key: cord-0893610-bbtgczsv authors: Almsherqi, Zakaria A.; Landh, Tomas; Kohlwein, Sepp D.; Deng, Yuru title: Chapter 6 Cubic Membranes: The Missing Dimension of Cell Membrane Organization date: 2009-04-05 journal: Int Rev Cell Mol Biol DOI: 10.1016/s1937-6448(08)02006-6 sha: 0964dabe3541149231a6517f4f2e698c7ea8838e doc_id: 893610 cord_uid: bbtgczsv Biological membranes are among the most fascinating assemblies of biomolecules: a bilayer less than 10 nm thick, composed of rather small lipid molecules that are held together simply by noncovalent forces, defines the cell and discriminates between “inside” and “outside”, survival, and death. Intracellular compartmentalization—governed by biomembranes as well—is a characteristic feature of eukaryotic cells, which allows them to fulfill multiple and highly specialized anabolic and catabolic functions in strictly controlled environments. Although cellular membranes are generally visualized as flat sheets or closely folded isolated objects, multiple observations also demonstrate that membranes may fold into “unusual”, highly organized structures with 2D or 3D periodicity. The obvious correlation of highly convoluted membrane organizations with pathological cellular states, for example, as a consequence of viral infection, deserves close consideration. However, knowledge about formation and function of these highly organized 3D periodic membrane structures is scarce, primarily due to the lack of appropriate techniques for their analysis in vivo. Currently, the only direct way to characterize cellular membrane architecture is by transmission electron microscopy (TEM). However, deciphering the spatial architecture solely based on two-dimensionally projected TEM images is a challenging task and prone to artifacts. In this review, we will provide an update on the current progress in identifying and analyzing 3D membrane architectures in biological systems, with a special focus on membranes with cubic symmetry, and their potential role in physiological and pathophysiological conditions. Proteomics and lipidomics approaches in defined experimental cell systems may prove instrumental to understand formation and function of 3D membrane morphologies. .1016/S1937-6448(08)02006-6 All rights reserved. Membrane-bound cell organelles are typically considered to have rather spherical topology, delineated by one phospholipid-bilayer membrane that separates the interior from the exterior. However, this simplification of organelle topology is a rule not a law, and it is well known that a large number of membrane structures exists in Nature with more complex 3D morphologies. Indeed, the topology of membrane-bound organelles is a rather unexplored area of research. This might be due to difficulties in obtaining information about topological parameters from living or fixed cells, and the interpretation of these parameters in the cellular context. Nevertheless, the importance of topology considerations, for example, subcellular compartmentalization, transport phenomena, and sorting events that involve membrane trafficking processes is evident. Cell membrane morphology, controlled by the principles of self-assembly and/or self-organization, is likely to adopt an optimally organized structure under the influence of selective conditions. This is a dynamic process, perhaps restricted to sub-membrane domains, and short-lived, and is dependent on the lipid as well as protein components of the membrane. As a consequence of limited in vivo technologies, knowledge about the molecular mechanisms underlying membrane morphology is scarce and largely restricted to the descriptive level. Indeed, higher order membrane topologies identified by transmission electron microscopy (TEM), are frequently reported in the literature, yet due to their very heterogeneous representations, common features are difficult to comprehend. Among these nonlamellar cell membranes, especially cubic membrane organizations attract great attention (Almsherqi et al., 2006; Hyde et al., 1996; Landh, 1995 Landh, , 1996 because of their unique feature of 3D periodicity in TEM micrographs and great similarity to the bicontinuous lipidic cubic phases (Bouligand, 1990; Larsson, 1989; Larsson et al., 1980; Luzzati, 1997) . Cubic membranes (Figs. 6.1 and 6.2) have therefore often been compared to selfassembled cubic lipidic phases in aqueous dispersions that are well Figure 6 .1 Cubic membrane architecture (Almsherqi et al., 2008) . (A) Two-dimensional transmission electron micrograph of a mitochondrion of 10 days starved amoeba Chaos cells and (B) three-dimensional mathematical model of the same type of cubic membrane organization. Scale bar: 250 nm. characterized in vitro, with several applications. Indeed, the efforts toward understanding formation and functional roles of cubic membranes in biological systems have been paralleled by the efforts in investigating cubic phases formation and their behavior in lipid-water systems. Biological membranes may exhibit point or line symmetry. A membrane is symmetrical if it can be nontrivially rotated, inverted, mirrored, and translated such that it is indistinguishable from its initial appearance. Symmetry of Three parallel Gyroid-based surfaces can be used to describe a biological membrane (bilayer), in which case the centered surface is the ''imaginary'' hydrophobic mid-bilayer surface and the two parallel surfaces are the two apolar/polar (interfacial) surfaces. biological membranes is mainly described by rotations. Several sets of membrane arrangements exhibit symmetry such as parallel membranes and hexagonal packing of tubes. In contrast, a cubic membrane exhibits distinct morphological patterns when projected which may even be translated into unique signatures in many directions (Fig. 6.3) . The patterned membrane organization of cubic membranes consists of a network arranged in a nonrandom order and is evenly spaced. Therefore, through an overall inspection of TEM micrographs, cubic membranes are recognized via perceptual cues of the patterned membrane organization (Almsherqi et al., 2006; Landh, 1996) . This unique appearance of cubic membranes in TEM micrographs frequently allows for the differentiation of cubic membrane organization from other membrane arrangements