structures of capsid and capsid-associated tegument ...10.1038... · pen1 p1 p6 p5 c6 p4 c1 e1 e2...

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ARTICLES https://doi.org/10.1038/s41564-020-0758-1 Structures of capsid and capsid-associated tegument complex inside the Epstein–Barr virus Wei Liu 1,2,3,8 , Yanxiang Cui  1,8 , Caiyan Wang 1,2,4 , Zihang Li  1,2 , Danyang Gong 5,6 , Xinghong Dai 1,2,7 , Guo-Qiang Bi  3 , Ren Sun 1,5 and Z. Hong Zhou  1,2 1 California NanoSystems Institute, University of California, Los Angeles, Los Angeles, CA, USA. 2 Department of Microbiology Immunology and Molecular Genetics, University of California, Los Angeles, Los Angeles, CA, USA. 3 Center for Integrative Imaging, Hefei National Laboratory for Physical Sciences at the Microscale, and School of Life Sciences, University of Science and Technology of China, Hefei, China. 4 International Institute for Translational Chinese Medicine, Guangzhou University of Chinese Medicine, Guangzhou, China. 5 Department of Molecular and Medical Pharmacology, University of California, Los Angeles, Los Angeles, CA, USA. 6 Present address: Department of Therapeutics Discovery, Amgen Research, Amgen Inc., Thousand Oaks, CA, USA. 7 Present address: Department of Physiology and Biophysics, School of Medicine, Case Western Reserve University, Cleveland, OH, USA. 8 These authors contributed equally: Wei Liu, Yanxiang Cui. e-mail: [email protected] SUPPLEMENTARY INFORMATION In the format provided by the authors and unedited. NATURE MICROBIOLOGY | www.nature.com/naturemicrobiology

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  • Articleshttps://doi.org/10.1038/s41564-020-0758-1

    Structures of capsid and capsid-associated tegument complex inside the Epstein–Barr virusWei Liu1,2,3,8, Yanxiang Cui   1,8, Caiyan Wang1,2,4, Zihang Li   1,2, Danyang Gong5,6, Xinghong Dai1,2,7, Guo-Qiang Bi   3, Ren Sun1,5 and Z. Hong Zhou   1,2 ✉

    1California NanoSystems Institute, University of California, Los Angeles, Los Angeles, CA, USA. 2Department of Microbiology Immunology and Molecular Genetics, University of California, Los Angeles, Los Angeles, CA, USA. 3Center for Integrative Imaging, Hefei National Laboratory for Physical Sciences at the Microscale, and School of Life Sciences, University of Science and Technology of China, Hefei, China. 4International Institute for Translational Chinese Medicine, Guangzhou University of Chinese Medicine, Guangzhou, China. 5Department of Molecular and Medical Pharmacology, University of California, Los Angeles, Los Angeles, CA, USA. 6Present address: Department of Therapeutics Discovery, Amgen Research, Amgen Inc., Thousand Oaks, CA, USA. 7Present address: Department of Physiology and Biophysics, School of Medicine, Case Western Reserve University, Cleveland, OH, USA. 8These authors contributed equally: Wei Liu, Yanxiang Cui. ✉e-mail: [email protected]

    SUPPLEMENTARY INFORMATION

    In the format provided by the authors and unedited.

    NatuRE MiCRoBioLoGY | www.nature.com/naturemicrobiology

    http://orcid.org/0000-0002-8909-6576http://orcid.org/0000-0002-4625-9283http://orcid.org/0000-0001-8735-3818http://orcid.org/0000-0002-8373-4717mailto:[email protected]://www.nature.com/naturemicrobiology

  • Supporting Information

    Structures of Capsid and Capsid-Associated Tegument Complex inside the Epstein-Barr Virus

    Wei Liu, Yanxiang Cui et al.

    List of Content Supplementary Discussion

    Supplementary Tables 1-3

    Supplementary Figures 1-5

  • 1

    Supplementary Discussion Inter-MCP interactions and structural plasticity of the 20 MCP conformers

    First recognized in HCMV1 and subsequently confirmed in HSV2-4, HHV-6B5, and

    KSHV6, the herpesvirus capsid floor is characterized by either type I, II, or III MCP-MCP

    interactions (Extended Data Fig. 3e-l). Type I interaction is intra-capsomeric while type

    II and type III are inter-capsomeric. Types I, II, and III interactions are formed between

    two or three adjacent MCP subunits by either β-strands in the N-lasso, E-loop in the

