Letter | Published:

Imaging molecular potentials using ultrahigh-resolution resonant photoemission

Nature Physics volume 8, pages 135138 (2012) | Download Citation

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  • A Corrigendum to this article was published on 01 December 2015

This article has been updated

Abstract

Electron-density distributions and potential-energy surfaces are important for predicting the physical properties and chemical reactivity of molecular systems. Whereas angle-resolved photoelectron spectroscopy enables the reconstruction of molecular-orbital densities of condensed species1, absorption or traditional photoelectron spectroscopy are widely employed to study molecular potentials of isolated species. However, the information they provide is often limited because not all vibrational substates are excited near the vertical electronic transitions from the ground state. Moreover, many electronic states cannot be observed owing to selection rules or low transition probabilities. In many other cases, the extraction of the potentials is impossible owing to the high densities of overlapping electronic states. Here we use resonant photoemission spectroscopy, where the absence of strict dipole selection rules in Auger decay enables access to a larger number of final states as compared with radiative decay. Furthermore, by populating highly excited vibrational substates in the intermediate core-excited state, it is possible to ‘pull out’ molecular states that were hidden by overlapping spectral regions before.

Main

Rydberg–Klein–Rees2 is one of the most popular methods to reconstruct molecular potentials for stable states of diatomic molecules from rovibrational spectroscopy data without requiring any assumption about the shape of the potential. It is in a way a complementary method to the direct imaging of molecular orbitals to study molecular structures3. Alternative approaches have been proposed on the basis of a fitting procedure of analytical potential functions to experimental data2,4. Here we show how powerful the use of core excitation can be for extracting molecular-potential curves of ionic states exclusively on the basis of ultrahigh-resolution resonant photoemission (RPE) data as obtained for N2. This has been achieved when controlling the extension of vibrational wavefunctions by fine tuning the X-ray energy. Indeed, tuning of the X-ray energy enables the spatial distribution of the vibrational wavefunctions in the intermediate state to be selected, and thus the extension of the probed region of the final-state potential to be controlled. Here we report the observation of the 12ϕg and 12Δu states of N2+and the accurate reconstruction of the 12Πg and 12ϕg molecular potentials, demonstrating that state-of-the-art RPE spectroscopy can be successfully used to solve the problem of potential reconstruction for excited molecular states directly from experimental data, and to identify such new states, invisible in conventional photoemission spectroscopy.

Unlike direct photoemission, where the absorption of an X-ray photon of energy ω (where ω is the X-ray frequency) leads to the emission of a photoelectron, in the RPE process the resonant absorption of an X-ray photon populates final ionic states of the molecule by ejecting resonant Auger electrons with kinetic energies Ek. Our measurements were made in the sublifetime regime (X-ray spectral bandwidth and spectrometer resolution considerably lower than the natural lifetime broadening 115±4 meV (ref. 5), enabling unprecedented total linewidth of less than 52 meV; Methods), following selective vibrational excitation within the N1sπ* transition in gas-phase nitrogen molecules. The data were collected at the soft-X-ray PLEIADES beamline dedicated to the investigation of isolated species, at the synchrotron SOLEIL, France. This state-of-the-art spectroscopy facility, briefly described in refs 6, 7, benefits from the improved spectral brightness of SOLEIL combined with innovative X-ray optics and instrumentation (Supplementary Information), and provides a unique opportunity to make highly demanding measurements. Indeed, in the present case its exceptional performance has enabled us to overcome the low number of ejected electrons due to (1) the normally low number of X-ray photons in the very narrow bandwidth and (2) the significant drop, of more than one order of magnitude, of the photoexcitation cross-section in the region far above the vertical transition from the ground-state geometry. However, reaching the highly excited and almost invisible vibrational level ν=6 in the 1s−1π* state has been crucial to the full exploration of the molecular potentials. On the basis of these conditions we have been able to solve the inverse problem of molecular potential reconstruction using ultrahigh-resolution RPE spectra obtained over a broad range of X-ray energies, enabling the size of the vibrational wavefunctions in the core-excited state to be accurately targeted. This Letter explains how this goal was achieved.

