44:
35:
219:
146:
493:: 13 million percent resistance increase in a magnetic field of 60 tesla at 0.5 kelvin. The resistance is proportional to the square of the magnetic field and shows no saturation. This may be due to the material being the first example of a compensated semimetal, in which the number of mobile holes is the same as the number of electrons. Tungsten ditelluride has layered structure, similar to many other
434:
1001:
Sie, Edbert J.; Nyby, Clara M.; Pemmaraju, C. D.; Park, Su Ji; Shen, Xiaozhe; Yang, Jie; Hoffmann, Matthias C.; Ofori-Okai, B. K.; Li, Renkai; Reid, Alexander H.; Weathersby, Stephen; Mannebach, Ehren; Finney, Nathan; Rhodes, Daniel; Chenet, Daniel; Antony, Abhinandan; Balicas, Luis; Hone, James;
1237:
Tang, Shujie; Zhang, Chaofan; Wong, Dillon; Pedramrazi, Zahra; Tsai, Hsin-Zon; Jia, Chunjing; Moritz, Brian; Claassen, Martin; Ryu, Hyejin; Kahn, Salman; Jiang, Juan; Yan, Hao; Hashimoto, Makoto; Lu, Donghui; Moore, Robert G.; Hwang, Chan-Cuk; Hwang, Choongyu; Hussain, Zahid; Chen, Yulin; Ugeda,
559:
instead acts like an insulator but with an offset current independent of doping by a local electrostatic gate. When using a contact geometry that shorted out conduction along the device edges, this offset current vanished, demonstrating that this nearly quantized conduction was localized to the
1291:
Cucchi, Irène; Gutiérrez-Lezama, Ignacio; Cappelli, Edoardo; McKeown Walker, Siobhan; Bruno, Flavio Y.; Tenasini, Giulia; Wang, Lin; Ubrig, Nicolas; Barreteau, Céline; Giannini, Enrico; Gibertini, Marco; Tamai, Anna; Morpurgo, Alberto F.; Baumberger, Felix (9 January 2019). "Microfocus
1420:
Sajadi, Ebrahim; Palomaki, Tauno; Fei, Zaiyao; Zhao, Wenjin; Bement, Philip; Olsen, Christian; Luescher, Silvia; Xu, Xiaodong; Folk, Joshua A.; Cobden, David H. (23 November 2018). "Gate-induced superconductivity in a monolayer topological insulator".
1175:
Wu, Sanfeng; Fatemi, Valla; Gibson, Quinn D.; Watanabe, Kenji; Taniguchi, Takashi; Cava, Robert J.; Jarillo-Herrero, Pablo (5 January 2018). "Observation of the quantum spin Hall effect up to 100 kelvin in a monolayer crystal".
568:. Identical measurements with two- and three-layer thick samples showed the expected semimetallic response. Subsequent studies using other techniques have been consistent with the transport results, including those using
587:, simultaneously hosting metallic behavior and switchable electric polarization. The polarization was theorized to originate from vertical charge transfer between the layers, which is switched by interlayer sliding.
1482:
Fei, Zaiyao; Zhao, Wenjin; Palomaki, Tauno A.; Sun, Bosong; Miller, Moira K.; Zhao, Zhiying; Yan, Jiaqiang; Xu, Xiaodong; Cobden, David H. (August 2018). "Ferroelectric switching of a two-dimensional metal".
1122:
Fei, Zaiyao; Palomaki, Tauno; Wu, Sanfeng; Zhao, Wenjin; Cai, Xinghan; Sun, Bosong; Nguyen, Paul; Finney, Joseph; Xu, Xiaodong; Cobden, David H. (July 2017). "Edge conduction in monolayer WTe2".
516:
is reduced. Above the pressure of 10.5 GPa magnetoresistance disappears and the material becomes a superconductor. At 13.0 GPa the transition to superconductivity happens below 6.5 K.
