Detecting handedness of spatially oriented molecules by Coulomb explosion imaging Free

Chiral molecules exist in structural forms known as enantiomers, which are mirror images of one another that are non-superimposable by translation and rotation. The chemical behavior of molecular enantiomers can be profoundly different. Particularly in the pharmaceutical industry, methods to differentiate between them or to determine the enantiomeric excess (ee) of a chiral sample are important. In recent years, there have been considerable advances in gas-phase chiroptical techniques and a variety of such methods have emerged, for example, using phase-sensitive microwave spectroscopy,^1,2 Coulomb explosion imaging with coincidence detection,^3,4 photoelectron circular dichroism (PECD),^5–9 chiral-sensitive high-harmonic generation,^10–12 or attosecond-time-resolved photoionization.¹³ These approaches offer improved sensitivity and their success is based on exploiting electric–dipole interactions for chiral discrimination,¹⁴ producing stronger signals than circular dichroism from magnetic–dipole interactions.

Coulomb explosion imaging is a powerful and efficient approach to retrieve the instantaneous absolute structures of complex molecules.^15–17 Applied to chiral molecules, coincident imaging of fragments emitted from the chiral center can be used to determine the handedness of their enantiomers, in the conceptually most straightforward way by coincident detection of all fragments attached to the stereocenter.^3,4 For axially chiral molecules, it has been demonstrated that it is sufficient to only correlate two different fragments, if the molecules are pre-aligned along their axis of chirality.¹⁸ 

For molecular enantiomers placed in a field coupling two molecular dipole moment projections or two off-diagonal polarizability elements, it was demonstrated that they exhibit transient dipole moments and spatial orientations with opposite signs for the different enantiomers.^1,19–22 Experiments inducing enantiomer-specific orientation, e.g., probed by Coulomb explosion imaging, were reported, albeit so far with very low sensitivity to the enantiomeric excess.²² 

Here, we explore the effect of spatial three-dimensional (3D) alignment of molecules in Coulomb explosion imaging in order to sensitively probe the ee and the handedness of chiral molecules with it. Using accurate computational procedures, we demonstrate that 3D alignment by an elliptically polarized non-resonant field can break the symmetry in a fragment position and momentum distribution in the detector plane, if the polarization ellipse is tilted by an angle 0 < β < 90° with respect to the norm vector of the detector. The asymmetry between the detector’s left and right halves gives access to the ee and handedness of chiral molecules. This method is more robust than previous Coulomb explosion-based approaches, e.g., regarding detector limitations and experimental imperfections. Our theoretical estimates for the sensitivity to the ee are comparable to other modern chiroptical techniques, such as PECD. To further enhance sensitivity, we also explore the effect of one-dimensional (1D) orientation combined with 3D alignment.

Figure 1 illustrates the underlying idea of our approach, which is demonstrated for the prototypical chiral molecule camphor (C₁₀H₁₆O). A non-resonant elliptically polarized laser field is applied to achieve 3D alignment. The most polarizable axis of the molecule p is aligned along the major axis Z_L of the elliptical field and the second most polarizable axis q along the minor elliptical axis X_L. We chose the three distinct methyl (CH₃) groups in camphor as marker fragments to differentiate between the R and S enantiomers in a Coulomb-explosion imaging. Their flight directions can be observed experimentally as momentum distributions of the $CH3+$ ions resulting from multiple ionization followed by Coulomb explosion of the molecule.^23,24

We assume that two-body dissociation events produce equal initial momenta for $CH3+$ fragments at three different molecular sites. By normalizing the size of the Newton sphere to one, the momentum distributions are given by the position distributions of the CH₃ groups. These methyl-group distributions in the detector plane are schematically plotted in Fig. 1 for the idealized case of perfect 3D alignment. Fixed in the X_LZ_L laser polarization plane, the molecule orients itself in one of the four equally preferred ways, which are related by 180° rotations about the most polarizable p and q axes of the molecule. Fixing the plane of elliptical polarization in the XZ laboratory plane, the Cartesian coordinates of an atom in the molecule projected onto the YZ plane of the detector for all four possible spatial molecular orientations are given by

where x, y, and z denote the Cartesian coordinates of an atom in the principal-axis-of-polarizability frame of the molecule. The subscript indices p and q denote Cartesian vectors obtained by 180° rotations about the respective molecular polarizability axes, which, in the case of perfect 3D alignment, coincide with the Z_L and X_L axes of the polarization ellipse. The angle β is the angle between the major Z_L axis of the ellipse and the norm (e_X) of the detector. It describes the rotation of the polarization ellipse about the Y axis.

