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1                                              POPE (Phylogeny, Ortholog and Paralog Extractor) provide
2                                              POPE allows the scientist to explore and understand the
3                                              POPE bilayers simulated at areas smaller than optimal ex
4                                              POPE is applied two biological simulators: a fast and st
5                                              POPE is available for download from the website: http://
6 tside, 2:1 mol:mol POPE:POPS inside (SMo/2:1 POPE:POPSi) the outer leaflet SM formed an ordered state
7 -oleoyl-phosphatidylglycerol (POPG), and 3:1 POPE:POPG were also conducted, and the presence of anion
8 layers composed of 4:1 POPC:cholesterol, 4:1 POPE:cholesterol, 3:1 POPC:1-palmitoyl-2-oleoyl-phosphat
9            The data collected reveal that 1) POPE is anionic and not neutral at pH 7.4; 2) high-anion
10 analogous mixtures of [(2)H(31)]16:0-18:1PE (POPE*) or [(2)H(31)]16:0-22:6PE (PDPE*) with egg SM and
11 -glycero-3-phosphoethanolamine (16:0-18:1PE, POPE) or 1-palmitoyl-2-docosahexaenoyl-sn-glycero-3-phos
12 ethanolamine (POPE); and 3) a mixture of 75% POPE, 20% 1-palmitoyl 2-oleoyl-phosphatidylglycerol (POP
13  cholesterol into J5 LPS/POPE liposomes at a POPE:cholesterol molar ratio of 1:0.15 blocked human SP-
14 roteins FhuA, LamB, NanC, OmpA and OmpF in a POPE/POPG (3:1) bilayer were performed to characterise t
15 hough there are differences between POPC and POPE/POPG bilayers, in both cases the toxin forms favora
16 m molecular dynamics simulations in POPC and POPE/POPG membranes.
17 tures of the monounsaturated lipids SOPC and POPE as a function of temperature and composition by NMR
18               Remarkably, when POPG/TOCL and POPE/POPG liposomes were co-incubated, Mac1 did not indu
19 ces to the lipid (31)P: 4.0-6.5 A in anionic POPE/POPG membranes and 6.5-8.0 A in zwitterionic POPC m
20 he inactive TPA4 in bacteria-mimetic anionic POPE/POPG bilayers and compared them with the wild-type
21 s with zwitterionic (POPC) and with anionic (POPE/POPG) lipid bilayers.
22 o or only small coupling differences between POPE and POPG in the presence of any of the cationic pep
23 e used in single-component membranes, binary POPE/POPG (3:1) membranes, and membranes containing one
24 l-2-oleoyl-phospha tidylcholine/cholesterol (POPE/POPC/CHOL) bilayers was measured as a function of P
25 mbrane of S. aureus (POPG/TOCL) and E. coli (POPE/POPG) were lysed at similar concentrations, whereas
26 s, but not B5 LPS/POPE liposomes or control (POPE only) liposomes.
27  for post optimization posterior evaluation (POPE) of simulators.
28  scans showed CHOL has a strong affinity for POPE, comparable to that observed between SM-CHOL.
29 ystalline phases coexist in the peptide-free POPE/POPG membrane, the peptides caused distinct quadrup
30 -incubated, Mac1 did not induce leakage from POPE/POPG liposomes, suggesting a preference toward POPG
31 2-oleoyl-sn-glycerophosphatidylethanolamine (POPE) or 1-palmitoyl-2-docosahexaenoyl-sn-glycerophospha
32 resulted in the formation of microdomains in POPE/POPS monolayers, but only SPM promoted a substantia
33 pectra also implied intimate lipid mixing in POPE/SM/CHOL (1:1:1 mol).
34 orming dipyrenylphosphatidylcholine probe in POPE/POPC mixtures were detected at X(PE) approximately
35 2-oleoyl-L-alpha-phosphatidylethano lam ine (POPE) multilamellar vesicles have been determined fluoro
36  observed with the incorporation of SPM into POPE/POPS membranes was, therefore, attributed to larger
37 ity of J5 LPS/POPE liposomes, but not B5 LPS/POPE liposomes or control (POPE only) liposomes.
38     Incorporation of cholesterol into J5 LPS/POPE liposomes at a POPE:cholesterol molar ratio of 1:0.
39 elittin increased the permeability of J5 LPS/POPE liposomes, but not B5 LPS/POPE liposomes or control
40 00 microg/mL, the permeability of the J5 LPS/POPE membranes increased 4.4-fold (p < 0.02) compared to
41                          Homogeneously mixed POPE/POPG membranes should give the same quadrupolar cou
42 nside (SMo/DOPCi) or SM outside, 2:1 mol:mol POPE:POPS inside (SMo/2:1 POPE:POPSi) the outer leaflet
43 POPE and POPG disorder: approximately 80% of POPE partitioned into the ordered phase, whereas all of
44 ured to determine the motional amplitudes of POPE and POPG acyl chains as a function of temperature.
