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Double-core excitations in formamide can be probed by X-ray double-quantum-coherence spectroscopy
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10.1063/1.4798635
/content/aip/journal/jcp/138/14/10.1063/1.4798635
http://aip.metastore.ingenta.com/content/aip/journal/jcp/138/14/10.1063/1.4798635
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

Schematics of self-consistent calculation of core-excited states. The ECA (left) replaces a core with the next highest element in the periodic table, the FCH (middle) fixes the occupation of the core-orbital, neglecting the excited electron, whereas the XCH (right) fixes the occupation of both orbitals.

Image of FIG. 2.
FIG. 2.

The XDQC technique.

Image of FIG. 3.
FIG. 3.

(Left) The two diagrams contributing to the double quantum coherence signal. (Right) Molecular structure and REW-TDDFT level scheme. |O j N i ⟩ refers to the double core-excited states with the O1s electron excited to the jth virtual orbital of the self-consistent core state, while the N1s to ith orbital excitation is obtained through response theory, as described in the text.

Image of FIG. 4.
FIG. 4.

Calculated (grey) nitrogen (left) and oxygen (right) K-edge XANES for formamide. Experimental EELS spectra 137 are given as black lines, and power spectra of the pulses used in the calculation of the 2D-QCS signals as dashed lines. The simulated energies were shifted (+13.065 eV for nitrogen and +14.5 eV for oxygen K-edge) to fit the EELS signals. 137

Image of FIG. 5.
FIG. 5.

The ONNO signal with XXXX polarization configuration. The total signal (left column) is the sum of the contributions from diagram A (middle column) and diagram B (right column) of Fig. 3 . Each circle in the stick spectra (top row) has a complex contribution to the signal from a combination of states, with the radius of the circle proportional to the square root of the amplitude, and colored according to the phase of the contributing peak. The following three rows show the absolute value, real and imaginary parts of the complex signal after convoluting with a Lorentzian of width 0.1 eV. All signals were scaled so that abs( ) has a maximum value of one.

Image of FIG. 6.
FIG. 6.

Same as Fig. 5 , but for the pulse sequence NONO.

Image of FIG. 7.
FIG. 7.

Comparison of the absolute parts of the ONNO (left) and NONO (right) signals. XANES spectra are shown in the marginals.

Image of FIG. 8.
FIG. 8.

Dominant MOs of single particle orbitals of different SCESs discussed in Sec. VI B . (a) For peak E and A′. (b) For peak F (c) For peak D. Peaks are labeled in Fig. 4 .

Image of FIG. 9.
FIG. 9.

Comparison of the two protocols to calculate the double-core excited states | f ⟩ for the all-parallel ONNO signal as discussed in Sec. VI B . Contributions from diagram A (left column) and B (right column) with protocols i (top row) or protocol ii (bottom row). All graphs were multiplied by the same scaling factor used in Fig. 5 .

Image of FIG. 10.
FIG. 10.

for the ONNO pulse configuration.

Image of FIG. 11.
FIG. 11.

for the NONO pulse configuration.

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/content/aip/journal/jcp/138/14/10.1063/1.4798635
2013-04-10
2014-04-23
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Double-core excitations in formamide can be probed by X-ray double-quantum-coherence spectroscopy
http://aip.metastore.ingenta.com/content/aip/journal/jcp/138/14/10.1063/1.4798635
10.1063/1.4798635
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