Searcharxiv⌕ Search

arXiv subjects

Keitaro Nagata

Publications and source records attributed to Keitaro Nagata.

At least 37 records · Page 2Linked to original sources

On early onset of quark number density at zero temperature

We study a longstanding problem in lattice QCD at low temperature and nonzero quark chemical potential on an onset of the quark number density at $μ=m_π/2$. We introduce a physical parametrization of the eigenvalues in the reduction formula of the fermion determinant. It is shown that the parametrization reduces the quark number density operator to an expression with the Fermi distribution of the quark. For each configuration, the eigenvalues of the reduced matrix correspond to one-particle energy states of a quark. The gap of the eigenspectrum of the reduced matrix corresponds to the gap of the energy states, which causes the $μ$-independence of the fermion determinant for small $μ$ at T=0. Once $μ$ exceeds the gap, the quark number density becomes nonzero for each configuration, which causes the early onset of the quark number density.

hep-lat↗

EoS of finite density QCD with Wilson fermions by Multi-Parameter Reweighting and Taylor expansion

The equation of state (EoS), quark number density and susceptibility at nonzero quark chemical potential $μ$ are studied in lattice QCD simulations with a clover-improved Wilson fermion of 2-flavors and RG-improved gauge action. To access nonzero $μ$, we employ two methods : a multi-parameter reweighting (MPR) in $μ$ and $β$ and Taylor expansion in $μ/T$. The use of a reduction formula for the Wilson fermion determinant enables to study the reweighting factor in MPR explicitly and heigher-order coefficients in Taylor expansion free from errors of noise method, although calculations are limited to small lattice size. As a consequence, we can study the reliability of the thermodynamical quantities through the consistency of the two methods, each of which has different origin of the application limit. The thermodynamical quantities are obtained from simulations on a $8^3\times 4$ lattice with an intermediate quark mass($m_{\rm PS}/m_{\rm V}=0.8)$. The MPR and Taylor expansion are consistent for the EoS and number density up to $μ/T\sim 0.8$ and for the number susceptibility up to $μ/T \sim 0.6$. This implies within a given statistics that the overlap problem for the MPR and truncation error for the Taylor expansion method are negligible in these regions. In order to make MPR methods work, the fluctuation of the reweighting factor should be small. We derive the equation of the reweighting line where the fluctuation is small, and show that the equation of the reweighting line is consistent with the fluctuation minimum condition.

hep-lat↗

Development of Lattice QCD Tool Kit on Cell Broadband Engine Processor

We report an implementation of a code for SU(3) matrix multiplication on Cell/B.E., which is a part of our project, Lattice Tool Kit on Cell/B.E.. On QS20, the speed of the matrix multiplication on SPE in single precision is 227GFLOPS and it becomes 20GFLOPS {this vaule was remeasured and corrcted.} together with data transfer from main memory by DNA transfer, which is 4.6% of the hardware peak speed (460GFLOPS), and is 7.4% of the theoretical peak speed of this calculation (268.77GFLOPS). We briefly describe our tuning procedure.

hep-lat↗

Lattice QCD and High Baryon Density State

We report our recent studies on the finite density QCD obtained from lattice QCD simulation with clover-improved Wilson fermions of two flavor and RG-improved gauge action. We approach the subject from two paths, i.e., the imaginary and real chemical potentials.

hep-lat↗

QCD Phase Diagram with Imaginary Chemical Potential

We report our recent results on the QCD phase diagram obtained from the lattice QCD simulation. The location of the phase boundary between hadronic and QGP phases in the two-flavor QCD phase diagram is investigated. The imaginary chemical potential approach is employed, which is based on Monte Carlo simulations of the QCD with imaginary chemical potential and analytic continuation to the real chemical potential region.

hep-lat↗

Imaginary Chemical Potential Approach for the Pseudo-Critical Line in the QCD Phase Diagram with Clover-Improved Wilson Fermions

The QCD phase diagram is studied in the lattice QCD simulation with the imaginary chemical potential approach. We employ a clover-improved Wilson fermion action of two-flavors and a renormalization-group improved gauge action, and perform the simulation at an intermediate quark mass on a $8^3\times 4$ lattice. The QCD phase diagram in the imaginary chemical potential $μ_I$ region is investigated by performing the simulation for more than 150 points on the $(β,μ_I)$ plane. We find that the Roberge-Weiss phase transition at $μ_I/T=π/3$ is first order and its endpoint is second order, which are identified by the phase of the Polyakov loop. We determine the pseudo-critical line from the susceptibility of the Polyakov loop modulus. We find a clear deviation from a linear dependence of the pseudo-critical line on $μ_I^2$.

hep-lat↗

Wilson Fermion Determinant in Lattice QCD

We present a formula for reducing the rank of Wilson fermions from $4 N_c N_x N_y N_z N_t$ to $4 N_c N_x N_y N_z$ keeping the value of its determinant. We analyse eigenvalues of a reduced matrix and coefficients $C_n$ in the fugacity expansion of the fermion determinant $\sum_n C_n (\exp(μ/T))^n$, which play an important role in the canonical formulation, using lattice QCD configurations on a $4^4$ lattice. Numerically, $\log |C_n|$ varies as $N_x N_y N_z$, and goes easily over the standard numerical range; We give a simple cure for that. The phase of $C_n$ correlates with the distribution of the Polyakov loop in the complex plain. These results lay the groundwork for future finite density calculations in lattice QCD.

