
 [312]

S. Ejima, F. H. Essler, F. Lange and H. Fehske
Phys. Rev. B 93, 235118 (2016)
Ising tricriticality in the extended Hubbard model with bond dimerization
highlighted as Editors' Suggestion
 [311]

M. Chakraborty, N. Mohanta, A. Taraphder, B. I. Min and H. Fehske
Phys. Rev. B 93, 155130 (2016)
Edwards polaron formation: From one to three dimensions
 [310]

C. Schulz, L. Bakemeier, A. Alvermann and H. Fehske
Europhys. Lett. 113, 64002 (2016)
Optomechanical multistability in the quantum regime
 [309]

E. Thiessen, R. L. Heinisch, F. X. Bronold and H. Fehske
Phys. Rev. A 93, 033827 (2016)
Surface mode hybridization in the optical response of coreshell particles
 [308]

D.N. Cho, J. v. Brink, H. Fehske, K. W. Becker and S. Sykora
Scientific Reports 6, 22548 (2016)
Unconventional superconductivity and interaction induced Fermi surface reconstruction in the twodimensional Edwards model
 [307]

VanNham Phan, K. W. Becker and H. Fehske
Phys. Rev. B 93, 075138 (2016)
Groundstate and spectral signatures of cavity excitonpolariton condensates
 [306]

A. Pieper and H. Fehske
Phys. Rev. B 93, 035123 (2016)
Topological insulators in random potentials
 [305]

M. RöhrigZöllner, J. Thies, M. Kreutzer, A. Alvermann, A. Pieper,
A. Basermann, G. Hager, G. Wellein, and
H. Fehske
SIAM Journal on Scientific Computing 37, C697C722 (2015)
Increasing the performance of the JacobiDavidson method by blocking
 [304]

M. Kreutzer, G. Hager, G. Wellein, A. Pieper, A. Alvermann, and H. Fehske
IEEE IPDPS15, 417426 (2015)
Performance Engineering of the Kernel Polynomial Method on LargeScale CPUGPU Systems
 [303]

F. X. Bronold and H. Fehske
Phys. Rev. Lett. 115, 225001 (2015)
Absorption of an electron by a dielectric wall
 [302]

M. Pamperin, F. X. Bronold and H. Fehske
Phys. Scr. T 165, 014008 (2015)
Mixedvalence correlations in chargetransferring atomsurface collisions
 [301]

L. Bakemeier, A. Alvermann and H. Fehske
Phys. Scr. T 165, 014001 (2015)
Variational treatment of entanglement in the Dicke model
 [300]

T. Kaneko, B. Zenker, H. Fehske and Y. Ohta
Phys. Rev. B 92, 115106 (2015)
Competition between excitonic charge and spin density waves: Influence of electronphonon and Hund's rule couplings
 [299]

D. Pagel and H. Fehske
Phys. Rev. A 92, 022342 (2015)
Entangled light from driven dissipative microcavities
 [298]

B. Zenker, H. Fehske and H. Beck
Phys. Rev. B 92, 081111(R) (2015)
Excitonic Josephson effect in doublelayer graphene junctions
 [297]

H. Fehske, G. Hager and A. Pieper
physica status solidi (b) 252, 1868 (2015)
Electron confinement in graphene with gatedefined quantum dots
 [296]

F. Lange, S. Ejima and H. Fehske
Phys. Rev. B 92, 041120(R) (2015)
Criticality at the Haldaneinsulator chargedensitywave quantum phase transition
 [295]

C. Schulz, R. L. Heinisch and H. Fehske
Quantum Matter 4, 346351 (2015)
Electron flow in circular graphene quantum dots
 [294]

E. Thiessen, F. X. Bronold, R. L. Heinisch and H. Fehske
Phys. Rev. A 91, 043837 (2015)
Scattering of infrared light by dielectric coreshell particles
 [293]

D. Pagel, A. Alvermann and H. Fehske
Phys. Rev. A 91, 043814 (2015)
Nonclassical light from few emitters in a cavity
 [292]

S. Ejima and H. Fehske
Proc. Int. Conf. Strongly Correlated Electron Systems,
Journal of Physics: Conference Series 592, 012134 (2015)
Entanglement properties of the nontrivial Haldane insulator in the 1D extended BoseHubbard model
 [291]

M. Pamperin, F. X. Bronold and H. Fehske
Phys. Rev. B 91, 035440 (2015)
Manybody theory of the neutralisation of strontium ions on gold surfaces
 [290]

C. Schulz, R. L. Heinisch, and H. Fehske
Phys. Rev. B 91, 045130 (2015)
Scattering of twodimensional Dirac fermions on gatedefined oscillating quantum dots
 [289]

S. Ejima and H. Fehske
Phys. Rev. B 91, 045121 (2015)
Comparative DMRG study of symmetryprotected topological phases in spin1 chain and BoseHubbard models
 [288]

L. Bakemeier, A. Alvermann and H. Fehske
Phys. Rev. Lett. 114, 013601 (2015)
Route to chaos in optomechanics
 [287]

M. Galgon, L. Krämer, B. Lang, A. Alvermann, H. Fehske and A. Pieper
Proceedings in Applied Mathematics and Mechanics (PAMM) 14, 821 (2014)
Improving robustness of the FEAST algorithm and solving eigenvalue problems from graphene nanoribbons
 [286]

A. Alvermann, A. Basermann, H. Fehske, Martin Galgon, G. Hager, M. Kreutzer, L. Krämer, B. Lang, A. Pieper, M. RöhrigZöllner, F. Shahzad, J. Thies and G. Wellein,
in EuroPar 2014: Parallel Processing Workshops,
L. Lopes et al. (Eds.),
LNCS vol. 8806, 577588, ISBN 9783319143125, Springer (2014)
ESSEX: Equipping Sparse Solvers for Exascale
 [285]

B. Zenker, H. Fehske and H. Beck
Phys. Rev. B 90, 195118 (2014)
Fate of the excitonic insulator in the presence of phonons
 [284]

M. Kreutzer, G. Hager, G. Wellein, H. Fehske and A. R. Bishop
SIAM J. Sci. Comput. 36(5), C401C423 (2014)
A unified sparse matrix data format for efficient general sparse matrixvector multiply on modern processors with wide SIMD units
 [283]

B. Zenker, D. Ihle, F. X. Bronold and H. Fehske
Journal of Physics: Conference Series 529, 012030 (2014)
Exciton formation in strongly correlated electronhole systems near the semimetalsemiconductor transition
 [282]

T. Kaneko, S. Ejima, H. Fehske and Y. Ohta
Proc. Int. Conf. Strongly Correlated Electron Systems,
JPS Conf. Proc. 3, 017006 (2014)
Excitonic BCSBEC crossover in doublelayer systems
 [281]

S. Ejima and H. Fehske
Proc. Int. Conf. Strongly Correlated Electron Systems,
JPS Conf. Proc. 3, 013006 (2014)
Chargedensitywave formation in the Edwards fermionboson model at onethird
band filling
 [280]

S. Ejima, F. Lange and H. Fehske
Phys. Rev. Lett. 113, 020401 (2014)
Spectral and entanglement properties of the bosonic Haldane insulator
 [279]

K. zu Münster, F. Gebhard, S. Ejima and H. Fehske
Phys. Rev. A 89, 063623 (2014)
Dynamical correlation functions for the onedimensional BoseHubbard insulator
 [278]

R. Heinisch, F. X. Bronold and H. Fehske,
in Complex Plasmas: Scientific Challenges and Technological Opportunities,
Eds. M. Bonitz, K. Becker, J. Lopez and H. Thomsen,
Springer Series on Atomic, Optical, and Plasma Physics
82, pp. 267298, SpringerVerlag Berlin Heidelberg (2014)
Surface electrons at plasma walls
 [277]

E. Thiessen, R. L. Heinisch, F. X. Bronold and H. Fehske
Eur. Phys. Jour. D 68, 98 (2014)
Infrared light extinction by charged dielectric corecoat particles
 [276]

T. Koch, J. Loos and H. Fehske
Phys. Rev. B 89, 155133 (2014)
Thermoelectric effects in molecular quantum dots with contacts
 [275]

A. Pieper, R. L. Heinisch, G. Wellein and H. Fehske
Phys. Rev. B 89, 165121 (2014)
Dotbound and dispersive states in graphene quantum dot superlattices
 [274]

V.N. Phan, H. Fehske and K. W. Becker
Eur. Phys. Jour. B 87, 66 (2014)
Linear response within the projectionbased renormalization method: Manybody corrections beyond the random phase approximation
 [273]

S. Ejima, T. Kaneko, Y. Ohta and H. Fehske
Phys. Rev. Lett. 112, 026401 (2014)
Order, criticality, and excitations in the extended FalicovKimball model
 [272]

A. Pieper, R. L. Heinisch and H. Fehske,
Europhys. Lett. 104, 47010 (2013)
Electron dynamics in graphene with gatedefined quantum dots
 [271]

