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Overproduction of magnetosomes by genomic amplification of biosynthetic gene clusters in a 1
magnetotactic bacterium 2
3
4
Anna Lohße,a Isabel Kolinko,a Oliver Raschdorf,a,b René Uebe,a* Sarah Borg,a Andreas 5
Brachmann,a Jürgen M. Plitzko,b Rolf Müller,c Youming Zhang,d Dirk Schülera*# 6
7
8
Ludwig-Maximilians-Universität München, Department of Biology I, Martinsried, Germanya; 9
Max Planck Institute of Biochemistry, Department of Molecular Structural Biology, 10
Martinsried, Germanyb; Saarland University - Helmholtz Institute for Pharmaceutical 11
Research Saarland, Helmholtz Centre for Infection Research and Department of 12
Pharmaceutical Biotechnology, Saarbrücken, Germanyc; Shandong University - Helmholtz 13
Joint Institute of Biotechnology, State Key Laboratory of Microbial Technology, Life Science 14
College, Shandong University, Qingdao, Chinad 15
16
Running Head: Magnetosome overproduction in magnetotactic bacteria 17
18
Address correspondence to D. Schüler, [email protected]. 19
*Present address: Universität Bayreuth, Department of Microbiology, Bayreuth, Germany. 20
A.L. and I.K. contributed equally to this work. 21
22
23
Word count abstract: 250 24
Word count text: 5, 046 25
26
AEM Accepted Manuscript Posted Online 11 March 2016Appl. Environ. Microbiol. doi:10.1128/AEM.03860-15Copyright © 2016, American Society for Microbiology. All Rights Reserved.
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Abstract 27
Magnetotactic bacteria biosynthesize specific organelles, the magnetosomes, which are 28
membrane-enclosed crystals of a magnetic iron mineral that are aligned in a linear chain. The 29
number and size of magnetosome particles have to be critically controlled to build a sensor 30
sufficiently strong to ensure efficient alignment of cells within the weak earth’s magnetic 31
field, while at the same time minimizing the metabolic costs imposed by excessive 32
magnetosome biosynthesis. 33
Apart from their biological function, bacterial magnetosomes have gained considerable 34
interest, since they provide a highly useful model for prokaryotic organelle formation and 35
represent biogenic magnetic nanoparticles with exceptional properties. However, potential 36
applications have been hampered by difficult cultivation of the fastidious bacteria and their 37
poor yields of magnetosomes. 38
In this study we found that size and number of magnetosomes within the cell are controlled by 39
many different Mam and Mms proteins. We present a strategy for overexpression of 40
magnetosome biosynthesis in the alphaprotebacterium Magnetospirillum gryphiswaldense by 41
chromosomal multiplication of individual and multiple magnetosome gene clusters via 42
transposition. While stepwise amplification of the mms6 operon resulted in the formation of 43
increasingly larger crystals (increase of about 35%), the duplication of all major magnetosome 44
operons (mamGFDC, mamAB, mms6 and mamXY, comprising 29 genes in total) yielded an 45
overproducing strain, in which magnetosome numbers were 2.2-fold increased. We 46
demonstrate that tuned expression of the mam and mms clusters provides a powerful strategy 47
for the control of magnetosome size and numbers, thereby setting the stage for high-yield 48
production of tailored magnetic nanoparticles by synthetic biology approaches. 49
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Importance 53
Before our study, it had remained unknown how the upper size and numbers of 54
magnetosomes are genetically regulated, and overproduction of magnetosome 55
biosynthesis has not been achieved, owing to the difficulties of large-scale 56
genome engineering in the recalcitrant magnetotactic bacteria. In this manuscript, 57
we established and systematically explored a strategy for overexpression of 58
magnetosome biosynthesis by genomic amplification of single and multiple 59
magnetosome gene clusters via sequential chromosomal insertion by 60
transposition. Our findings also indicate that the expression level of magnetosome 61
proteins together limits the upper size and number of magnetosomes within the 62
cell. We demonstrate that tuned overexpression of magnetosome genes clusters 63
provides a powerful strategy for the precise control of the magnetosome size and 64
numbers. 65
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Introduction 79
Magnetotactic bacteria (MTB) biosynthesize specific organelles, the magnetosomes, which 80
are membrane-enclosed crystals of a magnetic iron mineral. To most efficiently function as 81
magnetic sensors for navigation within the weak earth’s magnetic field, the size, shape, 82
number and intracellular arrangement of magnetosome particles are evolutionary optimized, 83
while at the same time minimizing the metabolic burden imposed by excessive magnetosome 84
biosynthesis (1). In accordance with these constraints, the alphaproteobacterium 85
Magnetospirillum gryphiswaldense MSR-1 (in the following referred to as MSR) and related 86
magnetospirilla under environmental conditions typically form around twenty cuboctahedral 87
crystals of magnetite (Fe3O4) with a mean diameter of about 42 nm (2, 3). Magnetosome 88
biosynthesis proceeds in several steps, which include the formation of magnetosome 89
membrane (MM) vesicles by invagination from the cytoplasmic membrane, the sorting of 90
MM-specific proteins, the magnetosomal iron uptake and redox-controlled magnetite 91
crystallization, which is followed by assembly of nascent crystals into a single regular chain 92
along an actin-like magnetosome cytoskeleton (4-8). 93
The high degree of biological control over their synthesis results in unprecedented properties 94
of the nano-scaled magnetite crystals, such as high crystallinity, strong magnetization, and 95
uniform composition, shape and size that cannot be replicated by abiogenic fabrication (8). 96
The structural perfection and exceptional magnetic properties as well as their biocompatibility 97
make magnetosomes highly attractive for many bio-nanotechnological applications (9), such 98
as magnetic drug targeting, immunoassays, magnetic resonance imaging, and hyperthermia 99