hep-lat↗

Quartet of spin-3/2 baryons in chiral multiplet $(1, 1/2) \oplus (1/2, 1) $ with mirror assignment

We study the possible existence of chiral partners in the spin-$\thalf$ sector of the baryon spectrum. We consider a quartet scheme where four spin-3/2 baryons, $P_{33}$, $D_{33}$, $D_{13}$ and $P_{13}$, group into higher-dimensional chiral multiplets $(1, \half)\oplus (\half,1)$ with a mirror assignment. With an effective $SU(2)_R\times SU(2)_L$ Lagrangian, we derive constraints imposed by chiral symmetry together with the mirror assignment on the masses and coupling constants of the quartet. Using the effective Lagrangian, we try to find a set of baryons suitable for the chiral quartet. It turns out that two cases reasonably agree with the mass pattern of the quartet: ($Δ(1600)$, $Δ(1940)$, $N(1520)$, $N(1720)$) and ($Δ(1920)$, $Δ(1940)$, $N(2080)$, $N(1900)$).

hep-ph↗

On the two-boson exchange corrections to parity-violating elastic electron-proton scattering

The details of the calculation of the two-boson exchange effects in the parity-violating elastic $ep$ scattering within a simple hadronic model, including both the nucleon and $Δ(1232)$-resonance intermediate states, are presented. We examine the sensitivity of our results with respect to choice of form factors. We emphasize the importance to use correct relations relating N to $Δ$ and $Δ$ to N transition vertex functions. The $NΔ$ Coulomb quadrupole transition is found to play important role at higher $Q^2\geq 3.0$ GeV$^2$. We also elucidate the relation between our results and the well-known result on the $γZE$ effect given by Marciano and Sirlin (MS). The effect of the nucleon contribution $δ_N$ to parity-asymmetry $A_{PV}$, is found to be in general, larger than the corresponding $Δ$ contribution $δ_Δ$ except at extreme forward angles. The corrections to the extracted values of the strange form factors $G^{s}_{E}+βG^{s}_{M}$ from the HAPPEX, A4, and G0 data are also presented. The total TBE corrections to the extracted values of $G^{s}_{E}+βG^{s}_{M}$ in recent experiments of HAPPEX G0, and A4 are, depending on kinematics, found to be small except in a few cases where they range from -20.6% to $48.3 %$.

nucl-th↗

Wilson fermions with imaginary chemical potential

We study the phase structure of imaginary chemical potential. We calculate the Polyakov loop using clover-improved Wilson action and renormalization improved gauge action. We obtain a two-state signals indicating the first order phase transition for $β= 1.9, μ_I = 0.2618, κ=0.1388$ on $8^3\times 4$ lattice volume We also present a result of the matrix reduction formula for the Wilson fermion.

hep-lat↗

Contribution of Two-Boson-Exchange with $Δ(1232)$ Excitation to Parity-Violating Elastic Electron-Proton Scattering

We study the leading electroweak corrections in the precision measurement of the strange form factors. Specifically, we calculate the two-boson-exchange (TBE), two-photon-exchange (TPE) plus $γZ$-exchange ($γZ$E), corrections with $Δ(1232)$ excitation to the parity-violating asymmetry of the elastic electron-proton scattering. The interplay between nucleon and $Δ$ contributions is found to depend strongly on the kinematics, as $δ_Δ$ begins as negligible at backward angles but becomes very large and negative and dominant at forward angles, while $δ_N$ always stays positive and decreases monotonically with increasing $ε$. The total TBE corrections to the extracted values of $G^{s}_{E}+βG^{s}_{M}$ in recent experiments of HAPPEX and G0 are, depending on kinematics, found to be large and range between 13% to -75% but small in the case of A4 experiments.

nucl-th↗

The Two-Boson-Exchange Correction to Parity-Violating Elastic Electron-Proton Scattering

We calculate the two-boson-exchange (TBE) corrections to the parity-violating asymmetry of the elastic electron-proton scattering in a simple hadronic model including the nucleon and the $Δ(1232)$ intermediate states. We find that $Δ$ contribution $δ_Δ$ is, in general, comparable with the nucleon contribution $δ_N$ and the current experimental measurements of strange-quark effects in the proton neutral weak current. The total TBE corrections to the current extracted values of $G^{s}_{E}+βG^{s}_{M}$ in recent experiments are found to lie in the range of $-7\sim +7%$.

