- magnetic moment
-
-
- deuteron, measurement
ESTERMAN 1934
KELLOGG 1939
-
- electron
DIRAC 1928
DIRAC 1928B
VAN DYCK 1987
-
- electron, calculation
SCHWINGER 1948B
-
- electron, first measurement
FOLEY 1948
KUSCH 1947
-
- muon, measurement
GARWIN 1957
-
- neutron, first direct measurement
ALVAREZ 1940
-
- neutron, measurement
ESTERMAN 1934
-
- neutron, prediction
ALTSHULER 1934
-
- positron
VAN DYCK 1987
-
- proton, first measurement
FRISCH 1933
-
- proton, further measurement
ESTERMAN 1933
-
- proton, measurement
KELLOGG 1939
magnetic monopole, possible existence prediction
DIRAC 1931
Majorana neutrino
MAJORANA 1937
Majorana, nuclear forces
MAJORANA 1933
Mandelstam representation
MANDELSTAM 1958
- mass generation, gauge fields
-
-
- Higgs mechanism
HIGGS 1964B
HIGGS 1966
-
- Higgs-Kibble mechanism
KIBBLE 1967
- mass
-
-
- K+, first precise measurement
CHUPP 1955
-
- Ko
THOMPSON 1953B
-
- KS-KL difference
BOLDT 1958B
-
- νμ, cosmological upper bound
GERSHTEIN 1966
-
- πo-π– difference
PANOFSKY 1951
-
- Σo, measurement
PLANO 1957
-
- W±
WEINBERG 1967
-
- W±, estimation
SALAM 1964
-
- Zo
WEINBERG 1967
-
- charged kaons, comparison
FUNG 1956
-
- charged kaons, measurement
BIRGE 1955B
-
- neutrino, first estimation
FERMI 1934
-
- neutrino, parity nonconservation
SALAM 1957
-
- neutron
CHADWICK 1934
-
- top quark
ABACHI 1995G
ABE 1995
mass-energy relation
EINSTEIN 1905C
massive muon pairs in hadron collisions, observation
CHRISTENSON 1970
- matrix formalism
-
-
- Heisenberg quantum mechanics, invention
BORN 1925
matrix formalism, Heisenberg quantum mechanics, invention
BORN 1926
McKay, semi-conductor detectors
MCKAY 1949
mesons, nonstrange, G-parity conception
LEE 1956B
- method
-
-
- complex orbital momenta
REGGE 1959
REGGE 1960
-
- extraction, pion-pion interaction
GOEBEL 1958
-
- Faddeev-Popov
FADDEEV 1967
-
- Regge poles
REGGE 1959
REGGE 1960
-
- regularization
’T~HOOFT 1972
’T~HOOFT 1972B
-
- renormalization
’T~HOOFT 1972
’T~HOOFT 1972B
- metrology
-
-
- fundamental constants, first step
BIRGE 1929
-
- fundamental constants, further development
DUNNINGTON 1939
-
- particle physics, high precision measurements
ARTAMONOV 1984B
-
- particle properties data
BARKAS 1958
GELL-MANN 1957
Millikan, precise measurement
MILLIKAN 1911
MILLIKAN 1913
MILLIKAN 1916
- mixing
-
-
- Bs- anti-Bs confirmation
ADEVA 1990R
DECAMP 1991D
-
- Bs- anti-Bs first indication
ALBAJAR 1987C
-
- Bo- anti-Bo confirmation
ARTUSO 1989C
BAND 1988
-
- Bo- anti-Bo first evidence
ALBRECHT 1987P
- model
-
-
- Chew-Low
CHEW 1956
-
- constituent quarks, hadrons
GELL-MANN 1964
ZWEIG 1964
ZWEIG 1964B
-
- Fermi-Yang
FERMI 1949
-
- hadrons, Nambu-Jona-Lasinio, nonlinear
NAMBU 1961
-
- paraquark
GREENBERG 1964
-
- pion-nucleon interaction
CHEW 1956
-
- quark-parton
BJORKEN 1969B
-
- Sakata
SAKATA 1956
-
- Salam-Weinberg
SALAM 1968
WEINBERG 1967
-
- weak interaction, hadron
CABIBBO 1963
GLASHOW 1970
-
- Yukawa nuclear forces
YUKAWA 1935
- monoatomic gases
-
-
- condensation effect
EINSTEIN 1924
EINSTEIN 1925
-
- quantization
FERMI 1926
FERMI 1926B
multiplate cloud chamber (MIT)
BRIDGE 1955
multiple hadron production, nucleon-nucleon interactions
LORD 1950
multiwire proportional chamber, invention
CHARPAK 1968
- muon
-
-
- confirmation
NISHINA 1937
STREET 1937
STREET 1937B
-
- decay, electron spectra continuity, confirmation
LEIGHTON 1949
-
- decay, first evidence
ROSSI 1939
-
- decay, first observation
WILLIAMS 1940
-
- decay, gamma-radiation search, negative result
HINCKS 1948
SARD 1948
-
- decay, search for gamma-radiation
PICCIONI 1948
-
- exponential decay rate
NERESON 1942
ROSSI 1942
-
- first evidence
NEDDERMEYER 1937
-
- lifetime, first estimation
ROSSI 1939
-
- lifetime, measurement
NERESON 1942
RASETTI 1941
RASETTI 1941B
ROSSI 1942
-
- magnetic moment, measurement
GARWIN 1957
-
- not a strong interaction mediator, evidence
CONVERSI 1947
-
- spin
LEIGHTON 1949
μ– → e– γ decay suppression
HINCKS 1948
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