Inhibited, Explosive and Anisotropic Relaxation in a Gas of Molecular Super-Rotors

Inhibited, Explosive and Anisotropic Relaxation in a Gas of Molecular Super-Rotors

Yuri Khodorkovsky Department of Chemical Physics, The Weizmann Institute of Science, Rehovot 76100, Israel    Uri Steinitz Department of Chemical Physics, The Weizmann Institute of Science, Rehovot 76100, Israel    Jean-Michel Hartmann Laboratoire Interuniversitaire des Systèmes Atmosphériques (LISA) CNRS (UMR 7583), Université Paris Est Créteil, Université Paris Diderot, Institut Pierre-Simon Laplace, Université Paris Est Créteil, 94010 Créteil Cedex, France    Ilya Sh. Averbukh 111corresponding author: ilya.averbukh@weizmann.ac.il Department of Chemical Physics, The Weizmann Institute of Science, Rehovot 76100, Israel
July 14, 2019

Recently, several femtosecond laser techniques have been developed  centrifuge_corkum1 (); centrifuge_corkum2 (); Mullin1 (); Mullin2 (); Valery (); Bucksbaum (); NJP (); Kitano_udr (); Khodorkovsky_udr_benzene (); Floss_prl () that are capable of bringing gas molecules to extremely fast rotation in a very short time, while keeping their translational motion intact and relatively slow. We investigate collisional equilibration dynamics of this new state of molecular gases, and find that it follows a remarkable generic scenario. The route to equilibrium starts with a durable metastable ‘gyroscopic stage’, in the course of which the molecules maintain their fast rotation and orientation of the angular momentum through many collisions. The inhibited rotational-translational relaxation is characterized by a persistent anisotropy in the molecular angular distribution, and is manifested in the long-lasting optical birefringence, and anisotropic diffusion in the gas. After a certain induction time, the ‘gyroscopic stage’ is abruptly terminated by a self-accelerating explosive rotational-translational energy exchange leading the gas towards the final thermal equilibrium. We illustrate our conclusions by direct Molecular Dynamics (MD) simulation of super-rotors in several gases consisting of common linear molecules (such , and ).

The efficiency of the collisional energy transfer from the internal molecular degrees of freedom (vibrational or rotational) to the translational ones is crucially dependent on the typical time scales of the processes involved. To analyze the rotational-translational (RT) energy transfer between colliding molecules in a gas, one has to compare the typical rotational period, ( is the angular rotational frequency) and the characteristic duration of a collision, . The latter may be estimated as the time it takes for a molecule of the typical speed to traverse the range of the intermolecular potential: . The ratio of these two time scales is the so-called adiabaticity parameter . When the is long enough for the molecule to complete several revolutions during the collision, i.e. , the collision is adiabatic with respect to the rotational dynamics of the molecule. During the encounter of two molecules, the molecular rotational dynamics adiabatically adjusts itself to a slowly varying intermolecular interaction, and the rotational energy of the molecules returns to its initial value after the end of the collision. In such cases the RT relaxation is suppressed, and the fast rotating molecules are dubbed super-rotors (SR)Stwalley2000 (). On the other hand, when (or smaller), the collisions are impulsive, and efficient energy transfer occurs between the rotational and the translational degrees of freedom. Similar arguments are relevant also to the vibrational-translational relaxation process, and they are known since the introduction of the Landau-Teller theory LandauTeller () describing the vibrational-translational energy exchange in a collision between an atom and a diatomic molecule. The main difference between rotations and vibrations is the much smaller typical timescale of the latter, which makes the ’adiabatic regime’ more accessible for the vibrations. Additionally, the dependence of rotational frequency on energy provides a threshold for adiabaticity. It has been known for a while, that highly rotationally excited molecules appearing in some exothermic chemical reactions and photodissociation processes may exhibit extended collisional relaxation Polanyi (). More recently, it has been predicted that trapped ultra-cold molecules may also experience adiabatic suppression of the rotational relaxation Stwalley2000 (); Forrey2001 () which may open new options for cold chemistry (see Forrey2011 () and references therein). In the latter case the translational temperatures are very low, and the adiabaticity is enhanced by the prolonged duration of the collisions that are quantum in nature. Nowadays, molecules can be excited to become SRs by optical techniques aiming at inducing molecular alignment by short laser pulses (for reviews see Refs. Stapelfeldt_review (); Ohshima (); my_review ()), especially utilizing the schemes using multiple laser pulses Bucksbaum (). Moreover, several methods have been suggested and demonstrated for converting the transient molecular alignment into a concerted unidirectional molecular rotation, including the techniques of “optical centrifuge” centrifuge_corkum1 (); centrifuge_corkum2 (); Mullin1 (); Mullin2 (); Valery (), “molecular propeller” NJP (); Kitano_udr (); Khodorkovsky_udr_benzene (), and “chiral train” of laser pulses Floss_prl ().

