The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays | Paper Citation Record

Observation e30d12ed-046f-400e-9cf6-5aaf391b056d · outbound

This paper cites An overview of $XYZ$ new particles.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays An overview of $XYZ$ new particles

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Observation 66454f2c-33cd-44df-b55d-c2826f080539 · outbound

This paper cites (11) It is convenient to deal with it by the dimensional regulariza- tion method, 16π2G(s, m2 1, m2.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays (11) It is convenient to deal with it by the dimensional regulariza- tion method, 16π2G(s, m2 1, m2

Reference 2

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Observation 3534674b-e999-4960-a791-9695666b3204 · outbound

This paper cites In addition,µ is the scale of dimensional regularization, and changes in the scale are reabsorbed in the subtraction constanta(µ), so that the results remain scale independent.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays In addition,µ is the scale of dimensional regularization, and changes in the scale are reabsorbed in the subtraction constanta(µ), so that the results remain scale independent

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Observation e61671a9-c9c1-4d92-9ff4-416f448c5e03 · outbound

This paper cites Exotic Hadrons with Heavy Flavors -X, Y, Z and Related States-.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Exotic Hadrons with Heavy Flavors -X, Y, Z and Related States-

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Observation c993f8d0-6c8d-473c-8339-525e82bf7f1a · outbound

This paper cites The hidden-charm pentaquark and tetraquark states.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays The hidden-charm pentaquark and tetraquark states

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Observation 63bfdce7-6f88-4ae8-a1e6-2c1d1bb8b80f · outbound

This paper cites Heavy-Quark QCD Exotica.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Heavy-Quark QCD Exotica

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Observation e277a4d8-a8f4-4e3d-b05e-92651e917c8d · outbound

This paper cites Hadronic molecules.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Hadronic molecules

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Observation 4a190314-6851-46d2-8bbe-2b7a471da865 · outbound

This paper cites Non-Standard Heavy Mesons and Baryons, an Experimental Review.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Non-Standard Heavy Mesons and Baryons, an Experimental Review

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Observation c48ac9eb-adf8-4b6a-aa72-14181bd4a8b1 · outbound

This paper cites The $XYZ$ states: experimental and theoretical status and perspectives.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays The $XYZ$ states: experimental and theoretical status and perspectives

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Observation b1905c95-c59e-43fe-8585-188601fc53b8 · outbound

This paper cites Exotic hadrons: review and perspectives.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Exotic hadrons: review and perspectives

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Observation 748bc33a-a340-49db-a48e-c2e0faa8fcb5 · outbound

This paper cites Chiral perturbation theory for heavy hadrons and chiral effective field theory for heavy hadronic molecules.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Chiral perturbation theory for heavy hadrons and chiral effective field theory for heavy hadronic molecules

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Observation 2821a20b-a47e-43cf-a0c5-7ba142755737 · outbound

This paper cites An updated review of the new hadron states.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays An updated review of the new hadron states

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Observation fde7a020-486c-4509-85d4-4481d4b7fae2 · outbound

This paper cites Three ways to decipher the nature of exotic hadrons: multiplets, three-body hadronic molecules, and correlation functions.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Three ways to decipher the nature of exotic hadrons: multiplets, three-body hadronic molecules, and correlation functions

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Observation 6e62ac76-f5b8-4e08-a028-ce5288e1b033 · outbound

This paper cites Pentaquark and Tetraquark states.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Pentaquark and Tetraquark states

Reference 14

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Observation 3aa2ac16-3bc5-49be-900a-d9e68c776ec4 · outbound

This paper cites an unresolved cited work.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Unresolved cited work

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Observation 9ef2420b-dbbf-42d1-aef3-65c896d146ce · outbound

This paper cites Non perturbative chiral approach to s-wave \bar{K}N interactions.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Non perturbative chiral approach to s-wave \bar{K}N interactions

Reference 16

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Observation 4256d821-c33a-4b35-8313-a3d07f376b6c · outbound

