Готові списки джерел за темами / Qed+qcd

Добірка наукової літератури з теми "Qed+qcd"

Автор: Grafiati
Опубліковано: 10 грудня 2022
Оновлено: 28 січня 2023

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Статті в журналах з теми "Qed+qcd"

1

Wong, Cheuk-Yin. "QED Mesons, the QED Neutron, and the Dark Matter." EPJ Web of Conferences 259 (2022): 13016. http://dx.doi.org/10.1051/epjconf/202225913016.

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Анотація:
Schwinger’s boson solution for massless fermions in QED in 1+1D has been applied and generalized to quarks interacting in QED and QCD interactions, leading to stable and confined open-string QED and QCD boson excitations of the quark-QCD-QED system in 1+1D. Just as the open-string QCD excitations in 1+1D can be the idealization of QCD mesons with a flux tube in 3+1D, so the open-string QED excitations in 1+1D may likewise be the idealization of QED mesons with masses in the tens of MeV region, corresponding possibly to the anomalous X17 and E38 particles observed recently. A further search for bound states of quarks interacting in the QED interaction alone leads to the examination on the stability of the QED neutron, consisting of two d quarks and one u quark. Theoretically, the QED neutron has been found to be stable and estimated to have a mass of 44.5 MeV, whereas the analogous QED proton is unstable, leading to a long-lived QED neutron that may be a good candidate for the dark matter.
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2

Yam, Philip. "QED for QCD." Scientific American 269, no. 1 (July 1993): 23–24. http://dx.doi.org/10.1038/scientificamerican0793-23.

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3

Jeong, Eue-Jin. "QCD QED Potentials, Quark Confinement." International Journal of Fundamental Physical Sciences 12, no. 3 (September 17, 2022): 29–34. http://dx.doi.org/10.14331/ijfps.2022.330153.

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One of the enduring puzzles in high energy particle physics is why quarks do not exist independently ‎despite their existence inside the hadron as quarks have never been found in isolation. This problem may ‎be solved by formulating a QCD potential for the entire range of interaction distances of the quarks. The ‎mystery could be related to the fundamental origin of the mass of elementary particles despite the success ‎of the quantum field theories to the highest level of accuracy. The renormalization program is an essential ‎part of the calculation of the scattering amplitudes, where the infinities of the calculated masses of the ‎elementary particles are subtracted for the progressive calculation of the higher-order perturbative terms. ‎The mathematical structure of the mass term from quantum field theories expressed in the form of infinities ‎suggests that there may exist a finite dynamical mass in the limit when the input mass parameter ‎approaches zero. The Lagrangian recovers symmetry at the same time as the input mass becomes zero, ‎whereas the self-energy diagrams acquire a finite dynamical mass in the 4-dimensional space when the ‎dimensional regularization method of renormalization is utilized. We report a new finding that using the ‎mathematical expression of the self-energy(mass) for photons and gluons calculated from this method, the ‎complex form of the QCD and QED interaction potentials can be obtained by replacing the fixed ‎interaction mediating particle’s mass and coupling constants in Yukawa potential with the scale-‎dependent running coupling constant and the corresponding dynamical mass. The derived QCD QED ‎potentials predict the behavior of the related elementary particles exactly as verified by experimental ‎observation.‎
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4

GROZIN, ANDREY. "DECOUPLING IN QED AND QCD." International Journal of Modern Physics A 28, no. 05n06 (March 10, 2013): 1350015. http://dx.doi.org/10.1142/s0217751x13500152.

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5

Bacchetta, Alessandro, and Miguel G. Echevarria. "QCD×QED evolution of TMDs." Physics Letters B 788 (January 2019): 280–87. http://dx.doi.org/10.1016/j.physletb.2018.11.019.

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6

GASSER, J., V. LYUBOVITSKIJ, and A. RUSETSKY. "Hadronic atoms in QCD+QED." Physics Reports 456, no. 5-6 (February 2008): 167–251. http://dx.doi.org/10.1016/j.physrep.2007.09.006.

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7

Westin, Alex, Waseem Kamleh, Ross Young, James Zanotti, Roger Horsley, Yoshifumi Nakamura, Holger Perlt, Paul Rakow, Gerrit Schierholz, and Hinnerk Stüben. "Anomalous magnetic moment of the muon with dynamical QCD+QED." EPJ Web of Conferences 245 (2020): 06035. http://dx.doi.org/10.1051/epjconf/202024506035.

