2015
DOI: 10.1002/chir.22421
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Atomistic Modeling of IR Action Spectra Under Circularly Polarized Electromagnetic Fields: Toward Action VCD Spectra

Abstract: The nonlinear response and dissociation propensity of an isolated chiral molecule, camphor, to a circularly polarized infrared laser pulse was simulated by molecular dynamics as a function of the excitation wavelength. The results indicate similarities with linear absorption spectra, but also differences that are ascribable to dynamical anharmonic effects. Comparing the responses between left- and right-circularly polarized pulses in terms of dissociation probabilities, or equivalently between R- and S-camphor… Show more

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Cited by 5 publications
(8 citation statements)
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References 76 publications
(89 reference statements)
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“…In addition to the electric dipole moment A=trueμ ${A = \vec \mu }$ or its derivative trueμ˙ ${{\dot {\vec \mu}} }$ , the VCD signal requires, for C AB , the magnetic dipole moment B=truem ${B = {\vec m}}$ that characterizes the rotation of the electric current around the axes of propagation, characteristic of circularly polarized light, to be considered. The resulting expression for the VCD intensity reads: [14,19,41,42] ΔAtrueμ˙(ω)=8πβω3Vcn(ω)-+trueμ˙(0)·m(τ)e-iωτdτ. $\vcenter{\openup.5em\halign{$\displaystyle{#}$\cr {\rm{\Delta }}A_{\dot \mu } (\omega ) = {{8\pi \beta \omega } \over {3Vcn(\omega )}}\int_{ - \infty }^{ + \infty } {\left\langle {{\dot {\vec \mu}} (0) \cdot {\vec m}(\tau )} \right\rangle } e^{ - i\omega \tau } d\tau .\hfill\cr}}$ …”
Section: Methodsmentioning
confidence: 99%
See 3 more Smart Citations
“…In addition to the electric dipole moment A=trueμ ${A = \vec \mu }$ or its derivative trueμ˙ ${{\dot {\vec \mu}} }$ , the VCD signal requires, for C AB , the magnetic dipole moment B=truem ${B = {\vec m}}$ that characterizes the rotation of the electric current around the axes of propagation, characteristic of circularly polarized light, to be considered. The resulting expression for the VCD intensity reads: [14,19,41,42] ΔAtrueμ˙(ω)=8πβω3Vcn(ω)-+trueμ˙(0)·m(τ)e-iωτdτ. $\vcenter{\openup.5em\halign{$\displaystyle{#}$\cr {\rm{\Delta }}A_{\dot \mu } (\omega ) = {{8\pi \beta \omega } \over {3Vcn(\omega )}}\int_{ - \infty }^{ + \infty } {\left\langle {{\dot {\vec \mu}} (0) \cdot {\vec m}(\tau )} \right\rangle } e^{ - i\omega \tau } d\tau .\hfill\cr}}$ …”
Section: Methodsmentioning
confidence: 99%
“…[1] In addition to the electric dipole moment A ¼ m or its derivative _ m, the VCD signal requires, for C AB , the magnetic dipole moment B ¼ m that characterizes the rotation of the electric current around the axes of propagation, characteristic of circularly polarized light, to be considered. The resulting expression for the VCD intensity reads: [14,19,41,42] DA _ m ðwÞ ¼ 8pbw 3VcnðwÞ…”
Section: Ir Absorption and Vcd Spectroscopies From Time Correlation F...mentioning
confidence: 99%
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“…[12,13] Alternatively, polarizable force fields have become sufficiently reliable to allow for the realistic modeling of entire infrared spectra, both in the gas [25][26][27][28] and condensed [25,26,[29][30][31] phases. However, so far only nonpolarizable FFs have been employed to determine VCD spectra, [10,32,33] whereas suitably parametrized polarizable FFs can handle both large systems, long sampling times, still remaining chemically accurate. The purpose of the present article is to extend the framework of polarizable force fields to the calculation of VCD spectra.…”
Section: Introductionmentioning
confidence: 99%