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@ARTICLE{einstein05,
  author = {Albert Einstein},
  title = {{Zur Elektrodynamik bewegter Körper}},
  journal = {Annalen der Physik},
  year = {1905},
  volume = {322},
  pages = {891--921},
  number = {10},
  doi = {10.1002/andp.19053221004}
}

@ARTICLE{Einstein1905,
  author = {Einstein, Albert},
  title = {The photoelectric effect},
  journal = {Ann. Phys},
  year = {1905},
  volume = {17},
  pages = {4},
  number = {132},
  url= {http://hexagon.physics.wisc.edu/teaching/2015f ph545 atomic structure/papers/einstein photoelectric 1905.pdf}
}

@ARTICLE{EinsteinRosen1936,
  author = {Einstein, Albert and Rosen, Nathan},
  title = {Two-body problem in general relativity theory},
  journal = {Physical Review},
  year = {1936},
  volume = {49},
  pages = {404},
  number = {5},
  publisher = {APS},
  doi = {10.1103/PhysRev.49.404.2},
  abstract= {The writers investigate the possibility of an atomistic theory of matter and electricity which, while excluding singularities of the field, makes use of no other variables than the gμν of the general relativity theory and the ϕμ of the Maxwell theory. By the consideration of a simple example they are led to modify slightly the gravitational equations which then admit regular solutions for the static spherically symmetric case. These solutions involve the mathematical representation of physical space by a space of two identical sheets, a particle being represented by a "bridge" connecting these sheets. One is able to understand why no neutral particles of negative mass are to be found. The combined system of gravitational and electromagnetic equations are treated similarly and lead to a similar interpretation. The most natural elementary charged particle is found to be one of zero mass. The many-particle system is expected to be represented by a regular solution of the field equations corresponding to a space of two identical sheets joined by many bridges. In this case, because of the absence of singularities, the field equations determine both the field and the motion of the particles. The many-particle problem, which would decide the value of the theory, has not yet been treated.}
}

@ARTICLE{einstein1935particle,
  author = {Einstein, Albert and Rosen, Nathan},
  title = {The particle problem in the general theory of relativity},
  journal = {Physical Review},
  year = {1935},
  volume = {48},
  pages = {73},
  number = {1},
  publisher = {APS},
  href = {10.1103/PhysRev.48.73}
}

@article{einstein_can_1935,
    title = {Can {Quantum}-{Mechanical} {Description} of {Physical} {Reality} {Be} {Considered} {Complete}?},
    volume = {47},
    url = {https://link.aps.org/doi/10.1103/PhysRev.47.777},
    doi = {10.1103/PhysRev.47.777},
    abstract = {In a complete theory there is an element corresponding to each element of reality. A sufficient condition for the reality of a physical quantity is the possibility of predicting it with certainty, without disturbing the system. In quantum mechanics in the case of two physical quantities described by non-commuting operators, the knowledge of one precludes the knowledge of the other. Then either (1) the description of reality given by the wave function in quantum mechanics is not complete or (2) these two quantities cannot have simultaneous reality. Consideration of the problem of making predictions concerning a system on the basis of measurements made on another system that had previously interacted with it leads to the result that if (1) is false then (2) is also false. One is thus led to conclude that the description of reality as given by a wave function is not complete.},
    number = {10},
    urldate = {2018-03-05},
    journal = {Phys. Rev.},
    author = {Einstein, A. and Podolsky, B. and Rosen, N.},
    month = may,
    year = {1935},
    pages = {777--780},
}
