A Computational details

Exploring Zeptosecond Quantum Equilibration Dynamics: From Deep-Inelastic to Fusion-Fission Outcomes in Ni+Ni Reactions


Energy dissipative processes play a key role in how quantum many-body systems dynamically evolve towards equilibrium. In closed quantum systems, such processes are attributed to the transfer of energy from collective motion to single-particle degrees of freedom; however, the quantum many-body dynamics of this evolutionary process are poorly understood. To explore energy dissipative phenomena and equilibration dynamics in one such system, an experimental investigation of deep-inelastic and fusion-fission outcomes in the Ni+Ni reaction has been carried out. Experimental outcomes have been compared to theoretical predictions using Time Dependent Hartree Fock and Time Dependent Random Phase Approximation approaches, which respectively incorporate one-body energy dissipation and fluctuations. Excellent quantitative agreement has been found between experiment and calculations, indicating that microscopic models incorporating one-body dissipation and fluctuations provide a potential tool for exploring dissipation in low-energy heavy ion collisions.

The dynamic evolution of perturbed quantum many-body systems towards equilibrium is a topic of great interest in many fields, including quantum information Suter and Álvarez (2016), condensed matter Polkovnikov et al. (2011); Gring et al. (2012); Aoki et al. (2014); Eisert et al. (2015), and nuclear physics Hinde et al. (2010); Simenel (2011); Aritomo et al. (2012); Lacroix, Denis and Ayik, Sakir (2014); Umar et al. (2015). Energy dissipation—the transfer of energy from collective motion to internal or external degrees of freedom—shapes this dynamic evolution, playing a significant role in whether and how such complex systems achieve full equilibration. To date, a great deal of effort has focused on quantum systems in which energy dissipation is brought about via contact with an external environment (e.g., gas, photons, etc.) Barontini et al. (2013); de Vega and Alonso (2017). Much less is known about energy dissipation that arises from internal degrees of freedom Polkovnikov et al. (2011); Eisert et al. (2015); Clos et al. (2016).

One testing ground for the exploration of energy dissipation due to internal degrees of freedom can be found in heavy ion collisions. The nuclear collision process results in a closed composite quantum system that is isolated from external environments during the time of the collision (a timescale of several zeptoseconds, prior to particle emission), rapidly evolves towards equilibration in many degrees of freedom, and undergoes significant excitation and internal rearrangement throughout the equilibration process. Through the manipulation of collision entrance channel parameters (projectile-target combinations and energies), a range of factors with the potential to affect energy dissipation can be explored. Typical timescales for energy dissipation in such systems could in principle vary from isospin and mass equilibration times on the order of 0.3-0.5 zs Jedele et al. (2017); Umar et al. (2017) and 5 zs Tōke et al. (1985); du Rietz et al. (2013), respectively.

In nuclear reactions, the observation of the total kinetic energy of the reaction products (TKE) offers a direct measure of energy dissipation. The observation of the masses of reaction products via direct or indirect methods offers a measure of system equilibration in a key degree of freedom, and can be used to explore fluctuations in reaction product masses as a function of TKE. One or both observables have often been used to explore energy dissipative outcomes in nuclear physics (see, e.g. Schröder and Huizenga (1984)). In this work, we will explore the TKE and mass degrees of freedom for binary outcomes of collisions between Ni and Ni at energies near the Coulomb barrier.

We have chosen to study low-energy collisions between Ni and Ni for several reasons. First, the entrance channel is close to symmetry. This means we can focus on quantum fluctuations without taking into account macroscopic mass drift effects while avoiding the experimental difficulties that come with symmetric reactions (e.g. normalization with Mott scattering, indistinguishability of projectile-like and target-like outcomes). Second, the system is relatively heavy—meaning it truly qualifies as a composite many-body system—but is still light enough that the charge product, and thus, the Coulomb repulsion, of the system is fairly small, allowing for long contact times. Most importantly, the system is accessible via both experiment and theory, using stable heavy ion beams in the former case, and microscopic approaches employing one-body dissipation (Time-Dependent Hartree Fock, or TDHF Dirac (1930)) and fluctuations (Time Dependent Random Phase Approximation, or TDRPA Balian and Vénéroni (1984)) in the latter.

The Ni+Ni experiment was performed at the ANU Heavy Ion Accelerator Facility (HIAF) using the 14UD tandem accelerator, CUBE two-body fission spectrometer Hinde et al. (1996) and two monitor detectors at 18 for cross section normalization. The Ni beam impinged upon the 60 /cm-thick Ni target for 20 separate beam energies ranging from 194-270 MeV. The CUBE spectrometer’s two large-area multiwire proportional counters (each 27.9 cm wide, 35.7 cm high) were placed at forward angles relative to the beam axis and a distance of 22.24 cm from the target. The detectors provided energy loss, time of flight, and position information with a resolution of 1 mm. From this, a full kinematic reconstruction of each two-body event was performed using the kinematic coincidence method Hinde et al. (1996); Rafiei et al. (2008), providing total kinetic energy (TKE), mass ratio , where are the masses of the two fission fragments, and scattering angle information.

Figure 1: (Color online) Mass ratio distributions from the Ni+Ni reaction for a range of . In (a), a gate has been used to ensure full detector coverage. The thin vertical lines indicate the expected mass ratios for the projectile and target nuclei. The inset shows a zoomed-in version of the =0.83 mass ratio distribution on a linear scale. In (b), a gate has been placed on TKE that excludes 99 of the Rutherford scattered events, together with a gate that isolates mass ratios corresponding to the region where fusion-fission events are expected to be found. The orange line shows Ni+Ni data at without angle or TKE gate. No background subtraction has been applied to any of these mass distributions.