Figure 1 shows the ab initio calculated potentials (Methods) of the molecular ion N2+ (centre panel) together with the experimental photoemission (left-hand panel) and RPE (right-hand panel) spectra plotted on a binding-energy scale Eb=ωEk. The RPE spectrum shown was obtained when the X-ray energy was tuned to the ν=0vibrational substate of the 1s−1π* state. Calculations (Methods) indicate a remarkably high density of final states in the region Eb=24–30 eV. Indeed, ten final electronic states build up the RPE spectrum (see Fig. 1 for the assignment of the individual bands). Partial contributions to the RPE spectrum drawn as coloured areas in Fig. 1 show the strong overlap of these ten bands associated with Auger decays, to either bound or dissociative (high- Eb region) final states. Consequently, the first impression might be that RPE does not enable the accurate characterization of molecular potentials to be made. Nevertheless, looking at the weak spectral feature below Eb≈23.5 eVin the bottom spectrum (ν=0) of Fig. 2 and its evolution when RPE spectra are recorded for a selection of X-ray energies successively tuned in resonance with the next six vibrational substates ν=1–6 of the 1s−1π* core-excited state (see Fig. 3b). Indeed, tuning the X-ray energy to higher vibrational substates enables this spectral feature, hidden in the region of overlap, to be ‘pulled out’ into the lower- Eb energy region, where it becomes available for investigation. This is experimentally very demanding because the RPE intensity drops dramatically for these low-cross-section highly excited states. The photoexcitation cross-section to the ν=6 vibrational sublevel is so low that it can barely be observed, even in the absorption spectrum shown in Fig. 3b.

Figure 1: Ab initio potential-energy curves, direct photoemission (PE) and RPE spectra of N2.
Figure 1

Ab initio calculated potential-energy curves of the ground, intermediate (core-excited) and final ionic (N2+) states are shown in the central panel. A strong congestion of states can be observed around the vertical transition from the zero-point vibrational level of the ground electronic state shown by the ascending grey arrow. In addition to the resulting spectral band overlap, some states are ‘dark’ in the photoemission spectrum recorded at 100 eV photon energy (left-hand panel). The ground-state nuclear wave packet excited to the intermediate-state potential (grey) continuously undergoes Auger decay (pink) to final ionic states, as indicated by the descending pink arrow. Owing to the nuclear dynamics in the core-excited state, the decay takes place at larger internuclear distances, providing the opportunity to visualize the potentials in a region free of any overlap. Experimental and calculated partial contributions to the RPE spectrum of the nitrogen molecule for the X-ray energy tuned to the lowest vibrational substate of the 1s−1π* core-excited state are shown in the right-hand panel. The assignment of the spectra is based on the present ab initio calculations and partially on available photoemission data23,26,27.

Figure 2: RPE spectra of nitrogen molecule obtained for a series ν=0–6 of vibrational substates of the 1s−1π* core-excited state.
Figure 2

The blue dots are the experimental data points, and the calculated RPE spectrum is shown by a black solid line. For the sake of clarity, the experimental and total theoretical RPE spectra are vertically shifted with respect to the partial RPE cross-sections shown by coloured lines. According to our simulations, five ionic states (12Πg, 12ϕg, 12Δu, 2Σu+ and 22Πg) lie in this spectral region. Previous photoelectron spectroscopy studies23,26,27,28 were only able to detect two of these states (2Σu+ and 22Πg), and earlier RPE measurements of ref. 31 show only a weak unresolved structure tentatively assigned to the 12Πg state. Tuning the photon energy in resonance with the higher vibrational sublevels (see Fig. 3b) ‘pulls out’ the 12Πg and 12ϕg spectral bands from the region of overlap (Fig. 1). Such a refinement of the RPE spectra enables us to reconstruct the potentials of individual electronic states.

Figure 3: Controlling the extension of the vibrational wavefunctions in the intermediate core-excited state through the X-ray photon energy.
Figure 3

a, Calculated potential of the 1s−1π* core-excited state and the squares of the vibrational wavefunctions of the first vibrational substates. Left (Rl) and right (Rr) classical turning points are shown for ν=6. b, Experimental (circles) and theoretical (solid line) N 1sπ* X-ray photoabsorption spectra of nitrogen molecule. c, Selected final ionic-state potentials that can be explored in the region free of mutual overlap are shown by the shaded areas.

