Ушбу ишга иқтибос қилган ишлар

3 та иш

Иш: One- versus two-pole<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mover accent="true"><mml:mi>K</mml:mi><mml:mo>¯</mml:mo></mml:mover><mml:mi>N</mml:mi></mml:mrow></mml:math>-<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>π</mml:mi><mml:mi>Σ</mml:mi></mml:mrow></mml:math>potential:<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mi>K</mml:mi><mml:mo>−</mml:mo></mml:msup><mml:mi>d</mml:mi></mml:mrow></mml:math>scattering length

1. Faddeev Treatment of the Quasi-Bound and Scattering States in the $${\bar{K}NN - \pi\Sigma N}$$ System

   N. V. Shevchenko

   МақолаQuantum Chromodynamics and Particle InteractionsFew-Body Systems20130 иқтибос

   ABIABI:AkademIndex/openalex/2013.article.000385

2. Faddeev Treatment of the Quasi-Bound and Scattering States in the $${\bar{K}NN - \pi\Sigma N}$$ K ¯ N N - π Σ N System: New Results

   N. V. Shevchenko

   МақолаQuantum Chromodynamics and Particle InteractionsFew-Body Systems20130 иқтибос

   ABIABI:AkademIndex/openalex/2013.article.000636

3. Scattering and bound states in the K − d system

   N. V. Shevchenko

   МақолаQuantum Chromodynamics and Particle InteractionsPhysics of Atomic Nuclei20140 иқтибос

   ABIABI:AkademIndex/openalex/2014.article.000440