There are 230 space groups in three dimensions, given by a number index, and a full name in Hermann–Mauguin notation , and a short name (international short symbol). The long names are given with spaces for readability. The groups each have a point group of the unit cell.
Contents
Symbols
In Hermann–Mauguin notation , space groups are named by a symbol combining the point group identifier with the uppercase letters describing the lattice type . Translations within the lattice in the form of screw axes and glide planes are also noted, giving a complete crystallographic space group.
These are the Bravais lattices in three dimensions :
P primitiveI body-centered (from the German Innenzentriert )F face-centered (from the German Flächenzentriert )S base-centered (from the German Seitenflächenzentriert ), or specifically:A centered on A faces onlyB centered on B faces onlyC centered on C faces onlyR rhombohedral
A reflection plane m within the point groups can be replaced by a glide plane , labeled as a , b , or c depending on which axis the glide is along. There is also the n glide, which is a glide along the half of a diagonal of a face, and the d glide, which is along a quarter of either a face or space diagonal of the unit cell. The d glide is often called the diamond glide plane as it features in the diamond structure.
a, b, or c: glide translation along half the lattice vector of this facen: glide translation along half the diagonal of this faced: glide planes with translation along a quarter of a face diagonale: two glides with the same glide plane and translation along two (different) half-lattice vectors.[note 1]
A gyration point can be replaced by a screw axis denoted by a number, n , where the angle of rotation is \color{Black}\tfrac{360^\circ}{n}. The degree of translation is then added as a subscript showing how far along the axis the translation is, as a portion of the parallel lattice vector. For example, 21 is a 180° (twofold) rotation followed by a translation of 1 ⁄2 of the lattice vector. 31 is a 120° (threefold) rotation followed by a translation of 1 ⁄3 of the lattice vector. The possible screw axes are: 21 , 31 , 32 , 41 , 42 , 43 , 61 , 62 , 63 , 64 , and 65 .
Wherever there is both a rotation or screw axis n and a mirror or glide plane m along the same crystallographic direction, they are represented as a fraction \frac{n}{m} or n/m . For example, 41 /a means that the crystallographic axis in question contains both a 41 screw axis as well as a glide plane along a .
In Schoenflies notation , the symbol of a space group is represented by the symbol of corresponding point group with additional superscript. The superscript doesn't give any additional information about symmetry elements of the space group, but is instead related to the order in which Schoenflies derived the space groups. This is sometimes supplemented with a symbol of the form \Gamma_x^y which specifies the Bravais lattice. Here x \in \{t, m, o, q, rh, h, c\} is the lattice system, and y \in \{\empty, b, v, f\} is the centering type.[1]
In Fedorov symbol , the type of space group is denoted as s (symmorphic ), h (hemisymmorphic ), or a (asymmorphic ). The number is related to the order in which Fedorov derived space groups. There are 73 symmorphic, 54 hemisymmorphic, and 103 asymmorphic space groups.
Symmorphic
The 73 symmorphic space groups can be obtained as combination of Bravais lattices with corresponding point group. These groups contain the same symmetry elements as the corresponding point groups. Example for point group 4/mmm (\tfrac{4}{m}\tfrac{2}{m}\tfrac{2}{m}): the symmorphic space groups are P4/mmm (P\tfrac{4}{m}\tfrac{2}{m}\tfrac{2}{m}, 36s ) and I4/mmm (I\tfrac{4}{m}\tfrac{2}{m}\tfrac{2}{m}, 37s ).
Hemisymmorphic