(10-14). However, all applications of magnetosome particles so far have been hampered by 100
their poor availability due to the fastidious growth requirements of MTB and the low 101
magnetosome content of biomass. Therefore, an attractive possibility to increase 102
magnetosome bioproduction would be genetic engineering or overexpression of the entire 103
biosynthesis pathway in native or foreign hosts. 104
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However, until recently magnetosome biosynthesis has remained poorly understood at the 105
molecular level. We previously discovered genes controlling magnetosome synthesis in MSR 106
to be clustered in several operons within a large genomic magnetosome island (15, 16). These 107
genes (approximately 30) also proved sufficient to induce biosynthesis of well-ordered 108
magnetosome chains upon transfer into the photosynthetic bacterium Rhodospirillum rubrum 109
as a foreign expression host (17). In the native host MSR, the large mamAB operon 110
(mamABop) alone is sufficient to sustain rudimentary magnetite biomineralization in the 111
absence of all other magnetosome genes (16). From the 17 mamABop genes, a subset of only 112
few (mamE, M, O, Q, B) is essential for magnetite biomineralization, while in single deletion 113
mutants of the other genes biomineralization was impaired to different degree (18). The 114
smaller mamGFDCop, mms6op and mamXYop are not essential but have accessory roles in 115
controlling the biomineralization of properly sized and shaped crystals (2, 16, 19). For 116
instance, the combined deletion of mamG, F, D, and C encoding some of the most abundant 117
magnetosome membrane proteins resulted in somewhat smaller and less regular magnetite 118
particles (2), whereas deletion of the entire 3.7 kb (5 genes) mms6op caused the synthesis of 119
substantially smaller and misaligned crystals (16). Consistent with these findings, the MmsF 120
and Mms6 proteins were predicted to be major regulators of crystal size and shape in the 121
closely related M. magneticum (20, 21). In MSR deletion of the entire mamXYop that encodes 122
various functions in redox and transport of iron also caused a mixed phenotype, characterized 123
by smaller, regular shaped magnetite crystals that were flanked by irregular shaped tiny flake-124
like hematite crystals. Unlike deletions of all other magnetosome genes which consistently 125
resulted in crystal size reduction of various degrees, loss of mms36 and mms48 (comprised 126
within mms6op) intriguingly caused the synthesis of fewer but larger magnetite crystals (18). 127
Plasmid expression of the entire mamGFDCop in the WT also resulted in the formation of 128
slightly enlarged (by 14.7%) magnetite particles (2). From these observations it was 129
concluded that magnetite biomineralization is affected in a cumulative manner by various 130
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different magnetosome proteins (18). However, it has remained unknown how maximum size 131
and numbers of magnetosomes are precisely regulated, and controlled genetic overproduction 132
of magnetosome biosynthesis has not been achieved, much due to the difficulties of large 133
scale genome engineering in the native MTB. 134
In this study, we established and systematically explored a strategy for overexpression of 135
magnetosome biosynthesis by genomic multiplication of single and multiple magnetosome 136
gene clusters via sequential chromosomal insertion by transposition. While stepwise insertion 137
of additional mms6op copies caused the formation of increasingly larger (up to 80 nm) 138
regularly shaped magnetite crystals, duplication of all four known magnetosome operons 139
resulted in an overproducing strain, in which magnetosome numbers were more than 2fold 140
increased on average. Our findings also indicate that the expression level of many Mam and 141
Mms proteins together limits the upper size and number of magnetosomes within the cell. We 142
demonstrate that genetically tuned expression of the mam and mms clusters provides a 143
powerful strategy for the control of the magnetosome size and numbers, thereby setting the 144
stage for high-yield production of tailored magnetic nanoparticles in various hosts by 145
synthetic biology approaches. 146
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Methods 157
Bacterial strains, plasmids, and culture conditions 158
MSR and its mutant strains (Tab. S1) were grown in liquid modified flask standard medium 159
(FSM) or low iron medium (LIM) at 30° C under microaerobic condition if not otherwise 160
specified (24). Therefore, cells were cultivated in gassed flasks with a mixture of 2% O2 and 161
98% N2 or in purged jars. For anaerobic cultivation, O2 was excluded from the gas mixture, 162
while aerobic conditions were generated by free gas exchange to air. Single colonies were 163
transferred into 100 μl FSM medium in 96-deep-well plates (Eppendorf, Hamburg, Germany 164
and incubated in anaerobic jars for 5 to 6 days. The liquid cultures were scaled up to an final 165
volume of 10 ml. Culture conditions for Escherichia coli strains (Tab. S1) were as previously 166
described (38). For strains BW29427 and WM3064 lysogeny broth medium was 167
supplemented with 1 mM DL-α, ε-diaminopimelic acid (DAP). For selection of antibiotic 168
resistant strains the following antibiotics concentrations were used: 25 µg ml-1 kanamycin 169
(Km), 12 µg ml-1 tetracycline (Tet), and 15 µg ml-1 gentamicin (Gm) for E. coli strains, and 170
5 µg ml-1 kanamycin, 5 µg ml-1 tetracycline, and 20 µg ml-1 gentamicin for MSR strains, 171
respectively. Magnetosomes were isolated as described in Grünberg et al. (2004) after 172
microaerobic cultivation of 5 liter cultures (39). Optical density and magnetic response (Cmag) 173
were analyzed photometrical at 565 nm (40). 174
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Molecular and genetic techniques 176
Oligonucleotide sequences for amplification of DNA fragments (Tab. 1) were deduced from 177
the working draft genome sequence of MSR (GenBank accession number No. CU459003) 178