45 R spectra of the perdeuterated sn-1 chain of POPE-d(31) increased by >50% upon addition of equimolar
46 components, were determined as a function of POPE mole fraction (X(PE)) at 22.4 degrees C.
47 OPE) mixtures were measured as a function of POPE mole fraction (X(PE)) at 23 degrees C.
48 CHOL) bilayers was measured as a function of POPE-to-phospholipid mole ratio (X(PE)) and cholesterol-
49  evaluated in reconstituted bilayers made of POPE/POPS (3.3:1), or POPE/POPS with an added 20% of eit
50       At 30 degrees C, i.e., above the Tm of POPE and POPC, deviations, or dips, as well as local dat
51 rted hexagonal (L - HII) phase transition of POPE.
52 te influence on the two-phase transitions of POPE brings a three-phase coexistence line when the two
53 or palmitoyl-oleoylphosphatidylethanolamine (POPE).
54 ential scanning calorimetric measurements on POPE/POPC liposomes with increasing X(PE) indicated that
55 tuted bilayers made of POPE/POPS (3.3:1), or POPE/POPS with an added 20% of either SPM (3.3:1:1), CER
56 ine and palmitoyloleoylphosphatidylglycerol (POPE/POPG) bilayers] or the red blood cell membrane [neu
57 leoyl-PC (POPC) and 1-palmitoyl-2-oleoyl-PE (POPE) binary mixtures as a function of the POPE mole fra
58 -2-oleoyl-PC (POPC)/1-palmitoyl-2-oleoyl-PE (POPE) mixtures were measured as a function of POPE mole
59                          Chain-perdeuterated POPE and POPG are used in single-component membranes, bi
60 leoyl-sn-glycero-3-phosphatidylethanolamine (POPE) and anionic 1-palmitoyl-2-oleoyl-sn-glycero-3-phos
61 -oleyl-3-n-glycero-phosphatidylethanolamine (POPE) lipid bilayer and its structural properties calcul
62 palmitoyl-2-oleoyl-phosphatidylethanolamine (POPE) and 1-palmitoyl-2-oleoyl-phosphatidylcholine (POPC
63 palmitoyl-2-oleoyl-phosphatidylethanolamine (POPE) in the inner leaflet.
64 palmitoyl-2-oleoyl-phosphatidylethanolamine (POPE) lipid bilayers.
65 palmitoyl 2-oleoyl-phosphatidylethanolamine (POPE); and 3) a mixture of 75% POPE, 20% 1-palmitoyl 2-o
66 of palmitoyloleoyl-phosphatidylethanolamine (POPE) and palmitoyloleoyl-phosphatidylglycerol (POPG) li
67 holesterol with PO phosphatidylethanolamine (POPE) and PO phosphatidylserine (POPS) or with brain PE
68 l-2-oleoyl-sn-glycero-3-phosphoethanolamine (POPE), using differential scanning calorimetry, and sequ
69 l-2-oleoyl-sn-glycero-3-phosphoethanolamine (POPE), with or without rough Escherichia coli LPS (J5),
70 or 1-palmitoyl 2-oleoyl phosphoethanolamine (POPE).
71 t not an oleic acid-containing phospholipid (POPE).
72 of polar headgroup heterogeneity (e.g., POPC/POPE).
73                           In a mixture [POPC/POPE/POPS/PI/ergosterol (30:20:5:20:25)] which mimicked
74      Interaction was also observed with POPC:POPE:cholesterol lipid vesicles (LUV) in equilibrium dia
75           As a Bayesian inference procedure, POPE provides a rigorous framework for the analysis of t
76                In comparison, TAT rigidified POPE and POPG similarly in the binary membrane at ambien
77 less for PDPE-d(31)/SM/CHOL (1:1:1 mol) than POPE-d(31)/SM/CHOL (1:1:1 mol).
78 IB549, caused even larger differences in the POPE and POPG disorder: approximately 80% of POPE partit
79 four to five subunits observed by NMR in the POPE/POPG bilayer.
80 minated the phase separation observed in the POPE/POPS bilayer.
81                    Penetratin maintained the POPE order but disordered POPG, suggesting moderate doma
82 eptide PG-1 ordered approximately 40% of the POPE lipids while disordering POPG.
83  (POPE) binary mixtures as a function of the POPE mole fraction (X(PE)) using fluorescence and Fourie
84 liquid-crystalline domain boundaries at this POPE content.
85                       The addition of CHL to POPE/POPS eliminated the phase separation observed in th
86                   Close proximity of CHOL to POPE even in the presence of SM is indicated.
87 d by >50% upon addition of equimolar CHOL to POPE-d(31)/SM (1:1 mol) bilayers.
88 PM but without its bulky polar head group to POPE/POPS, was without effect, as was the addition of CH
89 ayers, while this interaction tightened when POPE (1-hexadecanoyl-2-(9-Z-octadecenoyl)-sn-glycero-3-p

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