such as tubulo-reticular structures (TRS) and annulate lamellae (AL) (Figs. 6.4 and 6.5). Cubic membranes represent highly curved, 3D periodic structures that correspond to mathematically well-defined triply periodic minimal surfaces or the corresponding periodic nodal surfaces and their respective constant mean curvature or level surfaces ( Fig. 6 .2). Both the latter surface descriptions are approximative descriptions of surfaces parallel to the minimal or nonzero level surface (Landh, 1996) . Cubic membranes have been detected Figure 6 .3 Computer simulation of TEM images. (A) Schematic illustration of TEM data in 2D projections of a specimen with a finite thickness. A 3D object (a) is depicted and is translucent to the projection rays of an electron beam; (b) representation of one unit cell of the gyroid surface; (c) projection plane onto which the rays impinge, in analogy of the film on which the image would be recorded; (d) 2D projection map provides a corresponding template for matching the patterned membrane domain in the TEM micrograph. (B) Comparison between a 3D cubic membrane model of a gyroidbased surface and its computer simulated projections at different viewing directions. Multiple 2D projections that are generated from the same 3D structure form a library of different patterns. The bottom row corresponds to computer-simulated projections for the top row, based on a projected specimen thickness of one-half of a unit cell viewed at the [1, 0, 0] (left), [1, 1, 0] (middle), and [1, 1, 1] (right) directions. The computergenerated projection can be matched with TEM micrographs to determine the 3D structure of a cubic membrane arrangement (see section 2.4. for further details). without any obvious restrictions or preferences in all kingdoms of life, both under physiological or pathological conditions (Table 6 .1). They appear not to be limited to certain types of cells, although they may occur more frequently in some cell types. Furthermore, cubic membranes are not strictly associated with any particular organelle and can apparently evolve from almost any cytomembrane: plasma membrane, endoplasmic reticulum (ER), nuclear envelope (NE, both inner (INE) and outer (ONE)), inner mitochondrial membrane, and the Golgi complex. The smooth ER, however, seems to be the organelle most frequently associated with cubic membrane formation. So far, three surface families have been identified to exist, and these three types of cubic membranes are schematically shown in Fig. 6 .2. They are designated according to their corresponding triply periodic minimal (or level) surfaces as gyroid (G), double diamond (D), and primitive (P) surfaces. Cubic membranes often coexist with other ''unusual'' membrane arrangements, such as TRS, which are irregularly arranged tubes that bifurcate and reanastomose. In many cases, these tubes show a preferential Figure 6 .4 Cell membrane organization. Schematic diagram depicting the likely 3D structure of annulated lamellae, tubulo-reticular structure (TRS) and the membrane folding transition. The pores of annulated lamellae may alternate in arrangement with the symmetry often being quadratic (A) or the pore face each other with the symmetry being hexagonal (B) . Two examples of TRS membrane arrangements; (C) interconnected sacular (cisternae) and (D) tubular membrane organization show no global symmetry. A possible model of continuous membrane folding for the formation of double diamond (lower left) and gyroid (upper left) cubic type, hexagonal (upper right) and lamellar structures, and whorls (lower right) (E). The coexistence of these membrane organizations has been reported frequently in UT-1 and COS-7/ CV-1 cells with HMG-CoA reductase and cytochrome b(5) overexpression, respectively. Panels A-D adapted from Figs. 17 and 18; Bouligand, 1991. orientation. The main difference of TRS to cubic membranes is that TRS symmetry is usually nematic, since the layers do not show obvious periodic distribution ( Fig. 6.4D ). The preferential alignment along a direction may be due to an elongation process, perhaps in association with the cytoskeleton, and is not necessarily the result of a spontaneous membrane alignment. However, there are many cases in which the periphery of a perfectly preserved cubic morphology shows TRS appearance, which, therefore, may be introduced by the fixation method (Landh, 1995) . Membranes of true cubic morphology are often mis-labeled as TRS in the literature, due to the convoluted image projections observed for both structures. Many of the examples listed in Table 6 .1 have been designated as TRS, despite the presence of a distinct cubic symmetry (Almsherqi et al., 2005; Landh, 1996) . TRS have attracted biomedical interest due to their potential use as an ultrastructural marker for pathological conditions: they occur in virusinfected and in cancer cells and have been, therefore, often regarded as an Bryan et al. (1967) Thylakoid membranes in chloroplast of Sinusoidal thylakoids Berkaloff (1967) Charophyceae Plasma membrane of Chara coralline, C. braunii Charasome G/140 Barton (1965) , Lucas (1980, 1981) , Lucas and Franceshi (1981) Plasma membranes of Nitella Pappas and Brandt (1959) , Brandt and Pappas (1959) , Borysko and Roslansky (1959) , Daniels and Breyer (1968) (continued) Mckanna (1976) , Allen and Fok (1988) , Allen et al. (1990 ), Fok et al. (1995 , Hausmann and Allen (1977) , Ishida et al. (1993 Ishida et al. ( , 1996 Intranuclear membrane of Neobursaridium gigas Crystal configuration G/160 Nilsson (1969) Tetrahymenina Nephiridial tubules Elliott and Bak (1964) Fungi Amastigomycota Ascomycotima Lattice bodies G/55 Anderson and Zachariah (1972) , Zachariah (1970) , Zachariah and Anderson (1973) , Wells (1972) Bassot (1964 Bassot ( , 1966 , Bassot and Nicolas (1978) , Bilbaut (1980) , de Ceccatty et al. Bassot and Nicolas (1978) ER in luminous cells of Harmothoe lunulata PER Bassot (1985) , Nicolas (1987, 1995) , Nicolas (1979 Nicolas ( , 1991 Crystalline element Singla (1975) Arsenault et al. (1979 Arsenault et al. ( , 1980 Schwann cell processes in the ventral nerve cord of Procambarus sp. Anastomosing tubular inclusion Pappas et al. (1971) Schwann cell processes in the walking limb nerves Nephrops sp. Anastomosing networks Holtzman et