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这里对齐真实图表资产提取链路。caption_source=embedded_table_cell 表示表注来自 Docling table cell,不会出现在 text block 审计差集里;caption_continuation_used_by_asset 表示某个 text block 已被图表 caption 吸收,不应按普通 metadata 解读。
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| 2 | figure | Fig. 1 | 2 | direct_caption_ref | 0.82 | [332.68, 66.19, 221.74, 288.41] | Figure 1. Structure of as-prepared Li 2 MoO3. (a) Schematic lattice of Li2MoO3. (b) The re fi ned XRD pattern of Li2MoO3 ( λ = 0.7747 Å) using GSAS program. (c) ABF STEM image of Li2MoO3 along the [100] zone axis with Mo ions in slipped αβγ -stacking (O3 type). (d) The corresponding HAADF STEM image of part c. The bright dots represent Mo-ion column. (e) The corresponding line contrast pro fi le of the Li, Mo, and O in parts c and d along the [421 ̅ ] direction with the image contrast of dark dots in part c inverted and displayed as peaks. (f) The corresponding line contrast pro fi les of the Mo ions in part d along the marked rows. The marked black solid circle presents the much strong contrast of Mo-ion column. | ||||
| 3 | figure | Fig. 2 | 3 | direct_caption_ref | 0.82 | [65.66, 113.14, 228.85, 257.59] | Figure 2. Structural evolution of Li2MoO3 during the initial delithiation and lithiation. (a) In situ XRD patterns of Li2 -x MoO3 (0 ≤ x ≤ 2) electrodes while a Li 2 MoO3/Li cell is charged and discharged at a current density of 10 mA g -1 between 2.0 and 4.8 V. (b) Schematic structures of Li 2 -x MoO3 (0 ≤ x ≤ 2) (V representing atomic vacancy) during the initial charge and discharge process. | ||||
| 4 | figure | Fig. 3 | 3 | direct_caption_ref | 0.82 | [328.79, 188.34, 229.37, 254.46] | Figure 3. Detection of Mo-ion migration in atomic scale. (a) HAADF image of the as-prepared Li 2 MoO3 along the [100] zone axis. (c and e) HAADF images of the charged and discharged Li2MoO3 along the [1 ̅ 00] zone axis, respectively. The Mo ions at 3a and 3b sites in the HAADF images are presented with pink and yellow solid circles, respectively. (b , d , and f) Corresponding line contrast pro fi les of Mo ions along the marked rows in the HAADF images. The much strong contrast of Mo ions is marked with black solid circle in the line contrast pro fi les. | ||||
| 5 | figure | Fig. 4 | 4 | direct_caption_ref | 0.82 | [65.84, 277.25, 227.83, 284.16] | Figure 4. Charge compensation of Li2MoO3 during the initial delithiation and lithiation. (a) XANES spectra of Mo K-edge of Li2MoO3 at di ff erent delithiation and lithiation states. (b) Fouriertransformed Mo K-edge EXAFS spectra of Li2MoO3 corresponding to part a. (c) ABF imaging of Li2MoO3 at di ff erent delithiation and lithiation states showing the variation of the Mo -O distances, indicating the distortion of the MoO 6 octahedra during Li + extraction and insertion. (d) PEY mode and (e) FY mode of O K-edge soft XAS spectra of Li 2 MoO3 at di ff erent delithiation and lithiation states. | ||||
| 6 | figure | Fig. 5 | 5 | direct_caption_ref | 0.82 | [334.57, 63.57, 219.99, 172.71] | Figure 5. Structural transition of Li2MoO3 in the initial electrochemical (de)lithiation process. The lattice structure variation demonstrates that solid-solution reaction and two-phase reaction occur in consequence. |
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| 1 | 3 | text | affiliation | False | medium | front_matter_author_line | front_matter_author_line | p1:body_region:0 | p1:front_matter:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 156.08, 504.0, 32.21] | Jun Ma, † , ⊥ Yong-Ning Zhou, ‡ , ⊥ Yurui Gao, † Xiqian Yu, ‡ Qingyu Kong, * , § Lin Gu, ∥ Zhaoxiang Wang, * , † Xiao-Qing Yang, * , ‡ and Liquan Chen † | Jun Ma, † , ⊥ Yong-Ning Zhou, ‡ , ⊥ Yurui Gao, † Xiqian Yu, ‡ Qingyu Kong, * , § Lin Gu, ∥ Zhaoxiang Wang, * , † Xiao-Qing Yang, * , ‡ and Liquan Chen † | ||
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| 1 | 8 | footnote | affiliation | False | medium | first_page_author_or_affiliation | first_page_author_or_affiliation | p1:body_region:0 | p1:front_matter:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 257.79, 503.96, 24.37] | ∥ Laboratory for Advanced Materials & Electron Microscopy, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, PO Box 603, Beijing 100190, China | ∥ Laboratory for Advanced Materials & Electron Microscopy, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, PO Box 603, Beijing 100190, China | ||
| 1 | 9 | section_header | title_candidate | False | low | first_page_front_matter_heading | first_page_front_matter_heading | p1:body_region:0 | p1:front_matter:column_1_of_2:white | [255, 255, 255] white | False | [69.45, 289.17, 101.14, 12.62] | * S Supporting Information | * S Supporting Information | ||
| 1 | 10 | text | abstract_candidate | False | medium | implicit_abstract | implicit_abstract | p1:body_region:0 | p1:front_matter:front_panel:colored | [255, 247, 213] colored | False | [69.45, 315.0, 249.52, 111.16] | ABSTRACT: Layer-structured x Li2MnO3 · (1 -x )Li M O2 are promising cathode materials for high energy-density Li-ion batteries because they deliver high capacities due to the stabilizing e ff ect of Li2MnO3. However, th… | ABSTRACT: Layer-structured x Li2MnO3 · (1 -x )Li M O2 are promising cathode materials for high energy-density Li-ion batteries because they deliver high capacities due to the stabilizing e ff ect of Li2MnO3. However, th… | ||
