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Satoshi Nakajima

Publications and source records attributed to Satoshi Nakajima.

15 recordsLinked to original sources

Deriving Feynman's Consistency Condition from His Abandoned Energy--Momentum Approach

Feynman briefly considered a nonlinear theory of gravity in flat spacetime by imposing energy--momentum conservation on the sum of the energy--momentum tensor of matter and that of the gravitational field. He used the symmetrized canonical energy-momentum tensor as the energy--momentum tensor of the gravitational field.He reported that the resulting construction gave an incorrect value for Mercury's perihelion precession and abandoned this route in favor of a variational argument based on dynamical consistency. We reconsider the abandoned route. The key step is to identify the gravitational energy--momentum tensor not with the conventional Belinfante tensor, which becomes symmetric upon use of the field equations, but with its off--shell Belinfante--Rosenfeld tensor, which contains explicit Euler--Lagrange terms. If we apply the law of conservation of energy and momentum to the sum of this tensor and the matter energy-momentum tensor, we obtain Feynman's consistency condition.Thus Feynman's dynamical-consistency argument and the reconstructed energy--momentum argument, although based on different physical assumptions, yield the same identity. The Euler--Lagrange terms are essential to this result.

gr-qc

A Note on the Feynman Lectures on Gravitation

Following Feynman's lectures on gravitation, we consider the theory of the gravitational (massless spin-2) field in flat spacetime and present the third- and fourth-order Lagrangian densities for the gravitational field. In particular, we present detailed calculations for the third-order Lagrangian density. We point out that the expression for the third-order Lagrangian density which Feynman provided is not a solution of Feynman's condition that the third-order Lagrangian density must satisfy. However, Feynman's third-order Lagrangian density gives the correct perihelion shift.

hep-th

Speed-Accuracy Trade-Off Relations in Quantum Measurements and Computations

In practical measurements, it is widely recognized that reducing the measurement time leads to decreased accuracy. However, whether an inherent speed-accuracy trade-off exists as a fundamental physical constraint for quantum measurements is not obvious, and the answer remains unknown. Here, we establish a fundamental speed-accuracy trade-off relation based on the energy conservation law and the locality. Our trade-off works as a no-go theorem that the zero-error measurement for the operators that are non-commutative with the Hamiltonian cannot be implemented with finite time. This relation universally applies to various existing errors and disturbances defined for quantum measurements. We furthermore apply our methods to quantum computations and provide another speed-accuracy trade-off relation for unitary gate implementations, which works as another no-go theorem that any error-less implementations of quantum computation gates changing energy cannot be implemented with finite time, and a speed-disturbance trade-off for general quantum operations.

cond-mat.stat-mech

Improvement of Speed Limits: Quantum Effect on the Speed in Open Quantum Systems

In the context of quantum speed limits, it has been shown that the minimum time required to cause a desired state conversion via the open quantum dynamics can be estimated using the entropy production. However, the established entropy-based bounds tend to be loose, making it difficult to accurately estimate the minimum time for evolution. In this research, we have combined the knowledge of the entropy-based speed limits with that of the resource theory of asymmetry (RTA) and provided much stricter inequalities. Our results show that the limitation on the change rate of states and expectation values can be divided into two parts: quantum coherence for energy (i.e., asymmetry) contributed by the system and the heat bath and the classical entropy-increasing effect from the bath. As a result, our inequalities demonstrate that the difference in the speed of evolution between classical and quantum open systems, i.e., the quantum enhancement in speed, is determined by the quantum Fisher information, which measures quantum fluctuations of energy and serves as a standard resource measure in the resource theory of asymmetry. We further show that a similar relation holds for the rate of change of expectation values of physical quantities.