The four different positions r, r_p, r_q, and r_pq in the plane of the detector are plotted in Fig. 1 for the three carbon atoms that belong to the methyl groups for R and S camphor. Different enantiomers have opposite signs of the Y component of each position vector in (1). When β = n · 90°, n = 0, 1, 2, …, the four different positions in the plane of the detector for each atom produce an image, which is symmetric with respect to the inversion of both Y and Z axes, as shown in Fig. 1(a). Since the position vectors for the R and S enantiomers differ only in the sign of the Y coordinate, the resulting projections will look exactly the same for different enantiomers. However, when β ≠ n · 90°, the symmetry with respect to the inversion of the Y axis in (1) will be broken. As a result, the sums of the four equivalent molecular spatial orientations will exhibit distinctly different projections on the detector plane for the R and S enantiomers [see Fig. 1(b)]. The detector images of the enantiomers are asymmetric with respect to the left and right parts and are, in fact, mirror images of each other for the enantiomers. This allows for the determination of the ee and the handedness of chiral molecules. Notably, the present approach does not require coincidence measurements of different fragment species.

To benchmark our scheme, we performed quantummechanical calculations of the rotational dynamics of camphor using the accurate variational procedure RichMol,²⁵ which simulates the rotation-vibration dynamics of molecules in the presence of external fields. The field-free rotational motion was modeled using the rigid-rotor Hamiltonian with the rotational constants A = 1446.968 977 MHz, B = 1183.367 110 MHz, and C = 1097.101 031 MHz.²⁶ Simulations of the field-induced time-dependent quantum dynamics employed wavepackets built from superpositions of field-free eigenstates including all rotational states of the molecule with J ≤ 40, where J is the quantum number of overall angular momentum. Only the vibrational ground state was considered, reflecting the conditions in a cold molecular beam. The time-dependent coefficients were obtained from numerical solution of the time-dependent Schrödinger equation using the time-discretization method with a time step of Δt = 10 fs and a Lanczos-based approach for the time-evolution operator.²⁷ 

The field interaction potential was represented as a multipole moment expansion of order up to the polarizability interaction tensor. The dipole moment and polarizability tensor were calculated using the coupled cluster singles and doubles with a perturbative correction to triples [CCSD(T)] method with the augmented correlation-consistent basis set aug-cc-pVTZ^28,29 in the frozen-core approximation. The calculations were performed in the experimentally determined molecular geometry²⁶ using the CFOUR quantum chemistry package.³⁰ 

The long elliptically polarized laser pulse was represented as

with the parameters E₀ = 4 × 10⁹ V/cm, corresponding to a laser peak intensity of I = 6 × 10¹¹ W/cm², ω = 800 nm, t₀ = 440 ps, and τ = 250 ps. The calculations were performed for β angles ranging from 0° to 90°. For some calculations, we added the interaction between the permanent molecular dipole moment and a static electric field of 1 kV/cm or 5 kV/cm aligned along the detector norm vector e_X. A hypothetical strong probe pulse, causing the Coulomb explosion, was applied at a time of t = 440 ps corresponding to the peak intensity of the alignment field. Idealized simulations were performed at an initial rotational temperature of T = 0 K and for experimentally realistic conditions at T = 0.2 K. Sub-Kelvin rotational temperatures can routinely be achieved using carefully optimized supersonic expansions,^31–33 molecular beams coupled to the electrostatic deflector,^34–36 or focusers.^37–39 Alternatively, helium nanodroplets provide comparably low temperatures of 0.4 K⁴⁰ and allow for similar Coulomb explosion imaging experiments of aligned molecules,⁴¹ including some large and complex systems.⁴² Beyond that, buffer-gas-cooled molecular beams provide molecules in the gas phase at temperatures down to ∼1 K⁴³ or using dilution refrigerators even at <0.5 K.⁴⁴ Such buffer gas-cooled beams were demonstrated for complex molecules⁴⁵ and recently extended to arbitrarily large molecular systems and nanoparticles.⁴⁶ 

The degree of 3D alignment is characterized by $⟨cos2θp,ZL⟩=0.84$ and $⟨cos2θq,XL⟩=0.76$ for T = 0 K. For a finite initial temperature of T = 0.2 K, we obtained $⟨cos2θp,ZL⟩=0.64$ and $⟨cos2θq,XL⟩=0.50$⁠.