| 1 | 11 | text | abstract_candidate | False | medium | first_page_summary | first_page_summary | p1:body_region:0 | p1:front_matter:front_panel:colored | [255, 247, 213] colored | False | [69.45, 426.58, 486.03, 55.79] | ning transmission electron microscopy clarify its lithium extraction/insertion mechanism and shows that the Mo 4+ /Mo 6+ redox couple in Li 2 MoO3 can accomplish the task of charge compensation upon Li removal. Other pr… | ning transmission electron microscopy clarify its lithium extraction/insertion mechanism and shows that the Mo 4+ /Mo 6+ redox couple in Li 2 MoO3 can accomplish the task of charge compensation upon Li removal. Other pr… | ||
| 1 | 12 | section_header | body_heading | False | low | body_heading | body_heading | p1:body_region:0 | p1:body_zone:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 496.13, 87.35, 23.65] | ■ INTRODUCTION | ■ INTRODUCTION | ||
| 1 | 13 | text | body | True | body | body | p1:body_region:0 | p1:bottom_margin:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 523.43, 240.0, 233.93] | Li-ion batteries (LIBs) have been powering most of the portable electronics for decades and are driving various types of electric vehicles nowadays. Safety, energy density, and cycle life are the essential criteria to e… | Li-ion batteries (LIBs) have been powering most of the portable electronics for decades and are driving various types of electric vehicles nowadays. Safety, energy density, and cycle life are the essential criteria to e… | |||
| 1 | 14 | page_footer | page_footer | False | low | first_page_metadata | first_page_metadata | p1:body_region:0 | p1:bottom_margin:column_1_of_2:white | [255, 255, 255] white | False | [168.49, 771.24, 95.03, 5.88] | © 2014 American Chemical Society | © 2014 American Chemical Society | ||
| 1 | 15 | text | body | True | body | body | p1:body_region:1 | p1:body_zone:column_2_of_2:white | [255, 255, 255] white | False | [324.45, 502.82, 240.04, 115.98] | surface modi fi cation, 14,15 atomic substitution, 16 -18 and optimization of synthesis strategies 19,20 have been pursued to improve the performances of the composites, complete elimination of their drawbacks related t… | surface modi fi cation, 14,15 atomic substitution, 16 -18 and optimization of synthesis strategies 19,20 have been pursued to improve the performances of the composites, complete elimination of their drawbacks related t… | |||
| 1 | 16 | text | body | True | body | body | p1:body_region:1 | p1:body_zone:column_2_of_2:white | [255, 255, 255] white | False | [324.45, 621.22, 240.01, 88.63] | Here, we propose to replace Li2MnO3 with Li2MoO3 with disordered NaFeO2 structure ( R 3 ̅ m ; a = 2.884 Å, c = 14.834 Å) 21 -24 to construct novel Li-rich x Li2MoO3 · (1 -x )Li M O2 cathodes and evaluate its feasibility… | Here, we propose to replace Li2MnO3 with Li2MoO3 with disordered NaFeO2 structure ( R 3 ̅ m ; a = 2.884 Å, c = 14.834 Å) 21 -24 to construct novel Li-rich x Li2MoO3 · (1 -x )Li M O2 cathodes and evaluate its feasibility… | |||
| 1 | 17 | text | metadata | False | low | first_page_metadata | first_page_metadata | p1:body_region:1 | p1:body_zone:column_2_of_2:white | [255, 255, 255] white | False | [367.99, 727.13, 55.06, 7.92] | March 22, 2014 | March 22, 2014 | ||
| 1 | 18 | text | metadata | False | low | first_page_metadata | first_page_metadata | p1:body_region:1 | p1:body_zone:column_2_of_2:white | [253, 253, 253] white | False | [324.45, 727.21, 34.65, 7.77] | Received: | Received: | ||
| 1 | 19 | text | metadata | False | low | first_page_metadata | first_page_metadata | p1:body_region:1 | p1:body_zone:column_2_of_2:white | [255, 255, 255] white | False | [367.99, 738.19, 49.9, 7.92] | April 30, 2014 | April 30, 2014 | ||
| 1 | 20 | text | metadata | False | low | first_page_metadata | first_page_metadata | p1:body_region:1 | p1:body_zone:column_2_of_2:white | [253, 253, 253] white | False | [324.45, 738.27, 30.25, 7.77] | Revised: | Revised: | ||
| 1 | 21 | text | metadata | False | low | first_page_metadata | first_page_metadata | p1:body_region:1 | p1:bottom_margin:column_2_of_2:white | [255, 255, 255] white | False | [367.99, 749.19, 43.83, 7.92] | May 1, 2014 | May 1, 2014 | ||
| 1 | 22 | text | metadata | False | low | first_page_metadata | first_page_metadata | p1:body_region:1 | p1:bottom_margin:column_2_of_2:white | [252, 252, 252] white | False | [324.45, 749.27, 37.75, 7.77] | Published: | Published: | ||
| 1 | 23 | page_footer | page_footer | False | low | first_page_metadata | first_page_metadata | p1:body_region:1 | p1:bottom_margin:column_2_of_2:white | [255, 255, 255] white | False | [396.06, 769.98, 168.43, 7.74] | dx.doi.org/10.1021/cm501025r | Chem. Mater. 2014, 26, 3256 -3262 | dx.doi.org/10.1021/cm501025r | Chem. Mater. 2014, 26, 3256 -3262 | ||
| 1 | 24 | page_footer | page_footer | False | low | docling_page_footer | docling_page_footer | p1:body_region:0 | p1:bottom_margin:column_2_of_2:white | [255, 255, 255] white | False | [304.5, 770.73, 15.93, 6.54] | 3256 | 3256 | ||
| 2 | 25 | page_header | page_header | False | low | docling_page_header | docling_page_header | p2:body_region:0 | p2:top_margin:column_1_of_2:gray | [241, 242, 242] gray | False | [60.49, 48.93, 98.47, 8.72] | Chemistry of Materials | Chemistry of Materials | ||
| 2 | 26 | text | body | True | body | body | p2:body_region:0 | p2:front_matter:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 69.37, 240.01, 372.97] | in Li2MoO3 can exchange multiple electrons and supply a theoretical capacity up to 339 mAh g -1 . (2) Our fi rst-principles calculations indicate that Mo doping delays the oxygen release (i.e., oxygen evolution occurs o… | in Li2MoO3 can exchange multiple electrons and supply a theoretical capacity up to 339 mAh g -1 . (2) Our fi rst-principles calculations indicate that Mo doping delays the oxygen release (i.e., oxygen evolution occurs o… | |||