quant-ph

SLD Fisher information for kinetic uncertainty relations

We investigate a symmetric logarithmic derivative (SLD) Fisher information for kinetic uncertainty relations (KURs) of open quantum systems described by the GKSL quantum master equation with and without the detailed balance condition. In a quantum kinetic uncertainty relation derived by Vu and Saito [Phys. Rev. Lett. 128, 140602 (2022)], the Fisher information of probability of quantum trajectory with a time-rescaling parameter plays an essential role. This Fisher information is upper bounded by the SLD Fisher information. For a finite time and arbitrary initial state, we derive a concise expression of the SLD Fisher information, which is a double time integral and can be calculated by solving coupled first-order differential equations. We also derive a simple lower bound of the Fisher information of quantum trajectory. We point out that the SLD Fisher information also appears in the speed limit based on the Mandelstam-Tamm relation by Hasegawa [Nat. Commun. 14, 2828 (2023)]. When the jump operators connect eigenstates of the system Hamiltonian, we show that the Bures angle in the interaction picture is upper bounded by the square root of the dynamical activity at short times, which contrasts with the classical counterpart.

cond-mat.stat-mech

Noether currents and generators of local gauge transformations in the covariant canonical formalism

We investigate generators of local transformations in the covariant canonical formalism (CCF). The CCF treats space and time on an equal footing regarding the differential forms as the basic variables. The conjugate forms $π_A$ are defined as derivatives of the Lagrangian $d$-form $L(ψ^A, dψ^A)$ with respect to $dψ^A$, namely $π_A := \partial L/\partial dψ^A$, where $ψ^A $ are $p$-form dynamical fields. The form-canonical equations are derived from the form-Legendre transformation of the Lagrangian form $H:=dψ^A \wedge π_A - L$. We show that the Noether current form is the generator of an infinitesimal transformation $ψ^A \to ψ^A + δψ^A$ if the transformation of the Lagrangian form is given by $δL=dl$ and $δψ^A$ and $l$ depend on only $ψ^A$ and the parameters. As an instance, we study the local gauge transformation for the gauge field and the local Lorentz transformation for the second order formalism of gravity.

gr-qc

Speed limits of the trace distance for open quantum system

We investigate the speed limit of the state transformation in open quantum systems described by the Lindblad type quantum master equation. We obtain universal bounds of the total entropy production described by the trace distance between the initial and final states in the interaction picture. Our bounds can be tighter than the bound of Vu and Hasegawa [Phys. Rev. Lett. 126, 010601 (2021)] which measures the distance by the eigenvalues of the initial and final states: This distance is less than or equal to the trace distance. For this reason, our results can significantly improve Vu-Hasegawa's bound. The trace distance in the Schrödinger picture is bounded by a sum of the trace distance in the interaction picture and the trace distance for unitary dynamics described by only the Hamiltonian in the quantum master equation.

cond-mat.stat-mech

Generators of local gauge transformations in the covariant canonical formalism of fields

We investigate generators of local gauge transformations in the covariant canonical formalism (CCF) for matter fields, gauge fields and the second order formalism of gravity. The CCF treats space and time on an equal footing regarding the differential forms as the basic variables. The conjugate forms $π_A$ are defined as derivatives of the Lagrangian $d$-form $L(ψ^A, dψ^A)$ with respect to $dψ^A$, namely $π_A := \partial L/\partial dψ^A$, where $ψ^A $ are $p$-form dynamical fields. The form-canonical equations are derived from the form-Legendre transformation of the Lagrangian form $H:=dψ^A \wedge π_A - L$. We show that the generator of the local gauge transformation in the CCF is given by $\varepsilon^r G_r + d\varepsilon^r \wedge F_r$ where $\varepsilon^r$ are infinitesimal parameters and $G_r$ are the Noether currents which are $(d-1)$-forms. $\{G_r , G_s \} = f^t_{\ rs}G_t$ holds where $\{\bullet, \bullet \}$ is the Poisson bracket of the CCF and $f^t_{\ rs}$ are the structure constants of the gauge group. For the gauge fields and the gravity, $G_r=-\{F_r, H \}$ holds. For the matter fields, $F_r=0$ holds.

