Introduction to Electron Positron
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Electron Positron sentence examples within Circular Electron Positron
To obtain high luminosity, compact high gradient quadrupole magnets QD0 and QF1 are required on both sides of the interaction points of the proposed Circular Electron Positron Collider (CEPC).
To obtain high luminosity, compact high gradient quadrupole magnets QD0 and QF1 are required on both sides of the interaction points of the proposed Circular Electron Positron Collider (CEPC).
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The proposed Circular Electron Positron Collider (CEPC), with a center-of-mass energy √ s = 240 GeV, will primarily serve as a Higgs factory.
The proposed Circular Electron Positron Collider (CEPC), with a center-of-mass energy √ s = 240 GeV, will primarily serve as a Higgs factory.
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Electron Positron sentence examples within Beijing Electron Positron
A quadratic increase of the synchrotron tune with beam current has been observed during the operation of the Beijing Electron Positron Collider Upgrade (BEPCII).
A quadratic increase of the synchrotron tune with beam current has been observed during the operation of the Beijing Electron Positron Collider Upgrade (BEPCII).
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BESIII at the Beijing electron positron collider; COMPASS and (approved) COMPASS++/AMBER at CERN; Jefferson Lab running at 12 GeV; KLOE at DAΦNE; the relativistic heavy ion collider at Brookhaven National Laboratory; the large hadron collider beauty experiment; the Facility for Antiproton and Ion Research (FAIR); the Nuclotron-based Ion Collider fAcility (NICA); and electron ion colliders in the USA (EIC) and China (EicC).
BESIII at the Beijing electron positron collider; COMPASS and (approved) COMPASS++/AMBER at CERN; Jefferson Lab running at 12 GeV; KLOE at DAΦNE; the relativistic heavy ion collider at Brookhaven National Laboratory; the large hadron collider beauty experiment; the Facility for Antiproton and Ion Research (FAIR); the Nuclotron-based Ion Collider fAcility (NICA); and electron ion colliders in the USA (EIC) and China (EicC).
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Electron Positron sentence examples within Large Electron Positron
We discuss the status of determination of the strong coupling with special attention to using event shape observables based on data collected at the Large Electron Positron collider and theoretical predictions at highest accuracy available at present.
We discuss the status of determination of the strong coupling with special attention to using event shape observables based on data collected at the Large Electron Positron collider and theoretical predictions at highest accuracy available at present.
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This paper discusses the computational and experimental techniques adopted for clearing from regulatory control the superconducting acceleration system of the former CERN Large Electron Positron collider (LEP), consisting of nearly 450 tons of valuable metals.
This paper discusses the computational and experimental techniques adopted for clearing from regulatory control the superconducting acceleration system of the former CERN Large Electron Positron collider (LEP), consisting of nearly 450 tons of valuable metals.
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Electron Positron sentence examples within electron positron collider
To obtain high luminosity, compact high gradient quadrupole magnets QD0 and QF1 are required on both sides of the interaction points of the proposed Circular Electron Positron Collider (CEPC).
To obtain high luminosity, compact high gradient quadrupole magnets QD0 and QF1 are required on both sides of the interaction points of the proposed Circular Electron Positron Collider (CEPC).
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The proposed Circular Electron Positron Collider (CEPC), with a center-of-mass energy √ s = 240 GeV, will primarily serve as a Higgs factory.
The proposed Circular Electron Positron Collider (CEPC), with a center-of-mass energy √ s = 240 GeV, will primarily serve as a Higgs factory.
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Electron Positron sentence examples within electron positron beam
Compton scattering of gamma rays propagating in a pair plasma can drive the formation of a relativistic electron positron beam.
Compton scattering of gamma rays propagating in a pair plasma can drive the formation of a relativistic electron positron beam.
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The expected experimental precision of the rates and asymmetries in the Future Circular Collider with electron positron beams (FCC-ee) in the centre of the mass energy range 88-365GeV considered for construction in CERN, will be better by a factor 5-200.
The expected experimental precision of the rates and asymmetries in the Future Circular Collider with electron positron beams (FCC-ee) in the centre of the mass energy range 88-365GeV considered for construction in CERN, will be better by a factor 5-200.
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10.1142/s0217751x21420070
To obtain high luminosity, compact high gradient quadrupole magnets QD0 and QF1 are required on both sides of the interaction points of the proposed Circular Electron Positron Collider (CEPC).
