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51. Search for a heavy vector resonance decaying to a $${\mathrm{Z}}_{\mathrm{}}^{\mathrm{}}$$ <math> <msubsup> <mi>Z</mi> <mrow> <mrow></mrow> </mrow> <mrow></mrow> </msubsup> </math> boson and a Higgs boson in proton-proton collisions at $$\sqrt{s} = 13\,\text {Te}\text {V} $$ <math> <mrow> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> <mspace width='0.166667em'></mspace> <mrow> <mtext>Te</mtext> <mspace width='0.333333em'></mspace> </mrow> </mrow> </math>

52. Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at √s=13Te

53. Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at √s = 13 TeV

54. Search for a heavy vector resonance decaying to a \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${\mathrm{Z}}_{\mathrm{}}^{\mathrm{}}$$\end{document}Z boson and a Higgs boson in proton-proton collisions at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\sqrt{s} = 13\,\text {Te}\text {V} $$\end{document}s=13Te

55. Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at √s=13TeV

56. On the transition form factors of the axial-vector resonance f1(1285) and its decay into e+e−

58. On the transition form factors of the axial-vector resonance f1(1285) and its decay into e+e−.

59. Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at s√=13TeV

60. The LHC mass limits for the $SU(2)_{L+R}$ vector resonance triplet of a strong extension of the Standard model

61. Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at root s=13 TeV

62. Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at s√=13TeV

63. Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at root s=13 TeV

64. Search For A Heavy Vector Resonance Decaying To A Z Boson And A Higgs Boson İn Proton-Proton Collisions At √S = 13 Tev

65. Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at sqrt(s) = 13 TeV

66. Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at s=13 Te

67. Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at $\sqrt{s} = $ 13 TeV

68. Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at √s = 13TeV

69. Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at s=13 Te

70. Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at √s=13Te

71. Modelling top partner-vector resonance phenomenology

74. Nature Of The Vector Resonance $Y\Left(2175\Right)$

75. Nature of the vector resonance Y(2175)

79. Vector resonance X1(2900) and its structure

80. Two-photon production of vector resonance in e + e − collisions

83. Precision spectroscopy with COMPASS and the observation of a new iso-vector resonance

84. A Dark Vector Resonance at CLIC

85. THE LHC MASS LIMITS FOR THE SU(2)L+R VECTOR RESONANCE TRIPLET OF A STRONG EXTENSION OF THE STANDARD MODEL.

86. Vector-resonance-multimode instability

87. Vector-Resonance-Multimode Instability.

88. Inert two-Higgs-doublet model strongly coupled to a non-Abelian vector resonance

89. Rogue waves and mode locking driven by Vector Resonance Multimode instability

90. LHC vector resonance searches in the $t\bar{t} Z$ final state

96. Digital controller design based on APF's vector resonance control

98. Combined analysis of Z′→tt¯ and Z′→tt¯j production for vector resonance searches at LHC

100. Peak Locations and Relative Phase of Different Decay Modes of thea1Axial Vector Resonance in Diffractive Production

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