Erratum: Determination of structural chirality of berlinite and quartz using resonant x-ray diffraction with circularly polarized x-rays [Phys. Rev. B<b>81</b>, 144104 (2010)]

Tanaka, Yoshikazu; Kojima, Tokuzō; Takata, Y.; Chainani, A.; Lovesey, S. W.; Knight, Kevin S.; Takeuchi, Tomoyuki; Oura, M.; Senba, Yasunori; Ohashi, Haruhiko; Shin, Shik

doi:10.1103/physrevb.84.219905

Cited by 9 publications

(33 citation statements)

References 2 publications

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“…154. Figure 3 shows the RXS intensity as a function of azimuthal angle Ψ comparing with the observed ones in α-quartz and α-berlinite [4,5]. Although G is dened by k i − k f in the experiment, which is opposite to ours (see the errata in Ref.…”

Section: Calculated Results and Discussioncontrasting

confidence: 61%

“…Recently, another method has been attempted to distinguish chirality: the resonant x-ray scattering (RXS) with circularly polarized beam [4,5,6], using the Si K, Al K, and Te L1-edge resonances in α-quartz, α-berlinite, and tellurium, respectively. The tensor character of scattering matrix of RXS could give rise to the intensity on the reections forbidden in Thomson scattering [7,8,9].…”

Section: Introductionmentioning

confidence: 99%

“…The tensor character of scattering matrix of RXS could give rise to the intensity on the reections forbidden in Thomson scattering [7,8,9]. Measuring the spectra on the forbidden reections (001) and 001 , Tanaka et al [4,5,6] have found characteristic patterns depending on chirality in the spectral intensity by means of switching polarizations from the right-handed one (RCP) to the left-handed one (LCP). Regarding the oscillation of the intensity as a function of azimuthal angle, interesting phase shift has been also observed.…”

Section: Introductionmentioning

confidence: 99%

“…The amount of the phase shift strongly depends on the excitation energy. It has been suggested that the phase shift might be due to the interference between the parity even E1E1 and the parity-odd E1E2 or E1M1 events [4,5,6]. As a possible mechanism for the phase shift, the birefringence might not be ignored.…”

Section: Introductionmentioning

confidence: 99%

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Resonant x-ray scattering from chiral materials: α-quartz, α-berlinite, and tellurium

Takahashi

Igarashi

2014

J. Phys.: Conf. Ser.

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Section: Calculated Results and Discussioncontrasting

confidence: 61%

Section: Introductionmentioning

confidence: 99%

Section: Introductionmentioning

confidence: 99%

Section: Introductionmentioning

confidence: 99%

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Resonant x-ray scattering from chiral materials: α-quartz, α-berlinite, and tellurium

Takahashi

Igarashi

2014

J. Phys.: Conf. Ser.

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“…The structure factors and corresponding intensities of the screw-axis forbidden reflections in right-handed and left-handed crystals are very different for right and left circular polarizations even in pure d-d approximation. Only recently this was experimentally confirmed for low quartz [44] (SiO 2 , Si K-edge), berlinite [45] (AlPO 4 , P K-edge), CsCuCl 3 [46] Fig. 8.…”

Section: Resultsmentioning

confidence: 99%

Anisotropic resonant X-ray scattering: Beauty of forbidden reflections

Kokubun

Дмитриенко

2012

Eur. Phys. J. Spec. Top.

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Abstract. Experimental results and their theoretical explanation are reviewed for fundamentals of anisotropic resonant X-ray scattering. Resonant scattering depends on X-ray polarization, i.e. the scattering reflects anisotropic environment of atoms in crystal. The polarization anisotropy in atomic scattering can excite the forbidden Bragg reflections. Studying this type of forbidden reflections we can distinguish electronic orbitals of specific symmetry. This method is very useful for studying local electronic states in crystal. We reveal detailed property of the anisotropic scattering, effect of quadrupole transition, thermal motion, magnetic scattering and so on. Especially successful examples are given in detail: observation of phase of the scattering factor, the hybridization of states with different parity, local chirality of atom in centrosymmetric crystals, thermal-motion-induced resonant reflections, etc.

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Flexible chiral pyrazolate-based metal–organic framework containing saddle-type Cu^I₄(pyrazolate)₄units

et al. 2016

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The syntheses and crystal structures of [Cu I 2 (phbpz)]·MeOH (lp-CFA-9, lp = large-pore) and [Cu I 2 (phbpz)] (np-CFA-9, np = narrow-pore; H 2 -phbpz = 3,3′,5,5′-tetraphenyl-1H,1′H-4,4′-bipyrazole) are described. The copper(I)-containing metal-organic framework (termed C _oordination F _ramework A _ugsburg University-9, lp-CFA-9) crystallizes in the trigonal crystal system, within the chiral space group P3 2 21 (no. 154) and with the following unit cell parameters: a =18.2348(6), c = 16.3950(4) Å, and V = 4721.1(2) Å 3 . Lp-CFA-9 features a 3-D microporous framework structure of Cu 4 pz 4 (pz = pyrazolate) SBUs with the D 2d (= 42m) symmetry connected by single bonds creating one-dimensional channels expanding in the c-direction of the crystal lattice. The framework flexibility of CFA-9 has been demonstrated by single-crystal and powder X-ray analyses as well as by sorption measurements. CFA-9 exhibits weak binding of carbon monoxide on Cu(I) centers. The reactivity of CFA-9 towards oxidizing agents, such as H 2 O 2 , t-BuOOH and Br 2 was also investigated. Additionally, CFA-9 shows luminescence upon exposure to UV radiation. CrystEngComm, 2016, 18, 7883-7893 | 7883 This journal is † Electronic supplementary information (ESI) available: Ortep-style plot of the asymmetric units; topology analysis; XRPD patterns of lp-and np-CFA-9; and IR spectrum and gas sorption measurements of CFA-9. CCDC 1488850 and 1488851. For ESI and crystallographic data in CIF or other electronic format see

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Erratum: Determination of structural chirality of berlinite and quartz using resonant x-ray diffraction with circularly polarized x-rays [Phys. Rev. B81, 144104 (2010)]

Cited by 9 publications

References 2 publications

Resonant x-ray scattering from chiral materials: α-quartz, α-berlinite, and tellurium

Resonant x-ray scattering from chiral materials: α-quartz, α-berlinite, and tellurium

Anisotropic resonant X-ray scattering: Beauty of forbidden reflections

Flexible chiral pyrazolate-based metal–organic framework containing saddle-type Cu^I₄(pyrazolate)₄units

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Erratum: Determination of structural chirality of berlinite and quartz using resonant x-ray diffraction with circularly polarized x-rays [Phys. Rev. B81, 144104 (2010)]

Cited by 9 publications

References 2 publications

Resonant x-ray scattering from chiral materials: α-quartz, α-berlinite, and tellurium

Resonant x-ray scattering from chiral materials: α-quartz, α-berlinite, and tellurium

Anisotropic resonant X-ray scattering: Beauty of forbidden reflections

Flexible chiral pyrazolate-based metal–organic framework containing saddle-type CuI4(pyrazolate)4units

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Flexible chiral pyrazolate-based metal–organic framework containing saddle-type Cu^I₄(pyrazolate)₄units