


Publications
Regular Articles 

2016 

Constriction by Dynamin: elasticity vs. adhesion
Zachary A. McDargh, Pablo VázquezMontejo, Jemal Guven, and Markus Deserno
Biophys. J. 111, 2470–2480 (2016).
Any cellular fission process is completed when the neck connecting almostseparate membrane compartments is severed. This crucial step is somehow accomplished by proteins from the dynamin family, which polymerize into helical spirals around such necks. Much research has been devoted to elucidating the specifics of that “somehow”, but despite no shortage of ideas, the question is not settled. Pictorially obvious notions of “strangling” or “pushing” are difficult to render in mechanically precise terms. Moreover, since dynamin is a GTPase, it is tempting to speculate that it has a motor activity that assists the necessary severing “action”, but again the underlying mechanics is not obvious. We believe the difficulty to be the mechanically nontrivial nature of confining elastic filaments onto curved surfaces, for which efficient methods to conceptualize the associated forces and torques have only recently appeared. Here we investigate the implications of a conceptually simple yet mechanically challenging model: consider an elastic helical filament confined to a surface mimicking the neck between two membrane compartments, which we assume to take the shape of a catenoid. What can we say about the expected length of such adsorbed filaments, their shapes, and the forces they exert, as a function of the key parameters in the model? While real dynamin is surely more complex, we consider such a minimal model to be the indispensable baseline. Without knowing what such a model can and cannot explain, it is difficult to justify more complex mechanisms, or understand the constraints under which this machinery evolved in the first place. 

Modern simulation approaches in soft matter science:
From fundamental understanding to industrial applications
Festschrift on the occasion of Kurt Kremer’s 60^{th} birthday
Luigi Delle Site, Markus Deserno, Burkhard Dünweg, Christian Holm, Christine Peter, and Harald Pleiner
Eur. Phys. J. Sp. Topics 225, 1317–1321 (2016).
This special topics issue offers a broad perspective on recent theoretical and computational soft matter science, providing state of the art advances in many of its subfields. As is befitting for a discipline as diverse as soft matter, the papers collected here span a considerable range of subjects and questions, but they also illustrate numerous connections into both fundamental science and technological/industrial applications, which have accompanied the field since its earliest days. This issue is dedicated to Kurt Kremer, on the occasion of his 60^{th} birthday, honouring his role in establishing this exciting field and consolidating its standing in the frame of current science and technology.
A link to the whole special issue is can be found under http://link.springer.com/journal/11734/225/8 

Effect of intrinsic curvature and edge tension on the stability of binary mixedmembrane threejunctions
Jasmine M. Gardner, Markus Deserno, and Cameron F. Abrams
J. Chem. Phys. 145, 074901 (2016). (Feature article)
We use a combination of coarsegrained molecular dynamics simulations and theoretical modeling to examine threejunctions in mixed lipid bilayer membranes. These junctions are localized defect lines in which three bilayers merge in such a way that each bilayer shares one monolayer with one of the other two bilayers. The resulting local morphology is nonlamellar, resembling the threefold symmetric defect lines in inverse hexagonal phases, but it regularly occurs during membrane fission and fusion events. We realize a system of junctions by setting up a honeycomb lattice, which in its primitive cell contains two hexagons and four threeline junctions, permitting us to study their stability as well as their line tension. We specifically consider the effects of lipid composition and intrinsic curvature in binary mixtures, which contain a fraction of negatively curved lipids in a curvatureneutral background phase. Threejunction stability results from a competition between the junction and an open edge, which arises if one of the three bilayers detaches from the other two. We show that the stable phase is the one with the lower defect line tension. The strong and opposite monolayer curvatures present in junctions and edges enhance the mole fraction of negatively curved lipids in junctions and deplete it in edges. This lipid sorting affects the two line tensions and in turn the relative stability of the two phases. It also leads to a subtle entropic barrier for the transition between junction and edge that is absent in uniform membranes. 

Breaking a Virus: Identifying Molecular Level Failure Modes of a Viral Capsid by Multiscale Modeling
Venkatramanan Krishnamani, Christoph Globisch, Christine Peter, and Markus Deserno
Eur. Phys. J. Sp. Topics 225, 1757–1774 (2016).
We use coarsegrained (CG) simulations to study the de formation of empty Cowpea Chlorotic Mottle Virus (CCMV) capsids under uniaxial compression, from the initial elastic response up to capsid breakage. Our CG model is based on the MARTINI force field and has been amended by a stabilizing elastic network, acting only within individual proteins, that was tuned to capture the fluctuation spectrum of capsid proteins dimers, obtained from all atom simulations. We have previously shown that this model predicts forcecompression curves that match AFM indentation experiments on empty CCMV capsids. Here we investigate details of the actual breaking events in CCMV capsid during mechanical compression. We present a symmetry classification of all relevant protein contacts and show that they differ significantly in terms of stability. Specifically, we show that interfaces which break readily are precisely those which are believed to form last during assembly, even though some of them might share virtually the same contacts as other nonbreaking interfaces. Specifically, the interfaces that form pentamers of dimers never break, while the virtually identical interface between hexamers of dimers readily do so. Since these units differ in the largescale geometry and, in particular, the coneangle at the center of the 5 or 6fold vertex, we propose that the hexametric unit fails because it is prestressed. This not only suggests that hexamers of dimers form less frequently during the early stages of assembly; it also offers a natural explanation for the wellknown βbarrel motif at the hexametric center as a postaggregation stabilization mechanism. Finally, we identify those amino acid contacts within all key protein interfaces that are most persistent during com pressive deformation of the capsid, thereby providing potential targets for mutation studies aiming to elucidate the key contacts upon which overall stability rests. 

Determining the Lipid Tilt Modulus by Simulating Membrane Buckles
Xin Wang (王昕) and Markus Deserno
J. Phys. Chem. B 120, 6061–6073 (2016).
Lipid tilt affects the energy of membrane deformations on scales comparable to the membrane's thickness. The surface divergence of the tilt field creates a local spontaneous curvature, while tilt itself is quadratically penalized with a strength given by the tilt modulus. Traditionally, this modulus is determined by measuring the power spectrum of lipid orientation fluctuations. Here we present a novel approach which does not rely on fluctuations but instead exploits the fact that curvature gradients induce a tilt field. Its implementation extends a technique previously developed by us for localizing the position of the pivotal plane in buckling simulations, which quantifies the lipid imbalance across segments cut out from a complete buckle. Lipid tilt affects this count in a predictable way, and the signal can be quantified well enough to back out the tilt modulus—at no additional cost and with about 5% precision for not too coarse models. We apply our technique to three lipid models of very different resolution: the highly coarse grained Cooke model, and two versions of DMPC, using both the (less highly coarse grained) MARTINI and the (united atom) Berger force field. For Cooke we find an effective bilayer tilt modulus of 29±9 pN/nm, and for the less generic DMPC lipid we find 115±6 pN/nm for MARTINI and 39±2 pN/nm for Berger, both in reasonable agreement with existing studies for these models. We also show that the position of the pivotal plane for Berger DMPC lies just below the glycerol backbone—unlike for MARTINI DMPC, where this plane lies closer to the middle of the lipid. 

2015 

Folding and insertion thermodynamics of the transmembrane WALP peptide
Tristan Bereau, W. F. Drew Bennett, Jim Pfaendtner, Markus Deserno, and Mikko Karttunen
J. Chem. Phys. 143, 243127 (2015).
The anchor of most integral membrane proteins consists of one or several helices spanning the lipid bilayer. The WALP peptide, GWW(LA)_{n}(L)WWA, is a common model helix to study the fundamentals of protein insertion and folding, as well as helixhelix association in the membrane. Its structural properties have been illuminated in a large number of experimental and simulation studies. In this combined coarsegrained and atomistic simulation study, we probe the thermodynamics of a single WALP peptide, focusing on both the insertion across the watermembrane interface, as well as folding in both water and a membrane. The potential of mean force characterizing the peptide's insertion into the membrane shows qualitatively similar behavior across peptides and three force fields. However, the Martini force field exhibits a pronounced secondary minimum for an adsorbed interfacial state, which may even become the global minimum—in contrast to both atomistic simulations and the alternative PLUM force field. Even though the two coarsegrained models reproduce the free energy of insertion of individual amino acids side chains, they both underestimate its corresponding valu for the full peptide (as compared with atomistic simulations), hinting at cooperative physics beyond the residue level. Folding of WALP in the two environments indicates the helix as the most stable structure, though with different relative stabilities and chainlength dependence. 

Determining the pivotal plane of fluid lipid membranes in simulations
Xin Wang (王昕) and Markus Deserno
J. Chem. Phys. 143, 164109 (2015).
Each leaflet of a curved lipid membrane contains a surface at which the area strain vanishes, the socalled pivotal plane. Its distance z_{0} from the bilayer's midplane arises in numerous contexts, for instance the connection between monolayer and bilayer moduli, stressprofile moments, or areadifference elasticity theories. Here we propose two precise methods for determining the location of the pivotal plane in computer simulations, both of which rely on monitoring the lipid imbalance across a curved bilayer. The first method considers the ratio of lipid number between the two leaflets of cylindrical or spherical vesicles; it hence requires lipid flipflop for equilibration. The second method looks at the leaflet difference across local sections cut out from a buckled membrane; this observable equilibrates even in the absence of flipflop. We apply our methods to two different coarsegrained lipid models, the generic threebead solventfree Cooke model, and a tenbead representation of dimyristoylphosphocholine (DMPC) with the explicit solvent MARTINI model. The Cooke model is amenable to both methods and gives results that agree at the percent level. Using it, we also show that the pivotal plane moves outward as lipid curvature becomes more positive. The MARTINI model can only be analyzed with the buckling method; the obtained value z_{0}=0.850(11)nm lies about 0.4nm inwards of the glycerol backbone and is hence unexpectedly small. We attribute this to limitations of the coarsegrained description, suggesting that the location of the pivotal plane might be a good indicator for how well lipid models capture the microscopic origins of curvature elasticity. Finally, we also show that the pivotal plane position itself moves as the membrane is bent. The leading correction is linear in curvature, dependent on the Poisson ratio, and can matter when analyzing experimental results obtained from highly curved inverse hexagonal phases. 

