Three-body universality in the <i>B</i> meson sector

Abstract The charged exotic mesons Z b (10610) and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mi>Z</mml:mi> <mml:mi>b</mml:mi> <mml:mo>′</mml:mo> </mml:msubsup> <mml:mo stretchy="false">(</mml:mo> <mml:mn>10650</mml:mn> <mml:mo stretchy="false">)</mml:mo> </mml:math> observed by the Belle collaboration in 2011 are very close to the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msup> <mml:mrow> <mml:mi>B</mml:mi> </mml:mrow> <mml:mrow> <mml:mo>∗</mml:mo> </mml:mrow> </mml:msup> <mml:mover accent="true"> <mml:mrow> <mml:mi>B</mml:mi> </mml:mrow> <mml:mrow> <mml:mo>¯</mml:mo> </mml:mrow> </mml:mover> </mml:math> and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msup> <mml:mrow> <mml:mi>B</mml:mi> </mml:mrow> <mml:mrow> <mml:mo>∗</mml:mo> </mml:mrow> </mml:msup> <mml:msup> <mml:mrow> <mml:mover accent="true"> <mml:mrow> <mml:mi>B</mml:mi> </mml:mrow> <mml:mrow> <mml:mo>¯</mml:mo> </mml:mrow> </mml:mover> </mml:mrow> <mml:mrow> <mml:mo>∗</mml:mo> </mml:mrow> </mml:msup> </mml:math> thresholds, respectively. This suggests their interpretation as shallow hadronic molecules of B and B ∗ mesons. Using the masses of the Z b (10610) and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mi>Z</mml:mi> <mml:mi>b</mml:mi> <mml:mo>′</mml:mo> </mml:msubsup> <mml:mo stretchy="false">(</mml:mo> <mml:mn>10650</mml:mn> <mml:mo stretchy="false">)</mml:mo> </mml:math> as input, we rule out the possibility for universal bound states of three B and B ∗ mesons arising from the Efimov effect based on their spin-isospin structure. As a consequence, we can predict the phase shifts for the scattering of B and B ∗ mesons off the exotic mesons Z b (10610) and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mi>Z</mml:mi> <mml:mi>b</mml:mi> <mml:mo>′</mml:mo> </mml:msubsup> <mml:mo stretchy="false">(</mml:mo> <mml:mn>10650</mml:mn> <mml:mo stretchy="false">)</mml:mo> </mml:math> to leading order in a non-relativistic effective field theory with contact interactions based on two-body information alone.

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Publication Details

Journal
Journal of Physics G Nuclear and Particle Physics
Published
2025-09-15
DOI
https://doi.org/10.1088/1361-6471/ae06be
Primary Topic
Superconducting Materials and Applications
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article
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article

Three-body universality in the B meson sector

H.‐W. Hammer, Yong-Hui Lin, Ulf-G. Meißner, Erik Wilbring et al.
Journal of Physics G Nuclear and Particle Physics
Superconducting Materials and Applications
article

Three-body universality in the B meson sector

H.‐W. Hammer, Yong-Hui Lin, Ulf-G. Meißner, Erik Wilbring, Hailong Fu
article en

Abstract

Abstract The charged exotic mesons Z b (10610) and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mi>Z</mml:mi> <mml:mi>b</mml:mi> <mml:mo>′</mml:mo> </mml:msubsup> <mml:mo stretchy="false">(</mml:mo> <mml:mn>10650</mml:mn> <mml:mo stretchy="false">)</mml:mo> </mml:math> observed by the Belle collaboration in 2011 are very close to the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msup> <mml:mrow> <mml:mi>B</mml:mi> </mml:mrow> <mml:mrow> <mml:mo>∗</mml:mo> </mml:mrow> </mml:msup> <mml:mover accent="true"> <mml:mrow> <mml:mi>B</mml:mi> </mml:mrow> <mml:mrow> <mml:mo>¯</mml:mo> </mml:mrow> </mml:mover> </mml:math> and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msup> <mml:mrow> <mml:mi>B</mml:mi> </mml:mrow> <mml:mrow> <mml:mo>∗</mml:mo> </mml:mrow> </mml:msup> <mml:msup> <mml:mrow> <mml:mover accent="true"> <mml:mrow> <mml:mi>B</mml:mi> </mml:mrow> <mml:mrow> <mml:mo>¯</mml:mo> </mml:mrow> </mml:mover> </mml:mrow> <mml:mrow> <mml:mo>∗</mml:mo> </mml:mrow> </mml:msup> </mml:math> thresholds, respectively. This suggests their interpretation as shallow hadronic molecules of B and B ∗ mesons. Using the masses of the Z b (10610) and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mi>Z</mml:mi> <mml:mi>b</mml:mi> <mml:mo>′</mml:mo> </mml:msubsup> <mml:mo stretchy="false">(</mml:mo> <mml:mn>10650</mml:mn> <mml:mo stretchy="false">)</mml:mo> </mml:math> as input, we rule out the possibility for universal bound states of three B and B ∗ mesons arising from the Efimov effect based on their spin-isospin structure. As a consequence, we can predict the phase shifts for the scattering of B and B ∗ mesons off the exotic mesons Z b (10610) and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mi>Z</mml:mi> <mml:mi>b</mml:mi> <mml:mo>′</mml:mo> </mml:msubsup> <mml:mo stretchy="false">(</mml:mo> <mml:mn>10650</mml:mn> <mml:mo stretchy="false">)</mml:mo> </mml:math> to leading order in a non-relativistic effective field theory with contact interactions based on two-body information alone.

Journal of Physics G Nuclear and Particle PhysicsVol. 52(10)
Openalex Percentile: Top 77%
Superconducting Materials and Applications
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