This paper cites Meson-Meson interaction in a non-perturbative chiral approach.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Meson-Meson interaction in a non-perturbative chiral approach

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Observation 2cfb654f-d9d5-4161-a0bd-757e400524e6 · outbound

This paper cites Chiral unitary approach to S-wave meson baryon scattering in the strangeness S=0 sector.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Chiral unitary approach to S-wave meson baryon scattering in the strangeness S=0 sector

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Observation 1bc921a0-c66a-455e-95c0-7a3d17cd5dbc · outbound

This paper cites Chiral Dynamics of the Two \Lambda(1405) States.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Chiral Dynamics of the Two \Lambda(1405) States

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Observation aa3736c6-11ef-41fa-aec9-b410be9c8c33 · outbound

This paper cites Low lying axial-vector mesons as dynamically generated resonances.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Low lying axial-vector mesons as dynamically generated resonances

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Observation d9ebdc8b-0f75-4553-8959-7fb9df32994d · outbound

This paper cites Dynamically generated 0^+ heavy mesons in a heavy chiral unitary approach.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Dynamically generated 0^+ heavy mesons in a heavy chiral unitary approach

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Observation 8ad87070-c17d-470e-a04b-9498f91165d2 · outbound

This paper cites Unitary coupled channel analysis of the $\Lambda(1520)$ resonance.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Unitary coupled channel analysis of the $\Lambda(1520)$ resonance

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Observation 365db4f3-975b-4205-92ce-178db739ff1a · outbound

This paper cites Dynamically generated 1^+ heavy mesons.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Dynamically generated 1^+ heavy mesons

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Observation 0c7984bf-1cf5-4100-bca8-f4a7b27d63e0 · outbound

This paper cites Clues for the existence of two $K_1(1270)$ resonances.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Clues for the existence of two $K_1(1270)$ resonances

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Observation 76ab9f80-0a83-4b02-920e-c80c47b6f865 · outbound

This paper cites Dynamically Generated Open and Hidden Charm Meson Systems.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Dynamically Generated Open and Hidden Charm Meson Systems

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Observation 2ca29e14-9d96-43d0-8eba-f08b0603ff60 · outbound

This paper cites Axial Resonances in the Open and Hidden Charm Sectors.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Axial Resonances in the Open and Hidden Charm Sectors

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Observation 0ae734e0-398b-41ca-8289-2e4758c2b4bb · outbound

This paper cites The \rho\rho interaction in the hidden gauge formalism and the f_0(1370) and f_2(1270) resonances.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays The \rho\rho interaction in the hidden gauge formalism and the f_0(1370) and f_2(1270) resonances

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Observation fe0c9810-0964-460f-b61b-3604d0e624de · outbound

This paper cites Vector meson-vector meson interaction in a hidden gauge unitary approach.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Vector meson-vector meson interaction in a hidden gauge unitary approach

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Observation 0fab0228-8ea6-4fdc-b199-dc9cbe58099d · outbound

This paper cites Dynamically generated resonances from the vector octet-baryon decuplet interaction.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Dynamically generated resonances from the vector octet-baryon decuplet interaction

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Observation ce077236-31f8-4848-8ccf-7291839c171e · outbound

This paper cites Hidden beauty baryon states in the local hidden gauge approach with heavy quark spin symmetry.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Hidden beauty baryon states in the local hidden gauge approach with heavy quark spin symmetry

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Observation abf8bff9-20f6-4233-90be-56ee636c1159 · outbound

This paper cites Baryon states with open charm in the extended local hidden gauge approach.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Baryon states with open charm in the extended local hidden gauge approach

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Observation 5a17becd-73b8-4e13-ad55-2881190ba831 · outbound

This paper cites Pseudocalar meson and vector meson interactions and dynamically generated axial-vector mesons.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Pseudocalar meson and vector meson interactions and dynamically generated axial-vector mesons

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Observation 05d080d0-ddc0-4a41-b905-3d2036c9f39a · outbound