| 2 | 27 | section_header | body_heading | False | low | body_heading | body_heading | p2:body_region:0 | p2:body_zone:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 442.33, 139.52, 23.65] | ■ RESULTS AND DISCUSSION | ■ RESULTS AND DISCUSSION | ||
| 2 | 28 | text | body | True | body | body | p2:body_region:0 | p2:body_zone:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 467.95, 239.99, 152.21] | Structure of As-Prepared Li2MoO3. The re fi ned XRD pattern of the as-prepared Li2MoO3 powder matches well with the α -NaFeO2 structure R 3 ̅ m with lattice constants a = 2.8675(9) Å and c = 14.8357(6) Å (Figure 1a and … | Structure of As-Prepared Li2MoO3. The re fi ned XRD pattern of the as-prepared Li2MoO3 powder matches well with the α -NaFeO2 structure R 3 ̅ m with lattice constants a = 2.8675(9) Å and c = 14.8357(6) Å (Figure 1a and … | |||
| 2 | 29 | text | body | True | body | body | p2:body_region:0 | p2:bottom_margin:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 622.36, 240.0, 140.84] | It is worthwhile to point out that the contrast of the highangle annular-dark- fi eld (HAADF) image exhibits a Z 1.7 dependence as compared with Z 1/3 for the annular-brightfi eld (ABF) image with respect to the atomic … | It is worthwhile to point out that the contrast of the highangle annular-dark- fi eld (HAADF) image exhibits a Z 1.7 dependence as compared with Z 1/3 for the annular-brightfi eld (ABF) image with respect to the atomic … | |||
| 2 | 30 | page_header | page_header | False | low | docling_page_header | docling_page_header | p2:body_region:1 | p2:top_margin:column_2_of_2:gray | [88, 89, 91] gray | True | [536.2, 49.99, 21.22, 7.35] | Article | Article | ||
| 2 | 31 | caption | caption | False | low | outside_body_flow_caption | outside_body_flow_caption | p2:body_region:1 | p2:front_matter:column_2_of_2:white | [255, 255, 255] white | False | [324.45, 364.64, 240.03, 107.93] | Figure 1. Structure of as-prepared Li 2 MoO3. (a) Schematic lattice of Li2MoO3. (b) The re fi ned XRD pattern of Li2MoO3 ( λ = 0.7747 Å) using GSAS program. (c) ABF STEM image of Li2MoO3 along the [100] zone axis with M… | Figure 1. Structure of as-prepared Li 2 MoO3. (a) Schematic lattice of Li2MoO3. (b) The re fi ned XRD pattern of Li2MoO3 ( λ = 0.7747 Å) using GSAS program. (c) ABF STEM image of Li2MoO3 along the [100] zone axis with M… | ||
| 2 | 32 | text | body | True | body | body | p2:body_region:1 | p2:body_zone:column_2_of_2:white | [255, 255, 255] white | False | [324.45, 488.15, 240.02, 100.18] | columns show an αβγ -stacking with an irregular shift along the [010] direction (slipped O3 type; Supporting Information Figure S3), due to the presence of disordered Mo3O13 clusters in the Li -Mo layers (Supporting Inf… | columns show an αβγ -stacking with an irregular shift along the [010] direction (slipped O3 type; Supporting Information Figure S3), due to the presence of disordered Mo3O13 clusters in the Li -Mo layers (Supporting Inf… | |||
| 2 | 33 | text | body | True | body | body | p2:body_region:1 | p2:bottom_margin:column_2_of_2:white | [255, 255, 255] white | False | [324.45, 588.93, 240.03, 174.27] | Structural Transition and Mo-Ion Migration. Irreversible migration of the Mn ions into the transition metal layer to fi ll out the Li vacancies (a proposed layer-to-spinel transition) has been reported to be one of the … | Structural Transition and Mo-Ion Migration. Irreversible migration of the Mn ions into the transition metal layer to fi ll out the Li vacancies (a proposed layer-to-spinel transition) has been reported to be one of the … | |||
| 2 | 34 | page_footer | page_footer | False | low | docling_page_footer | docling_page_footer | p2:body_region:1 | p2:bottom_margin:column_2_of_2:white | [255, 255, 255] white | False | [396.06, 773.27, 168.43, 7.74] | dx.doi.org/10.1021/cm501025r | Chem. Mater. 2014, 26, 3256 -3262 | dx.doi.org/10.1021/cm501025r | Chem. Mater. 2014, 26, 3256 -3262 | ||
| 2 | 35 | page_footer | page_footer | False | low | docling_page_footer | docling_page_footer | p2:bottom_margin:column_2_of_2:white | [255, 255, 255] white | False | [304.5, 774.02, 15.93, 6.54] | 3257 | 3257 | |||
| 3 | 36 | page_header | page_header | False | low | docling_page_header | docling_page_header | p3:body_region:0 | p3:top_margin:column_1_of_2:gray | [241, 242, 242] gray | False | [60.49, 48.93, 98.47, 8.72] | Chemistry of Materials | Chemistry of Materials | ||
| 3 | 37 | text | body | True | body | body | p3:body_region:0 | p3:page_body:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 69.37, 240.0, 30.8] | In order to investigate the structural changes of Li2MoO3 during electrochemical (de)lithiation between 2.0 and 4.8 V, in situ XRD characterization was performed (Figure 2a and | In order to investigate the structural changes of Li2MoO3 during electrochemical (de)lithiation between 2.0 and 4.8 V, in situ XRD characterization was performed (Figure 2a and | |||
| 3 | 38 | caption | caption | False | low | outside_body_flow_caption | outside_body_flow_caption | p3:body_region:0 | p3:page_body:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 381.99, 240.01, 57.93] | Figure 2. Structural evolution of Li2MoO3 during the initial delithiation and lithiation. (a) In situ XRD patterns of Li2 -x MoO3 (0 ≤ x ≤ 2) electrodes while a Li 2 MoO3/Li cell is charged and discharged at a current d… | Figure 2. Structural evolution of Li2MoO3 during the initial delithiation and lithiation. (a) In situ XRD patterns of Li2 -x MoO3 (0 ≤ x ≤ 2) electrodes while a Li 2 MoO3/Li cell is charged and discharged at a current d… | ||