In general, the lifetime of the intermediate state is sufficiently long (5.7±0.2 fs in the present case5), and the Auger decay taking place at the left and right classical turning points of the core-excited-state potential (Fig. 3a) plays the main role in the formation of the RPE profile. Nevertheless, the Eb range corresponding to Auger transitions from the left classical turning point lies well above 24 eV (Fig. 3c) and does not contribute in the region of interest. Therefore, below 24 eV, the RPE spectrum mainly builds up from the Auger transitions in the vicinity of the right classical turning point (Fig. 3), which shifts to larger internuclear distances when the excitation energy is increased.

Detuning the X-ray energy from the nominal energy of the vertical transitions has been shown, in previous RPE studies, to be an efficient characterization tool for nuclear dynamics8,9,10,11,12,13,14,15. We demonstrate here that it may also represent the key for molecular-potential reconstruction on the basis of spectroscopic data. Indeed, the increase in excitation energy shifts the right turning point to larger internuclear distances (Fig. 3a) and provides access to the region where final-state potentials are well separated from one another, as can be inferred from Fig. 3c. It is thus possible to avoid the ‘contamination’ of individual spectral bands from neighbouring, overlapping states. If the ν=0 substate is selected in the intermediate state, the RPE profile consists of the extensive tail of the 12Πgstate overlapping with the 2Σu+ and 22Πg bands. When increasing the X-ray energy to select higher vibrational substates (ν=1–2), the 12Πg band progressively shifts out of the region of overlap (Fig. 2). From ν≥3, the 12ϕg state vibrational progression also becomes available. Moreover, it is fundamental to note that both 12Πg and 12ϕg states can be fully explored down to their ground vibrational substates only when the highest vibrational levels ν=5–6 are selected in the intermediate state. The visible modulation of the intensity distribution within the vibrational progression of the 12Πg state fingerprints accurately the nodal structure of the vibrational wavefunction of the core-excited state, in agreement with the reflection principle—the basis for the mapping technique16. The temptation to use the mapping technique to obtain information about molecular potentials has motivated several studies (see for instance refs 13, 17), but unfortunately the extracted information was rather poor. Instead, we propose here to accurately reconstruct the final-state potentials using the full vibrationally resolved RPE spectrum. The accuracy of this method is high as soon as a large number of vibrational states is populated. We used the sum of all RPE spectra recorded for the series ν=0–6 of vibrational substates to maximize the extension of the vibrational progressions observable in the resulting RPE spectrum. These progressions have been fitted following standard procedures described in Supplementary Information. The molecular constants were obtained from the fits, and the potential has been reconstructed using the general Morse function18. The same procedure has also been applied to reconstruct the 12ϕg-state potential. The reconstructed potentials for the 12Πg and 12ϕg ionic states are shown together with the ab initio calculated potentials in Fig. 4. It is important to note that remarkably good agreement is obtained with the Rydberg–Klein–Rees-based potential19 for the 12Πg state not only for the vibrational frequency ωeand the anharmonicity parameter, xeωe, but also for the dissociation energy (Supplementary Table S1). As our experiment provides the first observation of the 12ϕg state we are unable to compare the results (Supplementary Table S1) with independent data. Nevertheless, the reconstructed potential of this newly observed state is also in good agreement with the ab initio potential as shown in Fig. 4. We would like to emphasize that the 12Δu band, which becomes visible starting from ν≥2 (Fig. 2), is also observed experimentally for the first time.

Figure 4: Comparison between the reconstructed molecular potentials based on ultrahigh-resolution RPE data and ab initio calculated potentials (circles).
Figure 4

Solid lines show potential-energy curves of the 12Πg and 12ϕg final ionic states reconstructed from the RPE experimental data using the general Morse function18: E(r)=Emin+D[1+(λ2eλ1rλ1eλ2r)/(λ1λ2)]. Here r=RRe and Re is the bond length at the minimum of the potential as obtained from the fitting of the vibrational progression. The energy interval used for potential reconstruction is delimited by the darker areas. The uncertainty in the reconstructed potential curves (light blue) was obtained by error propagation for the general Morse function using the standard deviations for the spectroscopic constants (see Supplementary Information).

