English
Related papers

Related papers: Simple do-it-yourself experimental set-up for elec…

200 papers

We address the physics implications of a precision determination of the weak charge of the proton, QWP, from a parity violating elastic electron proton scattering experiment to be performed at the Jefferson Laboratory. We present the…

High Energy Physics - Phenomenology · Physics 2009-11-10 Jens Erler , Andriy Kurylov , Michael J. Ramsey-Musolf

In the report submitted here, an elementary formula is presented that allows calculation of the fine structure constant, derived on the basis of the unified theory of the electromagnetic and gravitational field elaborated by the author.…

General Physics · Physics 2007-05-23 Jaroslav Pavel

Electric charge conservation (ECC) is typically taken as an axiom in the standard model. Searching for small violations with high-performance experiments could lead us to new physics. In this work, we tested ``invisible" electric charge…

High Energy Physics - Experiment · Physics 2025-02-06 Z. H. Zhang , X. P. Geng , J. W. Hu , Z. H. Zhang

A fractional quasiparticle charge is a manifestation of strong interactions in the fractional quantum Hall effect. Nevertheless, shot noise of quasiparticles is well described by a formula, derived for noninteracting charges. We explain the…

Mesoscale and Nanoscale Physics · Physics 2017-03-22 D. E. Feldman , M. Heiblum

A measurement of the top quark electric charge is carried out in the ATLAS experiment at the Large Hadron Collider using 2.05 fb-1 of data at a centre-of-mass energy of 7 TeV. In units of the elementary electric charge, the top quark charge…

High Energy Physics - Experiment · Physics 2013-11-13 The ATLAS Collaboration

The Jefferson Lab Q_weak experiment determined the weak charge of the proton by measuring the parity-violating elastic scattering asymmetry of longitudinally polarized electrons from an unpolarized liquid hydrogen target at small momentum…

Instrumentation and Detectors · Physics 2015-01-08 Qweak Collaboration , T. Allison , M. Anderson , D. Androic , D. S. Armstrong , A. Asaturyan , T. D. Averett , R. Averill , J. Balewski , J. Beaufait , R. S. Beminiwattha , J. Benesch , F. Benmokhtar , J. Bessuille , J. Birchall , E. Bonnell , J. Bowman , P. Brindza , D. B. Brown , R. D. Carlini , G. D. Cates , B. Cavness , G. Clark , J. C. Cornejo , S. Covrig Dusa , M. M. Dalton , C. A. Davis , D. C. Dean , W. Deconinck , J. Diefenbach , K. Dow , J. F. Dowd , J. A. Dunne , D. Dutta , W. S. Duvall , J. R. Echols , M. Elaasar , W. R. Falk , K. D. Finelli , J. M. Finn , D. Gaskell , M. T. W. Gericke , J. Grames , V. M. Gray , K. Grimm , F. Guo , J. Hansknecht , D. J. Harrison , E. Henderson , J. R. Hoskins , E. Ihloff , K. Johnston , D. Jones , M. Jones , R. Jones , M. Kargiantoulakis , J. Kelsey , N. Khan , P. M. King , E. Korkmaz , S. Kowalski , A. Kubera , J. Leacock , J. P. Leckey , A. R. Lee , J. H. Lee , L. Lee , Y. Liang , S. MacEwan , D. Mack , J. A. Magee , R. Mahurin , J. Mammei , J. W. Martin , A. McCreary , M. H. McDonald , M. J. McHugh , P. Medeiros , D. Meekins , J. Mei , R. Michaels , A. Micherdzinska , A. Mkrtchyan , H. Mkrtchyan , N. Morgan , J. Musson , K. E. Mesick , A. Narayan , L. Z. Ndukum , V. Nelyubin , Nuruzzaman , W. T. H. van Oers , A. K. Opper , S. A. Page , J. Pan , K. D. Paschke , S. K. Phillips , M. L. Pitt , M. Poelker , J. F. Rajotte , W. D. Ramsay , W. R. Roberts , J. Roche , P. W. Rose , B. Sawatzky , T. Seva , M. H. Shabestari , R. Silwal , N. Simicevic , G. R. Smith , S. Sobczynski , P. Solvignon , D. T. Spayde , B. Stokes , D. W. Storey , A. Subedi , R. Subedi , R. Suleiman , V. Tadevosyan , W. A. Tobias , V. Tvaskis , E. Urban , B. Waidyawansa , P. Wang , S. P. Wells , S. A. Wood , S. Yang , S. Zhamkochyan , R. B. Zielinski