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There exists a long standing discrepancy of around 3.5σ between experimental measurements and standard model calculations of the magnetic moment of the muon. Current experiments aim to reduce the experimental uncertainty by a factor of 4, and Standard Model calculations must also be improved by a similar factor. The largest uncertainty in the Standard Model calculation comes from the QCD contribution, in particular the leading order hadronic vacuum polarisation (HVP). To calculate the HVP contribution, we use lattice gauge theory, which allows us to study QCD at low energies. In order to better understand this quantity, we investigate the effect of QED corrections to the leading order HVP term by including QED in our lattice calculations, and investigate flavour breaking effects. This is done using fully dynamical QCD+QED gauge configurations generated by the QCDSF collaboration and a novel method of quark tuning.
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8

WARD, B. F. L., C. GLOSSER, S. JADACH, and S. A. YOST. "THRESHOLD CORRECTIONS IN PRECISION LHC PHYSICS: QED⊗QCD." International Journal of Modern Physics A 20, no. 16 (June 30, 2005): 3735–38. http://dx.doi.org/10.1142/s0217751x05027461.

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With an eye toward LHC processes in which theoretical precisions of 1% are desired, we introduce the theory of the simultaneous YFS resummation of QED and QCD to compute the size of the expected resummed soft radiative threshold effects in precision studies of heavy particle production at the LHC. Our results show that both QED and QCD soft threshold effects must be controlled to be on the conservative side to achieve such precision goals.
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9

Minkowski, Peter. "Geometrodynamics and charge-like unification: On the vanishing of C, CP violation in QCD, in the limit GF → 0." International Journal of Modern Physics A 33, no. 31 (November 10, 2018): 1844008. http://dx.doi.org/10.1142/s0217751x18440086.

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10

Risch, Andreas, and Hartmut Wittig. "Towards leading isospin breaking effects in mesonic masses with O(a) improved Wilson fermions." EPJ Web of Conferences 175 (2018): 14019. http://dx.doi.org/10.1051/epjconf/201817514019.

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We present an exploratory study of leading isospin breaking effects in mesonic masses using O(a) improved Wilson fermions. Isospin symmetry is explicitly broken by distinct masses and electric charges of the up and down quarks. In order to be able to make use of existing isosymmetric QCD gauge ensembles we apply reweighting techniques. The path integral describing QCD+QED is expanded perturbatively in powers of the light quark’ mass deviations and the electromagnetic coupling. We employ QEDL as a finite volume formulation of QED.
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Дисертації з теми "Qed+qcd"

1

Gray, Norman. "Dimensionally regulated on-shell renormalisation in QCD and QED." Thesis, n.p, 1991. http://oro.open.ac.uk/19423/.

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2

Zemp, Peter. "Pionic hydrogen in QCD + QED : decay width at NNLO /." Bern : [s.n.], 2004. http://www.zb.unibe.ch/download/eldiss/04zemp_p.pdf.

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3

Gorbahn, Martin. "QCD and QED anomalous dimension matrix for weak decays at NNLO." [S.l. : s.n.], 2003. http://deposit.ddb.de/cgi-bin/dokserv?idn=970226101.

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4

Phipps, Martin. "Applications of perturbative QCD and QED using fully relativistic wave functions." Thesis, McGill University, 1992. http://digitool.Library.McGill.CA:80/R/?func=dbin-jump-full&object_id=56669.

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Анотація:
In this thesis, a method for calculating the decay rates and branching ratios using perturbative QCD and QED is proposed. Among the assumptions used are that heavy mesons are non-relativistic quark/anti-quark bound states and that light mesons can be treated as quarks in a bag. The method will be applied to the $ eta sb{c} to phi phi$ decay and to 1-loop contributions to the leptonic widths of mesons.
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5

Montero, J. C. [UNESP]. "Quebra dinamica da simetria quiral em teorias vetoriais: QED e QCD." Universidade Estadual Paulista (UNESP), 1987. http://hdl.handle.net/11449/132820.

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Made available in DSpace on 2016-01-13T13:28:06Z (GMT). No. of bitstreams: 0 Previous issue date: 1987. Added 1 bitstream(s) on 2016-01-13T13:33:38Z : No. of bitstreams: 1 000027534.pdf: 2451730 bytes, checksum: 30603905d1f09b5f573199e434a613d6 (MD5)
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6

Montero, J. C. (Juan Carlos). "Quebra dinamica da simetria quiral em teorias vetoriais : QED e QCD /." São Paulo, 1987. http://hdl.handle.net/11449/132820.

