Topologically controlled phase transitions and nanoscale film self-assemblies of cage poly(-caprolactone) and its counterparts
Here we report the first quantitative investigation of nanoscale film morphologies of a cage-shaped poly( -caprolactone) ( cg -PCL 9k ) and its counterparts in star, cyclic, and linear topologies ( st -PCL 9k , cy -PCL 6k , and l -PCL 6k ) with consideration of topological influence through synchrot...
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Veröffentlicht in: | Polymer chemistry 2021-02, Vol.12 (5), p.744-758 |
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creator | Ree, Brian J Mato, Yoshinobu Xiang, Li Kim, Jehan Isono, Takuya Satoh, Toshifumi |
description | Here we report the first quantitative investigation of nanoscale film morphologies of a cage-shaped poly(
-caprolactone) (
cg
-PCL
9k
) and its counterparts in star, cyclic, and linear topologies (
st
-PCL
9k
,
cy
-PCL
6k
, and
l
-PCL
6k
) with consideration of topological influence through synchrotron grazing incidence X-ray scattering analysis. The folded crystalline layer thickness
l
c
is found to be in the increasing order of:
st
-PCL
9k
<
l
-PCL
6k
<
cy
-PCL
6k
<
cg
-PCL
9k
. Additional structural parameters, such as lamellar orientation, crystallinity, and orientation of orthorhombic lattice in nanoscale film, exhibit intricate dependencies on their molecular topologies and steric influences from the molecular joints and end groups. Nevertheless, all topological PCLs form lamellar structures based on the orthorhombic crystal lattice in nanoscale films. In addition, crystallization temperature
T
c
and crystal melting temperature
T
m
of all PCLs in bulk are highly dependent on the molecular topology; both
T
c
and
T
m
follow the same increasing trend of:
st
-PCL
9k
<
l
-PCL
6k
<
cy
-PCL
6k
<
cg
-PCL
9k
. Phase transition characteristics such as heat of fusion and crystallinity in bulk state, and thermal stability also depend upon the topological and steric influences.
Here we report the first quantitative investigation of nanoscale film morphologies of a cage-shaped poly(
-caprolactone) and its counterparts in star, cyclic, and linear topologies through synchrotron grazing incidence X-ray scattering analysis. |
doi_str_mv | 10.1039/d0py01567a |
format | Article |
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-caprolactone) (
cg
-PCL
9k
) and its counterparts in star, cyclic, and linear topologies (
st
-PCL
9k
,
cy
-PCL
6k
, and
l
-PCL
6k
) with consideration of topological influence through synchrotron grazing incidence X-ray scattering analysis. The folded crystalline layer thickness
l
c
is found to be in the increasing order of:
st
-PCL
9k
<
l
-PCL
6k
<
cy
-PCL
6k
<
cg
-PCL
9k
. Additional structural parameters, such as lamellar orientation, crystallinity, and orientation of orthorhombic lattice in nanoscale film, exhibit intricate dependencies on their molecular topologies and steric influences from the molecular joints and end groups. Nevertheless, all topological PCLs form lamellar structures based on the orthorhombic crystal lattice in nanoscale films. In addition, crystallization temperature
T
c
and crystal melting temperature
T
m
of all PCLs in bulk are highly dependent on the molecular topology; both
T
c
and
T
m
follow the same increasing trend of:
st
-PCL
9k
<
l
-PCL
6k
<
cy
-PCL
6k
<
cg
-PCL
9k
. Phase transition characteristics such as heat of fusion and crystallinity in bulk state, and thermal stability also depend upon the topological and steric influences.