gr-qc

Asymptotic expansion of the solution of the master equation and its application to the speed limit

We investigate an asymptotic expansion of the solution of the master equation under the modulation of control parameters. In this case, the non-decaying part of the solution becomes the dynamical steady state expressed as an infinite series using the pseudo-inverse of the Liouvillian, whose convergence is not granted in general. We demonstrate that for the relaxation time approximation model, the Borel summation of the infinite series is compatible with the exact solution. By exploiting the series expansion, we obtain the analytic expression of the heat and the activity. In the two-level system coupled to a single bath, under the linear modulation of the energy as a function of time, we demonstrate that the infinite series expression is the asymptotic expansion of the exact solution. The equality of a trade-off relation between the speed of the state transformation and the entropy production (Shiraishi, Funo, and Saito, Phys. Rev. Lett. ${\bf 121}$, 070601 (2018)) holds in the lowest order of the frequency of the energy modulation in the two-level system. To obtain this result, the heat emission and absorption at edges (the initial and end times) or the differences of the Shannon entropy between the instantaneous steady state and the dynamical steady state at edges are essential: If we ignore these effects, the trade-off relation can be violated.

cond-mat.stat-mech

Theoretical studies on quantum pump and excess entropy production: Quantum master equation approach

In this thesis, we considered quantum systems coupled to several baths. We supposed that the system state is governed by the quantum master equation (QME). We investigated the quantum pump and the excess entropy production. In the first half of the thesis, we investigated the quantum pump using the full counting statistics with quantum master equation (FCS-QME) approach. In the latter part of the thesis, we investigated the excess entropy production. The average entropy production is composed of the time integral of the instantaneous steady entropy production rate and the excess entropy production. We define average entropy production rate using the average energy and particle currents, which are calculated by using the full counting statistics with QME. The excess entropy production is given by a line integral in the control parameter space and its integrand is called the Berry-Sinitsyn-Nemenman (BSN) vector. In the weakly nonequilibrium regime, we show that BSN vector is described by $\ln ρ_0^{(-1)}$ and $ρ_0$ where $ρ_0$ is the instantaneous steady state of the QME and $ρ_0^{(-1)}$ is that of the QME which is given by reversing the sign of the Lamb shift term. In general, the potential dose not exist. The origins of the non-existence of the potential are a quantum effect (the Lamb shift) and the breaking of the time-reversal symmetry. The non-existence of the potential means that the excess entropy essentially depends on the path of the modulation. If the system Hamiltonian is non-degenerate or the Lamb shift term is negligible, the excess entropy production approximately reduces to the difference between the von Neumann entropies of the system. We pointed out that the expression of the entropy production obtained in the classical Markov jump process is different from our result and showed that these are approximately equivalent only in the weakly nonequilibrium regime.

cond-mat.stat-mech

Excess entropy production in quantum system: Quantum master equation approach

For open systems described by the quantum master equation (QME), we investigate the excess entropy production under quasistatic operations between nonequilibrium steady states. The average entropy production is composed of the time integral of the instantaneous steady entropy production rate and the excess entropy production. We propose to define average entropy production rate using the average energy and particle currents, which are calculated by using the full counting statistics with QME. The excess entropy production is given by a line integral in the control parameter space and its integrand is called the Berry-Sinitsyn-Nemenman (BSN) vector. In the weakly nonequilibrium regime, we show that BSN vector is described by $\ln \breveρ_0$ and $ρ_0$ where $ρ_0$ is the instantaneous steady state of the QME and $\breveρ_0$ is that of the QME which is given by reversing the sign of the Lamb shift term. If the system Hamiltonian is non-degenerate or the Lamb shift term is negligible, the excess entropy production approximately reduces to the difference between the von Neumann entropies of the system. Additionally, we point out that the expression of the entropy production obtained in the classical Markov jump process is different from our result and show that these are approximately equivalent only in the weakly nonequilibrium regime.

