1994 Summary Table Index

(See also this same index in alphabetical order.)

GAUGE AND HIGGS BOSONS

gamma

g [or gluon]

W

Z

Searches for Higgs Bosons --- H0 and H+-

Searches for Heavy Bosons Other Than Higgs Bosons

Searches for Axions (A0) and Other Very Light Bosons

LEPTONS

Neutrinos

nu(e)

nu(mu)

nu(tau)

e

mu

tau

Number of Light Neutrino Types

Heavy Lepton Searches

Searches for Massive Neutrinos and Lepton Mixing

QUARKS

u

d

s

c

b

Searches for t Quark

Searches for b' (4**th Generation) Quark

LIGHT UNFLAVORED MESONS (S = C = B = 0)

pi+-

pi0

eta

rho(770)

omega(782)

eta'(958)

f(0)(980)

a(0)(980)

phi(1020)

h(1)(1170)

b(1)(1235)

a(1)(1260)

f(2)(1270)

f(1)(1285)

eta(1295)

f(0)(1300)

pi(1300)

a(2)(1320)

f(1)(1420)

omega(1420)

eta(1440)

rho(1450)

f(1)(1510)

f(2)'(1525)

f(0)(1590)

omega(1600)

omega(3)(1670)

pi(2)(1670)

phi(1680)

rho(3)(1690)

rho(1700)

f(J)(1710)

phi(3)(1850)

f(2)(2010)

f(4)(2050)

f(2)(2300)

f(2)(2340)

STRANGE MESONS (S = +-1, C = B = 0)

K+-

K0

K(S)0

K(L)0

K*(892)

K(1)(1270)

K(1)(1400)

K*(1410)

K(0)*(1430)

K(2)*(1430)

K*(1680)

K(2)(1770)

K(3)*(1780)

K(2)(1820)

K(4)*(2045)

CHARMED MESONS (C = +-1)

D+-

D0

D*(2007)0

D*(2010)+-

D(1)(2420)0

D(2)*(2460)

CHARMED, STRANGE MESONS (C = S = +-1)

D(s)+-

D(s)*+-

D(s1)(2536)+-

BOTTOM MESONS (B = +-1)

B+-

B0

B*

BOTTOM, STRANGE MESONS (B = +-1, S = -+1)

B(s)0

c cbar MESONS

eta(c)(1S) [or eta(c)(2980)]

J/psi(1S) [or J/psi(3097)]

chi(c0)(1P) [or chi(c0)(3415)]

chi(c1)(1P) [or chi(c1)(3510)]

chi(c2)(1P) [or chi(c2)(3555)]

psi(2S) [or psi(3685)]

psi(3770)

psi(4040)

psi(4160)

psi(4415)

b bbar MESONS

Upsilon(1S) [or Upsilon(9460)]

chi(b0)(1P) [or chi(b0)(9860)]

chi(b1)(1P) [or chi(b1)(9890)]

chi(b2)(1P) [or chi(b2)(9915)]

Upsilon(2S) [or Upsilon(10023)]

chi(b0)(2P) [or chi(b0)(10235)]

chi(b1)(2P) [or chi(b1)(10255)]

chi(b2)(2P) [or chi(b2)(10270)]

Upsilon(3S) [or Upsilon(10355)]

Upsilon(4S) [or Upsilon(10580)]

Upsilon(10860)

Upsilon(11020)

N BARYONS (S = 0, I = 1/2)

p

n

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)

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)

Lambda BARYONS (S = -1, I = 0)

Lambda

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)

Sigma BARYONS (S = -1, I = 1)

Sigma+

Sigma0

Sigma-

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)

Xi BARYONS (S = -2, I = 1/2)

Xi0

Xi-

Xi(1530) P(13)

Xi(1690)

Xi(1820) D(13)

Xi(1950)

Xi(2030)

Omega BARYONS (S = -3, I = 0)

Omega-

Omega(2250)-

CHARMED BARYONS (C = +1)

Lambda(c)+

Lambda(c)(2625)+

Sigma(c)(2455)

Xi(c)+

Xi(c)0

BOTTOM (BEAUTY) BARYON (B = -1)

Lambda(b)0

SEARCHES FOR FREE QUARKS, MONOPOLES, SUPERSYMMETRY, COMPOSITENESS, etc.

Free Quark Searches

Magnetic Monopole Searches

Supersymmetric Particle Searches

Searches for Quark and Lepton Compositeness

Go to Table of Contents , Review of Particle Properties.