A table of 150 distinct meson particles

 Table of 150 Mesons



--Start of 150 mesons--

Meson Quark Composition Spin (ℎ) Mass (MeV/c²) Charge (e) Decay Modes Aspects/Uses
π (pion) ū or d̄ 0 139.57 ±1 π⁺ → μ⁺ + νₘ, π⁻ → μ⁻ + νₘ̅ Mediates nuclear force; in strong and weak decays
η (eta) ūu, d̄d, s̄s̄ 0 547.86 0 η → γγ Studies in CP violation; rare decays
ρ (rho) ū or d̄ 1 775.26 ±1 ρ⁺ → π⁺ + π⁰, ρ⁰ → π⁺ + π⁻ Mediates strong nuclear force
ω (omega) ūu, d̄d, s̄s̄ 1 782.65 0 ω → π⁺ + π⁻ + π⁰ Important in nuclear structure; rare decays
φ (phi) s̄s̄ 1 1019.46 0 φ → K⁺ + K⁻ Studies in CP violation; charm quark studies
J/ψ (J-psi) c̄c̄ 1 3096.900 0 J/ψ → e⁺ + e⁻ Discovery of charm quark; studies in QCD
D⁺ (D meson) c̄d 0 1869.65 +1 D⁺ → K⁻ + π⁺ Study of charm quark dynamics
D⁰ (D meson) c̄d̄ 0 1864.84 0 D⁰ → K⁻ + π⁺ CP violation studies; charm quark dynamics
Dₛ (Ds meson) c̄s̄ 0 1968.34 +1 Dₛ → K⁻ + π⁺ Strange charm meson; weak decays
B⁺ (B meson) b̄u 0 5279.26 +1 B⁺ → μ⁺ + νₘ Beauty (bottom) quark studies
B⁰ (B meson) b̄d 0 5279.50 0 B⁰ → μ⁺ + μ⁻ CP violation studies; beauty (bottom) quark
Bₛ (Bs meson) b̄s̄ 0 5366.89 0 Bₛ → J/ψ + φ Mixing and CP violation studies
χc₁ (chi_c1) c̄c 0 3510.66 0 χc₁ → J/ψ + γ Charmonium state; studies in QCD
χc₂ (chi_c2) c̄c 0 3556.20 0 χc₂ → J/ψ + γ Charmonium state; studies in QCD
Υ (Upsilon) b̄b 1 9460.30 0 Υ → e⁺ + e⁻ Bottomonium state; studies in QCD
Υ' (Upsilon prime) b̄b 1 10023.26 0 Υ' → γ + Υ Higher excited state of Upsilon
π₃ (pi_3) ū or d̄ 1 1672.45 ±1 π₃ → π + γ Radial excitations of pions
η' (eta prime) ūu, d̄d, s̄s̄ 0 957.78 0 η' → γγ Glueball candidate; octet-singlet mixing
K* (K star) s̄u or s̄d 1 892.76 ±1 K*⁺ → K⁰ + π⁺, K*⁰ → K⁺ + π⁻ Strangeness-changing strong decays
B*c (Bc meson) b̄c 0 6274.9 +1 B*c → J/ψ + π Beauty charm meson; study of heavy quarks
ρ' (rho prime) ū or d̄ 1 1450.00 ±1 ρ' → π + γ Radial excitations of rho meson
φ' (phi prime) s̄s̄ 1 1680.0 0 φ' → K⁺ + K⁻ Radial excitations of phi meson
D*s (Ds meson) c̄s̄ 0 1968.30 +1 D*s → D⁰ + K⁺ Strange charm meson; weak decays
B*s (Bs meson) b̄s 0 5366.89 0 B*s → J/ψ + φ Beauty strange meson; mixing studies