Curvature softening and negative compressibility of gelphase lipid membranes
Patrick Diggins, Zachary A. McDargh, and Markus Deserno
J. Am. Chem. Soc. 137, 12752–12755 (2015).
We show that gelphase lipid membranes soften upon bending, leading to curvature localization and a negative compressibility. Using simulations of two very different lipid models to quantify shape and stressstrain relation of buckled membranes, we demonstrate that gel phase bilayers do not behave like Euler elastica and hence are not well described by a quadratic Helfrich Hamiltonian—much unlike their fluidphase counterparts. We propose a theoretical framework which accounts for the observed softening through an energy density that smoothly crosses over from a quadratic to a linear curvature dependence beyond a critical new scale ℓ^{1}. This simple model captures both the shape and the stressstrain relation for our two sets of simulations and permits the extraction of bending moduli, which are found to be about an order of magnitude larger than the corresponding fluid phase values. We also find surprisingly large crossover lengths ℓ, several times bigger than the bilayer thickness, rendering the exotic elasticity of gelphase membranes more strongly pronounced than that of homogeneous compressible sheets and even artificial metamaterials. We therefore suggest that such membranes have unexpected potential as nanoscale systems with striking materials characteristics. 

Design Principles for Nanoparticles Enveloped by a PolymerTethered Lipid Membrane
Mingyang Hu, Francesca Stanzione, Amadeu K. Sum, Roland Faller, and Markus Deserno
ACS Nano 9, 9942–9954 (2015).
We propose the design for a nanoparticle carrier that combines three existing motifs into a single construct: a liposome is stabilized by anchoring it to an enclosed solid core via extended polymeric tethers that are chemically grafted to the core and physisorb into the surrounding lipid membrane. Such a design would exhibit several enticing properties, among them: (i) the anchoring stabilizes the liposome against a variety of external stresses, while preserving an aqueous compartment between core and membrane; (ii) the interplay of design parameters such as polymer length or grafting density enforces strong constraints on nanoparticle size and hence ensures a high degree of uniformity; and (iii) the physical and chemical characteristics of the individual constituents equip the construct with numerous functionalities that can be exploited in many ways. However, navigating the large parameter space requires a sound prior understanding for how various design features work together, and how this impacts potential pathways for synthesizing and assembling these nanoparticles. In this paper we examine these connections in detail, using both soft matter theory and computer simulations at all levels of resolution. We thereby derive strong constraints on the experimentally relevant parameter space, and also propose potential equilibrium and nonequilibrium pathways for nanoparticle assembly. 

Cylindrical confinement of semiflexible polymers
Pablo VázquezMontejo, Zachary McDargh, Markus Deserno, and Jemal Guven
Phys. Rev. E 91, 063203 (2015).
Equilibrium states of a closed semiflexible polymer binding to a cylinder are described. This may be either by confinement or by constriction. Closed completely bound states are labeled by two integers: the number of oscillations, n, and the number of times it winds the cylinder, p, the latter being a topological invariant. We examine the behavior of these states as the length of the loop is increased by evaluating the energy, the conserved axial torque, and the contact force. The ground state for a given p is the state with n = 1; a short loop with p = 1 is an elliptic deformation of a parallel circle; as its length increases it elongates along the cylinder axis with two hairpin ends. Excited states with n ≥ 2 and p = 1 possess nfold axial symmetry. Short (long) loops possess energies E ≈ pE_{0} (nE_{0}), with E_{0} the energy of a circular loop with same radius as the cylinder; in long loops the axial torque vanishes. Confined bound excited states are initially unstable; however, above a critical length each nfold state becomes stable: The folded hairpin cannot be unfolded. The ground state for each p is also initially unstable with respect to deformations rotating the loop off the surface into the interior. A closed planar elastic curve aligned along the cylinder axis making contact with the cylinder on its two sides is identified as the ground state of a confined loop. Exterior bound states behave very differently, if free to unbind, as signaled by the reversal in the sign of the contact force. If p = 1, all such states are unstable. If p ≥ 2, however, a topological obstruction to complete unbinding exists. If the loop is short, the bound state with p = 2 and n = 1 provides a stable constriction of the cylinder, partially unbinding as the length is increased. This motif could be relevant to an understanding of the process of membrane fission mediated by dynamin rings. 

Fluid lipid membranes: From differential geometry to curvature stresses
Markus Deserno
Chem. Phys. Lipids, 185, 11–45 (2015).
A fluid lipid membrane transmits stresses and torques that are fully determined by its geometry. They can be described by a stress and torquetensor, respectively, which yield the force or torque per length through any curve drawn on the membrane's surface. In the absence of external forces or torques the surface divergence of these tensors vanishes, revealing them as conserved quantities of the underlying EulerLagrange equation for the membrane's shape. This review provides a comprehensive introduction into these concepts without assuming the reader's familiarity with differential geometry, which instead will be developed as needed, relying on little more than vector calculus. The Helfrich Hamiltonian is then introduced and discussed in some depth. By expressing the quest for the energyminimizing shape as a functional variation problem subject to geometric constraints, as proposed by Guven [J. Phys. A: Math. Gen. 37, L313–9 (2004)], stress and torque tensors naturally emerge, and their connection to the shape equation becomes evident. How to reason with both tensors is then illustrated with a number of simple examples, after which this review concludes with four more sophisticated applications: boundary conditions for adhering membranes, corrections to the classical micropipette aspiration equation, membrane buckling, and membrane mediated interactions. 

Enhanced Sampling of CoarseGrained TransmembranePeptide Structure Formation from HydrogenBond Replica Exchange
Tristan Bereau and Markus Deserno
J. Membrane Biol. 248, 395–405 (2015).
Protein structure formation in the membrane highlights a grand challenge of sampling in computer simulations, because kinetic traps and slow dynamics make it difficult to find the native state. Exploiting increased fluctuations at higher temperatures can help overcome freeenergy barriers, provided the membrane's structure remains stable. In this work, we apply Hamiltonian replicaexchange molecular dynamics, where we only tune the backbone hydrogenbond strength to help reduce the propensity of longlived misfolded states. Using a recently developed coarsegrained model, we illustrate the robustness of the method by folding different WALP transmembrane helical peptides starting from stretched, unstructured conformations. We show the efficiency of the method by comparing to simulations without enhanced sampling, achieving folding in one example after significantly longer simulation times. Analysis of the bilayer structure during folding provides insight into the local membrane deformation during helix formation as a function of chain length (from 16 to 23 residues). Finally, we apply our method to fold the 50residuelong major pVIII coat protein (fd coat) of the filamentous fd bacteriophage. Our results agree well with experimental structures and atomistic simulations based on implicit membrane models, suggesting that our explicit CG folding protocol can serve as a starting point for betterrefined atomistic simulations in a multiscale framework. 

2014 

An effective field theory of thermal Casimir interactions between anisotropic particles
Robert C. Haussman and Markus Deserno
Phys. Rev. E 89, 062102 (2014).
We employ an effective field theory (EFT) approach to study thermal Casimir interactions between objects bound to a fluctuating fluid surface or interface dominated by surface tension, with a focus on the effects of anisotropic particles. The EFT prescription disentangles the constraints imposed by the particles' boundaries from the calculation of the interaction free energy by constructing an equivalent point particle description. The finitesize information is captured in a derivative expansion that encodes the particles' response to external fields. The coefficients of the expansion terms correspond to generalized polarizabilities and are found by matching the results of a linear response boundary value problem computed in both the full and effective theories. We demonstrate the versatility of the EFT approach by constructing the general effective Hamiltonian for a collection of particles of arbitrary shapes. Taking advantage of the conformal symmetry of the Hamiltonian, we discuss a straightforward conformal mapping procedure to systematically determine the polarizabilities and derive a complete description for elliptical particles. We compute the pairwise interaction energies to several orders for nonidentical ellipses as well as their leadingorder triplet interactions. The resulting preferred pair and multibody configurations are discussed. 

More than the Sum of its Parts: CoarseGrained PeptideLipid Interactions from a Simple CrossParametrization
Tristan Bereau, ZunJing Wang, and Markus Deserno
J. Chem. Phys. 140, 115101 (2014). (Feature article)
Interfacial systems are at the core of fascinating phenomena in many disciplines, such as biochemistry, softmatter physics, and food science. However, the parametrization of accurate, reliable, and consistent coarsegrained (CG) models for systems at interfaces remains a challenging endeavor. In the present work we explore to what extent two independently developed solventfree CG models of peptides and lipids—of different mapping schemes, parametrization methods, target functions, and validation criteria—can be combined by only tuning the cross interactions. Our results show that the crossparametrization can reproduce a number of structural properties of membrane peptides (for example tilt and hydrophobic mismatch), in agreement with existing peptidelipid CG force fields. We find encouraging results for two challenging biophysical problems: (i) membrane pore formation mediated by the cooperative action of several antimicrobial peptides, and (ii) the insertion and folding of the helixforming peptide WALP23 in the membrane. 

The Effective Field Theory approach towards\\ membranemediated interactions between particles
Cem Yolcu, Robert C. Haussman, and Markus Deserno
Adv. Colloid Interface Sci. 208, 89–109 (2014).
Fluid lipid membranes can mediate forces between particles bound to them: A local deformation of the surface geometry created by some object spreads to distant regions, where other objects can respond to it. The physical characteristics of these geometric interactions, and how they are affected by thermal fluctuations, are well described by the simple continuum curvatureelastic Hamiltonian proposed 40 years ago by Wolfgang Helfrich. Unfortunately, while the underlying principles are conceptually straightforward, the corresponding calculations are not—largely because one must enforce boundary conditions for finitesized objects. This challenge has inspired several heuristic approaches for expressing the problem in a point particle language. While streamlining the calculations of leading order results and enabling predictions for higher order corrections, the ad hoc nature of the reformulation leaves its domain of validity unclear. In contrast, the framework of Effective Field Theory (EFT) provides a systematic way to construct a completely equivalent point particle description. In this review we present a detailed account for how this is accomplished. In particular, we use a familiar example from electrostatics as an analogy to motivate the key steps needed to construct an EFT, most notably capturing finite size information in pointlike "polarizabilities," and determining their value through a suitable "matching procedure." The interaction (free) energy then emerges as a systematic cumulant expansion, for which powerful diagrammatic techniques exist, which we also briefly revisit. We then apply this formalism to derive series expansions for interactions between flat and curved particle pairs, multibody interactions, as well as corrections to all these interactions due to thermal fluctuations. 

