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4+ components. See: Balzani, V.; Credi, A.; Mattersteig, G.; Matthews, O. A.; Raymo, F. M.; Stoddart, J. F.; Venturi, M.; White, A. J. P.; Williams, D. J. J. Org. Chem. 2000, 05, 1924-1936.
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38
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9744273430
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note
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Molecular force estimates were calculated using Coulombic repulsion assuming a 1 nm diameter ring carrying four evenly dispersed positive charges which is encircling a site containing two positive charges. Movement is assumed to proceed linearly, 3.7 nm away from the starting position.
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39
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0037012703
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Bourgoin, J.-P.6
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40
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0038443999
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(b) Hou, S.; Sagara, T.; Xu, D.; Kelly, T. R.; Gamz, E. Nanotechnology 2003, 14, 566-570.
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Hou, S.1
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41
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85042519082
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6, 4 have been reported recently in a full paper. See: Tseng, H.-R.; Vignon, S. A.; Celestre, P. C.; Perkins, J.; Jeppesen, J. O.; Di Fabio, A.; Ballardini, R.; Gandolfi, M. T.; Venturi, M.; Balzani, V.; Stoddart, J. F. Chem. Eur. J. 2003, 9, 155-172.
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Tseng, H.-R.1
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Celestre, P.C.3
Perkins, J.4
Jeppesen, J.O.5
Di Fabio, A.6
Ballardini, R.7
Gandolfi, M.T.8
Venturi, M.9
Balzani, V.10
Stoddart, J.F.11
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42
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9744281422
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note
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2/molecule-min. All isotherms, which were obtained for starting-state and oxidized molecules, were highly reproducible.
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43
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3142741598
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2. These data are consistent with results (Lee, I. C.; Frank, C. W.; Yamamoto, T.; Tseng, H.-R.; Flood, A. H.; Stoddart, J. F.; Jeppesen, J. O. Langmuir 2004, 20, 5809-5828) which suggest that, at pressures below the transition region, the rotaxane exists in a folded conformation, whereas, under similar conditions, the dumbbell is unfolded.
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(2004)
Langmuir
, vol.20
, pp. 5809-5828
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-
Lee, I.C.1
Frank, C.W.2
Yamamoto, T.3
Tseng, H.-R.4
Flood, A.H.5
Stoddart, J.F.6
Jeppesen, J.O.7
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44
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84862470830
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Nørgaard, K.; Jeppesen, J. O.; Laursen, B. O.; Simonsen, J. B.; Weygand, M. J.; Kjaer, K.; Stoddart, J. F.; Bjørholm, T. Submitted
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Nørgaard, K.; Jeppesen, J. O.; Laursen, B. O.; Simonsen, J. B.; Weygand, M. J.; Kjaer, K.; Stoddart, J. F.; Bjørholm, T. Submitted.
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45
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9744265960
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note
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The XPS data were obtained on a VG ESCALAB 5 electron spectrometer using Al Ka X-ray radiation (1486.6 eV) with a passenergy of 20 eV at a takeoff angle of 90° (normal to the film surface). The photoemission of surface carbon (C 1s) at 284.6 eV was used as the reference binding energy. The weak photoemission intensity of N 1s is a consequence of the low nitrogen atomic density (less than 1 at. %), which approaches the XPS detection limit.
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0000944801
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(a) Chang, J. P.; Green, M. L.; Donnelly, V. M.; Opila, R. L.; Eng, J., Jr.; Sapjeta, J.; Silverman, P. J.; Weir, B.; Lu, H. C.; Gustafsson, T.; Garfunkel, E. J. Appl. Phys. 2000, 87, 4449-4455.
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Chang, J.P.1
Green, M.L.2
Donnelly, V.M.3
Opila, R.L.4
Eng Jr., J.5
Sapjeta, J.6
Silverman, P.J.7
Weir, B.8
Lu, H.C.9
Gustafsson, T.10
Garfunkel, E.11
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48
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9744284465
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note
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6+ shows a similarly weak and red-shifted band at 550 nm that displays a linear correlation of intensity with the number of layers. These observations lend qualitative support to the redox-controlled mechanical switching of the amphiphilic bistable rotaxanes in Langmuir films.
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49
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9744286482
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note
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2: = 5:1) cleaning for 5 min, (ii) deionized water cleaning for 5 min, and (iii) air-drying.
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50
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9744228201
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note
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Film thickness measurements were performed using a Gaertner L116B ellipsometer with an index of refraction of 1.46.
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52
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9744249694
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note
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Molecular modeling was performed in ChemBats3D by extending the molecule fully and then optimizing with the MM2 force field to obtain "correct" bond lengths and angles. The distance was measured from the center of the TTF unit to the center of the DNP unit. This fully extended conformation, which is employed for convenience in the graphical representations, does not reflect the variety of folded conformations that these compounds may realistically occupy in solution or in Langmuir and LB monolayers.
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53
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9744255711
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note
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-3 M. Typically, the sample was immersed in the oxidant solution for 30-40 min. Ellipsometry data show that the thickness of the films did not change while the samples were immersed in the solution of the oxidant.
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