43:
1353:
Shi, Yanmeng; Kahn, Joshua; Niu, Ben; Fei, Zaiyao; Sun, Bosong; Cai, Xinghan; Francisco, Brian A.; Wu, Di; Shen, Zhi-Xun; Xu, Xiaodong; Cobden, David H.; Cui, Yong-Tao (February 2019).
447:
629:
Persson, Kristin (2020). "Materials Data on Te2W by
Materials Project". LBNL Materials Project; Lawrence Berkeley National Laboratory (LBNL), Berkeley, CA (United States).
1238:
Miguel M.; Liu, Zhi; Xie, Xiaoming; Devereaux, Thomas P.; Crommie, Michael F.; Mo, Sung-Kwan; Shen, Zhi-Xun (July 2017). "Quantum spin Hall state in monolayer 1T'-WTe2".
555:
was initially predicted to remain a Weyl semimetal in the 1T' crystal phase. It was later shown with transport measurements that, below 50K, a single layer of WTe
1605:
258:
527:
and, in particular, to be the first example of a Type II Weyl semimetal, where the Weyl nodes exist at the intersection of the electron and hole pockets.
34:
501:
hard to recognize. The tungsten atoms instead form zigzag chains, which are thought to behave as one-dimensional conductors. Unlike electrons in other
3126:
940:
Soluyanov, Alexey A.; Gresch, Dominik; Wang, Zhijun; Wu, Quansheng; Troyer, Matthias; Dai, Xi; Bernevig, B. Andrei (2015). "Type-II Weyl semimetals".
569:
742:
Pletikosic, I; Ali, M N; Fedorov, A V; Cava, R J; Valla, T (2014). "Electronic
Structure Basis for the Extraordinary Magnetoresistance in WTe
1002:
Devereaux, Thomas P.; Heinz, Tony F.; Wang, Xijie; Lindenberg, Aaron M. (January 2019). "An ultrafast symmetry switch in a Weyl semimetal".
873:
Kang, Defen; Zhou, Yazhou; Yi, Wei; Yang, Chongli; Guo, Jing; Shi, Youguo; Zhang, Shan; Wang, Zhe; Zhang, Chao; et al. (23 July 2015).
2136:
1544:
Yang, Qing; Wu, Menghao; Li, Ju (20 December 2018). "Origin of Two-Dimensional
Vertical Ferroelectricity in WTe 2 Bilayer and Multilayer".
1636:
1061:
Qian, X.; Liu, J.; Fu, L.; Li, J. (12 December 2014). "Quantum spin Hall effect in two-dimensional transition metal dichalcogenides".
613:
233:
1742:
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494:
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1984:
1976:
502:
454:
1968:
1900:
1881:
1591:
541:
197:
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2863:
545:
153:
2859:
576:
has also been observed to superconduct at moderate doping, with a critical temperature tunable by doping level.
123:
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2009:
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141:
3010:
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2146:
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1440:
1376:
1311:
1257:
1195:
1141:
1080:
1011:
959:
896:
765:
700:
530:
It has also been reported that terahertz-frequency light pulses can switch the crystal structure of
3131:
3116:
3057:
2681:
2425:
2380:
2298:
2260:
2194:
2122:
1960:
1952:
1861:
1830:
1790:
1714:
1675:
1659:
875:"Superconductivity emerging from a suppressed large magnetoresistant state in tungsten ditelluride"
214:
89:
497:, but its layers are so distorted that the honeycomb lattice many of them have in common is in WTe
2719:
2698:
2658:
2578:
2474:
2456:
2392:
2209:
2161:
2017:
1849:
1774:
1614:
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1526:
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1430:
1366:
1335:
1301:
1273:
1247:
1219:
1185:
1157:
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1104:
1070:
1043:
983:
949:
886:
848:
820:
789:
755:
724:
690:
2733:
2714:
2549:
2464:
2185:
1944:
1561:
1518:
1456:
1402:
1327:
1211:
1096:
1035:
1027:
975:
922:
840:
781:
716:
638:
609:
490:
486:
365:
2617:
2540:
2429:
2246:
1936:
1769:
1553:
1510:
1448:
1392:
1384:
1319:
1265:
1203:
1149:
1088:
1019:
967:
912:
904:
830:
773:
708:
630:
551:
Tungsten ditelluride can be exfoliated into thin sheets down to single layers. Monolayer WTe
399:
335:
281:
99:
663:
1292:
Laser–Angle-Resolved
Photoemission on Encapsulated Mono-, Bi-, and Few-Layer 1T′-WTe 2".