Here we report the first quantitative investigation of nanoscale film morphologies of a cage-shaped poly(
-caprolactone) and its counterparts in star, cyclic, and linear topologies through synchrotron grazing incidence X-ray scattering analysis.]]></description><identifier>ISSN: 1759-9954</identifier><identifier>EISSN: 1759-9962</identifier><identifier>DOI: 10.1039/d0py01567a</identifier><language>eng</language><publisher>Cambridge: Royal Society of Chemistry</publisher><subject>Cages ; Crystal lattices ; Crystal structure ; Crystallinity ; Crystallization ; Data analysis ; Grazing incidence ; Heat of fusion ; Lamellar structure ; Mathematical morphology ; Melt temperature ; Melting ; Orthorhombic lattice ; Phase transitions ; Polymer chemistry ; Synchrotrons ; Thermal stability ; Thickness ; Topology ; X-ray scattering</subject><ispartof>Polymer chemistry, 2021-02, Vol.12 (5), p.744-758</ispartof><rights>Copyright Royal Society of Chemistry 2021</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c347t-c2744ce8ab240eefff93bfc02a6b215701c635be1075403a8b875e11a4a4af633</citedby><cites>FETCH-LOGICAL-c347t-c2744ce8ab240eefff93bfc02a6b215701c635be1075403a8b875e11a4a4af633</cites><orcidid>0000-0003-3746-2084 ; 0000-0002-3959-9896 ; 0000-0001-5449-9642</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27901,27902</link.rule.ids></links><search><creatorcontrib>Ree, Brian J</creatorcontrib><creatorcontrib>Mato, Yoshinobu</creatorcontrib><creatorcontrib>Xiang, Li</creatorcontrib><creatorcontrib>Kim, Jehan</creatorcontrib><creatorcontrib>Isono, Takuya</creatorcontrib><creatorcontrib>Satoh, Toshifumi</creatorcontrib><title>Topologically controlled phase transitions and nanoscale film self-assemblies of cage poly(-caprolactone) and its counterparts</title><title>Polymer chemistry</title><description><![CDATA[Here we report the first quantitative investigation of nanoscale film morphologies of a cage-shaped poly(
-caprolactone) (
cg
-PCL
9k
) and its counterparts in star, cyclic, and linear topologies (
st
-PCL
9k
,
cy
-PCL
6k
, and
l
-PCL
6k
) with consideration of topological influence through synchrotron grazing incidence X-ray scattering analysis. The folded crystalline layer thickness
l
c
is found to be in the increasing order of:
st
-PCL
9k
<
l
-PCL
6k
<
cy
-PCL
6k
<
cg
-PCL
9k
. Additional structural parameters, such as lamellar orientation, crystallinity, and orientation of orthorhombic lattice in nanoscale film, exhibit intricate dependencies on their molecular topologies and steric influences from the molecular joints and end groups. Nevertheless, all topological PCLs form lamellar structures based on the orthorhombic crystal lattice in nanoscale films. In addition, crystallization temperature
T
c
and crystal melting temperature
T
m
of all PCLs in bulk are highly dependent on the molecular topology; both
T
c
and
T
m
follow the same increasing trend of:
st
-PCL
9k
<
l
-PCL
6k
<
cy
-PCL
6k
<
cg
-PCL
9k
. Phase transition characteristics such as heat of fusion and crystallinity in bulk state, and thermal stability also depend upon the topological and steric influences.
Here we report the first quantitative investigation of nanoscale film morphologies of a cage-shaped poly(
-caprolactone) and its counterparts in star, cyclic, and linear topologies through synchrotron grazing incidence X-ray scattering analysis.]]></description><subject>Cages</subject><subject>Crystal lattices</subject><subject>Crystal structure</subject><subject>Crystallinity</subject><subject>Crystallization</subject><subject>Data analysis</subject><subject>Grazing incidence</subject><subject>Heat of fusion</subject><subject>Lamellar structure</subject><subject>Mathematical morphology</subject><subject>Melt temperature</subject><subject>Melting</subject><subject>Orthorhombic lattice</subject><subject>Phase transitions</subject><subject>Polymer chemistry</subject><subject>Synchrotrons</subject><subject>Thermal stability</subject><subject>Thickness</subject><subject>Topology</subject><subject>X-ray scattering</subject><issn>1759-9954</issn><issn>1759-9962</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><recordid>eNpFkT1PxDAMhisEEghY2JEisQBSIV9tryPiW0KC4RiYKjfnHEW5pMS54RZ-O-EOgT3Yw-P3teyiOBL8QnDVXs74uOKiqhvYKvZEU7Vl29Zy-6-v9G5xSPTBcyihpar3iq9pGIML88GAcytmgk8xOIczNr4DIUsRPA1pCJ4Y-Bnz4ANlFpkd3IIROlsCES56NyCxYJmBObKsuTotDYxZDEwKHs_W40Oi7LH0CeMIMdFBsWPBER7-1v3i9e52ev1QPj3fP15fPZVG6SaVRjZaG5xALzVHtNa2qreGS6h7KaqGC1OrqkfBm0pzBZN-0lQoBOictlZqvzjZ6OaFPpdIqfsIy-izZSf1pFGqlZJn6nxDmRiIItpujMMC4qoTvPs5cXfDX97WJ77K8PEGjmT-uP8XqG_5SXra</recordid><startdate>20210209</startdate><enddate>20210209</enddate><creator>Ree, Brian J</creator><creator>Mato, Yoshinobu</creator><creator>Xiang, Li</creator><creator>Kim, Jehan</creator><creator>Isono, Takuya</creator><creator>Satoh, Toshifumi</creator><general>Royal