The 54 hemisymmorphic space groups contain only axial combination of symmetry elements from the corresponding point groups. Example for point group 4/mmm (\tfrac{4}{m}\tfrac{2}{m}\tfrac{2}{m}): hemisymmorphic space groups contain the axial combination 422, but at least one mirror plane m will be substituted with glide plane, for example P4/mcc (P\tfrac{4}{m}\tfrac{2}{c}\tfrac{2}{c}, 35h ), P4/nbm (P\tfrac{4}{n}\tfrac{2}{b}\tfrac{2}{m}, 36h ), P4/nnc (P\tfrac{4}{n}\tfrac{2}{n}\tfrac{2}{c}, 37h ), and I4/mcm (I\tfrac{4}{m}\tfrac{2}{c}\tfrac{2}{m}, 38h ).
Asymmorphic
The remaining 103 space groups are asymmorphic. Example for point group 4/mmm (\tfrac{4}{m}\tfrac{2}{m}\tfrac{2}{m}): P4/mbm (P\tfrac{4}{m}\tfrac{2_1}{b}\tfrac{2}{m}, 54a ), P42 /mmc (P\tfrac{4_2}{m}\tfrac{2}{m}\tfrac{2}{c}, 60a ), I41 /acd (I\tfrac{4_1}{a}\tfrac{2}{c}\tfrac{2}{d}, 58a ) - none of these groups contains the axial combination 422.
List of triclinic
Triclinic Bravais lattice
List of monoclinic
Monoclinic Bravais lattice Simple (P) Base (S)
Monoclinic crystal system Number Point group Orbifold Short name Full name(s) Schoenflies Fedorov Shubnikov Fibrifold (primary)Fibrifold (secondary)3 2 22P2 P 1 2 1 P 1 1 2 \Gamma_mC_2^13s (b:(c/a)):2(2_02_02_02_0)({*}_0{*}_0)4 P21 P 1 21 1 P 1 1 21 \Gamma_mC_2^21a (b:(c/a)):2_1(2_12_12_12_1)(\bar{\times}\bar{\times})5 C2 C 1 2 1 B 1 1 2 \Gamma_m^bC_2^34s \left ( \tfrac{a+b}{2}/b:(c/a)\right ) :2(2_02_02_12_1)({*}_1{*}_1), ({*}\bar{\times})6 m *Pm P 1 m 1 P 1 1 m \Gamma_mC_s^15s (b:(c/a))\cdot m[\circ_0]({*}{\cdot}{*}{\cdot})7 Pc P 1 c 1 P 1 1 b \Gamma_mC_s^21h (b:(c/a))\cdot \tilde c(\bar\circ_0)({*}{:}{*}{:}), ({\times}{\times}_0)8 Cm C 1 m 1 B 1 1 m \Gamma_m^bC_s^36s \left ( \tfrac{a+b}{2}/b:(c/a)\right ) \cdot m[\circ_1]({*}{\cdot}{*}{:}), ({*}{\cdot}{\times})9 Cc C 1 c 1 B 1 1 b \Gamma_m^bC_s^42h \left ( \tfrac{a+b}{2}/b:(c/a)\right ) \cdot \tilde c(\bar\circ_1)({*}{:}{\times}), ({\times}{\times}_1)10 2/m 2*P2/m P 1 2/m 1 P 1 1 2/m \Gamma_mC_{2h}^17s (b:(c/a))\cdot m:2[2_02_02_02_0](*2{\cdot}22{\cdot}2)11 P21 /m P 1 21 /m 1 P 1 1 21 /m \Gamma_mC_{2h}^22a (b:(c/a))\cdot m:2_1[2_12_12_12_1](22{*}{\cdot})12 C2/m C 1 2/m 1 B 1 1 2/m \Gamma_m^bC_{2h}^38s \left ( \tfrac{a+b}{2}/b:(c/a)\right ) \cdot m:2[2_02_02_12_1](*2{\cdot}22{:}2), (2\bar{*}2{\cdot}2)13 P2/c P 1 2/c 1 P 1 1 2/b \Gamma_mC_{2h}^43h (b:(c/a))\cdot \tilde c:2(2_02_022)(*2{:}22{:}2), (22{*}_0)14 P21 /c P 1 21 /c 1 P 1 1 21 /b \Gamma_mC_{2h}^53a (b:(c/a))\cdot \tilde c:2_1(2_12_122)(22{*}{:}), (22{\times})15 C2/c C 1 2/c 1 B 1 1 2/b \Gamma_m^bC_{2h}^64h \left ( \tfrac{a+b}{2}/b:(c/a)\right ) \cdot \tilde c:2(2_02_122)(2\bar{*}2{:}2), (22{*}_1)
List of orthorhombic
Orthorhombic Bravais lattice Simple (P) Body (I) Face (F) Base (S)
Orthorhombic crystal system Number Point group Orbifold Short name Full name Schoenflies Fedorov Shubnikov Fibrifold (primary)Fibrifold (secondary)16 222 222P222 P 2 2 2 \Gamma_oD_2^19s (c:a:b):2:2(*2_02_02_02_0)17 P2221 P 2 2 21 \Gamma_oD_2^24a (c:a:b):2_1:2(*2_12_12_12_1)(2_02_0{*})18 P21 21 2 P 21 21 2 \Gamma_oD_2^37a (c:a:b):2 2_1(2_02_0\bar{\times})(2_12_1{*})19 P21 21 21 P 21 21 21 \Gamma_oD_2^48a (c:a:b):2_1 2_1(2_12_1\bar{\times})20 C2221 C 2 2 21 \Gamma_o^bD_2^55a \left ( \tfrac{a+b}{2}:c:a:b\right ) :2_1:2(2_1{*}2_12_1)(2_02_1{*})21 C222 C 2 2 2 \Gamma_o^bD_2^610s \left ( \tfrac{a+b}{2}:c:a:b\right ) :2:2(2_0{*}2_02_0)(*2_02_02_12_1)22 F222 F 2 2 2 \Gamma_o^fD_2^712s \left ( \tfrac{a+c}{2}/\tfrac{b+c}{2}/\tfrac{a+b}{2}:c:a:b\right ) :2:2(*2_02_12_02_1)23 I222 I 2 2 2 \Gamma_o^vD_2^811s \left ( \tfrac{a+b+c}{2}/c:a:b\right ) :2:2(2_1{*}2_02_0)24 I21 21 21 I 21 21 21 \Gamma_o^vD_2^96a \left ( \tfrac{a+b+c}{2}/c:a:b \right ) :2:2_1(2_0{*}2_12_1)25 mm2 *22Pmm2 P m m 2 \Gamma_oC_{2v}^113s (c:a:b):m \cdot 2(*{\cdot}2{\cdot}2{\cdot}2{\cdot}2)[{*}_0{\cdot}{*}_0{\cdot}]26 Pmc21 P m c 21 \Gamma_oC_{2v}^29a (c:a:b): \tilde c \cdot 2_1(*{\cdot}2{:}2{\cdot}2{:}2)(\bar{*}{\cdot}\bar{*}{\cdot}), [{\times_0}{\times_0}]27 Pcc2 P c c 2 \Gamma_oC_{2v}^35h (c:a:b): \tilde c \cdot 2(*{:}2{:}2{:}2{:}2)(\bar{*}_0\bar{*}_0)28 Pma2 P m a 2 \Gamma_oC_{2v}^46h (c:a:b): \tilde a \cdot 