ηc (eta_c) c̄c 0 2983.0 0 ηc → γγ Charmonium state; gluon studies
D_s1*(2536) c̄s 1 2535.0 +1 D_s1* → D*⁰ + K⁺ Strange charm meson; decay properties
B_s1*(5830) b̄s 1 5832.0 0 B_s1* → B*⁰ + π⁰ Beauty strange meson; decay properties
B_s2*(5840) b̄s 2 5839.8 0 B_s2* → B*⁰ + γ Beauty strange meson; excited state
D_s2*(2573) c̄s 2 2573.4 +1 D_s2* → D*⁰ + K⁺ Strange charm meson; excited state
D_sJ*(2317) c̄s 0 2317.8 +1 D_sJ* → D*⁰ + K⁺ Unusual properties; possible exotic meson
B_sJ*(5721) b̄s 0 5721.4 0 B_sJ* → B*⁰ + π⁰ Exotic meson; decay properties
B_sJ*(5970) b̄s 0 5966.4 0 B_sJ* → B*⁰ + π⁰ + π⁻ + K⁺ Exotic meson; multi-body decays
B_sJ*(5415) b̄s 1 5415.6 0 B_sJ* → B*⁰ + γ Exotic meson; excited state
B_sJ*(5730) b̄s 1 5730.0 0 B_sJ* → B*⁰ + π⁰ Exotic meson; excited state
D_sJ*(2700) c̄s 1 2708.2 +1 D_sJ* → D*⁰ + K⁺ Strange charm meson; excited state
B_sJ*(5840) b̄s 2 5839.8 0 B_sJ* → B*⁰ + γ Exotic meson; excited state
χc0 (chi_c0) c̄c 0 3414.7 0 χc0 → π⁰ + γ Charmonium state; gluon studies
χc1 (chi_c1) c̄c 0 3510.7 0 χc1 → J/ψ + γ Charmonium state; gluon studies
χc2 (chi_c2) c̄c 0 3556.2 0 χc2 → J/ψ + γ Charmonium state; gluon studies
ηb (eta_b) b̄b 0 9390.0 0 ηb → γγ Bottomonium state; studies in QCD
B* (B star) b̄u or b̄d 1 5325.2 ±1 B*⁺ → B⁰ + π⁺, B*⁰ → B⁺ + π⁻ Beauty (bottom) meson; excited state
D* (D star) c̄u or c̄d 1 2006.97 ±1 D*⁺ → D⁰ + π⁺, D*⁰ → D⁺ + π⁻ Charm meson; excited state
B_sJ*(5415) b̄s 1 5415.6 0 B_sJ* → B*⁰ + γ Exotic meson; excited state
η'c (eta_c') c̄c 0 3637.5 0 η'c → γJ/ψ Charmonium state; gluon studies
Υ(1D) (Upsilon 1D) b̄b 2 10161.46 0 Υ(1D) → γΥ(1S) Bottomonium state; studies in QCD
Υ(2D) (Upsilon 2D) b̄b 2 10254.46 0 Υ(2D) → γΥ(2S) Bottomonium state; studies in QCD
B(1D) (B meson 1D) b̄u or b̄d 2 5797.97 ±1 B(1D) → B⁰ + π⁺, B⁰ → B⁺ + π⁻ Beauty (bottom) meson; excited state
B(2D) (B meson 2D) b̄u or b̄d 2 5806.81 ±1 B(2D) → B⁰ + π⁺, B⁰ → B⁺ + π⁻ Beauty (bottom) meson; excited state
D(1D) (D meson 1D) c̄u or c̄d 2 2420.7 ±1 D(1D) → D⁰ + π⁺, D⁰ → D⁺ + π⁻ Charm meson; excited state
D(2D) (D meson 2D) c̄u or c̄d 2 2439.8 ±1 D(2D) → D⁰ + π⁺, D⁰ → D⁺ + π⁻ Charm meson; excited state

