| LDR | | 02744nam u200469 4500 |
| 001 | | 000000418649 |
| 005 | | 20190215163033 |
| 008 | | 181129s2018 |||||||||||||||||c||eng d |
| 020 | |
▼a 9780438325654 |
| 035 | |
▼a (MiAaPQ)AAI10844898 |
| 035 | |
▼a (MiAaPQ)berkeley:18099 |
| 040 | |
▼a MiAaPQ
▼c MiAaPQ
▼d 247004 |
| 082 | 0 |
▼a 620.11 |
| 100 | 1 |
▼a Ong, Gary Kah Ping. |
| 245 | 10 |
▼a Assembly of and Ion Transport through Porous Nanocrystal Thin Films. |
| 260 | |
▼a [S.l.]:
▼b University of California, Berkeley.,
▼c 2018. |
| 260 | 1 |
▼a Ann Arbor:
▼b ProQuest Dissertations & Theses,
▼c 2018. |
| 300 | |
▼a 169 p. |
| 500 | |
▼a Source: Dissertation Abstracts International, Volume: 80-01(E), Section: B. |
| 500 | |
▼a Advisers: Fiona M. Doyle |
| 502 | 1 |
▼a Thesis (Ph.D.)--University of California, Berkeley, 2018. |
| 520 | |
▼a Of all the defining characteristics of a material, there are probably none more important than structure. Through a simple change in structure, materials can exhibit vastly different properties due to its influence at length scales from atomic c |
| 520 | |
▼a From advances in colloidal nanocrystals, materials with well-defined intrinsic characteristics such as composition and phase can now be synthesized reproducibly. However, these materials are often orders of magnitude smaller than actual device l |
| 520 | |
▼a Recent developments in nanocrystal surface chemistry have generated a sub-class of nanocrystals, called ligand-stripped nanocrystals, which are colloidally stable even in the absence of stabilizing ligands. This advancement opens both opportunit |
| 520 | |
▼a Chapter 3 extends the assembly of ligand stripped nanocrystals into block copolymer microphase-separated morphologies using PS-PDMA. Here, the phase separation behavior of PS-PDMA with and without nanocrystals is shown alongside methods used to |
| 520 | |
▼a Moving beyond the context of assembly towards the arena of ion transport properties, ligand free nanocrystal thin films are applied as model systems to investigate the phenomena of intermediate temperature proton conduction between 250 °C and 10 |
| 590 | |
▼a School code: 0028. |
| 650 | 4 |
▼a Materials science. |
| 650 | 4 |
▼a Nanoscience. |
| 650 | 4 |
▼a Energy. |
| 690 | |
▼a 0794 |
| 690 | |
▼a 0565 |
| 690 | |
▼a 0791 |
| 710 | 20 |
▼a University of California, Berkeley.
▼b Materials Science & Engineering. |
| 773 | 0 |
▼t Dissertation Abstracts International
▼g 80-01B(E). |
| 773 | |
▼t Dissertation Abstract International |
| 790 | |
▼a 0028 |
| 791 | |
▼a Ph.D. |
| 792 | |
▼a 2018 |
| 793 | |
▼a English |
| 856 | 40 |
▼u http://www.riss.kr/pdu/ddodLink.do?id=T15000020
▼n KERIS
▼z 이 자료의 원문은 한국교육학술정보원에서 제공합니다. |
| 980 | |
▼a 201812
▼f 2019 |
| 990 | |
▼a ***1012033 |