ライフサイエンスコーパス: unit cell

1 nit cell (1140 atoms per face-centered cubic unit cell).

2 unit cells) and thickness of 100 mum ( 300 unit cells).

3 sheets with a thickness of 5 nanometres (2.5 unit cells).

4 ate the deformation dynamics of the graphene unit cell.

5 ials on length scales that approach a single unit cell.

6 osition (H2O)2H2 and three formula units per unit cell.

7 which features one CuO2 plane per primitive unit cell.

8 actions of the flux quantum per superlattice unit cell.

9 rlattices that extend beyond an original MOF unit cell.

10 molecules in the asymmetric crystallographic unit cell.

11 macroscopic variables, for example, average unit cell.

12 coupling of the three resonators within the unit cell.

13 e, symmetry and composition of the nanoscale unit cell.

14 ne of the collective modes of the tripartite unit cell.

15 with symmetry breaking within the perovskite unit cell.

16 degrees +/- 0.8 degrees relative to the bulk unit cell.

17 gical sensors scaled down to a single atomic unit cell.

18 y and contain six monomers in the asymmetric unit cell.

19 idual C, S, or Au chiral centers per surface unit cell.

20 ace with a built-in potential of ~0.3 eV per unit cell.

21 order of one electron per pseudocubic planar unit cell.

22 b axis of the room-temperature orthorhombic unit cell.

23 ds enhances the toroidal magnetic moment per unit cell.

24 of Au30S(S-t-Bu)18 are found in the crystal unit cell.

25 ak-bonding positions along the a axis in the unit cell.

26 of the flux quantum pierces the superlattice unit cell.

27 for the arrangement of the lipids within the unit cell.

28 de crystal with 36 independent copies of the unit cell.

29 ments that are inaccessible from the average unit cell.

30 ed by a (6 radical5 x 6 radical5)R15 degrees unit cell.

31 hole array on the basis of trajectories in a unit cell.

32 r as well as the basis atom locations in the unit cell.

33 nd approximately eight solvent molecules per unit cell.

34 nanoscale lattices through the design of the unit cell.

35 kness can reach the theoretical limit of 3.5 unit cells.

36 or and liquid phases extending over many MOF unit cells.

37 nd magnetic nonlinearities in the individual unit cells.

38 confined to a critical film thickness of two unit cells.

39 y is made difficult by the complexity of the unit cells.

40 unit cells, while x >/= 0.9 gives monoclinic unit cells.

41 in why the total cell size is the sum of all unit cells.

42 spherical configurations leading to lighter unit cells.

43 n the average response of deep-subwavelength unit cells.

44 structures has so far been limited to small unit cells.

45 e of ~6858 A(3) and ~285 atoms per primitive unit cell (1140 atoms per face-centered cubic unit cell)

46 als that the exfoliated MFI nanosheet is 1.5 unit cells (3.0 nm) thick and wrinkled anisotropically w

47 d layered structure in space group Pbca with unit cell a = 18.901(4) A, b = 11.782(2) A, and c = 23.6

48 ts (AUs) and generate exact modes of a whole unit cell according to space group symmetry, while the t

49 entially layering La(1-x)Sr(x)MnO(3) and SrO unit cells aided by in situ reflection high energy elect

50 ructure calculations of the full 16-atom per unit cell alpha-phase structure within the framework of

51 beta-sheet antimicrobial peptides within the unit cell: an antiparallel trimer, which we suggest migh

52 structural correlations within an individual unit cell and between two adjacent unit cells, is best d

53 The unit cell and space group symmetry were found from the X

54 compounds, with crystal structures where the unit cell and the atom positions within it differ from k

55 ws a stiffness variability of the individual unit cells and can control the amplitude of transmitted

56 s (crystallites with thickness less than two unit cells) and thicker zeolite nanosheets for applicati

57 w to lateral dimensions of 1 cm ( 30,000 of unit cells) and thickness of 100 mum ( 300 unit cells)

58 Here, we visualize the Q = 0 (intra-unit-cell) and Q not equal 0 (density-wave) broken-symme

59 ily have the same symmetry, but an expanding unit cell, and are related by hitherto unrecognized stru

60 omic materials in terms of their crystalline unit cells, and propose means to obtain the local geomet

61 c planes, reveal the resonance oscillations, unit cell angular amplitudes, and the polarization direc

62 Here we show that CeNbO4.25 forms with a unit cell approximately 12 times larger than the stoichi

63 the electronegativity differences within the unit cell are less than in the layered compounds.

