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Graviton-Photon Scattering, N.E.J. Bjerrum-Bohr, Barry R. Holstein, Ludovic Planté, Pierre Vanhove Mar 2015

Graviton-Photon Scattering, N.E.J. Bjerrum-Bohr, Barry R. Holstein, Ludovic Planté, Pierre Vanhove

Barry R Holstein

We use the feature that the gravitational Compton scattering amplitude factorizes in terms of Abelian QED amplitudes to evaluate various gravitational Compton processes. We examine both the QED and gravitational Compton scattering from a massive spin-1 system by the use of helicity amplitude methods. In the case of gravitational Compton scattering we show how the massless limit can be used to evaluate the cross section for graviton-photon scattering and discuss the difference between photon interactions and the zero mass spin-1 limit. We show that the forward scattering cross section for graviton photoproduction has a very peculiar behavior, differing from the …


Bending Of Light In Quantum Gravity, N.E.J. Bjerrum-Bohr, John F. Donoghue, Barry R. Holstein, Ludovic Planté, Pierre Vanhove Feb 2015

Bending Of Light In Quantum Gravity, N.E.J. Bjerrum-Bohr, John F. Donoghue, Barry R. Holstein, Ludovic Planté, Pierre Vanhove

Barry R Holstein

We consider the scattering of lightlike matter in the presence of a heavy scalar object (such as the Sun or a Schwarzschild black hole). By treating general relativity as an effective field theory we directly compute the nonanalytic components of the one-loop gravitational amplitude for the scattering of massless scalars or photons from an external massive scalar field. These results allow a semiclassical computation of the bending angle for light rays grazing the Sun, including long-range ℏ contributions. We discuss implications of this computation, in particular the violation of some classical formulations of the equivalence principle.


Chiral Perturbation Theory And Nucleon Polarizabilities, Br Holstein Feb 2011

Chiral Perturbation Theory And Nucleon Polarizabilities, Br Holstein

Barry R Holstein

Compton scattering offers in principle an intriguing new window on nucleon structure. Existing experiments and future programs are discussed and the state of theoretical understanding of such measurements is explored.


Semileptonic Decays Of The Light J(P)=1/2(+) Ground State Baryon Octet, A Faessler, T Gutsche, Br Holstein, Ma Ivanov, Jg Korner, Ve Lyubovitskij Feb 2011

Semileptonic Decays Of The Light J(P)=1/2(+) Ground State Baryon Octet, A Faessler, T Gutsche, Br Holstein, Ma Ivanov, Jg Korner, Ve Lyubovitskij

Barry R Holstein

We calculate the semileptonic baryon octet-octet transition form factors using a manifestly Lorentz covariant quark model approach based on the factorization of the contribution of valence quarks and chiral effects. We perform a detailed analysis of SU(3)-breaking corrections to the hyperon semileptonic decay form factors. We present complete results on decay rates and asymmetry parameters including lepton mass effects for the rates.


Long Range Electromagnetic Effects Involving Neutral Systems And Effective Field Theory, Br Holstein Feb 2011

Long Range Electromagnetic Effects Involving Neutral Systems And Effective Field Theory, Br Holstein

Barry R Holstein

We analyze the electromagnetic scattering of massive particles with and without spin wherein one particle (or both) is electrically neutral. Using the techniques of effective field theory, we isolate the leading long distance effects, both classical and quantum mechanical. For spinless systems results are identical to those obtained earlier via more elaborate dispersive methods. However, we also find new results if either or both particles carry spin.


Generalized Polarizabilities And The Chiral Structure Of The Nucleon, Thomas R. Hemmert, Barry R. Holstein, Germar Knöchlein, Stefan Scherer Feb 2011

Generalized Polarizabilities And The Chiral Structure Of The Nucleon, Thomas R. Hemmert, Barry R. Holstein, Germar Knöchlein, Stefan Scherer

Barry R Holstein

No abstract provided.