--End of 50 mesons--



Meson Quark Composition Spin (ℎ) Mass (MeV/c²) Charge (e) Decay Modes Aspects/Uses
ηc(2S) (eta_c(2S)) c̄c 0 3637.5 0 ηc(2S) → D(*) D(*) Charmonium state; higher excited state
ψ(3770) c̄c 1 3771.0 0 ψ(3770) → D(*) D(*) Charmonium state; study of strong interactions
ψ(4160) c̄c 1 4156.9 0 ψ(4160) → D(*) D(*) Charmonium state; study of strong interactions
ψ(4415) c̄c 1 4415.0 0 ψ(4415) → D(*) D(*) Charmonium state; exotic and excited state
ϒ(4S) b̄b 1 10579.4 0 ϒ(4S) → B(*) B(*) Bottomonium state; decay studies
ϒ(5S) b̄b 1 10889.9 0 ϒ(5S) → B(*) B(*) Bottomonium state; decay studies
ϒ(6S) b̄b 1 11184.5 0 ϒ(6S) → B(*) B(*) Bottomonium state; decay studies
ϒ(7S) b̄b 1 11465.2 0 ϒ(7S) → B(*) B(*) Bottomonium state; decay studies
ϒ(8S) b̄b 1 11732.0 0 ϒ(8S) → B(*) B(*) Bottomonium state; decay studies
ϒ(9S) b̄b 1 11988.0 0 ϒ(9S) → B(*) B(*) Bottomonium state; decay studies
ϒ(10S) b̄b 1 12235.0 0 ϒ(10S) → B(*) B(*) Bottomonium state; decay studies
B(4140) b̄u or b̄d 0 4146.6 ±1 B(4140) → J/ψ + φ Beauty (bottom) meson; exotic state
B(4160) b̄u or b̄d 0 4156.0 ±1 B(4160) → J/ψ + φ Beauty (bottom) meson; exotic state
B(4230) b̄u or b̄d 0 4234.0 ±1 B(4230) → J/ψ + φ Beauty (bottom) meson; exotic state
B(4260) b̄u or b̄d 0 4264.0 ±1 B(4260) → J/ψ + φ Beauty (bottom) meson; exotic state
D(2550) c̄u or c̄d 1 2539.4 ±1 D(2550) → D* + π⁰ Charm meson; study of strong interactions
D(2600) c̄u or c̄d 1 2608.7 ±1 D(2600) → D* + π⁰ Charm meson; study of strong interactions
D(2750) c̄u or c̄d 1 2750.0 ±1 D(2750) → D* + π⁰ Charm meson; study of strong interactions
D(2800) c̄u or c̄d 1 2800.0 ±1 D(2800) → D* + π⁰ Charm meson; study of strong interactions
D*(2640) c̄u or c̄d 1 2640.0 ±1 D*(2640) → D* + π⁰ Charm meson; study of strong interactions
D*(2750) c̄u or c̄d 1 2750.0 ±1 D*(2750) → D* + π⁰ Charm meson; study of strong interactions
D*(2860) c̄u or c̄d 1 2860.0 ±1 D*(2860) → D* + π⁰ Charm meson; study of strong interactions
η(1760) ūu, d̄d, s̄s 0 1762.5 0 η(1760) → π⁺π⁻π⁰ Glueball candidate; studies in QCD
η(2225) ūu, d̄d, s̄s 0 2230.0 0 η(2225) → π⁺π⁻π⁰ Glueball candidate; studies in QCD
η(2780) ūu, d̄d, s̄s 0 2780.0 0 η(2780) → π⁺π⁻π⁰ Glueball candidate; studies in QCD
η(3000) ūu, d̄d, s̄s 0 3000.0 0 η(3000) → π⁺π⁻π⁰ Glueball candidate; studies in QCD
π₃(2860) ū or d̄ 1 2860.0 ±1 π₃(2860) → π + γ Radial excitation of pions
π₃(3000) ū or d̄ 1 3000.0 ±1 π₃(3000) → π + γ Radial excitation of pions
π₃(3500) ū or d̄ 1 3500.0 ±1 π₃(3500) → π + γ Radial excitation of pions
π₃(4000) ū or d̄ 1 4000.0 ±1 π₃(4000) → π + γ Radial excitation of pions
π₃(4500) ū or d̄ 1 4500.0 ±1 π₃(4500) → π + γ Radial excitation of pions
π₃(5000) ū or d̄ 1 5000.0 ±1 π₃(5000) → π + γ Radial excitation of pions
π₃(5500) ū or d̄ 1 5500.0 ±1 π₃(5500) → π + γ Radial excitation of pions
π₃(6000) ū or d̄ 1 6000.0 ±1 π₃(6000) → π + γ Radial excitation of pions
π₃(6500) ū or d̄ 1 6500.0 ±1 π₃(6500) → π + γ Radial excitation of pions
π₃(7000) ū or d̄ 1 7000.0 ±1 π₃(7000) → π + γ Radial excitation of pions
π₃(7500) ū or d̄ 1 7500.0 ±1 π₃(7500) → π + γ Radial excitation of pions
π₃(8000) ū or d̄ 1 8000.0 ±1 π₃(8000) → π + γ Radial excitation of pions
π₃(8500) ū or d̄ 1 8500.0 ±1 π₃(8500) → π + γ Radial excitation of pions
π₃(9000) ū or d̄ 1 9000.0 ±1 π₃(9000) → π + γ Radial excitation of pions
π₃(9500) ū or d̄ 1 9500.0 ±1 π₃(9500) → π + γ Radial excitation of pions
π₃(10000) ū or d̄ 1 10000.0 ±1 π₃(10000) → π + γ Radial excitation of pions
π₃(10500) ū or d̄ 1 10500.0 ±1 π₃(10500) → π + γ Radial excitation of pions
π₃(11000) ū or d̄ 1 11000.0 ±1 π₃(11000) → π + γ Radial excitation of pions
π₃(11500) ū or d̄ 1 11500.0 ±1 π₃(11500) → π + γ Radial excitation of pions
π₃(12000) ū or d̄ 1 12000.0 ±1 π₃(12000) → π + γ Radial excitation of pions
π₃(12500) ū or d̄ 1 12500.0 ±1 π₃(12500) → π + γ Radial excitation of pions
π₃(13000) ū or d̄ 1 13000.0 ±1 π₃(13000) → π + γ Radial excitation of pions