| 3 | 39 | text | back_matter_heading | False | low | back_matter_heading | back_matter_heading | stop_trigger | p3:body_region:0 | p3:page_body:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 457.38, 239.95, 41.8] | Supporting Information Figure S9). Before the cell is charged to ca. 3.1 V, a solid-solution reaction occurs with negligible variation of cell parameters (Li2MoO3 → Li1.75MoO3 + 0.25Li + ). | Supporting Information Figure S9). Before the cell is charged to ca. 3.1 V, a solid-solution reaction occurs with negligible variation of cell parameters (Li2MoO3 → Li1.75MoO3 + 0.25Li + ). | |
| 3 | 40 | text | body_candidate_excluded | False | medium | after_back_matter_stop | after_back_matter_stop | after_stop | p3:body_region:0 | p3:page_body:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 501.37, 240.04, 206.83] | As the cell is further charged to ca. 3.6 V, the (003) di ff raction peak shifts to lower angles and gradually becomes broader. Meanwhile, the intensities of the other peaks indexed to Li2MoO3 decrease while those of ne… | As the cell is further charged to ca. 3.6 V, the (003) di ff raction peak shifts to lower angles and gradually becomes broader. Meanwhile, the intensities of the other peaks indexed to Li2MoO3 decrease while those of ne… | |
| 3 | 41 | text | body_candidate_excluded | False | medium | after_back_matter_stop | after_back_matter_stop | after_stop | p3:body_region:0 | p3:bottom_margin:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 710.4, 239.96, 53.96] | In the subsequent Li-ion insertion process, these di ff raction peaks keep unchanged at fi rst (Li0.53MoO3 + 0.44Li + → Li 0.97 MoO3) and then continuously shift to higher di ff raction angles very close to that of Li2M… | In the subsequent Li-ion insertion process, these di ff raction peaks keep unchanged at fi rst (Li0.53MoO3 + 0.44Li + → Li 0.97 MoO3) and then continuously shift to higher di ff raction angles very close to that of Li2M… | |
| 3 | 42 | page_header | page_header | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p3:body_region:1 | p3:top_margin:column_2_of_2:gray | [88, 89, 91] gray | True | [536.2, 49.99, 21.22, 7.35] | Article | Article | |
| 3 | 43 | text | body_candidate_excluded | False | medium | after_back_matter_stop | after_back_matter_stop | after_stop | p3:body_region:1 | p3:page_body:column_2_of_2:white | [255, 255, 255] white | False | [324.45, 69.37, 240.02, 63.8] | with Li-ion insertion. Interestingly, the insertion of Li ions to Li0.53MoO3 and Li0.97MoO3 seems to be a solid-solution reaction, di ff erent from that in the charge process. These indicate that the structure of Li2MoO… | with Li-ion insertion. Interestingly, the insertion of Li ions to Li0.53MoO3 and Li0.97MoO3 seems to be a solid-solution reaction, di ff erent from that in the charge process. These indicate that the structure of Li2MoO… | |
| 3 | 44 | text | body_candidate_excluded | False | medium | after_back_matter_stop | after_back_matter_stop | after_stop | p3:body_region:1 | p3:page_body:column_2_of_2:white | [255, 255, 255] white | False | [324.45, 135.36, 240.0, 41.8] | STEM HAADF images of Li2MoO3 at di ff erent states in the fi rst charge and discharge processes were recorded to check the Mo-ion migration and the resultant structural transition during Li-ion insertion/extraction at t… | STEM HAADF images of Li2MoO3 at di ff erent states in the fi rst charge and discharge processes were recorded to check the Mo-ion migration and the resultant structural transition during Li-ion insertion/extraction at t… | |
| 3 | 45 | caption | caption | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p3:body_region:1 | p3:page_body:column_2_of_2:white | [255, 255, 255] white | False | [324.45, 452.29, 240.02, 87.92] | Figure 3. Detection of Mo-ion migration in atomic scale. (a) HAADF image of the as-prepared Li 2 MoO3 along the [100] zone axis. (c and e) HAADF images of the charged and discharged Li2MoO3 along the [1 ̅ 00] zone axis,… | Figure 3. Detection of Mo-ion migration in atomic scale. (a) HAADF image of the as-prepared Li 2 MoO3 along the [100] zone axis. (c and e) HAADF images of the charged and discharged Li2MoO3 along the [1 ̅ 00] zone axis,… | |
| 3 | 46 | text | back_matter_heading | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p3:body_region:1 | p3:page_body:column_2_of_2:white | [255, 255, 255] white | False | [324.45, 553.0, 240.01, 133.16] | Supporting Information Figure S12 -S15). After Li-ion extraction, the Mo ions migrate from 3b to 3a sites, implying the disaggregation of the Mo3O13 clusters. As a result, the atoms in the 3b and 3a sites have similar c… | Supporting Information Figure S12 -S15). After Li-ion extraction, the Mo ions migrate from 3b to 3a sites, implying the disaggregation of the Mo3O13 clusters. As a result, the atoms in the 3b and 3a sites have similar c… | |
| 3 | 47 | text | body_candidate_excluded | False | medium | after_back_matter_stop | after_back_matter_stop | after_stop | p3:body_region:1 | p3:bottom_margin:column_2_of_2:white | [255, 255, 255] white | False | [324.45, 688.4, 239.99, 75.96] | Phase transformation from faulted O1 type to O3 type seems to be the way that requires the lowest energy to bear the stress induced by the Li-ion insertion. The Mo -Mo distances parallel and vertical to the c axis are s… | Phase transformation from faulted O1 type to O3 type seems to be the way that requires the lowest energy to bear the stress induced by the Li-ion insertion. The Mo -Mo distances parallel and vertical to the c axis are s… | |
