@article{NishikawaHardeeZhangetal.2013,
  author    = {Nishikawa, Ken-Ichi and Hardee, P. and Zhang, B. and Dutan, I. and Medvedev, M. and Choi, E. J. and Min, K. W. and Niemiec, J. and Mizuno, Y. and Nordlund, Ake and Frederiksen, Jacob Trier and Sol, H. and Pohl, Martin and Hartmann, D. H.},
  title     = {Magnetic field generation in a jet-sheath plasma via the kinetic Kelvin-Helmholtz instability},
  series = {Annales geophysicae},
  volume    = {31},
  journal   = {Annales geophysicae},
  number    = {9},
  publisher = {Copernicus},
  address   = {G{\"o}ttingen},
  issn      = {0992-7689},
  doi       = {10.5194/angeo-31-1535-2013},
  pages     = {1535 -- 1541},
  year      = {2013},
  abstract  = {We have investigated the generation of magnetic fields associated with velocity shear between an unmagnetized relativistic jet and an unmagnetized sheath plasma. We have examined the strong magnetic fields generated by kinetic shear (Kelvin-Helmholtz) instabilities. Compared to the previous studies using counter-streaming performed by Alves et al. (2012), the structure of the kinetic Kelvin-Helmholtz instability (KKHI) of our jet-sheath configuration is slightly different, even for the global evolution of the strong transverse magnetic field. In our simulations the major components of growing modes are the electric field E-z, perpendicular to the flow boundary, and the magnetic field B-y, transverse to the flow direction. After the B-y component is excited, an induced electric field E-x, parallel to the flow direction, becomes significant. However, other field components remain small. We find that the structure and growth rate of KKHI with mass ratios m(i)/m(e) = 1836 and m(i)/m(e) = 20 are similar. In our simulations in the nonlinear stage is not as clear as in counter-streaming cases. The growth rate for a mildly-relativistic jet case (gamma(j) = 1.5) is larger than for a relativistic jet case (gamma(j) = 15).},
  language  = {en}
}
@article{NishikawaMizunoGomezetal.2017,
  author    = {Nishikawa, Ken-Ichi and Mizuno, Yosuke and Gomez, Jose L. and Dutan, Ioana and Meli, Athina and White, Charley and Niemiec, Jacek and Kobzar, Oleh and Pohl, Martin and Frederiksen, Jacob Trier and Nordlund, Ake and Sol, Helene and Hardee, Philip E. and Hartmann, Dieter H.},
  title     = {Microscopic Processes in Global Relativistic Jets Containing Helical Magnetic Fields: Dependence on Jet Radius},
  series = {Galaxies : open access journal},
  volume    = {5},
  journal   = {Galaxies : open access journal},
  publisher = {MDPI},
  address   = {Basel},
  issn      = {2075-4434},
  doi       = {10.3390/galaxies5040058},
  pages     = {7},
  year      = {2017},
  abstract  = {In this study, we investigate the interaction of jets with their environment at a microscopic level, which is a key open question in the study of relativistic jets. Using small simulation systems during past research, we initially studied the evolution of both electron-proton and electron-positron relativistic jets containing helical magnetic fields, by focusing on their interactions with an ambient plasma. Here, using larger jet radii, we have performed simulations of global jets containing helical magnetic fields in order to examine how helical magnetic fields affect kinetic instabilities, such as the Weibel instability, the kinetic Kelvin-Helmholtz instability (kKHI) and the mushroom instability (MI). We found that the evolution of global jets strongly depends on the size of the jet radius. For example, phase bunching of jet electrons, in particular in the electron-proton jet, is mixed with a larger jet radius as a result of the more complicated structures of magnetic fields with excited kinetic instabilities. In our simulation, these kinetic instabilities led to new types of instabilities in global jets. In the electron-proton jet simulation, a modified recollimation occurred, and jet electrons were strongly perturbed. In the electron-positron jet simulation, mixed kinetic instabilities occurred early, followed by a turbulence-like structure. Simulations using much larger (and longer) systems are required in order to further thoroughly investigate the evolution of global jets containing helical magnetic fields.},