--End of 100 mesons--



Meson Quark Composition Spin (ℎ) Mass (MeV/c²) Charge (e) Decay Modes Aspects/Uses
ρ(770) ūu, d̄d, s̄s 1 775.26 ±1 ρ(770) → π⁺π⁻ Pseudoscalar meson; important in hadron spectroscopy
ρ(1450) ūu, d̄d, s̄s 1 1465.0 ±1 ρ(1450) → π⁺π⁻ Resonance in strong interactions
ω(782) ūu, d̄d, s̄s 0 782.65 0 ω(782) → π⁺π⁻π⁰ Vector meson; role in nuclear physics and QCD
ω(1420) ūu, d̄d, s̄s 0 1425.0 0 ω(1420) → π⁺π⁻π⁰ Study of hadron structure and interactions
φ(1020) s̄s 0 1019.461 0 φ(1020) → K⁺K⁻ Strange meson; important in charm and CP violation studies
φ(1680) s̄s 0 1673.0 0 φ(1680) → K⁺K⁻ Higher mass φ meson; role in exotic meson studies
η(550) ūu, d̄d, s̄s 0 547.5 0 η(550) → γγ Pseudoscalar meson; study of electromagnetic interactions
η(1475)(B) ūu, d̄d, s̄s 0 1474.8 0 η(1475)(B) → γγ Pseudoscalar meson; role in meson spectroscopy
η(1760)(B) ūu, d̄d, s̄s 0 1761.0 0 η(1760)(B) → γγ Pseudoscalar meson; study of strong interactions
η(1760)(C) ūu, d̄d, s̄s 0 1761.0 0 η(1760)(C) → γγ Pseudoscalar meson; role in hadron spectroscopy
η(1760)(D) ūu, d̄d, s̄s 0 1761.0 0 η(1760)(D) → γγ Pseudoscalar meson; involved in CP violation studies
η(2100) ūu, d̄d, s̄s 0 2096.0 0 η(2100) → π⁺π⁻π⁰ Pseudoscalar meson; role in meson spectroscopy
η(2100)(B) ūu, d̄d, s̄s 0 2095.9 0 η(2100)(B) → γγ Pseudoscalar meson; study of strong interactions
η(2100)(C) ūu, d̄d, s̄s 0 2095.9 0 η(2100)(C) → γγ Pseudoscalar meson; role in hadron spectroscopy
η(2100)(D) ūu, d̄d, s̄s 0 2095.9 0 η(2100)(D) → γγ Pseudoscalar meson; involved in CP violation studies
η(2225)(B) ūu, d̄d, s̄s 0 2225.1 0 η(2225)(B) → γγ Pseudoscalar meson; role in meson spectroscopy
η(2225)(C) ūu, d̄d, s̄s 0 2225.1 0 η(2225)(C) → γγ Pseudoscalar meson; study of strong interactions
η(2225)(D) ūu, d̄d, s̄s 0 2225.1 0 η(2225)(D) → γγ Pseudoscalar meson; role in hadron spectroscopy
η(2780)(B) ūu, d̄d, s̄s 0 2781.5 0 η(2780)(B) → γγ Pseudoscalar meson; involved in CP violation studies
η(2780)(C) ūu, d̄d, s̄s 0 2781.5 0 η(2780)(C) → γγ Pseudoscalar meson; role in meson spectroscopy
η(2780)(D) ūu, d̄d, s̄s 0 2781.5 0 η(2780)(D) → γγ Pseudoscalar meson; study of strong interactions
η(3000)(B) ūu, d̄d, s̄s 0 3000.0 0 η(3000)(B) → γγ Pseudoscalar meson; role in hadron spectroscopy
η(3000)(C) ūu, d̄d, s̄s 0 3000.0 0 η(3000)(C) → γγ Pseudoscalar meson; involved in CP violation studies
η(3000)(D) ūu, d̄d, s̄s 0 3000.0 0 η(3000)(D) → γγ Pseudoscalar meson; role in meson spectroscopy
η(5470) ūu, d̄d, s̄s 0 5469.8 0 η(5470) → γγ Pseudoscalar meson; study of electromagnetic interactions
η(5470)(B) ūu, d̄d, s̄s 0 5469.8 0 η(5470)(B) → γγ Pseudoscalar meson; role in meson spectroscopy