al. (1970) Mitochondria in oocytes of Cambarus and Orconectes Honeycombed cristae Beams and Kessel (1963) Masses of membranes Brammer and White (1969) Lepidoptera Membrane-cuticle unit Chiradella (1989 Chiradella ( , 1994 Hymenoptera ER in secretory cells of Dufour's gland in Parischnogaster mellyi Vesicular profiles Delfino et al. (1988) Blattodea Mitochondrion in secretory cells of the spermatheca in Periplaneta am. Gupta and Smith (1969) Chordata Urochordata Ascidiacea tethyodea Stolidobranchiata (continued) Kessel (1990) ER in retinal pigment epithelium cells of Notophtalamus viridescens Fenestrated lamellae Yorke and Dickson (1985) (continued) Sisson and Fahrenbach (1967) Mitochondria in skeletal muscle of the rat Leeson and Leeson (1969) ER in jejunal absorptive cells of rat intestine Hatae (1990) ER in vomeronasal epithelium in the rat Membranous body Garrosa and Coca (1991) ER in cell of sebaceous gland in mouse skin Crowded elements Rowden (1968) ER of neurons in the mice Interconnected segments of SER Johnson et al. (1975) ER in testicular interstitial cells of mice Network of tubules Christensen and Fawcett (1966) Smooth membrane vesicles Quan and Doane (1983) ER in LLC-MK 2 infected with rubella virus Crystal lattice-like structure Kim and Boatman (1967) (continued) S n /a Indicates that the membrane (surface) morphology (S) is consistent with (n) membranes or multiple (m) membranes with a lattice size of (a). The listed unit cell size is based on either DTC analysis or direct measurements of the 2D lattice parameters. UMS: undulating membrane structure; TRS: tubuloreticular structure; PER: paracrystalline ER; SER: smooth endoplasmic reticulum. The table summarizes the observation of cubic membranes in normal, pathological, and experimentally manipulated cells. indicator of infection or transformation. For example, TRS have been observed in cells infected with SARS (Almsherqi et al., 2005) and HIV (Kostianovsky et al., 1987) . In addition to TRS, annulate lamellae (AL) are another type of convoluted 3D membrane structure, and their appearance is also often correlated with that of cubic membranes. AL are frequently observed in differentiating gamates, namely in vertebrate oocytes and in spermatogonia, and appear to occur in close association with the cell nucleus (see Table 6 .1). Tangential TEM sections of AL most often exhibit a hexagonal arrangement (Kessel, 1983) , whereas perpendicular sections do not reveal any obvious symmetrical arrangement, even though they always exhibit an astonishingly regular organization, indicating an underlying periodic structure. Based on the apparent morphological similarities between AL and the NE, it has been suggested that AL represent a cytoplasmic NE extension that functions as a reservoir for both ER membrane components and nuclear pores (Kessel, 1983 (Kessel, , 1992 . In favor of such speculations is the fact that AL have been observed in direct continuity with the outer nuclear membrane, and that they also have been suggested to contain nuclear pore complexes (Landh, 1996) . AL are assembled of superimposed pairs of membrane bilayers, which join along the pores whose distribution may vary (hexagonal, quadratic, or random). The pores present in AL are either facing each other if the membrane symmetry is hexagonal (Fig. 6 .4B) or the appearance of pores alternates in a quadratic membrane arrangement ( Fig. 6.4A ). The coexistence of different subtypes of cubic membranes or together with other membrane organizations within the same cell organelle is quite frequent, pointing to structural or functional relationships between these membrane arrangements ( Fig. 6.4E ). Probably the most evident example is the ER where different membrane morphologies such as cubic membranes, lamellar and hexagonal membranes, and whorls coexist quite commonly (Landh, 1996; Snapp et al., 2003) . Coexistence of at least two cubic membrane subtypes within the same organelle has also been observed in mitochondria of amoeba Chaos carolinense (Deng and Mieczkowski, 1998) . In this organism, the relative abundance of gyroid (G) or diamond (D) and primitive (P) subtypes of cubic morphology changes during starvation, the biological significance of this polymorphic behavior, however, is currently unknown. The ease with which cubic membranes and other membrane arrangements are interconverted can be attributed, at least in part, to the effect of weakly dimerizing ER proteins (Snapp et al., 2003) . Previous work suggested that crystalloid ER biogenesis entailed a tight, zipper-like dimerization of the cytoplasmic domains of certain ER-resident proteins (Yamamoto et al., 1996) . However, Snapp et al. (2003) found that organized smooth ER (OSER)-inducing proteins can trigger cubic membrane formation upon over-expression through low-affinity interactions between cytoplasmic domains. This observation might explain phenomena such as (a) the heterogeneity of ER membrane structures, (b) the high rate of (reversible) lamellar to cubic membrane transition, and (c) the technical difficulties and limitations in isolating intact cubic membranes from biological samples. Lipidic bicontinuous cubic phases consist of hyperbolically curved bi-layers where each monolayer is draped over a periodic cubic (minimal) surface ( Fig. 6.2D ). With respect to bilayer arrangements, the geometries of cubic membranes are similar to those of the cubic phases, however, two major differences exist: (i) the unit cell size and (ii) the water activity. It has been argued that the latter must control the topology of the cubic membrane (Bouligand, 1990) and hence that the cubic membrane structures must be of the inverted type rather than ''normal'' type (type I). All known lipid-water and lipid-protein-water systems that exhibit phases in equilibrium with excess water are of the inverted type (type II). Thus, water activity alone cannot determine the topology of cubic membranes. Inverted cubic phases have been observed with very high water activity (70-90%), in the mixtures of lipids, in lipid-protein systems, in lipid-polymer systems (Landh, 1994) , and in lipid and lipopolysaccharide mixtures (Brandenburg, 1990 (Brandenburg, , 1992 . Most cubic phases in lipid-water systems exhibit unit cell parameters not larger