Calibrations were performed with a Ni beam of 158.4 MeV bombarding (50, 60)-g/cm Ni targets. Mott or Rutherford scattering were used to calibrate the geometry of the setup, define the mass-ratio resolution of CUBE, and provide a solid angle calibration for cross section measurements.

Figure 1 shows the evolution of mass ratio distributions observed for Ni+Ni with , or energy relative to the experimental fusion barrier =96.87 MeV Rodríguez et al. (2010) in the center-of-mass frame. In Fig. 1 (a), an angular acceptance of has been used to exclude regions where detector coverage is incomplete. The lowest energy distribution (red line, ), exhibits a double-peaked structure as highlighted by the linear scale inset of the same data. This is consistent with expectation for elastically scattered projectile () and target () nuclei. As is increased, the double peak becomes a single peak due to mass equilibration, and the previously narrow mass ratio distribution develops a second, wide component.

In Fig. 1 (b), the wide component of the mass-ratio distribution at higher energies is highlighted by applying two gates: one around that minimizes elastic and deep-inelastic events, and one below TKE = MeV that excludes 99 of the Rutherford scattering events. As beam energy increases, the narrow (wide) component of the mass ratio distribution decreases (increases) in yield. At the highest energy, almost no trace of the narrow component remains. For reference, the Ni + Ni mass ratio (orange) shows the experimental mass-ratio resolution for an individual nuclide.

Figure 2: (Color online) Scattering angle versus total kinetic energy (TKE) differential cross section distributions TKE for Ni + Ni at three different energies overlaid with (, TKE) impact parameter trajectories calculated with TDHF. (Diamond symbols) Ni+Ni, where black diamonds are projectile-like fragments (PLF), white diamonds are target-like fragments (TLF); (Dotted lines) Ni+Ni. Differential cross sections are only a lower limit outside of the range of due to detector angular coverage. The impact parameter for selected points along the TDHF trajectories are shown.

To identify the various reaction outcomes contributing to the mass-ratio spectra in Fig. 1, the experimental TKE information must also be considered as it provides information on whether energy dissipation has occurred. In Fig. 2, versus TKE is shown for three representative energies (overlaid with calculations, to be discussed below). The highest intensity (light yellow) regions at high TKE values are consistent with elastic scattering energies. Events with lower TKE values, present in each case (for example, below 110 MeV in Fig. 1 (a)), provide evidence of energy dissipative reaction processes as early as . Such events could correspond to either deep-inelastic or fusion-fission outcomes.

The main distinguishing experimental features for deep-inelastic and fusion-fission processes here are that fusion-fission outcomes should have full energy dissipation (e.g. appear in a flat TKE band, like that seen in Fig. 2(c) around 80 MeV) and exhibit a wide mass distribution (indicating that significant mass transfer has occurred), while deep-inelastic collisions only need to show energy dissipation relative to expected elastic scattering TKE values and may involve only a small amount of mass transfer (i.e. the incoming and outgoing reaction channel masses can be similar). From Fig. 1(b), it is clear that the wide mass ratio component of the data (which is consistent with fusion-fission) does not become important until . Based on the experimental information alone, it is unclear whether the wide mass-ratio distributions observed in Fig. 1 are solely due to fusion-fission, a deep-inelastic process, or some combination of the two.

To explore the relationship between experimental observables (, TKE) and impact parameter , and to examine the origin of the wide mass ratio component, microscopic approaches TDHF and TDRPA have been used. TDHF is a mean-field approach incorporating one-body dissipation that has previously been used to explore dynamical reaction processes such as quasifission Simenel et al. (2012); Simenel (2012); Wakhle et al. (2014); Oberacker et al. (2014); Umar et al. (2015); Hammerton et al. (2015); Sekizawa and Yabana (2016); Umar et al. (2016). In this work, a 3D TDHF code Sekizawa and Yabana (2013, 2016), employing the SLy4d parametrization Kim et al. (1997) of the Skyrme energy-density functional Skyrme (1956) has been used to explore reaction outcomes for Ni+Ni at the three representative energies shown in Fig. 2. The code has been extended and also used for the TDRPA calculations.

TDHF calculations were performed for a reaction timescale of 13 zeptoseconds, and the minimum impact parameter for each calculation set was chosen to correspond to the minimum value at which the di-nuclear system was observed to reseparate into two components over this timescale. Below these minimum impact parameters, it is assumed that fusion is the most probable outcome—an assumption that is supported by calculated moments of inertia for impact parameters below the minimum range, which indicated convergence towards a compact system (see Supplemental Material SM ()). The maximum impact parameter for all calculations was chosen to be 10 fm. In Fig. 2, each experimental dataset has been overlaid with the results of these TDHF calculations. Each diamond pair represents the calculated average and TKE value obtained from a given impact parameter calculation for the Ni+Ni reactions. Impact parameters corresponding to selected points along these trajectories in (, TKE)-space have been noted; we will henceforth call these trajectories in (, TKE)-space “impact parameter trajectories”. Both reactions yield a similar evolution in (,TKE)-space. For the three representative calculations, the largest impact parameters (at high TKE values) result in little energy dissipation (yielding points near elastic scattering outcomes), while the smallest impact parameters (at low TKE values) exhibit significant energy dissipation. The impact parameters for each calculation are not evenly spaced to capture the rapid change in dynamics in the small impact parameter range.

As one can see from Fig. 2 (a-c), the TDHF impact parameter trajectories follow the trends in the data quite well over the full experimental angular range. Outcomes for small impact parameters exhibit increased energy dissipation and di-nuclear system rotation before re-separation relative to outcomes for large impact parameters. In the calculations, we define contact time as the time during which the density overlap between the fragments is 0.001 fm (selected to provide a smooth evolution in contact time as a function of , as discussed in SM ()). This generally increases as decreases, thus allowing more time for both rotation and energy dissipation to occur.