2013 

Computational Studies of Biomembrane Systems: Theoretical Considerations, Simulation Models, and Applications
Markus Deserno, Kurt Kremer, Harald Paulsen, Christine Peter, and Friederike Schmid
Adv. Polym. Sci., 1–47 (2013).
This chapter summarizes several approaches combining theory, simula tion, and experiment that aim for a better understanding of phenomena in lipid bilayers and membrane protein systems, covering topics such as lipid rafts, membranemediated interactions, attraction between transmembrane proteins, and aggregation in biomembranes leading to large superstructures such as the light harvesting complex of green plants. After a general overview of theoretical con siderations and continuum theory of lipid membranes we introduce different options for simulations of biomembrane systems, addressing questions such as: What can be learned from generic models? When is it expedient to go beyond them? And, what are the merits and challenges for systematic coarse graining and quasiatomistic coarsegrained models that ensure a certain chemical specificity? 

Determining the bending modulus of a lipid membrane by simulating buckling
Mingyang Hu (胡明暘), Patrick Diggins IV, and Markus Deserno
J. Chem. Phys. 138, 214110 (2013).
The force needed to buckle a thin elastic surface is proportional to its bending rigidity. This fact suggests using a buckling setup to measure the bending modulus of lipid membranes. Extending the work of Noguchi [Phys. Rev. E 83, 061919 (2011)], we systematically derive highly accurate analytical expressions for the forces along and perpendicular to the buckle, and we elucidate some of their counterintuitive properties using the framework of a surface stress tensor. Furthermore, we estimate the corrections to buckling forces due to thermal fluctuations and find them significant only for stresses along the ridges. We then apply this buckling protocol to four different lipid membrane models, which widely differ in their level of resolution and the treatment of solvent, and show that in all cases buckling is a reliable and accurate means for measuring their rigidity. Finally, we show that monitoring both stresses and energies during a simulation offers additional insights into the thermodynamics of curvature elasticity and permits one to predict the bending rigidity for a range of temperatures around the actual simulation temperature. 

Optimization of an Elastic Network Augmented Coarse Grained Model to Study CCMV Capsid Deformation
Christoph Globisch, Venkatramanan Krishnamani, Markus Deserno, and Christine Peter
PLOS ONE, 8(4): e60582. doi:10.1371/journal.pone.0060582.
The major protective coat of most viruses is a highly symmetric protein capsid that forms spontaneously from many copies of identical proteins. Structural and mechanical properties of such capsids, as well as their selfassembly process, have been studied experimentally and theoretically, including modeling efforts by computer simulations on various scales. Atomistic models include specific details of local protein binding but are limited in system size and accessible time, while coarse grained (CG) models do get access to longer time and length scales but often lack the specific local interactions. Multiscale models aim at bridging this gap by systematically connecting different levels of resolution. Here, a CG model for CCMV (Cowpea Chlorotic Mottle Virus), a virus with an icosahedral shell of 180 identical protein monomers, is developed, where parameters are derived from atomistic simulations of capsid protein dimers in aqueous solution. In particular, a new method is introduced to combine the MARTINI CG model with a supportive elastic network based on structural fluctuations of individual monomers. In the parametrization process, both network connectivity and strength are optimized. This elasticnetwork optimized CG model, which solely relies on atomistic data of small units (dimers), is able to correctly predict interprotein conformational flexibility and properties of larger capsid fragments of 20 and more subunits. Furthermore, it is shown that this CG model reproduces experimental (Atomic Force Microscopy) indentation measurements of the entire viral capsid. Thus it is shown that one obvious goal for hierarchical modeling, namely predicting mechanical properties of larger protein complexes from models that are carefully parametrized on elastic properties of smaller units, is achievable. 

Gaussian curvature elasticity determined from global shape transformations and local stress distributions: a comparative study using the MARTINI model
Mingyang Hu, Djurre H. de Jong, Siewert J. Marrink, and Markus Deserno
Faraday Discuss. 161, 365–382 (2013).
We calculate the Gaussian curvature modulus
κ of a systematically coarsegrained (CG) onecomponent lipid membrane by applying the method recently proposed by Hu et al. [Biophys. J., 2012, 102, 1403] to the MARTINI representation of 1,2dimyristoylsnglycero3phosphocholine (DMPC). We find the value
κ/κ= –1.04∓0.03 for the elastic ratio between the Gaussian and the mean curvature modulus and deduce
κ_{m}/κ_{m}= –0.95∓0.09 for the monolayer elastic ratio, where the latter is based on plausible assumptions for the distance z_{0} of the monolayer neutral surface from the bilayer midplane and the spontaneous lipid curvature K_{0m}. By also analyzing the lateral stress profile σ_{0}(z) of our system, two other lipid types and pertinent data from the literature, we show that determining K_{0m} and
κ through the first and second moment of σ_{0}(z) gives rise to physically implausible values for these observables. This discrepancy, which we previously observed for a much simpler CG model, suggests that the moment conditions derived from simple continuum assumptions miss the effect of physically important correlations in the lipid bilayer.


2012 

Membranemediated interactions between rigid inclusions: An effective field theory
Cem Yolcu and Markus Deserno
Phys. Rev. E 86, 031906 (2012).
An approach based on effective field theory (EFT) is discussed and applied to the problem of surfacemediated interactions between rigid inclusions of circular footprint on a membrane. Instead of explicitly constraining the surface fluctuations in accord with the boundary conditions around the inclusions, the EFT formalism rewrites the theory; the Hamiltonian of a freely fluctuating surface is augmented by pointwise localized terms that capture the same constraints. This allows one to compute the interaction free energy as an asymptotic expansion in inverse separations in a systematic, efficient and transparent way. Both entropic (fluctuationinduced, Casimirlike) and curvatureelastic (groundstate) forces are considered. Our findings include higher order corrections to known asymptotic results, both on the pair and multibody level. We also found that the few previous at tempts in the literature at predicting subleading orders missed some terms due to an uncontrolled pointparticle approximation. 

Hemifusion of giant unilamellar vesicles with planar hydrophobic surfaces: A fluorescence microscopy study
Goh Haw Zan, Cheemeng Tan, Markus Deserno, Frederick Lanni, and Mathias Lösche
Soft Matter 8, 10877–10886 (2012).
Vesicle adhesion and fusion to interfaces are frequently used for the construction of biomimetic surfaces in biosensors and drug delivery. Ubiquitous in cell biology, vesicle fusion involves the transformation of two separate membranes into one contiguous lipid bilayer. In distinction, the deposition of vesicle membranes to hydrophobic surfaces requires the transformation of a lipidic bilayer into a monomolecular layer—a topologically distinct process termed hemifusion. Here, we used hydrophobically terminated selfassembled monolayers (SAM) on solid surfaces to track the fusion of fluorescently labeled giant unilamellar vesicles (GUVs) at the single vesicle level with video time resolution (≈ 53 ms). We observed that a dilute monolayer, consisting of lipid abstracted from the outer GUV leaflet, spreads outward across the hydrophobic surface from the vesicle adhesion site. Subsequently, bilayer fusion occurs by vesicle rupture near the hydrophobic surface, followed by spreading of lipid in a dense monolayer. GUV lipids thus transfer to the SAM surface in two concentric zones: an outer fusion zone comprises lipids drawn from the outer GUV leaflet; an inner fusion zone comprises lipids from both the inner and outer GUV leaflets and grows at a rate of ≈ 1000 μm^{2}/s (dA/dt = 970 ± 430 μm^{2}/s in n = 22 independent experiments). This growth rate is quantitatively consistent with the assumption that the spreading of the monolayer is entirely driven by the difference in surface energies of the hydrophobic and the lipidcovered SAM surfaces, which is dissipated by friction of the spreading monolayer on the SAM. Lipid transfer between the inner and outer GUV leaflets occurs via a hemifusion pore that forms early in the process near the membrane contact site. This pore also permits expulsion of water from the GUV interior as the vesicle contracts onto the contact site. 

CoarseGrained and Atomistic Simulations of the SaltStable Cowpea Chlorotic Mottle Virus (SSCCMV) Subunit 26–49: βBarrel Stability of the Hexamer and Pentamer Geometries
Tristan Bereau, Christoph Globisch, Markus Deserno, and Christine Peter
J. Chem. Theory Comput. 8, 3750–3758 (2012).
A combination of coarsegrained (CG) and atomistic simulations provides a suitable computational framework to study unstructured regions of proteins, for which experimental data are often lacking or limited. In this work, we combine CG and atomistic simulations with clustering algorithms and free energy reweighting methods to explore the conformational equilibrium of certain regions of the saltstable cowpea chlorotic mottle virus (SSCCMV). In particular, we focus on the geometry of converging strands (residues 26–49) from contacting subunits at the 3fold (hexamer) and 5fold (pentamer) symmetry points of the capsid. We show the following: (i) The simulations reproduce the experimentally observed βbarrel for the hexamer. (ii) The pentamer geometry is unable to stabilize a βbarrel conformation; it assumes various states instead, again in accordance with the experimental results which do not indicate a welldefined structure for the pentameric interface. (iii) Atomistic simulations of the backmapped CG structures remain relatively stable, indicative of plausible CG conformations and slow kinetics on the atomistic level. 