S. Ejima, F. Lange, H. Fehske, F. Gebhard and K. zu Münster,
Phys. Rev. A 88, 063625 (2013)
Onedimensional BoseHubbard model with local threebody interactions
 [270]

A. Pieper, G. Schubert, G. Wellein and H. Fehske,
Phys. Rev. B 88, 195409 (2013)
Effects of disorder and contacts on transport through graphene nanoribbons
 [269]

V. N. Phan, K. W. Becker and H. Fehske,
Phys. Rev. B 88, 205123 (2013)
Exciton condensation due to electronphonon interaction
 [268]

L. Bakemeier, A. Alvermann and H. Fehske,
Phys. Rev. A 88, 043835 (2013)
Dynamics of the Dicke model close to the classical limit
 [267]

D. Pagel, H. Fehske, J. Sperling and W. Vogel,
Phys. Rev. A 88, 042310 (2013)
Multipartite entangled light from driven microcavities
 [266]

D. Pagel, P. Nalbach, A. Alvermann, H. Fehske and M. Thorwart,
New. J. Phys 15, 105008 (2013)
Nonequilibrium quantum fluctuation relations for harmonic systems in nonthermal environments
 [265]

R. Heinisch, F. X. Bronold and H. Fehske,
Phys. Rev. E 88, 023109 (2013)
Optical signatures of the charge of a dielectric particle in a plasma
 [264]

B. Zenker, H. Fehske, H. Beck, C. Monney and A. R. Bishop,
Phys. Rev. B 88, 075138 (2013)
Chiral charge order in 1TTiSe_{2}: importance of lattice degrees of freedom
 [263]

T. Kaneko, S. Ejima, H. Fehske and Y. Ohta
Phys. Rev. B 88, 035312 (2013)
Exactdiagonalization study of exciton condensation in electron bilayers
 [262]

D. Bauer, T. Brabec, H. Fehske, S. Lochbrunner, K.H. MeiwesBroer and R. Redmer
New. J. Phys. 15, 065015 (2013)
Editorial: Focus on correlation effects in radiation fields
 [261]

R. Heinisch, F. X. Bronold and H. Fehske
Phys. Rev. B 87, 155409 (2013)
Mie scattering analog in graphene: lensing, particle confinement, and depletion of Klein tunneling
 [260]

D. Pagel, A. Alvermann and H. Fehske
Phys. Rev. E 87, 012127 (2013)
Equilibration and thermalization of the quantum dissipative oscillator in a nonthermal environment
 [259]

S. Nishimoto, S. Ejima and H. Fehske
Phys. Rev. B 87, 045116 (2013)
Anderson localization versus chargedensitywave formation in disordered electron systems
 [258]

F. X. Bronold and H. Fehske,
in Nonthermal plasma chemistry and physics, Eds. M. Schmidt, J. Meichsner, R. Schneider, and H.E. Wagner, CRC Press, Taylor & Francis Group, Boca Raton (2013), Section 9.2,
pp. 427452
Elementary volume processes in gas discharges
 [257]

H. Fehske, S. Ejima, G. Wellein and A. R. Bishop
J. Phys.: Conf. Ser. 391, 012152 (2012)
Metalinsulator transition in the Edwards model
 [256]

S. Ejima, H. Fehske and F. Gebhard
J. Phys.: Conf. Ser. 391, 012143 (2012)
Dynamic densitydensity correlations in interacting Bose gases on optical lattices
 [255]

R. Heinisch, F. X. Bronold and H. Fehske
Phys. Rev. Lett. 109, 243903 (2012)
Mie scattering by a charged dielectric particle
 [254]

T. Koch, H. Fehske and J. Loos
Phys. Scr. T151, 014039 (2012)
Phononaffected steadystate transport through molecular quantum dots
 [253]

D. Pagel, H. Fehske, J. Sperling and W. Vogel
Phys. Rev. A 86, 052313 (2012)
Strongly entangled light from planar microcavities
 [252]

S. Ejima, S. Sykora, K. W. Becker and H. Fehske
Phys. Rev. B 86, 155149 (2012)
Phase separation in the Edwards model
 [251]

F. X. Bronold, H. Fehske, R. Heinisch and J. Marbach
Contr. Plasma Phys. 52, 856 (2012)
Wall charge and potential from a microscopic point of view
 [250]

G. Schubert, M. Haass, Th. Trottenberg, H. Fehske and H. Kersten
Contr. Plasma Phys. 52, 827 (2012)
Plasma sheath structure in complex geometries
 [249]

J. Schleede, A. Filinov, M. Bonitz and H. Fehske
Contr. Plasma Phys. 52, 819 (2012)
Phase Diagram of Bilayer ElectronHole Plasmas
 [248]

J. Meichsner, M. Bonitz, A. Piel and H. Fehske
Contr. Plasma Phys. 52, 789 (2012)
Recent Progress in Complex Plasmas
 [247]

A. Alvermann, H. Fehske and P. B. Littlewood
New. J. Phys. 14, 105008 (2012)
Numerical time propagation of quantum systems in radiation fields
 [246]

H. Stolz, R. Schwartz, F. Kieseling, S. Som, M. Kaupsch, S. Sobkowiak, D. Semkat, N. Naka, T. Koch and H. Fehske
New. J. Phys. 14, 105007 (2012)
Condensation of excitons in Cu_{2}O at ultracold temperatures: experiment and theory
 [245]

N. V. Phan and H. Fehske
New. J. Phys. 14, 075007 (2012)
Coulomb interaction effects in graphene bilayers: electronhole pairing and plasmaron formation
 [244]

M. Hohenadler, F. F. Assaad and H. Fehske
Phys. Rev. Lett 109, 116407 (2012)
Effect of electronphonon interaction range for a halffilled band in one dimension
 [243]

J. Marbach, F. X. Bronold and H. Fehske
Phys. Rev. B 86, 115417 (2012)
Pseudoparticle approach for chargetransferring moleculesurface collisions
 [242]

M. Kreutzer, G. Hager, G. Wellein, H. Fehske, A. Basermann and A. R. Bishop,
in Proceedings of the 2012 IEEE 26th International Parallel and Distributed Processing Symposium Workshops PhD Forum (IPDPSW), pp. 16961702, (2012)
Sparse Matrixvector Multiplication on GPGPU Clusters: A New Storage Format and a Scalable Implementation
 [241]

S. Ejima, H. Fehske, F. Gebhard, K. zu Münster, M. Knap, E. Arrigoni and
W. von der Linden
Phys. Rev. A 85, 053644 (2012)
Characterization of Mottinsulating and superfluid phases in the onedimensional BoseHubbard model
 [240]

G. Schubert, H. Fehske, L. Fritz and M. Vojta
Phys. Rev. B 85, 201105(R) (2012)
Fate of topologicalinsulator surface states under strong disorder
 [239]

J. Marbach, F. X. Bronold and H. Fehske
Eur. Phys. J. D 66, 106 (2012)
Resonant charge transfer at dielectric surfaces: Electron capture and release due to impacting metastable nitrogen molecules
 [238]

V. S. Filinov, H. Fehske, M. Bonitz, V. E. Fortov and P. R. Levashov
Contr. Plasma Phys. 52, 224 (2012)
Proton crystallization in a dense hydrogen plasma
 [237]

L. Bakemeier, A. Alvermann and H. Fehske
Phys. Rev. A 85, 043821 (2012)
Quantum phase transition in the Dicke model with critical and noncritical entanglement
 [236]

A. Alvermann, L. Bakemeier and H. Fehske
Phys. Rev. A 85, 043803 (2012)
Collapserevival dynamics and atomfield entanglement in the nonresonant Dicke model
 [235]

M. J. Bhaseen, S. Ejima, F. H. L. Essler, H. Fehske, M. Hohenadler and B. D. Simons
Phys. Rev. A 85, 033636 (2012)
Discrete symmetry breaking transitions between paired superfluids
 [234]

B. Zenker, D. Ihle, F. X. Bronold and H. Fehske
Phys. Rev. B 85, 121102R (2012)
Electronhole pair condensation at the semimetalsemiconductor transition: A BCSBEC crossover scenario
 [233]

G. Schubert and H. Fehske
Materials Science Forum 700, pp 8084 (2012)
Charge carrier localisation in disordered graphene nanoribbons
 [232]

R. Heinisch, F. X. Bronold and H. Fehske
Phys. Rev. B 85, 075323 (2012)
Electron surface layer at the interface of a plasma and a dielectric wall
 [231]

G. Schubert and H. Fehske
Phys. Rev. Lett. 108, 066402 (2012)
Metaltoinsulator transition and electronhole puddle formation in disordered graphene nanoribbons
 [230]

M. Berciu and H. Fehske
Phys. Rev. B 84, 165104 (2011)
AharonovBohm interference for a hole in a twodimensional Ising antiferromagnet in a transverse magnetic field
 [229]