cond-mat.stat-mech

Quantum adiabatic pumping by modulating tunnel phase in quantum dots

In a mesoscopic system, under zero bias voltage, a finite charge is transferred by quantum adiabatic pumping by adiabatically and periodically changing two or more control parameters. We obtained expressions for the pumped charge for a ring of three quantum dots (QDs) by choosing the magnetic flux penetrating the ring as one of the control parameters. We found that the pumped charge shows a steplike behavior with respect to the variance of the flux. The value of the step heights is not universal but depends on the trajectory of the control parameters. We discuss the physical origin of this behavior on the basis of the Fano resonant condition of the ring.

cond-mat.mes-hall

Interaction effect on adiabatic pump of charge and spin in quantum dot

We investigate the pumped charge and spin at zero-bias by adiabatic modulation of two control parameters using the full counting statistics with quantum master equation approach. First we study higher order effects of the pumping frequency in general Markov systems and show the equivalence between our approach and the real-time diagrammatic approach. An adiabatic modulation of the control parameters induces the Berry-Sinitsyn-Nemenman (BSN) phase. We show that the origin of the BSN phase is a non-adiabatic effect. The adiabatically pumped charge (spin) is given by a summation of (i) a time integral of the instantaneous steady charge (spin) current and (ii) a geometric surface integral of the BSN curvature, which results from the BSN phase. In quantum dots (QDs) weakly coupled to two leads, we show that (i) is usually dominant if the thermodynamic parameters are modulated although it is zero if the thermodynamic parameters are fixed to zero-bias. To observe the spin effects, we consider collinear magnetic fields, which relate to spins through the Zeeman effect, with different amplitudes applying to the QDs and the leads. For interacting one level QD, we calculate analytically the pumped charge and spin by modulating the magnetic fields and the coupling strengths to the leads in the weak and strong interacting limits. We show that the difference between these two limits appears through the averages of the numbers of the electron with up and down spin in the QD. For the quantum pump by the modulation of the magnetic fields of the QD and one lead, the energy-dependences of linewidth functions, which are usually neglected, are essential.

cond-mat.mes-hall

Reconsideration of De Donder-Weyl theory by covariant analytic mechanics

We show that the covariant analytic mechanics (CAM) is closely related to the De Donder-Weyl (DW) theory. To treat space and time on an equal footing, the DW theory introduces $D$ conjugate fields ($D$ is the dimension of space-time) for each field and the CAM regards the differential forms as the basic variables. The generalization of the canonical equations is called the DW equations. Although one of the DW equations is not correct for the gauge field and the gravitational field, we show the way to improve it. By rewriting the canonical equations of the CAM, which are manifestly general coordinate covariant and gauge covariant, using the components of the tensors, we show that these are equivalent to the improved DW equations. Additionally, we investigate the Dirac field. We present a modified Hamilton formalism which regards only the Dirac fields as the basic variables and show that it provides the Dirac equations correctly.

gr-qc

Application of covariant analytic mechanics with differential forms to gravity with Dirac field

We apply the covariant analytic mechanics with the differential forms to the Dirac field and the gravity with the Dirac field. The covariant analytic mechanics treats space and time on an equal footing regarding the differential forms as the basic variables. A significant feature of the covariant analytic mechanics is that the canonical equations, in addition to the Euler-Lagrange equation, are not only manifestly general coordinate covariant but also gauge covariant. Combining our study and the previous works (the scalar field, the abelian and non-abelian gauge fields and the gravity without the Dirac field), the applicability of the covariant analytic mechanics is checked for all fundamental fields. We study both the first and second order formalism of the gravitational field coupled with matters including the Dirac field. It is suggested that gravitation theories including higher order curvatures cannot be treated by the second order formalism in the covariant analytic mechanics.

gr-qc