000859490 001__ 859490
000859490 005__ 20210130000311.0
000859490 0247_ $$2doi$$a10.1007/s00269-018-1015-5
000859490 0247_ $$2ISSN$$a0342-1791
000859490 0247_ $$2ISSN$$a1432-2021
000859490 0247_ $$2WOS$$aWOS:000466218200002
000859490 037__ $$aFZJ-2019-00343
000859490 082__ $$a530
000859490 1001_ $$00000-0001-8348-7181$$aGatta, G. Diego$$b0$$eCorresponding author
000859490 245__ $$aH-bonding in lazulite: a single-crystal neutron diffraction study at 298 and 3 K
000859490 260__ $$aHeidelberg$$bSpringer$$c2019
000859490 3367_ $$2DRIVER$$aarticle
000859490 3367_ $$2DataCite$$aOutput Types/Journal article
000859490 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1556611463_30235
000859490 3367_ $$2BibTeX$$aARTICLE
000859490 3367_ $$2ORCID$$aJOURNAL_ARTICLE
000859490 3367_ $$00$$2EndNote$$aJournal Article
000859490 520__ $$aThe crystal structure and crystal chemistry of a lazulite from Crosscut Creek (Kulan Camp area, Dawson mining district, Yukon, Canada) was investigated by electron microprobe analysis in wavelength-dispersive mode (EMPA) and single-crystal neutron diffraction at 298 and 3 K. Its empirical formula, based on EMPA data, is: (Mg0.871Fe0.127)Σ0.998Al2.030(P1.985Ti0.008Si0.007O4)2(OH)2. The neutron diffraction experiments at room and low T proved that the H-free structural model of lazulite previously reported, on the basis of X-ray structure refinement, is correct: the building unit of the lazulite structure consists of a group of three face-sharing (Al-octahedron) + (Mg,Fe-octahedron) + (Al-octahedron), connected to the adjacent one via a corner-shared OH-group and two corner-shared oxygen sites of the P-tetrahedron, to form a dense 3D-edifice. Only one crystallographically independent H site occurs in the structure of lazulite, forming a hydroxyl group with the O5 oxygen, with O5–H = 0.9997 Å at room temperature (corrected for riding motion effect). The H-bonding scheme in the structure of lazulite is now well defined: a bifurcated bonding scheme occurs with the O4 and O2 oxygen sites as acceptors. The two H-bonds are energetically different, as shown by their bonding geometry: the H-bond with the O2 site as acceptor is energetically more favorable, being O5–H···O2 = 152.67(9)°, O5···O2 = 3.014(1) Å and H···O2 = 2.114(1) Å, whereas that with O4 as acceptor is energetically more costly, being O5–H···O4 = 135.73(8)°, O5···O4 = 3.156(1) Å and H···O4 = 2.383(1) Å, at room temperature. No T-induced phase transition occurs within the T-range investigated. At low temperature, the O5–H···O2 bond is virtually identical to the room-T one, whereas the effects of T on O5–H···O4 are more pronounced, with significant differences of the Odonor···Oacceptor and H···Oacceptor distances. The experimental findings of this study do not support the occurrence of HPO4 or H2PO4 units into the structure of lazulite, recently reported on the basis of infrared and Raman spectra.
000859490 536__ $$0G:(DE-HGF)POF3-6G4$$a6G4 - Jülich Centre for Neutron Research (JCNS) (POF3-623)$$cPOF3-623$$fPOF III$$x0
000859490 536__ $$0G:(DE-HGF)POF3-6G15$$a6G15 - FRM II / MLZ (POF3-6G15)$$cPOF3-6G15$$fPOF III$$x1
000859490 588__ $$aDataset connected to CrossRef
000859490 65027 $$0V:(DE-MLZ)SciArea-240$$2V:(DE-HGF)$$aCrystallography$$x0
000859490 65027 $$0V:(DE-MLZ)SciArea-140$$2V:(DE-HGF)$$aGeosciences$$x1
