Kell Mortensen

Prof. Kell Mortensen

Niels Bohr Institute, University of Copenhagen
orcid

Research Focus & Metrics

Academic Career Length

49Years (1978-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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1 December 1995 in Macromolecules
Verified
Journal Article
Closed access
AKAshish K. Khandpur
Ashish K. Khandpur
SFStephan Foerster
Stephan Foerster
FBFrank S. Bates
Frank S. Bates
IHIan W. Hamley
Ian W. Hamley
ARAnthony John Ryan
Anthony John Ryan
Kell MortensenKell Mortensen
Kell Mortensen


1 March 1980 in Solid State Communications
Verified
Journal Article
Closed access
KBK. Bechgaard
K. Bechgaard
CJC.S. Jacobsen
C.S. Jacobsen
Kell MortensenKell Mortensen
Kell Mortensen
HPH.J. Pedersen
H.J. Pedersen
NTN. Thorup
N. Thorup

30 September 1993 in Nature
Verified
Journal Article
Closed access
PDF file
RCR. Cubitt
R. Cubitt
EFE. M. Forgan
E. M. Forgan
GYG. Yang
G. Yang
SLS. L. Lee
S. L. Lee
DPD. McK. Paul
D. McK. Paul
Kell MortensenKell Mortensen
Kell Mortensen

1 August 1990 in Journal of Applied Crystallography
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Journal Article
Closed access
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Jan Skov PedersenJan Skov Pedersen
Jan Skov Pedersen
DPD. Posselt
D. Posselt
Kell MortensenKell Mortensen
Kell Mortensen

1 January 1994 in Faraday Discussions
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Journal Article
Closed access
PDF file
FBFrank S. Bates
Frank S. Bates
MSMark F. Schulz
Mark F. Schulz
AKAshish K. Khandpur
Ashish K. Khandpur
SFStephan Forster
Stephan Forster
JRJeffrey H. Rosedale
Jeffrey H. Rosedale
Kell MortensenKell Mortensen
Kell Mortensen
Phase behaviour near the order–disorder transition (ODT) of 58 model hydrocarbon diblock copolymers, representing four different systems, is summarized. Six distinct ordered-state microstructures are reported, including hexagonally modulated lamellae (HML), hexagonally perforated layers (HPL) and a bicontinuous cubic morphology with Ia3d space group symmetry. Two non-classical parameters, ε and text-decoration:overlineN, control the occurrence and distribution of these phases, in addition to the classical variables ƒ and χN, where ƒ, χ and N are the composition, segment–segment interaction parameter and degree of polymerization, respectively. ε accounts for differences in the conformational and volume-filling characteristics of each block. Conformational asymmetry, ε≠ 1, produces an asymmetric phase diagram around ƒ= 1/2. The importance of fluctuation effects are inversely related to the magnitude of text-decoration:overlineN, a type of Ginzburg parameter that is proportional to N. As text-decoration:overlineN decreases, the bicontinuous Ia3d phase appears adjacent to the ODT. Development of this cubic phase can be rationalized based on chain-packing frustration near the lamellar hexagonal state. Apparently the Ia3d cubic state is stabilized by fluctuations since it disappears when text-decoration:overlineN becomes large. These findings provide new insights into the origins of phase complexity in condensed soft matter.