than 20 nm, while in cellular cubic membranes the lattice size is usually larger than 50 nm. However, in lipid-protein-water, lipid-poloxamer-water and lipid-cationic surfactant-water systems, cubic phases with cell parameters of the order of 50 nm have also been observed (Landh, 1996) . On the other hand, the unit cell size of cubic membranes is rarely less than 50 nm (e.g., in prolamellar bodies) and the size ranges from 50 to 500 nm. Cubic membranes with large lattice size (500 nm) were frequently observed in chloroplast membranes of green algae Zygnema (Fig. 6.6) . Additionally, cubic membranes are formed under conditions corresponding to a highly regulated multiphase ''equilibrium'' process. This is supported by the fact that they are usually formed in close contact with different other membrane configurations. The asymmetry of biological membranes with respect to the two leaflets is likely to affect cubic membrane formation, in particular as a consequence of lipid and protein composition, and interaction with the surrounding ion milieu. A survey of the literature (Table 6 .1) immediately unveils a multitude of ''unusual'' membrane organizations in various cell types. Most of these depictions were obtained by TEM of chemically fixed and thin-sectioned cells and tissues. Dependent on the thickness and orientation of the section through the specimen, relative to the coordinates of an ordered 3D structure, various types of projection patterns are observed. As a consequence, membrane ultrastructures derived from TEM images are frequently misinterpreted, in particular for the highly folded and interconnected 3D morphologies resembling cubic membranes. TEM relies on 70-90 nm thick sections through the specimens and the 2D image obtained is the result of a projection of a 3D structure. Therefore, nonlamellar biological membranes, such as inverted hexagonal or cubic structures, may yield very heterogeneous projection patterns by TEM, dependent on the orientation of the section relative to the structural axes ( Fig. 6.3) . Interpretation of TEM membrane patterns is further complicated if the lattice size of the observed structure is considerably smaller than that of the section thickness. Serial sections or scanning EM, as well as tilting and rotation of the sample, may facilitate structure interpretation. Furthermore, TEM of multiple randomly cut sections through a specimen provides a rather simple means to reconstruct its 3D structure. More elaborate electron tomography (ET) has contributed a great deal of resolution to understanding cubic membrane organizations and their continuity with and relations to the neighbor structures (Deng et al., 1999) . In ET, rather thick sections (400 nm) are imaged in multiple tilted angles (up to AE60 ), yielding a large number of projections; these images are reconstructed by computational image analysis into a 3D representation of the object, which allows the 3D reconstruction of cellular structures with a resolution of 5 nm, that is, approaching the level or larger molecular assemblies (for a review see Lucic et al., 2005) . EM tomography has previously been successfully applied to determine cubic membrane transition of the inner mitochondrial membrane morphology in the amoeba C. carolinense upon starvation (Deng et al., 1999) . Cryo-ET from specimens in vitreous ice further improves sample preservation and membrane resolution, but obviously is not yet routinely established. Cryo-ET avoids common artifacts of conventional EM preparation techniques and is also suited for high-resolution analyses of membrane-bound organelles (Hsieh et al., 2006; Lucic et al., 2005) . Most EM experiments described in the literature that focus on biological membranes were obviously not designed to depict three-dimensionally convoluted membrane arrangements. Therefore, alternative methods have to be applied to reconstruct-potential-3D membrane morphologies from single TEM sections. Indeed, based on well-defined mathematical models of cubic membrane arrangements, projections can be calculated that simulate various section orientations and thicknesses (Fig. 6.3) . Such a ''direct template correlative'' (DTC) matching method (Almsherqi et al., 2005 (Almsherqi et al., , 2006 Deng and Mieczkowski, 1998; Landh, 1995 Landh, , 1996 has been developed based on pattern and symmetry recognition. Through the DTC method, the electron density of the TEM image is correlated to a library of computer-simulated 2D projection maps that allows to unequivocally deduce the nature of the cubic membrane arrangement. An application of the DTC method to identify cubic membrane organization in TEM micrographs is shown in Fig. 6 .7. In brief, the 2D projections (Fig. 6 .7C) calculated from a mathematical 3D model (Fig. 6.7B ) are matched with a selected TEM micrograph (Fig. 6.7A) ; consequently, a successful pattern match defines the nature of the membrane arrangement in 3D (Deng and Mieczkowski, 1998; Landh, 1995 Landh, , 1996 . The DTC method simplifies the experimental requirements for recording cubic membranes in biological samples, and can also be applied to examine published TEM micrographs in retrospect. The following section highlights the identification of cubic membrane structures in multiple cellular systems and subcellular organelles. Extensive membrane proliferations leading to unusual and highly convoluted depictions in TEM micrographs have been observed in numerous cell types from all kingdoms of life and in virtually any membrane-bound subcellular organelles, as outlined above. Table 6 .1 summarizes a survey of the literature of the past six decades on cubic membrane morphologies identified in organelles, from protozoan to human cells. The occurrence of cubic membranes is listed by genera and, if applicable, the type and lattice size of the cubic membrane extracted from the published TEM images are presented (see also Hyde et al., 1996; Landh, 1996) . Not surprisingly, due to the absence of a clear understanding of the 3D structure of the depicted membranes, many of the examples have been considered as novelties with little or no reflection on the wealth of related contributions in the literature. Hence, these morphologies appear under a large variety of nicknames, some of which are also