218:
145:
1506:
1444:
1380:
1315:
1261:
1199:
1145:
1084:
1015:
963:
900:
769:
704:
2728:
2420:
2400:
2169:
1397:
1354:
917:
874:
524:
425:
375:
17:
3110:
2594:
2566:
1992:
1468:
1277:
1223:
1161:
1108:
987:
489:. In October 2014, tungsten ditelluride was discovered to exhibit an extremely large
324:
134:
1573:
1530:
1339:
1047:
852:
793:
835:
777:
728:
371:
185:
1323:
1557:
584:
383:
1514:
1023:
346:
296:
1452:
1207:
1092:
534:
483:
480:
473:
1565:
1522:
1460:
1406:
1388:
1331:
1215:
1100:
1039:
979:
926:
844:
785:
720:
531:
470:
971:
808:
712:
908:
352:
314:
172:
154:
1269:
1153:
1031:
677:
Ali, Mazhar N. (2014). "Large, non-saturating magnetoresistance in WTe
642:
1583:
634:
424:
Except where otherwise noted, data are given for materials in their
1497:
1435:
1371:
1306:
1252:
1190:
1136:
954:
891:
825:
1075:
760:
695:
122:
112:
2118:
1587:
512:
When subjected to pressure, the magnetoresistance effect in WTe
608:(87 ed.). Boca Raton, Florida: CRC Press. pp. 4–92.
202:
809:"Viewpoint: Electrons Travel Between Loosely Bound Layers"
442:
1355:"Imaging quantum spin Hall edges in monolayer WTe 2"
2033:
2008:
1893:
1842:
1762:
1707:
1652:
1621:
572:and microwave-impedance microscopy. Monolayer WTe
184:
98:
2130:
1599:
8:
329:1,020 °C (1,870 °F; 1,290 K)
560:edge—behavior consistent with monolayer WTe
548:by altering the material's atomic lattice.
2137:
2123:
2115:
2005:
1606:
1592:
1584:
217:
144:
26:
1546:The Journal of Physical Chemistry Letters
1496:
1434:
1396:
1370:
1305:
1251:
1189:
1135:
1074:
953:
916:
890:
834:
824:
759:
694:
570:angle-resolved photoemission spectroscopy
2096:
2092:
2088:
2084:
596:
263:
238:
213:
2175:
2145:Salts and covalent derivatives of the
659:
648:
135:
2816:
245:Key: WFGOJOJMWHVMAP-UHFFFAOYSA-N
7:
2157:
509:can easily move between the layers.
175:
64:viewed from above. (W:gray, Te:red)
25:
606:Handbook of Chemistry and Physics
3127:Transition metal dichalcogenides
495:transition metal dichalcogenides
432:
42:
33:
807:Behnia, Kamran (22 July 2015).
428:(at 25 °C , 100 kPa).
836:10.1103/PhysRevLett.115.046602
778:10.1103/PhysRevLett.113.216601
583:have also been observed to be
579:Two- and three-layer thick WTe
503:two-dimensional semiconductors
1:
2010:Organotungsten(VI) compounds
1324:10.1021/acs.nanolett.8b04534
1558:10.1021/acs.jpclett.8b03654
3148:
2818:
301:439.04 g/mol
52:: Crystal structure of WTe
2177:
2154:
1515:10.1038/s41586-018-0336-3
1024:10.1038/s41586-018-0809-4
422:
358:
274:
254:
229:
82:
74:
69:
41:
32:
564:being a two-dimensional
1453:10.1126/science.aar4426
1208:10.1126/science.aan6003
1093:10.1126/science.1256815
748:Physical Review Letters
604:Lide, David R. (1998).