In this Letter, we investigate collisional dynamics in a gas of molecules initially at room temperature, but with extremely high rotational excitation. Our research is stimulated by recent laser experiments that achieved the SR regime at near-ambient conditions Mullin1 (); Mullin2 (); Valery (); Bucksbaum (). The theoretical analysis of these experiments is still in its infancy, and the previous quantum treatments focused on ultra-cold collisions of super-rotors Forrey2001 (); Forrey2011 () are intractable in this case. Our study provides the first modeling (to the best of our knowledge) of the collisional dynamics of molecular SRs by direct molecular dynamics (MD) simulation methods. The classical approach seems to be an appropriate tool for studying molecules at room temperature, excited to the quasiclassical rotational states with the angular momentum of tens to hundreds of . It has already been successfully used for analysis of the laser experiments on molecular alignment at dissipative conditions Hartmann12 (); Hartmann13b (); Karras2014 ().

We studied relaxation dynamics for several small linear molecules (such , and ) and found that they demonstrate a rather universal behavior in the SR regime. Therefore, we present below in detail our results for the representative case of molecular nitrogen, . The Supplementary Movie s1 (https://www.youtube.com/watch?v=2qyoPvJ_SpI) shows in an animated way a very similar relaxation dynamics in a gas of molecules.

We start by presenting results of a test case of a moderate rotational excitation of molecules by a single non-resonant short laser pulse having linear polarization. Such a pulse is quantified by the so called ”kick strength” parameter, that defines a typical amount of the angular momentum (in units of ) transferred from the laser pulse to a molecule (see the Methods section). The simulation of the initial rotational state by laser excitation was performed as in Ref. Khodorkovsky_udr_benzene (). Figure 1(a) demonstrates an exponential decay of the excess rotational energy of molecules after the pulse of , and the corresponding increase of the translational energy as a function of time. Such a kick strength (and even higher) can be achieved Bucksbaum () by a train of several laser pulses (50 fs duration, 800 nm central wavelength, peak intensity of ) separated in time by the rotational revival time ps of molecules. The magnitude of this kick is comparable with the thermal value of the angular momentum quantum number for nitrogen molecules at  K. At the end of the relaxation process, the ratio between the average translational and rotational energies is , as required by the equipartition theorem. The gas reaches equilibrium after about (after each molecule has experienced about 20 collisions). Such an exponential relaxation pattern is in agreement with other recent theoretical Ramakrishna (); Hartmann12 () and experimental Hartmann13b (); Karras2014 (); Owschimikow () studies on the collisional relaxation of laser-excited molecular rotations. For a stronger laser pulse of , a slight deviation from the exponential behavior appears at short times, see Fig. 1(b).