We calculate the noise spectrum of the output signal of a quantum detector during continuous measurement of a two-level system (qubit). We generalize the previous results obtained for the regime of high voltages (when $eV$ is much larger…

Mesoscale and Nanoscale Physics · Physics 2007-05-23 A. Shnirman , D. Mozyrsky , I. Martin

Lessons and homework problems involving a pendulum are often a big part of introductory physics classes and laboratory courses from high school to undergraduate levels. Although laboratory equipment for pendulum experiments is commercially…

Physics Education · Physics 2009-08-27 Vadas Gintautas , Alfred Hubler

In this paper, we study the quantum decoherence induced by accumulation of electron tunnelings during the quantum measurement of a charge qubit. The charge qubit is a single electron confined in coupled quantum dots. The measurement of the…

Mesoscale and Nanoscale Physics · Physics 2009-11-11 Ming-Tsung Lee , Wei-Min Zhang

We propose an approach to reconstruct any superconducting charge qubit state by using quantum state tomography. This procedure requires a series of measurements on a large enough number of identically prepared copies of the quantum system.…

Quantum Physics · Physics 2009-11-10 Yu-xi Liu , L. F. Wei , Franco Nori

In quantum electrodynamics with fermions f = e,\mu..., knowledge of the vacuum polarization spectral function determined from the tree level e^+e^- -> f^+f^- cross sections, together with a single low energy measurement of the fine…

High Energy Physics - Phenomenology · Physics 2009-10-30 J. Papavassiliou , E. de Rafael , N. J. Watson

A concept to measure the neutron electric charge is presented which employs a precision Talbot-Lau interferometer in a high-intensity pulsed neutron beam. It is demonstrated that the sensitivity for a neutron charge measurement can be…

Instrumentation and Detectors · Physics 2018-12-12 Florian M. Piegsa

Shot noise measurements were recently exploited to measure the charge of the quasiparticles in the Fractional Quantum Hall (FQH) regime. For fractional filling factors nu=1/3 and 2/5 of the first Landau level, fractional charges q=e/3 and…

Mesoscale and Nanoscale Physics · Physics 2009-11-07 E. Comforti , Y. C. Chung , M. Heiblum , V. Umansky , D. Mahalu

We manipulate a single electron in a fully tunable double quantum dot using microwave excitation. Under resonant conditions, microwaves drive transitions between the (1,0) and (0,1) charge states of the double dot. Local quantum point…

Mesoscale and Nanoscale Physics · Physics 2010-10-05 J. R. Petta , A. C. Johnson , C. M. Marcus , M. P. Hanson , A. C. Gossard

In semiconductor-based quantum technologies, the capability to shuttle charges between components is profoundly enabling. We numerically simulated various "conveyor-belt" shuttling scenarios for simple Si/SiO2 devices, explicitly modelling…

Mesoscale and Nanoscale Physics · Physics 2025-04-03 Minjun Jeon , Simon C. Benjamin , Andrew J. Fisher

A simple analytic model of point-ion electrostatics has been previously proposed in which the magnitude of the net charge q_i on each atom in an ordered or random alloy depends linearly on the number N_i^(1) of unlike neighbors in its first…

mtrl-th · Physics 2009-10-30 C. Wolverton , Alex Zunger , S. Froyen , S. H. Wei

We describe here the realization of a single electron source similar to single photon sources in optics. On-demand single electron injection is obtained using a quantum dot connected to the conductor via a tunnel barrier of variable…

We present a nonperturbative numerical evaluation of the one-photon electron self energy for hydrogenlike ions with low nuclear charge numbers Z=1 to 5. Our calculation for the 1S state has a numerical uncertainty of 0.8 Hz for hydrogen and…

Atomic Physics · Physics 2011-08-11 U. D. Jentschura , P. J. Mohr , G. Soff

Quantum Amplitude Estimation (QAE) can achieve a quadratic speed-up for applications classically solved by Monte Carlo simulation. A key requirement to realize this advantage is efficient state preparation. If state preparation is too…

Quantum Physics · Physics 2021-03-17 Almudena Carrera Vazquez , Stefan Woerner

We've performed precise measurements of electron scattering on molecular hydrogen and deuterium by using the "Troitsk nu-mass" setup. Electrons were generated by the electron gun with an energy line width better than 0.3 eV. The electron…

‹ Prev 1 4 5 6 7 8 10 Next ›