G. Krämer

The dual-electron cyclotron emission based measurement of 3D structures on DIII-D tokamak

Overview of results from the 2023 DIII-D negative triangularity campaign

Overview of the SPARC tokamak

<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msubsup><mml:mi mathvariant="normal">Λ</mml:mi><mml:mi>c</mml:mi><mml:mo>±</mml:mo></mml:msubsup></mml:math> production in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>p</mml:mi><mml:mi>p</mml:mi></mml:math> collisions with a new fragmentation function

<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>b</mml:mi></mml:math>-hadron production in the general-mass variable-flavor-number scheme and the LHC data

Study of heavy meson production in p–Pb collisions at <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" altimg="si1.gif" overflow="scroll"><mml:msqrt><mml:mrow><mml:mi>S</mml:mi></mml:mrow></mml:msqrt><mml:mo>=</mml:mo><mml:mn>5.02</mml:mn></mml:math> TeV in the general-mass variable-flavour-number scheme

Inclusive $$B$$ B -meson production at small $$p_T$$ p T in the general-mass variable-flavor-number scheme

Energetic particle instabilities in fusion plasmas

Overview of physics results from the conclusive operation of the National Spherical Torus Experiment

Fast-ion energy loss during TAE avalanches in the National Spherical Torus Experiment