G. Schubert, H. Fehske, G. Hager and G. Wellein
Parallel Processing Letters 21, 339 (2011)
Hybridparallel sparse matrixvector multiplication
with explicit communication overlap on current multicorebased systems
 [228]

T. Koch, J. Loos, A. Alvermann and H. Fehske
Phys. Rev. B 84, 125131 (2011)
Nonequilibrium transport through molecular junctions in the quantum regime
 [227]

G. Schubert, G. Hager, H. Fehske and G. Wellein
in 2011 IEEE International Parallel & Distributed Processing Symposium, Anchorage AK, USA,
IEEE Xplore, DOI: 10.1109/IPDPS.2011.332, pp. 17511757 (2011)
Parallel sparse matrixvector multiplication as a test case for
parallel hybrid MPI+OpenMP programming
 [226]

J. Marbach, F. X. Bronold and H. Fehske
Proceedings 30th ICPIG, Belfast UK (2011)
Secondary electron emission due to Auger deexcitation of metastable nitrogen molecules at metallic surfaces
 [225]

R. L. Heinisch, F. X. Bronold and H. Fehske
Proceedings 30th ICPIG, Belfast UK (2011)
Electronic physisorption at plasma walls
 [224]

J. Marbach, F. X. Bronold and H. Fehske
Phys. Rev. B 84, 085443 (2011)
Auger deexcitation of metastable molecules at metallic surfaces
 [223]

M. J. Bhaseen, S. Ejima, M. Hohenadler, A. O. Silver, F. H. L. Essler,
H. Fehske and B. D. Simons
Phys. Rev. A 84, 023635 (2011)
Magnetic properties of the second Mott lobe in pairing Hamiltonians
 [222]

A. Alvermann, P. B. Littlewood and H.Fehske
Phys. Rev. B 84, 035126 (2011)
A variational discrete variable representation for excitons on a
lattice
 [221]

G. Schubert, R. Basner, H. Kersten and H. Fehske
Eur. Phys. J. D 63, 431 (2011)
Determination of sheath parameters by test particles upon local
electrode bias and plasma switching
Determination of sheath parameters by test particles upon local electrode bias and plasma switching
In this paper, we report how microparticles trapped in the plasma sheath above a grounded or weakly biased electrode can be used to determine changes in the operating conditions of the plasma. We focus on two specific scenarios, (i) switching off the plasma while retaining the biasing of the electrode and (ii) changing the bias voltage during operation of the plasma. Above a critical bias, the microparticle is subject to an additional downward acceleration that cannot be explained solely by gravity and ion drag, but is attributed to a positive charging of the particle induced by extreme outofequilibrium conditions of the surrounding plasma sheath: locally, the plasma sheath can be completely deprived of electrons because of the bias. The observed particle dynamics in such a locally tailored plasma sheath environment directly monitors changes in electric field structures and plasma density profiles (see figure). The experimental results are discussed in the context of a theoretical model that uses basic equations with input data from particleincell (PIC) simulations.
Experiments for which the reported findings might be of relevance range from dusty plasmas to numerous technological plasma processing environments. Arcing and sudden surface charging have been observed in plasma enhanced chemical vapor deposition processes (PECVD) or magnetron sputtering. Similar conditions are important in plasma ion immersion implantation (PIII) for surface treatment, where an ion matrix sheath is created by an abrupt negative highvoltage pulse that is used to accelerate the ions for implantation. In both cases, the results of our studies will apply to microparticles (dust, flakes, powders etc.) present in those discharges.
Figure caption: PIC simulation of the electron and ion densities (left) and electric field (right) along the symmetry axis of the discharge at
different distances (z) from the electrode for various pixel bias voltages (UAE). The electric field declines and the electron increases with
increasing negative bias, whereas the ion density is large unaffected by a change in the bias voltage.
Source: http://www.epj.org/highlight_paper_d.html
 [220]

N. V. Phan, H. Fehske and K. W. Becker
Europhys. Lett. 95, 17006 (2011)
Excitonic resonances in the 2D extended FalicovKimball model
 [219]

B. Zenker, D. Ihle, F. X. Bronold and H. Fehske
Phys. Rev. B 83, 235123 (2011)
Slavefield fluctuation approach to the extended FalicovKimball model: charge, orbital, and excitonic susceptibilities
 [218]

A. Alvermann and H. Fehske
J. Comp. Phys. 230, 5930 (2011)
Highorder commutatorfree exponential timepropagation of
driven quantum systems
 [217]

R. L. Heinisch, F. X. Bronold and H. Fehske
Phys. Rev. B 83, 195407 (2011)
Physisorption of an electron in deep surface potentials
off a dielectric surface
 [216]

S. Sobkowiak, D. Semkat, H. Stolz, Th. Koch and H. Fehske
Phys. Stat. Sol. C 8, 1178 (2011)
Phase separation of multicomponent excitonic BoseEinstein condensates
[featured on front cover]
 [215]

M. Hohenadler, H. Fehske and F. F. Assaad
Phys. Rev. B 83, 115105 (2011)
Dynamic charge correlations near the Peierls transition
 [214]

F. X. Bronold, R. L. Heinisch, J. Marbach and H. Fehske
IEEE Trans. Plasma Science 39, 644 (2011)
Plasma walls beyond the perfect absorber approximation for electrons
 [213]

H. Fehske, G. Wellein and A. R. Bishop
Phys. Rev. B 83, 075104 (2011)
Spatiotemporal evolution of polaronic states in finite quantum
systems
 [212]

J. Kunstmann, C. Özdogan, A. Quandt, and H. Fehske
Phys. Rev. B 83, 045414 (2011)
Stability of edge states and edge magnetism in graphene
nanoribbons
 [211]

S. Ejima, H. Fehske, and F. Gebhard
Europhys. Lett. 93, 30002 (2011)
Dynamic properties of the onedimensional BoseHubbard model
 [210]

S. Ejima, M. J. Bhaseen, M. Hohenadler, F. H. L. Essler, H. Fehske and B. D. Simons
Phys. Rev. Lett. 106, 015303 (2011)
Ising Deconfinement Transition between FeshbachResonant Superfluids
 [209]

B. Zenker, H. Fehske and C. D. Batista
Phys. Rev. B 82, 165110 (2010)
Competing chiral and multipolar electric phases in the extended
FalicovKimball model
 [208]

D. M. Edwards, S. Ejima, A. Alvermann and H. Fehske
J. Phys. Condens. Matter 22, 435601 (2010)
A Green's function decoupling scheme for the Edwards fermionboson model
 [207]

G. Schubert, G. Hager and H. Fehske,
in High Performance Computing in Science and Engineering, Garching/Munich 2009,
Eds. S. Wagner, M. Steinmetz, A. Bode, and M. M. Müller, pp. 1326, Springer Berlin Heidelberg (2010)
Performance limitations for sparse matrixvector multiplications
on current multicore environments
 [206]

R. L. Heinisch, F. X. Bronold and H. Fehske
Phys. Rev. B 82, 125408 (2010)
Phononmediated sticking of electrons at dielectric surfaces
 [205]

M. Berciu and H. Fehske
Phys. Rev. B 82, 085116 (2010)
Momentum Average approximation for models with bosonmodulated hopping:
Role of closed loops in the dynamical generation of a finite quasiparticle mass
 [204]

S. Sobkowiak, D. Semkat, H. Stolz, Th. Koch and H. Fehske
Phys. Rev. B 82, 064505 (2010)
Interacting multicomponent exciton gases in a potential trap:
Phase separation and BoseEinstein condensation
 [203]

J. Schleede, G. Schubert and H. Fehske
Europhys. Lett. 90, 17002 (2010)
Comment on "Anderson transition in disordered graphene" by Amini M. et al.
 [202]

N. V. Phan, K. W. Becker and H. Fehske
Phys. Rev. B 81, 205117 (2010)
June issue of the Virtual Journal of Atomic Quantum Fluids
Spectral signatures of the BCSBEC crossover in the excitonic insulator phase
of the extended FalicovKimball model
 [201]

S. Sykora, K. W. Becker and H. Fehske
Phys. Rev. B 81, 195127 (2010)
Chargedensitywave formation in a twochannel
fermionboson transport model: A projective renormalization approach
 [200]

A. Alvermann, H. Fehske and S. A. Trugman
Phys. Rev. B 81, 165113 (2010)
Polarons and slow quantum phonons
 [199]

A. Alvermann, D. M. Edwards and H. Fehske
Journal of Physics: Conference Series 220, 012023 (2010)
Analytical calculation of the Green's function and Drude weight
for a correlated fermionboson system
 [198]

T. Koch, J. Loos, A. Alvermann, A. R. Bishop and H. Fehske
Journal of Physics: Conference Series 220, 012014 (2010)
Transport through a vibrating quantum dot: Polaronic effects
 [197]