Figure 3: (Color online) (a) TDRPA and observed values are plotted as a function of calculated impact parameter for . For the experimental data, is obtained from a Gaussian fit of the mass ratio within a (,TKE) gate corresponding to the equivalent trajectory given by the symmetric calculation; the impact parameter for each point is assigned based on the symmetric trajectory. The error bars on the experimental points and the gray dashed line show the detector mass resolution obtained from the of the below-barrier Ni+Ni data, corresponding to the detector mass-ratio resolution for a single atomic mass. Because data points have been selected along the projectile-like branch of the trajectory, points at high TKE values (large ) are expected to approach the resolution limit. (b) TDHF contact time versus from TDRPA. The dotted line indicates maximum from experiment with the shaded region representing the detector mass-ratio resolution.

So far, we have found that the reaction outcomes are characterized by (i) strong TKE-angle correlations, and (ii) a transition between narrow and wide components in the fragment mass distributions. The next step is to investigate the correlation between energy dissipation and mass fluctuations in the fragments. Experimentally, we can achieve this by examining the evolution of , the standard deviation of a Gaussian fit to the mass ratio distribution along the TDHF impact parameter trajectories. To compare this to theory, we need to first examine the ability of microscopic theories to reproduce this evolution of along the impact parameter trajectories shown in Fig. 2.

Because of its mean-field nature, TDHF is optimized to calculate the average of one-body observables (e.g., fragment mass, charge), but underestimates their fluctuations Dasso et al. (1979). A realistic estimate of the latter can be obtained with TDRPA Balian and Vénéroni (1984), an extension of TDHF that successfully reproduced mass distribution widths in Ca+Ca Simenel (2011). The TDRPA dispersion formula can be derived from the stochastic mean-field approach Ayik (2008). TDRPA is used to calculate fluctuations in particle number in the fragments, which can be interpreted as a standard deviation only in the case of symmetric collisions. can then be used to compute the calculated equivalent of by dividing by the compound nucleus mass number. As Fig. 2 showed, the TDHF trajectories for Ni+Ni were found to be very similar; therefore, the calculated Ni+Ni trajectories and values will be used in the discussion below. For completeness, we have also computed fragment mass fluctuations in Ni+Ni with TDRPA, to see if the asymmetry is small enough to allow an interpretation of the TDRPA mass fluctuations as in this system. The details of this calculation can be found in SM ().

To compare calculations to observation, a series of scattering angle and TKE gates were placed on the data along the TDHF trajectories identified in Fig. 2. Each gate was centred on the and TKE value resulting from each TDHF impact parameter calculation where detector coverage was complete. The gate widths were chosen as follows: (i) TKE gate widths were 5 MeV, corresponding to the observed full-width-half-max of the TKE for elastic scattering events in the Ni+Ni calibration run at , and (ii) gate widths were , as this width yielded reasonable statistics in the mass distributions. The resulting experimental values are shown as a function of TDHF impact parameter in Fig. 3 (a) for the highest energy measurement. Here, decreases sharply over a narrow impact parameter range. The largest values, found at the smallest impact parameters, correspond to mass ratio widths consistent with those observed for fusion-fission outcomes in heavier systems (see, e.g., Knyazheva et al. (2007); Rafiei et al. (2008); Williams et al. (2013)).

The TDRPA results for Ni+Ni are also shown in Fig. 3 (a). The agreement between the theoretical (mass-symmetric) and experimental is remarkable, considering the fact that the only input of TDRPA (and TDHF) is the choice of the effective interaction. This conclusion holds for all three energies. For the reaction at =1.14 and minimum impact parameter = 3.8 fm, and ; for the reaction at =1.27 and minimum impact parameter = 5.0 fm, and . Experimental errors on given here originate from the detector resolution, as determined from the Ni+Ni calibration data. In both cases, experimental values then decrease quickly to the CUBE resolution limit as is increased.

The TDHF and TDRPA calculations also reveal something about the wide mass component of the highest energy reaction that the experimental data cannot: the reaction timescale. As shown in Fig. 3 (b), the widest calculated values result from reactions with longer contact times ( zeptoseconds). These calculated mass distribution widths are consistent with those observed for the wide mass component of our experimental data, supporting the idea that this wide mass component results from systems that have more time to undergo mass exchange prior to reseparation. This suggests that the wide mass ratio component of the experimental data could originate from both deep-inelastic and fusion-fission processes, where the 4 zeptosecond timescale applies to the former process and a much longer ( s) timescale to the latter. Remarkably, the fact that the largest calculated mass ratio widths could be consistent with those expected for fusion-fission, where full mass equilibration has by definition occurred, also suggests that full mass equilibration can be achieved over a timescale of only 4 zeptoseconds for this reaction. This timescale range is consistent with the 5-10 zs timescales observed for quasifission outcomes in some heavier systems Tōke et al. (1985); du Rietz et al. (2011, 2013).

In summary, this work illustrates the strong quantitative agreement between experiment and a quantum many-body approach including only a one-body dissipation mechanism for low-energy heavy ion collisions, supporting the idea that such approaches are highly appropriate for exploring energy dissipative processes in composite quantum many-body systems. The 4-zeptosecond timescale for the mass equilibrated deep-inelastic outcome, as calculated by TDRPA, suggests that the microscopic mechanisms driving mass equilibration can operate very rapidly in low-energy heavy ion reactions.