This paper cites Doubly charmed $\Xi_{cc}$ molecular states from meson-baryon interaction.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Doubly charmed $\Xi_{cc}$ molecular states from meson-baryon interaction

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Observation 49d59ef9-1dab-4475-844f-2b4a2c99983d · outbound

This paper cites Molecular $\Xi_{bc}$ states from meson-baryon interaction.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Molecular $\Xi_{bc}$ states from meson-baryon interaction

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Observation 10888006-3e67-4be9-9e52-4808e3029a2f · outbound

This paper cites The hidden strange $B_{c}$-like molecular states.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays The hidden strange $B_{c}$-like molecular states

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Observation 869fe2a2-24b9-45d3-ae16-d2d04c51dfad · outbound

This paper cites Exotic molecular meson states of $B^{()} K^{()}$ nature.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Exotic molecular meson states of $B^{(*)} K^{(*)}$ nature

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Observation 40293f3b-af83-460e-97a5-c77588789096 · outbound

This paper cites The bottomed strange molecules with isospin 0.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays The bottomed strange molecules with isospin 0

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Observation 66ef9721-ddf4-4476-b76d-16825bb0ca1f · outbound

This paper cites Charm-beauty meson bound states from $B(B^)D(D^)$ and $B(B^)\bar D(\bar D^)$ interaction.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Charm-beauty meson bound states from $B(B^*)D(D^*)$ and $B(B^*)\bar D(\bar D^*)$ interaction

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Observation 82603bad-14a9-46c7-9ae9-9d02a84d021e · outbound

This paper cites Study of $B\bar{B}^$ and $B^\bar{B}^*$ interactions in $I=1$ and relationship to the $Z_b(10610)$, $Z_b(10650)$ states.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Study of $B\bar{B}^*$ and $B^*\bar{B}^*$ interactions in $I=1$ and relationship to the $Z_b(10610)$, $Z_b(10650)$ states

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Observation ee87e35e-3ded-4ae5-bdbf-6a8f151cb9f8 · outbound

This paper cites A new interpretation for the $D^*_{s2}(2573)$ and the prediction of novel exotic charmed mesons.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays A new interpretation for the $D^*_{s2}(2573)$ and the prediction of novel exotic charmed mesons

Reference 40

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Observation ff032005-df67-4284-b283-ea1a84f54c33 · outbound

This paper cites The Y(3940), Z(3930) and the X(4160) as dynamically generated resonances from the vector-vector interaction.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays The Y(3940), Z(3930) and the X(4160) as dynamically generated resonances from the vector-vector interaction

Reference 41

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Observation 32b35ed4-fb1f-4199-a2a8-b528cd8adaf7 · outbound

This paper cites Low lying S=-1 excited baryons and chiral symmetry.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Low lying S=-1 excited baryons and chiral symmetry

Reference 42

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Observation 642139ab-a7ba-480b-9f30-bcdb62060dcd · outbound

This paper cites Baryonic Resonances from Baryon Decuplet-Meson Octet Interaction.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Baryonic Resonances from Baryon Decuplet-Meson Octet Interaction

Reference 43

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Observation e42d8851-6eb3-43d7-8a7f-c8c08cfa983d · outbound

This paper cites Study of J/Psi decays into eta Kstar Kstar-bar.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Study of J/Psi decays into eta Kstar Kstar-bar

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Observation 844e2fd7-5968-4b00-9249-3ecb86e97d40 · outbound

This paper cites Signature of an $h_1$ state in the $J/\psi \to \eta h_1 \to \eta K^{0}\bar{K}^{0}$ decay.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Signature of an $h_1$ state in the $J/\psi \to \eta h_1 \to \eta K^{*0}\bar{K}^{*0}$ decay

Reference 45

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Observation 691bbff7-808c-4880-8dd3-ee787c9bb54d · outbound