Neutrino Physics, Wc Haxton, Br Holstein Feb 2011

Neutrino Physics, Wc Haxton, Br Holstein

Barry R Holstein

The basic concepts of neutrino physics are presented at a level appropriate for integration into elementary courses on quantum mechanics and/or modern physics


Klein's Paradox, Br Holstein Feb 2011

Klein's Paradox, Br Holstein

Barry R Holstein

Klein’s paradox is shown to be resolved by a careful consideration of Feynman’s picture of antiparticles as negative energy solutions traveling backward in time. Implications associated with the spin-statistics theorem are pointed out.


Parity-Violating Photoproduction Of Pi(+/-) On The Delta Resonance, Sl Zhu, Cm Maekawa, Br Holstein, Mj Ramsey-Musolf Feb 2011

Parity-Violating Photoproduction Of Pi(+/-) On The Delta Resonance, Sl Zhu, Cm Maekawa, Br Holstein, Mj Ramsey-Musolf

Barry R Holstein

We analyze the real-photon asymmetry Aγ± for the parity-violating (PV) π± production on the Δ resonance via the reactions γ⃗+p→Δ+→π++n and γ⃗+d→Δ0+p→π-+p+p. This asymmetry is nonvanishing due to a PV γNΔ coupling constant, dΔ±. We argue that an experimental determination of this coupling would be of interest for hadron dynamics, possibly shedding light on the S-wave/ P-wave puzzle in the hyperon nonleptonic decays and the violation of Hara’s theorem in weak radiative hyperon decays.


Hadronic Atoms And Effective Interactions, Br Holstein Feb 2011

Hadronic Atoms And Effective Interactions, Br Holstein

Barry R Holstein

We examine the problem of hadronic atom energy shifts using the technique of effective interactions and demonstrate the equivalence with the conventional quantum mechanical approach.


Fundamental Neutron Physics: Introduction And Overview Preface, Br Holstein Feb 2011

Fundamental Neutron Physics: Introduction And Overview Preface, Br Holstein

Barry R Holstein

In the 77 years since its discovery by Chadwick in 1932, the neutron has come to play an increasingly important role in contemporary physics. As the next to lightest baryon, it is, of course, one of the two primary components of the atomic nucleus and studies of isotopes (nuclei with varying numbers of neutrons but the same proton number) and of the neutron drip line are one of the important focuses of the recently approved radioactive beam machine to be built at Michigan State University. Precise knowledge of its ~900 second lifetime is crucial to determination of the time at …


Limit On 2nd Class Polar Vector Couplings In Semileptonic Weak-Interactions, Br Holstein Feb 2011

Limit On 2nd Class Polar Vector Couplings In Semileptonic Weak-Interactions, Br Holstein

Barry R Holstein

Although a great deal of experimental work has succeeded in limiting a possible second class axial coupling to about ten percent of the size of weak magnetism, published limits on the size of a possible second class polar vector current are one order of magnitude less sensitive. We summarize the present situation and demonstrate that muon capture provides the strictest present limit.


K(S)-]Gamma-Gamma, K(L)-]Pi(0)Gamma-Gamma And Unitarity, J Kambor, Br Holstein Feb 2011

K(S)-]Gamma-Gamma, K(L)-]Pi(0)Gamma-Gamma And Unitarity, J Kambor, Br Holstein

Barry R Holstein

Agreement between the experimental value Γ(KS→γγ) and the number predicted via a one-loop chiral perturbation theory calculation has been cited as a success for the latter. On the other hand the one-loop prediction for the closely related process KL→π0γγ has been found to be a factor 3 below the experimental value. Using the inputs of unitarity and dispersion relations, we demonstrate the importance of higher order loop effects to both of these processes.


Symmetry-Tests And Standard Model Backgrounds, Br Holstein Feb 2011

Symmetry-Tests And Standard Model Backgrounds, Br Holstein

Barry R Holstein

No abstract provided.


The Reaction Gamma-Gamma-]Pi-0-Pi-0 And Chiral Loops, Jf Donoghue, Br Holstein, Yc Lin Feb 2011

The Reaction Gamma-Gamma-]Pi-0-Pi-0 And Chiral Loops, Jf Donoghue, Br Holstein, Yc Lin

Barry R Holstein

Two-photon production of a neutral-pion pair is uniquely predicted near threshold by the theory of chiral symmetry. The prediction vanishes at the tree level and is nonzero only at one-loop order, yielding a finite result without any unknown counterterms. In this paper we calculate the cross section for both on-shell and off-shell photons, as both cases can both be studied at e+e- storage rings. This reaction is the most accessible process which directly probes the loop structure of chiral-SU(2) symmetry.