Acknowledgements: The authors thank the technical staff of the ANU Heavy Ion Accelerator Facility for their essential support during the experiments. The authors also acknowledge support from the Australian Research Council through Grants DE140100784, FT120100760, FL110100098, DP130101569, DP140101337, and DP160101254, from the NCRIS program for accelerator operations, and from the Polish National Science Centre (NCN) Grant, Decision No. DEC-2013/08/A/ST3/00708. This work used computational resources of the HPCI system (HITACHI SR16000/M1) provided by Information Initiative Center (IIC), Hokkaido University, through the HPCI System Research Projects (Project IDs: hp140010, hp150081, hp160062, and hp170007).

Supplemental Material for: “Exploring Zeptosecond Quantum Equilibration Dynamics: From Deep-Inelastic to Fusion-Fission Outcomes in Ni+Ni Reactions”

In this Supplemental Material, computational details of TDHF and TDRPA calculations are described. Supplemental results that show the reaction dynamics, the time-evolution of moment of inertia in fusing systems, and contact times are presented. We point out the difficulty of using TDRPA calculations for asymmetric systems. A short discussion on fluctuations and correlations in deep-inelastic reactions is provided.

Appendix A Computational details

For the TDHF calculations, we used a computational code developed in University of Tsukuba (41). In the code, single-particle orbitals are represented in three-dimensional Cartesian coordinates without any symmetry restrictions and with hard boundary conditions. The coordinate space is discretized into uniform grids with a mesh spacing of 0.8 fm. Spatial derivatives are evaluated by an 11-point finite-difference formula. For time evolution, a 4th-order Taylor-expansion method is used with  zs (1 zs  sec). The Coulomb potential is computed employing Fourier transformations.

For the energy density functional, we used the Skyrme SLy4d parameter set (42). TDHF calculations were performed for the Ni+Ni reactions at , 1.27, and 1.40. The Hartree-Fock ground state of Ni is slightly deformed in a prolate shape with , while that of Ni is of spherical shape. For the Ni+Ni reaction, the symmetry axis of Ni was always set perpendicular to the reaction plane. The initial separation distance between projectile and target nuclei for TDHF calculations was set to 24 fm along the collision axis. When binary reaction products were generated, time evolution was continued until after the collision, at which point the relative distance between the reaction products reaches 26 fm. When two nuclei merged, forming a composite system, time evolution was continued up to around 13 zs. If the composite system kept a compact shape (as quantified by moments of inertia, see Sec. C) within this period, we regarded it as a fusion reaction. The minimum impact parameter inside which fusion reactions take place was obtained by repeating TDHF calculations with an 0.01-fm impact parameter step. For the Ni+Ni reaction at , 1.27, and 1.40, respectively, we found , 4.61, and 5.03 fm, while those for the Ni+Ni reaction were found to be , 4.79, and 5.13 fm, respectively.

The TDRPA calculations were carried out by extending the computational code that was used for the TDHF calculations. Here we recall only an essential part of the computations, and we refer Refs. (43); (44) for details of the technique. The fluctuation and correlation can be computed based on TDRPA with minor modifications of an existing TDHF code. Generally, the correlation between two one-body observables is given by


where and denote arbitrary one-body operators. The fluctuation of a one-body observable corresponds to the case. To compute fluctuations and correlations of neutron, charge, and mass numbers of a reaction product, the operators are taken as the number operator for a spatial region in which the reaction product exists. At the time after collision, at which one wants to evaluate those fluctuations and correlations, one can transform single-particle orbitals as


where is an infinitesimal constant. The step function is equal to 1 within the subspace , and 0 elsewhere. denotes the th single-particle orbital at time with spatial, spin, and isospin coordinates , , and , respectively. Note that for , while for ( or ). For the transformed single-particle orbitals, Eq. (2), a “backward” TDHF evolution from to is performed, where is the initial time of the TDHF calculation. From the backward evolution, we obtain . The fluctuations and correlations can then be evaluated as




The subscript ’’ in Eq. (3) means that is computed by the backward evolution using , namely, without multiplying the phase factor at . The usage of improves numerical accuracy. In practice, the spatial region is taken as a sphere with a radius of 13 fm around the center-of-mass of the projectile-like fragment. The infinitesimal constant has to be small enough to ensure a convergence of the calculation. The convergence was confirmed taking , and . We used for the and 1.40 cases, while was used for the case.

Appendix B Reaction dynamics

Here we present typical reaction dynamics observed in the TDHF calculations. Figure 4 shows the contour plots of the density of colliding nuclei in the reaction plane at various times for the Ni+Ni reaction at . In upper panels (a), dynamics for the  fm case is shown, which we regarded as a fusion reaction (see discussion in Sec. C). Note that the times are not uniformly changed in the bottom panels in (a). In lower panels (b), dynamics for the fm case is shown, which corresponds to a binary reaction. Up to  zs, the dynamics is very similar in both two cases. In the  fm case, the system still holds clear dinuclear structure at  zs, and then it does not reseparate for a long time, showing a mononuclear shape without clear neck structure ( zs). On the other hand, for the  fm case, the system evolves toward reseparation, as can be seen from the thinner neck structure at  zs. The right-bottom frame corresponds to after the collision, at which point various quantities are computed.

Figure 4: The density of colliding nuclei at various times obtained from the TDHF calculations for the Ni+Ni reaction at . Upper panels (a) show the  fm case, while lower panels (b) show the  fm case.

An important quantity that characterizes the reaction dynamics is the total kinetic energy (TKE) of the fragments, which can be a direct measure of the energy dissipation. At after the collision [e.g. the right-bottom panel of Fig. 4 (b)], we evaluate the total kinetic energy as


where is the reduced mass ( is the mass of a nucleon), and () are the mass and charge of each fragment, and are a relative vector connecting center-of-mass positions of the fragments and its time derivative, respectively. From the information of the position and the velocity of the fragments, the scattering angle (an asymptotic value for including the correction of the Coulomb potential for ) can also be evaluated. Those quantities will be given in Sec. G.