000859490 65017 $$0V:(DE-MLZ)GC-170-2016$$2V:(DE-HGF)$$aEarth, Environment and Cultural Heritage$$x0
000859490 693__ $$0EXP:(DE-MLZ)HEIDI-20140101$$1EXP:(DE-MLZ)FRMII-20140101$$5EXP:(DE-MLZ)HEIDI-20140101$$6EXP:(DE-MLZ)SR9b-20140101$$aForschungs-Neutronenquelle Heinz Maier-Leibnitz $$eHEiDi: Single crystal diffractometer on hot source$$fSR9b$$x0
000859490 7001_ $$0P:(DE-HGF)0$$aVignola, Pietro$$b1
000859490 7001_ $$0P:(DE-HGF)0$$aRotiroti, Nicola$$b2
000859490 7001_ $$0P:(DE-Juel1)164297$$aMeven, Martin$$b3
000859490 773__ $$0PERI:(DE-600)1463021-7$$a10.1007/s00269-018-1015-5$$n5$$p449-458$$tPhysics and chemistry of minerals$$v46$$x1432-2021$$y2019
000859490 8564_ $$uhttps://juser.fz-juelich.de/record/859490/files/Gatta2019_Article_H-bondingInLazuliteASingle-cry.pdf$$yRestricted
000859490 8564_ $$uhttps://juser.fz-juelich.de/record/859490/files/Gatta2019_Article_H-bondingInLazuliteASingle-cry.pdf?subformat=pdfa$$xpdfa$$yRestricted
000859490 909CO $$ooai:juser.fz-juelich.de:859490$$pVDB$$pVDB:MLZ
000859490 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)164297$$aForschungszentrum Jülich$$b3$$kFZJ
000859490 9101_ $$0I:(DE-588b)36225-6$$6P:(DE-Juel1)164297$$aRWTH Aachen$$b3$$kRWTH
000859490 9101_ $$0I:(DE-588b)4597118-3$$6P:(DE-Juel1)164297$$aHeinz Maier-Leibnitz Zentrum$$b3$$kMLZ
000859490 9131_ $$0G:(DE-HGF)POF3-623$$1G:(DE-HGF)POF3-620$$2G:(DE-HGF)POF3-600$$3G:(DE-HGF)POF3$$4G:(DE-HGF)POF$$9G:(DE-HGF)POF3-6G4$$aDE-HGF$$bForschungsbereich Materie$$lVon Materie zu Materialien und Leben$$vFacility topic: Neutrons for Research on Condensed Matter$$x0
000859490 9131_ $$0G:(DE-HGF)POF3-6G15$$1G:(DE-HGF)POF3-6G0$$2G:(DE-HGF)POF3-600$$3G:(DE-HGF)POF3$$4G:(DE-HGF)POF$$9G:(DE-HGF)POF3-6G15$$aDE-HGF$$bForschungsbereich Materie$$lGroßgeräte: Materie$$vFRM II / MLZ$$x1
000859490 9141_ $$y2019
000859490 915__ $$0StatID:(DE-HGF)0420$$2StatID$$aNationallizenz
000859490 915__ $$0StatID:(DE-HGF)0200$$2StatID$$aDBCoverage$$bSCOPUS
000859490 915__ $$0StatID:(DE-HGF)0300$$2StatID$$aDBCoverage$$bMedline
000859490 915__ $$0StatID:(DE-HGF)0100$$2StatID$$aJCR$$bPHYS CHEM MINER : 2017
000859490 915__ $$0StatID:(DE-HGF)0600$$2StatID$$aDBCoverage$$bEbsco Academic Search
000859490 915__ $$0StatID:(DE-HGF)0030$$2StatID$$aPeer Review$$bASC
000859490 915__ $$0StatID:(DE-HGF)0199$$2StatID$$aDBCoverage$$bClarivate Analytics Master Journal List
000859490 915__ $$0StatID:(DE-HGF)0110$$2StatID$$aWoS$$bScience Citation Index
000859490 915__ $$0StatID:(DE-HGF)0150$$2StatID$$aDBCoverage$$bWeb of Science Core Collection
000859490 915__ $$0StatID:(DE-HGF)0111$$2StatID$$aWoS$$bScience Citation Index Expanded
000859490 915__ $$0StatID:(DE-HGF)1150$$2StatID$$aDBCoverage$$bCurrent Contents - Physical, Chemical and Earth Sciences
000859490 915__ $$0StatID:(DE-HGF)9900$$2StatID$$aIF < 5
000859490 920__ $$lyes
000859490 9201_ $$0I:(DE-Juel1)JCNS-FRM-II-20110218$$kJCNS-FRM-II$$lJCNS-FRM-II$$x0
000859490 9201_ $$0I:(DE-Juel1)JCNS-2-20110106$$kJCNS-2$$lStreumethoden$$x1
000859490 9201_ $$0I:(DE-588b)4597118-3$$kMLZ$$lHeinz Maier-Leibnitz Zentrum$$x2
000859490 980__ $$ajournal
000859490 980__ $$aVDB
000859490 980__ $$aI:(DE-Juel1)JCNS-FRM-II-20110218
000859490 980__ $$aI:(DE-Juel1)JCNS-2-20110106
000859490 980__ $$aI:(DE-588b)4597118-3
000859490 980__ $$aUNRESTRICTED