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@ARTICLE{Amano:485662,
author = {Amano, Takanobu and Matsumoto, Yosuke and Bohdan, Artem and
Kobzar, Oleh and Matsukiyo, Shuichi and Oka, Mitsuo and
Niemiec, Jacek and Pohl, Martin and Hoshino, Masahiro},
title = {{N}onthermal electron acceleration at collisionless
quasi-perpendicular shocks},
journal = {Reviews of modern plasma physics},
volume = {6},
number = {1},
issn = {2367-3192},
address = {Cham},
publisher = {Springer International Publishing},
reportid = {PUBDB-2022-06749, arXiv:2209.03521},
pages = {29},
year = {2022},
note = {To appear in Reviews of Modern Plasma Physics as an invited
review Waiting for fulltext},
abstract = {Shock waves propagating in collisionless heliospheric and
astrophysical plasmas have been studied extensively over the
decades. One prime motivation is to understand the
nonthermal particle acceleration at shocks. Although the
theory of diffusive shock acceleration (DSA) has long been
the standard for cosmic-ray acceleration at shocks, plasma
physical understanding of particle acceleration remains
elusive. In this review, we discuss nonthermal electron
acceleration mechanisms at quasi-perpendicular shocks, for
which substantial progress has been made in recent years.
The discussion presented in this review is restricted to the
following three specific topics: The first is stochastic
shock drift acceleration (SSDA), which is a relatively new
mechanism for electron injection into DSA. The basic
mechanism, related in-situ observations and kinetic
simulations results, and how it is connected with DSA will
be discussed. Second, we discuss shock surfing acceleration
(SSA) at very high Mach number shocks relevant to young
supernova remnants (SNRs). While the original proposal under
the one-dimensional assumption is unrealistic, SSA has now
been proven efficient by a fully three-dimensional kinetic
simulation. We discuss the multidimensional nature of SSA
and its role in electron injection. Finally, we discuss the
current understanding of the magnetized Weibel-dominated
shock. It is essentially a magnetized shock in which the
reflected-gyrating ions dominate the formation of the shock
structure but with a substantial magnetic field
amplification by the ion-Weibel instability. Spontaneous
magnetic reconnection of self-generated current sheets
within the shock structure is an interesting consequence of
Weibel-generated strong magnetic turbulence. Although the
exact condition for active magnetic reconnection has not
been clarified, we argue that high Mach number shocks with
both Alfvén and sound Mach numbers exceeding 20–40 will
likely behave as a Weibel-dominated shock. Despite a number
of interesting recent findings, the relative roles of SSDA,
SSA, and magnetic reconnection for electron acceleration at
collisionless shocks and how the dominant particle
acceleration mechanisms change depending on shock parameters
remain to be answered.},
keywords = {Particle acceleration (autogen) / Cosmic rays (autogen) /
Collisionless shock (autogen) / Wave-particle interaction
(autogen) / Plasma waves (autogen)},
cin = {$Z_THAT$},
ddc = {530},
cid = {$I:(DE-H253)Z_THAT-20210408$},
pnm = {613 - Matter and Radiation from the Universe (POF4-613)},
pid = {G:(DE-HGF)POF4-613},
experiment = {EXP:(DE-MLZ)NOSPEC-20140101},
typ = {PUB:(DE-HGF)16},
eprint = {2209.03521},
howpublished = {arXiv:2209.03521},
archivePrefix = {arXiv},
SLACcitation = {$\%\%CITATION$ = $arXiv:2209.03521;\%\%$},
UT = {WOS:001193699100038},
doi = {10.1007/s41614-022-00093-1},
url = {https://bib-pubdb1.desy.de/record/485662},
}