Society of Chemistry</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>8FD</scope><scope>JG9</scope><orcidid>https://orcid.org/0000-0003-3746-2084</orcidid><orcidid>https://orcid.org/0000-0002-3959-9896</orcidid><orcidid>https://orcid.org/0000-0001-5449-9642</orcidid></search><sort><creationdate>20210209</creationdate><title>Topologically controlled phase transitions and nanoscale film self-assemblies of cage poly(-caprolactone) and its counterparts</title><author>Ree, Brian J ; Mato, Yoshinobu ; Xiang, Li ; Kim, Jehan ; Isono, Takuya ; Satoh, Toshifumi</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c347t-c2744ce8ab240eefff93bfc02a6b215701c635be1075403a8b875e11a4a4af633</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><topic>Cages</topic><topic>Crystal lattices</topic><topic>Crystal structure</topic><topic>Crystallinity</topic><topic>Crystallization</topic><topic>Data analysis</topic><topic>Grazing incidence</topic><topic>Heat of fusion</topic><topic>Lamellar structure</topic><topic>Mathematical morphology</topic><topic>Melt temperature</topic><topic>Melting</topic><topic>Orthorhombic lattice</topic><topic>Phase transitions</topic><topic>Polymer chemistry</topic><topic>Synchrotrons</topic><topic>Thermal stability</topic><topic>Thickness</topic><topic>Topology</topic><topic>X-ray scattering</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Ree, Brian J</creatorcontrib><creatorcontrib>Mato, Yoshinobu</creatorcontrib><creatorcontrib>Xiang, Li</creatorcontrib><creatorcontrib>Kim, Jehan</creatorcontrib><creatorcontrib>Isono, Takuya</creatorcontrib><creatorcontrib>Satoh, Toshifumi</creatorcontrib><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><jtitle>Polymer chemistry</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Ree, Brian J</au><au>Mato, Yoshinobu</au><au>Xiang, Li</au><au>Kim, Jehan</au><au>Isono, Takuya</au><au>Satoh, Toshifumi</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Topologically controlled phase transitions and nanoscale film self-assemblies of cage poly(-caprolactone) and its counterparts</atitle><jtitle>Polymer chemistry</jtitle><date>2021-02-09</date><risdate>2021</risdate><volume>12</volume><issue>5</issue><spage>744</spage><epage>758</epage><pages>744-758</pages><issn>1759-9954</issn><eissn>1759-9962</eissn><abstract><![CDATA[Here we report the first quantitative investigation of nanoscale film morphologies of a cage-shaped poly(
-caprolactone) (
cg
-PCL
9k
) and its counterparts in star, cyclic, and linear topologies (
st
-PCL
9k
,
cy
-PCL
6k
, and
l
-PCL
6k
) with consideration of topological influence through synchrotron grazing incidence X-ray scattering analysis. The folded crystalline layer thickness
l
c
is found to be in the increasing order of:
st
-PCL
9k
<
l
-PCL
6k
<
cy
-PCL
6k
<
cg
-PCL
9k
. Additional structural parameters, such as lamellar orientation, crystallinity, and orientation of orthorhombic lattice in nanoscale film, exhibit intricate dependencies on their molecular topologies and steric influences from the molecular joints and end groups. Nevertheless, all topological PCLs form lamellar structures based on the orthorhombic crystal lattice in nanoscale films. In addition, crystallization temperature
T
c
and crystal melting temperature
T
m
of all PCLs in bulk are highly dependent on the molecular topology; both
T
c
and
T
m
follow the same increasing trend of:
st
-PCL
9k
<
l
-PCL
6k
<
cy
-PCL
6k
<
cg
-PCL
9k
. Phase transition characteristics such as heat of fusion and crystallinity in bulk state, and thermal stability also depend upon the topological and steric influences.
Here we report the first quantitative investigation of nanoscale film morphologies of a cage-shaped poly(
-caprolactone) and its counterparts in star, cyclic, and linear topologies through synchrotron grazing incidence X-ray scattering analysis.]]></abstract><cop>Cambridge</cop><pub>Royal Society of Chemistry</pub><doi>10.1039/d0py01567a</doi><tpages>15</tpages><orcidid>https://orcid.org/0000-0003-3746-2084</orcidid><orcidid>https://orcid.org/0000-0002-3959-9896</orcidid><orcidid>https://orcid.org/0000-0001-5449-9642</orcidid></addata></record> |
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language | eng |
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source | Royal Society Of Chemistry Journals 2008- |
subjects | Cages Crystal lattices Crystal structure Crystallinity Crystallization Data analysis Grazing incidence Heat of fusion Lamellar structure Mathematical morphology Melt temperature Melting Orthorhombic lattice Phase transitions Polymer chemistry Synchrotrons Thermal stability Thickness Topology X-ray scattering |
title | Topologically controlled phase transitions and nanoscale film self-assemblies of cage poly(-caprolactone) and its counterparts |
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