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7

Ahlig, Steven. "Analytical properties of the quark propagator QED 3, QCD and Kaon photoproduction /." [S.l. : s.n.], 2001. http://www.bsz-bw.de/cgi-bin/xvms.cgi?SWB9403127.

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8

Williams, Richard. "Schwinger-Dyson equations in QED and QCD : the calculation of fermion-antifermion condensates." Thesis, Durham University, 2007. http://etheses.dur.ac.uk/2558/.

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Анотація:
We present non-perturbative solutions for the fermion and boson propagators of QED in both three- and four-dimensions, and QCD. In doing so, we solve the coupled system of Schwinger-Dyson equations numerically in Euclidean space, investigating criticality, gauge dependence and phenomenology of the solutions. We do so by exploiting a new and novel three-point ansatz, the Kizilersü-Pennington vertex, designed to satisfy multiplicative renormalisability in unquenched QED. The efficacy of this is demonstrated numerically for QED(_4), where we find a marked improvement in the gauge-invarance of the photon wave-function. The critical coupling associated with dynamical mass generation is investigated for a variety of gauges; remarkably a lessening of this dependence is seen, despite the ansatz’s origins from a massless theory, which is improved further by constructing a hybrid system. As with many studies in the past, we apply this ansatz to the three-dimensional non-compact formulation of QED, checking gauge covariance of the propagators through a momentum-space formulation of the Landau-Khalatnikov-Pradkin transformations. The critical dependence on the number of active fermions was investigated, with the gauge dependence of the condensate unresolved. As an aside, we found numerically that LKF transforming the propagators gave rise to a constant condensate; a fact supported analytically through an explicit proof. We turn our attention towards QCD, where we explore a variety of phenomeno-logical models, including the full ghost-gluon system, in which we make comparisons between traditional vertices and the new KP-Vertex. These models are used in a determination of the physical quark condensate for massive quarks, through the exploitation of a class of non-positive definite solutions accessible for small quark masses. Finally, we examine Generalised Ward-Takahashi identities, which hold promise to further constrain the tranvserse part of the vertex. The identity is shown to hold true at one-loop through an explicit calculation, and a constraint on one of the basis coefficients is given as an example of its use.
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9

Schönherr, Marek. "Improving predictions for collider observables by consistently combining fixed order calculations with resummed results in perturbation theory." Doctoral thesis, Saechsische Landesbibliothek- Staats- und Universitaetsbibliothek Dresden, 2012. http://nbn-resolving.de/urn:nbn:de:bsz:14-qucosa-83876.

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Анотація:
With the constantly increasing precision of experimental data acquired at the current collider experiments Tevatron and LHC the theoretical uncertainty on the prediction of multiparticle final states has to decrease accordingly in order to have meaningful tests of the underlying theories such as the Standard Model. A pure leading order calculation, defined in the perturbative expansion of said theory in the interaction constant, represents the classical limit to such a quantum field theory and was already found to be insufficient at past collider experiments, e.g. LEP or Hera. Such a leading order calculation can be systematically improved in various limits. If the typical scales of a process are large and the respective coupling constants are small, the inclusion of fixed-order higher-order corrections then yields quickly converging predictions with much reduced uncertainties. In certain regions of the phase space, still well within the perturbative regime of the underlying theory, a clear hierarchy of the inherent scales, however, leads to large logarithms occurring at every order in perturbation theory. In many cases these logarithms are universal and can be resummed to all orders leading to precise predictions in these limits. Multiparticle final states now exhibit both small and large scales, necessitating a description using both resummed and fixed-order results. This thesis presents the consistent combination of two such resummation schemes with fixed-order results. The main objective therefor is to identify and properly treat terms that are present in both formulations in a process and observable independent manner. In the first part the resummation scheme introduced by Yennie, Frautschi and Suura (YFS), resumming large logarithms associated with the emission of soft photons in massive Qed, is combined with fixed-order next-to-leading matrix elements. The implementation of a universal algorithm is detailed and results are studied for various precision observables in e.g. Drell-Yan production or semileptonic B meson decays. The results obtained for radiative tau and muon decays are also compared to experimental data. In the second part the resummation scheme introduced by Dokshitzer, Gribov, Lipatov, Altarelli and Parisi (DGLAP), resumming large logarithms associated with the emission of collinear partons applicable to both Qcd and Qed, is combined with fixed-order next-to-leading matrix elements. While the focus rests on its application to Qcd corrections, this combination is discussed in detail and the implementation is presented. The resulting predictions are evaluated and compared to experimental data for a multitude of processes in four different collider environments. This formulation has been further extended to accommodate real emission corrections to beyond next-to-leading order radiation otherwise described only by the DGLAP resummation. Its results are also carefully evaluated and compared to a wide range of experimental data.
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10