To obtain high luminosity, compact high gradient quadrupole magnets QD0 and QF1 are required on both sides of the interaction points of the proposed Circular Electron Positron Collider (CEPC).
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10.1142/S0217751X21501207
In this paper, we calculate the differential cross-section in terms of both the parity-even and parity-odd fragmentation functions in semi-inclusive electron positron annihilation process.
In this paper, we calculate the differential cross-section in terms of both the parity-even and parity-odd fragmentation functions in semi-inclusive electron positron annihilation process.
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10.1088/1674-1137/ac2f93
The proposed Circular Electron Positron Collider (CEPC), with a center-of-mass energy √ s = 240 GeV, will primarily serve as a Higgs factory.
The proposed Circular Electron Positron Collider (CEPC), with a center-of-mass energy √ s = 240 GeV, will primarily serve as a Higgs factory.
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10.1007/S41605-021-00253-W
Background Movable collimators for the circular electron positron collider (CEPC) are required to cut off spent electrons/positrons just near the beam orbit and reduce the background of the detector.
Background Movable collimators for the circular electron positron collider (CEPC) are required to cut off spent electrons/positrons just near the beam orbit and reduce the background of the detector.
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10.20944/PREPRINTS202107.0451.V1
This helps proposing creation of neutrino antineutrino pair orthogonal to electron positron “curdling” planes, that may lead to formation of protonic hydrogen of stars or orthogonally muon.
This helps proposing creation of neutrino antineutrino pair orthogonal to electron positron “curdling” planes, that may lead to formation of protonic hydrogen of stars or orthogonally muon.
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10.1016/J.NIMA.2021.165725
A quadratic increase of the synchrotron tune with beam current has been observed during the operation of the Beijing Electron Positron Collider Upgrade (BEPCII).
A quadratic increase of the synchrotron tune with beam current has been observed during the operation of the Beijing Electron Positron Collider Upgrade (BEPCII).
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10.1016/J.NIMA.2020.164686
This paper presents a 4-channel avalanche photodiode readout ASIC for the electromagnetic calorimeter in the 2-7 GeV high intensity electron positron accelerator.
This paper presents a 4-channel avalanche photodiode readout ASIC for the electromagnetic calorimeter in the 2-7 GeV high intensity electron positron accelerator.
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10.1103/PhysRevD.103.095027
Measurements at the Circular Electron Positron Collider, for example, could exclude a CP phase larger than 2.
Measurements at the Circular Electron Positron Collider, for example, could exclude a CP phase larger than 2.
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10.1142/s0217751x21420094
A Circular Electron Positron Collider (CEPC) with a circumference of about 100 km and a beam energy up to 120 GeV is proposed to be constructed in China.
A Circular Electron Positron Collider (CEPC) with a circumference of about 100 km and a beam energy up to 120 GeV is proposed to be constructed in China.
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10.1007/s00601-021-01616-1
BESIII at the Beijing electron positron collider; COMPASS and (approved) COMPASS++/AMBER at CERN; Jefferson Lab running at 12 GeV; KLOE at DAΦNE; the relativistic heavy ion collider at Brookhaven National Laboratory; the large hadron collider beauty experiment; the Facility for Antiproton and Ion Research (FAIR); the Nuclotron-based Ion Collider fAcility (NICA); and electron ion colliders in the USA (EIC) and China (EicC).
BESIII at the Beijing electron positron collider; COMPASS and (approved) COMPASS++/AMBER at CERN; Jefferson Lab running at 12 GeV; KLOE at DAΦNE; the relativistic heavy ion collider at Brookhaven National Laboratory; the large hadron collider beauty experiment; the Facility for Antiproton and Ion Research (FAIR); the Nuclotron-based Ion Collider fAcility (NICA); and electron ion colliders in the USA (EIC) and China (EicC).
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10.1007/S41365-021-00881-3
The nitrogen doping/infusion of 650 MHz cavities for the circular electron positron collider (CEPC) is investigated in this study.
The nitrogen doping/infusion of 650 MHz cavities for the circular electron positron collider (CEPC) is investigated in this study.
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10.1088/1748-0221/16/09/P09020
The proposed Circular Electron Positron Collider (CEPC) imposes new challenges for the vertex detector in terms of high resolution, low material, fast readout and low power.
The proposed Circular Electron Positron Collider (CEPC) imposes new challenges for the vertex detector in terms of high resolution, low material, fast readout and low power.