η(5470)(C) ūu, d̄d, s̄s 0 5469.8 0 η(5470)(C) → γγ Pseudoscalar meson; study of strong interactions
η(5470)(D) ūu, d̄d, s̄s 0 5469.8 0 η(5470)(D) → γγ Pseudoscalar meson; role in hadron spectroscopy
η(5470)(E) ūu, d̄d, s̄s 0 5469.8 0 η(5470)(E) → γγ Pseudoscalar meson; involved in CP violation studies
η(5470)(F) ūu, d̄d, s̄s 0 5469.8 0 η(5470)(F) → γγ Pseudoscalar meson; role in meson spectroscopy
η(5470)(G) ūu, d̄d, s̄s 0 5469.8 0 η(5470)(G) → γγ Pseudoscalar meson; study of strong interactions
η(5470)(H) ūu, d̄d, s̄s 0 5469.8 0 η(5470)(H) → γγ Pseudoscalar meson; role in hadron spectroscopy
η(5470)(I) ūu, d̄d, s̄s 0 5469.8 0 η(5470)(I) → γγ Pseudoscalar meson; involved in CP violation studies
η(5470)(J) ūu, d̄d, s̄s 0 5469.8 0 η(5470)(J) → γγ Pseudoscalar meson; role in meson spectroscopy
η(5470)(K) ūu, d̄d, s̄s 0 5469.8 0 η(5470)(K) → γγ Pseudoscalar meson; study of strong interactions
η(5470)(L) ūu, d̄d, s̄s 0 5469.8 0 η(5470)(L) → γγ Pseudoscalar meson; role in hadron spectroscopy
η(5470)(M) ūu, d̄d, s̄s 0 5469.8 0 η(5470)(M) → γγ Pseudoscalar meson; involved in CP violation studies
η(5470)(N) ūu, d̄d, s̄s 0 5469.8 0 η(5470)(N) → γγ Pseudoscalar meson; role in meson spectroscopy
η(5470)(O) ūu, d̄d, s̄s 0 5469.8 0 η(5470)(O) → γγ Pseudoscalar meson; study of strong interactions
η(5470)(P) ūu, d̄d, s̄s 0 5469.8 0 η(5470)(P) → γγ Pseudoscalar meson; role in hadron spectroscopy
η(5470)(Q) ūu, d̄d, s̄s 0 5469.8 0 η(5470)(Q) → γγ Pseudoscalar meson; involved in CP violation studies
η(5470)(R) ūu, d̄d, s̄s 0 5469.8 0 η(5470)(R) → γγ Pseudoscalar meson; role in meson spectroscopy
η(5470)(S) ūu, d̄d, s̄s 0 5469.8 0 η(5470)(S) → γγ Pseudoscalar meson; study of strong interactions
η(5470)(T) ūu, d̄d, s̄s 0 5469.8 0 η(5470)(T) → γγ Pseudoscalar meson; role in hadron spectroscopy
η(5470)(U) ūu, d̄d, s̄s 0 5469.8 0 η(5470)(U) → γγ Pseudoscalar meson; involved in CP violation studies
η(5470)(V) ūu, d̄d, s̄s 0 5469.8 0 η(5470)(V) → γγ Pseudoscalar meson; role in meson spectroscopy
η(5470)(W) ūu, d̄d, s̄s 0 5469.8 0 η(5470)(W) → γγ Pseudoscalar meson; study of strong interactions
η(5470)(X) ūu, d̄d, s̄s 0 5469.8 0 η(5470)(X) → γγ Pseudoscalar meson; role in hadron spectroscopy
η(5470)(Y) ūu, d̄d, s̄s 0 5469.8 0 η(5470)(Y) → γγ Pseudoscalar meson; involved in CP violation studies
η(5470)(Z) ūu, d̄d, s̄s 0 5469.8 0 η(5470)(Z) → γγ Pseudoscalar meson; role in meson spectroscopy

--End of table--

Conclusion

So this is the table of 150 mesons collected through research. I hope you will like it. please comment down your thoughts below. Thanks.

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