This paper cites Test of the $h_1(1830)$ made of $K^{}\bar{K}^$ with the $\eta_c\rightarrow \phi K^{}\bar{K}^{}$ decay.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Test of the $h_1(1830)$ made of $K^{*}\bar{K}^*$ with the $\eta_c\rightarrow \phi K^{*}\bar{K}^{*}$ decay

Reference 46

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Observation 8f7a6b7d-0291-46dd-9d79-1d4acfcac98e · outbound

This paper cites Hidden gauge formalism for the radiative decays of axial-vector mesons.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Hidden gauge formalism for the radiative decays of axial-vector mesons

Reference 47

Resolution: unresolved; no resolver link, observed 2026-08-03T09:32:09.394196Z

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Observation 05933c59-1554-43ee-a5ac-f92274994a2e · outbound

This paper cites Two-pole structures as a universal phenomenon dictated by coupled-channel chiral dynamics.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Two-pole structures as a universal phenomenon dictated by coupled-channel chiral dynamics

Reference 48

Resolution: unresolved; no resolver link, observed 2026-08-03T09:32:09.448536Z

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Observation d47a9476-dea1-4782-ab3f-513a6770a11f · outbound

This paper cites Xie, Z.-W.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Xie, Z.-W

Reference 49

Resolution: unresolved; no resolver link, observed 2026-08-03T09:32:09.529798Z

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Observation d32c7f68-b87e-4024-987b-f163c35f8db8 · outbound

This paper cites Quantum loops in radiative decays of the $a_1$ and $b_1$ axial-vector mesons.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Quantum loops in radiative decays of the $a_1$ and $b_1$ axial-vector mesons

Reference 50

Resolution: unresolved; no resolver link, observed 2026-08-03T09:32:09.585197Z

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Observation 83a37c5a-f1c1-4650-b68a-d6186d84c83f · outbound

This paper cites $f_1(1285)$ decays into $a_0(980)\pi^0$, $f_0(980)\pi^0$ and isospin breaking.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays $f_1(1285)$ decays into $a_0(980)\pi^0$, $f_0(980)\pi^0$ and isospin breaking

Reference 51

Resolution: unresolved; no resolver link, observed 2026-08-03T09:32:09.662057Z

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Observation 3657132d-3386-466d-ab19-6d38598026b0 · outbound

This paper cites The $K \bar K \pi$ decay of the $f_1(1285)$ and its nature as a $K^* \bar K -cc$ molecule.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays The $K \bar K \pi$ decay of the $f_1(1285)$ and its nature as a $K^* \bar K -cc$ molecule

Reference 52

Resolution: unresolved; no resolver link, observed 2026-08-03T09:32:09.744272Z

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Observation a407a7c9-1fe9-457b-97e1-ae9cc5c962ee · outbound

This paper cites The $K^- p \to f_1(1285) \Lambda$ reaction within an effective Lagrangian approach.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays The $K^- p \to f_1(1285) \Lambda$ reaction within an effective Lagrangian approach

Reference 53

Resolution: unresolved; no resolver link, observed 2026-08-03T09:32:09.827309Z

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Observation f46cfe69-db0a-40c3-a3ca-c6058ca76b10 · outbound

This paper cites The $\pi f_0(500)$ decay of the $a_1(1260)$.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays The $\pi f_0(500)$ decay of the $a_1(1260)$

Reference 54

Resolution: unresolved; no resolver link, observed 2026-08-03T09:32:09.886960Z

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Observation 6b2f11c3-5b3e-440c-9d17-654b1fab2141 · outbound

This paper cites Strong decays of $a_0$, $f_0$, $f_2$, and $K^*_2$ resonances as dynamically generated states of two vector mesons.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Strong decays of $a_0$, $f_0$, $f_2$, and $K^*_2$ resonances as dynamically generated states of two vector mesons

Reference 55

Resolution: unresolved; no resolver link, observed 2026-08-03T09:32:09.963908Z

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Observation e0e178c1-1cc3-4797-bc9c-9a25b532df16 · outbound

