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## pZ{FSs̋L^

 p̍Z{󂯂éAǂǂꂽׂĂ݂܂B̃TCg̍҂̉p͂΂邵Ap炷悤łȂ̂łAłȂ̂ōZ{Ђ̏𓾂ČJĂ݂܂BƓl邩܂񂵁BAԈႢȂ߂̎gւ̉߂ł܂B łAv̋Ǝ҂ɒĂƂāA[łC΂ł͂܂B܂AƎ҂łZ{҂ɂĎwEقȂꍇ܂BƂNative琳ƂȂAԈႢł͂ȂPȂ镶̂̍D݂ȂBȋƎ҂ł肢܂Âɂ̌ʂ܂MpłȂꍇĂ܂B]āAR̂ƂłAŌ͎Ŕf邵܂Bϕ׋ƁB ɒӂȂႢȂ̂́AZ{҂͉p͂ł̂ȂǁAnƂ͌ȂĂƁBȑOAȊw\L@܂ĂȂɂƂ܂B

 Z{O A small moment on the site to be near perpendicular to the field has a disadvantageous direction to the field, which is realised through the strong AFM interactions @@ A small moment on the site that is almost perpendicular to the field has a disadvantageous direction, that is realised through the strong AFM interactions (corrected by ASL) which߂that߂̎g킩ȂB Z{O This magnetic structure model explains the magnetisation process well @@ This magnetic structure models well explains the magnetisation process. (corrected by ASL) explainŏ\wellȂĂ咣ɕωȂAwell͌łƂ񂾂B Z{O The unit cell is a*a*4c in phase II. @@ The unit cell has dimensions of a*a*4c in phase II. (corrected by ASL) ujbgZa*a*4c̑傫Bv {ŋc_Ƃ̂܂܏񂾂ǁAԈႢ炵B͂̂܂܉悤BdimensionɂȂ񂾂ȁB Z{O , in order to clarify magnetic structures of field-induced phases. @@ , in order to elucidate the magnetic structures of field-induced phases. (corrected by ASL) uUNł̎C\炩ɂ߂ɁAv clarifýAӖ͂肳AƂɏdS炵B̂Aclarify the roles of the interactions͂ȂĂȂB the͂悭킩ȂBeł͂ЂƂC\Ȃ炩Hǂ̑̂ƂĂ邩ĂȂAC\ɂthe͂ȂƂ񂾂ǁB Z{O The purpose of this study is to measure the profile of the magnetic diffuse scattering in 3D reciprocal space by SXD in ISIS. @@ The purpose of this study is to measure the profile of the magnetic diffuse scattering in 3D reciprocal space on SXD in ISIS. SXD͒P\͗pܑ̉u̖OAISIS͉pɂ钆qU{݁B͂Uuon炵BlIɃFbNĂ炢܂B Z{O iDiscussionsection̖Łj Let us discuss the origin of the magnetic diffuse scattering. @@ In this section, we discuss the origin of the magnetic diffuse scattering. (corrected by ASL) ԈႢł͂Ȃ낤B̖͂ɂ͕sK؂H Z{O From the fitting procedures in Fig.~4, the half width of each Lorentzian function was estimated to be 0.038(8) r.l.u. for the broad peaks @@ Based on the fitting procedures in Fig.~4, the half width of each Lorentzian function was estimated to be (i) 0.038(8) r.l.u. for the broad peaks (corrected by ASL) from͂鋳ȏɂłĂȂ̂ŁAԈႢĂقǂłȂƎvB Z{O Detailed neutron diffraction measurements on a single crystalline sample of ErB2C2 were performed. @@ Detailed neutron diffraction measurements were performed on a single crystalline sample of ErB2C2. (corrected by ASL) ǂقǈႤ񂾂낤BԈႢł͂Ȃ̂ŁA₷̂ȁB Z{O the sharp satellite peaks which are due to the long-periodic magnetic ordering were observed. @@ iȂj sharp satellite peaks caused by the long-periodic magnetic ordering were observed. (corrected by ASL) due tołȂcaused byBʂ̂Ƃłresulting fromƂȂĂƂBwhich߂ȂȂĂȁBłATeCgs[N͂OɂȂǂoĂĂ̂theɂ񂾂ǁB Z{O The scan direction in the reciprocal space is shown above the figures with the arrow. @@ The scan direction in the reciprocal space is indicated above the figures with an arrow. (corrected by ASL) ŃXL}ĂB}ɂ󂾂the