Determining the Gaussian curvature modulus in simulations
Mingyang Hu, John J. Briguglio, and Markus Deserno
Biophys. J. 102, 1403–1410 (2012).
The Gaussian curvature modulus κ' of lipid bilayers likely contributes more than 100 kcal/mol to every cellular fission or fusion event. This huge impact on membrane remodeling energetics might be a factor that codetermines the complex lipid composition of biomembranes through tuning of κ'. Yet, its value has been measured only for a handful of simple lipids, and no simulation has so far determined it better than a factor of two, rendering a systematic investigation of such enticing speculations impossible.
Here we propose a highly accurate method to determine κ' in computer simulations. It relies on the interplay between curvature stress and edge tension of partially curved axisymmetric membrane discs and requires determining their closing probability.
For a simplified lipid model we obtain κ' and its relation to the normal bending modulus κ for membranes differing both in stiffness and spontaneous lipid curvature. The elastic ratio κ'/κ can be determined with a few percent statistical accuracy. Its value agrees with the scarce experimental data, and its change with spontaneous lipid curvature is compatible with theoretical expectations, thereby granting additional information on monolayer properties. We also show that an alternative determination of these elastic parameters based on moments of the lateral stress profile gives markedly different and unphysical values. 

Effective field theory approach to fluctuationinduced forces between colloids at an interface
Cem Yolcu, Ira Z. Rothstein, and Markus Deserno
Phys. Rev. E 85, 011140 (2012).
We discuss an effective field theory (EFT) approach to the computation of fluctuationinduced interactions between particles bound to a thermally fluctuating fluid surface controlled by surface tension. By describing particles as points, EFT avoids computing functional integrals subject to difficult constraints. Still, all information pertaining to particle size and shape is systematically restored by amending the surface Hamiltonian with a derivative expansion. The free energy is obtained as a cumulant expansion, for which straightforward techniques exist. We derive a completedescription for rigid axisymmetric objects, which allows us to develop a full asymptotic expansion—in powers of the inverse distance—for the pair interaction. We also demonstrate by a few examples the efficiency with which multibody interactions can be computed. Moreover, although the main advantage of the EFT approach lies in explicit computation, we discuss how one can infer certain features of cases involving flexible or anisotropic objects. The EFT description also permits a systematic computation of groundstate surfacemediated interactions, which we illustrate with a few examples. 

2011 

Effective field theory approach to Casimir interactions on soft matter surfaces
Cem Yolcu, Ira Z. Rothstein, and Markus Deserno
Europhys. Lett. 96 20003 (2011).
A shorter version can also be found here: arXiv:1007.4760v2 [condmat.soft]
We utilize an effective field theory approach to calculate Casimir interactions between
objects bound to thermally fluctuating fluid surfaces or interfaces. This approach circumvents
the complicated constraints imposed by such objects on the functional integration measure by
reverting to a point particle representation. To capture the finitesize effects, we augment the
Hamiltonian by a term ΔH that encapsulates the particles' response to external fields. ΔH is
systematically expanded in a series of terms, each of which scales homogeneously in the two power
counting parameters: λ = R/r, the ratio of the typical object size (R) to the typical distance
between them (r), and δ = k_{B}T/k, where k is the modulus characterizing the surface energy. The
coefficients of the terms in ΔH correspond to generalized polarizabilities and thus the formalism
applies to rigid as well as deformable objects. We first illustrate and verify our approach by rederiving known pair forces between circular objects bound to films or membranes. To demonstrate
its efficiency and versatility, we then derive a number of new results, among them the triplet
interactions present in these systems, a higherorder correction to the film interaction, and general
scaling laws for the leadingorder interaction valid for objects of arbitrary shape and internal
flexibility. 

Membrane mediated interactions between circular particles in the strongly curved regime
Benedict J. Reynwar and Markus Deserno
Soft Matter 7, 8567–8575 (2011).
Particles binding to a fluid lipid membrane can induce bilayer deformations, for instance when these particles are curved.
Since the energy of two overlapping warp fields depends on the mutual distance between the two particles creating them, they will
experience forces mediated by the curvature of the membrane. If the deformations are sufficiently weak, the associated differential
equations for the membrane shape are linear, and the resulting interactions are understood very well; but for stronger curvature
imprint very little is known, owing to the highly nonlinear nature of the problem. Here we numerically calculate the magnitude
of such membranemediated interactions in the case of two axisymmetric particles over a wide range of curvature imprints, deep
into the nonlinear regime. We show that over an intermediate distance range the sign of the force reverses beyond a sufficiently
strong deformation. These findings are quantitatively confirmed by a simple analytical closedistance expansion. The sign flip
can be traced to a change in magnitude between the two principal curvatures midway between the two particles, which can only
occur at sufficient particle tilt, a condition which is by construction ruled out in the linearized description. We also show these
large perturbation results to agree with coarsegrained molecular dynamics simulations and suggest that a favorable comparison
is indeed more likely to hold in the strongly deformed regime. 

Structural basis of Folding Cooperativity in Model Proteins: Insights from a Microcanonical Perspective
Tristan Bereau, Markus Deserno, and Michael Bachmann
Biophys. J. 100, 2764–2772 (2011).
Twostate cooperativity is an important characteristic in protein folding. It is defined by a depletion of states that lie energetically between folded and unfolded conformations. There are different ways to test for twostate cooperativity; however, most of these approaches probe indirect proxies of this depletion. Generalizedensemble computer simulations allow us to unambiguously identify this transition by a microcanonical analysis on the basis of the density of states. Here, we present a detailed characterization of several helical peptides obtained by coarsegrained simulations. The level of resolution of the coarsegrained model allowed to study realistic structures ranging from small α–helices to a de novo threehelix bundle without biasing the force field toward the native state of the protein. By linking thermodynamic and structural features, we are able to show that whereas short α–helices exhibit twostate cooperativity, the type of transition changes for longer chain lengths because the chain forms multiple helix nucleation sites, stabilizing a significant population of intermediate states. The helix bundle exhibits signs of twostate cooperativity owing to favorable helixhelix interactions, as predicted from theoretical models. A detailed analysis of secondary and tertiary structure formation fits well into the framework of several folding mechanisms and confirms features that up to now have been observed only in lattice models. 

2010 

Systematic implicit solvent coarsegraining of bilayer membranes:
lipid and phase transferability of the force field
ZunJing Wang and Markus Deserno
New Journal of Physics 12, 095004 (2010).
We study lipid and phase transferability of our recently developed systematically coarsegrained solventfree membrane model. The force field was explicitly parametrized to describe a fluid 1palmitoyl2oleoylphosphatidylcholine (POPC) bilayer at 310 K with correct structure and area per lipid, while gaining at least three orders of magnitude in computational effciency (see Ref. 1).
Here we show that exchanging CG tails, without any subsequent reparameterization, creates reliable models of 1,2dioleoylphosphatidylcholine (DOPC) and 1,2dipalmitoylphosphatidylcholine
(DPPC) lipids in terms of structure and area per lipid. Furthermore, all CG lipids undergo a liquidgel transition upon cooling, with characteristics as observed in experiments and allatom
simulations during phase transformation. These studies suggest a promising transferability of our force field parameters to different lipid species and thermodynamic statepoints, properties that
are prerequisite for even more complex systems, such as mixtures. 

Interplay between secondary and tertiary structure formation in protein folding cooperativity
Tristan Bereau, Michael Bachmann, and Markus Deserno
J. Am. Chem. Soc. 132, 13129–13131 (2010).
Protein folding cooperativity is defined by the nature of the finitesize thermodynamic transition exhibited upon folding: twostate transitions
show a free energy barrier between the folded and unfolded ensembles, while downhill folding is barrierless. A microcanonical analysis,
where the energy is the natural variable, has shown better suited to unambiguously characterize the nature of the transition compared to its
canonical counterpart. Replica exchange molecular dynamics simulations of a high resolution coarsegrained model allow for the accurate
evaluation of the density of states, in order to extract precise thermodynamic information, and measure its impact on structural features. The
method is applied to three helical peptides: a short helix shows sharp features of a twostate folder, while a longer helix and a threehelix
bundle exhibit downhill and twostate transitions, respectively. Extending the results of lattice simulations and theoretical models, we find
that it is the interplay between secondary structure and the loss of nonnative tertiary contacts which determines the nature of the transition.


Cell Model Approach to Membrane Mediated Protein Interactions
Martin M. Müller and Markus Deserno
Progr. Theor. Phys. Suppl. 184, 351–363 (2010).
Membranedeforming proteins can interact through the curvature fields they create. In the case of many such proteins a cell model approach can be used to calculate the energy per protein and predict, whether it would lead to phase segregation or budformation. Using covariant differential geometry exact results are derived for the lateral pressure in terms of geometric properties at the cell boundary. Numerical solutions of the exact shape equations in the highly nonlinear regime are found and it is seen that both phase segregation and bud formation can occur. 

A systematically coarsegrained solventfree model for quantitative phospholipid bilayer simulations
ZunJing Wang and Markus Deserno
J. Phys. Chem. B 114, 11207 (2010).
We presented an implicit solvent coarsegrained (CG) model for quantitative simulations of
1palmitoyl2oleoylsnglycero3phosphocholine (POPC) bilayers. The use of implicit solvent enables membrane simulations on large length and timescales at moderate computational expense. Despite an improved computational efficiency, the model preserves chemical specificity and quantitative accuracy. The bonded and nonbonded interactions together with the effective cohesion mimicking the hydrophobic effect were systematically tuned by matching structural and mechanical properties from experiments and allatom bilayer simulations, such as saturated area per lipid, radial distribution functions, density and pressure profiles across the bilayer, P_{2} order, etc. The CG lipid model is shown to selfassemble into a bilayer starting from a random dispersion. Its elastic properties, such as bending and stretching modulus, are semiquantitatively consistent with experiments. The effects of (i) reduced molecular friction and (ii) more efficient integration combine to an overall speedup of three to four orders of magnitude compared to allatom bilayer simulations. Our CG lipid model is especially useful for studies of largescale phenomena in membranes which nevertheless require a fair description of chemical specificity, e.g. membrane patches interacting with movable and transformable membrane proteins and peptides. 