This paper cites A chiral covariant approach to $\rho\rho$ scattering.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays A chiral covariant approach to $\rho\rho$ scattering

Reference 56

Resolution: unresolved; no resolver link, observed 2026-08-03T09:32:10.044753Z

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Observation 9e2663db-11e7-4597-b1b7-dcdc5657d687 · outbound

This paper cites Further study of $f_0(1710)$ with coupled-channel approach and hadron molecular picture.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Further study of $f_0(1710)$ with coupled-channel approach and hadron molecular picture

Reference 57

Resolution: unresolved; no resolver link, observed 2026-08-03T09:32:10.126903Z

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Observation 1512d6a0-60bb-4c23-bb98-d8df458ec92a · outbound

This paper cites Two dynamical generated $a_0$ resonances by interactions between vector mesons.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Two dynamical generated $a_0$ resonances by interactions between vector mesons

Reference 58

Resolution: unresolved; no resolver link, observed 2026-08-03T09:32:10.243005Z

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Observation 13eaeda3-9393-4cbe-a4dc-a7a799521bdd · outbound

This paper cites Production of \phi Mesons in Near-Threshold \pi N and N N Reactions.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Production of \phi Mesons in Near-Threshold \pi N and N N Reactions

Reference 59

Resolution: unresolved; no resolver link, observed 2026-08-03T09:32:10.303243Z

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Observation c3352764-7942-4e27-9b45-b9a1df02e667 · outbound

This paper cites Production of $\omega$ and $\phi$ Mesons in Near-Threshold $\pi N$ Reactions: Baryon Resonances and Validity of the OZI Rule.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Production of $\omega$ and $\phi$ Mesons in Near-Threshold $\pi N$ Reactions: Baryon Resonances and Validity of the OZI Rule

Reference 60

Resolution: unresolved; no resolver link, observed 2026-08-03T09:32:10.371248Z

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Observation 262e51aa-7ccd-45dc-a04e-6e1dbc190f23 · outbound

This paper cites Tau decay into $\nu_\tau$ and $a_1(1260)$, $b_1(1235)$, and two $K_1(1270)$.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Tau decay into $\nu_\tau$ and $a_1(1260)$, $b_1(1235)$, and two $K_1(1270)$

Reference 61

Resolution: unresolved; no resolver link, observed 2026-08-03T09:32:10.431126Z

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Observation f5b0062a-87f9-4fa1-8472-e4a39b34d9ec · outbound

This paper cites Hadronic molecular states from the $K\bar{K}^*$ interaction.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Hadronic molecular states from the $K\bar{K}^*$ interaction

Reference 62

Resolution: unresolved; no resolver link, observed 2026-08-03T09:32:10.600242Z

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Observation fd8204d8-c9b8-4bf0-8adf-318d3f64d8e1 · outbound

This paper cites $\tau$ decay into a pseudoscalar and an axial-vector meson.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays $\tau$ decay into a pseudoscalar and an axial-vector meson

Reference 63

Resolution: unresolved; no resolver link, observed 2026-08-03T09:32:10.770581Z

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Observation 008b1a6a-5c00-4a4f-92dd-5709de62899e · outbound

This paper cites Theoretical study of the $\Omega(2012)$ state in the $\Omega_c^0 \to \pi^+ \Omega(2012)^- \to \pi^+ (\bar{K}\Xi)^-$ and $\pi^+ (\bar{K}\Xi\pi)^-$ decays.

The dynamically generated $h_1$ state by the $K^*\bar{K}^*$ interaction and its $K_1(1270)\bar{K}$ and $b_1(1235)\pi$ decays Theoretical study of the $\Omega(2012)$ state in the $\Omega_c^0 \to \pi^+ \Omega(2012)^- \to \pi^+ (\bar{K}\Xi)^-$ and $\pi^+ (\bar{K}\Xi\pi)^-$ decays

Reference 64

Resolution: unresolved; no resolver link, observed 2026-08-03T09:32:10.986389Z

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