and were purchased from Sigma-Aldrich (Steinheim, Germany). Standard polymerase chain 179
reaction (PCR) procedures were used to amplify genetic fragments, and plasmids were 180
sequenced using BigDye Terminator v3.1 chemistry on an in-house ABI 3730 capillary 181
sequencer (Applied Biosystems, Darmstadt, Germany). Sequences were analyzed with 182
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Software Vector NTI Advance® 11.5 (Invitrogen, Darmstadt, Germany). For genomic 183
sequencing of overexpression strains tagged libraries (about 200-300 bp insert size) were 184
constructed from 1 ng of genomic DNA with the Nextera XT DNA kit (Illumina) according to 185
the manufacturer's protocol. The eight libraries were sequenced in multiplex format using the 186
Illumina MiSeq technology. The obtained sequences were assembled de novo as well as to the 187
reference genome with a commercial software, CLC Genomics Workbench 5.5. 188
189
Analytical methods 190
Iron content of magnetosomes or whole cells was measured three times in triplicates by 191
ferrozine assay (41). After 16 hours of cultivation cells were washed with 20 mM Tris-HCl, 5 192
mM EDTA, pH 7.4 to remove extracellular iron. 1 ml cultures were centrifuged for 1 min at 193
11,000 xg and resuspended in 90 µl HNO3 (65%) for 3 h at 99° C. Afterwards, the lysate was 194
cleared by centrifugation and resuspended in 1 ml H2O and ferrozine assay was performed as 195
previously described (22, 41). 196
197
Construction of plasmids for overexpression and conjugative transfer 198
Plasmids pTps_AB and pTps_XYZ were constructed in a previous study by Kolinko et al., 199
2014 (17). For cloning of plasmid Gm-pTps_AB, the Km resistance gene on plasmid 200
pTps_AB was exchanged by gentamicin via recombinogenic cloning (42, 43). To this end, a 201
cloning cassette comprising the gentamicin gene and the respective promoter was PCR-202
amplified (oligonucleotides IB173/IB174) and transferred into electrocompetent E. coli cells 203
(DH10ß+pTps_AB) expressing phage derived recombinases from a plasmid (pSC101-BAD-204
gbaA). After transfer of the cassette, recombination between homologous regions on the 205
linear fragment and the plasmid pTps_AB occurred. 206
For overexpression of the mms6 and mamGFDC operon, a modified pBam-1 vector was 207
designed. To this end, egfp (enhanced green fluorescent protein) was amplified with 208
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oligonucleotides IB102 and IB103 and integrated after digestion with KpnI and EcoRI into 209
pBam-1, resulting in pBam-gfp. The mamGFDC (2185 bp) and mms6 operons (3638 bp) were 210
amplified by PCR from the genome of MSR (AL179/AL301) and were inserted into the 211
XbaI+KpnI digested pBam-gfp, resulting in pBam_mamGFDC and pBam_mms6 1x, 212
respectively with a C-terminal fusion to mamC or mms48 of egfp. For generation of 213
pBam_mms6 2x and pBam_GFDC/mms6, the mms6 operon of pBam_mms6 1x was amplified 214
with oligonucleotides AL377/AL379 and integrated into pBam_mamGFDC as well as 215
pBam_mms6 1x after digestion with EcoRI. To realize the insertion of four mms6 operons the 216
gentamicin gene, flanked by a lox71 and lox66 sequence was generated by amplification with 217
oligonucleotides AL300/AL303 from pBBR-MCS5 and cloned into the SanDI/AatII side of 218
pBam_mamGFDC, resulting in pBam_GFDC/Gm. The mamGFDC operon was exchanged by 219
the mms6 operon after digestion of pBam_GFDC/Gm with XbaI+KpnI, generating 220
pBam_mms6/Gm. Generated plasmids were examined by restriction analysis with a set of 221
different enzymes or PCR and transferred into different recipients via conjugation as 222
described elsewhere (22). 223
224
Fluorescence microscopy 225
For localization studies of the EGFP-fusion proteins and cell length measurements, generated 226
mutant strains of MSR were immobilized on agarose pads (FSM salts in H2O, supplemented 227
with 1% agarose), and analyzed with an Olympus BX81 microscope provided with a 100 228
UPLSAPO100XO objective (numerical aperture of 1.40) and a Hamamatsu Orca AG camera. 229
Data were evaluated with the Olympus cell software. 230
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Electron microscopy techniques 232
Cells or magnetosomes were concentrated and adsorbed onto carbon-coated copper grids for 233
TEM analyses. Isolated magnetosomes were treated with 1% (v/v) uranyl acetate for staining 234
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of magnetosome membrane. Cells and vesicles were imaged with a FEI Morgagni 268 (FEI, 235
Eindhoven, Netherlands) at an accelerating voltage of 200 kV. 236
For Cryo-electron tomography (CET) analysis, cells were cultivated anaerobically in FSM or 237
aerobically in LIM and treated with formaldehyde (Fluka, Switzerland) to a final 238
concentration of 0.1% v/v after 16 h of cultivation. A FEI Tecnai F30 Polara transmission 239
electron microscope (FEI; Eindhoven, the Netherlands), equipped with a 300 kV field 240
emission gun, a Gatan GIF 2002 Post-Column Energy Filter, and a 2048 x 2048 pixel Gatan 241
CCD camera (Gatan; Pleasanton, CA) was used for data generation, whereby image 242
acquisition was performed at 300 kV, with the energy filter operated in the zero-loss mode 243
(slit width of 20 eV). Sample preparation and acquisition scheme were implemented as 244
described previously (5). Tilt series were acquired with Serial EM software and three-245
dimensional reconstructions were performed with the weighted back-projection method using 246
TOM toolbox (44). 247
248
Statistical analysis of magnetosome size and number 249
The t-test (http://www.socscistatistics.com/tests/studentttest/Default.aspx) was used to 250
determine the significance of differences in crystal size distributions. For statistical analysis of 251
the differences in crystal numbers, the u-test was performed (https://ccb-compute2.cs.uni-252
saarland.de/wtest/?id=www/www-ccb/html/wtest). 253
254
Cell fractionation 255
Mutant strains IK-1, 3xmms6op, and 2xABG6Xop were grown in 5 liter FSM under 256
microaerobic conditions. After centrifugation at 9,000 xg, cells were resuspended in 20 mM 257