Inplane homogeneity and lipid dynamics in tethered Bilayer Lipid Membranes (tBLMs)
Siddharth Shenoy, Radu Moldovan, James Fitzpatrick, David J. Vanderah, Markus Deserno, and Mathias Lösche
Soft Matter 6, 1263 (2010).
Tethered bilayer lipid membranes (tBLMs) were prepared by the selfassembly of thiolated lipidic anchor molecules on gold, followed by phospholipid precipitation via rapid solvent exchange. They were characterized in their inplane structure, dynamics and dielectric properties. We find that the inplane homogeneity and resistivity of the tBLMs depends critically on a wellcontrolled sample environment during the rapid solvent exchange procedure. The inplane dynamics of the systems, assessed by fluorescence correlation spectroscopy (FCS) as the diffusivity of free, labeled phospholipid dissolved in the membrane, depends on the density of the lipidic anchors in the bilayer leaflet proximal to the substrate as well as on details of the molecular structure of the anchor lipid. In DOPC tBLMs in which tethers are laterally dilute (sparselytethered bilayer lipid membranes, stBLMs), measured diffusivities, D ~ 4 μm^{2}/s, are only slightly greater than those reported in physisorbed bilayers. However, when we distinguish label diffusion in the proximal and in the distal bilayer leaflets, we observe distinct diffusivities, D ~ 2 μm^{2}/s and ~ 7 μm^{2}/s, respectively. The value observed in the distal leaflet is identical to that in free membranes. stBLMs completed with phytanoyl lipids (DPhyPC) show consistently lower label diffusivity than those completed with unsaturated chains (DOPC). As the flexibility of the tether chain increases, a reduction in the apparent diffusivityis observed, which we interpret as an increased propensity of the proximal bilayer leaflet to host free lipid. Finally, in laterally heterogeneous bilayers, the label diffusivity varies only by a factor of ~ 2× – 4×, indicating that the distinct regions in the bilayers do not correspond to distinct phases such as a fluid phase coexisting with a gel phase. 

2009 

Generic coarsegrained model for protein folding and aggregation
Tristan Bereau and Markus Deserno
J. Chem. Phys. 130, 235106 (2009).
A generic coarsegrained (CG) protein model is presented. The intermediate level of resolution (four beads per amino acid, implicit solvent) allows for accurate sampling of local conformations. It relies on simple interactions that emphasize structure, such as hydrogen bonds and hydrophobicity. Realistic alpha/beta content is achieved by including an effective nearestneighbor dipolar interaction. Parameters are tuned to reproduce both local conformations and tertiary structures. The thermodynamics and kinetics of a threehelix bundle are studied. We check that the CG model is able to fold proteins with tertiary structures and amino acid sequences different from the one used for parameter tuning. By studying both helical and extended conformations we make sure the force field is not biased toward any particular secondary structure. The accuracy involved in folding not only the test protein but also other ones show strong evidence for amino acid cooperativity embedded in the model. Without any further adjustments or bias a realistic oligopeptide aggregation scenario is observed. 

Multiscale modeling of emergent materials: biological and soft matter
Teemu Murtola, Alex Bunker, Ilpo Vattulainen, Markus Deserno, Mikko Karttunen
Phys. Chem. Chem. Phys. 11, 1869–1892 (2009).
In this review, we focus on four current related issues in multiscale modeling of soft and biological matter. First, we discuss how to use structural information from detailed models (or experiments) to construct coarsegrained ones in a hierarchical and systematic way. This is discussed in the context of the socalled Henderson theorem and the inverse Monte Carlo method of Lyubartsev and Laaksonen. In the second part, we take a different look at coarse graining by analyzing conformations of molecules. This is done by the application of selforganizing maps, i.e., a neural network type approach. Such an approach can be used to guide the selection of the relevant degrees of freedom. Then, we discuss technical issues related to the popular dissipative particle dynamics (DPD) method. Importantly, the potentials derived using the inverse Monte Carlo method can be used together with the DPD thermostat. In the final part we focus on solventfree modeling which offers a different route to coarse graining by integrating out the degrees of freedom associated with solvent. 

Mesoscopic Membrane Physics: Concepts, Simulations, and Selected Applications
Markus Deserno
Macromol. Rapid. Comm. 30, 752–771 (2009).
The window of a few tens to a few hundred nanometers in length scale is a booming field in lipid membrane research, owing largely to two reasons. First, many exciting biophysical and cell biological processes take place within it. Second, experimental techniques manage to zoom in on this suboptical scale, while computer simulations zoom out to system sizes previously unattainable, and both will be meeting soon. This paper reviews a selection of questions and concepts in this field and demonstrates that they can often be favorably addressed with highly simplified simulation models. Among the topics discussed are membrane adhesion to substrates, mixed lipid bilayers, lipid curvature coupling, pore formation by antimicrobial peptides, compositiondriven protein aggregation, and curvature driven vesiculation. 

2008 

Membrane compositionmediated proteinprotein interactions
Benedict J. Reynwar, Markus Deserno
Biointerphases 3, FA117 (2008).
The authors investigate membrane compositionmediated interactions between proteins adsorbed onto a twocomponent lipid bilayer close to critical demixing using coarsegrained molecular dynamics simulations and a phenomenological GinzburgLandau theory. The simulations consist of threebead lipids and platelike proteins, which adsorb onto the membrane by binding preferentially to one of the two lipid species. The composition profile around one protein and the pair correlation function between two proteins are measured and compared to the analytical predictions. The theoretical framework is applicable to any scalar field embedded in the membrane, and although in this work the authors treat flat membranes, the methodology extends readily to curved geometries. Neglecting fluctuations, both lipid composition profile and induced protein pair potential are predicted to follow a zeroth order modified Bessel function of the second kind with the same characteristic decay length. These predictions are consistent with our molecular dynamics simulations, except that the interaction range is found to be larger than the single profile correlation length. 

Coarsegrained modeling of interactions of lipid bilayers with supports
Matthew I. Hoopes, Markus Deserno, Margie L. Longo, Roland Faller
J. Chem. Phys. 129, 175102 (2008).
We characterize the differences between supported and unsupported lipid bilayer membranes using a mesoscopic simulation model and a simple particlebased realization for a flat support on to which the lipids are adsorbed. We show that the nanometer roughness of the support affects membrane binding strength very little. We then compare the lipid distributions and pressure profiles of free and supported membranes. The surface localization of the proximal leaflet breaks the symmetry seen in a free bilayer, and we quantify the entropic penalty for binding and the increased lateral compression modulus. 

Adhesion promotes phase separation in mixedlipid membranes
Vernita D. Gordon, Markus Deserno, Carolyn M. J. Andrew, Stefan U. Egelhaaf, Wilson C. K. Poon
Europhys. Lett. 84, 48003 (2008).
We investigate the interplay of domain formation and adhesion in mixedlipid membranes. Giant unilamellar vesicles consisting of two and threecomponent lipid mixtures are studied using confocal fluorescence microscopy. Upon driving the system towards the demixing transition, phase separation is invariably found to occur first in regions where membranes adhere to one another, despite identical lipid headgroups and negligible curvature effects. We propose a simple generic mechanism based on the suppression of thermal shape fluctuations to explain these observations. Our findings suggest novel possibilities by which biomembranes can create and utilize lateral lipid heterogeneities. 

CoarseGrained Simulation Studies of PeptideInduced Pore Formation
Gregoria Illya, Markus Deserno
Biophys. J. 95, 4163–4173 (2008).
We investigate the interactions between lipid bilayers and amphiphilic peptides using a solventfree coarsegrained simulation technique. In our model, each lipid is represented by one hydrophilic and three hydrophobic beads. The amphiphilic peptide is modeled as a hydrophobichydrophilic cylinder with hydrophilic caps. We find that with increasing peptidelipid attraction the preferred state of the peptide changes from desorbed, to adsorbed, to inserted. A single peptide with weak attraction binds on the bilayer surface, while one with strong attraction spontaneously inserts into the bilayer. We show how several peptides, which individually bind only to the bilayer surface, cooperatively insert. Furthermore, hydrophilic strips along the peptide cylinder induce the formation of multipeptide pores, whose size and morphology depend on the peptides' overall hydrophilicity, the distribution of hydrophilic residues, and the peptidepeptide interactions. Strongly hydrophilic peptides insert less readily, but prove to be more destructive to bilayer integrity. 

2007 

Aggregation and vesiculation of membrane proteins by curvaturemediated interactions
Benedict J. Reynwar, Gregoria Illya, Vagelis A. Harmandaris, Martin M. Müller, Kurt Kremer, and Markus Deserno
Nature 447, 461–464 (2007).
Membrane remodelling plays an important role in cellular tasks such as endocytosis, vesiculation and protein sorting, and in the biogenesis of organelles such as the endoplasmic reticulum or the Golgi apparatus. It is well established that the remodelling process is aided by specialized proteins that can sense as well as create membrane curvature, and trigger tubulation when added to synthetic liposomes. Because the energy needed for such largescale changes in membrane geometry significantly exceeds the binding energy between individual proteins and between protein and membrane, cooperative action is essential. It has recently been suggested that curvaturemediated attractive interactions could aid cooperation and complement the effects of specific binding events on membrane remodelling. But it is difficult to experimentally isolate curvaturemediated interactions from direct attractions between proteins. Moreover, approximate theories predict repulsion between isotropically curving proteins. Here we use coarsegrained membrane simulations to show that curvatureinducing model proteins adsorbed on lipid bilayer membranes can experience attractive interactions that arise purely as a result of membrane curvature. We find that once a minimal local bending is realized, the effect robustly drives protein cluster formation and subsequent transformation into vesicles with radii that correlate with the local curvature imprint. Owing to its universal nature, curvaturemediated attraction can operate even between proteins lacking any specific interactions, such as newly synthesized and still immature membrane proteins in the endoplasmic reticulum. 