    Johnson-fold and dimerization domains (Extended Data Fig. 3g,i-j), or α-helices in the

    dimerization domains (Extended Data Fig. 3h) of the neighboring MCPs. The lasso

    action (type III) occurs only between hexon-hexon MCPs (Extended Data Fig. 3i-j) but

    not penton-hexon MCPs (Extended Data Fig. 3k,l); this is due to the flexibility of the

    penton MCP N-terminus, which causes P6 MCP to refold into a conformation that

    effectively eliminates its lassoing ability (Extended Data Fig. 3k). Additionally, the inter-

    capsomeric interactions between α-helices in the dimerization domains (i.e., type II) also

    only occur between hexon-hexon MCPs because the dimerization domain of penton

    MCP adopts a configuration which makes it unable to form type II interactions with the

    dimerization domain of P1 hexon MCP, rendering the P1 dimerization domain flexible

    (Extended Data Fig. 3k,l).

    In contrast to these conserved MCP domain organization and MCP-MCP

    interaction schemes, the structures among individual MCP subunits of the capsid exhibit

    an unprecedented level of variability which we refer to as structural plasticity

    (Supplementary Video 8). We identified 20 unique conformations among the MCP

    structures resolved in each EBV capsid (Fig. 3; Extended Data Fig. 4): 16 within an

    icosahedral asymmetric triangle (Fig. 3e), 2 portal proximal (Extended Data Fig. 4a,

    right panel), and 2 related to CATC binding (Extended Data Fig. 4a, middle panel).

    These MCPs show structural plasticity at different degrees depending on their

    surroundings. 16 MCPs within the asymmetric unit vary in their local structures

    throughout multiple domains, particularly at their floor regions (Fig. 3e-p). Compared

    with P1, P6 and Pen MCPs, the structures of C1-C6, E1-E3, and P2-P5 MCPs do not

    have dramatic changes. The alignment of these 13 MCP models highlights not only the

  • 2

    conformational changes at their N-lasso domains (Fig. 3j) and two fragments (a.a. 124-

    172 and a.a. 1072-1091) in their Johnson-fold domains (Fig. 3k), but also the orientation

    switch (i.e., being “up” and “down”) of two MCP fragments (a.a. 1149-1169 and a.a.

    1256-1267) in their buttress domains (Fig. 3h,i). Each triplex adopts a unique direction,

    but still can be stabilized by interacting with three quasi-equivalent neighboring MCPs.

    Different interacting sites on the heterotrimeric triplexes (Supplementary Figs. 4-5)

    might be responsible for the multiple binding states found in the buttress sub-domains

    (Fig. 3h,i).

    Variations among MCP subunits can be observed in the floor regions of P1, P6

    and Pen MCPs, particularly in N-lasso (Fig. 3o) and dimerization (Fig. 3n) domains. N-

    lasso of P1 MCP folds similarly with that of C1 MCP, but is completely different from

    those of P6 and Pen MCPs (Fig. 3o). Likewise, the fragment of a.a. 295-374 of P6 MCP

    folds in conformity with that of C1 MCP while differing vastly compared with those of P1

    and Pen MCPs (Fig. 3n). It is worth noting that the fragment a.a. 1277-1323 in the

    buttress domain of Pen MCP folds into a long helix instead of two short helices in those

    of other 15 MCPs (Fig. 3m). As shown in Fig. 3p, the spine helix in the Johnson-fold

    domain of Pen MCP tilts downward ~40º compared with the 15 hexon MCPs.

    There are also variations in the P1 (and P6) MCP structures in the CATC-absent

    vertex (Extended Data Fig. 4a, left panel), CATC-binding vertex (Extended Data Fig. 4a,

    middle panel), and portal vertex (Extended Data Fig. 4a, right panel). Among these

    three, the portal vertex displays the greatest level of structural plasticity (P1 in Extended

    Data Fig. 4b-e; P6 in Extended Data Fig. 4f,g). Such structural variations may result

    from differences in capsid-bindings by CATC and portal proteins. For instance, fragment

    a.a. 80-96 of P1 MCP in the portal vertex flips up rather than down as those in the P1

    MCPs of CATC-absent and CATC-binding vertices (Extended Data Fig. 4d). Fragments

    of a.a. 305-340 and a.a. 1146-1168 are missing in P1 MCP (Extended Data Fig. 4c,e)

    while a.a. 26-63 is invisible in P6 MCP (Extended Data Fig. 4g) in the portal vertex

    reconstruction. These variations in hexons MCPs, particularly P1 and P6 MCPs, and

    penton MCP reveal the intrinsic plasticity of MCP structure in EBV; the folding of

    individual domains is preserved with gradual structural changes spreading out across

  • 3

    different domains, rather than through an abrupt large-scale conformational switch (Fig.