Tris-HCl, pH 7.4, 5 mM EDTA and stored at 4° C. Cell fractionation and magnetosomes 258
isolation were executed as described elsewhere (45). 259
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Gel electrophoresis and Western blot experiments 261
The BCA-Protein Micro assay kit (Pierce) was used for determination of protein 262
concentrations, according to the manufacturer’s recommendation. Protein samples from the 263
magnetosome membrane fraction were resuspended in electrophoresis sample buffer and 264
denatured at 98° C for 5 min. Polyacrylamide gels were prepared according to the procedure 265
of Laemmli (46). 10 µg of protein extracts were separated on a 15% SDS-polyacrylamide gel. 266
Protein bands were visualized by Coomassie brilliant blue staining. Western blot analysis for 267
detection of MamM, MamA and MamC was performed as previously described (39). The 268
intensity of the protein bands of MamM, MamA and MamC was compared via the ImageJ 269
software. 270
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Results 287
Magnetosome gene clusters can be multiplied by sequential chromosomal 288
transposition 289
In the absence of appropriate promoters for transcriptional overexpression (13), we 290
explored the effects of genetic multiplication of magnetosome operons by sequential 291
transposition. For stabilization of multiple identical gene copies we chose the recA mutant 292
strain IK-1 (22) of MSR as chassis, which is otherwise wildtype (WT) with respect to 293
magnetosome biosynthesis (Tab. 2). As described below, multiple copies of various 294
magnetosome gene clusters between 2 and 17 kb in size cloned on non-replicative vectors 295
were inserted into the chromosome of the parental strain IK-1. Therefore sequential rounds 296
of mariner or Tn5 transposon driven random chromosomal insertions were selected by 297
multiple antibiotic resistances (Fig. 1), similar as previously applied for genetic transfer of 298
the entire magnetosome biosynthesis pathway into a foreign host (17). Transconjugants 299
were typically obtained at frequencies of 10-7 and 10-8 and found inserted in single copies 300
as revealed by genome sequencing (Tab. S2). As tested for several of the resulting strains, 301
antibiotic resistance and magnetosome phenotypes remained stable for >100 generations in 302
the absence of selective pressure. 303
304
Multiplication of mms6 and mamGFDC operons causes enlargement of 305
magnetite crystals 306
First, we tested the approach by attempting to insert one, two, three and four additional 307
copies of the mms6 operon by consecutive transposition of pBam_mms6 1x, pBam_mms6 308
2x and pBam_mms6/Gm, resulting in strains 2xmms6op, 3xmms6op, 4xmms6op and 309
5xmms6op, respectively. The merodiploidic strain 2xmms6op, which now harbored one 310
additional copy of the mms6op, displayed a slightly increased magnetic response, an 311
increased intracellular iron accumulation (+15%), and the number of magnetosome crystals 312
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per cell (47 particles, p<1.3 E-6) was higher (+37%) than in IK-1 with the mean particle 313
size increased by 26% (46 nm, p<1. 0 E-5, Tab. 2). Insertion of two and three additional 314
copies resulted in strains 3xmms6op and 4xmms6op, respectively, and caused a further 315
increase in crystal size and number by about 32% and 70% compared to IK-1. However, 316
insertion of an additional mms6op copy (yielding strain 5xmms6op) did not further enhance 317
biomineralization, but caused reduction of particle size and number compared to its parent 318
strain 4xmms6op (Tab. 2). Also, increasing extracellular iron concentrations up to 250 µM 319
had no effect on biomineralization in the overproducing strains (data not shown). 320
Within some cells of 2xmms6op and 2xmamABop, a variable proportion of enlarged 321
vesicles were visible in cryo electron tomograms (Fig. 3a). These “giant” vesicles 322
appeared spherically shaped as in the WT, but their size was increased up to nearly 110 nm 323
(2xmms6op) or 81 nm respectivley (2xmamABop), whereas vesicles of the WT had a 324
maximum size of 63 nm. In addition, increase in mms6op copy number caused a slight 325
gradual cell elongation with a maximum mean cell length of 5.3 µm for strain 5xmms6op, 326
(IK-1: 4.4 µm, Tab. 2, Fig. 2a). Cell length seemed to be correlated with the magnetosome 327
number within the same strain. For example shorter cells of strain 2xmms6op contained 328
fewer (43 particles) and smaller (43 nm) crystals. On the other hand highly elongated cells 329
(>10 µm) contained significantly more (53-138 particles, mean: 104) and larger (49 nm) 330
magnetosome crystals with a maximum size of 80 nm (Fig. S1). While magnetosome 331
chains in cells of strains 2xmms6op and 3xmms6op were persistently located at midcell and 332
split during cell division as in the WT (23), daughter cells of 2xmms6op and 3xmms6op 333
remained frequently connected by deformed separation sites, sometimes even extending 334
into tubular structures connecting the daughter cells, which probably result from 335
incomplete separation of the cells during or after division (Fig. 4). Within these structures 336
often up to 20 magnetosome particles were found to be enclosed (Fig. 4b). 337
Next, we explored the effects of overexpressing the mamGFDCop, which is adjacent to the 338
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mms6op and which was previously shown to be involved in size control of magnetosomes 339
(2). While duplication of mamGFDCop (strain 2xGFDCop) alone only resulted in only 340
moderate increase in number (+7%, p<0.32, Tab. 2) and size (+24%, p<1. 0 E-5, Tab. 2) of 341
crystals, the simultaneous duplication of both mms6op and mamGFDCop 342
(2xmms6op+2xGFDCop) caused the synthesis of 33% more crystals per cell (p<8.2 E-6, 343
Tab. 2), consistent with the iron content increased by 7.4% in 2xGFDCop and even further 344
by 14.1% in strain 2xmms6op+2xGFDCop (Tab. 2). Magnetosome crystals of strains 345
2xGFDCop and 2xmms6op+2xGFDCop were larger by approximately 25% compared to 346
