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Department of Biochemistry and Pharmacy, Åbo Akademi University, Tykistökatu 6 A, FIN 20520 Turku, Finland
Correspondence: Address reprint requests to Bodil Ramstedt, Tel.: 358-2-2154816; Fax: 358-2-2154010; E-mail: boramste{at}abo.fi.
| ABSTRACT |
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| INTRODUCTION |
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Cholestatrienol (CTL) is a fluorescent cholesterol analog that has been shown to mimic the membrane behavior of cholesterol quite well (Fischer et al., 1984
; Hyslop et al., 1990
; Scheidt et al., 2003
; Schroeder et al., 1988
; Yeagle et al., 1990
). A recent study that utilized electron paramagnetic resonance, NMR, and fluorescence spectroscopy to investigate the potential of several fluorescent and spin-labeled sterol probes to function as cholesterol analogs found CTL to mimic cholesterol extraordinarily well in orientation and motion, to have similar membrane topology, and to have a comparable condensing effect on surrounding lipids (Scheidt et al., 2003
). CTL exerts intrinsic fluorescence due to two additional double bonds compared to cholesterol. Dehydroergosterol (DHE), which is another commonly used fluorescent sterol, has three more double bonds than cholesterol and an additional methyl group in the hydrocarbon tail. It is known that the addition of a methyl group to the sterol side chain affects the membrane and domain properties of the sterol significantly (Halling and Slotte, 2004
). CTL therefore seems to be a better choice as a fluorescent cholesterol analog, promoting the formation of sterol-rich Lo domains and having membrane properties that most closely resemble those of cholesterol. The fluorescence properties of CTL have earlier been characterized in POPC vesicles (Schroeder et al., 1988
). It was observed that CTL at concentrations below 6 mol % did not self-quench. In complex lipid bilayers, in which lateral domains are expected to be formed, CTL can be used as a fluorescent sterol analog together with a quencher (12SLPC) located outside the Lo domains (Ahmed et al., 1997
). The amount of CTL exposed to quenching by 12SLPC thereby gives a measure of CTL distribution between Lo and Ld membrane domains. However, our method does not report whether ordered domains are in the Lo or the gel phase, if such phases were present in the experimental system studied. Glycosphingolipids have long been known to form microdomains in bilayer membranes due to their saturated nature and because of the extensive hydrogen-bonding network formed between the sugar-headgroups (Masserini and Ravasi, 2001
; Schroeder et al., 1994
). The importance of cholesterol in these domains is yet a debated subject. The formation of domains by cerebrosides has been found to be only weakly influenced by the presence of cholesterol (Xu et al., 2001
). It also seems that in the presence of both glycosphingolipids and sphingomyelin, cholesterol prefers to interact with sphingomyelin over other sphingolipids (Ferraretto et al., 1997
; Masserini and Ravasi, 2001
). Cholesterol (or another cholesterol-like sterol) promotes phase separation of saturated sphingomyelins and formation of Lo phase (Ipsen et al., 1987
; Patra et al., 1999
; Wolf et al., 2001
). Dihydrosphingomyelin, which is a sphingomyelin species that is common in the human eye lens and has a saturated sphinganine base, seems to be more strongly associated with cholesterol than other sphingomyelin species (Kuikka et al., 2001
; Nyholm et al., 2003
). In this study, we examined how sterol-rich domains formed in complex bilayer membranes based on the fluorescence properties of CTL. We included two domain-forming glycerophospholipids (DPPC and DSPC), two sphingomyelins (PSM and DHPSM), and PGalCer and studied the stability of sterol-rich domains formed as a function of temperature.
Ceramides are intermediates of sphingolipid biogenesis and are involved in cell signaling (Kolesnick et al., 2000
; Merrill, 2002
). It has recently been suggested that the effect of ceramide as a second messenger may be mediated by the effects of ceramide on membrane structure (van Blitterswijk et al., 2003
). Natural ceramide is composed of a long-chain sphingosine base and a long saturated acyl chain. These structural features make ceramide increase the order of the acyl-chain region in bilayer membranes, much as cholesterol does (Holopainen et al., 1998
). As other sphingolipids, ceramide may also be involved in hydrogen-bonding interactions with other membrane components. A recent publication suggests that ceramide would compete with cholesterol for association with domain-forming lipids in bilayer membranes (Megha and London, 2004
). The ability of PCer to displace cholesterol from ordered domains in our mixed membrane systems was studied using tParCer as a fluorescent ceramide analog.