Appendix C Moment of inertia

TDHF-TDRPA simulations only give access to the early stage of the formation of the compound nucleus. These calculations are generally run over few 10 zs (13 zs in this work). Beyond these relatively short timescales, neglecting the collision terms of the residual interaction would not be valid. As a result, TDHF calculations, as well as their extensions, cannot be run long enough to allow for investigation of the competition between evaporation and fission of the compound nucleus. Instead, we determine whether an outcome (on average) leads to fusion by looking at how the moment of inertia of the dinuclear system evolves as a function of time.

In order to examine stability of a fusing system, we investigate its effective moment of inertia, . The effective moment of inertia is given by (45)


where denotes an eigenvalue of the moment-of-inertia tensor,


where denote , , and coordinates, respectively. corresponds to the smallest eigenvalue, while corresponds to average of the other two eigenvalues.

Figure 5: Time evolution of the effective moment of inertia, , for the Ni+Ni (top) and Ni+Ni (bottom) reactions () for various impact parameters.

In Fig. 5, we show the time evolution of a ratio, , in the Ni+Ni (top) and Ni+Ni (bottom) reactions for the highest energy case () at various impact parameters. corresponds to the moment of inertia of a spherical nucleus, , where is the mass number of the composite system and .

For Ni+Ni (Ni+Ni), we observed binary reaction products for  fm ( fm). As shown in the figure, for  fm cases, the composite system becomes a compact shape within relatively short time,  zs. Then, the system persists in a compact shape, as one can see from the convergent behavior of the moment of inertia in Fig. 5. At impact parameters very close to the border between capture and binary reactions, the moment of inertia first increases up to around  zs, then decreases, showing a convergent trend [see also Fig. 4 (a)] (strictly speaking, except  fm case in Ni+Ni, where the moment of inertia is not converging, but remains almost constant). From the convergent behavior of the moment of inertia, we consider that the average outcome of those reactions would correspond to fusion.

Appendix D Contact time

Figure 6: Contact times with different criteria (, 0.01, 0.005, 0.001 fm) for the Ni+Ni reaction () are shown as a function of the impact parameter.

The TDHF approach allows the evaluation of contact (sticking or interaction) time of two nuclei directly from the time evolution of the colliding system. From a TDHF calculation, one obtains the total density of the system at each time, . By monitoring the density between two colliding nuclei, we can measure how long they stick together, forming a dinuclear system connected with a neck structure.

In Fig. 6, we show the contact time in the Ni+Ni reaction at as a function of the impact parameter. The contact time is shown in zeptoseconds, and is defined as a time duration in which the lowest total density between the colliding nuclei exceeds a critical value, . In the figure, contact times obtained with four different critical densities, , 0.005, 0.01, and 0.08 fm are presented.

From the figure, one can see that the contact time is zero for trajectories at large impact parameters,  fm. As the impact parameter decreases, the contact time increases sharply, reaching the maximum value ( zs), at the border between fusion and binary reactions. We find that a smaller value of the critical density provides a contact time which is more sensitive to a formation of a dilute neck (–7 fm). As we observe a smooth decrease of the contact time as a function of the impact parameter for the  fm case, we employed this criteria in the present work.

Appendix E Remarks on TDRPA results

Figure 7: Graphical interpretation of the failure of TDRPA calculations for the quasi-symmetric Ni+Ni reaction. (a) A Gaussian distribution around with standard deviation . (b) A skew-normal distribution with mean , standard deviation and skewness . Curvature of the distribution around the mean value (highlighted by pink) is detected in TDRPA calculations (see text for details). Horizontal axis is rescaled like the mass width to have correspondence with our analyses.

In this Letter, we have examined dissipation and equilibration mechanisms in the Ni+Ni reaction. If one applies TDRPA to the Ni+Ni reaction, however, fluctuations and correlations can be unphysically large due to a fundamental problem that lies in the present formulation of TDRPA. The fluctuations and correlations of one-body operators, , can be computed from the expectation value of


in the limit as


where . The Balian-Vénéroni variational principle (46), which leads to Eq. (3), is optimized for the time-evolution of observables in the form like in the Heisenberg picture. Since higher-order terms are neglected in the derivation, it implicitly assumes that the distribution is symmetric around the average value. Thus, if the distribution becomes asymmetric, it may lead to unphysical results. Our analysis confirmed that this problem arises even in a quasi-symmetric system, Ni+Ni.

Figure 8: A comparison of the values calculated using TDRPA for both Ni+Ni and Ni+Ni reactions plotted as a function of impact parameter. The inset allows a closer comparison of the two calculation sets for larger impact parameters.

Figure 7 depicts the difference of situations encountered in (a) a symmetric system, like Ni+Ni, and (b) in a quasi-symmetric system, like Ni+Ni. In Fig. 7 (a), a Gaussian distribution, , with and is shown. The distribution is, of course, symmetric by definition. In the case of symmetric reactions, the distribution must also be symmetric and TDRPA should work well (as long as the distribution remains approximately Gaussian). On the other hand, in Fig. 7 (b), we show a skew-normal distribution with the average value , standard deviation and skewness , as an illustrative example. Because of the positive skewness, the distribution is slightly leaning to the left, showing a longer tail toward the right. As can be seen from the figure, the average value of the skewed distribution does not correspond to the peak centroid, and the curvature around the mean is more moderate compared to the Gaussian distribution shown in Fig. 7 (a). Since TDRPA detects the curvature of the distribution around the average value assuming the Gaussian distribution, it could provide an unphysically large value as illustrated in the figure. One may need to extend the theoretical framework to take into account higher-order terms, like the skewness, to correctly describe the fluctuations and correlations in asymmetric reactions. This goes beyond the scope of the present work.