arrowłƂ񂾂ǁBłA̍Z{ҕʂȂƂłthe ĂAǂł̂ȂB Z{O In this paper, we report results of detailed neutron diffraction experiments for the rare earth compound ErB2C2, and discuss anomalous magnetic diffuse scattering which is also observed in TbB2C2 @@ In this paper, we report the results of detailed neutron diffraction experiments on the rare earth compound ErB2C2 and discuss the anomalous magnetic diffuse scattering that is also observed in TbB2C2 (corrected by ASL) _Ŝwhich߂that߂ɂȂꂽBʂ킩ȂB Z{O We performed neutron powder diffraction experiments of the lithium imide Li2NH, @@ We performed neutron powder diffraction experiments on lithium imide Li2NH, (corrected by ASL) Z{O we report results of crystal structure refinement of the lithium imide material Li2NH using neutron powder diffraction technique @@ we report the results of crystal structure refinement of the lithium imide material Li2NH using the neutron powder diffraction technique (corrected by ASL) ̑SĂ̌ʂ񍐂킯ł͂Ȃu resultsvɂ̂ǁAtheɂȂꂽB Z{O i镨̌\̐āj The structure looks, however, strange, because~ @@ However, its structure appears to be peculiar because~ (corrected by ASL) however̈ʒu͑SȂĂBƂł͂̈ʒu悭݂̂ǁA_ނł͂Ȃ̂ȂB its structurethe structurëႢ͂悭킩ȂB̎gɏd_uAƂB܂AbecausȇOɂ͂܂͂ȂȁB̍Z{ҁAڂĂ܂B Z{O because it has different characters from the lithium amide Li2NH @@ because its characteristics differ from lithium amide Li2NH (corrected by ASL) ʂȂƂit is different from͒ĂȂ̂ŁAhasĝ̂ȂB ulithium amide v͖Ałuthe lithium amide material v. Z{O We expected, thus, that the crystal structure model of Li2NH in Fig.1 is not correct; @@ Thus, we expected the crystal structure model of Li2NH in Fig.1 to be incorrect, (corrected by ASL) that߂Ⴞ߂Ȃ̂H ̈ʒuɕ͕̂ȂɂȂĂB悳B Z{O We confirmed that no structure model with these symmetries represent the data in Fig.2, @@ we confirmed that no structure model with these symmetries represented the data in Fig.2, (corrected by ASL) ̈vB΂ƎvǁAł͂قƂɎɂ͎MĂȂB̏ꍇ́AՓIȎƂĂ̌݌̂肾̂ǁB Z{O Thus, either Model I or II in Fig.4 is the correct model, @@ Thus, either Model I or II in Fig.4 can be considered to be the correct model, (corrected by ASL) is̕Xg[gł悤ȋĈǁB Z{O iQ̃fIɋʂłȂAƐāA̗RƂāj these give nearly the same agreement with the data @@ these exhibit nearly the same agreement between the data (corrected by ASL) ̕łgive͑Sق̌ɒĂBgiveŊԈႢł͂ȂƎv̂ǁA_ނł͂Ȃ̂ȂBqۂ̂Bbetween͂悭킩ȂB Z{O estimations of performance of 3He cells using lower PHe will give reasonable results @@ estimations of performance of 3He cells using lower PHe value can provide reasonable results łgiveȂꂽBB Z{O iQ̃f}Ŏāj Comparing the two models in Fig.4, we have concluded that~ @@ By comparing the two models in Fig.4, we have concluded that~ (corrected by ASL) comparing͕\̂ŏ̂ǁA߂炵BǂŁABy comparing̈Ӗ\Ă񂾋C񂾂ǁB uƌ_v͌݊ł炵B Z{O Note that the occupancy of the hydrogen site is about 80%. @@ It is notable that the occupancy of the hydrogen site is approximately 80%. (corrected by ASL) Ӗ͓͂BuNote