TY - JOUR
T1 - The structure and phase diagram of chiral alkyl-serine monolayers on mercury
AU - Tamam, L.
AU - Medina, D. D.
AU - Menahem, T.
AU - Mastai, Y.
AU - Sloutskin, E.
AU - Yefet, S.
AU - Deutsch, M.
PY - 2010
Y1 - 2010
N2 - The structure of liquid-mercury-supported Langmuir films (LFs) of chiral serine-modified fatty acid molecules was studied as a function of length, n = 8-22 carbons, temperature, T = 5-25 °C, and surface coverage, A ≈ 40-200 Å2 per molecule, for both homochiral and heterochiral compounds. Using surface pressure π-area A isotherms and surface-specific synchrotron X-ray diffraction methods the phase diagram was determined in detail. No lateral order was found for phases comprising surface-parallel molecules, in contrast with unmodified fatty acid LFs on mercury. For phases comprising standing-up molecules, long range lateral order was found for n ≥ 12, but no order for n = 8. The molecules in the ordered phases are extended, and tilt rigidly by ∼40° from the surface normal. The homochiral LFs pack in an oblique, single-molecule, unit cell. The heterochiral LFs pack in a body-centered rectangular unit cell, containing two molecules. Unlike unmodified fatty acid LFs, the structure of the standing-up phase does not vary with n, T or A. The interactions underlying these characteristics, and the role of chirality, are discussed.
AB - The structure of liquid-mercury-supported Langmuir films (LFs) of chiral serine-modified fatty acid molecules was studied as a function of length, n = 8-22 carbons, temperature, T = 5-25 °C, and surface coverage, A ≈ 40-200 Å2 per molecule, for both homochiral and heterochiral compounds. Using surface pressure π-area A isotherms and surface-specific synchrotron X-ray diffraction methods the phase diagram was determined in detail. No lateral order was found for phases comprising surface-parallel molecules, in contrast with unmodified fatty acid LFs on mercury. For phases comprising standing-up molecules, long range lateral order was found for n ≥ 12, but no order for n = 8. The molecules in the ordered phases are extended, and tilt rigidly by ∼40° from the surface normal. The homochiral LFs pack in an oblique, single-molecule, unit cell. The heterochiral LFs pack in a body-centered rectangular unit cell, containing two molecules. Unlike unmodified fatty acid LFs, the structure of the standing-up phase does not vary with n, T or A. The interactions underlying these characteristics, and the role of chirality, are discussed.
UR - http://www.scopus.com/inward/record.url?scp=75949120630&partnerID=8YFLogxK
U2 - 10.1039/b914714d
DO - 10.1039/b914714d
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AN - SCOPUS:75949120630
SN - 1744-683X
VL - 6
SP - 526
EP - 541
JO - Soft Matter
JF - Soft Matter
IS - 3
ER -