R. L. Heinisch, F. X. Bronold and H. Fehske
Phys. Rev. B 81, 155420 (2010)
Phononmediated desorption of imagebound electrons from dielectric surfaces
 [196]

B. Zenker, D. Ihle, F. X. Bronold and H. Fehske
Phys. Rev. B 81, 115112 (2010)
On the existence of the excitonic insulator phase in the extended FalicovKimball model: a SO(2)invariant slaveboson approach
 [195]

G. Schubert, J. Schleede, K. Byczuk, H. Fehske and D. Vollhardt
Phys. Rev. B 81, 155106 (2010)
Distribution of the local density of states as a criterion for Anderson localization: Application to various lattices in two and three dimensions
highlighted as Editors' Suggestion
 [194]

S. Ejima and H. Fehske
Journal of Physics: Conference Series 200, 012031 (2010)
DMRG analysis of the SDWCDW crossover region in the 1D halffilled HubbardHolstein model
 [193]

A. Alvermann and H. Fehske
Journal of Physics: Conference Series 200, 012005 (2010)
Nonequilibrium current and electron pumping in nanostructures
 [192]

H. Fehske and G. Hager,
in MetaltoNonmetal Transitions,
F. Hensel, P. Edwards and R. Redmer (Eds.),
Springer Series in Material Sciences 132, pp. 122, Springer, Berlin, Heidelberg (2010)
Luttinger, Peierls or Mott? Quantum Phase Transitions in
Strongly Correlated 1D ElectronPhonon Systems
 [191]

F. X. Bronold, H. Deutsch, and H. Fehske,
Proceedings ISPC 19, Bochum 2009,
edited by A. von Keudell, J. Winter, M. Böke, V. Schulzvon der Gathen, (2009)
Microphysics of electrons at plasma boundaries
 [190]

S. Ejima and H. Fehske,
Phys. Rev. B 80, 155101 (2009)
Quantum Transport Affected by a Background Medium:
Fluctuations versus Correlations
 [189]

J. Loos, T. Koch, A. Alvermann, A. R. Bishop and H. Fehske,
J. Phys.: Condens. Matter 21, 395601 (2009)
Phonon affected transport through molecular quantum dots
 [188]

G. Schubert, V. S. Filinov, K. Matyash, R. Schneider and H. Fehske,
Int. J. Mod. Phys. C 20, 1155 (2009)
Comparative study of semiclassical approaches to quantum dynamics
 [187]

G. Wellein, G. Hager, M. Wittmann, T. Zeiser and H. Fehske,
in Proceedings 33rd Annual IEEE International Computer Software and Applications Conference,
IEEE Computer Society Conference Publishing Services, DOI 10.1109/COMPSAC.2009,
p. 579 (2009)
Efficient temporal blocking for stencil computations by
multicoreaware wavefront parallelization
[best paper award]
 [186]

F. X. Bronold, H. Deutsch and H. Fehske,
Eur. Phys. Jour. D 54, 519 (2009)
Physisorption kinetics of electrons at plasma boundaries
 [185]

S. Ejima and H. Fehske,
Europhys. Lett. 87, 27001 (2009)
Luttinger parameters and momentum distribution function
for the halffilled spinless fermion Holstein model: A DMRG approach
 [184]

G. Schubert, J. Schleede and H. Fehske,
Phys. Rev. B 79, 235116 (2009)
June 22, 2009 issue of APS Virtual Journal of Nanoscale Science & Technology
Anderson disorder in graphene nanoribbons:
A local distribution approach
 [183]

V. S. Filinov, M. Bonitz, H. Fehske, P. R. Levashov and V. E. Fortov,
J. Phys. A: Math. General 42, 214014 (2009)
Structures of quantum 2D electronhole plasmas
 [182]

F. X. Bronold, H. Fehske, H. Kersten and H. Deutsch,
Contr. Plasma Phys. 49, 303 (2009)
Towards a microscopic theory of particle charging
 [181]

G. Schubert and H. Fehske,
in Quantum and Semiclassical Percolation and Breakdown in Disordered Solids,
Lecture Notes in Physics 762, pp. 135162, SpringerVerlag, Berlin, Heidelberg, New York (2009)
Quantum percolation in disordered structures
 [180]

H. Fehske, J. Schleede, G. Schubert, G. Wellein, V. S. Filinov and A. R. Bishop,
Phys. Lett. A 373, 2182 (2009)
Numerical approaches to time evolution of complex quantum systems
 [179]

A. S. Mishchenko, N. Nagaosa, A. Alvermann, H. Fehske, G. De Filippis, V. Cataudella and O. P. Sushkov,
Phys. Rev. B (Rapid Comm.) 79, 180301(R) (2009)
Localizationdelocalization transition of a polaron near a impurity
 [178]

A. Alvermann and H. Fehske,
Phys. Rev. Lett. 102, 150601 (2009)
Sparse polynomial space approach to dissipative quantum systems: Application to the subohmic spinboson model
 [177]

S. Ejima, G. Hager, and H. Fehske,
Phys. Rev. Lett. 102, 106404 (2009)
Quantum phase transition in a 1D transport model with boson affected hopping: Luttinger liquid versus
chargedensitywave behavior
 [176]

R. Basner, F. Sigeneger, D. Loffhagen, G. Schubert, H. Fehske, and H. Kersten,
New J. Phys. 11, 013041 (2009)
Particles as probes for complex plasmas in front of biased surfaces
 [175]