thatv̕ZčD܂AƋ̂ł񂾂ǁAꂽBʂȍZ{҂ɂ́Ait must be notedƂȂꂽB Z{O The anomalous diffuse scattering exists in the small region in the reciprocal space surrounded by satellite peaks @@ The anomalous diffuse scattering exists in a small region in the reciprocal space surrounded by satellite peaks uTeCgs[NɈ͂܂ꂽvŌłƎvtheɂ̂ATeCgs[N肵ĂȂ肪s\Bthe͍Z{ĂȂȁB Z{O but no AFQ ordering under zero magnetic field was found so far. @@ but no AFQ ordering under zero magnetic field has been found so far. ݂܂݂ĂȂĂ̂猻݊AĎBso farƉߋ̑gݍ킹͂B͂킩ȂBZ{΂KvȂƁB Z{O as an appendant component of a much dominant k=(1,0,1/2) type AFM structure with a small k=(0,0,1/2) component @@ as an appendant component of a very dominant k=(1,0,1/2) type AFM structure with a small k=(0,0,1/2) component muchverÿႢ܂ĂȂBeĈveryBłvery dominant́AȂ񂩂Ђ鉹B u͂邩ɎxzIk=(101/2)^ɕt鐬Ƃāv Z{O R̕ł̎CIȎڋ߂ĂAƂ̌A The nearly the same periodicity probably indicates that the long periodicity is base on some common characters in RB$_2$C$_2$ system. @@ The close similarity periodicities probably indicates that the long periodicity is base on some common characters in RB$_2$C$_2$ system. ͂Ȃł߂Ȃ̂ȂB Z{O it is important to compare the long periodic states with each other to understand characteristics in RB$_2$C$_2$. @@ it is important to compare the long periodic states with each other to understand characteristics of RB$_2$C$_2$. uRB2C2nƂĂ̓v̂肾̂ǁAofł炵B Z{O The profile of the magnetic diffuse scattering can not be understood by magnetic short range correlation or critical phenomena around $T_{\rm N}$. @@ The profile of the magnetic diffuse scattering can not be understood in terms of magnetic short range correlation or critical phenomena around $T_{\rm N}$. Ȃ񂩂̖{ŁAbyin terms of ͉ŒZby̕AƓǂ񂾂̂ǁBɂĂAbyԈႢƂ͎vȂȁB Z{O comparing **** is important to understand roles of AFQ interactions for the anomaly. @@ comparing **** is important for understanding roles of AFQ interactions in the anomaly. Z{O The single crystalline sample was mounted at the cold head of a closed cycle He-gas refrigerator as the $c$-plane to be horizontal. @@ The single crystalline sample was mounted at the cold head of a closed cycle He-gas refrigerator with the $c$-plane horizontal. uíjcʂɂȂ悤ɃZbgBvB̕twith̎g͂ȂȂ}X^[łȂB Z{O Figure 2 shows a contour map of intensity of the magnetic scattering in ErB$_2$C$_2$ @@ Figure 2 shows a contour map of the intensity of the magnetic scattering in ErB$_2$C$_2$ ۓIȈӖłIntensityixĵ肾AłȂƎvĖɂ̂ǁAtheĎ́A̓IȂ̂Ɍ肳ĂĎB Z{O the authors conclude that characteristics found in the long periodic magnetic states in HoB$_2$, TbB$_2$C$_2$ and ErB$_2$C$_2$ are based on a common property in the RB$_2$C$_2$ @@ the authors conclude that characteristics found for the long periodic magnetic states in HoB$_2$, TbB$_2$C$_2$ and ErB$_2$C$_2$ are based on a common property in the RB$_2$C$_2$ uCŌvȂ̂ŁAinƂ̂ǁAforH̍Z{ҁA₽forɒĂ̂ǁB

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