2(2_02_0{*}{\cdot})[{*}_0{:}{*}_0{:}], (*{\cdot}{*}_0)29 Pca21 P c a 21 \Gamma_oC_{2v}^511a (c:a:b): \tilde a \cdot 2_1(2_12_1{*}{:})(\bar{*}{:}\bar{*}{:})30 Pnc2 P n c 2 \Gamma_oC_{2v}^67h (c:a:b): \tilde c \odot 2(2_02_0{*}{:})(\bar{*}_1\bar{*}_1), ({*}_0{\times}_0)31 Pmn21 P m n 21 \Gamma_oC_{2v}^710a (c:a:b): \widetilde{ac} \cdot 2_1(2_12_1{*}{\cdot})(*{\cdot}\bar{\times}), [{\times}_0{\times}_1]32 Pba2 P b a 2 \Gamma_oC_{2v}^89h (c:a:b): \tilde a \odot 2(2_02_0{\times}_0)(*{:}{*}_0)33 Pna21 P n a 21 \Gamma_oC_{2v}^912a (c:a:b): \tilde a \odot 2_1(2_12_1{\times})(*{:}{\times}), ({\times}{\times}_1)34 Pnn2 P n n 2 \Gamma_oC_{2v}^{10}8h (c:a:b): \widetilde{ac} \odot 2(2_02_0{\times}_1)(*_0{\times}_1)35 Cmm2 C m m 2 \Gamma_o^bC_{2v}^{11}14s \left ( \tfrac{a+b}{2}:c:a:b\right ) :m \cdot 2(2_0{*}{\cdot}2{\cdot}2)[*_0{\cdot}{*}_0{:}]36 Cmc21 C m c 21 \Gamma_o^bC_{2v}^{12}13a \left ( \tfrac{a+b}{2}:c:a:b\right ) :\tilde c \cdot 2_1(2_1{*}{\cdot}2{:}2)(\bar{*}{\cdot}\bar{*}{:}), [{\times}_1{\times}_1]37 Ccc2 C c c 2 \Gamma_o^bC_{2v}^{13}10h \left ( \tfrac{a+b}{2}:c:a:b\right ) : \tilde c \cdot 2(2_0{*}{:}2{:}2)(\bar{*}_0\bar{*}_1)38 Amm2 A m m 2 \Gamma_o^bC_{2v}^{14}15s \left ( \tfrac{b+c}{2}/c:a:b\right ):m \cdot 2(*{\cdot}2{\cdot}2{\cdot}2{:}2)[{*}_1{\cdot}{*}_1{\cdot}], [*{\cdot}{\times}_0]39 Aem2 A b m 2 \Gamma_o^bC_{2v}^{15}11h \left ( \tfrac{b+c}{2}/c:a:b\right ) :m \cdot 2_1(*{\cdot}2{:}2{:}2{:}2)[{*}_1{:}{*}_1{:}], (\bar{*}{\cdot}\bar{*}_0)40 Ama2 A m a 2 \Gamma_o^bC_{2v}^{16}12h \left ( \tfrac{b+c}{2}/c:a:b\right ) : \tilde a \cdot 2(2_02_1{*}{\cdot})(*{\cdot}{*}_1), [*{:}{\times}_1]41 Aea2 A b a 2 \Gamma_o^bC_{2v}^{17}13h \left ( \tfrac{b+c}{2}/c:a:b\right ) : \tilde a \cdot 2_1(2_02_1{*}{:})(*{:}{*}_1), (\bar{*}{:}\bar{*}_1)42 Fmm2 F m m 2 \Gamma_o^fC_{2v}^{18}17s \left ( \tfrac{a+c}{2}/\tfrac{b+c}{2}/\tfrac{a+b}{2}:c:a:b\right ) :m \cdot 2(*{\cdot}2{\cdot}2{:}2{:}2)[{*}_1{\cdot}{*}_1{:}]43 Fdd2 F d d 2 \Gamma_o^fC_{2v}^{19}16h \left ( \tfrac{a+c}{2}/\tfrac{b+c}{2}/\tfrac{a+b}{2}:c:a:b \right ) : \tfrac{1}{2} \widetilde{ac} \odot 2(2_02_1{\times})({*}_1{\times})44 Imm2 I m m 2 \Gamma_o^vC_{2v}^{20}16s \left ( \tfrac{a+b+c}{2}/c:a:b \right ) :m \cdot 2(2_1{*}{\cdot}2{\cdot}2)[*{\cdot}{\times}_1]45 Iba2 I b a 2 \Gamma_o^vC_{2v}^{21}15h \left ( \tfrac{a+b+c}{2}/c:a:b \right ) : \tilde c \cdot 2(2_1{*}{:}2{:}2)(\bar{*}{:}\bar{*}_0)46 Ima2 I m a 2 \Gamma_o^vC_{2v}^{22}14h \left ( \tfrac{a+b+c}{2}/c:a:b \right ) : \tilde a \cdot 2(2_0{*}{\cdot}2{:}2)(\bar{*}{\cdot}\bar{*}_1), [*{:}{\times}_0]47 2/m 2/m 2/m (mmm) *222Pmmm P 2/m 2/m 2/m \Gamma_oD_{2h}^118s \left ( c:a:b \right ) \cdot m:2 \cdot m[*{\cdot}2{\cdot}2{\cdot}2{\cdot}2]48 Pnnn P 2/n 2/n 2/n \Gamma_oD_{2h}^219h \left ( c:a:b \right ) \cdot \widetilde{ab}:2 \odot \widetilde{ac}(2\bar{*}_12_02_0)49 Pccm P 2/c 2/c 2/m \Gamma_oD_{2h}^317h \left ( c:a:b \right ) \cdot m:2 \cdot \tilde c[*{:}2{:}2{:}2{:}2](*2_02_02{\cdot}2)50 Pban P 2/b 2/a 2/n \Gamma_oD_{2h}^418h \left ( c:a:b \right ) \cdot \widetilde{ab}:2 \odot \tilde a(2\bar{*}_02_02_0)(*2_02_02{:}2)51 Pmma P 21 /m 2/m 2/a \Gamma_oD_{2h}^514a \left ( c:a:b \right ) \cdot \tilde a :2 \cdot m[2_02_0{*}{\cdot}][*{\cdot}2{:}2{\cdot}2{:}2], [*2{\cdot}2{\cdot}2{\cdot}2]52 Pnna P 2/n 21 /n 2/a \Gamma_oD_{2h}^617a \left ( c:a:b \right ) \cdot \tilde a:2 \odot \widetilde{ac}(2_02\bar{*}_1)(2_0{*}2{:}2), (2\bar{*}2_12_1)53 Pmna P 2/m 2/n 21 /a \Gamma_oD_{2h}^715a \left ( c:a:b \right ) \cdot \tilde a:2_1 \cdot \widetilde{ac}[2_02_0{*}{:}](*2_12_12{\cdot}2), (2_0{*}2{\cdot}2)54 Pcca P 21 /c 2/c 2/a \Gamma_oD_{2h}^816a \left ( c:a:b \right ) \cdot \tilde a:2 \cdot \tilde c(2_02\bar{*}_0)(*2{:}2{:}2{:}2), (*2_12_12{:}2)55 Pbam P 21 /b 21 /a 2/m \Gamma_oD_{2h}^922a \left ( c:a:b \right ) \cdot m:2 \odot \tilde a[2_02_0{\times}_0](*2{\cdot}2{:}2{\cdot}2)56 Pccn P 21 /c 21 /c 2/n \Gamma_oD_{2h}^{10}27a \left ( c:a:b \right ) \cdot \widetilde{ab}:2 \cdot \tilde c(2\bar{*}{:}2{:}2)(2_12\bar{*}_0)57 