H. Fehske, A. Alvermann, and G. Wellein,
in High Performance Computing in Science and Engineering, Garching/Munich 2007,
Eds. S. Wagner, M. Steinmetz, A. Bode, and M. Brehm, pp. 649668, Springer Berlin Heidelberg (2009)
Quantum transport within a background medium: Fluctuations versus Correlations
 [174]
 H. Fehske, G. Hager, and E. Jeckelmann,
Europhys. Lett. 84, 57001 (2008) Metallicity in the halffilled HolsteinHubbard model
 [173]
 D. Ihle, M. Pfafferott, E. Burovski, F. X. Bronold, and H. Fehske,
Phys. Rev. B 78, 193103 (2008) Bound state formation and nature of the excitonic insulator phase in the extended FalicovKimball model
 [172]
 F. X. Bronold, H. Fehske, H. Kersten, and H. Deutsch,
Phys. Rev. Lett. 101, 175002 (2008) Surface states and the charge of a dust particle in a plasma
 [171]
 G. Schubert and H. Fehske,
Phys. Rev. B 78, 155115 (2008) Diffusion and localization in quantum random resistor networks
 [170]
 A. Alvermann, H. Fehske, and S. A. Trugman,
Phys. Rev. B 78, 165106 (2008) Solution of the Holstein polaron anisotropy problem
 [169]
 G. Wellein, H. Fehske, A. Alvermann, and D. M. Edwards,
Phys. Rev. Lett. 101, 136402 (2008) CorrelationInduced Metal Insulator Transition in a TwoChannel FermionBoson Model
 [168]
 A. Quandt, C. Özdogan, J. Kunstmann and H. Fehske,
phys. stat. sol. (b) 245, 2077 (2008) Boron doped graphene nanostructures
 [167]
 E. Burovski, H. Fehske, A. S. Mishchenko,
Phys. Rev. Lett. 101, 116403 (2008) Exact Treatment of ExcitonPolaron Formation by Diagrammatic Monte Carlo Simulations
 [166]
 V.S. Filinov, H. Fehske, M. Bonitz, V.E. Fortov and P. Levashov,
Phys. Lett. A 372, 52085214 (2008) Ordered structure formation in 2D mass asymmetric electronhole plasmas
 [165]
 V.S. Filinov, G. Schubert, P. Levashov, M. Bonitz, H. Fehske, V.E. Fortov and A.V. Filinov,
Phys. Lett. A 372, 50645070 (2008) Centerofmass tomographic approach to quantum dynamics
 [164]
 A. Quandt, C. Özdogan, J. Kunstmann and H. Fehske,
Nanotechnology 19, 335707 (2008) Functionalizing graphene by embedded boron clusters
 [163]
 G. Schubert and H. Fehske,
Phys. Rev. B 77, 245130 (2008) Dynamical aspects of twodimensional quantum percolation
 [162]
 F. X. Bronold and Holger Fehske,
Superlattices and Microstructures 43, 512 (2008) On the possibility of excitonic phases at the semiconductorsemimetal transition
 [161]
 M. Bonitz, P. Ludwig, H. Baumgartner, C. Henning, A. Filinov, D. Block, O. Arp, A. Piel, S. Käding, Y. Ivanov, A. Melzer, H. Fehske, and V. Filinov,
Physics of Plasmas 15, 055704 (2008) Classical and quantum Coulomb crystals
 [160]
 A. Weisse and H. Fehske,
in Computational Many Particle Physics, Lecture Notes in Physics 739, pp. 545577, Springer Berlin Heidelberg 2008 Chebyshev expansion techniques
 [159]
 A. Weisse and H. Fehske,
in Computational Many Particle Physics, Lecture Notes in Physics 739, pp. 529544, Springer Berlin Heidelberg 2008 Exact diagonalization techniques
 [158]
 A. Alvermann and H. Fehske,
in Computational Many Particle Physics, Lecture Notes in Physics 739, pp. 505526, Springer Berlin Heidelberg 2008 The local distribution approach
 [157]
 H. Fehske, G. Wellein, J. Loos and A.R. Bishop, Phys. Rev. B 77, 085117 (2008).
Localized polarons and doorway vibrons in finite quantum structures
 [156]
 A. Alvermann and H. Fehske, Phys. Rev. B 77, 045125 (2008).
Chebyshev approach to quantum systems coupled to a bath
 [155]
 F.X. Bronold, K. Matyash, D. Tskhakaya, R. Schneider, and H. Fehske, Proceedings of the 28th International Conference on Phenomena in Ionized Gases, Prague, Czech Republic, July 2007,
Particlebased modeling of oxygen discharges
 [154]
 K.Dittmann, K. Matyash, F.X. Bronold, R.Schneider, H. Fehske, and J.Meichsner, Proceedings of the 28th International Conference on Phenomena in Ionized Gases, Prague, Czech Republic, July 2007,
Heavy particle impact excitation of atomic oxygen in front of the powered elctrode of oxygen rf plasmas  Experiment and PICSimulation
 [153]
 K. Matyash, H. Baumgartner, G. Schubert, R. Schneider, A. Filinov, A. Melzer, H. Fehske, and M. Bonitz, Proceedings of the 34th European Physical Society Conference on Plasma Physics, Warsaw, Poland, June 2007,
Modeling dust in plasmas: From 2d dust crystals to Coulomb balls
 [152]
 M. Hohenadler, P. B. Littlewood, and H. Fehske, Phys. Rev. B 76, 184303 (2007).
Lattice excitonpolaron problem by quantum Monte Carlo simulations
 [151]
 F. X. Bronold, K. Matyash, D. Tskhakaya, R. Schneider and H. Fehske, J. Phys. D: Appl. Phys. 40, 6583 (2007).
Radiofrequency discharges in oxygen: I. Particlebased modelling
 [150]
 H. Fehske and S. A. Trugman in Polarons in Advanced Materials edited by A. S. Alexandrov, Springer Series in Material Sciences 103 pp. 393461, Springer Verlag, Dordrecht (2007).
Numerical solution of the Holstein polaron problem
 [149]
 F. X. Bronold, H. Fehske and G. Roepke, J. Phys. Soc. Japan, Suppl. A 76, 27 (2007).
Excitonic versus electronhole liquid phases in Tm[Se,Te] compounds
 [148]
 M. Hohenadler and H. Fehske, J. Phys.: Condens. Matter 19, 255210 (2007).
Bipolaron formation in 1D to 3D quantum dots: A lattice quantum Monte Carlo approach
 [147]
 M. Hohenadler, G. Hager, G. Wellein, and H. Fehske, J. Phys.: Condens. Matter 19, 255202 (2007).
Carrierdensity effects in manypolaron systems
 [146]
 J. Loos, M. Hohenadler, A. Alvermann, and H. Fehske, J. Phys.: Condens. Matter 19, 236233 (2007).
Optical conductivity of polaronic charge carriers
 [145]
 G. Hager, A. Weisse, G. Wellein, E. Jeckelmann, and H. Fehske, J. Magn. Magn. Mat 310, 1380 (2007).
Phase diagram of the spinPeierls chain revisited J. Magn. Magn. Mat 316, 43 (2007). Erratum
 [144]
 V.S. Filinov, H. Fehske, M. Bonitz, V.E. Fortov, and P.R. Levashov, Phys. Rev. E 75, 036401 (2007).
Correlation effects in partially ionized mass asymmetric electronhole plasmas
 [143]
 V.S. Filinov, M. Bonitz, V.E. Fortov, H. Fehske, and P.R. Levashov, phys. stat. sol. (b) 244, 474 (2007).
Coulomb crystal and quantum melting in electronhole plasmas of semiconductors under high pressure
 [142]
 A. Alvermann, D. M. Edwards, and H. Fehske, Phys. Rev. Lett. 98, 056602 (2007).
Bosoncontrolled quantum transport
 [141]
 A. Weiße, G. Hager, A. R. Bishop, and H. Fehske, Phys. Rev. B 74, 214426 (2006)
Phase diagram of the spinPeierls chain with local coupling: Density matrix renormalizationgroup calculations and unitary transformations
 [140]
 R. Basner, G. Thieme, F. Sigeneger, H. Kersten, G. Schubert, and H. Fehske, Proceedings of the 33th European Physical Society Conference on Plasma Physics, Rome, Italy, June 2006, pp. 2082
Plasma sheath diagnostics by microparticles of different sizes
 [139]
 F. X. Bronold and H. Fehske, Phys. Rev. B 74, 165107 (2006)
Possibility of an excitonic insulator at the semiconductorsemimetal transition
 [138]
 M. Bonitz, V.S. Filinov, A. Filinov, V. Golubnychiy, P. Ludwig, H. Baumgartner, P.R. Levashov, V.E. Fortov, and H. Fehske, ``Irreversible Prozesse und Selbstorganisation'', Eds. Th. Pöschel, H. Malchow, and L. SchimanskyGeyer, Logos Verlag, Berlin (2006), pp 143158:
Structure formation in strongly correlated Coulomb systems.
 [137]
 J. Loos, M. Hohenadler, A. Alvermann, and H. Fehske, J. Phys.: Condens. Matter 18, 7299 (2006)
Phonon spectral function of the Holstein polaron.
 [136]
 M. Hohenadler, G. Wellein, A. R. Bishop, A. Alvermann, and H. Fehske, Phys. Rev. B 74, 245120 (2006)
Spectral signatures of the Luttinger liquid to chargedensitywave transition.
 [135]
 H. Fehske, F.X. Bronold, and A. Alvermann, Proc. Int. School of Physics ``Enrico Fermi'', Course CLXI, Polarons in Bulk Materials and Systems with Reduced Dimensionality, Eds. G. Iadonisi, J. Ranninger, G. de Filippis, IOS Press, Amsterdam, Oxford, Tokio, Washington DC (2006), pp 313325
Localisation versus selftrapping: Polaron formation in the AndersonHolstein model.