Contact lines for fluid surface adhesion
Martin M. Müller, M. Deserno, and J. Guven
Phys. Rev. E 76, 011605 (2007); see also condmat/0703019
When a fluid surface adheres to a substrate, the location of the contact line adjusts in order to minimize the overall energy. This implies boundary conditions which depend on the characteristic surface deformation energies. We develop a general geometrical framework within which these conditions can be derived in a completely systematic way. We treat both adhesion to a rigid substrate and adhesion between two fluid surfaces, and illustrate our general results for several important Hamiltonians involving both curvature and curvature gradients. Some of these have previously been studied using very different techniques. With the exception of capillary phenomena, the Hamiltonian will not only be sensitive to boundary translations, but may also respond to changes in slope and even in curvature. The functional form of the additional contributions will follow readily from our treatment. We will show that the boundary conditions describing adhesion between two fluid surfaces express the balance of stresses and torques, as one would expect. At a rigid substrate, however, this simple identification will generally fail. This is because local rotations of the surface normal will be entirely "enslaved" to translations on the substrate. As a consequence, stresses and torques enter a single balance condition and cannot be disentangled. 

Balancing torques in membranemediated interactions: exact results and numerical illustrations
Martin M. Müller, M. Deserno, and J. Guven
Phys. Rev. E 76, 011921 (2007); see also condmat/0702340.
Torques on interfaces can be described by a divergencefree tensor which is fully encoded in the geometry. This tensor consists of two terms, one originating in the couple of the stress, the other capturing an intrinsic contribution due to curvature. In analogy to the description of forces in terms of a stress tensor, the torque on a particle can be expressed as a line integral along a contour surrounding the particle. Interactions between particles mediated by a fluid membrane are studied within this framework. In particular, torque balance places a strong constraint on the shape of the membrane. Symmetric twoparticle configurations admit simple analytical expressions which are valid in the fully nonlinear regime; in particular, the problem may be solved exactly in the case of two membranebound parallel cylinders. This apparently simple system provides some flavor of the remarkably subtle nonlinear behavior associated with membranemediated interactions. 

2006 

A novel method for measuring the bending rigidity of model lipid membranes by simulating tethers
Vagelis A. Harmandaris and Markus Deserno
J. Chem. Phys. 125, 204905 (2006); see also condmat/0611012.
The tensile force along a cylindrical lipid bilayer tube is proportional to the membrane's bending modulus and inversely proportional to the tube radius. We show that this relation, which is experimentally exploited to measure bending rigidities, can be applied with even greater ease in computer simulations. Using a coarsegrained bilayer model we efficiently obtain bending rigidities that compare very well with complementary measurements based on an analysis of thermal undulation modes. We furthermore illustrate that no deviations from simple quadratic continuum theory occur up to a radius of curvature comparable to the bilayer thickness. 

How to determine local elastic properties of lipid bilayer membranes from atomicforcemicroscope measurements: A theoretical analysis
Davood Norouzi, Martin M. Müller, and Markus Deserno
Phys. Rev. E 74, 061914 (2006); see also condmat/0602662.
Measurements with an atomic force microscope (AFM) offer a direct way to probe elastic properties of lipid bilayer membranes locally: provided the underlying stressstrain relation is known, material parameters such as surface tension or bending rigidity may be deduced. In a recent experiment a porespanning membrane was poked with an AFM tip, yielding a linear behavior of the forceindentation curves. A theoretical model for this case is presented here which describes these curves in the framework of Helfrich theory. The linear behavior of the measurements is reproduced if one neglects the influence of adhesion between tip and membrane. Including it via an adhesion balance changes the situation significantly: forcedistance curves cease to be linear, hysteresis and nonzero detachment forces can show up. The characteristics of this rich scenario are discussed in detail in this paper. 

Mechanical properties of porespanning lipid bilayers probed by atomic force microscopy
Siegfried Steltenkamp, Martin M. Müller, Markus Deserno, Christian Hennesthal, Claudia Steinem, and Andreas Janshoff
Biophys. J. 91, 217–226 (2006).
We measure the elastic response of a freestanding lipid membrane to a local indentation by using an atomic force microscope (AFM). Starting point is a planar goldcoated alumina substrate with a chemisorbed 3mercaptopropionic acid monolayer displaying circular pores of very well defined and tunable size, over which N,N,dimethylN,N, dioctadecylammonium bromide or 1,2dioleoyl3trimethylammoniumpropane chloride were spread. Centrally indenting these "nanodrums" with an AFM tip yields forceindentation curves, which we quantitatively analyze by solving the corresponding shape equations of continuum curvature elasticity. Since the measured response depends in a known way on the system geometry (pore size, tip radius) and on material parameters (bending modulus, lateral tension), this opens the possibility to monitor local elastic properties of lipid membranes in a wellcontrolled setting. 

Coupling between lipid shape and membrane curvature
Ira R. Cooke and Markus Deserno
Biophys. J. 91, 487–495 (2006).
Using molecular dynamics simulations, we examine the behavior of lipids whose preferred curvature can be systematically varied. This curvature is imposed by controlling the head group size of a coarse grained lipid model recently developed by us. In order to validate this approach we examine self assembly of each individual lipid type and observe the complete range of expected bilayer and micelle phases. We then examine binary systems consisting of lipids with positive and negative preferred curvature and find a definite sorting effect. Lipids with positive preferred curvature are found in greater proportions in outer monolayers with the opposite observed for lipids with negative preferred curvature. We also observe a similar, but slightly stronger effect for lipids in a developing spherical bud formed by adhesion to a colloid (eg a viral capsid). Importantly, the magnitude of this effect in both cases was large only for regions with strong mean curvature (radii of curvature <10nm). Our results suggest that lipid shape must act in concert with other physicochemical effects such as phase transitions or interactions with proteins to produce strong sorting in cellular pathways.


2005 

Solvent free model for selfassembling fluid bilayer membranes: Stabilization of the fluid phase based on broad attractive tail potentials
Ira R. Cooke and Markus Deserno
J. Chem. Phys. 123, 224710 (2005).
We present a simple and highly adaptable method for simulating coarsegrained lipid membranes without explicit solvent. Lipids are represented by one headbead and two tailbeads, with the interaction between tails being of key importance in stabilizing the fluid phase. Two such tailtail potentials were tested, with the important feature in both cases being a variable range of attraction. We examined phase diagrams of this range versus temperature for both functional forms of the tailtail attraction and found that a certain threshold attractive width was required to stabilize the fluid phase. Within the fluid phase region we find that material properties such as area per lipid, orientational order, diffusion constant, interleaflet flipflop rate and bilayer stiffness all depend strongly and monotonically on the attractive width. For three particular values of the potential width we investigate the transition between gel and fluid phases via heating or cooling and find that this transition is discontinuous with considerable hysteresis. We also investigated the stretching of a bilayer to eventually form a pore and found excellent agreement with recent analytic theory. 

Interface mediated interactions between particles—a geometrical approach
Martin M. Müller, M. Deserno, and J. Guven
Phys. Rev. E 72, 061407 (2005).
Particles bound to an interface interact because they deform its shape. The stresses that result are fully encoded in the geometry and described by a divergencefree surface stress tensor. This stress tensor can be used to express the force on a particle as a line integral along any conveniently chosen closed contour that surrounds the particle. The resulting expression is exact (i.e., free of any "smallness" assumptions) and independent of the chosen surface parametrization. Additional surface degrees of freedom, such as vector fields describing lipid tilt, are readily included in this formalism. As an illustration, we derive the exact force for several important surface Hamiltonians in various symmetric twoparticle configurations in terms of the midplane geometry; its sign is evident in certain interesting limits. Specializing to the linear regime, where the shape can be analytically determined, these general expressions yield forcedistance relations, several of which have originally been derived by using an energy based approach. 

Tunable generic model for fluid bilayer membranes
Ira R. Cooke, Kurt Kremer, and Markus Deserno
Phys. Rev. E 72, 011506 (2005).
We present a model for the efficient simulation of generic bilayer membranes. Individual lipids are represented by one head bead and two tailbeads. By means of simple pair potentials these robustly selfassemble to a fluid bilayer state over a wide range of parameters, without the need for an explicit solvent. The model shows the expected elastic behavior on large length scales, and its physical properties (e.g. fluidity or bending stiffness) can be widely tuned via a single parameter. In particular, bending rigidities in the experimentally relevant range are obtained, at least within 3–30kT. The model is naturally suited to study many physical topics, including selfassembly, fusion, bilayer melting, lipid mixtures, rafts, and proteinbilayer interactions. 

Geometry of surface mediated interactions
Martin M. Müller, M. Deserno, and J. Guven
Europhys. Lett. 69, 482–488 (2005).
Soft interfaces can mediate interactions between particles bound to them. The force transmitted through the surface geometry on a particle may be expressed as a closed line integral of the surface stress tensor around that particle. This contour may be deformed to exploit the symmetries present; for two identical particles, one obtains an exact expression for the force between them in terms of the local surface geometry of their midplane; in the case of a fluid membrane the sign of the interaction is often evident. The approach, by construction, is adapted directly to the surface and is independent of its parameterization. Furthermore, it is applicable for arbitrarily large deformations; in particular, it remains valid beyond the linear smallgradient regime. 

2004 

When do fluid membranes engulf sticky colloids?
Markus Deserno
J. Phys.: Condens. Matter 16, S2061S2070 (2004).
Binding of a spherical colloid to a fluid membrane, which is an interplay between the energies of adhesion and elastic deformation, is studied within the framework of a Helfrich Hamiltonian. The solution of the full nonlinear shape equations for the membrane profile reveals a continuous binding and a discontinuous envelopment transition, the latter with a tension dependent substantial energy barrier. In the bending dominated regime this scenario is analytically confirmed by a small gradient expansion. 

Screening of Spherical Colloids beyond Mean Field—A Local Density Functional Approach
Marcia C. Barbosa, Markus Deserno, Christian Holm, and René Messina
Phys. Rev. E 69, 051401 (2004).
We study the counterion distribution around a spherical macroion and its osmotic pressure in the framework of the recently developed DebyeHückelHoleCavity (DHHC) theory. This is a local density functional approach which incorporates correlations into PoissonBoltzmann theory by adding a free energy correction based on the One Component Plasma. We compare the predictions for ion distribution and osmotic pressure obtained by the full theory and by its zero temperature limit with Monte Carlo simulations. They agree excellently for weakly developed correlations and give the correct trend for stronger ones. In all investigated cases the DHHC theory and its computationally simpler zero temperature limit yield better results than the PoissonBoltzmann theory. 

