@unpublished{HenkelPieplow2014, author = {Henkel, Carsten and Pieplow, Gregor}, title = {Reply to Comment on 'Fully covariant radiation force on a polarizable particle'}, series = {New journal of physics : the open-access journal for physics}, volume = {16}, journal = {New journal of physics : the open-access journal for physics}, publisher = {IOP Publ. Ltd.}, address = {Bristol}, issn = {1367-2630}, doi = {10.1088/1367-2630/16/11/118002}, pages = {8}, year = {2014}, abstract = {We argue that the theories of Volokitin and Persson (2014 New J. Phys. 16 118001), Dedkov and Kyasov (2008 J. Phys.: Condens. Matter 20 354006), and Pieplow and Henkel (2013 New J. Phys. 15 023027) agree on the electromagnetic force on a small, polarizable particle that is moving parallel to a planar, macroscopic body, as far as the contribution of evanescent waves is concerned. The apparent differences are discussed in detail and explained by choices of units and integral transformations. We point out in particular the role of the Lorentz contraction in the procedure used by Volokitin and Persson, where a macroscopic body is 'diluted' to obtain the force on a small particle. Differences that appear in the contribution of propagating photons are briefly mentioned.}, language = {en} } @article{HaakhHenkelSpagnoloetal.2014, author = {Haakh, Harald R. and Henkel, Carsten and Spagnolo, Salvatore and Rizzuto, Lucia and Passante, Roberto}, title = {Dynamical Casimir-Polder interaction between an atom and surface plasmons}, series = {Physical review : A, Atomic, molecular, and optical physics}, volume = {89}, journal = {Physical review : A, Atomic, molecular, and optical physics}, number = {2}, publisher = {American Physical Society}, address = {College Park}, issn = {1050-2947}, doi = {10.1103/PhysRevA.89.022509}, pages = {11}, year = {2014}, abstract = {We investigate the time-dependent Casimir-Polder potential of a polarizable two-level atom placed near a surface of arbitrary material, after a sudden change in the parameters of the system. Different initial conditions are taken into account. For an initially bare ground-state atom, the time-dependent Casimir-Polder energy reveals how the atom is "being dressed" by virtual, matter-assisted photons. We also study the transient behavior of the Casimir-Polder interaction between the atom and the surface starting from a partially dressed state, after an externally induced change in the atomic level structure or transition dipoles. The Heisenberg equations are solved through an iterative technique for both atomic and field operators in the medium-assisted electromagnetic field quantization scheme. We analyze, in particular, how the time evolution of the interaction energy depends on the optical properties of the surface, in particular on the dispersion relation of surface plasmon polaritons. The physical significance and the limits of validity of the obtained results are discussed in detail.}, language = {en} } @article{MkrtchianHenkel2014, author = {Mkrtchian, Vanik E. and Henkel, Carsten}, title = {On non-equilibrium photon distributions in the Casimir effect}, series = {Annalen der Physik}, volume = {526}, journal = {Annalen der Physik}, number = {1-2}, publisher = {Wiley-VCH}, address = {Weinheim}, issn = {0003-3804}, doi = {10.1002/andp.201300135}, pages = {87 -- 101}, year = {2014}, abstract = {The electromagnetic field in a typical geometry of the Casimir effect is described in the Schwinger-Keldysh formalism. The main result is the photon distribution function (Keldysh Green function) in any stationary state of the field. A two-plate geometry with a sliding interface in local equilibrium is studied in detail, and full agreement with the results of Rytov fluctuation electrodynamics is found.}, language = {en} } @article{JoulainBenAbdallahChapuisetal.2014, author = {Joulain, Karl and Ben-Abdallah, Philippe and Chapuis, Pierre-Olivier and De Wilde, Y. and Babuty, A. and Henkel, Carsten}, title = {Strong tip-sample coupling in thermal radiation scanning tunneling microscopy}, series = {Journal of quantitative spectroscopy \& radiative transfer}, volume = {136}, journal = {Journal of quantitative spectroscopy \& radiative transfer}, publisher = {Elsevier}, address = {Oxford}, issn = {0022-4073}, doi = {10.1016/j.jqsrt.2013.12.006}, pages = {1 -- 15}, year = {2014}, language = {en} } @article{PapkeYadavalliHenkeletal.2014, author = {Papke, Thomas and Yadavalli, Nataraja Sekhar and Henkel, Carsten and Santer, Svetlana}, title = {Mapping a plasmonic hologram with photosensitive polymer films: standing versus propagating waves}, series = {ACS applied materials \& interfaces}, volume = {6}, journal = {ACS applied materials \& interfaces}, number = {16}, publisher = {American Chemical Society}, address = {Washington}, issn = {1944-8244}, doi = {10.1021/am503501y}, pages = {14174 -- 14180}, year = {2014}, abstract = {We use a photosensitive layer containing azobenzene moieties to map near-field intensity patterns in the vicinity of nanogrids fabricated within a thin silver layer. It is known that azobenzene containing films deform permanently during irradiation, following the pattern of the field intensity. The photosensitive material reacts only to stationary waves whose intensity patterns do not change in time. In this study, we have found a periodic deformation above the silver film outside the nanostructure, even if the latter consists of just one groove. This is in contradiction to the widely accepted viewpoint that propagating surface plasmon modes dominate outside nanogrids. We explain our observation based on an electromagnetic hologram formed by the constructive interference between a propagating surface plasmon wave and the incident light. This hologram contains a stationary intensity and polarization grating that even appears in the absence of the polymer layer.}, language = {en} }