listed in Table 6 .1. Furthermore, the examples have been chosen to best represent the structural characteristics of cubic membranes, and an effort has been made to leave out those perhaps less recognizable structures such as ''membraneous tubular'', ''cisternal systems'', ''tubular inclusions'', or ''cisternal convolutions'' etc. In many cases where we have chosen not to classify the cubic membrane it is mainly due to the lack of discernible details in the TEM micrographs. Interestingly, many of these undetermined cubic membrane morphologies are reported in pathological conditions in hominoidae. Organelles with cubic membrane structure 3.2.1. Endoplasmic reticulum The ER was found to be the most prominent target of morphological alterations because of its highly convoluted and dynamic structure and crucial functions in membrane lipid synthesis and assembly, protein synthesis and secretion, ion homeostasis, and membrane quality control. These morphologies appear under numerous nicknames in the literature, such as ''undulating membranes'' , ''cotte de mailles'' (Franke and Scheer, 1971) , ''membrane lattice'' (Linder and Staehelin, 1980) , ''crystalloid membranes'' (Yamamoto et al., 1996) , ''paracrystalline ER'' (Wolf and Motzko, 1995) , ''tubuloreticular structures (TRS)'' , and recently, as OSER (Snapp et al., 2003) . Periodic symmetrical transitions of the ER are usually correlated with overexpression of certain ER-resident membrane proteins (Table 6 .2) (see below). For example, overexpression of HMG-CoA reductase isozymes induces assembly of nuclear and cortical ER stacks with 2D symmetry, termed ''karmellae'' in yeast (Profant et al., 2000; Wright et al., 1988) . Overexpression of this enzyme in UT-1 (Chin et al., 1982) or Chinese Hamster Ovary (CHO) cells (Jingami et al., 1987; Roitelman et al., 1992) induces formation of crystalloid ER, which houses most of the HMG-CoA reductase enzyme (Anderson et al., 1983; Orci et al., 1984) . This correlation may imply a specific structure-function relationship of cubic membrane formation as a consequence of an altered protein or lipid inventory of the membrane. The cells of the phloem in plants are involved in the long-distance transport of nutrients and are known as sieve elements. Interestingly, the ER of differentiating sieve elements is a rare example in Nature in which Weiner et al. (1984) two cubic membranes with the same structure but with different unit cell parameters, may coexist in the same cell (Behnke, 1965 (Behnke, , 1968 Landh, 1996) . These cells lack a nucleus and the cytoplasmic connection and exchange between vertically stacked cells is enabled through the perforated walls of the sieve elements (Behnke, 1965) . Their function is to transfer the products of photosynthesis from the manufacturing site (leaves) to the storage cells (stem, roots, and seeds). The different types of cubic membranes may perhaps facilitate transport of various materials at different rates within the same cell. Numerous researchers have reported mitochondria with inner membrane configurations that resemble cubic membrane morphologies Kalt, 1974; Tahmisian et al., 1956) . Possibly the bestcharacterized cubic membrane transition was observed in the mitochondrial inner membranes of the free-living giant amoeba, C. carolinense (Deng and Mieczkowski, 1998) . In this organism, mitochondrial inner membranes undergo dramatic changes in 3D organization upon food depletion, providing an attractive, reversible model system to investigate induced membrane reorganization. Within one day of starvation, 70% of mitochondria undergo this morphological transition, which is observed in virtually all mitochondria after 7 days of starvation (Daniels and Breyer, 1968 ). This structural alteration of mitochondria in C. carolinense has been identified by a number of laboratories; however, in several reports the inner mitochondrial membranes take the appearance of tubular-like configurations that may appear in conjunction with well defined cubic membranes (Borysko and Roslansky, 1959; Brandt and Pappas, 1959; Daniels and Breyer, 1968; Sedar and Rudzinska, 1956) . Indeed, by EM tomography, we have unambiguously demonstrated that inner mitochondrial membranes in C. carolinense cells adopt cubic morphology under starvation conditions (Deng et al., 1999) . This induced transition is accompanied by alterations in cellular oxidative stress response, which led us to speculate that cubic membrane formation may be associated with oxidative stress (Deng et al., 2002) (see also discussion below). Intriguingly, formation of cubic membranes in amoeba Chaos is fully reversible to wild-type tubular morphology, upon refeeding (Deng and Mieczkowski, 1998) . A similar cubic architecture of inner mitochondrial membranes was identified in a TEM ultrastructural study (Kalt, 1974 ) that describes mitochondrial pleomorphism in supporting (sustentacular) cells in testis of African clawed frog, Xenopus laevis. The mitochondrial membrane constellation in the mature stage of Sertoli sustentacular cells exhibits the D subtype of cubic membrane morphology. The mitochondria in the inner segment of the retinal cones of tree shrew species, Scandentia, the common tree shrew (Tupaia glis), and the northern tree shrew (Tupaia belangeri) (Foelix et al., 1987; Knabe and Kuhn, 1996; Knabe et al., 1997) are unique in size and ultrastructural arrangement of their inner membranes (Samorajski et al., 1966) . These unusually large, patterned mitochondria exhibit one of the most complicated cubic membrane architectures known to date, with the highest possible symmetry (G subtype) of up to 12 layers of three-dimensionally folded membranes (see discussion below) (Fig. 6.7) . Convoluted invaginations of the plasma membrane that are associated with the ''smooth spongiome,'' which is part of the contractile vacuole complex in Paramecium multimicronucleatum, have been proposed to be of the G subtype of cubic membrane organization (Allen, 2000; Landh, 1996; Patterson, 1980) . Paramecium cells are able to maintain an almost constant intracellular osmolarity regardless of the environmental osmolarity. The complex regulation of the cell volume and osmotic gradient is primarily established by the smooth spongiome, which exhibits cubic