

@article{Kelbg:Annalen:1963,
  author =        {Kelbg, G.},
  journal =       {Annalen der Physik},
  number =        {3-4},
  pages =         {219-224},
  title =         {Theorie des Quanten-Plasmas},
  volume =        {467},
  year =          {1963},
  abstract =      {Abstract Es wird die quantenstatistische
                   Zustandssumme eines N-Teilchensystems im Falle
                   weitreichender zwischenmolekularer Wechselwirkungen
                   berechnet. Das Verfahren ist anwendbar, wenn die
                   Potentiale Fourier-Transformierte besitzen. Durch
                   Einführung effektiver Potentiale, die von der
                   Temperatur und dem Planckschen Wirkungsquantum
                   abhängen, wird es möglich, bekannte klassische
                   Gleichungen heranzuziehen und Formeln für die freie
                   Energie und die radiale Verteilungsfunktion
                   aufzustellen. Im Falle eines Plasmas tritt an die
                   Stelle des Coulomb-Potentials eine in der Nähe des
                   Nullpunktes davon abweichende nichtsinguläre
                   Potentialfunktion, deren Betrag im Nullpunkt durch
                   den reziproken Wert der thermischen Wellenlänge
                   bestimmt wird.},
  doiurl =        {https://doi.org/10.1002/andp.19634670308},
}

@article{Filinov:PRE:2004,
  author =        {Filinov, A. V. and Golubnychiy, V. O. and Bonitz, M. and
                   Ebeling, W. and Dufty, J. W.},
  journal =       {Phys. Rev. E},
  month =         {Oct},
  number =        {4},
  pages =         {046411},
  publisher =     {American Physical Society},
  title =         {Temperature-dependent quantum pair potentials and
                   their application to dense partially ionized hydrogen
                   plasmas},
  volume =        {70},
  year =          {2004},
  doiurl =        {10.1103/PhysRevE.70.046411},
  url =           {https://link.aps.org/doi/10.1103/PhysRevE.70.046411},
}

@article{Filinov:IOP:2001,
  author =        {V S Filinov and M Bonitz and W Ebeling and
                   V E Fortov},
  journal =       {Plasma Physics and Controlled Fusion},
  month =         {may},
  number =        {6},
  pages =         {743--759},
  publisher =     {{IOP} Publishing},
  title =         {Thermodynamics of hot dense H-plasmas: path integral
                   Monte Carlo simulations and analytical
                   approximations},
  volume =        {43},
  year =          {2001},
  abstract =      {This work is devoted to the thermodynamics of
                   high-temperature dense hydrogen plasmas in the
                   pressure region between 10-1 and 102 Mbar. In
                   particular, we present for this region results of
                   extensive calculations based on a recently developed
                   path integral Monte Carlo scheme (direct PIMC). This
                   method allows for a correct treatment of the
                   thermodynamic properties of hot dense Coulomb
                   systems. Calculations were performed in a broad
                   region of the non-ideality parameter Γ≲3 and
                   degeneracy parameter neΛ3≲10. We give a comparison
                   with a few available results from other path integral
                   calculations (restricted PIMC) and with analytical
                   calculations based on Padé approximations for
                   strongly ionized plasmas. Good agreement between the
                   results obtained from the three independent methods
                   is found.},
  doiurl =        {10.1088/0741-3335/43/6/301},
  url =           {https://doi.org/10.1088/0741-3335/43/6/301},
}

@article{Fraser:PRB:1996,
  author =        {Fraser, Louisa M. and Foulkes, W. M. C. and
                   Rajagopal, G. and Needs, R. J. and Kenny, S. D. and
                   Williamson, A. J.},
  journal =       {Phys. Rev. B},
  month =         {Jan},
  number =        {4},
  pages =         {1814--1832},
  publisher =     {American Physical Society},
  title =         {Finite-size effects and Coulomb interactions in
                   quantum Monte Carlo calculations for homogeneous
                   systems with periodic boundary conditions},
  volume =        {53},
  year =          {1996},
  doiurl =        {10.1103/PhysRevB.53.1814},
  url =           {https://link.aps.org/doi/10.1103/PhysRevB.53.1814},
}