nucl-th↗

Origin of Generalized Adler-Weisberger Sum Rule for the Nucleon and $Δ(1232)$

We derive a relation for the axial-coupling constants of the nucleon and spin-3/2 baryons including the $Δ(1232)$ with the use of an $SU(2)_R\times SU(2)_L$ invariant Lagrangian. Therein the nucleon belongs to the fundamental representation of the chiral group, while the spin-3/2 baryons belong to higher-dimensional representations $(1,\half)\oplus (\half,1)$. The resulting relation reproduces the one derived from the generalized Adler-Weisberger (GAW) sum rule for the forward $πN$ scattering. We clarify the origin of the GAW sum rule for the nucleon and $Δ$ by taking into account both the group-theoretical aspects and the spontaneous breaking of chiral symmetry. It turns out that the GAW sum rule for the nucleon and $Δ$ is a consequence of the existence of interactions involving a derivative-pion-field and spontaneous chiral symmetry breaking. This implies that the couplings between $N$ and $Δ$ in the GAW sum rule vanish with the change of the chiral condensate towards chiral restoration.

hep-ph↗

Chiral Properties of Baryon Fields with Flavor SU(3) Symmetry

We investigate chiral properties of local (non-derivative) fields of baryons consisting of three quarks with flavor SU(3) symmetry. We construct explicitly independent local three-quark fields belonging to definite Lorentz and flavor representations. Chiral symmetry is spontaneously broken and therefore the baryon fields can have different chiral representations. It turns out that the allowed chiral representations are strongly correlated with the Lorentz group representations due to the color and spatial structure of the local three-quark fields. We discuss some implications of the allowed chiral symmetry representations on phenomenological Lagrangians with chiral U(3)_L \otimes U(3)_R symmetry.

hep-ph↗

Structure of the Roper Resonance with Diquark Correlations

We study electromagnetic properties of the nucleon and Roper resonance in a chiral quark-diquark model including two kinds of diquarks needed to describe the nucleon: scalar and axial-vector diquarks. The nucleon and Roper resonance are described as superpositions of two quark-diquark bound states of a quark and a scalar diquark and of a quark and an axial-vector diquark. Electromagnetic form factors of the nucleon and Roper resonance are obtained from one-loop diagrams where the quark and diquarks are coupled by a photon. We include the effects of intrinsic properties of the diquarks: the intrinsic form factors both of the diquarks and the anomalous magnetic moment of the axial-vector diquark. The electric form factors of the proton and neutron reasonably agree with the experiments due to the inclusions of the diquark sizes, while the magnetic moments become smaller than the experimental values because of the scalar dominance in the nucleon. The charge radii of the Roper resonance are almost comparable with those of the nucleon.

hep-ph↗

Chiral Properties of Baryon Interpolating Fields

We study the chiral transformation properties of all possible local (non-derivative) interpolating field operators for baryons consisting of three quarks with two flavors, assuming good isospin symmetry. We derive and use the relations/identities among the baryon operators with identical quantum numbers that follow from the combined colour, Dirac and isospin Fierz transformations. These relations reduce the number of independent baryon operators with any given spin and isospin. The Fierz identities also effectively restrict allowed baryon chiral multiplets. It turns out that the chiral multiplets of the baryons are equivalent to their Lorentz representation. For the two independent nucleon operators the only permissible chiral multiplet is the fundamental one $(\frac12,0)\oplus(0,\frac12)$. For the $Δ$, admissible Lorentz representations are $(1,\frac12)\oplus (\frac12,1)$ and $(\frac32,0)\oplus(0,\frac32)$. In the case of the $(1,\frac12)\oplus (\frac12,1)$ chiral multiplet the $I(J)=\frac32(\frac32)$ $Δ$ field has one $I(J)=\frac12(\frac32)$ chiral partner; otherwise it has none. We also consider the Abelian ($U_A(1)$) chiral transformation properties of fields and show that each baryon comes in two varieties: 1) with Abelian axial charge +3; and 2) with Abelian axial charge -1. In case of the nucleon these are the two Ioffe's fields; in case of the $Δ$, the $(1,\frac12)\oplus (\frac12,1)$ multiplet has Abelian axial charge -1 and the $(\frac32,0)\oplus(0,\frac32)$ multiplet has Abelian axial charge +3.

hep-ph↗

Two Nucleon-States in a Chiral Quark-Diquark Model

We study the ground and first excited states of nucleons in a chiral quark-diquark model. We include two quark-diquark channels of the scalar-isoscalar and axial-vector-isovector types for the nucleon states. The diquark correlation violating the spin-flavor SU(4)$_{SF}$ symmetry allows to treat the two quark-diquark channels independently. Hence the two states appear as the superpositions of the two quark-diquark channels; one is the nucleon and the other is a state which does not appear in the SU(4)$_{SF}$ quark models. With a reasonable choice of model parameters, the mass of the excited state appears at around 1.5 GeV, which we identify with the Roper resonance N(1440).

hep-ph↗

The Nucleon and Roper Resonance in a Chiral Quark Diquark Model

A description of the nucleon and Roper resonance in a quark-diquark approach is presented. We show that two states with the quantum number of the nucleon can appear in the ground state of the spatial configuration, when there are two types of diquarks: scalar-isoscalar and axial-vector-isovector diquarks. The mass difference between the two states is generated by the mass difference between the two diquarks, which is due to the spin-spin interaction between the two quarks in the diquarks. The two states are then identified with the nucleon and Roper resonance.

hep-ph↗