3122:Tungsten(IV) compounds
1389:10.1126/sciadv.aat8799
658:Cite journal requires
523:was predicted to be a
505:, the electrons in WTe
18:Tungsten(IV) telluride
879:Nature Communications
566:topological insulator
413: = 6.34 Å,
409: = 3.50 Å,
60:: Single layer of WTe
28:Tungsten ditelluride
467:Tungsten ditelluride
77:tungsten ditelluride
2034:Polytungstate salts
1507:2018Natur.560..336F
1445:2018Sci...362..922S
1381:2019SciA....5.8799S
1316:2019NanoL..19..554C
1262:2017NatPh..13..683T
1200:2018Sci...359...76W
1146:2017NatPh..13..677F
1085:2014Sci...346.1344Q
1069:(6215): 1344–1347.
1016:2019Natur.565...61S
972:10.1038/nature15768
964:2015Natur.527..495S
901:2015NatCo...6.7804K
770:2014PhRvL.113u6601P
713:10.1038/nature13763
705:2014Natur.514..205A
417: = 15.4 Å
336:Solubility in water
29:
1615:Tungsten compounds
909:10.1038/ncomms8804
455:Infobox references
27:
3102:
3101:
3096:
3095:
2112:
2111:
2108:
2107:
1552:(24): 7160–7164.
1491:(7718): 336–339.
1429:(6417): 922–925.
1270:10.1038/nphys4174
1154:10.1038/nphys4091
491:magnetoresistance
487:chemical compound
463:Chemical compound
461:
460:
366:Crystal structure
319:9.43 g/cm, solid
198:CompTox Dashboard
124:Interactive image
16:(Redirected from
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635:10.17188/1198898
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282:Chemical formula
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2887:
2883:
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2871:
2867:
2862:
2855:
2851:
2846:
2839:
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2830:
2741:
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2723:
2710:
2704:
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2646:
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2603:
2598:
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2582:
2574:
2569:
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2544:
2524:
2516:
2508:
2500:
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2478:
2455:
2453:
2449:
2444:
2442:
2438:
2428:
2419:
2417:
2413:
2408:
2396:
2391:
2387:
2384:
2361:
2356:
2349:
2345:
2340:
2333:
2322:
2318:
2302:
2283:
2279:
2268:
2264:
2250:
2230:
2226:
2217:
2213:
2208:
2206:
2189:
2168:
2165:
2150:
2143:
2113:
2104:
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1582:
1581:
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1542:
1538:
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1480:
1476:
1419:
1418:
1414:
1365:(2): eaat8799.
1352:
1351:
1347:
1290:
1289:
1285:
1236:
1235:
1231:
1184:(6371): 76–79.
1174:
1173:
1169:
1121:
1120:
1116:
1060:
1059:
1055:
1010:(7737): 61–66.
1000:
999:
995:
948:(7579): 495–8.
939:
938:
934:
872:
871:
867:
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740:
736:
689:(7521): 205–8.
680:
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616:
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602:
598:
593:
582:
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450: ?)