 [134]
 H. Fehske and E. Jeckelmann, Proc. Int. School of Physics ``Enrico Fermi'', Course CLXI, Polarons in Bulk Materials and Systems with Reduced Dimensionality, Eds. G. Iadonisi, J. Ranninger, G. de Filippis, IOS Press, Amsterdam, Oxford, Tokio, Washington DC (2006), pp 297311
Quantum phase transitions in onedimensional electronphonon systems. Rivista del Nuovo Cimento, 30 (2007), pp.259292
 [133]
 H. Fehske, A. Alvermann, M. Hohenadler, and G. Wellein, Proc. Int. School of Physics ``Enrico Fermi'', Course CLXI, Polarons in Bulk Materials and Systems with Reduced Dimensionality, Eds. G. Iadonisi, J. Ranninger, G. de Filippis, IOS Press, Amsterdam, Oxford, Tokio, Washington DC (2006), pp 285296
Spectral signatures of Holstein polarons.
 [132]
 E. Jeckelmann and H. Fehske, Proc. Int. School of Physics ``Enrico Fermi'', Course CLXI, Polarons in Bulk Materials and Systems with Reduced Dimensionality, Eds. G. Iadonisi, J. Ranninger, G. de Filippis, IOS Press, Amsterdam, Oxford, Tokio, Washington DC (2006), pp 247283
Exact numerical methods for electronphonon problems.
 [131]
 H. Fehske, G. Hager, G. Wellein, and E. Jeckelmann, Physica B 378380, 319 (2006)
Hole doped Hubbard ladders
 [130]
 G. Wellein, A. R. Bishop, M. Hohenadler, G. Schubert, and H. Fehske, Physica B 378380, 281 (2006)
Optical response of manypolaron systems
 [129]
 B. Hülsen, F. X. Bronold, H. Fehske, and Y. Yonemitsu, Physica B 378380, 267 (2006)
Phase diagram of the excitonic insulator
 [128]
 M. Hohenadler, G. Wellein, A. Alvermann, and H. Fehske, Physica B 378380, 64 (2006)
Manypolaron problem by cluster perturbation theory
 [127]
 A. Alvermann and H. Fehske, Journal of Physics: Conference Series 35, 145 (2006).
Stochastic Green's function approach to disordered systems
 [126]
 V. Golubnychiy, H. Baumgartner, M. Bonitz, A. Filinov, and H. Fehske, J. Phys. A 39, 4527 (2006).
Screened Coulomb balls  structural properties and melting behaviour
 [125]
 M. Bonitz, V.S. Filinov, V.E. Fortov, P.R. Levashov, and H. Fehske, J. Phys. A 39, 4717 (2006).
Hole crystallization in semiconductors
 [124]
 V.S. Filinov, M. Bonitz, V.E. Fortov, W. Ebeling, H. Fehske, D. Kremp, W.D. Kraeft, V. Bezkrovniy, P. Levashov, J. Phys. A 39, 4421 (2006).
Monte Carlo simulations of dense quantum plasmas
 [123]
 G. Schubert, A. Alvermann, A. Weiße, G. Hager, G. Wellein, and H. Fehske, NIC Symposium 2006, edited by Gernot Münster, Dietrich Wolf, and Manfred Kremer, NIC Series Volume 32, John von Neumann Institut for Computing, (2006), pp.201210.
Spectral properties of strongly correlated electron phonon systems
 [122]
 J. Loos, M Hohenadler, and H Fehske, J. Phys.: Condens. Matter 18, 2453 (2006).
Spectral functions of the spinless Holstein model
 [121]
 A. Weiße, G. Wellein, A. Alvermann, and H. Fehske, Rev. Mod. Phys. 78, 275 (2006).
The kernel polynomial method
 [120]
 A. Alvermann and H. Fehske, Eur. Phys. J. B 48, 295 (2005).
Local distribution approach to disordered binary alloys
 [119]
 M. Bonitz, V.S. Filinov, V.E. Fortov, P.R. Levashov, and H. Fehske, Phys. Rev. Lett. 95, 235006 (2005).
Crystallization in TwoComponent Coulomb Systems
 [118]
 R. Basner, H. Fehske, H. Kersten, S. Kosse, and G. Schubert, VIP 17, 259 (2005).
Gezielte Manipulation von Mikropartikeln in einem Plasma
 [117]
 G. Schubert, G. Wellein, A. Weiße, A. Alvermann and H. Fehske, Phys. Rev. B 72, 104304 (2005).
Optical absorption and activated transport in polaronic systems
 [116]
 O. Arp, D. Block, M. Bonitz, H. Fehske, V. Golubnychiy, S. Kosse, P. Ludwig, A. Melzer, and A. Piel, Journal of Physics: Conference Series 11, 234 (2005).
3D Coulomb balls: Experiment and simulation
 [115]
 H. Fehske, V. S. Filinov, M. Bonitz, V. E. Fortov, and P. Levashov, Journal of Physics: Conference Series 11, 139 (2005).
Exciton formation and dissociation in massasymmetric electronhole plasmas
 [114]
 M. Hohenadler, D. Neuber, W. von der Linden, G. Wellein, J. Loos, and H. Fehske, Phys. Rev. B 71, 245111 (2005).
Photoemission spectra of manypolaron systems
 [113]
 G. Schubert, A. Weiße, and H. Fehske, Physica B 359361, 801 (2005).
Delocalization transition in chains with correlated disorder
 [112]
 A. Alvermann, G. Schubert, A. Weiße, F. X. Bronold, and H. Fehske, Physica B 359361, 789 (2005).
Characterisation of Anderson localisation using distributions
 [111]
 A. Weiße, G. Schubert, and H. Fehske, Physica B 359361, 786 (2005).
Optical response of electrons in a random potential
 [110]
 A. Weiße, H. Fehske, and D. Ihle, Physica B 359361, 702 (2005).
Spinlattice coupling effects in the Holstein doubleexchange model
 [109]
 H. Fehske, G. Wellein, G. Hager, A. Weiße, K. W. Becker, and A.R. Bishop, Physica B 359361, 699 (2005).
Luttinger liquid versus charge density wave behaviour in the onedimensional spinless fermion Holstein model
 [108]
 G. Hager, G. Wellein, E. Jeckelmann and H. Fehske, Phys. Rev. B 71, 075108 (2005).
Stripe formation in doped Hubbard ladders
 [107]
 G. Schubert, A. Weiße and H. Fehske, Phys. Rev. B 71, 045126 (2005).
Localization effects in quantum percolation
 [106]
 G. Schubert, A. Weiße, G. Wellein and H. Fehske in High Performance Computing in Science and Engineering, Garching 2004 edited by A. Bode and F. Durst, SpringerVerlag, Berlin, Heidelberg, New York (2005), pp.237250.
Comparative numerical study of Anderson localization in disordered electron systems.
 [105]
 S. Sykora, A. Hübsch, K. W. Becker, G. Wellein, H. Fehske, Phys. Rev. B 71, 045112 (2005).
Singleparticle excitations and soft phonon mode in the onedimensional Holstein model
 [104]
 G. Hager, E. Jeckelmann, H. Fehske, and G. Wellein, in Modelling, Simulation and Optimization of Complex Processes, Eds. H. G. Bock, E. Kostina, H.X. Phu, R. Rannacher, SpringerVerlag Berlin Heidelberg (2005), pp 165175.
Exact numerical treatment of finite quantum systems using leadingedge supercomputers
 [103]
 S. Krivenko, A. Yaresko, G. Khaliullin, and H. Fehske, J. Magn. Magn. Mat. 272276, 458459 (2004).
Magnon softening and damping in the ferromagnetic manganites due to orbital correlations
 [102]
 A. Weiße and H. Fehske, J. Magn. Magn. Mat. 272276, 9293 (2004).
Lattice and superexchange effects in doped CMR manganites
 [101]
 A. Weiße and H. Fehske, New J. Phys. 6 (Orbital Physics Focus Issue), 158 (2004).
Microscopic modelling of doped manganites
 [100]
 H. Fehske, G. Wellein, G. Hager, A. Weiße and A. R. Bishop, Phys. Rev. B 69 , 165115 (2004).
Quantum lattice dynamical effects on the singleparticle excitations in 1D Mott and Peierls insulators
 [99]
 G. Hager, E. Jeckelmann, G. Wellein, and H. Fehske, High Performance Computing in Science and Engineering, Munich 2004, edited by S. Wagner, W. Hanke, A. Bode, F. Durst, SpringerVerlag Berlin Heidelberg (2004), pp 339.
DMRG investigation of stripe formation in doped Hubbard ladders
 [98]
 F. X. Bronold, A. Alvermann, and H. Fehske, Phil. Mag. B 84 , 673 (2004).
Anderson localization in strongly coupled disordered electronphonon systems
 [97]
 G. Hager, E. Jeckelmann, H. Fehske, and G. Wellein, J. Comp. Phys. 194 , 795 (2004).
Parallelzation strategies for density matrix renormalization group algorithms on sharedmemory systems
 [96]
 A. Alvermann, F.X. Bronold and H. Fehske Phys. Status Solidi B 1 63 (2004).
Electron transport in the Anderson model
 [95]
 U. Glaser, H. Büttner, and H. Fehske, Phys. Rev. A 68 , 032318 (2003).
Entanglement and correlation in anisotropic quantum spin systems
 [94]
 A. Weiße, J. Loos, and H. Fehske, Phys. Rev. B 68 , 024402 (2003).
Mixedphase description of colossal magnetoresistive manganites
 [93]
 H. Fehske, G. Wellein, A. P. Kampf, M. Sekania, G. Hager, A. Weiße, H. Büttner, and A. R. Bishop,
in High Performance Computing in Science and Engineering, Munich 2002, edited by S. Wagner, W. Hanke, A. Bode, F. Durst, SpringerVerlag Berlin Heidelberg (2003), pp 339349 Onedimensional electronphonon systems: Mott versus Peierls insulators