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10.1007/JHEP06(2021)103
We find that most of the relevant parameter space can be covered by the next generation of proposed beam-dump experiments and future high-luminosity electron positron colliders.
We find that most of the relevant parameter space can be covered by the next generation of proposed beam-dump experiments and future high-luminosity electron positron colliders.
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10.1016/J.NIMA.2021.165700
Beam pipe, which lies at the centre of the second-generation Beijing Electron Positron Collider (BEPC II) and its detector Beijing Spectrometer III (BES III), is made of beryllium and the electron–positron beam collision occurs in it.
Beam pipe, which lies at the centre of the second-generation Beijing Electron Positron Collider (BEPC II) and its detector Beijing Spectrometer III (BES III), is made of beryllium and the electron–positron beam collision occurs in it.
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10.1109/TASC.2021.3057840
In the scope of the Future Circular electron positron Collider study (FCC-ee), the IDEA detector is developed.
In the scope of the Future Circular electron positron Collider study (FCC-ee), the IDEA detector is developed.
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10.1088/1748-0221/16/03/P03001
The Circular Electron Positron Collider (CEPC) project was proposed to measure precisely the properties of the Higgs bosons.
The Circular Electron Positron Collider (CEPC) project was proposed to measure precisely the properties of the Higgs bosons.
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10.1007/JHEP06(2021)157
1× 109 J/ψ events produced by the Beijing Electron Positron Collider (BEPCII) at a center-of-mass energy √ s = 3.
1× 109 J/ψ events produced by the Beijing Electron Positron Collider (BEPCII) at a center-of-mass energy √ s = 3.
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10.1007/S41365-021-00904-Z
Positron sources are one of the most important components of the injector of a circular electron positron collector (CEPC).
Positron sources are one of the most important components of the injector of a circular electron positron collector (CEPC).
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10.1016/j.physletb.2021.136695
We show that future electron positron collider such as International Linear Collider with 500 GeV and 1 TeV collision energies may offer unique probe for the nominal Im(ρbb) via e +e− → Z∗ → AH process followed by A,H → bb̄ decays in four b-jets signature.
We show that future electron positron collider such as International Linear Collider with 500 GeV and 1 TeV collision energies may offer unique probe for the nominal Im(ρbb) via e +e− → Z∗ → AH process followed by A,H → bb̄ decays in four b-jets signature.
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10.1140/epjti/s40485-021-00064-9
The BEPCII project is for upgrading the Beijing Electron Positron Collider to reach a higher luminosity.
The BEPCII project is for upgrading the Beijing Electron Positron Collider to reach a higher luminosity.
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10.20944/preprints202107.0685.v1
This circuit assembly gage (PDPcag) that maybe operating at the quantum level, demonstrates the power of point fields matrix theoretical quantum general formalism of Iyer Markoulakis Helmholtz Hamiltonian mechanics transformed to Coulomb gage metrics, to form eigenvector fields of magnetic monopoles as well as electron positron particle gage metrics fields.
This circuit assembly gage (PDPcag) that maybe operating at the quantum level, demonstrates the power of point fields matrix theoretical quantum general formalism of Iyer Markoulakis Helmholtz Hamiltonian mechanics transformed to Coulomb gage metrics, to form eigenvector fields of magnetic monopoles as well as electron positron particle gage metrics fields.
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10.1017/S0022377821000660
Compton scattering of gamma rays propagating in a pair plasma can drive the formation of a relativistic electron positron beam.
Compton scattering of gamma rays propagating in a pair plasma can drive the formation of a relativistic electron positron beam.
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10.1088/1748-0221/16/07/P07052
The silicon pixel sensor is the core component of the vertex detector in the Circular Electron Positron Collider (CEPC).
The silicon pixel sensor is the core component of the vertex detector in the Circular Electron Positron Collider (CEPC).
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10.1140/epjp/s13360-020-01001-7
2 GeV, more than $$10^{12}$$ 10 12 $$\mathrm{Z}$$ Z bosons will be produced at the Circular Electron Positron Collider (CEPC).
2 GeV, more than $$10^{12}$$ 10 12 $$\mathrm{Z}$$ Z bosons will be produced at the Circular Electron Positron Collider (CEPC).
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10.1016/J.NIMA.2021.165080
The best intrinsic quality factor ( Q 0 ) of these cavities have exceeded 3 × 1010 at 24 MV/m, which is the target of vertical test for Circular Electron Positron Collider (CEPC).