Taken together, our results showed that the saturated lipids used in this study formed sterol-rich domains to varying degrees and that the stability of the domains varied with acyl chain length and headgroup composition of the lipids. We showed that PGalCer, which was not able to form sterol-rich domains to any appreciable degree at physiological temperature, was able to accommodate more sterol at higher temperatures. We also showed that PCer effectively displaced sterols from ordered membrane domains.
| EXPERIMENTAL PROCEDURES |
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Cholestatrienol (CTL) was synthesized using the method published by Fischer et al. (1984)
. tParCer and tParGalCer were synthesized from trans-parinaric acid (Molecular Probes, Eugene, OR) and D-sphingosine (Sigma Chemicals) or psychosine (Avanti Polar Lipids) through a modified version of the method for synthesis of sphingomyelins by Cohen et al. (1984)
. Briefly, equimolar amounts of sphingosine or psychosine and trans-parinaric acid were dissolved in argon-saturated dichloromethane containing 9 vol % methanol together with dicyclohexylcarbodiimide as a catalyst. Butylated hydroxytoluene was added to the reaction mixture to prevent oxidation, and molecular sieves (Fluka, Buchs, Switzerland) were added to keep the solvent dry. The reactions were carried out for 3 h at room temperature in the dark under an argon atmosphere. The fluorescent probes were identified by mass spectrometry. The purity was checked by reverse-phase HPLC on a RP-18 column before use, with methanol/acetonitrile (30:70, vol/vol) as eluent for CTL, methanol/H2O (80:20, vol/vol) for tParCer, and 100% methanol for tParGalCer. The fluorescent molecules were stored in the dark at 87°C until solubilized in argon-purged methanol. Stock solutions of fluorescent lipids were stored in the dark at 20°C and used within a week.
Preparation of bilayer vesicles
Bilayer vesicles used in steady-state and time-resolved fluorescence measurements were prepared at a lipid concentration of 50 µM. The lipid mixtures were dried under nitrogen, dispersed in water, and heated above the Tm. The warm samples were vortexed briefly and sonicated for 2 min (20% duty cycle, power output 15 W) with a Branson probe sonifier W-250 (Branson Ultrasonics, Danbury, CT). The water used was purified by reverse osmosis followed by passage through a Millipore UF Plus water purification system to yield a product with a resistivity of 18.2 M
cm.
CTL properties were studied with steady-state and time-resolved fluorescence spectroscopy in samples composed of phospholipid/cholesterol/CTL at a molar ratio of 95:4:1, where the phospholipid was POPC, DPPC, PSM, or DHPSM. In fluorescence quenching studies, F samples consisted of POPC/12SLPC/variable lipid/cholesterol/CTL (30:30:30:9:1, molar ratio), and POPC replaced 12SLPC in Fo samples. The membrane lipid here was POPC, DPPC, DSPC, PSM, DHPSM, or PGalCer. When the effect of ceramide was examined, PCer replaced half of the domain-forming phospholipid, and the samples were thus made of POPC/12SLPC/phospholipids/PCer/cholesterol (30:30:15:15:10, molar ratio). These samples were studied with CTL or tParCer, which replaced cholesterol or PCer, respectively (final concentration 1 mol %). The fluorescent probes were protected from light during all steps, and all solvents were saturated with argon before being used to minimize the risk of oxidation.
For the DSC experiments, we prepared liposomes of different compositions. The lipids were mixed in hexane/2-propanol after which the solvent was evaporated under a constant flow of N2 and put in vacuum for 1 h. The dry lipids were hydrated in water in a sealed vial above the main phase transition of the lipid with the highest melting temperature and vortexed briefly followed by 2 min of bath sonication at 90°C with a Branson bath sonifier 2510 (Branson Ultrasonics). The final concentration of lipids in the solution was 1 mg/ml. After sonication, the samples were cooled to room temperature and analyzed by DSC.
Steady-state fluorescence measurements
Fluorescence measurements were performed either on a PTI QuantaMaster-1 spectrofluorimeter (Photon Technology International, Lawrenceville, NJ) operating in the T-format or on a PTI QuantaMaster-2 spectrofluorimeter operating in the L-format. Both the excitation and emission slits were set to 5 nm on the former, whereas they were set to 5 nm and 10 nm, respectively, on the other filter-based spectrofluorimeter. The temperature was controlled by a Peltier element, with a temperature probe immersed in the sample solution. All experiments were made in quartz cuvettes, and the sample solutions were kept at constant stirring (260 rpm) during the measurements.