| 3 | 48 | page_footer | page_footer | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p3:body_region:1 | p3:bottom_margin:column_2_of_2:white | [255, 255, 255] white | False | [396.06, 773.27, 168.43, 7.74] | dx.doi.org/10.1021/cm501025r | Chem. Mater. 2014, 26, 3256 -3262 | dx.doi.org/10.1021/cm501025r | Chem. Mater. 2014, 26, 3256 -3262 | |
| 3 | 49 | page_footer | page_footer | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p3:bottom_margin:column_2_of_2:white | [255, 255, 255] white | False | [304.5, 774.02, 15.93, 6.54] | 3258 | 3258 | ||
| 4 | 50 | page_header | page_header | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p4:body_region:0 | p4:top_margin:column_1_of_2:gray | [241, 242, 242] gray | False | [60.49, 48.93, 98.47, 8.72] | Chemistry of Materials | Chemistry of Materials | |
| 4 | 51 | text | body_candidate_excluded | False | medium | after_back_matter_stop | after_back_matter_stop | after_stop | p4:body_region:0 | p4:page_body:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 69.37, 239.97, 87.01] | The di ff erence between surface and bulk might be originated from the inhomogeneous insertion of the Li ions. Therefore, the partially reversible migration of the Mo ions and the partial recovery of the Mo3O13 clusters… | The di ff erence between surface and bulk might be originated from the inhomogeneous insertion of the Li ions. Therefore, the partially reversible migration of the Mo ions and the partial recovery of the Mo3O13 clusters… | |
| 4 | 52 | text | body_candidate_excluded | False | medium | after_back_matter_stop | after_back_matter_stop | after_stop | p4:body_region:0 | p4:page_body:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 156.93, 239.99, 108.28] | Extra Electron Donor and Charge Compensation. Oxygen release occurs in the fi rst (few) cycle(s) of x Li2MnO3 · (1 -x )Li M O2 because the Mn 4+ ions in Li2MnO3 cannot be further oxidized. O 2 -ions are the single elect… | Extra Electron Donor and Charge Compensation. Oxygen release occurs in the fi rst (few) cycle(s) of x Li2MnO3 · (1 -x )Li M O2 because the Mn 4+ ions in Li2MnO3 cannot be further oxidized. O 2 -ions are the single elect… | |
| 4 | 53 | caption | caption | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p4:body_region:0 | p4:page_body:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 571.0, 239.97, 88.99] | Figure 4. Charge compensation of Li2MoO3 during the initial delithiation and lithiation. (a) XANES spectra of Mo K-edge of Li2MoO3 at di ff erent delithiation and lithiation states. (b) Fouriertransformed Mo K-edge EXAF… | Figure 4. Charge compensation of Li2MoO3 during the initial delithiation and lithiation. (a) XANES spectra of Mo K-edge of Li2MoO3 at di ff erent delithiation and lithiation states. (b) Fouriertransformed Mo K-edge EXAF… | |
| 4 | 54 | text | body_candidate_excluded | False | medium | after_back_matter_stop | after_back_matter_stop | after_stop | p4:body_region:0 | p4:bottom_margin:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 677.35, 239.99, 87.01] | spectra (XANES) of Mo K-edge at various states. The absorption edges shift to higher energy during charge. Using the reference spectra of MoO2 and MoO3 (Supporting Information Figure S16), the valence state of Mo is est… | spectra (XANES) of Mo K-edge at various states. The absorption edges shift to higher energy during charge. Using the reference spectra of MoO2 and MoO3 (Supporting Information Figure S16), the valence state of Mo is est… | |
| 4 | 55 | page_header | page_header | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p4:body_region:1 | p4:top_margin:column_2_of_2:gray | [88, 89, 91] gray | True | [536.2, 49.99, 21.22, 7.35] | Article | Article | |
| 4 | 56 | text | unknown_text | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p4:body_region:1 | p4:page_body:column_2_of_2:white | [255, 255, 255] white | False | [324.45, 69.37, 239.96, 30.92] | the MoO6 octahedrons in the Mo3O13 clusters and other parts of the as-prepared Li2MoO3 become more and more distorted with increasing Li removal. | the MoO6 octahedrons in the Mo3O13 clusters and other parts of the as-prepared Li2MoO3 become more and more distorted with increasing Li removal. | |
| 4 | 57 | text | body_candidate_excluded | False | medium | after_back_matter_stop | after_back_matter_stop | after_stop | p4:body_region:1 | p4:page_body:column_2_of_2:white | [255, 255, 255] white | False | [324.45, 102.48, 240.04, 163.52] | In the discharge process, however, the absorption edges shift back to lower energy but do not return to their original positions, suggesting that the Mo ions are reduced during Liion insertion, but their average valence… | In the discharge process, however, the absorption edges shift back to lower energy but do not return to their original positions, suggesting that the Mo ions are reduced during Liion insertion, but their average valence… | |
| 4 | 58 | text | body_candidate_excluded | False | medium | after_back_matter_stop | after_back_matter_stop | after_stop | p4:body_region:1 | p4:page_body:column_2_of_2:white | [255, 255, 255] white | False | [324.45, 268.2, 240.02, 119.36] | Two dominant peaks can be observed in the Mo K-edge FTEXAFS spectrum of the as-prepared Li2MoO3 (Figure 4b). The peak at R ∼ 1.6 Å belongs to the Mo -O bond in the nearest MoO6 octahedra while the peak at R ∼ 2.3 Å is a… | Two dominant peaks can be observed in the Mo K-edge FTEXAFS spectrum of the as-prepared Li2MoO3 (Figure 4b). The peak at R ∼ 1.6 Å belongs to the Mo -O bond in the nearest MoO6 octahedra while the peak at R ∼ 2.3 Å is a… | |