We now demonstrate that the relaxation scenario is drastically different for higher rotational excitation attainable by the “optical centrifuge” technique centrifuge_corkum1 (); centrifuge_corkum2 (); Mullin1 (); Mullin2 (); Valery (). Figure 2 presents the results of MD simulations for an ensemble of nitrogen molecules that were initially aligned along the -axis and brought to fast rotation in the -plane with the same initial angular momentum oriented along the -axis. This is a rather crude model for molecules suddenly released from an optical centrifuge, however simulations using a more realistic description of the centrifugation process lead to similar outcomes. Figure 2 displays the RT energy transfer dynamics for molecules initially excited to and .

Two distinct relaxation stages are clearly seen. Initially, for a relatively long period covering several tens of collisions, there is almost no change in the mean rotational energy of the molecules (plateau region). After a certain induction period, the plateau is followed by an abrupt, explosive-like energy dump from the rotational motion into the translational one, leading to the final thermal equilibration of the heated gas. The duration of the induction period grows with the initial rotational excitation. A deeper insight is given by the numerically simulated time-dependent distribution functions for the rotational (Fig. 3(a)) and translational (Fig. 3(b)) energies. They show that during the plateau period, the rotational distribution broadens mainly due to the rotation-rotation energy exchange, and both distributions dramatically change their shapes in the course of the explosive relaxation. There is a clear physical reason for such relaxation dynamics. During the plateau period, the RT relaxation is inhibited due to the high value of the adiabaticity parameter, . However, as the rotational distribution broadens, and the energy leaks from rotations to translations, there is an increasing fraction of molecules colliding at lower values of . This makes the RT relaxation more efficient and triggers a positive feedback mechanism. The increase in the translational speeds shortens the typical collision time and raises the heating rate of the gas, which in turn accelerates further the RT energy transfer and ignites an explosive thermalization. This mechanism resembles the famous phenomenon of thermal explosion Semenov () in heat-generating solids, which was first considered by N. Semenov in 1928. The Supplementary Movie s1 (https://www.youtube.com/watch?v=2qyoPvJ_SpI) presents in an animated way this relaxation scenario in the gas of oxygen super-rotors. It shows the same generic relaxation stages (inhibited and explosive) as in the above example of the nitrogen gas. A shorter time scale is attributed to the higher gas pressure chosen for that numerical example.

To get a deeper insight into the collisional relaxation of SRs, we investigated the process of isotropization of the molecular orientation, and of the direction of the rotational angular momentum. Figure 4(a) shows that during the plateau period (until about ), the factor of alignment along the -axis, , remains close to zero. This means that the molecules continue rotating mainly in the -plane with the angular momentum vector oriented along the -axis. This is also supported by Fig. 4(b) that shows the time dependence of the component (parallel to the exciting laser’s propagation direction) of the molecular angular momentum, . The ability to keep orientation of the angular momentum is characteristic of gyroscopes (even as small as a rotating molecule). Such a tendency is consistent with a much weaker propensity observed in recent studies of laser excited molecules Hartmann12 () at lower degrees of rotational excitation. For this reason, we term the whole period before the self-accelerating RT energy exchange, as a “gyroscopic stage” of relaxation. As seen from Fig. 4, the isotropization of the super-rotors occurs mainly during the stage of the explosive relaxation, after which the alignment factor takes the isotropic value of , and there is no preferred orientation of the angular momentum vector.

Figure 5 schematically shows the anisotropic (pancake-like) angular distribution maintained by the molecular super-rotors in the course of many collisions during the gyroscopic stage. The initial fast rotation was set by an optical centrifuge operating in the -plane. The macroscopic polarizability of such a gas is anisotropic as well, which can be detected by measuring birefringence for a polarized light propagating along any direction in the -plane. Such a persistent birefringence may serve as an optical indicator of the gyroscopic relaxation stage. However, here we will focus on the gas-kinetics manifestations of this anisotropy. Just looking at Fig. 5, one may expect that the collisional cross-section for the face-to-face colliding molecular ‘pancakes’ should be different from the cross-section for the side-to-side collisions. Also, the rotational-translational energy exchange happens differently in the cases of the face-to-face and side-to-side collisions Mullin2 (). This suggests the emergence of anisotropic transport phenomena in the gas, such as anisotropic mass and energy diffusion. Moreover, the explosive RT energy exchange at the end of the gyroscopic phase should have its manifestations in the transport effects as well.

