in terms of their electronic structure 601 .5.6 Matter at Extreme ConditionsA strong advantage of ab <strong>initio</strong> simulations is their predictive power also at extremeconditions, an area where <strong>molecular</strong> <strong>dynamics</strong> relying on fitted potentialmodels might encounter severe difficulties. Thus, high pressures <strong>and</strong> / or high temperaturessuch as those in the earth’s core, on other planets, or on stars can beeasily achieved in the virtual laboratory. This opens up the possibility to studyphase transformations <strong>and</strong> chemical reactions at such conditions 56 . Furthermore,conditions of geophysical <strong>and</strong> astrophysical interest can nowadays be produced inthe real laboratory, using techniques based on diamond anvil cells, shock waves, orlasers. The limitations of these experimental approaches are, however, not so muchrelated to generating the extreme conditions as one might expect, but rather tomeasuring observables.In the virtual laboratory this information is accessible <strong>and</strong> the melting ofdiamond at high pressure 222 , the phase transformation from the antiferromagneticinsulating δ–O 2 phase to a nonmagnetic metallic <strong>molecular</strong> ζ–O 2 phase 557 ,the phase diagram of carbon at high pressures <strong>and</strong> temperatures 261 as well astransformations of methane 13 , carbon monoxide 54 , <strong>molecular</strong> CO 2 267,558 , waterice 363,364,58,50,51,52 , solid 305,337,65,66,333 <strong>and</strong> hot fluid 5 hydrogen, solid Ar(H 2 ) 253under pressure could be probed. Along similar lines properties of a liquid Fe–S mixtureunder earth’s core conditions 11 , the viscosity of liquid iron 690,592 , the soundvelocity of dense hydrogen at conditions on jupiter 6 , the phase diagram of water<strong>and</strong> ammonia up to 7000 K <strong>and</strong> 300 GPa 118 , the laser heating of silicon 570,572<strong>and</strong> graphite 574 etc. were investigated at extreme state points. A review on ab<strong>initio</strong> simulations relevant to minerals at conditions found in the earth’s mantle isprovided in Ref. 683 .5.7 Clusters, Fullerenes, <strong>and</strong> NanotubesInvestigations of clusters by ab <strong>initio</strong> <strong>molecular</strong> <strong>dynamics</strong> were among the firstapplications of this technique. Here, the feasibility to conduct finite–temperaturesimulations <strong>and</strong> in particular the possibility to search globally for minima turnedout to be instrumental 302,31,303,550,517,519 , see e.g. Refs. 16,321,32 for reviews.Such investigations focus more <strong>and</strong> more on clusters with varying composition518,293,199,348,349,161 . Cluster melting is also accessible on an ab <strong>initio</strong> footing84,531,525,526 <strong>and</strong> <strong>molecular</strong> clusters, complexes or cluster aggregates are activelyinvestigated 612,645,613,70,596,597,133,701,524 .Iii–v semiconductor clusters embedded in sodalite show quantum confinement<strong>and</strong> size effects that can be rationalized by ab <strong>initio</strong> simulations 625,95 . Supportedclusters such as Cu n on an MgO(100) surface are found to diffuse by “rolling” <strong>and</strong>“twisting” motions with very small barriers 438 . The diffusion of protonated heliumclusters in various sodalite cages was generated using ab <strong>initio</strong> <strong>dynamics</strong> 198 . Photo–induced structural changes in Se chains <strong>and</strong> rings were generated by a verticalhomo → lumo excitation <strong>and</strong> monitored by ab <strong>initio</strong> <strong>dynamics</strong> 306 . With thediscovery <strong>and</strong> production of finite carbon assemblies ab <strong>initio</strong> investigations of the123
properties of fullerenes 19,17,451 , the growth process of nanotubes 127,62,72 , or theelectrical conductivity of nanowires 38,272 became of great interest.5.8 Complex <strong>and</strong> Floppy MoleculesThe determination of the structure of a RNA duplex including its hydration water311 , investigations of geometry <strong>and</strong> electronic structure of porphyrins <strong>and</strong> porphyrazines356 , <strong>and</strong> the simulation of a bacteriochlorophyll crystal 381 are someapplications to large molecules. Similarly, the “carboplatin” complex 623 – a drugwith large lig<strong>and</strong>s – as well as the organometallic complex Alq(3) 148 – an electroluminescentmaterial used in organic light–emitting diodes – were investigated withrespect to structural, dynamical <strong>and</strong> electronic properties.The organometallic compound C 2 H 2 Li 2 has an unexpected ground–state structurethat was found by careful ab <strong>initio</strong> simulated annealing 521 . In addition, thiscomplex shows at high temperatures intra<strong>molecular</strong> hydrogen migration that ismediated via a lithium hydride unit 521 . Ground–state fluxionality of protonatedmethane CH + 5 397,408 including some isotopomers 409 <strong>and</strong> of protonated acetyleneC 2 H + 3 400 was shown to be driven by quantum effects. The related dynamicalexchange of atoms in these molecules can also be excited by thermal fluctuations630,85,401 . In addition it was