    3e-p). Despite remaining consistent with its role in organizing the three types of MCP-

    MCP interactions (Extended Data Fig. 3e-l), the greatest structural changes were

    observed in N-lasso areas. Taken together, the 20 unique conformers of MCP—16

    MCPs within an asymmetric unit, 2 P1 and 2 P6 MCPs in CATC-binding penton and

    portal vertexes—unveil a remarkable level of structural plasticity of MCP not previously

    reported for any herpesviruses.

    Supplementary Tables Supplementary Table 1. Statistics of cryoEM imaging, data processing and model refinement.

    Supplementary Table 2. Model building statistics.

    Supplementary Table 3. RMSD statistics for MCP and Tri1.

    References 1. Yu, X., Jih, J., Jiang, J. & Zhou, Z.H. Atomic structure of the human cytomegalovirus

    capsid with its securing tegument layer of pp150. Science 356, eaam6892 (2017). 2. Dai, X. & Zhou, Z.H. Structure of the herpes simplex virus 1 capsid with associated

    tegument protein complexes. Science 360(2018). 3. Wang, J. et al. Structure of the herpes simplex virus type 2 C-capsid with capsid-vertex-

    specific component. Nature Communications 9, 3668 (2018). 4. Yuan, S. et al. Cryo-EM structure of a herpesvirus capsid at 3.1 Å. Science 360(2018). 5. Zhang, Y. et al. Atomic structure of the human herpesvirus 6B capsid and capsid-

    associated tegument complexes. Nature Communications 10, 5346 (2019). 6. Dai, X. et al. Structure and mutagenesis reveal essential capsid protein interactions for

    KSHV replication. Nature 553, 521 (2018).

  • 1000 Å

    Viral envelope

    Virus-like vesicles

    Virion

    Supplementary Figure 1. A representative cryoEM micrograph containing one EBV virionparticle. Two types of particles can be seen: virion containing a nucleocapsid (marked by a green box,middle) and virus-like vesicles39 (upper left). Zoomed-in in the right panel is the nucleocapsid showingfingerprint-like pattern, characteristic of dsDNA.

    4

  • C6 hexon sub‐particle reconstruction

    C5 portal vertex sub‐particle reconstruction (cut‐away view) 

    CATC‐binding penton vertex  sub‐particle reconstruction

    10Å

    C12 portal vertex sub‐particle reconstruction

    CATC‐absent penton vertex sub‐particle reconstruction C1 3‐fold sub‐particle 

    reconstruction

    C3 3‐fold sub‐particle reconstruction 

    C2 2‐fold sub‐particle reconstruction 

    C5 penton sub‐particle reconstruction

    7Åa

    b

    FSC = 0.143

    0.00.0 0.1 0.2 0.3

    0.5

    1.0

    3.0Å3.4Å

    4.0Å4.4Å

    5.5 Å

    Fourier she

    ll correctio

    n (FSC) coe

    fficie

    nt

    Resolution (1/Å)

    7.8 Å6.7 Å

    0.4

    C2 2‐fold sub‐particle reconstruction C3 3‐fold sub‐particle reconstruction 

    CATC‐absent penton vertex sub‐particle reconstructionCATC‐binding penton vertex sub‐particle reconstructionC5 portal vertex sub‐particle reconstruction  

    C6 hexon sub‐particle reconstruction

    Icosahedral capsid reconstruction (bin2)C5 capsid reconstruction with portal vertex (bin2)

    C5 penton sub‐particle reconstruction C1 3‐fold sub‐particle reconstruction

    C12 portal vertex sub‐particle reconstruction  

    3.5Å

    Supplementary Figure 3. Resolution assessment of 3D reconstructions. (A) Local resolutionevaluation of sub-particle reconstructions by ResMap59. Color bar represents resolution range. (B)“Gold-standard” Fourier shell correlation (FSC) curves of the 3D reconstructions. The resolutions ofthe icosahedral reconstruction and C5 whole virus reconstruction are 5.6 Å and 7.8 Å, respectively;those for the other sub-particles are as follow: 3.0 Å (C6 hexon sub-particle reconstruction), 3.4 Å (C22-fold sub-particle reconstruction), 3.4 Å (C3 3-fold sub-particle reconstruction), 3.5 Å (C5 pentonvertex sub-particle reconstruction), 4.0 Å (CATC-binding sub-particles reconstruction), 4.1 Å (C1 3-fold sub-particles reconstruction), 3.5 Å (CATC-absent penton sub-particle reconstruction) and 4.4 Å(C5 portal vertex sub-particles reconstruction). All resolutions are based on the 0.143 FSC criterion 51.