Pbcm P 2/b 21 /c 21 /m \Gamma_oD_{2h}^{11}23a \left ( c:a:b \right ) \cdot m:2_1 \odot \tilde c(2_02\bar{*}{\cdot})(*2{:}2{\cdot}2{:}2), [2_12_1{*}{:}]58 Pnnm P 21 /n 21 /n 2/m \Gamma_oD_{2h}^{12}25a \left ( c:a:b \right ) \cdot m:2 \odot \widetilde{ac}[2_02_0{\times}_1](2_1{*}2{\cdot}2)59 Pmmn P 21 /m 21 /m 2/n \Gamma_oD_{2h}^{13}24a \left ( c:a:b \right ) \cdot \widetilde{ab}:2 \cdot m(2\bar{*}{\cdot}2{\cdot}2)[2_12_1{*}{\cdot}]60 Pbcn P 21 /b 2/c 21 /n \Gamma_oD_{2h}^{14}26a \left ( c:a:b \right ) \cdot \widetilde{ab}:2_1 \odot \tilde c(2_02\bar{*}{:})(2_1{*}2{:}2), (2_12\bar{*}_1)61 Pbca P 21 /b 21 /c 21 /a \Gamma_oD_{2h}^{15}29a \left ( c:a:b \right ) \cdot \tilde a:2_1 \odot \tilde c(2_12\bar{*}{:})62 Pnma P 21 /n 21 /m 21 /a \Gamma_oD_{2h}^{16}28a \left ( c:a:b \right ) \cdot \tilde a:2_1 \odot m(2_12\bar{*}{\cdot})(2\bar{*}{\cdot}2{:}2), [2_12_1{\times}]63 Cmcm C 2/m 2/c 21 /m \Gamma_o^bD_{2h}^{17}18a \left ( \tfrac{a+b}{2}:c:a:b\right ) \cdot m:2_1 \cdot \tilde c[2_02_1{*}{\cdot}](*2{\cdot}2{\cdot}2{:}2), [2_1{*}{\cdot}2{:}2]64 Cmce C 2/m 2/c 21 /a \Gamma_o^bD_{2h}^{18}19a \left ( \tfrac{a+b}{2}:c:a:b\right ) \cdot \tilde a :2_1 \cdot \tilde c[2_02_1{*}{:}](*2{\cdot}2{:}2{:}2), (*2_12{\cdot}2{:}2)65 Cmmm C 2/m 2/m 2/m \Gamma_o^bD_{2h}^{19}19s \left ( \tfrac{a+b}{2}:c:a:b\right ) \cdot m:2 \cdot m[2_0{*}{\cdot}2{\cdot}2][*{\cdot}2{\cdot}2{\cdot}2{:}2]66 Cccm C 2/c 2/c 2/m \Gamma_o^bD_{2h}^{20}20h \left ( \tfrac{a+b}{2}:c:a:b\right ) \cdot m:2 \cdot \tilde c[2_0{*}{:}2{:}2](*2_02_12{\cdot}2)67 Cmme C 2/m 2/m 2/e \Gamma_o^bD_{2h}^{21}21h \left ( \tfrac{a+b}{2}:c:a:b\right ) \cdot \tilde a :2 \cdot m(*2_02{\cdot}2{\cdot}2)[*{\cdot}2{:}2{:}2{:}2]68 Ccce C 2/c 2/c 2/e \Gamma_o^bD_{2h}^{22}22h \left ( \tfrac{a+b}{2}:c:a:b\right ) \cdot \tilde a :2 \cdot \tilde c(*2_02{:}2{:}2)(*2_02_12{:}2)69 Fmmm F 2/m 2/m 2/m \Gamma_o^fD_{2h}^{23}21s \left ( \tfrac{a+c}{2}/\tfrac{b+c}{2}/\tfrac{a+b}{2}:c:a:b\right ) \cdot m:2 \cdot m[*{\cdot}2{\cdot}2{:}2{:}2]70 Fddd F 2/d 2/d 2/d \Gamma_o^fD_{2h}^{24}24h \left ( \tfrac{a+c}{2}/\tfrac{b+c}{2}/\tfrac{a+b}{2}:c:a:b\right ) \cdot \tfrac{1}{2}\widetilde{ab}:2 \odot \tfrac{1}{2}\widetilde{ac}(2\bar{*}2_02_1)71 Immm I 2/m 2/m 2/m \Gamma_o^vD_{2h}^{25}20s \left ( \tfrac{a+b+c}{2}/c:a:b\right ) \cdot m:2 \cdot m[2_1{*}{\cdot}2{\cdot}2]72 Ibam I 2/b 2/a 2/m \Gamma_o^vD_{2h}^{26}23h \left ( \tfrac{a+b+c}{2}/c:a:b\right ) \cdot m:2 \cdot \tilde c[2_1{*}{:}2{:}2](*2_02{\cdot}2{:}2)73 Ibca I 2/b 2/c 2/a \Gamma_o^vD_{2h}^{27}21a \left ( \tfrac{a+b+c}{2}/c:a:b\right ) \cdot \tilde a :2 \cdot \tilde c(*2_12{:}2{:}2)74 Imma I 2/m 2/m 2/a \Gamma_o^vD_{2h}^{28}20a \left ( \tfrac{a+b+c}{2}/c:a:b\right ) \cdot \tilde a :2 \cdot m(*2_12{\cdot}2{\cdot}2)[2_0{*}{\cdot}2{:}2]
List of tetragonal
Tetragonal Bravais lattice Simple (P) Body (I)
Tetragonal crystal system Number Point group Orbifold Short name Full name Schoenflies Fedorov Shubnikov Fibrifold 75 4 44P4 P 4 \Gamma_qC_4^122s (c:a:a):4(4_04_02_0)76 P41 P 41 \Gamma_qC_4^230a (c:a:a) :4_1(4_14_12_1)77 P42 P 42 \Gamma_qC_4^333a (c:a:a) :4_2(4_24_22_0)78 P43 P 43 \Gamma_qC_4^431a (c:a:a) :4_3(4_14_12_1)79 I4 I 4 \Gamma_q^vC_4^523s \left ( \tfrac{a+b+c}{2}/c:a:a\right ) :4(4_24_02_1)80 I41 I 41 \Gamma_q^vC_4^632a \left ( \tfrac{a+b+c}{2}/c:a:a\right ) :4_1(4_34_12_0)81 4 2\timesP4 P 4 \Gamma_qS_4^126s (c:a:a):\tilde 4(442_0)82 I4 I 4 \Gamma_q^vS_4^227s \left ( \tfrac{a+b+c}{2}/c:a:a\right ) :\tilde 4(442_1)83 4/m 4*P4/m P 4/m \Gamma_qC_{4h}^128s (c:a:a)\cdot m:4[4_04_02_0]84 P42 /m P 42 /m \Gamma_qC_{4h}^241a (c:a:a)\cdot m:4_2[4_24_22_0]85 P4/n P 4/n \Gamma_qC_{4h}^329h (c:a:a)\cdot \widetilde{ab}:4(44_02)86 P42 /n P 42 /n \Gamma_qC_{4h}^442a (c:a:a)\cdot \widetilde{ab}:4_2(44_22)87 I4/m I 4/m \Gamma_q^vC_{4h}^529s \left ( \tfrac{a+b+c}{2}/c:a:a\right ) \cdot m:4[4_24_02_1]88 I41 /a I 41 /a \Gamma_q^vC_{4h}^640a \left ( \tfrac{a+b+c}{2}/c:a:a\right ) \cdot \tilde a :4_1(44_12)89 422 224P422 P 4 2 2 \Gamma_qD_4^130s (c:a:a):4:2(*4_04_02_0)90 P421 2 P421 2 \Gamma_qD_4^243a (c:a:a):4 2_1(4_0{*}2_0)91 P41 22 P 41 2 2 \Gamma_qD_4^344a (c:a:a):4_1:2(*4_14_12_1)92 P41 21 2 P 41 21 2 \Gamma_qD_4^448a (c:a:a):4_1 2_1(4_1{*}2_1)93 P42 22 P 42 2 2 \Gamma_qD_4^547a (c:a:a):4_2:2(*4_24_22_0)94 P42 21 2 P 42 21 2 \Gamma_qD_4^650a (c:a:a):4_2 2_1(4_2{*}2_0)95 P43 22 P 43 2 2 \Gamma_qD_4^745a (c:a:a):4_3:2(*4_14_12_1)96 P43 21 2 P 43 21 2 \Gamma_qD_4^849a (c:a:a):4_3 2_1(4_1{*}2_1)97 I422 I 4 2 2 \Gamma_q^vD_4^931s \left ( \tfrac{a+b+c}{2}/c:a:a\right ) :4:2(*4_24_02_1)98 I41 22 I 41 2 2 \Gamma_q^vD_4^{10}46a \left ( \tfrac{a+b+c}{2}/c:a:a\right ) :4:2_1(*4_34_12_0)99 4mm *44P4mm P 4 m m \Gamma_qC_{4v}^124s (c:a:a):4\cdot m(*{\cdot}4{\cdot}4{\cdot}2)100 P4bm P 4 b m \Gamma_qC_{4v}^226h (c:a:a):4\odot \tilde a(4_0{*}{\cdot}2)101 P42 cm P 42 c m \Gamma_qC_{4v}^337a (c:a:a):4_2\cdot \tilde c(*{:}4{\cdot}4{:}2)102 P42 nm P 42 n m \Gamma_qC_{4v}^438a (c:a:a):4_2\odot \widetilde{ac}(4_2{*}{\cdot}2)103 P4cc P 4 c c \Gamma_qC_{4v}^525h (c:a:a):4\cdot \tilde c(*{:}4{:}4{:}2)104 P4nc P 4 n c \Gamma_qC_{4v}^627h (c:a:a):4\odot \widetilde{ac}(4_0{*}{:}2)105 P42 mc P 42 m c \Gamma_qC_{4v}^736a (c:a:a):4_2\cdot m(*{\cdot}4{:}4{\cdot}2)106 P42 bc P 42 b c \Gamma_qC_{4v}^839a (c:a:a):4\odot \tilde a(4_2{*}{:}2)107 I4mm I 4 m m \Gamma_q^vC_{4v}^925s \left ( \tfrac{a+b+c}{2}/c:a:a\right ) :4\cdot m(*{\cdot}4{\cdot}4{:}2)108 I4cm I 4 c m \Gamma_q^vC_{4v}^{10}28h \left ( \tfrac{a+b+c}{2}/c:a:a\right ) :4\cdot \tilde c(*{\cdot}4{:}4{:}2)109 I41 md I 41 m d \Gamma_q^vC_{4v}^{11}34a \left ( \tfrac{a+b+c}{2}/c:a:a\right ) :4_1\odot m(4_1{*}{\cdot}2)110 I41 cd I 41 c d \Gamma_q^vC_{4v}^{12}35a \left ( \tfrac{a+b+c}{2}/c:a:a\right ) :4_1\odot \tilde c(4_1{*}{:}2)111 4 2m2{*}2P4 2m P 4 2 m \Gamma_qD_{2d}^132s (c:a:a):\tilde 4 :2(*4{\cdot}42_0)112 P4 2c P 4 2 c \Gamma_qD_{2d}^230h (c:a:a):\tilde 4 2(*4{:}42_0)113 P4 21 m P 4 21 m \Gamma_qD_{2d}^352a (c:a:a):\tilde 4 \cdot \widetilde{ab}(4\bar{*}{\cdot}2)114 P4 21 c P 4 21 c \Gamma_qD_{2d}^453a (c:a:a):\tilde 4 \cdot \widetilde{abc}(4\bar{*}{:}2)115 P4 m2 P 4 m 2 \Gamma_qD_{2d}^533s (c:a:a):\tilde 4 \cdot m(*{\cdot}44{\cdot}2)116 P4 c2 P 4 c 2 \Gamma_qD_{2d}^631h (c:a:a):\tilde 4 \cdot \tilde c(*{:}44{:}2)117 P4 b2 P 4 b 2 \Gamma_qD_{2d}^732h (c:a:a):\tilde 4 \odot \tilde a(4\bar{*}_02_0)118 P4 n2 P 4 n 2 \Gamma_qD_{2d}^833h (c:a:a):\tilde 4 \cdot \widetilde{ac}(4\bar{*}_12_0)119 I4 m2 I 4 m 2 \Gamma_q^vD_{2d}^935s \left ( \tfrac{a+b+c}{2}/c:a:a\right ) :\tilde 4 \cdot m(*4{\cdot}42_1)120 I4 c2 I 4 c 2 \Gamma_q^vD_{2d}^{10}34h \left ( \tfrac{a+b+c}{2}/c:a:a\right ) :\tilde 4 \cdot \tilde c(*4{:}42_1)121 I4 2m I 4 2 m \Gamma_q^vD_{2d}^{11}34s \left ( \tfrac{a+b+c}{2}/c:a:a\right ) :\tilde 4 :2(*{\cdot}44{:}2)122 I4 2d I 4 2 d \Gamma_q^vD_{2d}^{12}51a \left ( \tfrac{a+b+c}{2}/c:a:a\right ) :\tilde 4 \odot \tfrac{1}{2}\widetilde{abc}(4\bar{*}2_1)123 4/m 2/m 2/m (4/mmm) *224P4/mmm P 4/m 2/m 2/m \Gamma_qD_{4h}^136s (c:a:a)\cdot m:4\cdot m[*{\cdot}4{\cdot}4{\cdot}2]124 P4/mcc P 4/m 2/c 2/c \Gamma_qD_{4h}^235h (c:a:a)\cdot m:4\cdot \tilde c[*{:}4{:}4{:}2]125 P4/nbm P 4/n 2/b 2/m \Gamma_qD_{4h}^336h (c:a:a)\cdot \widetilde{ab}:4\odot \tilde a(*4_04{\cdot}2)126 P4/nnc P 4/n 2/n 2/c \Gamma_qD_{4h}^437h (c:a:a)\cdot \widetilde{ab}:4\odot \widetilde{ac}(*4_04{:}2)127 P4/mbm P 4/m 21 /b 2/m \Gamma_qD_{4h}^554a (c:a:a)\cdot m:4\odot \tilde a[4_0{*}{\cdot}2]128 P4/mnc P 4/m 21 /n 2/c \Gamma_qD_{4h}^656a (c:a:a)\cdot m:4\odot \widetilde{ac}[4_0{*}{:}2]129 P4/nmm P 4/n 21 /m 2/m \Gamma_qD_{4h}^755a (c:a:a)\cdot \widetilde{ab}:4\cdot m(*4{\cdot}4{\cdot}2)130 P4/ncc P 4/n 21 /c 2/c \Gamma_qD_{4h}^857a (c:a:a)\cdot \widetilde{ab}:4\cdot \tilde c(*4{:}4{:}2)131 P42 /mmc P 42 /m 2/m 2/c \Gamma_qD_{4h}^960a (c:a:a)\cdot m:4_2\cdot m[*{\cdot}4{:}4{\cdot}2]132 P42 /mcm P 42 /m 2/c 2/m \Gamma_qD_{4h}^{10}61a (c:a:a)\cdot m:4_2\cdot \tilde c[*{:}4{\cdot}4{:}2]133 P42 /nbc P 42 /n 2/b 2/c \Gamma_qD_{4h}^{11}63a (c:a:a)\cdot \widetilde{ab}:4_2\odot \tilde a(*4_24{:}2)134 P42 /nnm P 42 /n 2/n 2/m \Gamma_qD_{4h}^{12}62a (c:a:a)\cdot \widetilde{ab}:4_2\odot \widetilde{ac}(*4_24{\cdot}2)135 P42 /mbc P 42 /m 21 /b 2/c \Gamma_qD_{4h}^{13}66a (c:a:a)\cdot m:4_2\odot \tilde a[4_2{*}{:}2]136 P42 /mnm P 42 /m 21 /n 2/m \Gamma_qD_{4h}^{14}65a (c:a:a)\cdot m:4_2\odot \widetilde{ac}[4_2{*}{\cdot}2]137 P42 /nmc P 42 /n 21 /m 2/c \Gamma_qD_{4h}^{15}67a (c:a:a)\cdot \widetilde{ab}:4_2\cdot m(*4{\cdot}4{:}2)138 P42 /ncm P 42 /n 21 /c 2/m \Gamma_qD_{4h}^{16}65a (c:a:a)\cdot \widetilde{ab}:4_2\cdot \tilde c(*4{:}4{\cdot}2)139 I4/mmm I 4/m 2/m 2/m \Gamma_q^vD_{4h}^{17}37s \left ( \tfrac{a+b+c}{2}/c:a:a\right ) \cdot m:4\cdot m[*{\cdot}4{\cdot}4{:}2]140 I4/mcm I 4/m 2/c 2/m \Gamma_q^vD_{4h}^{18}38h \left ( \tfrac{a+b+c}{2}/c:a:a\right ) \cdot m:4\cdot \tilde c[*{\cdot}4{:}4{:}2]141 I41 /amd I 41 /a 2/m 2/d \Gamma_q^vD_{4h}^{19}59a \left ( \tfrac{a+b+c}{2}/c:a:a\right ) \cdot \tilde a :4_1\odot m(*4_14{\cdot}2)142 I41 /acd I 41 /a 2/c 2/d \Gamma_q^vD_{4h}^{20}58a \left ( \tfrac{a+b+c}{2}/c:a:a\right ) \cdot \tilde a :4_1\odot \tilde c(*4_14{:}2)
List of trigonal
Trigonal Bravais lattice Rhombohedral (R) Hexagonal (P)
Trigonal crystal system Number Point group Orbifold Short name Full name Schoenflies Fedorov Shubnikov Fibrifold 143 3 33P3 P 3 \Gamma_hC_3^138s (c:(a/a)):3(3_03_03_0)144 P31 P 31 \Gamma_hC_3^268a (c:(a/a)):3_1(3_13_13_1)145 P32 P 32 \Gamma_hC_3^369a (c:(a/a)):3_2(3_13_13_1)146 R3 R 3 \Gamma_{rh}C_3^439s (a/a/a)/3(3_03_13_2)147 3 3\timesP3 P 3 \Gamma_hC_{3i}^151s (c:(a/a)):\tilde 6(63_02)148 R3 R 3 \Gamma_{rh}C_{3i}^252s (a/a/a)/\tilde 6(63_12)149 32 223P312 P 3 1 2 \Gamma_hD_3^145s (c:(a/a)):2:3(*3_03_03_0)150 P321 P 3 2 1 \Gamma_hD_3^244s (c:(a/a))\cdot 2:3(3_0{*}3_0)151 P31 12 P 31 1 2 \Gamma_hD_3^372a (c:(a/a)):2:3_1(*3_13_13_1)152 P31 21 P 31 2 1 \Gamma_hD_3^470a (c:(a/a))\cdot 2:3_1(3_1{*}3_1)153 P32 12 P 32 1 2 \Gamma_hD_3^573a (c:(a/a)):2:3_2(*3_13_13_1)154 P32 21 P 32 2 1 \Gamma_hD_3^671a (c:(a/a))\cdot 2:3_2(3_1{*}3_1)155 R32 R 3 2 \Gamma_{rh}D_3^746s (a/a/a)/3:2(*3_03_13_2)156 3m *33P3m1 P 3 m 1 \Gamma_hC_{3v}^140s (c:(a/a)):m\cdot 3(*{\cdot}3{\cdot}3{\cdot}3)157 P31m P 3 1 m \Gamma_hC_{3v}^241s (c:(a/a))\cdot m\cdot 3(3_0{*}{\cdot}3)158 P3c1 P 3 c 1 \Gamma_hC_{3v}^339h (c:(a/a)):\tilde c:3(*{:}3{:}3{:}3)159 P31c P 3 1 c \Gamma_hC_{3v}^440h (c:(a/a))\cdot\tilde c :3(3_0{*}{:}3)160 R3m R 3 m \Gamma_{rh}C_{3v}^542s (a/a/a)/3\cdot m(3_1{*}{\cdot}3)161 R3c R 3 c \Gamma_{rh}C_{3v}^641h (a/a/a)/3\cdot\tilde c(3_1{*}{:}3)162 3 2/m (3 m)2{*}3P3 1m P 3 1 2/m \Gamma_hD_{3d}^156s (c:(a/a))\cdot m\cdot\tilde 6(*{\cdot}63_02)163 P3 1c P 3 1 2/c \Gamma_hD_{3d}^246h (c:(a/a))\cdot\tilde c \cdot\tilde 6(*{:}63_02)164 P3 m1 P 3 2/m 1 \Gamma_hD_{3d}^355s (c:(a/a)):m\cdot\tilde 6(*6{\cdot}3{\cdot}2)165 P3 c1 P 3 2/c 1 \Gamma_hD_{3d}^445h (c:(a/a)):\tilde c \cdot\tilde 6(*6{:}3{:}2)166 R3 m R 3 2/m \Gamma_{rh}D_{3d}^557s (a/a/a)/\tilde 6 \cdot m(*{\cdot}63_12)167 R3 c R 3 2/c \Gamma_{rh}D_{3d}^647h (a/a/a)/\tilde 6 \cdot\tilde c(*{:}63_12)
List of hexagonal
Hexagonal Bravais lattice
Hexagonal crystal system Number Point group Orbifold Short name Full name Schoenflies Fedorov Shubnikov Fibrifold 168 6 66P6 P 6 \Gamma_hC_6^149s (c:(a/a)):6(6_03_02_0)169 P61 P 61 \Gamma_hC_6^274a (c:(a/a)):6_1(6_13_12_1)170 P65 P 65 \Gamma_hC_6^375a (c:(a/a)):6_5(6_13_12_1)171 P62 P 62 \Gamma_hC_6^476a (c:(a/a)):6_2(6_23_22_0)172 P64 P 64 \Gamma_hC_6^577a (c:(a/a)):6_4(6_23_22_0)173 P63 P 63 \Gamma_hC_6^678a (c:(a/a)):6_3(6_33_02_1)174 6 3*P6 P 6 \Gamma_hC_{3h}^143s (c:(a/a)):3:m[3_03_03_0]175 6/m 6*P6/m P 6/m \Gamma_hC_{6h}^153s (c:(a/a))\cdot m :6[6_03_02_0]176 P63 /m P 63 /m \Gamma_hC_{6h}^281a (c:(a/a))\cdot m :6_3[6_33_02_1]177 622 226P622 P 6 2 2 \Gamma_hD_6^154s (c:(a/a))\cdot 2 :6(*6_03_02_0)178 P61 22 P 61 2 2 \Gamma_hD_6^282a (c:(a/a))\cdot 2 :6_1(*6_13_12_1)179 P65 22 P 65 2 2 \Gamma_hD_6^383a (c:(a/a))\cdot 2 :6_5(*6_13_12_1)180 