Schönwald, Kay [Verfasser], Johannes [Akademischer Betreuer] Blümlein, and Gudrun [Gutachter] Hiller. "Massive two- and three-loop calculations in QED and QCD / Kay Schönwald ; Gutachter: Gudrun Hiller ; Betreuer: Johannes Blümlein." Dortmund : Universitätsbibliothek Dortmund, 2019. http://nbn-resolving.de/urn:nbn:de:101:1-2019111502475898135000.

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Книги з теми "Qed+qcd"

1

Gastmans, R. The ubiquitous photon: Helicity methods for QED and QCD. Oxford: Clarendon Press, 1990.

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2

Shtabovenko, Vladyslav. Nonrelativistic Effective Field Theories of QED and QCD: Applications and Automatic Calculations. München: Universitätsbibliothek der TU München, 2017.

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3

Zeuthen Workshop on Elementary Particle Theory: QCD and QED in Higher Orders (1996 Rheinsberg, Germany). QCD and QED in high orders: Proceedings of the 1996 Zeuthen Workshop on Elementary Particle Theory : QCD and QED in Higher Orders : Rheinsberg, Germany, 21-26 April 1996. [Amsterdam, Netherlands]: North-Holland, 1996.

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4

Lectures on QED and QCD: Practical calculations and renormalization of one- and multi-loop Feynman diagrams. Singapore: World Scientific, 2007.

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5

Campbell, John, Joey Huston, and Frank Krauss. Hard Scattering Formalism. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780199652747.003.0002.

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The hard scattering formalism is introduced, starting from a physical picture based on the idea of equivalent quanta borrowed from QED, and the notion of characteristic times. Contact to the standard QCD treatment is made after discussing the running coupling and the Altarelli–Parisi equations for the evolution of parton distribution functions, both for QED and QCD. This allows a development of a space-time picture for hard interactions in hadron collisions, integrating hard production cross sections, initial and final state radiation, hadronization, and multiple parton scattering. The production of a W boson at leading and next-to leading order in QCD is used to exemplify characteristic features of fixed-order perturbation theory, and the results are used for some first phenomenological considerations. After that, the analytic resummation of the W boson transverse momentum is introduced, giving rise to the notion of a Sudakov form factor. The probabilistic interpretation of the Sudakov form factor is used to discuss patterns in jet production in electron-positron annihilation.
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6

Bostock, Christopher J. Introduction to Quantized Fields: QED, Electroweak Theory, and QCD via a Selection of Original Papers. Springer, 2020.

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7

Grozin, Andrey. LECTURES ON QED AND QCD: PRACTICAL CALCULATION AND RENORMALIZATION OF ONE- AND MULTI-LOOP FEYNMAN DIAGRAMS. World Scientific Publishing, 2007.

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Частини книг з теми "Qed+qcd"

1

Telegdi, V. L., and S. J. Brodsky. "General QED/QCD Aspects of Simple Systems." In The Hydrogen Atom, 257–67. Berlin, Heidelberg: Springer Berlin Heidelberg, 1989. http://dx.doi.org/10.1007/978-3-642-88421-4_25.

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2

Fried, H. M. "Functional Approach to Strong-Coupling in (QED)4 and (QCD)4." In Vacuum Structure in Intense Fields, 293–313. Boston, MA: Springer US, 1991. http://dx.doi.org/10.1007/978-1-4757-0441-9_19.

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3

Ioffe, B. L. "The Revival of Longitudinal Photons and Gluons in Massless QED and QCD. The Infrared Problems in QCD." In High Energy Spin Physics, 211–20. Berlin, Heidelberg: Springer Berlin Heidelberg, 1991. http://dx.doi.org/10.1007/978-3-642-86995-2_17.

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4

Martinovič, L'ubomír. "Massive Light Front QED(1+1) in the Weyl Gauge." In Confinement, Topology, and Other Non-Perturbative Aspects of QCD, 269–76. Dordrecht: Springer Netherlands, 2002. http://dx.doi.org/10.1007/978-94-010-0502-9_29.

