000916374 001__ 916374
000916374 005__ 20221222131702.0
000916374 0247_ $$2arXiv$$aarXiv:2212.03118
000916374 0247_ $$2Handle$$a2128/33291
000916374 037__ $$aFZJ-2022-06174
000916374 1001_ $$0P:(DE-Juel1)188816$$aKim, Jangho$$b0$$ufzj
000916374 1112_ $$a39th International Symposium on Lattice Field Theory$$cBonn$$d2022-08-08 - 2022-08-13$$gLattice2022$$wGermany
000916374 245__ $$aNuclear Transition in the Strong Coupling Limit
000916374 260__ $$c2022
000916374 300__ $$a158
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000916374 520__ $$aLattice QCD at finite baryon chemical potential has the infamous sign problem which hinders Monte Carlo simulations. This can be remedied by a dual representation that makes the sign problem mild. In the strong coupling limit, the dual formulation with staggered quarks is well established. We have used this formulation to study the quark mass dependence of the baryon mass and the nuclear transition. This allows us to quantify the nuclear interaction. We have also compared our Monte Carlo results with mean field predictions.
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000916374 7001_ $$0P:(DE-HGF)0$$aPattanaik, Pratitee$$b1$$eCorresponding author
000916374 7001_ $$0P:(DE-HGF)0$$aUnger, Wolfgang$$b2
000916374 8564_ $$uhttps://juser.fz-juelich.de/record/916374/files/2212.03118.pdf$$yOpenAccess
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000916374 9141_ $$y2022
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000916374 9201_ $$0I:(DE-Juel1)IAS-4-20090406$$kIAS-4$$lTheorie der Starken Wechselwirkung$$x0
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