></math></span>. A locally faithful <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>&#x1D4A2;</mi></math></span>-representation <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>&#x2131;</mi></math></span> defines a line bundle <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><mi>&#x2112;</mi><mo>=</mo><mi>&#x2112;</mi><mo>(</mo><mi>&#x2131;</mi><mo>)</mo></mrow></math></span> on <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><msup><mrow><mi>&#x2133;</mi></mrow> <mn>0</mn> </msup><mrow><mo>(</mo><mi>&#x1D4A2;</mi><mo>)</mo></mrow></mrow></math></span>. Then the pullback of <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>&#x2112;</mi></math></span> to <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mrow><msubsup><mrow><mi>&#x2133;</mi></mrow> <mi>&#x02207;</mi> <mn>0</mn> </msubsup><mrow><mo>(</mo><mi>&#x1D4A2;</mi><mo>)</mo></mrow></mrow></math></span> has a connection <span><math xmlns='http://www.w3.org/1998/Math/MathML'><mi>&#x02207;</mi></math></span>. Its curvature can be described explicitly.</p> <p>The final part V discusses parabolic structures in the sense of C. Seshadri. The parabolic analogue of a Higgs bundle is introduced and a theory parallel to the one in the foregoing parts is sketched.</p>
      <div class="right">Reviewer: <a class="meta" href="search/?q=rv:W.W.J.Hulsbergen">W.W.J.Hulsbergen (Breda)</a></div>
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    <strong>MSC 2010</strong>
    <dl class="msc">
      <dt><a class="meta" href="search/?q=cc:14H10">14H10</a></dt>
      <dd>Families, algebraic moduli (curves)</dd>
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      <dt><a class="meta" href="search/?q=cc:14H60">14H60</a></dt>
      <dd>Vector bundles on curves and their moduli</dd>
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      <dd>Sheaves, derived categories of sheaves, etc.</dd>
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      <strong>Keywords</strong>
    </div>
    <div>
      <a class="meta" href="search/?q=ut:%22torsor%22">torsor</a>;      <a class="meta" href="search/?q=ut:%22moduli%20space%20of%20Higgs%20bundle%22">moduli space of Higgs bundle</a>;      <a class="meta" href="search/?q=ut:%22determinant%20of%20the%20cohomology%20of%20coherent%20sheaves%20on%20a%20curve%22">determinant of the cohomology of coherent sheaves on a curve</a>;      <a class="meta" href="search/?q=ut:%22theorem%20of%20the%20cube%22">theorem of the cube</a>;      <a class="meta" href="search/?q=ut:%22characteristic%20variety%22">characteristic variety</a>;      <a class="meta" href="search/?q=ut:%22theta%20functions%22">theta-functions</a>;      <a class="meta" href="search/?q=ut:%22semistable%20pairs%22">semistable pairs</a>;      <a class="meta" href="search/?q=ut:%22moduli%20stack%22">moduli stack</a>;      <a class="meta" href="search/?q=ut:%22abelianisation%22">abelianisation</a>;      <a class="meta" href="search/?q=ut:%22connection%22">connection</a>    </div>
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    <strong>Cited in 16 reviews</strong>
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    <a href="search/?q=an:1239.14009">Zbl 1239.14009</a>;     <a href="search/?q=an:1211.14038">Zbl 1211.14038</a>;     <a href="search/?q=an:1156.14026">Zbl 1156.14026</a>;     <a href="search/?q=an:1119.14032">Zbl 1119.14032</a>;     <a href="search/?q=an:1056.14047">Zbl 1056.14047</a>;     <a href="search/?q=an:1074.14022">Zbl 1074.14022</a>;     <a href="search/?q=an:1058.14018">Zbl 1058.14018</a>;     <a href="search/?q=an:1099.14502">Zbl 1099.14502</a>;     <a href="search/?q=an:1048.14016">Zbl 1048.14016</a>;     <a href="search/?q=an:1116.14007">Zbl 1116.14007</a>;     <a href="search/?q=an:0983.14028">Zbl 0983.14028</a>;     <a href="search/?q=an:0909.14018">Zbl 0909.14018</a>;     <a href="search/?q=an:0915.14007">Zbl 0915.14007</a>;     <a href="search/?q=an:0948.14006">Zbl 0948.14006</a>;     <a href="search/?q=an:0890.14017">Zbl 0890.14017</a>;     <a href="search/?q=an:0809.14009">Zbl 0809.14009</a>    </div>
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