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81

13 Eliashberg Theory Giovanni A.C. Ummarino Departement of Applied Science and Technology Politecnico di Torino, 10129 Turin, Italy Contents

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Source URL: www.cond-mat.de

- Date: 2013-09-03 06:05:14
    82

    Hedin Equations, GW, GW+DMFT, and All That

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    Source URL: www.cond-mat.de

    - Date: 2014-05-26 12:52:53
      83

      http://www.swissinfo.ch/ita/norma-antirazzismo_razzismo-da-cond

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      Source URL: bunte-schweiz.ch

      - Date: 2016-05-29 15:12:28
        84

        Appendix 1. How to work with the CO2 data from the SchoolCO2web 1. How to download the CO2 data Within the SchoolCO2web a tool has been developed to download or graphically display the CO2-concentrations and weather cond

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        Source URL: www.carboeurope.org

        - Date: 2015-11-05 04:59:56
          85

          The Hubbard Model and its Properties

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          Source URL: www.cond-mat.de

          - Date: 2015-09-07 08:29:41
            86

            Nuclear Magnetic Resonance in a Ferromagnet-Semiconductor Heterostructure J. Strand,1 B. D. Schultz,2 A. F. Isakovic,1 X. Lou,1 C. J. Palmstrøm,2 and P. A. Crowell1, ∗ arXiv:cond-matv1 21 Jul

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            Source URL: groups.physics.umn.edu

            - Date: 2011-07-06 22:41:14
              87

              2 Density Functional Theory and Applications to Transition Metal Oxides David J. Singh Oak Ridge National Laboratory

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              Source URL: www.cond-mat.de

              - Date: 2012-08-20 13:43:11
                88

                Spectroscopic Properties of Mixed-Valence Compounds in the Impurity Model

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                Source URL: www.cond-mat.de

                - Date: 2015-09-16 08:20:33
                  89

                  BUS 702  Cochemer Stadtverkehr Cochem Cond

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                  Source URL: www.vrminfo.de

                  - Date: 2016-08-02 04:31:06
                    90

                    The Dynamic Cluster Approximation and its DCA+ Extension

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                    Source URL: www.cond-mat.de

                    - Date: 2015-09-07 08:29:40
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