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 F.X. Bronold and H. Fehske, Acta Physica Polonica 34, 851 (2003)
Statistical dynamical meanfield description of strongly correlated disordered electronphonon systems
 [91]
 A. Weiße, G. Wellein, and H. Fehske, in High Performance Computing in Science and Engineering '02 edited by E. Krause and W. Jäger, SpringerVerlag Berlin Heidelberg (2003), pp. 157167
Exact diagonalization study of spin, orbital, and lattice correlations in CMR manganites
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 G. Wellein, G. Hager, A. Basermann, and H. Fehske, in High Performance Computing for Computational Science  VECPAR2002 edited by J. Palma, J. Dongarra, V. Hernandez, A. A. Sousa, Lecture Notes in Computer Science 2565, Springer Verlag Berlin Heidelberg (2003), pp. 287301
Fast sparse matrixvector multiplication for TFlop/s computers
 [89]
 H. Fehske, A. P. Kampf, M. Sekania, and G. Wellein, Eur. Phys. Jour. B 31, 11 (2003)
Nature of the Peierls to Mottinsulator transition in 1D
 [88]
 A. Weiße and H. Fehske, Eur. Phys. Jour. B 30, 487 (2002).
Interplay of charge, spin, orbital and lattice correlations in colossal magnetoresistance manganites
 [87]
 F.X. Bronold and H. Fehske, Phys. Rev. B 66 , 073102 (2002).
Anderson localization of polaron states
 [86]
 H. Fehske, A. Weiße, and Gerhard Wellein, NIC Symposium 2001, edited by H. Rollnik and D. Wolf, NIC Series Volume 9, John von Neumann Institut for Computing, (2002), pp 259.
Exact diagonalization results for strongly correlated electronphonon systems
 [85]
 A. Weiße and H. Fehske, Physica B 312313 , 721 (2002).
Numerical study of quantum percolation
 [84]
 H. Fehske, G. Wellein, A. Weiße, F. Göhmann, H. Büttner, and A. R. Bishop, Physica B 312313 , 562 (2002).
Peierlsinsulator Mottinsulator transition in 1D
 [83]
 A. Weiße, G. Wellein, and H. Fehske, in High Performance Computing in Science and Engineering '01
edited by E. Krause and W. Jäger, SpringerVerlag Berlin Heidelberg (2002), pp. 131; arXiv:condmat/0104533. DensityMatrix Algorithm for Phonon Hilbert Space Reduction in the Numerical Diagonalization of Quantum ManyBody Systems
 [82]
 G. Wellein, G. Hager, A. Basermann, and H. Fehske, CD CUG 2001,
Exact Diagonalization of Large Sparse Matrices: A Challenge for Modern Supercomputers
 [81]
 D. Ihle, C. Schindelin, and H. Fehske, Phys. Rev. B. 64 , 054419 (2001).
Magnetic order in the quasitwodimensional easyplane XXZ model
 [80]
 A. Weiße, J. Loos, and H. Fehske, Phys. Rev. B. 64 , 104413 (2001).
Twophase scenario for the metalinsulator transition in CMR manganites
 [79]
 A. Weiße, J. Loos, and H. Fehske, Phys. Rev. B. 64 , 054406 (2001); 64 , 149903(E) (2001).
Considerations on the quantum doubleexchange Hamiltonian; Erratum
 [78]
 H. Fehske, M. Kinateder, G. Wellein, and A. R. Bishop, Phys. Rev. B. 63 , 245121 (2001).
Quantum lattice effects in mixedvalence transitionmetal chain complexes
 [77]
 C. Schindelin, H. Fehske, H. Büttner, and D. Ihle J. Magn. Magn. Mater. 226230 , 403 (2001).
Quantum effects in the 2D XY model
 [76]
 M. Holicki and H. Fehske, J. Magn. Magn. Mater. 226230 , 397 (2001).
Landau approach to the spinPeierls transition
 [75]
 M. Kinateder, G. Wellein, A. Basermann, and H. Fehske, in High Performance Computing in Science and Engineering '00
edited by E. Krause and W. Jäger, SpringerVerlag Berlin Heidelberg (2001), pp. 188204. JacobiDavidson algorithm with fast matrix vector multiplication on massively parallel and vector supercomputers
 [74]
 M. Holicki, H. Fehske, and R. Werner, Phys. Rev. B. 63 , 174417 (2001).
Magnetoelastic excitations in spinPeierls systems
 [73]
 H. Fehske, C. Schindelin, A. Weiße, H. Büttner, and D. Ihle, Brazil. Jour. Phys. (2001) 30 , 720 (2000).
Quantum to classical crossover in the 2D easyplane XXZ model
 [72]
 C. Schindelin, H. Fehske, H. Büttner, and D. Ihle, Phys. Rev. B. 62 , 12141 (2000).
Spin correlation functions and susceptibilities in the easyplane XXZ chain
 [71]
 H. Fehske, M. Holicki, and A. Weiße, Advances in Solid State Physics, 40 , 235 (2000).
Lattice dynamical effects on the Peierls transition in onedimensional metals and spin chains
 [70]
 H. Fehske, M. Deeg, and H. Büttner, in DFG: Macromolecular Systems: Microscopic Interactions and Macroscopic Properties
edited by H. Hoffmann, M. Schwoerer, and T. Vogtmann, WileyVCH Weinheim (2000), pp. 88112. SlaveBoson Approach to Strongly Correlated Electron Systems
 [69]
 A. Weiße, H. Fehske, G. Wellein, and A. R. Bishop, Phys. Rev. B 62 , R747 (2000).
Optimized phonon approach for the diagonalization of electronphonon problems
 [68]
 H. Fehske, J. Loos, and G. Wellein, Phys. Rev. B 61 , 8016 (2000).
Lattice polaron formation: Effects of nonscreened electronphonon interaction
 [67]
 G. Wellein and H. Fehske, in High Performance Computing in Science and Engineering '99 edited by E. Krause and W. Jäger, SpringerVerlag Berlin Heidelberg (2000), pp. 112129.
Towards the limits of presentday supercomputers: Exact diagonalization of strongly correlated electronphonon systems
 [66]
 C. Schindelin, D. Ihle, S.L. Drechsler, and H. Fehske, Physica B 281 & 282, 819 (2000).
Spin correlation functions and Neel order in the 2D Heisenberg model: Effects of spatial anisotropy
 [65]
 H. Fehske, G. Wellein, H. Büttner, A. R. Bishop, and M. I. Salkola, Physica B 281 & 282, 673 (2000).
Local mode behaviour in quasi1D CDW systems
 [64]
 D. Ihle, C. Schindelin, A. Weiße, and H. Fehske, Phys. Rev. B 60, 9240 (1999).
Magnetic orderdisorder transition in the twodimensional spatially anisotropic Heisenberg model at zero temperature
 [63]
 A. Weiße, G. Wellein and H. Fehske, Phys. Rev. B 60, 6566 (1999).
Quantum lattice fluctuations in a frustrated Heisenberg spinPeierls chain
 [62]
 H. Fehske, G. Wellein, and H. Büttner, J. Supercond., 12 , 65 (1999).
Pairing susceptibility of strongly correlated electrons weakly coupled to the lattice
 [61]
 J. Loos and H. Fehske, Physica B, 259261, 801 (1999).
Spin excitations in ferromagnetic manganites
 [60]
 B. Büchner, H. Fehske, A. P. Kampf, and G. Wellein, Physica B, 259261, 956 (1999).
Lattice dimerization for the spinPeierls compound CuGeO_{3}
 [59]
 A. Weiße, G. Bouzerar, and H. Fehske, Eur. Phys. Jour. B 7, 5 (1999).
A new model to describe the physics of (VO)_{2}P_{2}O_{7}
 [58]
 A. Weiße and H. Fehske, Phys. Rev. B 58, 13526 (1998).
Peierls instability and optical response in the onedimensional halffilled Holstein model of spinless fermions
 [57]
 G. Wellein, H. Fehske, and A. P. Kampf, Phys. Rev. Lett. 81, 3956 (1998).
Peierls dimerization with nonadiabatic spinphonon coupling
 [56]
 G. Wellein and H. Fehske, Phys. Rev. B 58, 6208 (1998).
Selftrapping problem of electrons or excitons in one dimension
 [55]
 B. Bäuml, G. Wellein and H. Fehske, Phys. Rev. B 58, 3663 (1998).
Optical absorption and singleparticle excitations in the 2D Holstein tJ model
 [54]
 G. Wellein, B. Bäuml, and H. Fehske, Recent Progress in ManyBody theories, edited by D. Neilson and R. F. Bishop, World Scientific, Singapore (1998), p. 481.
Dynamical pairing correlations in the tJ model with nonadiabatic holephonon coupling
 [53]
 U. Trapper, D.Ihle, H. Büttner, and H. Fehske, J. Magn. Magn. Mater. 177181, 577 (1998).
Magnetic shortrange order effects in the 2D tJ model
 [52]
 H. Fehske, J. Loos and G. Wellein, Z. Phys. B 104, 619 (1997).
Spectral properties of the 2D Holstein polaron
 [51]
 H. Fehske, G. Wellein, B. Bäuml, and R. N. Silver, Physica C 282287, 1829 (1997).
Spectral properties of the 2D Holstein tJ model
 [50]
 G. Wellein, H. Fehske, H. Büttner, and A. R. Bishop, Physica C 282287, 1827 (1997).
On the stability of polaronic superlattices in strongly coupled electronphonon systems
 [49]