The best intrinsic quality factor ( Q 0 ) of these cavities have exceeded 3 × 1010 at 24 MV/m, which is the target of vertical test for Circular Electron Positron Collider (CEPC).
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10.1016/J.NIMA.2021.165649
8 MHz radio frequency (rf) cavities have been adopted for the Upgrade project of Beijing Electron Positron Collider (BEPCII), a double-ring electron–positron collider as well as a synchrotron radiation (SR) light source.
8 MHz radio frequency (rf) cavities have been adopted for the Upgrade project of Beijing Electron Positron Collider (BEPCII), a double-ring electron–positron collider as well as a synchrotron radiation (SR) light source.
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10.1016/J.NIMA.2018.06.059
A small prototype SOI pixel sensor with in-pixel discriminator and binary readout has been developed as a part of R&D for the Circular Electron Positron Collider (CEPC).
A small prototype SOI pixel sensor with in-pixel discriminator and binary readout has been developed as a part of R&D for the Circular Electron Positron Collider (CEPC).
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10.1142/S0217751X19501185
The measurement of Born cross section of $e^+e^-\to ZH$ process is one of the major goals of the future Circular Electron Positron Collider, which may reach a precision of 0.
The measurement of Born cross section of $e^+e^-\to ZH$ process is one of the major goals of the future Circular Electron Positron Collider, which may reach a precision of 0.
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10.1088/1742-6596/1350/1/012158
Beijing Electron Positron Collider is studying a deQing circuit aiming at improving the stability of less than 0.
Beijing Electron Positron Collider is studying a deQing circuit aiming at improving the stability of less than 0.
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10.18429/JACOW-IPAC2019-MOPTS065
INTRODUCTION In September 2012, Chinese scientists proposed a Circular Electron Positron Collider (CEPC) in China at 240 GeV centre of mass for Higgs studies [1].
INTRODUCTION In September 2012, Chinese scientists proposed a Circular Electron Positron Collider (CEPC) in China at 240 GeV centre of mass for Higgs studies [1].
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10.1140/epjc/s10052-019-7255-9
The expected experimental precision of the rates and asymmetries in the Future Circular Collider with electron positron beams (FCC-ee) in the centre of the mass energy range 88-365GeV considered for construction in CERN, will be better by a factor 5-200.
The expected experimental precision of the rates and asymmetries in the Future Circular Collider with electron positron beams (FCC-ee) in the centre of the mass energy range 88-365GeV considered for construction in CERN, will be better by a factor 5-200.
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10.1088/1674-1137/43/4/043002
The Circular Electron Positron Collider (CEPC) is one of such proposed Higgs factories.
The Circular Electron Positron Collider (CEPC) is one of such proposed Higgs factories.
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10.1088/1674-1137/43/11/113104
We propose to study the flavor properties of the top quark at the future Circular Electron Positron Collider (CEPC) in China.
We propose to study the flavor properties of the top quark at the future Circular Electron Positron Collider (CEPC) in China.
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10.1109/TNS.2019.2906220
The Circular Electron Positron Collider (CEPC) is a proposing electron–positron collider in China, which aims for generating high center-of-mass energy colliding above 250 GeV.
The Circular Electron Positron Collider (CEPC) is a proposing electron–positron collider in China, which aims for generating high center-of-mass energy colliding above 250 GeV.
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10.1063/1.5064526
The results obtained may be related to the observations and experimental results in the electron positron plasma.
The results obtained may be related to the observations and experimental results in the electron positron plasma.
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10.18429/JACoW-LINAC2018-WE1A06
In 2017, sixty-four pulsed magnets (28 quadrupoles and 36 steerings) were installed in the KEK electron positron linac for simultaneous injection to four different rings.
In 2017, sixty-four pulsed magnets (28 quadrupoles and 36 steerings) were installed in the KEK electron positron linac for simultaneous injection to four different rings.
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10.1103/PhysRevD.99.032001
08 GeV with the BESIII detector at the Beijing Electron Positron Coll.
08 GeV with the BESIII detector at the Beijing Electron Positron Coll.
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10.1088/1748-0221/14/05/C05023
Initial R\&D work has been conducted for the vertex detector for the proposed Circular Electron Positron Collider that will allow precision Higgs measurements.
Initial R\&D work has been conducted for the vertex detector for the proposed Circular Electron Positron Collider that will allow precision Higgs measurements.