64 we show that the two actin molecules in the unit cell are related to each other by a local twofold n

65 .5 A and a total coverage of >9 Pu atoms per unit cell area of muscovite (0.77 mug Pu/cm(2)) (determi

66 resonators of different sizes within a super-unit-cell arranged in mirror symmetry.

67 f W(4+) inducing an expansion of the anatase unit cell as determined by XRD.

68 the limited number of asymmetric units in a unit cell as well as limited common symmetry groups for

69 dgroups at the border and also inside of the unit cell at a well-defined position (+/-21 A from the u

70 charge density decays laterally within a few unit cells away from the nanowire; thus providing a mech

71 up was found to lie slightly inward from the unit cell boundary and the tail of the molecule located

72 he fatty acid headgroups were located at the unit cell boundary with their acyl chains straddling the

73 A 'unit cell breathing' mechanism is proposed based on crys

74 grown on a LaSrAlO4 substrate with a single unit cell buffer layer, when ultra-high electric fields

75 d not by compensation of dipole moments in a unit cell but by molecular polarizabilities.

76 h exciton wavefunction extends over multiple unit cells, but with extraordinarily large binding energ

77 M maps can be placed in the crystallographic unit cell by molecular replacement, and how initial phas

78 Here, using unit cell by unit cell superlattice growth technique, we

79 on of over 60 angstroms and 148 atoms in the unit cell, by using a combination of this method and exp

80 tion to measure TiO6 octahedral tilt angles, unit-cell-by-unit-cell, in perovskite-based Li(0.5-3x)Nd

81 ow that the type of the modulation along the unit cell can significantly affect the position of the t

82 Crystallographic unit cells can be assembled into a regular right hexagon

83 ed metamaterials with designed inhomogeneous unit cells can turn a normally incident plane wave into

84 at a well-defined position (+/-21 A from the unit cell center), indicative of a three-layer lipid arr

85 al interdigitation of the acyl chains in the unit cell center.

86 undary with their acyl chains straddling the unit cell center.

87 the molecule located 6.2 +/- 0.2 A from the unit cell center.

88 temperatures (structure solved at 30 K) the unit cell changes to body-centered with Imma symmetry.

89 the YPtAs-type structure, and have a doubled unit cell compared to other LnAuZ phases as a result of

90 thermal conductivity is inversely linked to unit cell complexity, we set out to synthesize a highly

91 non-reciprocal active acoustic metamaterial unit cell composed of a single piezoelectric membrane au

92 res and lattice materials based on repeating unit cells composed of webs or trusses, when made from m

93 aterial, which is constructed by an array of unit cell consisting of a cut-wire and a pair of varacto

94 at optical frequency in metamaterials whose unit cell consists of three identical Ag nanodisks and a

95 ows us to control the lattice symmetries and unit cell constants, as well as the compositions and hab

96 This result shows that the single bulk unit cell contained within Cd84Se56X56L56 is sufficient

97 e12 } macrocycle forms a giant ca. 220 nm(3) unit cell containing 16 macrocycles clustered into eight

98 metamaterials composed of periodic arrays of unit cells containing inductive-capacitive resonators an

99 r the existence of intermetallics with giant unit cells containing thousands of atoms.

100 The designed monolayer unit cell contains six molecules and spans 23 nm x 1 nm.

101 s reported in the original structure, the P1 unit cell contains two nearly identical copies of actin

102 This arrangement of lipids in the LPP unit cell corresponds with the location of their lipid h

103 rsal phonon mean free path spectrum in small unit cell crystalline semiconductors at high temperature

104 The finding of a photoinduced elastic unit cell deformation elucidates a microscopic picture o

105 ent with a latent but very rapid anisotropic unit cell deformation in a two-stage process that ultima

106 on increases, resulting in a decrease in the unit-cell density and concomitant disordering of the cha

107 )Ca(3.48)Fe(7.44)Cu(0.56)O21, with a largest unit cell dimension of over 60 angstroms and 148 atoms i

108 h a nominal thickness of 17 A, the same as a unit-cell dimension for calcite (c-axis = 17.062 A), int

109 noclinic system with space group P2(1)/c and unit cell dimensions a = 12.2575(5) A, b = 7.7596(2) A,

110 tion was employed to systematically vary the unit cell dimensions and tune the proton conducting path

111 1) to P2(1), with 1-A decreases in all three unit cell dimensions.