  language  = {en}
}
@article{NishikawaMizunoNiemiecetal.2016,
  author    = {Nishikawa, Ken-Ichi and Mizuno, Yosuke and Niemiec, Jacek and Kobzar, Oleh and Pohl, Martin and Gomez, Jose L. and Dutan, Ioana and Frederiksen, Jacob Trier and Nordlund, Ake and Meli, Athina and Sol, Helene and Hardee, Philip E. and Hartmann, Dieter H.},
  title     = {Microscopic Processes in Global Relativistic Jets Containing Helical Magnetic Fields},
  series = {Galaxies : open access journal},
  volume    = {4},
  journal   = {Galaxies : open access journal},
  publisher = {MDPI},
  address   = {Basel},
  issn      = {2075-4434},
  doi       = {10.3390/galaxies4040038},
  pages     = {9},
  year      = {2016},
  abstract  = {In the study of relativistic jets one of the key open questions is their interaction with the environment on the microscopic level. Here, we study the initial evolution of both electron-proton (e(-)-p(+)) and electron-positron (e(+/-)) relativistic jets containing helical magnetic fields, focusing on their interaction with an ambient plasma. We have performed simulations of "global" jets containing helical magnetic fields in order to examine how helical magnetic fields affect kinetic instabilities such as the Weibel instability, the kinetic Kelvin-Helmholtz instability (kKHI) and the Mushroom instability (MI). In our initial simulation study these kinetic instabilities are suppressed and new types of instabilities can grow. In the e(-)-p(+) jet simulation a recollimation-like instability occurs and jet electrons are strongly perturbed. In the e(+/-) jet simulation a recollimation-like instability occurs at early times followed by a kinetic instability and the general structure is similar to a simulation without helical magnetic field. Simulations using much larger systems are required in order to thoroughly follow the evolution of global jets containing helical magnetic fields.},
  language  = {en}
}
@misc{NishikawaMizunoNiemiecetal.2016,
  author    = {Nishikawa, Ken-Ichi and Mizuno, Yosuke and Niemiec, Jacek and Kobzar, Oleh and Pohl, Martin and G{\´o}mez, Jose L. and Duţan, Ioana and Pe'er, Asaf and Frederiksen, Jacob Trier and Nordlund, {\AA}ke and Meli, Athina and Sol, Helene and Hardee, Philip E. and Hartmann, Dieter H.},
  title     = {Microscopic processes in global relativistic jets containing helical magnetic fields},
  series = {Galaxies},
  journal   = {Galaxies},
  url       = {http://nbn-resolving.de/urn:nbn:de:kobv:517-opus4-407604},
  pages     = {9},
  year      = {2016},
  abstract  = {In the study of relativistic jets one of the key open questions is their interaction with the environment on the microscopic level. Here, we study the initial evolution of both electron-proton (e(-)-p(+)) and electron-positron (e(+/-)) relativistic jets containing helical magnetic fields, focusing on their interaction with an ambient plasma. We have performed simulations of "global" jets containing helical magnetic fields in order to examine how helical magnetic fields affect kinetic instabilities such as the Weibel instability, the kinetic Kelvin-Helmholtz instability (kKHI) and the Mushroom instability (MI). In our initial simulation study these kinetic instabilities are suppressed and new types of instabilities can grow. In the e(-)-p(+) jet simulation a recollimation-like instability occurs and jet electrons are strongly perturbed. In the e(+/-) jet simulation a recollimation-like instability occurs at early times followed by a kinetic instability and the general structure is similar to a simulation without helical magnetic field. Simulations using much larger systems are required in order to thoroughly follow the evolution of global jets containing helical magnetic fields.},
  language  = {en}
}