Nevertheless, the equivalent of Fig. 3(a) in the manuscript is provided for the symmetric and asymmetric calculations in Fig. 8, in order to allow a visual comparison of the two results. As one can see, the values for the asymmetric reaction are unphysical for small impact parameters, but eventually converge to those for the symmetric calculations at larger impact parameters.

Figure 9: Fluctuations and correlations for the Ni+Ni reaction (). Fluctuations of mass, neutron, and charge numbers in TDHF (, , and ) are shown by red, green, and blue solid lines, respectively. While, those in TDRPA (, , and ) are shown by red circles, green down triangles, and blue squares, respectively. Correlations between neutron and charge numbers in TDRPA () are shown by pink triangles. The mass fluctuation in TDRPA, computed by , is also shown by black crosses.

Appendix F Fluctuations and correlations

Let us briefly investigate fluctuations and correlations in deep-inelastic Ni+Ni reaction at the highest incident energy examined (). In Fig. 9, we show fluctuations of mass, neutron, and charge numbers from TDHF, , (solid lines) and from TDRPA, , (symbols), as a function of the impact parameter. The correlation from TDRPA, , is also shown by pink triangles. Those quantities are shown in logarithmic scale.

From the figure, we find that, for reactions at relatively large impact parameters ( fm), the fluctuations from TDHF and TDRPA are quantitatively very similar to each other. In this case, the neutron-number fluctuation is significantly larger than that of protons, and correlations (, pink triangles) are several times smaller than the proton-number fluctuation.

As the impact parameter decreases ( fm), we see that the fluctuations from TDHF and TDRPA start to deviate noticeably. In this regime, the magnitude of the correlations becomes comparable to the proton-number fluctuation, and TDRPA provides significantly larger fluctuations as compared to the TDHF results. These results are consistent with the observation in the Ca+Ca reaction reported in Ref. (43).

As we computed the neutron- and proton-number fluctuations as well as the correlations between them, we can compute the mass fluctuation from the identity, . As this expression serves an accuracy test of the computation, the mass fluctuation computed in the latter way is also shown in Fig. 9 by black crosses. As can be seen from the figure, the results coincide with those evaluated with Eq. (3). Actual values are given in Sec. G.

Appendix G Tables of TDHF and TDRPA results

Here we provide numerical results of the TDHF and TDRPA calculations for the Ni+Ni reaction in Table 1.

Ni+Ni ()
(fm) () TKEL (MeV) (deg) (zs)
5.130 71.917 37.399 95.006 4.10 1.494 7.533 3.079 5.057 3.233 7.480
5.140 72.057 37.088 60.531 3.42 1.493 6.287 5.142 2.171 2.040 6.283
5.150 72.198 37.923 48.472 3.16 1.531 7.428 3.531 4.448 3.376 7.419
5.200 72.899 37.282 24.952 2.73 1.482 4.378 2.841 1.769 1.996 4.378
5.250 73.599 36.231 14.245 2.51 1.518 4.089 2.723 1.651 1.813 4.089
5.500 77.104 35.071 5.512 2.14 1.514 3.292 2.288 1.352 1.373 3.292
5.750 80.609 35.920 44.395 1.37 1.378 2.301 1.464 1.108 0.981 2.301
6.000 84.114 14.971 59.472 0.94 1.093 1.578 1.222 0.617 0.555 1.578
6.250 87.618 4.904 62.702 0.76 0.821 0.974 0.866 0.320 0.220 0.974
6.500 91.123 2.608 62.481 0.68 0.656 0.732 0.675 0.226 0.121 0.732
7.000 98.133 1.274 60.178 0.57 0.447 0.472 0.448 0.135 0.048 0.473
8.000 112.152 0.624 54.536 0.38 0.223 0.227 0.219 0.059 0.014 0.228
9.000 126.170 0.432 49.408 0.00 0.115 0.116 0.112 0.031 0.007 0.117
10.000 140.189 0.342 45.040 0.00 0.064 0.066 0.062 0.023 0.006 0.066
Ni+Ni ()
(fm) () TKEL (MeV) (deg) (zs)
4.790 63.958 28.412 33.574 3.52 1.446 5.585 7.733 9.338 7.613 16.214
4.800 64.092 26.636 9.072 2.97 1.439 6.637 3.900 3.036 3.128 6.632
4.850 64.759 24.999 31.020 2.10 1.397 3.104 2.261 1.094 1.289 3.103
4.900 65.427 28.466 43.179 1.80 1.391 2.737 1.768 1.258 1.179 2.737
4.950 66.094 30.291 51.123 1.62 1.327 2.393 1.553 1.111 1.019 2.393
5.000 66.762 28.301 57.338 1.47 1.268 1.986 1.336 0.918 0.811 1.986
5.250 70.100 12.010 72.917 1.00 1.025 1.456 1.158 0.536 0.496 1.456
5.500 73.438 3.904 75.313 0.81 0.779 0.908 0.823 0.265 0.196 0.908
5.750 76.776 2.215 74.451 0.73 0.636 0.699 0.654 0.191 0.113 0.699
6.000 80.114 1.537 72.944 0.68 0.531 0.567 0.538 0.149 0.072 0.568
7.000 93.467 0.694 65.881 0.47 0.274 0.280 0.272 0.066 0.018 0.281
8.000 106.819 0.453 59.376 0.19 0.145 0.146 0.142 0.034 0.009 0.147
9.000 120.172 0.344 53.832 0.00 0.079 0.080 0.077 0.023 0.007 0.081
10.000 133.524 0.286 49.147 0.00 0.048 0.050 0.046 0.020 0.007 0.051
Ni+Ni ()
(fm) () TKEL (MeV) (deg) (zs)
3.740 47.313 17.896 45.713 2.68 1.253 3.043 2.040 1.816 0.924 3.028
3.750 47.439 17.691 56.969 2.37 1.260 3.683 2.779 1.182 1.483 3.677
3.800 48.072 19.416 73.002 1.83 1.186 2.034 1.503 0.965 0.689 2.034
3.850 48.704 18.950 80.793 1.58 1.109 1.682 1.138 0.783 0.678 1.682
3.900 49.337 18.937 84.244 1.46 1.060 1.548 1.058 0.709 0.623 1.548
3.950 49.969 18.918 86.766 1.38 1.056 1.486 1.037 0.673 0.582 1.486
4.000 50.602 16.850 89.906 1.28 1.065 1.675 1.145 0.744 0.686 1.675
4.250 53.765 4.230 95.617 0.93 0.812 0.999 0.914 0.247 0.225 0.999
4.375 55.346 2.962 95.085 0.87 0.733 0.854 0.799 0.196 0.162 0.854
4.500 56.927 2.291 94.204 0.83 0.670 0.755 0.715 0.167 0.126 0.756
4.750 60.090 1.598 92.033 0.77 0.570 0.618 0.593 0.132 0.084 0.618
5.000 63.252 1.236 89.664 0.72 0.491 0.520 0.502 0.108 0.058 0.520
6.000 75.903 0.650 80.228 0.51 0.276 0.280 0.275 0.055 0.019 0.281
7.000 88.553 0.435 71.938 0.20 0.153 0.155 0.152 0.031 0.009 0.156
8.000 101.204 0.333 64.931 0.00 0.086 0.088 0.085 0.022 0.006 0.088
9.000 113.854 0.268 59.020 0.00 0.052 0.053 0.050 0.019 0.006 0.054
10.000 126.505 0.227 54.013 0.00 0.036 0.038 0.035 0.017 0.006 0.040
Table 1: Results of the TDHF and TDRPA calculations for the Ni+Ni reaction at , 1.27, and 1.40. From left to right, the table shows: impact parameter in fm, corresponding angular momentum () in units of , total kinetic energy loss [TKEL ()] in MeV, deflection angle in the center-of-mass frame in degrees, contact time in zeptoseconds, fluctuations from TDHF , TDRPA , , , and correlation from TDRPA , and the mass width from TDRPA, computed from .