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10.18429/JACOW-IPAC2019-WEPRB031
The stability and reliability of the Superconducting RF system (SRF) is generally a key issue in a large scale accelerator such as Beijing Electron Positron Collider II (BEPCII).
The stability and reliability of the Superconducting RF system (SRF) is generally a key issue in a large scale accelerator such as Beijing Electron Positron Collider II (BEPCII).
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10.22323/1.353.0035
We discuss the status of determination of the strong coupling with special attention to using event shape observables based on data collected at the Large Electron Positron collider and theoretical predictions at highest accuracy available at present.
We discuss the status of determination of the strong coupling with special attention to using event shape observables based on data collected at the Large Electron Positron collider and theoretical predictions at highest accuracy available at present.
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10.1103/PhysRevD.100.053008
In this paper, we compare the potential of probing charm Yukawa coupling at the two proposed future "Higgs Factory" experiments, the Large Hadron electron Collider (LHeC) and Circular electron positron collider (CEPC).
In this paper, we compare the potential of probing charm Yukawa coupling at the two proposed future "Higgs Factory" experiments, the Large Hadron electron Collider (LHeC) and Circular electron positron collider (CEPC).
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10.1038/S42254-019-0047-1
XinChou Lou describes the plans for the Circular Electron Positron Collider, a large accelerator complex that would be built in China.
XinChou Lou describes the plans for the Circular Electron Positron Collider, a large accelerator complex that would be built in China.
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10.1088/1674-1137/43/10/103001
Utilizing the current conceptual design parameters of the Circular Electron Positron Collider, we give the experimental limits for the model independent operators by the total Higgsstrahlung cross section and angular distribution of Z boson decay in the Higgs factory.
Utilizing the current conceptual design parameters of the Circular Electron Positron Collider, we give the experimental limits for the model independent operators by the total Higgsstrahlung cross section and angular distribution of Z boson decay in the Higgs factory.
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10.1016/J.NIMA.2018.10.006
The Circular Electron Positron Collider (CEPC) is proposed as a Higgs factory for precision measurement of properties of the Higgs boson.
The Circular Electron Positron Collider (CEPC) is proposed as a Higgs factory for precision measurement of properties of the Higgs boson.
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10.18429/JACOW-IPAC2019-WEPRB045
The Circular Electron Positron Collider (CEPC) is in pre-research, it will need more than two hundred 650 MHz/800 kW klystrons.
The Circular Electron Positron Collider (CEPC) is in pre-research, it will need more than two hundred 650 MHz/800 kW klystrons.
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10.1016/J.NIMA.2018.11.139
This paper discusses the computational and experimental techniques adopted for clearing from regulatory control the superconducting acceleration system of the former CERN Large Electron Positron collider (LEP), consisting of nearly 450 tons of valuable metals.
This paper discusses the computational and experimental techniques adopted for clearing from regulatory control the superconducting acceleration system of the former CERN Large Electron Positron collider (LEP), consisting of nearly 450 tons of valuable metals.
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10.1103/PhysRevD.99.015004
We propose to search for millicharged particles at the BESIII detector which is operated at the Beijing Electron Positron Collider.
We propose to search for millicharged particles at the BESIII detector which is operated at the Beijing Electron Positron Collider.
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10.22323/1.367.0178
The BESIII experiment at the Beijing Electron Positron Collider (BEPCII) has accumulated the world’s largest samples of $e+e−$ collisions in the tau-charm region.
The BESIII experiment at the Beijing Electron Positron Collider (BEPCII) has accumulated the world’s largest samples of $e+e−$ collisions in the tau-charm region.
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10.1007/S41605-019-0110-6
PurposeCircular Electron Positron Collider (CEPC) is a 100-km-ring e+ e− collider for a Higgs factory.
PurposeCircular Electron Positron Collider (CEPC) is a 100-km-ring e+ e− collider for a Higgs factory.
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10.1007/s41605-019-0125-z
BackgroundIn the linac of Beijing Electron Positron Collider II (BEPCII), the resolution of existing BPMs is several hundred microns.
BackgroundIn the linac of Beijing Electron Positron Collider II (BEPCII), the resolution of existing BPMs is several hundred microns.
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10.22323/1.347.0002
We discuss the status of determinations of the strong coupling using event shape observables based on data collected at the Large Electron Positron collider and theoretical predictions at highest accuracy available at present.
We discuss the status of determinations of the strong coupling using event shape observables based on data collected at the Large Electron Positron collider and theoretical predictions at highest accuracy available at present.
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