Quantum-Mechanics In Curved Space, Jf Donoghue, Br Holstein Feb 2011

Quantum-Mechanics In Curved Space, Jf Donoghue, Br Holstein

Barry R Holstein

The quantum mechanical wave equation for a particle in a Schwarzschild metric is derived using general relativity in the linearized approximation. The significance of the various terms in the effective Hamiltonian is discussed and shown to be associated with the post‐Newtonian terms for the corresponding classical motion.


Mass Ratios Of The Light Quarks, Jf Donoghue, Br Holstein, D Wyler Feb 2011

Mass Ratios Of The Light Quarks, Jf Donoghue, Br Holstein, D Wyler

Barry R Holstein

We derive a consistent set of light quark mass ratios which are compatible with the available constraints of chiral symmetry treated to next-to-leading order. Also required as input is resonance saturation of a set of low-energy amplitudes, in particular for the pion and kaon electromagnetic mass difference. The results (md+mu)/ms=1/15.5, (md-mu)/ms=1/29 are modestly different from previous values, and resolve the long-standing puzzle of the η→3π decay rate.


Is Su(3) Chiral Perturbation Theory An Effective Field Theory?, Br Holstein Feb 2011

Is Su(3) Chiral Perturbation Theory An Effective Field Theory?, Br Holstein

Barry R Holstein

We argue that the difficulties associated with the convergence properties of conventional SU(3) chiral perturbation theory can be ameliorated by use of a cutoff, which suppresses the model-dependent short distance effects in such calculations.


Hadronic Parity Violation, Br Holstein Feb 2011

Hadronic Parity Violation, Br Holstein

Barry R Holstein

We review the state of hadronic parity violation and propose a program based on a new effective field theory potential which can resolve the present confusion.


Spin Effects In Long Range Electromagnetic Scattering, Br Holstein, Andreas Ross Feb 2011

Spin Effects In Long Range Electromagnetic Scattering, Br Holstein, Andreas Ross

Barry R Holstein

We analyze the electromagnetic scattering of massive particles with and without spin and, using the techniques of effective field theory, we isolate the leading long distance effects beyond one photon exchange, both classical and quantum mechanical. Spin-independent and spin-dependent effects are isolated and shown to have a universal structure.


A Status Report On Chiral Dynamics: Theory And Experiment, Aron M. Benstein, Barry Holstein Feb 2011

A Status Report On Chiral Dynamics: Theory And Experiment, Aron M. Benstein, Barry Holstein

Barry R Holstein

This paper gives an overview of a Workshop on Chiral Dynamics: Theory and Experiment which was held at MIT July 25-29, 1994; its unique feature was the equal mixture of theory and experiment. The purpose of the workshop was to bring together many of the active participants to assess the status of the field and to explore fruitful future directions. The foundations and present status of the theory were reviewed as well as the experimental status of the field. To facilitate the discussion of future directions working groups were organized on Threshold Photo/Electropion Production, Two-Pion Threshold and the Chiral Anomaly, …


Strong Bounds On Weak Couplings, Jf Donoghue, Br Holstein Feb 2011

Strong Bounds On Weak Couplings, Jf Donoghue, Br Holstein

Barry R Holstein

Analysis of nonleptonic ΔS = 1 weak decays strongly restricts the possible size of right-handed weak couplings. Limits thus obtained are competitive with those obtained via other means.


Effective Effective Interactions, Br Holstein Feb 2011

Effective Effective Interactions, Br Holstein

Barry R Holstein

The use of effective field theory techniques allows the basic physics to be extracted from otherwise complex systems. We cite examples from quantum mechanics, condensed-matter physics, QCD, and quantum gravity.