  1. D. Suter and G. A. Álvarez, Rev. Mod. Phys. 88, 041001 (2016), URL http://journals.aps.org/rmp/pdf/10.1103/RevModPhys.88.041001.
  2. A. Polkovnikov, K. Sengupta, A. Silva, and M. Vengalattore, Rev. Mod. Phys. 83, 863 (2011), URL http://journals.aps.org/rmp/pdf/10.1103/RevModPhys.83.863.
  3. M. Gring, M. Kuhnert, T. Langen, T. Kitagawa, R. Rawer, M. Schreitl, I. Mazets, D. A. Smith, E. Demler, and J. Schmiedmayer, Science 337, 1318 (2012), URL http://science.sciencemag.org/content/337/6100/1318.full.
  4. H. Aoki, N. Tsuji, M. Eckstein, M. Kollar, T. Oka, and P. Werner, Rev. Mod. Phys. 86, 779 (2014).
  5. J. Eisert, M. Friesdorf, and C. Gogolin, Nature Physics 11, 124 (2015), URL http://www.nature.com/nphys/journal/v11/n2/full/nphys3215.html.
  6. D. J. Hinde, M. Dasgupta, A. Diaz-Torres, and M. Evers, Nucl. Phys. A 834, 117c (2010).
  7. C. Simenel, Phys. Rev. Lett. 106, 112502 (2011).
  8. Y. Aritomo, K. Hagino, K. Nishio, and S. Chiba, Phys. Rev. C 85, 044614 (2012).
  9. Lacroix, Denis and Ayik, Sakir, Eur. Phys. J. A 50, 95 (2014), URL https://doi.org/10.1140/epja/i2014-14095-8.
  10. A. S. Umar, V. E. Oberacker, and C. Simenel, Phys. Rev. C 92, 024621 (2015).
  11. G. Barontini, R. Labouvie, F. Stubenrauch, A. Vogler, V. Guarrera, and H. Ott, Phys. Rev. Lett. 110, 035302 (2013).
  12. I. de Vega and D. Alonso, Rev. Mod. Phys. 89, 015001 (2017), URL http://journals.aps.org/rmp/pdf/10.1103/RevModPhys.89.015001.
  13. G. Clos, D. Porras, U. Warring, and T. Schaetz, Phys. Rev. Lett. 117, 170401 (2016), URL http://journals.aps.org/prl/pdf/10.1103/PhysRevLett.117.170401.
  14. A. Jedele, A. B. McIntosh, K. Hagel, M. Huang, L. Heilborn, Z. Kohley, L. W. May, E. McCleskey, M. Youngs, A. Zarrella, et al., Phys. Rev. Lett. 118, 062501 (2017), URL https://link.aps.org/doi/10.1103/PhysRevLett.118.062501.
  15. A. S. Umar, C. Simenel, and W. Ye, Phys. Rev. C 96, 024625 (2017), URL https://link.aps.org/doi/10.1103/PhysRevC.96.024625.
  16. J. Tōke, B. Bock, G. X. Dai, A. Gobbi, S. Gralla, K. D. Hildenbrand, J. Kuzminski, W. Müller, A. Olmi, and H. Stelzer, Nucl. Phys. A440, 327 (1985).
  17. R. du Rietz, E. Williams, D. J. Hinde, M. Dasgupta, M. Evers, C. J. Lin, D. H. Luong, C. Simenel, and A. Wakhle, Phys. Rev. C 88, 054618 (2013), URL http://link.aps.org/doi/10.1103/PhysRevC.88.054618.
  18. W. U. Schröder and J. R. Huizenga, in Treatise on Heavy-Ion Science, edited by D. Bromley (Plenum Press, 1984), vol. 2, pp. 115–726.
  19. P. A. M. Dirac, Proc. Camb. Philos. Soc. 26, 376 (1930).
  20. R. Balian and M. Vénéroni, Physics Letters B 136, 301 (1984), ISSN 0370-2693, URL http://www.sciencedirect.com/science/article/pii/0370269384920082.
  21. D. J. Hinde, M. Dasgupta, J. R. Leigh, J. C. Mein, C. R. Morton, J. O. Newton, and H. Timmers, Phys. Rev. C 53, 1290 (1996).
  22. R. Rafiei, R. G. Thomas, D. J. Hinde, M. Dasgupta, C. R. Morton, L. R. Gasques, M. L. Brown, and M. D. Rodriguez, Phys. Rev. C 77, 024606 (2008).
  23. M. D. Rodríguez, M. L. Brown, M. Dasgupta, D. J. Hinde, D. C. Weisser, T. Kibédi, M. A. Lane, P. J. Cherry, A. G. Muirhead, R. B. Turkentine, et al., Nucl. Inst. Meth. Phys. Res. A614, 119 (2010).