112 gurable metasurfaces, i.e. metasurfaces with unit-cell dimensions much smaller than the terahertz wav

113 nteraction along the longer crystallographic unit cell direction of mica.

114 ty (i.e., ability to donate), and cord-blood-unit cell dose.

115 phases prepared with the new cations show a unit cell doubling along z, and the refined structures a

116 e 2M polymorph to the 4M polymorph (expanded unit cell due to cation ordering) in zirconolite was obs

117 nsity functional theory, that if a crystal's unit cell elastically deforms in an inhomogeneous manner

118 valent), resulting in a 173.3-angstrom cubic unit cell enclosing 816 uranium nodes and 816 organic li

119 Analysis of unit cell evolutions and ab initio band structure calcul

120 All of the unit cells exhibit highly uniform PCEs of 16.1 +/- 0.9%

121 The unit cell exhibited variation in C(delta)-H/C(gamma)-O a

122 elatively larger MBBs in P11-Cu permit a 20% unit cell expansion and afford a higher surface area and

123 The observation of replica bands in single-unit-cell FeSe on SrTiO3 (STO)(001) by angle-resolved ph

124 l an unexpected characteristic of the single-unit-cell FeSe/SrTiO3 system: shake-off bands suggesting

125 conducting gap opening temperature in single-unit-cell FeSe/SrTiO3.

126 n of a similar superconducting gap in single-unit-cell FeSe/STO(110) raised the question of whether a

127 We report the surface unit cell for CoOEP on HOPG in phenyloctane at 25 degree

128 um nodes and 816 organic linkers-the largest unit cell found to date for any nonbiological material.

129 ured, setting an intrinsic limit of 3 and 10 unit cells from the surface, respectively, for (Ga,Mn)As

130 ixed minimum feature size, differing only in unit cell geometry, were fabricated.

131 ultrathin PbTiO3 films scaled down to three unit cells grown on NdGaO3 (110) substrates with La0.7 S

132 al La2O2CO3 structures, La in the monoclinic unit cell has a much lower number of neighboring oxygen

133 ctions, such as the ubiquitously existed one-unit-cell-high terrace edges, can dramatically affect th

134 micrometers and with thickness of just a few unit cells (i.e., below 5 nm), hence in the strong quant

135 comprised, almost entirely, of the intended unit cell, (ii) exhibiting patterned domains spanning 10

136 cium phosphate control, a contraction of the unit cell in the a-direction but not the c-direction in

137 llography represent a global average of many unit cells in a crystal.

138 posites that are patterned into self-similar unit cells in a fractal-like geometry.

139 he context of two nucleosomes in neighboring unit cells in the crystal structure.

140 a 12-atom and 18-atom rhombohedral primitive unit cells in the symmetry, which are characterized as t

141 ain data from protein crystals with only 100 unit cells in volume using currently available XFELs and

142 se is characterized by a gigantic tetragonal unit cell, in which 30 sub-2-nm quasispherical micelles

143 re TiO6 octahedral tilt angles, unit-cell-by-unit-cell, in perovskite-based Li(0.5-3x)Nd(0.5+x)TiO3,

144 itioning at tetrahedral sites in the crystal unit cell, indicating the distribution of Si(-O-Si)4-n (

145 We observe an ultrathin (2-3 unit cells) interlayer best described as highly strained

146 BFO from the LSMO/BFO interface extends 3-4 unit cells into BFO.

147 The out-of-plane elongation of the unit cell is accompanied by the in-plane shrinkage with

148 This anisotropic elastic deformation of the unit cell is driven by localized electric field as a res

149 The perovskite unit cell is the fundamental building block of many func

150 We find that the unit cell is unaffected in-plane by vanadium doping chan

151 A minor population of unit cells is characterized by reduced water content, 31

152 ry, while the translational symmetry between unit cells is maintained via the periodic boundary condi

153 sponding to a few tens of molecules within a unit cell) is achieved with high signal-to-noise ratio i

154 on per origin, namely the initiation mass or unit cell, is remarkably invariant under perturbations t

155 ndividual unit cell and between two adjacent unit cells, is best described by a tetragonal P4mm space

156 ctivity onset at the critical thickness of 4-unit cell LaAlO3 on SrTiO3 substrate is accompanied with

157 y carriers in the bulk SrTiO3, and the three-unit-cell LaAlO3 capping layer passivates the surface an

158 caused by rotational intergrowths of single-unit-cell lamellae.