To test these predictions, we investigated the process of self-diffusion of a nitrogen molecular super-rotor by means of the above direct MD simulations. Following the random-walk trajectory for each molecule of an ensemble prepared in a centrifuged state, we calculated the average square of the cumulative molecular displacement along each of the Cartesian axes as a function of time. The time-dependent diffusion coefficients for the motion along every axis was derived by differentiating this function with respect to time (e.g., ). Figure 6(b) shows that as long as the molecules keep the original orientation of their rotation axis (gyroscopic stage), the diffusion coefficients in the and directions are indeed about larger than the one corresponding to the diffusion along the axis. The diffusion coefficients grow with time (as seen in Fig. 6) because of the gradual heating of the translational motion of the molecules due to the RT energy exchange. With the ignition of the explosive relaxation, the diffusion coefficients grow abruptly together with the translational speeds, and all three coefficients reach the same high value corresponding to the final hot equilibrated state.

Nontrivial regimes of mass and heat transfer in the gas of super-rotors may happen when the laser excitation takes place in a spatially-confined domain, like the focal spot of a focused laser beam, which implies that the ‘cloud’ of centrifuged molecules disperses differently in the axial and radial directions. The explosive-like delivery of the rotational energy to the translational motion leads to an increased local pressure and to the subsequent generation of sound waves, as well as to the creation of a hot area with a reduced molecular concentration which may be optically observed Steinitz (); Zahedpour2014 (); Segev (). This density hole is then slowly healed via the diffusion of cold unexcited molecules from the area outside the focal spot, while the hot molecules diffuse outwards. The multi-scale long decay of rotational signals from the optically centrifuged molecules in dense gases reported recently Mullin1 (); Mullin2 () may be actually related to the above interplay of the kinetic and hydrodynamic phenomena, which requires additional theoretical analysis of these experiments.

Finally, we emphasize that although the molecular gas arrives to a microscopically thermalized state, macroscopic non-equilibrium flows can still exist in the gas. For molecules that are initially excited into a rotation with a preferred sense of spinning (with oriented mean angular momentum), it was shown recently that a vortex flow appears around the laser focal spot after thermalization Steinitz ().

To summarize, we investigated theoretically the collisional relaxation in a gas of molecular super-rotors, excited with the help of ultrashort laser pulses. We found that the SRs behave like tiny gyroscopes after the excitation, and maintain their fast rotation and orientation of the angular momentum through many collisions. This leads to the anisotropic diffusion in the gas, and to a long-lasting optical birefringence. The rotational-translational energy transfer is effectively suppressed during the gyroscopic stage. This metastable state of the gas terminates abruptly after some induction period (depending on the initial rotational excitation) due to development of an explosive self-accelerating energy transfer from the rotational degrees of freedom to the translational ones. We discussed optical means for detecting the macroscopic effects associated with SRs relaxation. Other manifestations may include filamentation effects, anisotropic diffusion of selected species in a molecular mixture of different components, anisotropic viscosity in the gas, and directed acousto-optical signals produced by the laser-generated rotationally excited gas Schippers ().