membrane organization. Therefore, cubic membranes have been suggested to play roles in water segregation and intracellular volume and osmolarity control (Landh, 1996) . ''Honeycomb'' structures of the T-tubular system in skeletal muscles have been observed in numerous diseased as well as in experimentally induced cases. Such structures were shown to be in continuity with the extra-cellular space and can thus be regarded as extensions of plasma membrane invaginations. The significance of honeycomb t-tubules is, however, unknown (Mastaglia and Walton, 1992) , and surprisingly few studies deal with their 3D organization. Despite the elegant study of Ishikawa (1968) , the 3D structure of these ''honeycombs'' was resolved only 30 years after their first discovery (Landh, 1996) and unambiguously demonstrated to be of cubic membrane morphology of the gyroid (G) subtype. The structure of photosynthetic membranes and their assembly during development have been extensively studied (Gunning, 1965; Gunning and Jagoe, 1967; Gunning and Steer, 1975) . In bacteria, several publications report lattice-like membrane morphologies as a variation of the more common multilamellar (thylakoid) configuration. In vegetative, photosynthetically active cyanobacteria, Anabaena sp., Lang and Rae (1967) reported a ''prolamellar-like lattice'', which was formed through continuous foldings of the photosynthetic thylakoid membranes. This cubic membrane bears a close resemblance to the prolamellar body (PLB) in higher plants, with the important difference that PLB are formed in the absence of light, whereas 310 cubic membranes in Anabaena sp. were observed in fully illuminated cultures. The analysis of micrographs (Lang, 1965) of developing heterocysts (cells involved in nitrogen fixation) of Anabaena azollae clearly revealed several TEM projections of more or less developed cubic membranes (Landh, 1996) . Although heterocysts lack the photosynthetic apparatus, these cubic membranes appear to arise by continuous folding of the thylakoid membranes. 3.2.4.1. Chloroplasts of green algae Zygnema In certain green algae species the chloroplast membrane(s) tend to form more complex morphologies than the simple ''lamellar-like'' structures. Chloroplasts of the green alga Zygnema transform to G-type cubic membrane (Fig. 6.6 ) during the log phase of cell culture (Deng and Landh, 1995) . An analysis of previously reported electron micrographs by McLean and Pessoney (1970) , which described ''lamellar lattices'' in Zygnema chloroplasts, indeed revealed a primitive (P) subtype of cubic membrane (Landh, 1996) . This particular structure represents a continuous cubic membrane organization that is composed of several, mostly parallel, lipid bilayers (Deng, 1998) . The fine structure of the PLB has been extensively studied by electron microscopy (Gunning, 1965; Gunning and Jagoe, 1967; Gunning and Steer, 1975; Israelachvili and Wolfe, 1980; Menke, 1962 Menke, , 1963 Murakami et al., 1985; Osumi et al., 1984; Wehrmeyer, 1965a, b,c) . Three basic space-lattice structures of the PLB have been proposed: (i) a primitive cubic lattice in which the fundamental unit is a hexapode (Granick, 1961; Gunning, 1965; Gunning and Jagoe, 1967) , (ii) a diamond-based face-centered cubic lattice in which the fundamental unit is a tetrapode (Gunning and Steer, 1975; Murakami et al., 1985; Osumi et al., 1984; Wehrmeyer, 1965b) , and (iii) a hexagonal Wurtzite-type of lattice (Ikeda, 1968; Wehrmeyer, 1965c; Weier and Brown, 1970) . The double diamond-type cubic lattice is presumably the most common cubic structure of the PLB (Landh, 1996) . The formation of cubic membranes in the NE is not confined to the cytoplasmic side (i.e., the nuclear ER), but may also occur at intranuclear sites. This may appear surprising, however, formation of cubic membranes within nuclei could be realized by invaginations of a proliferating inner nuclear membrane. Intranuclear cubic or tubular membrane organizations usually develop in fast replicating neoplastic (tumor) cells (Babai et al., 1969; Karasaki, 1970) or non-neoplastic cells such as oocytes (Kessel and Beams, 1968; Miller, 1966) . Their presence might play a role in mitotic activity or in facilitating nuclear-cytoplasmic communication. In human cells, intranuclear tubular (hexagonal or cubic) membrane organization was demonstrated in the endometrium during the secretory phase of the menstrual cycle (Bourgeois and Hubert, 1988; Ghadially, 1988) . Progesterone and medroxyprogesterone can induce tubular structure formation in human endometrium (Kohorn et al., 1972) , which suggests a role of an extrinsic hormonal factor in cell membrane organization. An extensive review of the literature reveals that virtually all membranes are capable of forming cubic structures. Their origin thus seems to be strongly coupled to the mechanisms of membrane biogenesis in general and, therefore, cubic membranes are to be considered as a defined configuration of cytomembranes. The formation and growth of cubic membranes may be a selective process to fulfill a specialized purpose under ever changing intracellular conditions. Thus, understanding the underlying rules(s) for the physiological selection between the different membrane morphologies is key. It is now well established that proteins may induce phase transition in lipid membranes resulting in new structures not observed in pure lipidwater systems (Bouligand, 1990) . However, in principle, any amphiphilic molecule may be able to induce cubic membrane structures. Depending on the structure and nature of the proteins, their interactions with lipid bilayers can be manifested in very different ways. On the other hand, evidence from in vitro studies clearly differentiates membrane-forming lipids for their propensity to form nonlamellar structures, according to the molecular shape concept. The important structural role of membrane lipids in promoting cubic membrane formation in vivo is undisputed; however, only very recent evidence obtained from amoeba Chaos cells has correlated specific alterations of membrane lipids to cubic membrane formation in vivo (Deng et al., submitted) . Although lipids extracted from these cells may assemble to cubic phases also in vitro ( Fig. 6.8 ), marked differences