159 le in the reported nanolattice is the 500 nm unit-cell lattice constant, allowing the film to behave

160 odifies structure and composition beyond the unit cell length scale on the B sublattice alone.

161 been possible to monitor dissolution at the unit cell level and to extract activation energies for s

162 Growth monitoring at the single-unit-cell level reveals novel nanoscale crystal-growth p

163 he LSMO/BFO interface is studied on a single unit-cell level through a combination of direct order pa

164 have structures that have linkers mixed at a unit-cell-level as opposed to separated or highly cluste

165 r not been possible to obtain information on unit-cell-level linker distribution, an understanding of

166 This unit-cell-level surface engineering approach is promisin

167 erconducting transition temperature (Tc) and unit cell metrics of tetragonal (NH3)yCs0.4FeSe were inv

168 The mass-in-mass unit cell model is transformed into a cantilever-in-mass

169 ere derived and applied in a two-dimensional unit-cell model.

170 that can be naturally explained as an intra-unit-cell nematic charge order with d-wave symmetry, poi

171 structure of Si24, which has 24 Si atoms per unit cell (oC24), contains open channels along the cryst

172 s to introduce more than one period into the unit cell of a periodic structure.

173 The unit cell of Au28(TBBT)20 single crystals contains a pai

174 ion of the different constituents within the unit cell of monoclinic La2O2CO3 and use this informatio

175 The state of each unit cell of the coding metasurface can be switched betw

176 coding metasurface, where the state of each unit cell of the coding metasurface can be switched elec

177 ty graphene superlattices where the complete unit cell of the Hofstadter spectrum is accessible.

178 e domains in a heterostructure or within the unit cell of the host lattice.

179 The complex unit cell of the metasurface solar absorber consists of

180 deformation pattern extends beyond a single unit cell of the original structure.

181 gement around the transition metal atom in a unit cell of the photoferroelectric archetype BiFeO3 fil

182 e molecular arrangement of the lipids in the unit cell of these lamellar phases is very desirable.

183 he Miura-ori tessellation, we find that each unit cell of this crease pattern is mechanically bistabl

184 form stable spatially periodic patterns, the unit cells of a two-dimensional wave-based material.

185 We used a simulation cell comprised of two unit cells of cellulose Ibeta periodically repeated in t

186 n be artificially created by inserting a few unit cells of delta doping EuTiO3 at the interface betwe

187 d spin configurations on a linear chain, the unit cells of square and triangular lattices, a disorder

188 -temperature homoepitaxial growth of several unit cells of SrTiO3 introduces oxygen vacancies and hig

189 The neighboring unit cells of the central metasurface layer of the linea

190 ved when a resonance condition occurs in the unit-cell of the blazed grating.

191 mmetry-independent molecules within the same unit cell or as polymorphs.

192 For a thickness of six unit cells or more, the LaMnO3 film abruptly becomes fer

193 e monotonically decreases with pressure, the unit cell parameter ratio of Os exhibits anomalies at ap

194 The nonlinear increase of the unit cell parameter with ReO4-/NO3- ratios suggests form

195 iffraction revealed a triclinic crystal with unit cell parameters (at 6.5 GPa and 20 degrees C) of a

196 onnectivities and separation distances, with unit cell parameters (though not space group symmetry) p

197 e in the monoclinic P2(1)/n space group with unit cell parameters a = 6.0936(1) A, b = 20.5265(4) A,

198 ture in the tetragonal I42m space group with unit cell parameters a=6.9016(5) A and c=8.7153(9) A.

199 arises from anisotropic changes in the three unit cell parameters across the phase transition, notabl

200 b7 crystallizes in a new structure type with unit cell parameters of a = 15.029(1) A, b = 7.7310(5) A

201 Unit cell parameters of the obtained crystals were deter

202 ty of the single crystal is retained and the unit cell parameters revert to their original values aft

203 ons at each temperature to be calculated and unit cell parameters to be accurately quantified as a fu

204 he structural similarities extend beyond the unit cell parameters to positions of free acid groups an

205 raction data confirms a linear dependence of unit cell parameters upon K content as well as the tetra

206 ization calculations, yield the space group, unit cell parameters, and atomic positions of MPS.