Delta(1232) And The Polarizabilities Of The Nucleon, Tr Hemmert, Br Holstein, J Kambor Feb 2011

Delta(1232) And The Polarizabilities Of The Nucleon, Tr Hemmert, Br Holstein, J Kambor

Barry R Holstein

Previous calculations of the polarizabilities of the nucleon within the framework of heavy baryon chiral perturbation theory have included the contribution of the Δ(1232) only in its effects on various contact terms or have been performed in chiral SU(3) where systematic errors are difficult to control. Herein, we perform a corresponding calculation in chiral SU(2) wherein Δ(1232) is treated as an explicit degree of freedom and the expansion is taken to third order in soft momenta, the pion mass, and the quantity MΔ-MN, collectively denoted ε. We present the results of a systematic O(ε3) calculation of forward Compton scattering off …


Electromagnetic Simulation Of T Noninvariance In Nuclear Beta-Decay, Br Holstein Feb 2011

Electromagnetic Simulation Of T Noninvariance In Nuclear Beta-Decay, Br Holstein

Barry R Holstein

We calculate the simulation of T-violating correlations induced by final state electromagnetic interactions in nuclear beta decay. RADIOACTIVITY Nuclear beta decay, calculated final state Coulomb simulation of T violation.


Lowest Order Effective Field Theory For The Weak #3;N Interaction, A Parreno, C Bennhold, Br Holstein Feb 2011

Lowest Order Effective Field Theory For The Weak #3;N Interaction, A Parreno, C Bennhold, Br Holstein

Barry R Holstein

The $|\Delta S|=1$ $\Lambda N$ interaction, responsible for the decay of hypernuclei, is studied by means of an Effective Field Theory where the long range physics is described by pion and kaon exchange mechanisms, and its short range counterpart is obtained from the most general non-derivative local four-fermion interaction. We show that, including the Lowest Order Parity Conserving contact terms, allows us to reproduce the total decay rates for $^5_\Lambda {\rm He}$, $^{11}_\Lambda {\rm B}$ and $^{12}_\Lambda {\rm C}$ with a reasonable value of ${\hat \chi^2}$, while in order to get a prediction for the Parity Violating (PV) asymmetry compatible …


Low Energy Tests Of Chiral Symmetry1, Br Holstein Feb 2011

Low Energy Tests Of Chiral Symmetry1, Br Holstein

Barry R Holstein

The present status of low energy test of chiral invariance via chiral perturbation theory is reviewed, both in the meson and baryon sectors, and future prospects are discussed.


Subleading Corrections To Parity-Violating Pion Photoproduction, Sl Zhu, S Puglia, Br Holstein, Mj Ramsey-Musolf Feb 2011

Subleading Corrections To Parity-Violating Pion Photoproduction, Sl Zhu, S Puglia, Br Holstein, Mj Ramsey-Musolf

Barry R Holstein

We compute the photon asymmetry Bγ for near threshold parity-violating (PV) pion photoproduction through subleading order. We show that subleading contributions involve a new combination of PV couplings not included in previous analyses of hadronic PV. We argue that existing constraints on the leading order contribution to Bγ—obtained from the PV γ-decay of 18F—suggest that the impact of the subleading contributions may be more significant than expected from naturalness arguments.


Effective Field Theory In Nuclear Physics, Martin J. Savage, Br Holstein Feb 2011

Effective Field Theory In Nuclear Physics, Martin J. Savage, Br Holstein

Barry R Holstein

The Electromagnetic and Hadronic Physics sub-community of nuclear physics held a town hall meeting at Jefferson Lab during November 30 to December 4 of 2000. This is is our combined contribution to the white paper that will result from this meeting.


Higgs-Boson-Exchange Models Of Cp Violation And K-]2pi, Jf Donoghue, Js Hagelin, Br Holstein Feb 2011

Higgs-Boson-Exchange Models Of Cp Violation And K-]2pi, Jf Donoghue, Js Hagelin, Br Holstein

Barry R Holstein

Work by Deshpande and Sanda, which appears to invalidate Higgs-boson-exchange models of CP noninvariance, is buttressed by (i) use of the MIT bag model to calculate matrix elements, (ii) use of experimental rather than calculated numbers for the K→2π decay amplitude and the KL-KS mass difference, and (iii) inclusion of possible t-quark effects. We conclude that, barring accidental cancellations, such Higgs-boson-exchange models are incompatible with experiment.