IK-1 (Tab. 2). 347
348
Multiplication of the mamABop results in heterogeneous magnetosome morphotypes 349
We next attempted to multiply the large mamABop that was shown to encode all 350
magnetosome proteins essential for magnetosome formation (16, 18). The merodiploidic 351
strain 2xmamABop (i. e., harboring one native and one additional mamABop copy) showed 352
a similar magnetic response and iron content as the parental strain (Tab. 2). Remarkably, 353
the mean number of crystals per cell was increased by 115%. However, closer inspection 354
by TEM revealed that cultures of strain 2xmamABop were heterogeneous with respect to 355
magnetosome phenotypes. Three distinct morphotypes were present in variable 356
proportions, comprising i) ~50% cells in which the number of regular-sized magnetosomes 357
was increased to 77 particles per cell with a regular chain like organization, ii) ~40% cells 358
with increased number of magnetosomes (68 per cell), but with smaller crystal sizes and 359
aberrant intracellular localization, and iii) 10% WT-like cells (Fig. S2). This pattern 360
remained constant even after repeated clonal selection by colony purification of the strain. 361
Compared to the single chain typically found in WT cells, we frequently observed two 362
distinct magnetosome chains within cells of 2xmamABop, which were aligned along two 363
separate bundles of cytoskeletal filaments located at opposite sides of the cell as detected 364
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by Cryo-electron tomography (CET) (Fig. 3b). Purified magnetosome crystals from strain 365
2xmamABop were enveloped by a magnetosome membrane (MM) with the same 366
appearance and thickness as in the WT. Coomassie-stained SDS-PAGE profiles of the MM 367
from strains 2xmamABop and 3xmms6op displayed also similar band patterns as the MM 368
of strain IK-1. However, the intensity of bands at 33 and 24 kDa (corresponding to 369
magnetosome proteins MamA and MamM that were among the duplicated genes) was 370
increased, and quantitative Western blot analysis confirmed higher abundance of these 371
proteins by about 130% and 145%, respectively. On the contrary, the abundance of MamC, 372
which is encoded outside the mamABop was not significantly affected (below 10% 373
variation, Fig. S3). 374
The merotriploidic insertion mutant 3xmamABop (obtained by transfer of pTps-mamAB-375
Gm into strain 2xmamABop) showed a similar phenotype as strain 2xmamABop, and the 376
number of magnetosomes did not further increase, despite of a slightly increased 377
intracellular iron content (+9.4%). The Cmag (magnetic response) of strain 3xmamABop 378
was even lower than that of the parental strain (0.5±0.2), possibly caused by the altered cell 379
dimensions (Tab. 2). In summary, overexpression of mamABop alone caused a 380
heterogeneous phenotype, but overall did not consistently enhance magnetosome 381
biosynthesis. 382
383
Chromosomal duplication of all magnetosome gene clusters causes magnetosome 384
overproduction 385
The previous experiments had revealed that chromosomal insertion of up to three 386
additional mms6 operons gradually enhanced the biosynthesis of magnetosomes. However, 387
neither introduction of additional mms6op copies nor the combined overexpression of 388
mamGFDCop, and mamABop alone did further increase biomineralization, suggesting that 389
magnetosome synthesis in these strains was likely limited by different factors encoded 390
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outside the multiplied operons. Therefore, we next attempted the combined overexpression 391
of all four major operons (mms6op, mamGFDCop, mamABop and mamXYop). To this end, 392
mamABop, mms6op, and mamGFDCop were altogether inserted into the chromosome of 393
IK-1 by transposition of pTps_ABG6. Next, in addition we inserted the mamXYZop 394
(lacking ftsZm to avoid interference with cell division during cloning (17) resulting in 395
strain 2xABG6Xop, which is merodiploidic for all four key magnetosome operons (Fig. 1). 396
Transconjugants of 2xABG6Xop were obtained at frequencies of only 2-5x10-9. Compared 397
to strains in which the copy number of a single operon was increased and which showed 398
essentially WT-like growth under all tested conditions, growth of strain 2xABG6Xop was 399
severely impaired at temperatures ≥30 °C. However, since WT-like growth was observed 400
at 23 °C, cells were cultivated at this temperature in all subsequent experiments. Cells on 401
average were more elongated (5.1 µm) than the parent strain IK-1, and we also observed 402
deformed separation sites during or after cell division similar to those in 4xmms6op (data 403
not shown). 404
While the magnetic response of strain 2xABG6Xop was similar to that of IK-1, the 405
intracellular iron content was 2.4 fold increased. Cells contained 74 electron-dense 406
particles on average, equivalent to an increase in number by 118% (Tab. 2; Fig. 1). 407
Magnetosome yields (mg Fe3O4 per g biomass (wet weight)) were also substantially 408
increased during anaerobic, nitrate-fed growth experiments at larger scale in a 30 liter 409
fermenter, in which strain 2xABG6Xop showed similar cell yields (cells per ml) to the WT 410
(OD565nm = 0.5 after 36 h), and 2.8 mg Fe3O4 per g of biomass (wet weight) could be 411
isolated, compared to the about 1.20 mg/g obtained from fermenter-grown WT cells. 412
As we recently found that co-expression of the ferrous iron uptake system FeoAB1 413
encoded next to the MAI together with the four key magnetosome operons further 414
enhanced heterologous magnetosome biosynthesis (17), we tested whether overexpression 415
of these proteins also may enhance biomineralization in overproducing MSR. To this end, 416
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feoA and feoB genes (comprised on Tet-pBam_feoAB1) were inserted into 2xABG6Xop by 417
Tn5 transposition. Whereas crystal sizes were not significantly increased (41 nm vs. 39 nm 418
in 2xABG6Xop) in the resulting strain 2xABG6X+2xfeo, the crystal number per cell was 419
slightly decreased (69 particles instead of 74 in strain for 2xABG6Xop, Tab. 2). 420