207 frustration can be controlled by tuning the unit cell parameters.

208 llizes into a monoclinic C2/c structure with unit-cell parameters a = 9.859(2) A, b = 8.7507(18) A, c

209 by monitoring Vegard's law evolution of the unit-cell parameters with changing rhodium content, to a

210 The small size of the crystals-50 unit cells per edge, on average-has impeded structural c

211 atically varying the interface density, with unit-cell precision, using two different epitaxial-growt

212 rus OBs consists, on average, of about 9,000 unit cells, representing the smallest protein crystals t

213 the high-symmetry directions of the surface unit cell resulting in a perpendicular spin component, k

214 The unit cell's internal structure and packing are driven by

215 hen the ferroelectric films are downsized to unit cell scale.

216 to know the distribution of vacancies on the unit-cell scale.

217 The combination of change in unit cell shape, long range of elastic distortion and fl

218 rvations made on arrays of 4 x 4 x 6 lattice unit cells show excellent agreement with elastic wave ve

219 s, containing four independent donors in the unit cell, show semiconducting behavior supported by ban

220 e we report integration of thin (down to one unit cell) single crystalline, complex oxide films onto

221 mer intermediates, subject to constraints of unit cell size and energy.

222 rates is inherently small due to their large unit cell size and open-framework structure, the current

223 phase type from Im3m to Pn3m and reduced the unit cell size from approximately 38 nm for the Im3m pha

224 The conventional strategy to increase unit cell size is tweaking membrane composition to inclu

225 amples with (a/w) > 0.3, and notch length-to-unit cell size ratios of (a/l) > 5.2, failed at a lower

226 ear the interface with a depth resolution of unit cell size.

227 e active and stable phase consists of single unit cell sized hollandite-like structural domains that

228 Single-unit-cell Sn-MFI, with the detectable Sn uniformly distr

229 e of the higher sample compliance when fewer unit cells span the intact region.

230 The unit cell structure changed from parallel bilayers to a

231 s of a pentacene dimer that approximates the unit cell structure of crystalline pentacene.

232 rees C and exhibits the typical orthorhombic unit cell structure with two characteristic wide-angle X

233 That the order may be within one unit cell, such as nematic, was only recently considered

234 Here, using unit cell by unit cell superlattice growth technique, we determine th

235 nergy gap of approximately 0.25 eV and intra-unit cell symmetry breaking of charge distribution in in

236 e pseudogap (PG) state and its related intra-unit-cell symmetry breaking remain the focus in the rese

237 so far been achieved at the cost of reduced unit-cell symmetry, yielding a refractive index that is

238 meta-atoms with no spatial variation of the unit cell that derives appreciable optical chirality sol

239 ic crystals are metamaterials with repeating unit cells that result in internal resonances leading to

240 Despite the rectangular unit cell, the band structure is topologically equivalen

241 thick forms Kittel-like domains, while at 6 unit cells there is a complex flux-closure curling behav

242 Reducing the thickness to 3 unit cells, there is an almost complete loss of switchab

243 ermal metamaterials that use the assembly of unit-cell thermal shifters for a remarkable enhancement

244 formation thermodynamics are disassembled as unit-cells thermal shifters in tiny areas, representing

245 Films of iron selenide (FeSe) one unit cell thick grown on strontium titanate (SrTiO3 or S

246 We studied structural changes in a 5 unit cell thick La1.96Sr0.04CuO4 film, epitaxially grown

247 foliated zeolites are single- or near single-unit cell thick silicates that can function as molecular

248 al films of La(2- x)Sr(x)CuO(4) that are one unit cell thick, and fabrication of double-layer transis

249 p- and n-type semiconductors--each just one unit cell thick--are predicted to exhibit completely dif

250 interface between epitaxial LaFeO3 layers >3 unit cells thick and the surface of SrTiO3 single crysta

251 , the polarization in active PbTiO3 layers 9 unit cells thick forms Kittel-like domains, while at 6 u

252 a chemical phase La2Ni2O5 (Ni(2+)) for a few unit-cell thick films.

