1994 Summary Table Index in Alphabetic Order
(See also this same index in
book order.)
- a(0)(980)
- a(1)(1260)
- a(2)(1320)
- b bbar MESONS
- b(1)(1235)
- B(s)0
- B*
- B+-
- B0
- b (quark)
- BOTTOM (BEAUTY) BARYON (B = -1)
- BOTTOM MESONS (B = +-1)
- BOTTOM, STRANGE MESONS (B = +-1, S = -+1)
- c cbar MESONS
- c (quark)
- CHARMED BARYONS (C = +1)
- CHARMED MESONS (C = +-1)
- CHARMED, STRANGE MESONS (C = S = +-1)
- chi(b0)(1P) [or chi(b0)(9860)]
- chi(b0)(2P) [or chi(b0)(10235)]
- chi(b1)(1P) [or chi(b1)(9890)]
- chi(b1)(2P) [or chi(b1)(10255)]
- chi(b2)(1P) [or chi(b2)(9915)]
- chi(b2)(2P) [or chi(b2)(10270)]
- chi(c0)(1P) [or chi(c0)(3415)]
- chi(c1)(1P) [or chi(c1)(3510)]
- chi(c2)(1P) [or chi(c2)(3555)]
- D(1)(2420)0
- D(2)*(2460)
- D(s)*+-
- D(s)+-
- D(s1)(2536)+-
- D*(2007)0
- D*(2010)+-
- D+-
- D0
- d (quark)
- Delta BARYONS (S = 0, I = 3/2)
- Delta(1232) P(33)
- Delta(1600) P(33)
- Delta(1620) S(31)
- Delta(1700) D(33)
- Delta(1900) S(31)
- Delta(1905) F(35)
- Delta(1910) P(31)
- Delta(1920) P(33)
- Delta(1930) D(35)
- Delta(1950) F(37)
- Delta(2420) H(3,11)
- e
- eta'(958)
- eta(1295)
- eta(1440)
- eta(c)(1S) [or eta(c)(2980)]
- eta
- f(0)(1300)
- f(0)(1590)
- f(0)(980)
- f(1)(1285)
- f(1)(1420)
- f(1)(1510)
- f(2)'(1525)
- f(2)(1270)
- f(2)(2010)
- f(2)(2300)
- f(2)(2340)
- f(4)(2050)
- f(J)(1710)
- Free Quark Searches
- g [or gluon]
- gamma
- GAUGE AND HIGGS BOSONS
- h(1)(1170)
- Heavy Lepton Searches
- J/psi(1S) [or J/psi(3097)]
- K(0)*(1430)
- K(1)(1270)
- K(1)(1400)
- K(2)(1770)
- K(2)(1820)
- K(2)*(1430)
- K(3)*(1780)
- K(4)*(2045)
- K(L)0
- K(S)0
- K*(1410)
- K*(1680)
- K*(892)
- K+-
- K0
- Lambda BARYONS (S = -1, I = 0)
- Lambda(1405) S(01)
- Lambda(1520) D(03)
- Lambda(1600) P(01)
- Lambda(1670) S(01)
- Lambda(1690) D(03)
- Lambda(1800) S(01)
- Lambda(1810) P(01)
- Lambda(1820) F(05)
- Lambda(1830) D(05)
- Lambda(1890) P(03)
- Lambda(2100) G(07)
- Lambda(2110) F(05)
- Lambda(2350) H(09)
- Lambda(b)0
- Lambda(c)(2625)+
- Lambda(c)+
- Lambda
- LEPTONS
- LIGHT UNFLAVORED MESONS (S = C = B = 0)
- Magnetic Monopole Searches
- mu
- N BARYONS (S = 0, I = 1/2)
- N(1440) P(11)
- N(1520) D(13)
- N(1535) S(11)
- N(1650) S(11)
- N(1675) D(15)
- N(1680) F(15)
- N(1700) D(13)
- N(1710) P(11)
- N(1720) P(13)
- N(2190) G(17)
- N(2220) H(19)
- N(2250) G(19)
- N(2600) I(1,11)
- n (neutron)
- Neutrinos
- nu(e)
- nu(mu)
- nu(tau)
- Number of Light Neutrino Types
- Omega BARYONS (S = -3, I = 0)
- omega(1420)
- omega(1600)
- Omega(2250)-
- omega(3)(1670)
- omega(782)
- Omega-
- p (proton)
- phi(1020)
- phi(1680)
- phi(3)(1850)
- pi(1300)
- pi(2)(1670)
- pi+-
- pi0
- psi(2S) [or psi(3685)]
- psi(3770)
- psi(4040)
- psi(4160)
- psi(4415)
- QUARKS
- rho(1450)
- rho(1700)
- rho(3)(1690)
- rho(770)
- s (quark)
- Searches for Axions (A0) and Other Very Light Bosons
- Searches for b' (4**th Generation) Quark
- SEARCHES FOR FREE QUARKS, MONOPOLES, SUPERSYMMETRY, COMPOSITENESS, etc.
- Searches for Heavy Bosons Other Than Higgs Bosons
- Searches for Higgs Bosons --- H0 and H+-
- Searches for Massive Neutrinos and Lepton Mixing
- Searches for Quark and Lepton Compositeness
- Searches for t Quark
- Sigma BARYONS (S = -1, I = 1)
- Sigma(1385) P(13)
- Sigma(1660) P(11)
- Sigma(1670) D(13)
- Sigma(1750) S(11)
- Sigma(1775) D(15)
- Sigma(1915) F(15)
- Sigma(1940) D(13)
- Sigma(2030) F(17)
- Sigma(2250)
- Sigma(c)(2455)
- Sigma+
- Sigma-
- Sigma0
- STRANGE MESONS (S = +-1, C = B = 0)
- Supersymmetric Particle Searches
- tau
- u (quark)
- Upsilon(10860)
- Upsilon(11020)
- Upsilon(1S) [or Upsilon(9460)]
- Upsilon(2S) [or Upsilon(10023)]
- Upsilon(3S) [or Upsilon(10355)]
- Upsilon(4S) [or Upsilon(10580)]
- W
- Xi BARYONS (S = -2, I = 1/2)
- Xi(1530) P(13)
- Xi(1690)
- Xi(1820) D(13)
- Xi(1950)
- Xi(2030)
- Xi(c)+
- Xi(c)0
- Xi-
- Xi0
- Z
Go to
Table of Contents, Review of Particle Properties.
Betty Armstrong
27-APR-1995