@article{DORNHEIM:PhysRep:2018,
  author =        {Tobias Dornheim and Simon Groth and Michael Bonitz},
  journal =       {Physics Reports},
  pages =         {1-86},
  title =         {The uniform electron gas at warm dense matter
                   conditions},
  volume =        {744},
  year =          {2018},
  abstract =      {Motivated by the current high interest in the field
                   of warm dense matter research, in this article we
                   review the uniform electron gas (UEG) at finite
                   temperature and over a broad density range relevant
                   for warm dense matter applications. We provide an
                   exhaustive overview of different simulation
                   techniques, focusing on recent developments in the
                   dielectric formalism (linear response theory) and
                   quantum Monte Carlo (QMC) methods. Our primary focus
                   is on two novel QMC methods that have recently
                   allowed us to achieve breakthroughs in the
                   thermodynamics of the warm dense electron gas:
                   Permutation blocking path integral MC (PB-PIMC) and
                   configuration path integral MC (CPIMC). In fact, a
                   combination of PB-PIMC and CPIMC has allowed for a
                   highly accurate description of the warm dense UEG
                   over a broad density–temperature range. We are able
                   to effectively avoid the notorious fermion sign
                   problem, without invoking uncontrolled approximations
                   such as the fixed node approximation. Furthermore, a
                   new finite-size correction scheme is presented that
                   makes it possible to treat the UEG in the
                   thermodynamic limit without loss of accuracy. In
                   addition, we in detail discuss the construction of a
                   parametrization of the exchange–correlation free
                   energy, on the basis of these data — the central
                   thermodynamic quantity that provides a complete
                   description of the UEG and is of crucial importance
                   as input for the simulation of real warm dense matter
                   applications, e.g., via thermal density functional
                   theory. A second major aspect of this review is the
                   use of our ab initio simulation results to test
                   previous theories, including restricted PIMC,
                   finite-temperature Green functions, the classical
                   mapping by Perrot and Dharma-wardana, and various
                   dielectric methods such as the random phase
                   approximation, or the
                   Singwi–Tosi–Land–Sjölander (both in the static
                   and quantum versions), Vashishta–Singwi and the
                   recent Tanaka scheme for the local field correction.
                   Thus, for the first time, thorough benchmarks of the
                   accuracy of important approximation schemes regarding
                   various quantities such as different energies, in
                   particular the exchange–correlation free energy,
                   and the static structure factor, are possible. In the
                   final part of this paper, we outline a way how to
                   rigorously extend our QMC studies to the
                   inhomogeneous electron gas. We present first ab
                   initio data for the static density response and for
                   the static local field correction.},
  doiurl =        {https://doi.org/10.1016/j.physrep.2018.04.001},
  issn =          {0370-1573},
  url =           {https://www.sciencedirect.com/science/article/pii/
                  S0370157318300516},
}

@misc{Mathematica,
  author =        {Wolfram Research{,} Inc.},
  note =          {Champaign, IL, 2021},
  title =         {Mathematica, {V}ersion 12.3.1},
}

@book{Feynman:1972:SMS,
  address =       {},
  author =        {Richard P. Feynman},
  note =          {Notes taken by R. Kikuchi and H. A. Feiveson. Edited
                   by Jacob Shaham},
  pages =         {xii + 354},
  publisher =     {},
  series =        {Frontiers in physics},
  title =         {Statistical mechanics: a set of lectures by {R. P.
                   Feynman}},
  year =          {1972},
  isbn =          {0-8053-2508-5, 0-8053-2509-3 (paperback)},
}

@book{Kleinert:book:2009,
  author =        {Kleinert, Hagen},
  publisher =     {World scientific},
  title =         {Path integrals in quantum mechanics, statistics,
                   polymer physics, and financial markets},
  year =          {2009},
}