P62 22 P 62 2 2 \Gamma_hD_6^484a (c:(a/a))\cdot 2 :6_2(*6_23_22_0)181 P64 22 P 64 2 2 \Gamma_hD_6^585a (c:(a/a))\cdot 2 :6_4(*6_23_22_0)182 P63 22 P 63 2 2 \Gamma_hD_6^686a (c:(a/a))\cdot 2 :6_3(*6_33_02_1)183 6mm *66P6mm P 6 m m \Gamma_hC_{6v}^150s (c:(a/a)):m\cdot 6(*{\cdot}6{\cdot}3{\cdot}2)184 P6cc P 6 c c \Gamma_hC_{6v}^244h (c:(a/a)):\tilde c \cdot 6(*{:}6{:}3{:}2)185 P63 cm P 63 c m \Gamma_hC_{6v}^380a (c:(a/a)):\tilde c \cdot 6_3(*{\cdot}6{:}3{:}2)186 P63 mc P 63 m c \Gamma_hC_{6v}^479a (c:(a/a)):m\cdot 6_3(*{:}6{\cdot}3{\cdot}2)187 6 m2*223P6 m2 P 6 m 2 \Gamma_hD_{3h}^148s (c:(a/a)):m\cdot 3:m[*{\cdot}3{\cdot}3{\cdot}3]188 P6 c2 P 6 c 2 \Gamma_hD_{3h}^243h (c:(a/a)):\tilde c \cdot 3:m[*{:}3{:}3{:}3]189 P6 2m P 6 2 m \Gamma_hD_{3h}^347s (c:(a/a))\cdot m:3\cdot m[3_0{*}{\cdot}3]190 P6 2c P 6 2 c \Gamma_hD_{3h}^442h (c:(a/a))\cdot m:3\cdot \tilde c[3_0{*}{:}3]191 6/m 2/m 2/m (6/mmm) *226P6/mmm P 6/m 2/m 2/m \Gamma_hD_{6h}^158s (c:(a/a))\cdot m:6\cdot m[*{\cdot}6{\cdot}3{\cdot}2]192 P6/mcc P 6/m 2/c 2/c \Gamma_hD_{6h}^248h (c:(a/a))\cdot m:6\cdot\tilde c[*{:}6{:}3{:}2]193 P63 /mcm P 63 /m 2/c 2/m \Gamma_hD_{6h}^387a (c:(a/a))\cdot m:6_3\cdot\tilde c[*{\cdot}6{:}3{:}2]194 P63 /mmc P 63 /m 2/m 2/c \Gamma_hD_{6h}^488a (c:(a/a))\cdot m:6_3\cdot m[*{:}6{\cdot}3{\cdot}2]
List of cubic
Cubic Bravais lattice Simple (P) Body centered (I) Face centered (F)
Cubic crystal system Number Point group Orbifold Short name Full name Schoenflies Fedorov Shubnikov Conway Fibrifold (preserving z) Fibrifold (preserving x, y, z) 195 23 332P23 P 2 3 \Gamma_cT^159s \left ( a:a:a\right ) :2/32^\circ(*2_02_02_02_0){:}3(*2_02_02_02_0){:}3196 F23 F 2 3 \Gamma_c^fT^261s \left ( \tfrac{a+c}{2}/\tfrac{b+c}{2}/\tfrac{a+b}{2}:a:a:a\right ) :2/31^\circ(*2_02_12_02_1){:}3(*2_02_12_02_1){:}3197 I23 I 2 3 \Gamma_c^vT^360s \left ( \tfrac{a+b+c}{2}/a:a:a\right ) :2/34^{\circ\circ}(2_1{*}2_02_0){:}3(2_1{*}2_02_0){:}3198 P21 3 P 21 3 \Gamma_cT^489a \left ( a:a:a\right ) :2_1/31^\circ/4(2_12_1\bar{\times}){:}3(2_12_1\bar{\times}){:}3199 I21 3 I 21 3 \Gamma_c^vT^590a \left ( \tfrac{a+b+c}{2}/a:a:a\right ) :2_1/32^\circ/4(2_0{*}2_12_1){:}3(2_0{*}2_12_1){:}3200 2/m 3 (m3 ) 3{*}2Pm3 P 2/m 3 \Gamma_cT_h^162s \left ( a:a:a\right ) \cdot m/ \tilde 64^-[*{\cdot}2{\cdot}2{\cdot}2{\cdot}2]{:}3[*{\cdot}2{\cdot}2{\cdot}2{\cdot}2]{:}3201 Pn3 P 2/n 3 \Gamma_cT_h^249h \left ( a:a:a\right ) \cdot \widetilde{ab} / \tilde 64^{\circ+}(2\bar{*}_12_02_0){:}3(2\bar{*}_12_02_0){:}3202 Fm3 F 2/m 3 \Gamma_c^fT_h^364s \left ( \tfrac{a+c}{2}/\tfrac{b+c}{2}/\tfrac{a+b}{2}:a:a:a\right ) \cdot m/ \tilde 62^-[*{\cdot}2{\cdot}2{:}2{:}2]{:}3[*{\cdot}2{\cdot}2{:}2{:}2]{:}3203 Fd3 F 2/d 3 \Gamma_c^fT_h^450h \left ( \tfrac{a+c}{2}/\tfrac{b+c}{2}/\tfrac{a+b}{2}:a:a:a\right ) \cdot \tfrac{1}{2}\widetilde{ab} / \tilde 62^{\circ+}(2\bar{*}2_02_1){:}3(2\bar{*}2_02_1){:}3204 Im3 I 2/m 3 \Gamma_c^vT_h^563s \left ( \tfrac{a+b+c}{2}/a:a:a\right ) \cdot m/\tilde 68^{-\circ}[2_1{*}{\cdot}2{\cdot}2]{:}3[2_1{*}{\cdot}2{\cdot}2]{:}3205 Pa3 P 21 /a 3 \Gamma_cT_h^691a \left ( a:a:a\right ) \cdot \tilde a /\tilde 62^-/4(2_12\bar{*}{:}){:}3(2_12\bar{*}{:}){:}3206 Ia3 I 21 /a 3 \Gamma_c^vT_h^792a \left ( \tfrac{a+b+c}{2}/a:a:a\right ) \cdot \tilde a /\tilde 64^-/4(*2_12{:}2{:}2){:}3(*2_12{:}2{:}2){:}3207 432 432P432 P 4 3 2 \Gamma_cO^168s \left ( a:a:a\right ) :4/34^{\circ-}(*4_04_02_0){:}3(*2_02_02_02_0){:}6208 P42 32 P 42 3 2 \Gamma_cO^298a \left ( a:a:a\right ) :4_2//34^+(*4_24_22_0){:}3(*2_02_02_02_0){:}6209 F432 F 4 3 2 \Gamma_c^fO^370s \left ( \tfrac{a+c}{2}/\tfrac{b+c}{2}/\tfrac{a+b}{2}:a:a:a\right ) :4/32^{\circ-}(*4_24_02_1){:}3(*2_02_12_02_1){:}6210 F41 32 F 41 3 2 \Gamma_c^fO^497a \left ( \tfrac{a+c}{2}/\tfrac{b+c}{2}/\tfrac{a+b}{2}:a:a:a\right ) :4_1//32^+(*4_34_12_0){:}3(*2_02_12_02_1){:}6211 I432 I 4 3 2 \Gamma_c^vO^569s \left ( \tfrac{a+b+c}{2}/a:a:a\right ) :4/38^{+\circ}(4_24_02_1){:}3(2_1{*}2_02_0){:}6212 P43 32 P 43 3 2 \Gamma_cO^694a \left ( a:a:a\right ) :4_3//32^+/4(4_1{*}2_1){:}3(2_12_1\bar{\times}){:}6213 P41 32 P 41 3 2 \Gamma_cO^795a \left ( a:a:a\right ) :4_1//32^+/4(4_1{*}2_1){:}3(2_12_1\bar{\times}){:}6214 I41 32 I 41 3 2 \Gamma_c^vO^896a \left ( \tfrac{a+b+c}{2}/:a:a:a\right ) :4_1//34^+/4(*4_34_12_0){:}3(2_0{*}2_12_1){:}6215 4 3m*332P4 3m P 4 3 m \Gamma_cT_d^165s \left ( a:a:a\right ) :\tilde 4 /32^\circ{:}2(*4{\cdot}42_0){:}3(*2_02_02_02_0){:}6216 F4 3m F 4 3 m \Gamma_c^fT_d^267s \left ( \tfrac{a+c}{2}/\tfrac{b+c}{2}/\tfrac{a+b}{2}:a:a:a\right ) :\tilde 4 /31^\circ{:}2(*4{\cdot}42_1){:}3(*2_02_12_02_1){:}6217 I4 3m I 4 3 m \Gamma_c^vT_d^366s \left ( \tfrac{a+b+c}{2}/a:a:a\right ) :\tilde 4 /34^\circ{:}2(*{\cdot}44{:}2){:}3(2_1{*}2_02_0){:}6218 P4 3n P 4 3 n \Gamma_cT_d^451h \left ( a:a:a\right ) :\tilde 4 //34^\circ(*4{:}42_0){:}3(*2_02_02_02_0){:}6219 F4 3c F 4 3 c \Gamma_c^fT_d^552h \left ( \tfrac{a+c}{2}/\tfrac{b+c}{2}/\tfrac{a+b}{2}:a:a:a\right ) :\tilde 4 //32^{\circ\circ}(*4{:}42_1){:}3(*2_02_12_02_1){:}6220 I4 3d I 4 3 d \Gamma_c^vT_d^693a \left ( \tfrac{a+b+c}{2}/a:a:a\right ) :\tilde 4 //34^\circ/4(4\bar{*}2_1){:}3(2_0{*}2_12_1){:}6221 4/m 3 2/m (m3 m) *432Pm3 m P 4/m 3 2/m \Gamma_cO_h^171s \left ( a:a:a\right ) :4/\tilde 6 \cdot m4^-{:}2[*{\cdot}4{\cdot}4{\cdot}2]{:}3[*{\cdot}2{\cdot}2{\cdot}2{\cdot}2]{:}6222 Pn3 n P 4/n 3 2/n \Gamma_cO_h^253h \left ( a:a:a\right ) :4/\tilde 6 \cdot \widetilde{abc}8^{\circ\circ}(*4_04{:}2){:}3(2\bar{*}_12_02_0){:}6223 Pm3 n P 42 /m 3 2/n \Gamma_cO_h^3102a \left ( a:a:a\right ) :4_2//\tilde 6 \cdot \widetilde{abc}8^\circ[*{\cdot}4{:}4{\cdot}2]{:}3[*{\cdot}2{\cdot}2{\cdot}2{\cdot}2]{:}6224 Pn3 m P 42 /n 3 2/m \Gamma_cO_h^4103a \left ( a:a:a\right ) :4_2//\tilde 6 \cdot m4^+{:}2(*4_24{\cdot}2){:}3(2\bar{*}_12_02_0){:}6225 Fm3 m F 4/m 3 2/m \Gamma_c^fO_h^573s \left ( \tfrac{a+c}{2}/\tfrac{b+c}{2}/\tfrac{a+b}{2}:a:a:a\right ) :4/\tilde 6 \cdot m2^-{:}2[*{\cdot}4{\cdot}4{:}2]{:}3[*{\cdot}2{\cdot}2{:}2{:}2]{:}6226 Fm3 c F 4/m 3 2/c \Gamma_c^fO_h^654h \left ( \tfrac{a+c}{2}/\tfrac{b+c}{2}/\tfrac{a+b}{2}:a:a:a\right ) :4/\tilde 6 \cdot \tilde c4^{--}[*{\cdot}4{:}4{:}2]{:}3[*{\cdot}2{\cdot}2{:}2{:}2]{:}6227 Fd3 m F 41 /d 3 2/m \Gamma_c^fO_h^7100a \left ( \tfrac{a+c}{2}/\tfrac{b+c}{2}/\tfrac{a+b}{2}:a:a:a\right ) :4_1//\tilde 6 \cdot m2^+{:}2(*4_14{\cdot}2){:}3(2\bar{*}2_02_1){:}6228 Fd3 c F 41 /d 3 2/c \Gamma_c^fO_h^8101a \left ( \tfrac{a+c}{2}/\tfrac{b+c}{2}/\tfrac{a+b}{2}:a:a:a\right ) :4_1//\tilde 6 \cdot \tilde c4^{++}(*4_14{:}2){:}3(2\bar{*}2_02_1){:}6229 Im3 m I 4/m 3 2/m \Gamma_c^vO_h^972s \left ( \tfrac{a+b+c}{2}/a:a:a\right ) :4/\tilde 6 \cdot m8^\circ{:}2[*{\cdot}4{\cdot}4{:}2]{:}3[2_1{*}{\cdot}2{\cdot}2]{:}6230 Ia3 d I 41 /a 3 2/d \Gamma_c^vO_h^{10}99a \left ( \tfrac{a+b+c}{2}/a:a:a\right ) :4_1//\tilde 6 \cdot \tfrac{1}{2}\widetilde{abc}8^\circ/4(*4_14{:}2){:}3(*2_12{:}2{:}2){:}6
Notes
^ The symbol e was introduced by the IUCR in 1992. Prior to this, the space groups Aem2 (No. 39), Aea2 (No. 41), Cmce (No. 64), Cmme (No. 67), and Ccce (No. 68) were known as Abm2 (No. 39), Aba2 (No. 41), Cmca (No. 64), Cmma (No. 67), and Ccca (No. 68) respectively. Historical literature may refer to the old names, but their meaning is unchanged.[2]
References
^ Bradley, C. J. & Cracknell, A. P. (2010). The mathematical theory of symmetry in solids: representation theory for point groups and space groups . Oxford New York: Clarendon Press. pp. 127–134. ISBN 978-0-19-958258-7. OCLC 859155300
^ de Wolff, P. M.; Billiet, Y.; Donnay, J. D. H.; Fischer, W.; Galiulin, R. B.; Glazer, A. M.; Hahn, T.; Senechal, M.; Shoemaker, D. P.; Wondratschek, H.; Wilson, A. J. C.; Abrahams, S. C. (1992-09-01). "Symbols for symmetry elements and symmetry operations. Final report of the IUCr Ad-Hoc Committee on the Nomenclature of Symmetry". Acta Crystallographica Section A . 48 (5): 727–732. Bibcode:1992AcCrA..48..727D . doi:10.1107/s0108767392003428 . ISSN 0108-7673
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