I Methods

The simulations were carried out with molecules residing in a cubic volume at room translational temperature and pressure. Initially, the molecules were uniformly distributed in space, while their initial velocity followed the Maxwell-Boltzmann distribution. The initial distribution of the rotational degrees of freedom (direction of molecular axes, angular velocity vectors) was obtained by simulating the process of ultra-fast laser excitation of SRs. In the case of the excitation by a linearly polarized aligning laser pulse (see Fig. 1), the details of the simulation procedure are described in Ref. Khodorkovsky_udr_benzene (). Specifically, the molecules were impulsively excited as if affected by a linearly polarized femtosecond laser pulse with a kick strength (where is the molecular polarizability anisotropy and is the envelope of the electric field of the laser pulse). Parameter defines a typical amount of the angular momentum (in units of ) transferred from the laser pulse to a molecule. Excitation by the optical centrifuge was simulated by solving classical equations of motion for a thermal ensemble of polarizable linear molecules subject to a pulsed electric field with rotating polarization. The parameters of the centrifuge were similar to those used in the experiment Valery (). Starting from these initial conditions, we let the molecules propagate in space using the standard Verlet algorithm, and periodic boundary conditions, while the propagation of the rotational motion was done as described in Ref. Allen (). The classical intermolecular interaction potential was taken from Ref. Cheung ().

Ii Acknowledgements

This research was made possible in part by the historic generosity of the Harold Perlman Family. I.A. acknowledges support as the Patricia Elman Bildner Professorial Chair. He also acknowledges kind hospitality and support from the Université Paris Est Créteil during a one week stay with J-M.H. at LISA.

Iii Author contributions

All authors contributed to the formulation of the problem and analysis of the results. Numerical simulations were mainly performed by Y.K. and U.S.. I.A. and J-M.H. supervised the research. All authors discussed the results and the manuscript.

Iv Additional information

Supplementary Movie s1.

Animated visualization of the collisional dynamics in a gas of oxygen super-rotors. This video depicts the simulation of spinning oxygen molecules, initially at room translational temperature, all rotating fast at . For visualization purposes the initial concentration is 20 times that of atmospheric gas and the boundary conditions are periodic. The resulting dynamics follows the same generic scenario as observed in the molecular dynamics simulations for nitrogen molecules in the main text of the paper, only faster by a factor of about 20 (due to the increased pressure). In the left box each particle is represented by a spindle whose axis corresponds to the rotation axis, and its length depicts the rotation speed. The color of each particle codes the translational speed. On the right panel, the evolution of the mean translational and rotational energy is shown (compare with Fig. 2 in the main text), along with the momentary distribution of the rotational energy (green markers). The first quarter of the movie features the metastable gyroscopic stage, where the molecules’ rotation axes are still parallel to the original preferred direction, despite the many collisions each of them has undergone. The stage is followed by the explosive relaxation (at around halfway through the movie) where the molecules suddenly transform from slow (blue) parallel spindles into fast moving (red) ones with slowed, isotropic rotation.

V Competing financial interests

The authors declare no competing financial interests.

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Figure 1: Equilibration of energy with time for a gas of molecules being initially at ambient temperature and pressure, and kicked by a linearly polarized laser pulse with a kick strength of (a) , and (b) . The translational and rotational energy of the molecules are plotted in blue and red, respectively.
Figure 2: Equilibration of energy with time for a gas of molecules being at ambient temperature and pressure, and subject to an optical centrifuge at . Panels (a)and (b) correspond to the initial angular momentum of and , respectively. The mean translational and rotational energies of the molecules are plotted in blue and red, respectively.
Figure 3: Density plots for time-dependent distributions of the rotational and translational energy (panels (a) and (b), respectively). The molecules are initially centrifuged to . An explosive transition towards the thermal Maxwell distribution of the heated gas is clearly seen near 5 ns (compare with Fig. 2(b)).
Figure 4: Orientation dynamics of the molecules that are initially centrifuged in the -plane, . Panel (a)- time dependence of the alignment factor along axis. Panel (b) - decay of the normalized component of the angular momentum.
Figure 5: Schematic illustration of the anisotropic angular distribution of gas molecules spun by an optical centrifuge rotating in the -plane.
Figure 6: Time-dependent diffusion coefficients along the axes are plotted as a function of time. The molecules in panels (a) and (b) are initially centrifuged in the -plane with an angular momentum of and , respectively.
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