Fluorescence emission intensity of CTL was measured at 25°C and 37°C with excitation and emission wavelengths at 324 nm and 374 nm, respectively. Fluorescence emission of tParCer was detected at 410 nm, whereas excitation occurred at 305 nm. When studying temperature dependence of emission intensity, the samples were heated at a rate of 5°C/min during the measurements.
Quenching of steady-state fluorescence
The quenching of steady-state cholestatrienol fluorescence by 12SLPC was measured on a PTI QuantaMaster 1 spectrofluorimeter, essentially following the procedure described by Ahmed et al. (1997)
. Briefly, vesicles with a total lipid concentration of 50 µM with 1 mol % CTL were used. F samples contained quencher (12SLPC) and a complex lipid mixture as described above, and POPC replaced 12SLPC in Fo samples. The fluorescence intensity in the F samples was compared to the fluorescence intensity in Fo samples giving the fraction of quenched CTL fluorescence. The temperature in the samples was controlled by a Peltier element with a temperature probe immersed in the sample solution.
Time-resolved fluorescence measurements
Time-resolved fluorescence measurements were performed on a PTI TimeMaster fluorimeter, with an N2 laser as the light source. The temperature of the sample was controlled by a Peltier element, with a temperature probe immersed in the sample solution. All experiments were made in quartz cuvettes, and the sample solutions were kept at constant stirring (240 rpm) during the measurements. Data analysis was performed with the software (TimeMaster 1.2) supplied by the instrument manufacturer. The fit was determined from the reduced
2, Durbin-Watson, z value, and the weighted residuals.
Unilamellar phospholipid vesicles containing POPC, DPPC, PSM, or DHPSM together with cholesterol and CTL (molar ratio 95:4:1, total lipid concentration 50 µM) were used. The samples were excited at 337 nm, the wavelength generated by the N2 laser, and the emission was measured at 370 nm. The slits were set at 8 nm for all time-resolved measurements.
Differential scanning calorimetry
DSC measurements were performed in a Calorimetry Sciences (Provo, UT) Nano II DSC. Liposomes of equimolar mixtures of PSM and PGalCer (with varying amounts of cholesterol) and of PSM and PCer were prepared as described above. The samples were heated and cooled at a rate of 0.5°C/min. Sequential up and down scans between 15°C and 100°C were performed to study the reversibility of the melting process.
| RESULTS |
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2) given by us (1.52.8 ns) differ somewhat from those reported earlier, which varied between 3 and 3.7 ns. This may be a consequence of vesicle size and curvature due to different procedures for preparing the liposomes, i.e., probe- versus bath sonication, of which we prefer the former. From our results, we can see that the differences in fluorescence intensity detected by steady-state fluorescence measurement were not a consequence of differences in fluorescence lifetimes but rather of shifts in the fractional intensities of the two lifetime components, which were present for CTL in all phospholipid environments studied. In POPC vesicles, the shorter lifetime (
1) dominated to
90%, whereas in sphingomyelin bilayers at 25°C only 25%30% of the fluorescence intensity came from the shorter lifetime component. In DPPC, membranes at 25°C
50% of the steady-state fluorescence originated from the shorter lifetime component. At 37°C, the fraction of the shorter lifetime component increased for all lipids studied.
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46, 40, and 41°C, respectively, which are the temperatures given by previous DSC results for bilayers containing 5 mol % of cholesterol (McMullen et al., 1993
Stability of sterol-rich domains in complex lipid bilayers
The stability of sterol-enriched domains in mixed lipid bilayers was studied by determining the fraction of CTL emission that was quenchable by 12SLPC (a quencher located outside the Lo domains) as a function of temperature. Fluorescence emission intensity was measured in F samples consisting of POPC/12SLPC/phospholipid/cholesterol/CTL (30:30:30:9:1, molar ratio) and compared to Fo samples, in which 12SLPC was replaced by POPC. The ratio F/Fo is plotted as a function of temperature in Fig. 2. The melting of sterol-rich domains formed with DPPC, DSPC, PSM, and DHPSM was clearly detected. The sterol-rich domains formed with the DHPSM were the most stable because they melted at higher temperatures than those formed with the other phospholipids. Relatively low melting temperatures for the sterol-rich domains in phosphatidylcholine-containing membranes were detected, compared to the DSC-derived Tm values of
40°C and 54°C, respectively, for DPPC and DSPC liposomes containing 10 mol % cholesterol (McMullen et al., 1993
; McMullen and McElhaney, 1997
). This indicates a larger effect of POPC on these domains than on the sterol-rich domains formed with sphingomyelins. No melting of sterol-enriched domains was detected in POPC bilayers in the temperature range studied.