About 28% of the cells from the overproducer strain 2xABG6Xop had more than 100 421
magnetosomes (maximum: 170), whereas IK-1 cells were found to never contain more 422
than about 60 magnetosomes. However, the mean size of crystals was only slightly 423
increased to 39 nm (Fig. S4, Tab. 2), and empty and partially filled MM vesicles 424
(approximately 54 nm in size) were not significantly enlarged compared to the WT (Fig. 425
2). Most cells contained multiple (two to four) magnetosome chains (9% one chain, 23% 426
two chains, 34% three chains, 18% four chains) (Fig. 2), whereas the WT typically exhibits 427
not more than 2 chains per cell (76% one chain, 20% two chains, 4% three chains, 0% four 428
chains) (23). Beside cells with proper WT-like chains (localized near the inner curvature of 429
the cell), we frequently observed cells with ectopically positioned chains (Fig. 2bi). The 430
plentiful particles present in some cells often lacked any clearly ordered chain-like 431
alignment, but appeared “stuffed” into compact bundles or large irregular clusters (Fig. 432
2bii). Cells exhibited a tendency to spontaneously disintegrate as indicated by the presence 433
of released magnetosome particles in the vicinity of partially lysed cell bodies in TEM 434
micrographs (Fig. 2biii). 435
436
437
438
439
440
441
442
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Discussion 443
Despite of some progress by growth optimization (24, 25) previous attempts to increase 444
magnetosome yields at large scale were met only by limited success. In this work, we 445
established a strategy to enhance magnetosome production by genetic engineering. In the 446
absence of well characterized promoters for very strong and inducible transcription, we 447
attempted overexpression by increasing copy numbers of several or all mam and mms operons 448
comprised within the genomic magnetosome island. Since we previously found that 449
unbalanced multi-copy expression of the large mamABop from replicative plasmids was 450
unstable in MSR and caused spontaneous deletions and rearrangements (data not shown), we 451
employed chromosomal insertion via transposition. In striking contrast to plasmid expression, 452
chromosomally multiplied gene clusters apparently remained stable at least within the tested 453
>100 generations grown under laboratory-scale conditions. 454
Similar amplification via chromosomal multi-copy insertion of gene clusters has been applied 455
in several other studies. For instance, Tang et al. recently increased production of the 456
secondary metabolite spinosyn in the native host by partial gene cluster duplication (26). 457
Using a chemically inducible chromosomal evolution approach, 40 copies of a poly-3-458
hydroxybutyrate gene cluster were consecutively inserted into the chromosome of E. coli, 459
thereby causing a significant productivity increase for this biopolymer (27). 460
In our study, dupli- or triplication of the mms6 operon alone caused a gradual strong 461
enlargement of magnetite crystals, but only a moderate increase in their numbers. In contrast, 462
duplication of all mam and mms gene clusters yielded an overproducing strain (2xABG6Xop), 463
in which average magnetosome numbers per cell were greatly increased by at least 120% 464
compared to previous studies (16, 10). This strain is also highly promising for future 465
magnetosome production at larger scale as it continued to produce large magnetosome 466
numbers per cell (up to 170 cell-1) even during mass cultivation while cell yield remained 467
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wildtype-like. Thus, magnetosome yields from the overproducing strain (2xABG6Xop) were 468
2.3-fold increased compared to the WT. 469
On the other hand, the mean size of magnetite crystals was only weakly increased by 470
duplication of all MAI clusters, compared to the strong effect of mms6 operon multiplication 471
alone. This suggests that the engineering of distinct determinants can control both 472
magnetosome size and number independently. However, the fact that the iron contents of less 473
magnetic strains with fewer particles were in similar to those with more particles, such as 474
2xmms6op and 2xABG6Xop, raises the question whether the less magnetic strains might have 475
accumulated iron in form other than magnetite, or other substantial iron pools. The existence 476
of such variable iron pools could have been affected to different degrees by inserted mutations 477
in a yet unknown way and will be subject to future studies. 478
It is well established that various physical characteristics of magnetic nanoparticles, such as 479
sedimentation stability and magnetic remanence, are functions of their size (14). While 480
particles smaller than about 30 nm are superparamagnetic (i. e. no permanent magnetic signal 481
at room temperature in the absence of an external field), particles between 30 and about 60-482
100 nm have stable single domains (i. e., a remanent magnetization), and the large single 483
domain particles generated in this study can be expected to be close to the maximum with 484
respect to coercivity (28). Although full characterization of their magnetic properties remains 485
to be completed, initial analysis of some of the engineered large particles indeed indicated 486
stable single domain behavior and a higher magnetic coercivity than WT magnetosome 487
particles (29). Since so far no synthetic routes are available for the abiogenic fabrication of 488
such large magnetic single domain nanoparticles, our findings will be of particular interest in 489
applications, which depend on the specific magnetic properties of such large and size-490
adjustable particles, such as magnetic resonance imaging (30) or hyperthermia (14). 491
Size, shape, number and intracellular organization of magnetosomes also critically affect the 492
strength of the cellular dipole moment that aligns cells by magnetic torque (1). Under 493
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environmental conditions, magnetosome biosynthesis has to be precisely regulated to be 494