Twistbend instability for toroidal DNA condensates
Igor M. Kulic, Denis Andrienko, and Markus Deserno
Europhys. Lett. 67, 418–424 (2004).
We propose that semiflexible polymers in poor solvent collapse in two stages. The first stage is the well known formation of a dense toroidal aggregate. However, if the solvent is sufficiently poor, the condensate will undergo a second structural transition to a twisted entangled state, in which individual filaments lower their bending energy by additionally orbiting around the mean path along which they wind. This ``topological ripening'' is consistent with known simulations and experimental results. It connects and rationalizes various experimental observations ranging from strong DNA entanglement in viral capsids to the unusually short pitch of the cholesteric phase of DNA in spermheads. We propose that topological ripening of DNA toroids could improve the efficiency and stability of gene delivery.


A StatisticalThermodynamic Model of Viral Budding
Shelly Tzlil, Markus Deserno, William M. Gelbart, and Avinoam BenShaul
Biophys. J. 86, 2037–2048 (2004).
We present a simple statistical thermodynamic model for budding of viral nucleocapsids at the cell membrane. The membrane is modeled as a flexible lipid bilayer embedding linker (``spike'') proteins, which serve to anchor and thus wrap the membrane around the viral capsids. The free energy of a single bud is expressed as a sum of the bending energy of its membrane coat, the spikemediated capsidmembrane adhesion energy, and the line energy associated with the bud's rim; all depending on the extent of wrapping (i.e., bud size), and density of spikes in the curved membrane. This ``selfenergy'' is incorporated into a simple free energy functional for the manybud system, allowing for different spike densities, and hence entropy, in the curved (budding) and planar membrane regions, as well as for the configurational entropy of the polydisperse bud population. The equilibrium spike densities in the coexisting, curved and planar, membrane regions are calculated as a function of the membrane bending energy and the spikemediated adhesion energy, for different spike and nucleocapsid concentrations in the membrane plane, as well as for several values of the bud's rim energy. We show that complete budding (full wrapping of nucleocapsids) can only take place if the adhesion energy exceeds a certain, critical, bending free energy. Whenever budding takes place, the spike density in the mature virions is saturated, i.e., all spike adhesion sites are occupied. The rim energy plays an important role in determining the size distribution of buds. The fraction of fully wrapped buds increases as this energy increases, resulting eventually in an ``all or nothing'' mechanism, whereby nucleocapsids at the plasma membrane are either fully enveloped or completely ``naked'' (just touching the membrane). We also find that at low concentrations all capsids arriving at the membrane get tightly and fully enveloped. Beyond a certain concentration, corresponding approximately to a ``stoichiometric'' spiketocapsid ratio, newly arriving capsids cannot be fully wrapped, i.e., the budding yield decreases. 

Elastic deformation of a fluid membrane upon colloid binding
Markus Deserno
Phys. Rev. E 69, 031903 (2004).
When a colloidal particle adheres to a fluid membrane, it induces elastic deformations in the membrane which oppose its own binding. The structural and energetic aspects of this balance are investigated within the framework of a Helfrich Hamiltonian. Based on the full nonlinear shape equations for the membrane profile, a line of continuous binding transitions and a second line of discontinuous envelopment transitions are found, which meet at an unusual triple point. The regime of low tension is studied analytically using a small gradient expansion, while in the limit of large tension scaling arguments are derived which quantify the asymptotic behavior of phase boundary, degree of wrapping, and energy barrier. The maturation of animal viruses by budding is discussed as a biological example of such colloidmembrane interaction events. 

2003 

Osmotic Shock and the Strength of Viral Capsids
Amado Cordova, Markus Deserno, William M. Gelbart, and Avinoam BenShaul
Biophys. J. 85, 70–74 (2003).
Osmotic shock is a familiar means for rupturing viral capsids and exposing their genomes intact. The necessary conditions for providing this shock involve incubation in highconcentration salt solutions, and lower permeability of the capsids to salt ions than to water molecules. We discuss here how values of the capsid strength can be inferred from calculations of the osmotic pressure differences associated with measured values of the critical concentration of incubation solution. 

Wrapping of a spherical colloid by a fluid membrane
Markus Deserno and Thomas Bickel
Europhys. Lett. 62, 767–773 (2003).
We theoretically study the elastic deformation of a fluid membrane induced by an adhering spherical colloidal particle within the framework of a Helfrich energy. Based on a full optimization of the membrane shape we find a continuous binding and a discontinuous envelopment transition, the latter displaying a potentially substantial energy barrier. A smallgradient approximation permits membrane shape and complex energy to be calculated analytically. While this only leads to a good representation of the complex geometry for very small degrees of wrapping, it still gives the correct phase boundaries in the regime of low tension. 

Attraction and ionic correlations between charged stiff polyelectrolytes
Markus Deserno, Axel Arnold, and Christian Holm
Macromolecules 36, 249–259 (2003).
We use molecular dynamics simulations to study attractive interactions and the underlying ionic correlations between parallel likecharged rods in the absence of additional salt. For a generic bulk system of rods we identify a reduction of shortrange repulsions as the origin of a negative osmotic coefficient. The counterions show signs of a weak threedimensional order in the attractive regime only once the rodimposed charge inhomogeneities are divided out. We also treat the case of attraction between a single pair of rods for a few selected line charge densities and rod radii. Measurements of the individual contributions to the force between close rods are studied as a function of Bjerrum length. We find that even though the total force is always attractive at sufficiently high Bjerrum length, the electrostatic contribution can ultimately become repulsive. We also measure azimuthal and longitudinal correlation functions to answer the question how condensed ions are distributed with respect to each other and to the neighboring rod. For instance, we show that the prevalent image of mutually interlocked ions is qualitatively correct, even though modifications due to thermal fluctuations are usually strong. 

2002 

Theory and simulations of rigid polyelectrolytes
Markus Deserno and Christian Holm
Mol. Phys. 100, 2941–2956 (2002).
Theoretical and numerical studies are reported on stiff, linear polyelectrolytes within the framework of the cell model, first reviewing analytical results obtained on a meanfield PoissonBoltzmann level, and then using molecular dynamics simulations to show the circumstances under which these fail quantitatively and qualitatively. For the hexagonally packed nematic phase of the polyelectrolytes the osmotic coefficient is computed as a function of density. In the presence of multivalent counterions it can become negative, leading to effective attractions. This is shown to result from a reduced contribution of the virial part to the pressure. The osmotic coefficient and ionic distribution functions are computed from PoissonBoltzmann theory with and without a recently proposed correlation correction. Simulation results for the case of poly(pphenylene) are presented and compared with recently obtained experimental data on this stiff polyelectrolyte. Ionion correlations in the strong coupling regime are studied and compared with the predictions of the recently advocated Wigner crystal theories. 

The osmotic pressure of charged colloidal suspensions: A unified approach to linearized PoissonBoltzmann theory
Markus Deserno and HansHennig von Grünberg
Phys. Rev. E 66, 011401 (2002).
We study theoretically the equation of state of a fluid suspension of charged objects (e.g., colloids, polyelectrolytes, clay platelets, etc.) dialyzed against an electrolyte solution using the cell model and linear PoissonBoltzmann (PB) theory. From the volume derivative of the grand potential functional of linear theory we obtain two expressions for the osmotic pressure in terms of the potential or ion profiles, neither of which coincides with the expression known from nonlinear PB theory, namely, the density of microions at the cell boundary. We show that the range of validity of linearization depends strongly on the linearization point and prove that expansion about the selfconsistently determined average potential is optimal in several respects. For instance, screening inside the suspension is automatically described by the actual ionic strength, resulting in the correct asymptotics at high colloid concentration. Together with the analytical solution of the linear PB equation for cell models of arbitrary dimension and electrolyte composition, explicit and very general formulas for the osmotic pressure ensue. A comparison with nonlinear PB theory is provided. Our analysis also shows that whether or not linear theory predicts a phase separation depends crucially on the precise definition of the pressure, showing that depending on the choice, an artificial phase separation in systems as important as DNA in physiological salt solution may result. 

Adhesion and Wrapping in ColloidVesicle Complexes
Markus Deserno and William M. Gelbart
J. Phys. Chem. B 106, 5543–5552 (2002).
We present a simple theoretical model for adsorption of colloidal particles onto vesicles. The contact energy of adhesion is balanced by the tension and curvature energies of the vesicle membrane under the constraint of fixed volume, with the geometry of the complex determined by a variational calculation. Physical observables, such as the degree of penetration or the membrane tension, are investigated as functions of colloidal size and adhesion, tension, and bending energies. We find various new (and discontinuous) transitions in the geometry of the complex compared to those from a description that neglects the curvature contribution. Particular emphasis is put on the transition from the partly to the fully wrapped state and on unbinding of the complex at weak adhesion energy or small colloidal size. The above model can be thought of as a phenomenological theory of the initial steps involved in biological endocytosis and aims toward an improved physical understanding of this process. 

2001 

Rayleigh instability of charged droplets in the presence of counterions
Markus Deserno
Eur. Phys. J. E 6, 163–168 (2001).
The classical instability of a charged spherical droplet is reconsidered in the presence of counterions. An ensemble of such droplets is studied within a simplified cell model. Screening of the electric field by the counterions is found to increase the equilibrium droplet size. Furthermore, if the ions can enter the droplet, a firstorder phase transition occurs upon increasing Bjerrum length, surface tension or droplet density, leading to a phase separation. Simple scaling properties of the free energy give the shape of the phase boundary and show the system to be scaleinvariant there. Pearlnecklace structures of hydrophobic polyelectrolytes are discussed as an application. 