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50% at all temperatures studied. Just below the domain-melting temperature, the quenching efficiency in DPPC- and DSPC-containing membranes was between 35% and 40%, whereas the sphingomyelins were able to shield CTL from quenching better so that the corresponding value was only
20%. Above the domain-melting temperatures, the quenching efficiency was almost equal (
45%) in DPPC-, DSPC-, PSM-, and DHPSM-containing membranes. Another interesting feature seen in Fig. 2 is the apparent increased association of sterols with increasing temperature seen as an increase in shielding of CTL from quenching before domain melting.
Formation of ordered domains in the presence of galactosylceramide
The fluorescence-quenching assay described above was used to study formation of sterol-enriched domains in bilayers containing PGalCer. The bilayer membranes contained PGalCer (30 mol %), PSM (30 mol %), or an equimolar mixture of the two (15 mol % each), in addition to POPC, 12SLPC, and sterols (1 mol % CTL and 9 mol % cholesterol). The ratio of the quenched and unquenched emission (F/Fo) is plotted as a function of temperature in Fig. 3 A. It can be seen that some of the CTL associated with PGalCer as temperature was increased and detected a melting at
80°C. The addition of an equimolar amount of PGalCer into PSM-containing bilayers led to the formation of sterol-rich domains which were somewhat more thermostable than the sterol-rich domains formed with PSM alone. The fluorescent reporter molecule tParGalCer detected domain melting at
40° in PGalCer-containing mixed membranes containing 29 mol % PGalCer and 1 mol % tParGalCer, POPC, 12SLPC, and 10 mol % cholesterol (Fig. 3 B). tParGalCer also detected the melting of domains in membranes where an equimolar mixture of PGalCer and PSM represented the sphingolipid fraction. These domains melted at
30°C, which is a little lower than the domain-melting temperature reported by CTL for similar mixed membranes, indicating that the fluorescent probes are sensing different microenvironments in the membranes.
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| DISCUSSION |
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Fluorescence properties of CTL in different phospholipid environments
The CTL fluorescence emission was sensitive to the phospholipid environment in bilayer membranes, showing higher fluorescence intensity in sphingomyelin than in phosphatidylcholine bilayers. The fluorescence intensity differences might arise from differences in packing or in the ability of the matrix phospholipids to shield the probe from interaction with water. The fluorescence intensity for CTL was higher in lipid bilayers than in all neat solvents examined (results not shown). At low mol % (as used in this study) CTL has previously been found to be sensitive to dielectric effects (Schroeder et al., 1988
). All conditions that might give larger exposure of CTL to water also gave a reduction in fluorescence intensity. A reduction in CTL fluorescence was also observed at the gel-to-liquid phase transition in DPPC, PSM, and DHPSM bilayers, again suggesting sensitivity to changes in packing density or penetration of water into the membrane. This would also explain the apparent difference in CTL fluorescence in the more ordered DPPC versus the less ordered POPC membranes. Cholesterol desorption from mixed monolayers to ß-cyclodextrin in the subphase is a convenient tool to measure how well a phospholipid interacts with cholesterol, since the desorption rate is influenced by packing and interactions with surrounding membrane components that the sterol experiences at the surface of the donor membrane (Ohvo and Slotte, 1996
). Cholesterol desorption to ß-cyclodextrin from monolayers with DPPC, PSM, and DHPSM has been measured in our previous studies and shows good correlation with the fluorescence intensities seen in this study, with the lowest rates of desorption from DHPSM-containing monolayers and the highest desorption rates from DPPC (Kuikka et al., 2001
; Ramstedt and Slotte, 1999b
). This might again suggest that the exposure of the sterol at the interface, which is influenced by the interaction of the sterol with the other lipids in the bilayer, also is of importance for the detected CTL fluorescence.