253 stack of five ionic layers, forming a single-unit-cell-thick crystalline PbFBr precursor film, which

254 the solution-phase growth of single- and few-unit-cell-thick single-crystalline 2D hybrid perovskites

255 s approaches its fundamental limit (i.e. one unit-cell-thick), the electronic state of the SLs change

256 ated layers of La(2)CuO(4) that are only one-unit-cell-thick.

257 e area two-dimensional semiconducting GaS of unit cell thickness ( approximately 1.5 nm).

258 iation into two-dimensional layers of single unit cell thickness.

259 tructure and basal cleavage down to a single unit cell thickness.

260 search for optimal placements in the crystal unit-cells through replica-exchange Monte Carlo simulati

261 simulations of the villin headpiece crystal unit cell to examine its stability at different concentr

262 er several length scales from the individual unit cell to the macroscopic device, and with dynamics s

263 ostructures reveal about 0.1 electron per 2D unit cell transferred between the interfacial Mn and Ni

264 omic-thick tin telluride (SnTe), down to a 1-unit cell (UC) limit.

265 MnO3 (LSMO) samples with varying underlying unit cells (uc) of BaTiO3 (BTO) layer on (001) and (110)

266 emical and physical modification of graphene unit cell unfurls the opportunity to design carbon-based

267 tural complexity varies from a few atoms per unit cell up to thousands of atoms.

268 part from a small (few %) contraction of the unit cells upon incorporation of the guest cations.

269 The diffusion problem is solved in a unit cell using a coordinate system conforming to the he

270 hoice and film thickness on the (Bi, Sb)2Te3 unit cell using high-resolution X-ray diffractometry.

271 he total active area of 6 cm(2) (1 cm(2) x 6 unit cells) via a single-turn solution process is succes

272 a very low symmetry (triclinic) and a large unit cell volume (1874.6 A(3)), containing 16 silicon an

273 nother related cubic structure of comparable unit cell volume (space group Pa3, a = 22.4310(15) A, V

274 ition is first-order and is accompanied by a unit cell volume change of about 10%.

275 Although the unit cell volume decreases over 27%, the quality of the

276 Sn(112), a complex material with a primitive unit cell volume of ~6858 A(3) and ~285 atoms per primit

277 ity by a factor of 100, despite a contracted unit cell volume reflecting a positive chemical pressure

278 , in the lattice parameter axial ratios, the unit cell volume, as well as in specific interatomic bon

279 created resulting in larger band gap, larger unit cell volume, lower trap-state density, and much lon

280 ttice parameter ratio with minimal change in unit cell volume, reveals the existence of a three-stage

281 ng through 140 K, with a 23 % contraction in unit cell volume.

282 nnel space of up to approximately 24% of the unit-cell volume as highly positive-charged organic temp

283 e transition under compression with ca. 22 % unit-cell volume changes, which was found to be coupled

284 ure of zeolite ZSM-25, which has the largest unit-cell volume of all known zeolites (91,554 cubic ang

285 These two zeolites have much larger unit cell volumes (422,655 A(3) and 614,912 A(3), respec

286 The observation that crystals with reduced unit-cell volumes and tighter macromolecular packing oft

287 By this means, the locations within the unit cell were determined for the cholesterol and fatty

288 % decrease in c parameters of the tetragonal unit cells, which results in disintegration of ceramic b

289 ImNN)((1-x)) with x < 0.8 gives orthorhombic unit cells, while x >/= 0.9 gives monoclinic unit cells.

290 In the nanostructured unit cells whose chirality matches that of light, superc

291 1 symmetry and resides in a pseudotetragonal unit cell with a distance of >5.5 A between Pt sites in

292 uch GO battery depends on its length and one unit cell with length of 0.5 cm can generate energy capa

293 t different X sites in each Re-X6 octahedral unit cell with perfect matching between their atomic rad

294 structure which crystallized in a hexagonal unit cell with space group P63/m.

295 ominantly located in the central part of the unit cell with substantial interdigitation of the acyl c

296 hains is also located near the border of the unit cell with their acyl chains directing toward the ce

297 rom a network of nearly isotropic microscale unit cells with high structural connectivity and nanosca

298 wo-dimensional array of resonant metasurface unit-cells with electronically-controlled phase-change m

299 e CAs were found to pack into 2D crystalline unit cells within ribbon-shaped nanostructures, whereas

300 ymmetric units and a loss of symmetry of the unit cell without significantly affecting protein dynami