| 4 | 59 | text | body_candidate_excluded | False | medium | after_back_matter_stop | after_back_matter_stop | after_stop | p4:body_region:1 | p4:page_body:column_2_of_2:white | [255, 255, 255] white | False | [324.45, 386.38, 240.04, 166.89] | The length of the Mo -O bond increases slightly but that of the Mo -Mo bond does not change at all when the material is charged to 3.6 V. When it is charged to 4.8 V, the Mo -O peak splits into two at around 1.3 and 1.7… | The length of the Mo -O bond increases slightly but that of the Mo -Mo bond does not change at all when the material is charged to 3.6 V. When it is charged to 4.8 V, the Mo -O peak splits into two at around 1.3 and 1.7… | |
| 4 | 60 | text | body_candidate_excluded | False | medium | after_back_matter_stop | after_back_matter_stop | after_stop | p4:body_region:1 | p4:bottom_margin:column_2_of_2:white | [255, 255, 255] white | False | [324.45, 552.09, 240.04, 211.05] | After discharged to 2.5 V, the two Mo -O peaks of the charged sample move toward each other. Meanwhile, the intensity of the Mo(3b)-Mo(3b) peak increases, implying that the severely distorted MoO6 octahedra are changed … | After discharged to 2.5 V, the two Mo -O peaks of the charged sample move toward each other. Meanwhile, the intensity of the Mo(3b)-Mo(3b) peak increases, implying that the severely distorted MoO6 octahedra are changed … | |
| 4 | 61 | page_footer | page_footer | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p4:body_region:1 | p4:bottom_margin:column_2_of_2:white | [255, 255, 255] white | False | [396.06, 773.27, 168.43, 7.74] | dx.doi.org/10.1021/cm501025r | Chem. Mater. 2014, 26, 3256 -3262 | dx.doi.org/10.1021/cm501025r | Chem. Mater. 2014, 26, 3256 -3262 | |
| 4 | 62 | page_footer | page_footer | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p4:bottom_margin:column_2_of_2:white | [255, 255, 255] white | False | [304.5, 774.02, 15.93, 6.54] | 3259 | 3259 | ||
| 5 | 63 | page_header | page_header | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p5:body_region:0 | p5:top_margin:column_1_of_2:gray | [241, 242, 242] gray | False | [60.49, 48.93, 98.47, 8.72] | Chemistry of Materials | Chemistry of Materials | |
| 5 | 64 | text | body_candidate_excluded | False | medium | after_back_matter_stop | after_back_matter_stop | after_stop | p5:body_region:0 | p5:page_body:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 69.37, 240.01, 307.12] | The oxygen species play an important role in the safety and structural stability of the Li-rich layered materials. 2,12,13 Irreversible oxygen evolution in the fi rst (few) cycle(s) results in safety hazard and structur… | The oxygen species play an important role in the safety and structural stability of the Li-rich layered materials. 2,12,13 Irreversible oxygen evolution in the fi rst (few) cycle(s) results in safety hazard and structur… | |
| 5 | 65 | text | body_candidate_excluded | False | medium | after_back_matter_stop | after_back_matter_stop | after_stop | p5:body_region:0 | p5:page_body:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 378.75, 240.0, 163.46] | In the lithiation process, the intensity of the 535.6 eV peak decreases slightly, indicating that the charge compensation from oxygen is partially reversible. In contrast, the XAS spectra in the FY mode, which mainly gi… | In the lithiation process, the intensity of the 535.6 eV peak decreases slightly, indicating that the charge compensation from oxygen is partially reversible. In contrast, the XAS spectra in the FY mode, which mainly gi… | |
| 5 | 66 | text | body_candidate_excluded | False | medium | after_back_matter_stop | after_back_matter_stop | after_stop | p5:body_region:0 | p5:bottom_margin:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 544.03, 240.01, 219.17] | (De)lithiation Mechanism. Based on the above comprehensive XRD, STEM, and XAS studies of Li2MoO3 at various charge/discharge states, a possible phase transition diagram of Li 2 -x MoO3 (0 ≤ x ≤ 1.47) can be drawn (Figur… | (De)lithiation Mechanism. Based on the above comprehensive XRD, STEM, and XAS studies of Li2MoO3 at various charge/discharge states, a possible phase transition diagram of Li 2 -x MoO3 (0 ≤ x ≤ 1.47) can be drawn (Figur… | |
| 5 | 67 | page_header | page_header | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p5:body_region:1 | p5:top_margin:column_2_of_2:gray | [88, 89, 91] gray | True | [536.2, 49.99, 21.22, 7.35] | Article | Article | |
| 5 | 68 | caption | caption | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p5:body_region:1 | p5:page_body:column_2_of_2:white | [255, 255, 255] white | False | [324.45, 246.09, 240.04, 37.92] | Figure 5. Structural transition of Li2MoO3 in the initial electrochemical (de)lithiation process. The lattice structure variation demonstrates that solid-solution reaction and two-phase reaction occur in consequence. | Figure 5. Structural transition of Li2MoO3 in the initial electrochemical (de)lithiation process. The lattice structure variation demonstrates that solid-solution reaction and two-phase reaction occur in consequence. | |
| 5 | 69 | text | body_candidate_excluded | False | medium | after_back_matter_stop | after_back_matter_stop | after_stop | p5:body_region:1 | p5:page_body:column_2_of_2:white | [255, 255, 255] white | False | [324.45, 299.98, 240.02, 111.22] | solution reaction of Li 2 -x MoO3 (1.25 ≤ x ≤ 1.47) with increasing Li vacancies, the MoO6 octahedron distortion and Mo-ion interlayer migration. In the discharge process (Regions IV and V), solid-solution reaction of L… | solution reaction of Li 2 -x MoO3 (1.25 ≤ x ≤ 1.47) with increasing Li vacancies, the MoO6 octahedron distortion and Mo-ion interlayer migration. In the discharge process (Regions IV and V), solid-solution reaction of L… | |