Analysis of the time-resolved fluorescence data gave the best fits with a model containing two exponential decays. At 25°C in POPC vesicles the shorter lifetime component (
1) dominated to
90%, whereas only 2530% of the fluorescence intensity in sphingomyelin bilayers originated from the shorter lifetime component. In DPPC membranes at 25°C,
50% of the steady-state fluorescence came from the shorter lifetime component. The two lifetime components might originate from CTL molecules at different depths in the membrane, much as has been seen for some other fluorescent membrane probes (Klymchenko et al., 2004
). The shorter lifetime component would then originate from less shielded CTL molecules, whereas the longer lifetime component could originate from a more shielded population. The CTL fluorescence in sphingomyelin bilayers might be affected by possible hydrogen bonding in the headgroup region of these bilayers (Mombelli et al., 2003
; Niemela et al., 2004
; Talbott et al., 2000
). Sphingomyelins can function as both hydrogen-bond donors and acceptors, which might lead to hydrogen bonding between the probe and sphingomyelins; however, at present we cannot determine whether or not such hydrogen bonding takes place. A recent molecular dynamics simulation study showed clearly slower rotational and lateral diffusion in PSM bilayers compared to DPPC bilayers, most likely due to the differences in hydrogen-bonding patterns in the interfacial area (Niemela et al., 2004
). The fluorescence intensity also decreases with higher temperature in all phospholipid bilayers studied. An increase in diffusional rates in the membrane decreases the CTL fluorescence intensity most likely due to increased quenching.
Domain formation studied by quenching of CTL fluorescence
The fraction of CTL emission that was quenchable by 12SLPC was larger in phosphatidylcholine bilayers than in sphingomyelin bilayers, indicating a higher affinity of the sterol for the latter and/or a higher packing density in the sterol-rich domains formed with sphingomyelins. The Lo domains formed in sphingomyelin-containing bilayers were recently compared by atomic force microscopy to sterol-rich domains formed with DPPC in a DOPC matrix (van Duyl et al., 2003
). The size and shape of the Lo domains in these two systems differed markedly, with bigger Lo domains in the sphingomyelin-containing membranes. Based on those findings, it is possible that some of our results also may depend on domain morphology, since CTL at the domain interface may be susceptible to quenching by 12SLPC. The small differences seen between DHPSM and PSM can originate from known differences in hydrogen-bonding patterns in the interfacial region in membranes formed by these two lipids (Ferguson-Yankey et al., 2000
; Talbott et al., 2000
).
The effect of temperature on the formation of sterol-rich domains in complex lipid mixtures
CTL reported the melting of sterol-rich domains formed with DPPC, DSPC, PSM, and DHPSM clearly. Increasing the temperature increased the fraction of CTL that was shielded from quenching in all our lipid mixtures below the domain melting temperature. The domain-forming lipids were probably able to accommodate more sterol as the packing in the domains gradually became less restricted at higher temperatures.
The sterol-rich domains formed with the sphingomyelins and DSPC were more thermostable than those formed with DPPC. The relatively low melting temperature for the sterol-rich domains in DPPC- and DSPC-containing membranes, compared to what might be expected on the basis of DSC results (McMullen et al., 1993
; McMullen and McElhaney, 1997
), indicates a larger effect (i.e., miscibility) of POPC on these domains than on the sterol-rich domains formed with sphingomyelins. It is also possible that formation of sterol-rich domains in phosphatidylcholine bilayers actually requires more sterol than in sphingomyelin-containing membranes as recently suggested by Kahya and co-workers (Kahya et al., 2004
). No melting of POPC-sterol domains was detected in the temperature range studied, but could probably have been detected at lower experimental temperatures.
In membranes containing PGalCer together with PSM, we could also observe sterol-rich domains. In an equimolar mixture of PSM and PGalCer, stable sterol-rich domains were formed. tParGalCer also detected domain-melting in such membranes although at slightly lower temperatures than CTL, indicating that the probes were sensing different environments to some extent.