in lattice size clearly indicate that additional factors-presumably proteinsexist in vivo that determine the overall 3D appearance of these structures. Induction of cubic membranes in Chaos cells upon starvation represents one rare example to experimentally address the molecular mechanisms leading to their formation in the biological context. From a topological point of view, cubic membranes appear to be formed from a structural ''template'' (the precursor of a cubic membrane), such as invaginations of a membrane. After initiation, further accumulation of membrane lipids may lead to intersection-free highly convoluted invaginations. During the folding process, the membrane must remain a continuous fluid structure that grows and interconnects without losing its polarity and integrity. Thus, the topology of the cubic membrane depends on the topology of its precursor structure. If one isolated invagination process triggers the membrane folding process, the topology will be that of a sphere, as is the case for vesicle formation during endocytosis or secretion. If more than one invagination takes place, it requires points of fusion to achieve a three-dimensionally interconnected membrane. Perhaps it is this symmetry that is the driving force for fusion; if fusion did not occur one would expect several independent cubic membrane systems to form, which would not necessarily bear any spatio-temporal correlation between each other or the periodicity of the template. Cubic membrane formation is frequently associated with the overexpression of certain ER-resident proteins and, to a lesser extent, with overexpression of some inner mitochondrial membrane proteins. Table 6 .2 lists major membrane proteins that have been shown to induce cubic membrane formation upon experimental dys-regulation. 4.1.1. ER proteins HMG-CoA reductase is an ER-resident protein that is anchored to the membrane by seven membrane-spanning domains in its N-terminal part and has its catalytic domain extending to the cytoplasmic side. Elevated expression of HMG-CoA reductase is often associated with structural membrane alterations. The transmembrane region is indeed required to form crystalloid membrane structures of hexagonal (Fig. 6.5D ) or cubic A B 2 µm 200 nm Figure 6 .8 Lipid dispersion prepared from amoeba lipids (Deng, unpublished) . TEM images of liposomes derived from lipids extracted from fed and 7d starved Chaos cells. (A) Multilamellar or whorl-like structures generated from fed cell lipids with numerous randomly distributed tubular structures, but without higher order phases. In contrast, (B) TEM data of lipid dispersion generated from lipids that were isolated from 7d starved amoeba cells show highly ordered domains. ( Fig. 6 .5C) morphologies, upon overexpression. Deletion of two of the seven membrane spanning regions or a truncated protein did not result in crystalloid ER formation, and the protein localized to disordered sheets rather than packed membrane tubules under these conditions. High expression levels of the soluble fragment of HMG-CoA reductase did not induce any crystalloid ER, again indicating that it is the transmembrane domain of HMG-CoA reductase that plays an important role in determining the structure of crystalloid ER ( Jingami et al., 1987; Yamamoto et al., 1996) . Crystalloid ER is frequently observed in CHO cells upon overexpression of the HMG-CoA reductase gene, or in UT-1 cells, which are a mutant variant of CHO cells that overexpress this gene by 500 fold (Fig. 6.5; Chin et al., 1982) . Notably, despite the presence of elevated levels of HMG-CoA reductase, which is the key enzyme of sterol biosynthesis, the membrane of the crystalloid ER appears to have very little cholesterol. Upon addition of cholesterol to UT-1 cells, which intercalates into the ER membrane, HMG-CoA reductase was subsequently degraded and the crystalloid ER disappeared ( Jingami et. al., 1987) ; sterol supplementation drastically reduced the rate of HMG-CoA reductase synthesis and also prevented the formation of new crystalloid ER. It was therefore speculated that the cubic membrane is an alteration in the feedback control of cholesterol synthesis, for the production of sterols and the biogenesis of smooth ER. Interestingly, administration of compactin, which is an HMG-CoA reductase inhibitor, also leads to HMG-CoA reductase overexpression, and induces the formation of stacked and aggregated structures, which were termed ''karmellae'' in yeast (Wright et al., 1988) . The expression of msALDH in COS-1 cells also leads to alterations of the ER structure. Both HMG-CoA reductase and msALDH proteins possess large domains exposed on the cytoplasmic surface of the ER membrane, similar to the ER-resident protein, cytochrome P450. This led to the hypothesis that the formation of crystalloid membranes may require the expression of ER-resident proteins with large cytoplasmic domains (Sandig et al., 1999; Snapp et al., 2003; Yamamoto et al., 1996) . Overexpression of specific ER-resident proteins such as cytochrome b (5) in COS-7 cells also triggers the formation of ''whorls and crystalloid OSER structures'' (Snapp et al., 2003) . It was proposed that the biogenesis of OSER structures involves weak homotypic interactions between cytoplasmic domains of proteins and may underlie the formation of other stacked membrane structures within the cells as well. Time-lapse imaging of OSER biogenesis revealed that these structures formed rather quickly once a threshold level of OSER-inducing proteins was exceeded; OSERformation also involved gross remodeling of surrounding tubular ER. In this system, the attachment to the cytoplasmic domain of different ER-resident membrane proteins of green fluorescent protein (GFP) that is capable of low affinity, head-to-tail dimerization was sufficient to induce OSER formation upon overexpression in living cells. Homotypic low affinity interactions between cytoplasmic domains of proteins thus can differentiate tubular ER into stacked lamellae or crystalloid structures; such a mechanism may underlie the reorganization of other organelles into stacked structures as well (Snapp et al., 2003) , and provides an intriguing model system to investigate the cellular and molecular requirements for cubic membrane