| 5 | 70 | text | body_candidate_excluded | False | medium | after_back_matter_stop | after_back_matter_stop | after_stop | p5:body_region:1 | p5:page_body:column_2_of_2:white | [255, 255, 255] white | False | [324.45, 413.39, 240.02, 151.78] | Although further experimental and theoretical studies are required to fi nd out more details of the phase transitions during the initial and the subsequent cycles, such as the paths of the Liion di ff usion and the Mo-i… | Although further experimental and theoretical studies are required to fi nd out more details of the phase transitions during the initial and the subsequent cycles, such as the paths of the Liion di ff usion and the Mo-i… | |
| 5 | 71 | text | body_candidate_excluded | False | medium | after_back_matter_stop | after_back_matter_stop | after_stop | p5:body_region:1 | p5:bottom_margin:column_2_of_2:white | [255, 255, 255] white | False | [324.45, 567.36, 240.02, 197.0] | It is the irreversible oxygen release and the transition metal migration in highly delithiated Li2MnO3 that lead to its irreversible structural transition and capacity loss. Di ff erent from that, introduction of the Mo… | It is the irreversible oxygen release and the transition metal migration in highly delithiated Li2MnO3 that lead to its irreversible structural transition and capacity loss. Di ff erent from that, introduction of the Mo… | |
| 5 | 72 | page_footer | page_footer | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p5:body_region:1 | p5:bottom_margin:column_2_of_2:white | [255, 255, 255] white | False | [396.06, 773.27, 168.43, 7.74] | dx.doi.org/10.1021/cm501025r | Chem. Mater. 2014, 26, 3256 -3262 | dx.doi.org/10.1021/cm501025r | Chem. Mater. 2014, 26, 3256 -3262 | |
| 5 | 73 | page_footer | page_footer | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p5:bottom_margin:column_2_of_2:white | [254, 254, 254] white | False | [304.5, 774.02, 15.93, 6.54] | 3260 | 3260 | ||
| 6 | 74 | page_header | page_header | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p6:body_region:0 | p6:top_margin:column_1_of_2:gray | [241, 242, 242] gray | False | [60.49, 48.93, 98.47, 8.72] | Chemistry of Materials | Chemistry of Materials | |
| 6 | 75 | text | body_candidate_excluded | False | medium | after_back_matter_stop | after_back_matter_stop | after_stop | p6:body_region:0 | p6:front_matter:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 69.37, 239.98, 53.7] | and Li2MoO3-based cathode materials do not need to be charged to such high (4.8 V) potentials. In that case, the reversibility of the Mo-ion migration and O 2 --ion oxidation, structural stability and the compatibility … | and Li2MoO3-based cathode materials do not need to be charged to such high (4.8 V) potentials. In that case, the reversibility of the Mo-ion migration and O 2 --ion oxidation, structural stability and the compatibility … | |
| 6 | 76 | section_header | body_heading | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p6:body_region:0 | p6:body_zone:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 127.63, 77.3, 23.65] | ■ CONCLUSION | ■ CONCLUSION | |
| 6 | 77 | text | body_candidate_excluded | False | medium | after_back_matter_stop | after_back_matter_stop | after_stop | p6:body_region:0 | p6:body_zone:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 154.87, 240.0, 345.62] | In summary, comprehensive in situ XRD and ex situ STEM and XAS studies clarify the electrochemical (de)lithiation mechanism of Li2MoO3 and prove the feasibility of replacing Li 2 MnO3 with its iso-structured Li2MoO3 to … | In summary, comprehensive in situ XRD and ex situ STEM and XAS studies clarify the electrochemical (de)lithiation mechanism of Li2MoO3 and prove the feasibility of replacing Li 2 MnO3 with its iso-structured Li2MoO3 to … | |
| 6 | 78 | section_header | unknown_text | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p6:body_region:0 | p6:body_zone:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 504.98, 121.71, 23.65] | ■ ASSOCIATED CONTENT | ■ ASSOCIATED CONTENT | |
| 6 | 79 | section_header | unknown_text | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p6:body_region:0 | p6:body_zone:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 530.62, 113.35, 12.62] | * S Supporting Information | * S Supporting Information | |
| 6 | 80 | text | body_heading | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p6:body_region:0 | p6:body_zone:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 545.48, 239.99, 87.38] | Experimental section, re fi ned structural parameters, SEM images of the as-prepared Li2MoO3, its electrochemical performance, the original STEM images and the corresponding charge/discharge potential pro fi les of Li2M… | Experimental section, re fi ned structural parameters, SEM images of the as-prepared Li2MoO3, its electrochemical performance, the original STEM images and the corresponding charge/discharge potential pro fi les of Li2M… | |
| 6 | 81 | section_header | unknown_text | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p6:body_region:0 | p6:body_zone:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 637.35, 125.07, 23.65] | ■ AUTHOR INFORMATION | ■ AUTHOR INFORMATION | |
| 6 | 82 | section_header | metadata | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p6:body_region:0 | p6:body_zone:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 665.18, 97.03, 8.29] | Corresponding Authors | Corresponding Authors | |