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5:
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2200:
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2187:
2182:
2181:
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1124:Nature Physics
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615:0-8493-0594-2
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354:
351:insoluble in
350:
348:
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333:
332:
328:
326:
325:Melting point
323:
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318:
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215:DTXSID3065243
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136:ECHA InfoCard
133:
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109:
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51:
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40:
36:
31:
19:
3104:
2707:
2701:
2666:
2600:
1894:Tungsten(VI)
1763:Tungsten(IV)
1748:
1653:Tungsten(II)
1549:
1545:
1539:
1488:
1484:
1477:
1426:
1422:
1415:
1362:
1358:
1348:
1297:
1294:Nano Letters
1293:
1286:
1243:
1239:
1232:
1181:
1177:
1170:
1127:
1123:
1117:
1066:
1062:
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1007:
1003:
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945:
941:
935:
882:
878:
868:
856:. Retrieved
816:
812:
802:
751:
747:
737:
686:
682:
672:
651:cite journal
624:
605:
599:
585:polar metals
578:
550:
542:orthorhombic
529:
518:
511:
484:semimetallic
466:
465:
414:
410:
406:
372:orthorhombic
83:Identifiers
75:Other names
57:
49:
1843:Tungsten(V)
1622:Tungsten(0)
384:Space group
341:negligible
306:Appearance
275:Properties
142:100.031.884
3132:Monolayers
3117:Tellurides
3111:Categories
1498:1809.04575
1436:1809.04691
1372:1807.09342
1307:1811.04629
1253:1703.03151
1191:1711.03584
1137:1610.07924
955:1507.01603
892:1502.00493
826:1506.02214
591:References
546:monoclinic
359:Structure
347:Solubility
297:Molar mass
111:3D model (
100:12067-76-4
90:CAS Number
2147:telluride
1469:206665871
1278:119327399
1224:206660894
1162:104152529
1109:206559705
1076:1406.2749
988:205246491
819:(4): 71.
761:1407.3576
696:1405.0973
481:inorganic
393:, No. 31
163:235-086-0
155:EC Number
1574:56147713
1566:30540485
1531:49907122
1523:30038286
1461:30361385
1407:30783621
1340:53685202
1332:30570259
1216:29302010
1101:25504715
1048:57373505
1040:30602749
980:26607545
927:26203807
885:: 7804.
853:22977747
845:26252701
794:30058910
786:25479512
721:25219849
540:between
479:) is an
2819:
1503:Bibcode
1441:Bibcode
1423:Science
1398:6368433
1377:Bibcode
1312:Bibcode
1258:Bibcode
1196:Bibcode
1178:Science
1142:Bibcode
1081:Bibcode
1063:Science
1032:1492730
1012:Bibcode
960:Bibcode
918:4525168
897:Bibcode
858:28 July
813:Physics
766:Bibcode
729:4446498
701:Bibcode
643:1198898
448:what is
446: (
353:ammonia
315:Density
291:
173:PubChem
2087:[H
1572:
1564:
1529:
1521:
1485:Nature
1467:
1459:
1405:
1395:
1338:
1330:
1276:
1222:
1214:
1160:
1107:
1099:
1046:
1038:
1030:
1004:Nature
986:
978:
942:Nature
925:
915:
851:
843:
792:
784:
727:
719:
683:Nature
641:
612:
443:verify
440:
259:SMILES
70:Names
58:Bottom
1696:(hpp)
1684:W(OH)
1637:W(PMe
1629:W(CO)
1570:S2CID
1527:S2CID
1493:arXiv
1465:S2CID
1431:arXiv
1367:arXiv
1336:S2CID
1302:arXiv
1274:S2CID
1248:arXiv
1220:S2CID
1186:arXiv
1158:S2CID
1132:arXiv
1105:S2CID
1071:arXiv
1044:S2CID
984:S2CID
950:arXiv
887:arXiv
849:S2CID
821:arXiv
790:S2CID
756:arXiv
725:S2CID
691:arXiv
234:InChI
186:82913
113:JSmol
3047:ThTe
3023:YbTe
3007:TmTe
2991:ErTe
2975:HoTe
2959:DyTe
2943:TbTe
2927:GdTe
2911:EuTe
2895:SmTe
2876:NdTe
2860:PrTe
2844:CeTe
2828:LaTe
2760:RaTe
2729:PbTe
2715:HgTe
2682:ReTe
2659:TaTe
2651:HfTe
2635:LuTe
2627:BaTe
2571:SnTe
2567:SnTe
2550:CdTe
2521:MoTe
2513:NbTe
2505:ZrTe
2486:SrTe
2426:GeTe
2406:GaTe
2401:ZnTe
2393:CuTe
2389:CuTe
2376:NiTe
2371:CoTe
2366:FeTe
2358:MnTe
2354:MnTe
2338:CrTe
2308:CaTe
2256:MgTe
2195:BeTe
2170:-TeH
2018:W(CH
1977:WOCl
1969:WOBr
1882:LiWF
1562:PMID
1519:PMID
1457:PMID
1403:PMID
1328:PMID
1212:PMID
1097:PMID
1036:PMID
1028:OSTI
976:PMID
923:PMID
860:2015
841:PMID
782:PMID
717:PMID
664:help
639:OSTI
610:ISBN
544:and
389:Pmn2
376:oP12
3092:No
3089:Md
3086:Fm
3083:Es
3080:Cf
3077:Bk
3074:Cm
3071:Am
3068:Pu
3065:Np
3058:UTe
3054:Pa
3043:Ac
3040:**
2891:Pm
2812:Og
2809:Ts
2806:Lv
2803:Mc
2800:Fl
2797:Nh
2794:Cn
2791:Rg
2788:Ds
2785:Mt
2782:Hs
2779:Bh
2776:Sg
2773:Db
2770:Rf
2767:Lr
2764:**
2756:Fr
2751:Rn
2748:At
2745:Po
2695:Pt
2692:Ir
2689:Os
2674:WTe
2667:WTe
2612:Xe
2537:Pd
2534:Rh
2531:Ru
2528:Tc
2469:Kr
2465:+Br
2461:Se
2457:+As
2430:-Ge
2421:-Ga
2330:VTe
2326:Ti
2293:Ar
2290:Cl
2282:0.2
2278:0.8
2272:Si
2241:Ne
2223:(NH
2210:(CH
2203:CTe
2180:He
2149:ion
2057:(NH
1985:WOF
1961:WAs
1921:WCl
1913:WBr
1862:WBr
1823:WBr
1815:WCl
1799:WTe
1791:WSe
1751:Bu)
1727:WCl
1668:WCl
1660:WSi
1554:doi
1511:doi
1489:560
1449:doi
1427:362
1393:PMC
1385:doi
1320:doi
1266:doi
1204:doi
1182:359
1150:doi
1089:doi
1067:346
1020:doi
1008:565
968:doi
946:527
913:PMC
905:doi
831:doi
774:doi
752:113
746:".
709:doi
687:514
681:".
631:doi
519:WTe
287:WTe
203:EPA
176:CID
50:Top
3113::
3031:Te
3027:Yb
3015:Te
3011:Tm
2999:Te
2995:Er
2983:Te
2979:Ho
2967:Te
2963:Dy
2951:Te
2947:Tb
2935:Te
2931:Gd
2919:Te
2915:Eu
2903:Te
2899:Sm
2884:Te
2880:Nd
2868:Te
2864:Pr
2852:Te
2848:Ce
2836:Te
2832:La
2824:*
2738:Te
2734:Bi
2724:Te
2720:Tl
2705:Te
2699:Au
2643:Te
2639:Lu
2631:*
2622:Te
2618:Cs
2609:I
2595:Te
2591:Te
2583:Te
2579:Sb
2559:Te
2555:In
2545:Te
2541:Ag
2497:Te
2479:Te
2475:Rb
2450:Te
2446:As
2439:Te
2435:As
2414:Te
2410:Ga
2385:Te
2381:Cu
2346:Te
2342:Cr
2319:Te
2315:Sc
2303:Te
2287:S
2280:Te
2265:Te
2261:Al
2251:Te
2247:Na
2238:F
2235:O
2231:Te
2218:Te
2199:B
2190:Te
2186:Li
2166:Te
2097:40
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2083:Na
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