Unified coupled-channel description for the five near-threshold structures <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:mi>ψ</mml:mi> <mml:mo stretchy="false">(</mml:mo> <mml:mn>3770</mml:mn> <mml:mo stre

The recent observation of multiple near-threshold structures in <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"> <a:msup> <a:mi>e</a:mi> <a:mo>+</a:mo> </a:msup> <a:msup> <a:mi>e</a:mi> <a:mo>−</a:mo> </a:msup> </a:math> annihilation—including <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"> <c:mi>ψ</c:mi> <c:mo stretchy="false">(</c:mo> <c:mn>3770</c:mn> <c:mo stretchy="false">)</c:mo> </c:math> , <g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline"> <g:mi>G</g:mi> <g:mo stretchy="false">(</g:mo> <g:mn>3900</g:mn> <g:mo stretchy="false">)</g:mo> </g:math> , <k:math xmlns:k="http://www.w3.org/1998/Math/MathML" display="inline"> <k:mi>R</k:mi> <k:mo stretchy="false">(</k:mo> <k:mn>3760</k:mn> <k:mo stretchy="false">)</k:mo> </k:math> , <o:math xmlns:o="http://www.w3.org/1998/Math/MathML" display="inline"> <o:mi>R</o:mi> <o:mo stretchy="false">(</o:mo> <o:mn>3780</o:mn> <o:mo stretchy="false">)</o:mo> </o:math> , and <s:math xmlns:s="http://www.w3.org/1998/Math/MathML" display="inline"> <s:mi>R</s:mi> <s:mo stretchy="false">(</s:mo> <s:mn>3810</s:mn> <s:mo stretchy="false">)</s:mo> </s:math> —reveals limitations in existing models of charmonium and exotic hadrons. In this paper, we propose a unified coupled-channel description that simultaneously incorporates all five near-threshold structures using parameters constrained by hadron spectroscopy. Our model accurately reproduces the line shapes in both <w:math xmlns:w="http://www.w3.org/1998/Math/MathML" display="inline"> <w:mi>D</w:mi> <w:mover accent="true"> <w:mi>D</w:mi> <w:mo stretchy="false">¯</w:mo> </w:mover> </w:math> and nonopen-charm hadron (nOCH) channels, resolves the asymmetric profile of <ab:math xmlns:ab="http://www.w3.org/1998/Math/MathML" display="inline"> <ab:mi>ψ</ab:mi> <ab:mo stretchy="false">(</ab:mo> <ab:mn>3770</ab:mn> <ab:mo stretchy="false">)</ab:mo> </ab:math> , and produces the <eb:math xmlns:eb="http://www.w3.org/1998/Math/MathML" display="inline"> <eb:mi>G</eb:mi> <eb:mo stretchy="false">(</eb:mo> <eb:mn>3900</eb:mn> <eb:mo stretchy="false">)</eb:mo> </eb:math> bump. We identify the <ib:math xmlns:ib="http://www.w3.org/1998/Math/MathML" display="inline"> <ib:mi>R</ib:mi> <ib:mo stretchy="false">(</ib:mo> <ib:mn>3780</ib:mn> <ib:mo stretchy="false">)</ib:mo> </ib:math> as the dominant manifestation of <mb:math xmlns:mb="http://www.w3.org/1998/Math/MathML" display="inline"> <mb:mi>ψ</mb:mi> <mb:mo stretchy="false">(</mb:mo> <mb:mn>3770</mb:mn> <mb:mo stretchy="false">)</mb:mo> </mb:math> , attribute <qb:math xmlns:qb="http://www.w3.org/1998/Math/MathML" display="inline"> <qb:mi>R</qb:mi> <qb:mo stretchy="false">(</qb:mo> <qb:mn>3760</qb:mn> <qb:mo stretchy="false">)</qb:mo> </qb:math> to <ub:math xmlns:ub="http://www.w3.org/1998/Math/MathML" display="inline"> <ub:mi>D</ub:mi> <ub:mover accent="true"> <ub:mi>D</ub:mi> <ub:mo stretchy="false">¯</ub:mo> </ub:mover> <ub:mo stretchy="false">→</ub:mo> <ub:mtext>nOCH</ub:mtext> </ub:math> rescattering and suggest that <zb:math xmlns:zb="http://www.w3.org/1998/Math/MathML" display="inline"> <zb:mi>R</zb:mi> <zb:mo stretchy="false">(</zb:mo> <zb:mn>3810</zb:mn> <zb:mo stretchy="false">)</zb:mo> </zb:math> arises from coupling between the <dc:math xmlns:dc="http://www.w3.org/1998/Math/MathML" display="inline"> <dc:mi>ψ</dc:mi> <dc:mo stretchy="false">(</dc:mo> <dc:mn>1</dc:mn> <dc:mi>D</dc:mi> <dc:mo stretchy="false">)</dc:mo> </dc:math> state and the <hc:math xmlns:hc="http://www.w3.org/1998/Math/MathML" display="inline"> <hc:msub> <hc:mi>h</hc:mi> <hc:mi>c</hc:mi> </hc:msub> <hc:mi>π</hc:mi> <hc:mi>π</hc:mi> </hc:math> channel. The significant non- <jc:math xmlns:jc="http://www.w3.org/1998/Math/MathML" display="inline"> <jc:mi>D</jc:mi> <jc:mover accent="true"> <jc:mi>D</jc:mi> <jc:mo stretchy="false">¯</jc:mo> </jc:mover> </jc:math> decay of <nc:math xmlns:nc="http://www.w3.org/1998/Math/MathML" display="inline"> <nc:mi>ψ</nc:mi> <nc:mo stretchy="false">(</nc:mo> <nc:mn>3770</nc:mn> <nc:mo stretchy="false">)</nc:mo> </nc:math> is explained by its near-threshold position. This analysis provides a coherent, unquenched framework centered on a charmonium <rc:math xmlns:rc="http://www.w3.org/1998/Math/MathML" display="inline"> <rc:mi>ψ</rc:mi> <rc:mo stretchy="false">(</rc:mo> <rc:mn>1</rc:mn> <rc:mi>D</rc:mi> <rc:mo stretchy="false">)</rc:mo> </rc:math> core for near-threshold phenomena and offers a predictive approach extendable to bottomonium systems and future data from Belle II.