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5

"QED at one loop." In Lectures on QED and QCD, 21–41. WORLD SCIENTIFIC, 2007. http://dx.doi.org/10.1142/9789812706751_0002.

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6

"QCD at one loop." In Lectures on QED and QCD, 43–72. WORLD SCIENTIFIC, 2007. http://dx.doi.org/10.1142/9789812706751_0003.

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7

"One-loop diagrams." In Lectures on QED and QCD, 3–20. WORLD SCIENTIFIC, 2007. http://dx.doi.org/10.1142/9789812706751_0001.

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8

"Two-loop corrections in QED and QCD." In Lectures on QED and QCD, 73–99. WORLD SCIENTIFIC, 2007. http://dx.doi.org/10.1142/9789812706751_0004.

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9

"On-shell renormalization scheme." In Lectures on QED and QCD, 101–20. WORLD SCIENTIFIC, 2007. http://dx.doi.org/10.1142/9789812706751_0005.

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10

"Decoupling of heavy-particle loops." In Lectures on QED and QCD, 121–33. WORLD SCIENTIFIC, 2007. http://dx.doi.org/10.1142/9789812706751_0006.

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Тези доповідей конференцій з теми "Qed+qcd"

1

Wagman, Michael. "Charged hadron interactions in QCD+QED." In Charged hadron interactions in QCD+QED. US DOE, 2020. http://dx.doi.org/10.2172/1827376.

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2

Mangano, Michelangelo. "Algorithmic solutions for QED and QCD." In Workshop on qed structure functions. AIP, 1990. http://dx.doi.org/10.1063/1.39095.

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3

Lepage, G. Peter, D. J. Wineland, C. E. Wieman, and S. J. Smith. "Atomic Physics in QED and QCD." In ATOMIC PHYSICS 14: Fourteenth International Conference on Atomic Physics. AIP, 1994. http://dx.doi.org/10.1063/1.2946005.

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4

Ilderton, Anton. "Physical charges in QED and QCD." In International Workshop on QCD Green’s Functions, Confinement and Phenomenology. Trieste, Italy: Sissa Medialab, 2010. http://dx.doi.org/10.22323/1.087.0019.

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5

Chetyrkin, Konstantin. "Massless propagators: applications in QCD and QED." In 8th International Symposium on Radiative Corrections. Trieste, Italy: Sissa Medialab, 2008. http://dx.doi.org/10.22323/1.048.0023.

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6

Sborlini, Germán, Daniel DE FLORIAN, and Germán Rodrigo. "Mixed QCD-QED corrections to DGLAP equations." In 38th International Conference on High Energy Physics. Trieste, Italy: Sissa Medialab, 2017. http://dx.doi.org/10.22323/1.282.0793.

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7

Zhou, Ran, and Steven Gottlieb. "Dynamical QCD+QED simulation with staggered quarks." In The 32nd International Symposium on Lattice Field Theory. Trieste, Italy: Sissa Medialab, 2015. http://dx.doi.org/10.22323/1.214.0024.

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8

Wagman, Michael. "Exploring large charge density systems with lattice QCD+QED." In Exploring large charge density systems with lattice QCD+QED. US DOE, 2021. http://dx.doi.org/10.2172/1827858.

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9

GERHOLD, A., A. IPP, and A. REBHAN. "ANOMALOUS SPECIFIC HEAT IN ULTRADEGENERATE QED AND QCD." In Proceedings of the SEWM2004 Meeting. WORLD SCIENTIFIC, 2005. http://dx.doi.org/10.1142/9789812702159_0065.

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10

WARD, B. F. L., C. GLOSSER, S. JADACH, and S. A. YOST. "THRESHOLD CORRECTIONS IN QED⊗QCD AT THE LHC." In Proceedings of the 32nd International Conference. World Scientific Publishing Company, 2005. http://dx.doi.org/10.1142/9789812702227_0100.

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Звіти організацій з теми "Qed+qcd"

1

Dixon, Lance. QCD and QED Corrections to Light-by-Light Scattering. Office of Scientific and Technical Information (OSTI), September 2001. http://dx.doi.org/10.2172/798870.

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2

Melnikov, Kirill. The Three Loop On-Shell Renormalization of QCD and QED. Office of Scientific and Technical Information (OSTI), May 2000. http://dx.doi.org/10.2172/763774.

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Anastasiou, Charalampos. Two-Loop QED and QCD Corrections to Massless Fermion-Boson Scattering. Office of Scientific and Technical Information (OSTI), February 2002. http://dx.doi.org/10.2172/798998.

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