Brain galactocerebrosides have been shown (by DSC) to be immiscible with cholesterol in the gel phase (Johnston and Chapman, 1988
). According to another study, cholesterol also has only moderate effects on domain formation by cerebrosides (Xu et al., 2001
). A small amount of the sterol in our study, however, seemed to be able to associate with PGalCer with increasing temperature, since quenching of CTL fluorescence decreased at higher temperatures. CTL also detected a melting at
80°C, which is close to the melting temperature of pure PGalCer, which is 82.3°C (Curatolo and Jungalwala, 1985
; Ruocco et al., 1981
, 1983
).
Including tParGalCer as a fraction of the PGalCer reported domain melting at
40°C indicating partial miscibility of POPC in the domains formed by PGalCer. Partial miscibility of POPC with natural cerebrosides has been reported before (Curatolo, 1986
). Our own DSC data on POPC/PGalCer mixtures showed complex thermotropic behavior with several transitions, including one at 40°C. The transitions seen appeared to be dependent on the thermal history of the sample (results not shown). From the results obtained regarding PGalCer in this study, we conclude that PGalCer was unable to form sterol-enriched domains to any significant degree when sphingomyelin was not present in the lipid mixture.
Effect of ceramide on phospholipid/cholesterol domains
Ceramides have been shown to stabilize the ordered gel phase in lipid bilayers (Massey, 2001
; Xu et al., 2001
). The formation of ordered domains in mixed bilayer membranes is also promoted by ceramide (Wang and Silvius, 2003
). It was recently suggested that ceramide is able to displace sterols from liquid-ordered domains (Megha and London, 2004
). We show that PCer displaced CTL from sterol-rich domains in membranes with DHPSM, PSM, or DPPC. This can be seen from the failure of CTL fluorescence to report a domain melting-induced discontinuity in the quenching susceptibility of PCer-containing membranes. The inclusion of tParCer as a fraction of the ceramide content of similar membranes gave a clear-cut melting of domains with accompanying quenching of the trans-parinaric acid fluorescence at approximately the temperature expected from DSC results. This observation clearly suggests that the ceramide was actually forming domains with the other domain-forming lipids in the bilayers, but the sterols were excluded from these ceramide-enriched domains. It was interesting to find that PCer was able to displace sterols from ordered domains with PSM and DHPSM although both sphingomyelins readily colocalize with cholesterol. The weak discontinuity in the CTL fluorescence curves approximately at the melting temperature for ceramide-rich domains might reflect the changes in packing occurring in the bilayer at this temperature.
| CONCLUDING REMARKS |
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Increasing the temperature increased the amount of sterol associated with all sterol-rich domains. PGalCer was, however, not able to form sterol-rich domains although a small amount of sterol associated with PGalCer when temperature was increased. PGalCer was, on the other hand, able to stabilize sterol-rich domains formed in PSM-containing bilayers.
The ability of tParCer to detect domain melting in complex membranes (containing both sterol and ceramide) in which CTL showed no domain melting strongly suggests that the sterols and ceramides resided in different domains in these membranes. The mechanisms and consequences of such molecular competition must await further clarification.
| ACKNOWLEDGEMENTS |
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This study was supported by the Academy of Finland, the Sigrid Juselius Foundation, the Magnus Ehrnrooth Foundation, the Oskar Öflund Foundation, and Medicinska Understödsföreningen Liv och Hälsa.
| FOOTNOTES |
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Abbreviations used: 12SLPC, 1-palmitoyl-2-stearoyl-(12-DOXYL)-sn-glycero-3-phosphocholine; CTL, cholesta-5,7,9(11)-trien-3-beta-ol; DHE, ergosta-5,7,9(11),22-tetraen-3ß-ol; DHPSM, D-erythro-N-palmitoyl-dihydrosphingomyelin; DPPC, 1,2-dipalmitoyl-sn-glycero-3-phosphocholine; DSC, differential scanning calorimetry; DSPC, 1,2-distearoyl-sn-glycero-3phosphocholine; Ld, liquid-disordered; Lo, liquid-ordered; PC, phosphatidylcholine; PCer, D-erythro-N-palmitoyl-sphingosine; PGalCer, D-erythro-N-palmitoyl-galactosylceramide; POPC, 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine; PSM, D-erythro-N-palmitoyl-sphingomyelin; Tm, mid temperature of the gel to liquid-crystalline phase transition; tParCer, D-erythro-N-trans-parinoyl-sphingosine; tParGalCer, D-erythro-N-trans-parinoyl-galactosylceramide.
Submitted on October 18, 2004; accepted for publication March 9, 2005.
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