The distributions of the methyl-group fragments of camphor in the YZ detector plane were simulated by computing the probability density distributions of the corresponding carbon atoms using the rotational wavepackets at the peak of the laser pulse. The total distribution was modeled as a normalized sum of contributions from the three individual methyl-group carbon atoms with equal weights. As the recoil axes, we chose vectors along the molecular bonds connecting the carbon atoms in the methyl groups with the backbone of the molecule. To account for non-axial recoil, the calculated probability density distributions of the methyl-group carbon atoms were convoluted with a Gaussian function of a solid angle representing angular displacement from the recoil vector. The full-width at half maximum (FWHM) parameter of the Gaussian function was chosen at 30°, which is near typical experimental values.⁴⁷ 

Figure 2(a) shows the calculated 2D projections of the probability density distributions for the carbon atoms in the methyl groups of R and S camphor for different β angles and an initial rotational temperature of T = 0 K. As expected, for β = 0°, 90°, the 2D projections are symmetric with respect to inversion of Y and Z axes. Thus, their averages for the four orientations appear identical for the different enantiomers. The 2D density projections become asymmetric with respect to inversion of the Y axis for intermediate values of the β angle. In Fig. 2(a), the results are shown for β = 30° and 60°. For different enantiomers, the distributions are exact mirror images of each other in the YZ plane. For racemic mixtures, the 2D density, and consequently the momentum projections of the methyl-group fragments, will be symmetric to inversion of the Y axis, and the presence of an asymmetry between the left and right halves of the detector will, thus, indicate the ee.

To identify the parts of the detector images, which have the largest asymmetry and are, therefore, most sensitive to the ee, we propose to define an asymmetry parameter as a normalized difference $A(θ)=[NΩ(θ)−NΩ(−θ)]/[NΩ(θ)+NΩ(−θ)]$ between sectors in the right and left halves of the detector. Here, N_Ω(θ) is the intensity in an angular sector of fixed width Ω at θ = 0° … 180°, i.e., in the right half of the detector. Thus, N_Ω(−θ) is the corresponding intensity in the left half of the detector. The asymmetry $A(θ)$ is linearly dependent on the ee: it is zero for the racemic mixture and attains its maximum value for the pure enantiomer. The asymmetry $A(θ)$ for Ω = 30° for different β values is shown in Fig. 2(b). The largest values of $A$ for the R and S enantiomers are obtained as $A≈0.22$ for β = 30° … 50° and $A≈−0.3$ for θ = 90°, respectively.

Generally, the asymmetry values $A$ depend on the molecule, its marker fragments, and their recoil axes with respect to the alignment plane. In the case of a large number of indistinguishable fragment groups attached at various molecular sites, e.g., hydrogen atoms,⁴⁸ the total probability density will appear to be more isotropic, even for strong 3D alignment. The degree of angular asymmetry will also be lowered when looking at fragments dissociating in directions nearly co-planar to either the alignment plane or the plane of detector.

In the present case, there are three indistinguishable CH₃ fragments attached at different sites of camphor. The optimal value of the β angle can be thought of as the one that maximizes the overlap of the 2D probability density distributions of different CH₃ fragments. This leads to a more anisotropic total density distribution and a better contrast with respect to variation of θ.