strong enough to orient the cell within the weak geomagnetic field with sufficient efficiency. 495
On the other hand increasing the number and size beyond the rather narrow evolutionary 496
optimum that has been calculated for magnetic spirilla with about 20-25 particles per cell (31) 497
would not significantly improve orientation because of the asymptotic Langevin function for 498
alignment of magnetic dipoles (1), but would increase metabolic burden and energetic costs of 499
excessive magnetosome biosynthesis as well as potential harmful effects related to increased 500
iron uptake (1). However, it has remained unknown, how the maximum number and upper 501
size limit of magnetic single-domain particles are controlled at the molecular and structural 502
levels. One important factor spatially constraining the growth of crystals can be expected the 503
size of magnetosome vesicles (2). In fact, we sometimes observed significantly enlarged 504
vesicles in the mms6 insertion strains by CET (Fig. 3). This indicates that overexpression of a 505
subset of proteins might directly influence the vesicle diameter prior to crystallization, thereby 506
defining the increase in crystal size. Besides vesicle biogenesis, also magnetosomal iron 507
import into the vesicles is required to sustain growth of magnetite (Fe3O4) crystals. While 508
none of the proteins encoded by the mms6 operon likely function as iron transport proteins, 509
amplification of putative iron transporters (MamB, M, H, and Z) might explain the increase in 510
magnetosome number in 2xABG6Xop. In fact, in strain 2xmamABop, expression of MamM in 511
the MM was markedly increased by about 130% compared to the parent strain. 512
Overexpression of a subset of magnetosome genes might also influence expression or 513
recruitment of other proteins controlling accessory processes during magnetosome formation 514
(32, 33). 515
Altogether, our findings suggest that the balanced expression level of magnetosome proteins 516
is one important factor for determination of the number and size of magnetite crystals. 517
However, this also raises the intriguing question of what might potentially define the upper 518
limit of number or size of magnetosomes in overexpression strains. For instance, the 519
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extracellular supply is known to be critical for magnetosome formation in MSR and iron 520
concentrations of 100 µM were found to be already saturating for cell yield and magnetism 521
(34). Surprisingly, increasing extracellular iron beyond that concentration had no effect on 522
biomineralization in the overproducing strains, and chromosomal duplication of genes 523
encoding the ferrous iron transporter FeoAB1 also had only minor effects (Tab. 2), indicating 524
that the iron supply is not a limiting factor for magnetite overproduction under tested 525
conditions. However, biomineralization of the mixed-valence iron oxide magnetite was found 526
to be critically dependent on proper ferric-to-ferrous iron ratio (35-37), and thus regulation by 527
general metabolic pathways such as aerobic and anaerobic respiration processes might 528
become limiting with increasing expression of the magnetosome synthesis machinery. 529
It might be also possible that further increase in magnetosome overproduction might be 530
simply limited by spatial constraints imposed by the shape and confined size of the cell 531
lumen. We also found that magnetosome overexpression increasingly impaired growth of 532
overproducing cells. For instance, strain 2xABG6Xop eventually reached similar cell yields, it 533
no longer grew at the usual 30° C, but required incubation at lower temperatures around 23° 534
C, possibly due to accumulation of misfolded overexpressed proteins or effects on lipid 535
biosynthesis required for increased MM biosynthesis. In addition, we observed that cell 536
division was slightly impaired in cells, as indicated by the presence of conspicuously 537
elongated cells that often remained connected by deformed separation sites at advanced stages 538
of constriction. This phenotype might be caused by the stronger magnetostatic interactions 539
between the larger and more abundant particles within the chains, which require higher 540
mechanical forces to be overcome (23). Altogether, in addition to the maximum cell size, 541
there are likely multiple factors, which set an upper limit for future overexpression 542
approaches that may require engineering of the native host or use of alternative foreign 543
expression hosts. 544
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In conclusion, our results are very promising for the construction of further engineered strains 545
of magnetotactic bacteria, overproducing for example genetically engineered magnetosomes 546
with enhanced functionalities and even higher magnetosome yields (9, 13). Furthermore, 547
overexpression of selected magnetosome genes and clusters in homologous and heterologous 548
hosts might be exploited for the design and mass production of size-adjusted nanocrystals 549
with tuned magnetic properties. 550
551
Funding Information 552
This work was supported by the Human Frontier Science Foundation (grant RGP0052/2012), 553
the Deutsche Forschungsgemeinschaft (grant SCHU 1080/15-2) and the European Union 554
(Bio2MaN4MRI). A.L. was supported by the Konrad-Adenauer-Stiftung. The funders had no 555
role in study design, data collection and interpretation, or the decision to submit the work for 556
publication. 557
558
Acknowledgment 559
We are thankful to A. Nieto, R. Susen, and A. Hähle for expert technical and experimental 560
assistance. All authors declare that no competing interests exist. 561
562
Supplemental Material 563
Table S1 564
Figure S1 565
Figure S2 566
Figure S3 567
Figure S4 568
569
570
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715
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Figures 717
Figure 1. (a) Schematic overview of cloned magnetosome operons (brown: mms6, green: 718
mamGFDC, dark blue: mamAB, pale blue: mamXY, pink: feoAB1) and the respective 719