 U. Trapper, H. Fehske, and D. Ihle, Physica C 282287, 1779 (1997).
Magnetic properties of the 2D tt'Hubbard model
 [48]
 G. Wellein and H. Fehske, Phys. Rev. B 55, 4513 (1997).
Polaron band formation in the Holstein model
 [47]
 J. Loos and H. Fehske, Phys. Rev. B 56, 3544 (1997).
Effective oneband electronphonon Hamiltonian for nickel perovskites
 [46]
 U. Trapper, D. Ihle, and H. Fehske, Int. J. Mod. Phys. B 11, 1337 (1997).
Theory of magnetic shortrange order for itinerant electron systems
 [45]
 H. Fehske, G. Wellein, B. Bäuml, and H. Büttner, Physica B 230232, 899 (1997).
Polaronic effects in strongly coupled electronphonon systems: Exact diagonalization results for the 2D Holstein tJ model
 [44]
 U. Trapper, D. Ihle, and H. Fehske, Physica B 230232, 906 (1997).
Theory of magnetic shortrange order for highTc superconductors
 [43]
 C. Schindelin, U. Trapper, H. Fehske, and H. Büttner, Czech. J. Physics 46, 1881 (1996).
Theory of shortrange magnetic order for the tJ model
 [42]
 J. Loos and H. Fehske, Czech. J. Physics 46 1879 (1996).
Interplay of charge and spin correlations in nickel perovskites
 [41]
 U. Trapper, D. Ihle, and H. Fehske, Phys. Rev. B 54, 7614 (1996).
Spin susceptibility and magnetic shortrange order in the Hubbard model
 [40]
 G. Wellein, H. Röder, and H. Fehske, Phys. Rev. B 52, 9666 (1996).
Polarons and bipolarons in strongly interacting electronphonon systems
 [39]
 U. Trapper, D. Ihle, and H. Fehske, Phys. Rev. B 52, R 11553 (1995).
Magnetic shortrange versus longrange order in the Hubbard model
 [38]
 H. Fehske, H. Röder, G. Wellein, and A. Mistriotis, Phys. Rev. B 51, 16582 (1995).
Holepolaron formation in the 2D HolsteintJ model: A variational Lanczos study
 [37]
 D. Ihle and H. Fehske, J. Phys. A 28, L 275 (1995).
Unitarytransformation scheme for bi/polaron correlation models
 [36]
 M. Deeg, H. Fehske, and H. Büttner, J. Phys.: Condensed Matter 7, L 245 (1995).
Magnetic correlations and spin dynamics in the tt'J model
 [35]
 H. Fehske and M. Deeg, J. Low Temp. Phys. 99, 425 (1995).
Magnetism and transport in the tt'J model
 [34]
 H. Fehske and M. Deeg, Solid State Commun. 93, 41 (1995).
Hall resistivity of hole and electrondoped highTc cuprates
 [33]
 M. Deeg and H. Fehske, Phys. Rev. B 50, 17874 (1994).
Slaveboson study of the tt'J model: phase diagram, spin susceptibility and Hall resistivity
 [32]
 H. Röder, H. Fehske, and R. N. Silver, Europhys. Lett. 28, 257 (1994).
The ordering of polarons in the HolsteintJ model: An application to La_{2x}Sr_{x}NiO_{4+y}
 [31]
 D. Ihle, H. Fehske, J. Loos, and U. Trapper, Physica C 235240, 2363 (1994).
Bi/Polaron formation and optical conductivity in the HolsteinHubbard model
 [30]
 H. Fehske and M. Deeg, Physica C 235240, 2243 (1994).
Transport and charge/magnetic order in the 2D (Holstein) tt'J model
 [29]
 M. Deeg, H. Fehske, S. Körner, S. Trimper, and D. Ihle, Z. Phys. B 95, 87 (1994).
Dynamic spin and charge susceptibilities in the tJ model
 [28]
 M. Deeg, H. Fehske, and H. Büttner, Europhys. Lett. 26, 109 (1994).
Magnetic Phase Diagram and Transport Properties of the tJ Model: A SpinRotationInvariant SlaveBoson Approach
 [27]
 H. Fehske, D. Ihle, J. Loos, U. Trapper, and H. Büttner, Z. Phys. B 94, 91 (1994).
Polaron formation and hopping conductivity in the HolsteinHubbard model
 [26]
 H. Fehske and H. Röder, NATO Advanced Research Workshop on Nonlinear Coherent Structures in Physics and Biology, Bayreuth 1993, edited by K. H. Spatschek and F. G. Mertens, NATO ASI series B 329, p. 233, Plenum Press, New York, (1994).
The phase diagram of the 2D HolsteintJ model
 [25]
 H.Fehske, U. Trapper, M. Deeg, and H. Büttner, NATO Advanced Research Workshop on Nonlinear Coherent Structures in Physics and Biology, Bayreuth 1993, edited by K. H. Spatschek and F. G. Mertens, NATO ASI series B 329, p. 229, Plenum Press, New York, (1994).
Variational slave boson approach to the HolsteinHubbard model
 [24]
 U. Trapper, H. Fehske, M. Deeg and H. Büttner, Z. Phys. B 93, 465 (1994).
Electron correlations and quantum lattice vibrations in strongly coupled electronphonon systems: a variational slave boson approach
 [23]
 V. Waas, H. Fehske, and H. Büttner, Phys. Rev. B 48, 9106 (1993).
Exact diagonalization study of the tJ model in the lowdensity limit: Implications for phase separation
 [22]
 H. Fehske, H. Röder, A. Mistriotis, and H. Büttner, J. Phys. Condens. Matter 5, 3565 (1993).
The phase diagram of the 2D HolsteintJ model near halffilling
 [21]
 H. Röder, H. Fehske, and H. Büttner, Phys. Rev. B 47, 12420 (1993).
Exact diagonalisation study of the 2D tJ model with adiabatic Holstein phonons: Single hole case
 [20]
 M. Deeg, H. Fehske, and H. Büttner, Z. Phys. B 91, 31 (1993).
Slaveboson phase diagram of the twodimensional extended Hubbard model: Influence of electronphonon coupling
 [19]
 M. Deeg, H. Fehske, and H. Büttner, Z. Phys. B 88, 283 (1992).
Slave boson mean field theory for the 2D Peierls Hubbard system
 [18]
 H. Fehske, M. Deeg, and H. Büttner, Phys. Rev. B 46, 3713 (1992).
Twodimensional PeierlsHubbard model within the slaveboson approach
 [17]
 H. Röder, H. Fehske, V. Waas, and H. Büttner, Phys. Rev. B 45, 13092 (1992).
Thermodynamics of the twodimensional tJ model
 [16]
 H. Fehske, V. Waas, H. Röder, and H. Büttner, Phys. Rev. B 44, 8473 (1991).
Hole dynamics in a strongly correlated twodimensional spin background
 [15]
 H. Röder, V. Waas, H. Fehske, and H. Büttner, Phys. Rev. B 43, 6284 (1991).
Holes in a twodimensional Hubbard antiferromagnet
 [14]
 H. Fehske, V. Waas, H. Röder, and H. Büttner, Solid State Commun. 76, 1333 (1990).
On the possibility of phase separation in the extended Hubbard model
 [13]
 H. Fehske and D. Ihle, J. Phys. Soc. Jpn. 58, 360 (1989).
On the T^{ 3}lnT law in the specific heat of spinfluctuation compounds
 [12]
 D. Ihle and H. Fehske, Phys. Rev. B 39, 2106 (1989).
Fermisurface geometry and pressure effects on the spinfluctuation contributions to the specific heat: Anisotropic spinfluctuation model for heavyfermion UPt3
 [11]
 H. Fehske and D. Ihle, J. Phys. C 21, 4663 (1988).
On the coexistence of ferro and antiferromagnetic spin fluctuations and their contributions to the specific heat
 [10]
 H. Fehske and D. Ihle, J. Phys. F 18, 33 (1988).
Flatness in the wavevectordependent response function of metals with a corrugated cylindrical Fermi surface: Consequences for the paramagnon mass enhancement
 [9]
 H. Fehske and D. Ihle, Proceedings of the 6 th International Seminar on Magnetism, Wiss. Zeitschrift der Hochschule für Verkehrswesen Dresden 31, 113, Dohma(1987).
Effects of Fermi surface geometry on the spin susceptibility: Model calculation
 [8]
 H. Fehske and D. Ihle, J. Phys. F 17, 2109 (1987).
Effects of Fermi surface anisotropy and topology on the spin susceptibility of metals
 [7]
 H. Fehske, Phys. Status Solidi B 130, K121 (1985).
On a simple functional moment approach to itinerant magnetism: Application to Ni
 [6]
 B. Lorenz and H. Fehske, Phys. Status Solidi B 126, 235 (1984).
Critical study of the static functional integral method in the Hubbard model
 [5]
 H. Fehske and B. Lorenz, Lecture Notes in Physics 206 Static Critical Phenomena in Inhomogeneous System, edited by A. Pekalski and J. Sznajd (Berlin 1984). SpringerVerlag.
Some remarks on the spin fluctuation theories for itinerant electrons
 [4]
 H. Fehske and B. Lorenz, J. Phys. C 17, 5031 (1984).
On the validity of the static approximation in the spinfluctuation theory for itinerant electrons
 [3]
 H. Fehske, E. Kolley, and W. Kolley, Phys. Status Solidi B 123, 553 (1984).
Spinglass behaviour in disordered Hubbard alloys
 [2]
 H. Fehske, Phys. Status Solidi B 120, 611 (1983).
Spin fluctuations in alloys with random transfer
 [1]
 E. Kolley, W. Kolley, and H. Fehske, Phys. Status Solidi B 109, 551 (1982).
CPA study of the electrical coductivity for various percolation models