The magnitude of angular asymmetry $A(θ)$ also depends on the degree of 3D alignment. The lower degree of alignment for a 0.2 K sample leads to more diffuse 2D projections of the probability density distributions and, therefore, to smaller values of asymmetry $A(θ)$⁠. These are plotted in Fig. 3 for a selected optimal value of β = 40°. The maximum value of $A(θ=90°)=±0.1$ at T = 0.2 K is decreased by a factor of three as compared to the T = 0 K results. For higher temperatures close to 1 K, the asymmetry drops further by a factor of 5.3. The loss of asymmetry will vary for different molecules depending on the density of rotational states as well as their polarizability anisotropy. The present estimates of the maximum asymmetry for cold (T ≤ 0.4 K) molecular beams of camphor are comparable to those achieved in PECD experiments, where the asymmetry is defined as the normalized difference between the number of electrons emitted by the molecule in the forward and backward hemispheres relative to the laser beam.⁷ Fenchone, for example, a chiral molecule with a structure similar to the one of camphor, showed an asymmetry value of ±0.15 in PECD experiments.⁸ A key advantage of our approach over methods such as PECD or microwave three-wave mixing is access to the absolute handedness of the ee. Indeed, the position of the methyl groups with respect to the plane of 3D alignment is unique for the R and S enantiomers. As a result, the absolute sign of the left-right asymmetry in the ion momentum distributions can be unambiguously assigned to the enantiomer’s absolute configuration. Notably, in order to predict the absolute sign of the asymmetry parameter in the axial recoil approximation, it is sufficient to know the geometry of the molecule and its polarizability tensor, where only relative magnitudes of tensor elements matter.

One may consider increasing the degree of asymmetry by rendering the four equivalent alignment orientations of unequal probability. This can be achieved, for instance, by applying a dc electric field along the norm vector of the detector plane, known as mixed-field orientation.^38,49–51 We calculated the asymmetry $A(θ)$ for dc field strengths of 1 kV/cm and 5 kV/cm at T = 0 K, shown in Fig. 4; note that $A(S)=−A(R)$⁠. As the dc field breaks the symmetry with respect to the inversion of Y and Z axes, although the simultaneous inversion of both axes is still symmetric, the non-zero asymmetry can be observed even at β = 0°, 90°. The maximal degree of asymmetry increases up to ±0.4 with increasing dc field strength, and the effect, however, quickly saturates at stronger dc fields.^34,50 The absolute sign of the asymmetry, defined as the difference between the left and right halves of the detector, and the optimal values of β and θ remain the same as those for pure alignment. This is rationalized by the fact that the mixed-field orientation in camphor still allows for two of the four orientations producing the effect of 3D alignment with 1D orientation.⁵² The mixed-field orientation effect, however, can only be achieved for polar molecules with a non-vanishing projection of the dipole moment onto the pq plane of the most polarizable axes.

In conclusion, we demonstrated a novel and robust approach for detecting chirality based on the Coulomb explosion imaging of 3D aligned molecules. The method employs elliptically polarized non-resonant laser pulses in a standard setup, as is typically used for studying molecular alignment.^53,54 The chirality is revealed by an asymmetry in the 2D projections of ion momentum distributions. This paves the way for the sensitive analytical use of Coulomb explosion imaging for detecting the ee with a sensitivity comparable to PECD.^7,8,55 Any molecule with three different principal polarizability components can be investigated in this way. We note that, different from PECD, our technique requires strong alignment that is typically achieved by utilizing cold molecular beams.

Although we found that for camphor, the methyl-group fragments deliver sufficient asymmetry, these fragments could possibly exhibit larger non-axial recoil velocities not fit by the Gaussian-distribution model assumed. This would result in additional smearing effects on the structures in the ion momentum distributions. Thus, the present approach is best suited for chiral molecules with nearly axially recoiling leaving groups, but could be extended further through a more general analysis based on time-resolved measurements.⁴⁸ 

When compared to existing coincidence Coulomb explosion imaging techniques, our approach can distinguish between the left- and right-handed enantiomers without correlated detection of multiple different fragments.^3,4,18 This enables much faster data acquisition, which is highly advantageous for ultrafast time-resolved studies. For the present method, the asymmetry signal quickly declines with the beam temperature, with the efficiency similar to coincident imaging at ∼1 K. The advantage, however, is that, in principle, only one fragment type is necessary to detect chirality and handedness, as opposed to standard methods demanding up to five different fragments. The external fields can be further optimized to improve the sensitivity. In particular, we demonstrated that mixed-field orientation can be exploited to enhance the asymmetry in the ion momentum distributions and, thus, the method’s ee sensitivity. The approach could be combined with PECD in ion-electron coincidence measurements⁵⁶ to extract the ee from the photo-electron distributions together with the handedness obtained from the ion momentum distributions.

This work was supported by the Deutsche Forschungsgemeinschaft (DFG) through the priority program “Quantum Dynamics in Tailored Intense Fields” (QUTIF, SPP1840, KU 1527/3, and YA 610/1) and the cluster of excellence “Advanced Imaging of Matter” (AIM, EXC 2056, ID 390715994).