    6

  • C1C2C3C4

    P1P2P3 E3P4

    E1E2

    PenC5C6

    P5P6Pen

    P1

    P2

    P3P4

    P5

    P6

    C1

    C2

    C3C4

    C5

    C6E1

    E2

    E3

    Tri1Tri2ATri2B

    a.a., 1149-1169MCPa.a., 1256-1267

    “up” in Fig. 3, H and I

    “down” in Fig. 3, H and I

    Un-modeled

    E1 E2

    E3

    E1E2

    E3

    E1

    E2

    E3

    P1

    Pen

    PenPen

    Pen

    P2

    P3

    P4P5

    P6

    Ta

    Tc

    Tb

    Te

    Tf

    Td

    Te

    MCP within one asymmetric unit

    MCP neighboring to one asymmetric unit

    Triplex within one asymmetric unit

    Triplex neighboring to one asymmetric unit

    Supplementary Figure 4. Schematic diagram of plasticity of triplex interactions with MCP buttress domain shown inFigure 3h,i.

    7

  • Tri2ATa

    Tc

    Tb Td

    Te

    Tri2BTri2A

    Tri2BTri1

    Tri2A

    P2

    Pen1

    P1

    P6

    P5

    C6

    P4

    C1E1

    E2 C5

    C4

    C2

    E5

    P3

    Triplex Ta

    Pen1

    P6P1Tri1

    Tri2BTri2A

    Tri1

    Tri2B

    P6Tri2B

    Tri1

    Tri2AP1

    P1Tri2A

    a.a. 1149-1169

    a.a. 1256-1267Tri2B

    Pen1

    a.a. 1256-1267

    a.a. 1256-1267

    a

    b

    C6

    P5

    P2

    Tri1

    Tri2BTri2A

    Triplex Tc

    Tri1

    Tri1

    Tri2B

    P2

    a.a. 1149-1169

    P2

    a.a. 1256-1267

    c

    a.a. 1149-1169missing

    Tri2A

    P5

    C6

    Tri2B

    a.a. 1256-1267

    a.a. 1256-1267

    P3

    E1

    C5

    Tri1

    Tri2BTri2A

    Triplex Tb

    dTri1Tri2B

    C5Tri1

    Tri1

    Tri2B

    Tri2A

    E1

    E1

    Tri2AP3

    Tri2B

    a.a. 1149-1169

    a.a. 1256-1267

    a.a. 1256-1267

    a.a. 1149-1169

    a.a. 1256-1267

    C5

    Tri1

    Tri2BTri2A

    Triplex Td

    E5

    C1

    P4

    C1

    C1

    Tri1

    Tri2B

    Tri1e

    a.a. 1149-1169

    a.a. 1256-1267

    E5

    E5

    Tri2A

    Tri2B

    a.a. 1149-1169

    a.a. 1256-1267

    P4

    P4Tri2A

    Tri2A

    Tri2B

    Tri1 a.a. 1149-1169

    a.a. 1256-1267

    Triplex Te

    Tri1

    Tri2BTri2A

    C2

    E2

    C4

    E2E2

    Tri1

    Tri1

    Tri2Ba.a. 1149-1169

    a.a. 1256-1267

    Tri1

    Tri2B Tri2A C4

    C4Tri2A

    a.a. 1256-1267

    a.a. 1149-1169

    a.a. 1256-1267

    Tri2BTri2A

    C2

    missing

    a.a.1149-1169

    f

    Tri1

    Tri2ATri2B

    Tri1

    Tri2ATri2B

    Tri1

    Tri1

    Tri2B

    Supplementary Figure 5. Details of plasticity of triplex interactions with MCP buttress domain shown in Figure3h,i. (A) Distribution of triplexes Ta, Tb, Tc, Td, and Te in the MCP network. (B-F) Magnified profile views of the regionssurrounding triplexes Ta (B), Tb (D), Tc (C), Td (E), and Te (F) as viewed from the outside of the capsid. Away from thecapsid floor, triplex Ta is dominantly stabilized by two long loop-containing segments (a.a. 1149-1169 and a.a. 1256-1267) from the buttress domains of P1 MCP (purple), P6 MCP (orange), and Pen1 MCP (green) (B). Tb (D), Tc (C), Td(E), and Te (F) triplexes are stabilized by their surrounding MCPs in an architecturally similar but locally different manner.

    8

    SpringerNature_NatMicro_758_ESM.pdfReferencesSfig2-only-largesize.pdfSlide Number 2