  24. C. Simenel, D. J. Hinde, R. du Rietz, M. Dasgupta, M. Evers, C. J. Lin, D. H. Luong, and A. Wakhle, Phys. Lett. B710, 607 (2012).
  25. C. Simenel, Eur. Phys. J. A 48, 152 (2012).
  26. A. Wakhle, C. Simenel, D. J. Hinde, M. Dasgupta, M. Evers, D. H. Luong, R. du Rietz, and E. Williams, Phys. Rev. Lett. 113, 182502 (2014), URL https://link.aps.org/doi/10.1103/PhysRevLett.113.182502.
  27. V. E. Oberacker, A. S. Umar, and C. Simenel, Phys. Rev. C 90, 054605 (2014), URL https://link.aps.org/doi/10.1103/PhysRevC.90.054605.
  28. K. Hammerton, Z. Kohley, D. J. Hinde, M. Dasgupta, A. Wakhle, E. Williams, V. E. Oberacker, A. S. Umar, I. P. Carter, K. J. Cook, et al., Phys. Rev. C 91, 041602 (2015), URL https://link.aps.org/doi/10.1103/PhysRevC.91.041602.
  29. K. Sekizawa and K. Yabana, Phys. Rev. C 93, 054616 (2016), URL http://journals.aps.org/prc/abstract/10.1103/PhysRevC.93.054616.
  30. A. S. Umar, V. E. Oberacker, and C. Simenel, Phys. Rev. C 94, 024605 (2016), URL https://doi.org/10.1103/PhysRevC.94.024605.
  31. K. Sekizawa and K. Yabana, Phys. Rev. C 88, 014614 (2013), URL https://link.aps.org/doi/10.1103/PhysRevC.88.014614.
  32. K. Sekizawa and K. Yabana, Phys. Rev. C 93, 029902(E) (2016), URL https://link.aps.org/doi/10.1103/PhysRevC.88.014614.
  33. K.-H. Kim, T. Otsuka, and P. Bonche, J. Phys. G: Nucl. Part. Phys. 23, 1267 (1997).
  34. T. H. R. Skyrme, Phil. Mag. 1, 1043 (1956), URL Skyrme␣energyΩdensity␣functional.
  35. See supplemental material.
  36. C. H. Dasso, T. Dossing, and H. C. Pauli, Z. Physik A 289, 395 (1979).
  37. S. Ayik, Phys. Lett. B 658, 174 (2008).
  38. G. N. Knyazheva, E. M. Kozulin, R. N. Sagaidak, A. Y. Chizhov, M. G. Itkis, N. A. Kondratiev, V. M. Voskressensky, A. M. Stefanini, B. R. Behera, L. Corradi, et al., Phys. Rev. C 75, 064602 (2007).
  39. E. Williams, D. J. Hinde, M. Dasgupta, R. du Rietz, I. P. Carter, M. Evers, D. H. Luong, S. D. McNeil, D. C. Rafferty, K. Ramachandran, et al., Phys. Rev. C 88, 034611 (2013), URL http://link.aps.org/doi/10.1103/PhysRevC.88.034611.
  40. R. du Rietz, D. J. Hinde, M. Dasgupta, R. G. Thomas, L. R. Gasques, M. Evers, N. Lobanov, and A. Wakhle, Phys. Rev. Lett. 106, 052701 (2011), URL https://link.aps.org/doi/10.1103/PhysRevLett.106.052701.
  41. K. Sekizawa and K. Yabana, Phys. Rev. C 88, 014614 (2013); 93, 029902(E) (2016).
  42. K.-H. Kim, T. Otsuka, and P. Bonche, J. Phys. G 23, 1267 (1997).
  43. C. Simenel, Phys. Rev. Lett. 106, 112502 (2011).
  44. C. Simenel, Eur. Phys. J. A 48, 152 (2012).
  45. A.S. Umar, V.E. Oberacker, and C. Simenel, Phys. Rev. C 92, 024621 (2015).
  46. R. Balian and M. Vénéroni, Phys. Lett. B136, 301 (1984).
This is a comment super asjknd jkasnjk adsnkj
The feedback must be of minumum 40 characters
The feedback must be of minumum 40 characters
Comments 0
Request comment
The feedback must be of minumum 40 characters
Add comment
Loading ...

You are asking your first question!
How to quickly get a good answer:
  • Keep your question short and to the point
  • Check for grammar or spelling errors.
  • Phrase it like a question
Test description