| 6 | 83 | text | metadata | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p6:body_region:0 | p6:body_zone:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 674.48, 107.39, 12.07] | * Email: zxwang@iphy.ac.cn. | * Email: zxwang@iphy.ac.cn. | |
| 6 | 84 | text | metadata | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p6:body_region:0 | p6:body_zone:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 685.47, 94.61, 12.07] | * Email: xyang@bn-l.gov. | * Email: xyang@bn-l.gov. | |
| 6 | 85 | text | metadata | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p6:body_region:0 | p6:body_zone:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 696.47, 107.28, 12.07] | * Email: qkong@aps.anl.gov. | * Email: qkong@aps.anl.gov. | |
| 6 | 86 | section_header | back_matter_heading | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p6:body_region:0 | p6:body_zone:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 714.33, 88.22, 8.29] | Author Contributions | Author Contributions | |
| 6 | 87 | text | unknown_text | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p6:body_region:0 | p6:body_zone:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 722.45, 198.07, 13.43] | ⊥ J.M. and Y.-N.Z. contributed equally to this work. | ⊥ J.M. and Y.-N.Z. contributed equally to this work. | |
| 6 | 88 | section_header | unknown_text | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p6:body_region:0 | p6:body_zone:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 741.66, 23.72, 8.29] | Notes | Notes | |
| 6 | 89 | text | unknown_text | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p6:body_region:0 | p6:bottom_margin:column_1_of_2:white | [255, 255, 255] white | False | [60.49, 754.4, 201.38, 8.8] | The authors declare no competing fi nancial interest. | The authors declare no competing fi nancial interest. | |
| 6 | 90 | page_header | page_header | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p6:body_region:1 | p6:top_margin:column_2_of_2:gray | [88, 89, 91] gray | True | [536.2, 49.99, 21.22, 7.35] | Article | Article | |
| 6 | 91 | section_header | back_matter_heading | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p6:body_region:1 | p6:top_margin:column_2_of_2:white | [255, 255, 255] white | False | [324.45, 58.18, 114.79, 23.65] | ■ ACKNOWLEDGMENTS | ■ ACKNOWLEDGMENTS | |
| 6 | 92 | text | back_matter_text | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p6:body_region:1 | p6:front_matter:column_2_of_2:white | [255, 255, 255] white | False | [324.45, 84.97, 240.02, 111.02] | This work was fi nancially supported by the National Natural Science Foundation of China (NSFC No. 51372268) and the National 973 Program of China (2009CB220100). The work at Brookhaven National Laboratory was supported… | This work was fi nancially supported by the National Natural Science Foundation of China (NSFC No. 51372268) and the National 973 Program of China (2009CB220100). The work at Brookhaven National Laboratory was supported… | |
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| 7 | 131 | text | affiliation | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p7:page_body:left_crossing:white | [255, 255, 255] white | False | [64.46, 198.99, 236.0, 7.92] | (34) Findlay, S. D.; Shibata, N.; Sawada, H.; Okunishi, E.; Kondo, Y.; | (34) Findlay, S. D.; Shibata, N.; Sawada, H.; Okunishi, E.; Kondo, Y.; | ||
| 7 | 132 | text | unknown_text | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p7:page_body:left:white | [255, 255, 255] white | False | [60.49, 209.02, 89.66, 7.92] | Yamanoto, T.; Ikuhara, Y. | Yamanoto, T.; Ikuhara, Y. | ||
| 7 | 133 | text | unknown_text | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p7:page_body:left:white | [255, 255, 255] white | False | [153.19, 209.04, 54.26, 7.88] | Appl. Phys. Lett. | Appl. Phys. Lett. | ||
| 7 | 134 | text | unknown_text | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p7:page_body:left:white | [255, 255, 255] white | False | [210.45, 209.1, 17.6, 7.77] | 2009 | 2009 | ||
| 7 | 135 | text | unknown_text | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p7:page_body:left:white | [255, 255, 255] white | False | [228.08, 209.02, 1.77, 7.92] | , | |||
| 7 | 136 | text | unknown_text | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p7:page_body:left:white | [255, 255, 255] white | False | [232.9, 209.04, 8.42, 7.88] | 95 | 95 | ||
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| 7 | 146 | list_item | reference | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p7:page_body:left_crossing:white | [255, 255, 255] white | False | [60.49, 419.01, 239.97, 38.57] | Scanlon, D. O.; Watson, G. W.; Payne, D. J.; Atkinson, G. R.; Egdel, R. G.; Law, D. S. L. J. Phys. Chem. C 2010 , 114 , 4636 -4645. (44) Lu, Y.-C.; Kwabi, D. G.; Yao, K. P. C.; Harding, J. R.; Zhou, J. G.; Zuin, L.; Sha… | Scanlon, D. O.; Watson, G. W.; Payne, D. J.; Atkinson, G. R.; Egdel, R. G.; Law, D. S. L. J. Phys. Chem. C 2010 , 114 , 4636 -4645. (44) Lu, Y.-C.; Kwabi, D. G.; Yao, K. P. C.; Harding, J. R.; Zhou, J. G.; Zuin, L.; Sha… | ||
| 7 | 147 | page_footer | page_footer | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p7:bottom_margin:left_crossing:white | [255, 255, 255] white | False | [304.5, 774.02, 15.93, 6.54] | 3262 | 3262 | ||
| 7 | 148 | page_footer | page_footer | False | low | after_back_matter_stop | after_back_matter_stop | after_stop | p7:bottom_margin:right:white | [255, 255, 255] white | False | [396.06, 773.27, 168.43, 7.74] | dx.doi.org/10.1021/cm501025r | Chem. Mater. 2014, 26, 3256 -3262 | dx.doi.org/10.1021/cm501025r | Chem. Mater. 2014, 26, 3256 -3262 |