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By Donghang Yan, Haibo Wang, Baoxun Du(auth.)
It's popular that the majority vital digital units use Schottky junctions and heterojunctions. regrettably there's not a complicated ebook introducing heterojunctions systematically. Introduction to natural Semiconductor Heterojunctions fills the distance. during this publication, the authors offer a finished dialogue and systematic advent at the state of the art applied sciences in addition to program of natural semiconductor heterojunctions.
- First e-book to systematically introduce natural heterojunctions
- Arms readers with theoretical, experimental and utilized elements of natural heterojunctions
- The chinese language variation of the booklet is a part of the chinese language Academy of Sciences’ special younger student medical ebook sequence
Introduction to natural Semiconductor Heterojunctions is a perfect and valued reference for researchers and graduate scholars targeting natural skinny movie units like natural light-emitting diodes (OLEDs), natural photovoltaic (OPV) cells, and natural field-effect transistors (OFETs). teachers can use the ebook as a supplementary textual content for a semiconductor physics or natural electronics direction, giving scholars a greater consider for the appliance of natural skinny movie devices.Content:
Chapter 1 natural Heterostructure in digital units (pages 1–6):
Chapter 2 vulnerable Epitaxy progress of natural Semiconductor skinny movie (pages 7–85):
Chapter three Interfacial digital constitution in natural Semiconductor Heterojunctions (pages 87–123):
Chapter four cost delivery in natural Heterojunctions (pages 125–153):
Chapter five natural Heterojunction functions in digital units (pages 155–207):
Chapter 6 natural Heterojunction Semiconductors (pages 209–242):
Read or Download Introduction to Organic Semiconductor Heterojunctions PDF
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Example text
38 Relationship between island density and coverage during the four steps of p-6P ultrathin film growth. 088/mm2, respectively [21]. L. , “Ultrathin-film growth of para-sexiphenyl (I): submonolayer thin-film growth as a function of the substrate temperature,” Journal of Physical Chemistry B, 112(26), 7816, 2008. ) (b) Third and fourth steps: the small gray-shadowed area in (b) is expanded and shown in detail in (a) [22]. L. , “Ultrathin-film growth of parasexiphenyl (II): formation of large-size domain and continuous thin film,” Journal of Physical Chemistry B, 112(26), 7821, 2008.
5 nm H2Pc thin films grown on p-6P ultrathin film (3 nm). ZnPc and H2Pc crystals take on several in-plane orientations on the p-6P monolayer film and only one in-plane orientation on the p-6P double layer film [29]. L. , “Weak epitaxy growth of metal-free phthalocyanine on p-sexiphenyl monolayer and double-layer films,” Journal of Physical Chemistry B, 112(10), 3132, 2008. 5 nm H2Pc grown on p-6P (a) monolayer film and (b) double layer film, respectively. H2Pc crystals exhibit three in-plane orientations on the p-6P monolayer film and only one in-plane orientation on the p-6P double layer film [29].
The thermodynamically metastable monolayer is transiting to thermodynamically stable double layer. The transition rate is about equal to the growth rate of monolayer [22]. L. , “Ultrathin-film growth of para-sexiphenyl (II): formation of large-size domain and continuous thin film,” Journal of Physical Chemistry B, 112(26), 7821, 2008. ) critical nucleus and a stable nucleus when meeting. The low island density supplies the precondition for the formation of large-size domains. During the growth process of monolayer islands, new molecules or molecular clusters should nucleate on each domain.