It has been argued that the leading scalar-isoscalar weakly interacting massive particle (WIMP) -nucleus interactions receive parametrically enhanced contributions in the context of nuclear effective field theories [1]. These contributions arise from meson-exchange currents (MECs) and potentially modify the impulse approximation estimates of these interactions by 10%–60%. We point out that these MECs also contribute to the quark mass dependence of nuclear binding energies, that is, nuclear σ terms. In this work, we use recent lattice QCD calculations of the binding energies of the deuteron, [superscript 3]He and [superscript 4]He at pion masses near 500 and 800 MeV, combined with the experimentally determined binding energies at the physica...
The fraction of the longitudinal momentum of ^{3}He that is carried by the isovector combination of ...
At the present time there is a lively debate within the nuclear community concerning the relevance o...
We perform an analysis of a binding energy difference called δVpn(N,Z)≡-1/4[E(Z,N)-E(Z,N-2)-E(Z-2,N)...
Complete flavor decompositions of the matrix elements of the scalar, axial, and tensor currents in t...
In recent years, a persistent tension between phenomenological and lattice QCD determinations of the...
We present an analysis of the pion-nucleon σ-term σπN using six ensembles with 2 þ 1 þ 1-flavor high...
Nucleon-nucleon systems are studied with lattice quantum chromodynamics at a pion mass of m(pi) simi...
We discuss the role of QCD symmetries and confinement in understanding η- and η′-mesic nuclei. η and...
The ground-state energies of systems containing up to 12 π + 's in a spatial volume V ∼ ( 2.5 fm...
The fraction of the longitudinal momentum of 3He that is carried by the isovector combination of u a...
Complete flavor decompositions of the matrix elements of the scalar, axial, and tensor currents in t...
We perform an analysis of a binding energy difference called δV pn(N,Z)-14[E(Z,N)-E(Z,N-2)-E(Z-2,N)+...
A systematic calculation of nuclear matter is performed which includes the long-range correlations b...
We study SU(3) flavor-breaking corrections to the relation between the octet baryon masses and the n...
We calculate both the connected and disconnected contributions to the π-N σ term in quenched lattice...
The fraction of the longitudinal momentum of ^{3}He that is carried by the isovector combination of ...
At the present time there is a lively debate within the nuclear community concerning the relevance o...
We perform an analysis of a binding energy difference called δVpn(N,Z)≡-1/4[E(Z,N)-E(Z,N-2)-E(Z-2,N)...
Complete flavor decompositions of the matrix elements of the scalar, axial, and tensor currents in t...
In recent years, a persistent tension between phenomenological and lattice QCD determinations of the...
We present an analysis of the pion-nucleon σ-term σπN using six ensembles with 2 þ 1 þ 1-flavor high...
Nucleon-nucleon systems are studied with lattice quantum chromodynamics at a pion mass of m(pi) simi...
We discuss the role of QCD symmetries and confinement in understanding η- and η′-mesic nuclei. η and...
The ground-state energies of systems containing up to 12 π + 's in a spatial volume V ∼ ( 2.5 fm...
The fraction of the longitudinal momentum of 3He that is carried by the isovector combination of u a...
Complete flavor decompositions of the matrix elements of the scalar, axial, and tensor currents in t...
We perform an analysis of a binding energy difference called δV pn(N,Z)-14[E(Z,N)-E(Z,N-2)-E(Z-2,N)+...
A systematic calculation of nuclear matter is performed which includes the long-range correlations b...
We study SU(3) flavor-breaking corrections to the relation between the octet baryon masses and the n...
We calculate both the connected and disconnected contributions to the π-N σ term in quenched lattice...
The fraction of the longitudinal momentum of ^{3}He that is carried by the isovector combination of ...
At the present time there is a lively debate within the nuclear community concerning the relevance o...
We perform an analysis of a binding energy difference called δVpn(N,Z)≡-1/4[E(Z,N)-E(Z,N-2)-E(Z-2,N)...