shown that CH + 5 is three–center two–electronbonded <strong>and</strong> that this bonding topology does not qualitatively change in the presenceof strong quantum motion 402 . The fluxional behavior of the protonated ethane<strong>molecular</strong> ion C 2 H + 7 was investigated by ab <strong>initio</strong> <strong>molecular</strong> <strong>dynamics</strong> as well 172 .The neutral <strong>and</strong> ionized SiH 5 <strong>and</strong> Si 2 H 3 species display a rich dynamical behaviorwhich was seen during ab <strong>initio</strong> <strong>molecular</strong> <strong>dynamics</strong> simulations 246 . Thelithium pentamer Li 5 was found to perform pseudorotational motion on a timescale of picoseconds or faster at temperatures as low as 77 K 231 . Using ab <strong>initio</strong>instanton <strong>dynamics</strong> the inversion splitting of the NH 3 , ND 3 , <strong>and</strong> PH 3 moleculesdue to the umbrella mode was estimated 325 . Similarly, a semiclassical ab <strong>initio</strong><strong>dynamics</strong> approach as used to compute the tunneling rate for intra<strong>molecular</strong> protontransfer in malonaldehyde 47 . <strong>Ab</strong> <strong>initio</strong> simulated annealing can be used toexplore the potential energy l<strong>and</strong>scape <strong>and</strong> to locate various minima, such as forinstance done for protonated water clusters 673 . Molecular <strong>dynamics</strong> simulations ofthe trimethylaluminum Al(CH 3 ) 3 have been carried out in order to investigate theproperties of the gas–phase dimer 29 . The structures <strong>and</strong> vibrational frequenciesof tetrathiafulvalene in different oxidation states was probed by ab <strong>initio</strong> <strong>molecular</strong><strong>dynamics</strong> 324 . Implanted muons in organic molecules (benzene, 3–quinolylnitronyl nitroxide, para–pyridyl nitronyl nitroxide, phenyl nitronyl nitroxide <strong>and</strong>para–nitrophenyl nitronyl nitroxide) were investigated using approximate ab <strong>initio</strong>path integral simulations that include the strong quantum broadening of themuonium 656,657 .5.9 Chemical Reactions <strong>and</strong> TransformationsEarly applications of ab <strong>initio</strong> <strong>molecular</strong> <strong>dynamics</strong> were devoted to reactive scatteringin the gas phase such as CH 2 + H 2 → CH 4 669 or H − + CH 4 → CH 4 +H − 365 . The “on–the–fly” approach can be compared to classical trajectory cal-124
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John von Neumann Institute for Comp
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2500Number200015001000CP PRL 1985AI
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The goal of this section is to deri
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¡the Newtonian equation of motion
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Ehrenfest molecular dynamics is cer
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the Car-Parrinello approach 108 , s
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Figure 4. (a) Comparison of the x-c
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parameters are those used to repres
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in terms of a linear combination of
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structure calculations, see e.g. Re
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“unbound electrons” dissolved i
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Table 1. Timings in cpu seconds and
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stressed that the energy conservati
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see e.g. the discussion following E
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from a set of one-particle spin orb
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is used, which represents exactly a
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2.8.3 Generalized Plane WavesAn ext
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disposable parameters that can be o
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The index i runs over all states an
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f(G) are related by three-dimension
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where j l are spherical Bessel func
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andE self = ∑ I1√2πZ 2 IR c I.
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¢££¤¤¢¢¢n tot (G)inv FTn to
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correlation energyΩ ∑E xc = ε x
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The local part of the pseudopotenti
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¢¢¢¢¢i = 1 . . .N b¢c i (G)¢
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¢¢¢¢¢c i (G)123g, E self∆V I
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where G c is a free parameter that
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The two sets of equations are coupl
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- Page 142 and 143: 442. S. Nosé and M. L. Klein, Mol.
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- Page 146 and 147: 562. F. Shimojo, K. Hoshino, and Y.
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