In conclusion, recording ultrahigh-resolution RPE spectra over a wide excitation-energy range offers a unique opportunity to image the potential-energy curves in an extended spatial domain where the X-ray-driven nuclear wave packet in the core-excited state plays the role of a local probe controlled by the photon energy. Tuning the excitation energy is a key feature to overcome the rather common issue of overlapping molecular spectral bands. We show that state-of-the-art RPE spectroscopy can be successfully used to solve the problem of potential reconstruction for excited molecular states directly from experimental data, and to identify such new states, invisible in conventional photoemission spectroscopy. The demonstration was made using a textbook case—the nitrogen molecule. However, we suggest that our method is general and can be extended to larger species and easily transposed to neutral molecular-state potentials by detecting the radiative decay.

Methods

The experiment was carried out at the PLEIADES beamline6,7 at the SOLEIL synchrotron in Saint-Aubin, France. The beamline covers the 7–1,000 eV energy range, with any polarization. Monochromatic light is obtained from a plane grating monochromator with no entrance slit. Typical photon fluxes up to 1013 photons s−1 per 0.1% bandwidth are available and an ultimate resolving power of approximately 105 is achievable at 50 eV. The measurements were made using a VG-Scienta R4000 electron spectrometer mounted with the electron detection axis vertical. X-ray polarization was set at the magic angle of 54.7° with respect to this axis. Pure nitrogen (99.998%) from Air Liquide was used and the pressure in the vacuum chamber was kept constant around 1×10−5 mbar. The monochromator slit was 40 μm, corresponding to a photon bandwidth better than 20 meV at 401 eV. The electron spectrometer was operated at a 20 eV pass energy, providing a kinetic energy resolution of 15 meV. The resulting total instrumental broadening was less than 52 meV.

The potential-energy curves of the ground, core-excited and final ionic states of N2 were computed using the configuration-interaction approach implemented in the GSCF3 quantum chemical package20,21. We used the basis set and polarization function (10s7p1d) of ref. 22 contracted as [5221/52/1]. The full valence configuration interaction for the 2σg, 3σg, 2σu, 3σu*, 1πu and 1πg* orbitals, and single and double configuration interaction for external orbitals from the full valence space (namely, second-order configuration interaction), was carried out. The results obtained are in good agreement with previous calculations23,24,25 and experiments26,27,28 for N2+. To simulate the RPE spectra, the time-dependent wave-packet approach was used29,30. The total spectrum has been obtained as a superposition of contributions of the individual electronic states. Calculated spectra were convoluted with appropriate Gaussian functions to account for the experimental broadenings.

Change history

  • 19 November 2015

    In the version of this Letter originally published the state with Emin = 23 eV was mislabelled throughout and should have been labelled 12ϕg. This has been corrected in the online versions 19 November 2015.

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Acknowledgements

Experiments were carried out at the PLEIADES beamline at SOLEIL Synchrotron, France (proposal number 99090106). We are grateful to J. B. A. Mitchell for his suggestions, to E. Robert for technical assistance and to the SOLEIL staff for smoothly running the facility. The research leading to these results has received funding from the European Union Seventh Framework Programme (FP7/2007-2013) under grant agreement 252781, from Triangle de la physique under contract 2007-010T, from JSPS and from the Swedish Research Council.

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Affiliations

  1. Synchrotron SOLEIL, l’Orme des Merisiers, Saint-Aubin, BP 48, 91192 Gif-sur-Yvette Cedex, France

    • Catalin Miron
    • , Christophe Nicolas
    • , Oksana Travnikova
    • , Paul Morin
    •  & Victor Kimberg
  2. Theoretical Chemistry, Royal Institute of Technology, S-106 91 Stockholm, Sweden

    • Yuping Sun
    •  & Faris Gel’mukhanov
  3. Institute for Molecular Science, Myodaiji, 444-8585 Okazaki, Japan

    • Nobuhiro Kosugi

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Contributions

C.M. suggested and planned the experiment. C.N., O.T. and C.M. collected the data, and V.K. and O.T. carried out the data analysis. Y.S., F.G., N.K. and V.K. carried out the theoretical analysis. C.M., F.G. and V.K. wrote the paper and O.T. contributed to figure production. All authors discussed the results and commented on the manuscript.

Competing interests

The authors declare no competing financial interests.

Corresponding author

Correspondence to Catalin Miron.

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https://doi.org/10.1038/nphys2159

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