Overcharging of DNA in the Presence of Salt: Theory and Simulation
Markus Deserno, Felipe JiménezÁngeles, Christian Holm, and Marcelo LozadaCassou
J. Phys. Chem. B 105, 10983–10991 (2001).
A study of a model rodlike polyelectrolyte molecule immersed in a monovalent or divalent electrolyte is presented. Results for the local concentration profile, mean electrostatic potential, charge distribution function, and zetapotential are obtained from hypernettedchain/mean spherical approximation (HNC/MSA) theory and compared with molecular dynamics (MD) simulations. As a particular case, the parameters of the polyelectrolyte molecule are mapped to those of a DNA molecule. Both HNC/MSA and MD predict the occurrence of overcharging, which is not present in the PoissonBoltzmann theory. Further an excellent qualitative, and in some cases quantitative, agreement between HNC/MSA and MD is found. Oscillations observed in the mean electrostatic potential, local concentration profiles, and the curvature of the zetapotential are discussed in terms of the observed overcharging effect. Particularly interesting results are a very nonmonotonic behavior of the zetapotential, as a function of the rod charge density, and the overcharging by monovalent counterions. 

The osmotic coefficient of rodlike polyelectrolytes: Computer simulation, analytical theory, and experiment
Markus Deserno, Christian Holm, Jürgen Blaul, Matthias Ballauff, and Matthias Rehahn
Eur. Phys. J. E 5, 97–103 (2001).
The osmotic coefficient of solutions of rodlike polyelectrolytes is considered by comparing current theoretical treatments and simulations to recent experimental data. The discussion is restricted to the case of monovalent counterions and dilute, saltfree solutions. The classical PoissonBoltzmann solution of the cell model correctly predicts a strong decrease in the osmotic coefficient, but upon closer look systematically overestimates its value. The contribution of ionioncorrelations are quantitatively studied by MD simulations and the recently proposed DHHC theory. However, our comparison with experimental data obtained on synthetic, stiffchain polyelectrolytes shows that correlation effects can only partly explain the discrepancy. A quantitative understanding thus requires theoretical efforts beyond the restricted primitive model of electrolytes. 

2000 

Ionion correlations: an improved onecomponent plasma correction
Marcia C. Barbosa, Markus Deserno, and Christian Holm
Europhys. Lett. 52, 80–86 (2000).
We propose a new approach for incorporating counterion correlations into PoissonBoltzmannlike theories, which is based on a local density functional for the system of counterions. Our derivation is inspired by the DebyeHückel approach to the onecomponent plasma (OCP). An artificial instability due to the OCP's homogeneous background charge – which is absent in the original counterion system – is overcome by excluding the background from the vicinity of a central ion. The resulting free energy density is convex and thus applicable within a local density approximation. For the simple example of a strongly charged stiff rod surrounded by its counterions we demonstrate that the PoissonBoltzmann free energy functional augmented by our new correction accounts for the correlations present in this system when compared to molecular dynamics simulations. 

A MonteCarlo approach to PoissonBoltzmann like freeenergy functionals
Markus Deserno
Physica A 278, 405–413 (2000).
A simple technique is proposed for numerically determining equilibrium ion distribution functions belonging to free energies of the PoissonBoltzmann type. The central idea is to perform a conventional MonteCarlo simulation using the free energy as the "Hamiltonian" entering the Metropolis criterion and the spatially discretized density as degrees of freedom. This approach is complementary to the possibility of numerically solving the differential equations corresponding to the variational problem, but it is much easier to implement and to generalize. Its utility is demonstrated in two examples: valence mixtures and hard core interactions of ions surrounding a charged rod. 

Fraction of condensed counterions around a charged rod: Comparison of PoissonBoltzmann theory and computer simulations
Markus Deserno, Christian Holm, and Sylvio May
Macromolecules 33, 199–206 (2000).
We investigate the phenomenon of counterion condensation in a solution of highly charged rigid polyelectrolytes within the cell model. A method is proposed whichbased on the charge distribution functionidentifies both the fraction of condensed ions and the radial extension of the condensed layer. Within saltfree PoissonBoltzmann (PB) theory it reproduces the wellknown fraction 11/ξ of condensed ions for a Manning parameter ξ > 1. Furthermore, it predicts a weak salt dependence of this fraction and a breakdown of the concept of counterion condensation in the highsalt limit. We complement our theoretical investigations with molecular dynamics simulations of a celllike model, which constantly yield a stronger condensation than predicted by PB theory. While the agreement between theory and simulation is excellent in the monovalent, weakly charged case, it deteriorates with increasing electrostatic interaction strength and, in particular, increasing valence. For instance, at a high concentration of divalent salt and large xi our computer simulations predict charge oscillations, which meanfield theory is unable to reproduce. 

1998 

How to mesh up Ewald sums (II): An accurate error estimate for the P3M algorithm
Markus Deserno and Christian Holm
J. Chem. Phys. 109, 7694–7701 (1998).
We construct an accurate estimate for the root mean square force error of the particleparticle–particlemesh (P3M) algorithm by extending a single particle pair error measure which has been given by Hockney and Eastwood. We also derive an easytouse analytic approximation to the error formula. This allows a straightforward and precise determination of the optimal splitting parameter (as a function of system specifications and P3M parameters) and hence knowledge of the force accuracy prior to the actual simulation. The high quality of the estimate is demonstrated in several examples. 

How to mesh up Ewald sums (I): A theoretical and numerical comparison of various particle mesh routines
Markus Deserno and Christian Holm
J. Chem. Phys. 109, 7678–7693 (1998).
Standard Ewald sums, which calculate e.g. the electrostatic energy or the force in periodically closed systems of charged particles, can be efficiently speeded up by the use of the Fast Fourier Transformation (FFT). In this article we investigate three algorithms for the FFTaccelerated Ewald sum, which attracted a widespread attention, namely, the socalled particleparticle–particlemesh (P3M), particle mesh Ewald (PME) and smooth PME method. We present a unified view of the underlying techniques and the various ingredients which comprise those routines. Additionally, we offer detailed accuracy measurements, which shed some light on the influence of several tuning parameters and also show that the existing methods – although similar in spirit – exhibit remarkable differences in accuracy. We propose combinations of the individual components, mostly relying on the P3M approach, which we regard as most flexible. The issue of estimating the errors connected with particle mesh routines is reserved to part II of this series. 

1997 

Tricriticality and the BlumeCapel model: A Monte Carlo study within the microcanonical ensemble
Markus Deserno
Phys. Rev. E 56, 5204–5210 (1997).
The microcanonical partition function Ω_{α,N}(E) of a threedimensional ferromagnetic simple cubic BlumeCapel model is calculated for several coupling ratios alpha close to and on the firstorder side of the tricritical point. To this end a single Monte Carlo simulation of a suitably extended partition function for systems of L×L×L spins with L in {8,10,12,14,18} was performed. A finite system analog of the latent heat is introduced in order to define a tricritical point in finite systems as well. An empirical scaling of its coordinates to the thermodynamic limit yields α_{t}=2.844 79 + 0.00030 for the tricritical coupling ratio, and kT_{t}/J=1.4182 + 0.0055 for the tricritical transition temperature. The results are compared with values obtained on FCC lattices. 


Proceeding, Schools, ... 

Membrane Elasticity and Mediated Interactions in Continuum Theory: A Differential Geometric Approach
Markus Deserno
in: Biomembrane Frontiers: Nanostructures, Models, and the Design of Life, Volume 2, edited by Roland Faller, Thomas Jue, Marjorie L. Longo, and Subhash H. Risbud,Humana Press (Springer, New York, 2009).
Objects in contact with membranes can locally deform these membranes, and several such objects can interact by means of the elastic stresses thus created. For fluid surfaces the Hamiltonian is purely geometric, and this permits a very efficient treatment of this scenario using methods of covariant differential geometry. This article provides a pedagogical introduction into the philosophy behind this approach. The relation between geometry and elasticity is first derived in a very intuitive way and then extended to more complex (but very relevant) examples. The relation between stresses and geometry is introduced and illustrated in three very different examples: interactions mediated by (a) composition variations, (b) lipid tilt fields, and (c) membrane curvature. 

Solventfree lipidbilayer simulations: From Physics to Biology
Markus Deserno
in: Computer Simulation Studies in Condensed Matter Physics XIX, Eds. D.P. Landau, S.P. Lewis, and H.B. Schüttler (Springer, Heidelberg, Berlin, 2006).
Coarsegrained solventfree simulation models enabling the study of selfassembling fluid lipid bilayers have been the goal of much recent modeling efforts, since their realization appeared to be quite intricate. This contribution reviews some of the challenges faced along the way, presents a surprisingly simple solution, and illustrates its capacity by means of three examples of biological interest. 

Cell Model and PoissonBoltzmann Theory: A brief introduction
Markus Deserno and Christian Holm
in: Electrostatic Effects in Soft Matter and Biophysics, Vol 46 of NATO Advanced Studies Institute, Series II: Mathematics, Physics and Chemistry, ed. by Christian Holm, Patrick Kékicheff, and Rudolf Podgornik (Kluwer, Dordrecht, 2001).
The cellmodel and its treatment on the PoissonBoltzmann level are two important concepts in the theoretical description of charged macromolecules. In this brief contribution we provide an introduction to both ideas and summarize a few important results which can be obtained from them. Our article is organized as follows: Section 1 outlines the sequence of approximations which ultimately lead to the cellmodel. Section 2 is devoted to two exact results, namely, an expression for the osmotic pressure and a formula for the ion density at the surface of the macromolecule, known as the contact value theorem. Section 3 provides a derivation of the PoissonBoltzmann equation from a variational principle and the assumption of a product state. Section 4 applies PoissonBoltzmann theory to the cellmodel of linear polyelectrolytes. In particular, the behavior of the exact solution in the limit of zero density is compared to the concept of Manning condensation. Finally, Section 5 shows how a system described by a cell model can be coupled to a salt reservoir, i.e., how the socalled Donnan equilibrium is established. 

Molecular Dynamics Simulation of the Cell Model
Markus Deserno, Christian Holm, and Kurt Kremer
in: Physical Chemistry of Polyelectrolytes, Vol. 99 of the surfactant science series, ed. by Tsetska Radeva (Marcel Dekker, New York, 2001).

















