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title  ="Predicting crystal structures of organic compounds",
journal  ="Chem. Soc. Rev.",
year  ="2014",
volume  ="43",
issue  ="7",
pages  ="2098-2111",
publisher  ="The Royal Society of Chemistry",
doi  ="10.1039/C3CS60279F",
url  ="http://dx.doi.org/10.1039/C3CS60279F",
abstract  ="Currently{,} organic crystal structure prediction (CSP) methods are based on searching for the most thermodynamically stable crystal structure{,} making various approximations in evaluating the crystal energy. The most stable (global minimum) structure provides a prediction of an experimental crystal structure. However{,} depending on the specific molecule{,} there may be other structures which are very close in energy. In this case{,} the other structures on the crystal energy landscape may be polymorphs{,} components of static or dynamic disorder in observed structures{,} or there may be no route to nucleating and growing these structures. A major reason for performing CSP studies is as a complement to solid form screening to see which alternative packings to the known polymorphs are thermodynamically feasible."}

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@article{TANGLEDTALE,
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@article{CHAOSAT50,
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  year    = 2013,
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@techreport{CHAOSFORJAVA,
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@techreport{ADVLABCHAOS,
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@techreport{AMERICIUM-241,
  title        = {Americium-241},
  institution  = {University of Cincinnati},
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@unpublished{unpublished,
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@ONLINE{Doe:2009:Online,
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@manual{ORTEC:Alpha:Exp4,
  title        = {Alpha Spectroscopy with Silicon Charged-Particle Detectors},
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  organization = {ORTEC},
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  %edition      = ,
  %month        = ,
  %year         = ,
  note         = {Instruction Manual}
}

@manual{ORTEC:Alpha:Exp5,
  title        = {Energy Loss with Heavy Charged Particles},
  author       = {}, 
  organization = {ORTEC},
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  %edition      = ,
  %month        = ,
  %year         = ,
  note         = {Instruction Manual}
}

@ONLINE{EngToolbox:AirDensity,
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}

@misc{larsen2004thorium,
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}












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@ARTICLE{2010MNRAS.409..619K,
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