promoters (angled arrows). (b) Strategy for construction of overexpression strains by 720
amplification of different magnetosome operons. Genomic fragments from 721
M. gryphiswaldense were cloned into transposon-based vectors. Plasmids contain the 722
magnetosome operons mamAB (blue, AB), mamGFDC (green, GFDC), mms6 (brown) and the 723
mamXY operon lacking ftsZm (pale blue, XYZ). The vector backbone (genes are indicated in 724
red) contains a transposase gene (tps), inverted repeats (IR), origin of transfer (oriT), an R6K 725
or p15A origin of replication (ori) and antibiotic resistance cassette (abR). After conjugative 726
transfer of the plasmids, the transposase recognizes IR sequences and catalyzes chromosomal 727
insertion of the target sequence. Additional copies of respective magnetosome operons in the 728
chromosome (oval shape) are marked with asterisks. 729
730
Figure 2. TEM analysis of overexpression strains compared to the parental strain IK-1. (a) 731
TEM of the overexpression strains 4xmms6op (aii), 2xmamABop (aiii) and 2xABG6Xop (aiv) 732
compared to IK-1 (ai). Arrows 1 and 2 in (aiii) illustrate two different morphotypes found for 733
2xmamABop. (b) Transmission electron micrographs of 2xABG6Xop. Cells with one chain 734
located at the inner convex cell curvature and up to three magnetosome chains with ectopic 735
localization (bii). Cells that lack a clearly ordered chain-like alignment of the produced 736
particles and tend to burst during TEM grid preparation (biii). Scale bar = 500 nm. 737
738
Figure 3. Cryo-electron tomographs of 3xmms6op, 2xmamABop and 2xABG6Xop. (a) 739
Segmented tomogram of a 3xmms6op cell, illustrating the intracellular position of the 740
magnetosome chain as well as the membrane vesicles (ai). Slightly enlarged vesicles are 741
indicated by white arrows. Tomogram section of the same 3xmms6op cell with enlarged 742
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vesicles (white arrows, aii). (b) Tomograms of a 2xmamABop mutant cell (bi and bii) from 743
different angles, which illustrate two independent magnetosome chains aligned along two 744
parallel filaments at opposite sites of the cell. (c) Segmented tomograms of a 2xABG6Xop cell 745
shown from different angles (ci and cii), which contains three intertwined magnetosome 746
chains, and regularly sized vesicles. Different colors indicate the outer and inner membrane 747
(blue), magnetosome membrane vesicles (yellow), magnetosome filament (green), and 748
magnetite crystals (red). 749
750
Figure 4. TEM micrographs of dividing cells of 4xmms6op (a) and 2xABG6X+2xfeo (b), 751
which remained connected by deformed separation sites with enclosed magnetosomes 752
(arrows). Scale bar = 500 nm. 753
754
755
756
757
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Tables 770
Tab. 1: DNA oligonucleotides used in this work. 771
Name Sequence
IB102 GGCGGTACCGGAGGCGGAGGCGGT
IB103 GGCGAATTCTTACTTGTACAGCTCGTCCATG
IB173 CCGGAATTGCCAGCTGGGGCGCCCTCTGGTAAGGTTGGGAAGCCCTGCAACGTA
TAATATTTGCCCATG
IB174 AGGCGATAGAAGGCGATGCGCTGCGAATCGGGAGCGGCGATACCGTAAAGCGA
TCTCGGCTTGAA
AL179 CATATGTTGGGCTTGTGGTTTTGGCGG
AL301 GGTACCTGTACTGCGGAACAGTCGCG
AL377 GAATTCCAACTTTTTCGCTTTACTAG
AL379 GAATTCTCATGTACTGCGGAACAGTC
AL300 TATGGGACCCTACCGTTCGTATAATGTATGCTATACGAAGTTATCGATCTCGGCT
TGAA
AL303 AATGACGTCTACCGTTCGTATAGCATACATTATACGAAGTTATCGTATAATATTT
GCCCATG
772
773
774
775
776
777
778
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Tab. 2. Characteristics of generated overexpression strains compared to the parental strain IK-1 (n.d. = not determined). 779
Strain Genotypeb Number of
measured
crystals
Mean
crystal size
Cmag Increase in
crystal size
(%)*
Statistical
analysis of
difference in
crystal size
(p-value)*
Crystal
number per
cell
Increase in
crystal
number
(%)a
Statistical
analysis of
difference in
crystal number
(p-value)*
Iron content
(% of the dry
weight) a
Cell
length
(µm)
IK-1
1x MAI
(=WT)s
390 36.2±11.0
0.8±0.2
-
- 33.9±10.3
-
- (3.9±0.2)
4.4± 1.3
2xGFDCop
2x
mamGFDC
operon
424 44.9±13.5
0.9±0.03
24.0
p<1.0 E-5 36.3±12.4
7.1
p<0.303 7.4±1.1
n.d.
2xmms6op
2x mms6
operon
616 45.7±14.2
0.9±0.03
26.2
p<1.0 E-5 46.5±14.3
36.8
p<1.3 E-6 14.9±2.9
4.5±1.6
2xmms6op+
2xGFDC
2x mms6
2x
mamGFDC
operon
483 45.1±12.2
0.9±0.01
24.6
p<3.4 E-5 45.1±14.3
32.7
p<8.2 E-6 14.1±1.9
n.d.
3xmms6op
3x mms6
operon
1183 47.9±12.8
1.0±0.2
32.3
p<1.0 E-5 54.3±29.9
59.5
p<7.2 E-7 34.8±2.5
4.6 ±1.5
4xmms6op 4x mms6 665 44.4±13.2 1.0±0.03 22.6 p<1.0 E-5 57.8±26.9 69.7 p<4.2 E-10 38.8±2.5 5.1 ±1.9
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operon
5xmms6op
5x mms6
operon
545 41.9±12.0
0.9±0.1
15.7
p<1.0 E-5 46.0±14.8
35.3
p<9.5 E-7 n.d.
5.3±1.7
2xmamABop
2x mamAB
operon
436 34.0±17.6
1.0±0.04
-6.1
p<0.05
73.4±43.1
115.2
p<1.5 E-9 0.4±0.5
4.8± 1.8
3xmamABop
3x mamAB
operon
477 35.6±15.4
0.5±0.1
-1.6
p<0.05
68.8±13.2
102.9
p<1.5 E-9 9.4±0.5
6.0± 2.6
2xABG6Xop
2x
mamGFDC
2x mms6
2x mamAB
2x mamXYZ
operon
708 38.7±11.9
0.8 ± 0.1
6.9
p<1.0 E-5 74.5±34.9
118.3
p<9.8 E-15 140.7±2.4
5.1 ±2.1
2xAG6X+
2xfeo
2x
mamGFDC
2x mms6
2x mamAB
2x mamXYZ
operon
2x feoAB
operon
697 41.1 ± 8.4
0.7 ± 0.2
13.5
p<0.00001 69.3±13.4
104.4
p<1.5 E-15 135.9±6.4
n.d.
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780
781
a Compared to IK-1. b with respect to magnetosome genes 782
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mms6mamXY
Plasmid construction
b
mms6abR
tps
IR IR
ori
ABabR
tps
IR IR
ori
AB
abR
tps
IR IR
ori
mms6
GFDC
XYZ
abR
tps
IR IR
ori
4xmms6op
genomic
insertion
2xmamABop 2xABG6Xop
MAI
mms6 IR
MAIMAI
mamGFDC
genomic
insertion
genomic
insertion
MAI
IK-1
DNA
extraction
mamAB oriTabR oriTabR oriTabR oriTabR
IR ABIR IRabRabR ABIR IR
abR
mms6
GFDC
IR IRabRXYZ
a
mamABmms6 mamGFDC
J
mamXY
H I E K L M N O P A Q R B S T U
mmsF
G F D Cmms6
1 kb
mms36
mms48PmamH
PmamDC
Pmms
ftsZmZXY
PmamXY
feoBfeoA
feoAB1
PmamH
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4xmms6op
2
1
2xmamABop 2xABG6Xop
100 nm
IK-1
ai
500 nm
bi
500 nm
bii biii
aii aiii aiv
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200 nm
ai aii
cii
cibi bii
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500 nm
a b
500 nm
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