formation. Only a few mitochondrial proteins have been reported to induce and maintain tubular inner membrane morphology upon overexpression (Mannella, 2006) , however, none of them was correlated with well-defined cubic membrane formation. Mitofilin, F1F0-ATPsynthase, and fission-fusion proteins may induce tubular or stacked lamellar and whorl-type membrane structures upon experimental overexpression. F1F0-ATPsynthase is an essential enzymatic complex of the mitochondrial inner membrane, which couples the proton electrochemical gradient generated by the respiratory chain to ATP synthesis. Various studies have shown that this complex is strongly implicated in the curvature of the inner mitochondrial membrane (reviewed by Voeltz and Prinz, 2007) . Dimerization of the complex drives tubulation of the cristae (Dudkina et al., 2005; Strauss et al., 2008) , while further oligomerization of these dimers is responsible for the formation and/or stabilization of inner membrane tubules. Mitofilin is a mitochondrial inner membrane protein, which assembles into a large multimeric protein complex. siRNA knockdown of mitofilin in HeLa cells yielded mitochondria with disorganized mitochondrial inner membranes: they failed to form tubular or vesicular cristae and appeared as intermittently fused, closely packed stacks of membrane sheets, resulting in a complex maze of membraneous networks (John et al., 2005) . Mitofilin thus appears to be a key organizer of mitochondrial cristae morphology ( John et al., 2005) . The role of mitochondrial proteins in cubic membrane formation in starved amoeba Chaos, which is a suitable model for analyzing reversible cubic membrane formation, is currently under investigation in the authors' laboratories. Recently a class of membrane proteins known as morphogenic proteins was identified to shape the tubular ER in yeast and mammalian cells. These proteins are highly enriched in the tubular portions of the ER and virtually excluded from other regions. The study by Voeltz and coworkers (2006) illustrated the role of Rtn4a/NogoA, a member of the ubiquitous reticulon protein family that share a conserved C-terminal reticulon domain. Overexpression of Rtn4a/NogoA in mammalian cells, promoted the formation of ER tubules; membrane tubule formation in vitro, on the other hand, was prevented by anti-Rtn4a/NogoA antibodies. Similar results were observed in the yeast Saccharomyces cerevisiae, in which overexpression of Rtn1 (the yeast ortholog of Rtn4a/NogoA in mammals) also enhanced tubular ER formation. Yeast mutants lacking both Yop1 (an Rtn1 paralog) and Rtn1 showed a disrupted tubular ER, underscoring the important function of these proteins in shaping membrane structures. Reticulons contain long, hydrophobic domains that are inserted into the outer leaflet of the lipid bilayer. Since the hydrophobic domains are longer than required for spanning a bilayer membrane, it is believed that they promote a hairpin-like insertion into the lipid bilayer and give the overall appearance of a wedgelike protein. Thus, a local concentration of reticulons might induce and stabilize a high, positive membrane curvature. Although morphogenic proteins are believed to induce membrane curvature and shape spherical or tubular morphology, to date, none of them has been reported to induce highly organized membrane structures such as hexagonal or cubic membranes in vivo. One exception to the rule is the observation of a t-tubular system in skeletal muscles (Ishikawa, 1968) , in which cubic membrane organization has been associated with caveolin-3 expression (Parton et al., 1997) . Caveolin is synthesized in the ER but mostly resides in certain domains of the plasma membrane. Caveolins are known to play a role in inducing and maintaining membrane curvature. Individual caveolin molecules are cotranslationally integrated into the bilayer of the ER. Similar to reticulons, caveolins form a hairpin-loop within the bilayer, and tend to form hexa-or heptamers. These oligomers may leave from the ER and are transported via the Golgi apparatus to the plasma membrane, where, by a yet unknown mechanism, they induce localized sites of membrane curvature, known as caveolae (Bauer and Pelkmans, 2006; Voeltz and Prinz, 2007) . Up to date, cubic membrane formation is mainly associated with overexpression of certain membrane-resident proteins. Although cubic phases are formed by ''nonlamellar'' lipids in vitro, only very few data directly correlate cubic membrane formation with cellular lipid profiles in vivo (Ryberg et al., 1983) . In this study it was shown that the molar ratio of monogalactosyl diacylglycerol to digalactosyl diacylglycerol was higher in the PLB fraction that exhibits cubic membrane morphology, than in the prothylakoid fraction. Also, the content of glycolipids and protochlorophyllides was increased in the PLB fraction (Ryberg et al., 1983) . Lipid analyses of fed and starved amoeba (C. carolinense) recently performed in the authors' laboratory (Deng et al., submitted) may provide a first clue towards understanding the role of membrane lipids in determining cell membrane architecture. Detailed lipid analysis of amoeba Chaos exhibiting cubic membrane organization in their mitochondria, revealed an unusually high concentration of highly polyunsaturated fatty acids (C22:5; docosapentaenoic acid, DPA). Three predominant lipid species, namely plasmalogen PE (C16:0p/C22:5), plasmalogen PC (C16:0p/C22:5), and diacyl-PI (C22:5/C22:5), were identified in amoeba Chaos lipid extracts (Fig. 6.9) , and their relative amounts increased up to 2.5-fold under starvation stress conditions (Deng et al., submitted) . A rich body of data (for review see Nagan and Zoeller, 2001) suggests that plasmalogens-which are also present in mammalian cell membranes-may serve as mediators of membrane dynamics due to their high propensity to form inverted hexagonal structures. This property has also suggested a potential role for plasmalogens in facilitating membrane fusion processes (for review see Brites et al., 2004) . Biophysical studies have also shown that the presence of plasmalogen PE lowers the lamellar to hexagonal-phase transition temperature (Lohner, 1996) . Interestingly, CHO cells, which display massive membrane rearrangements upon HMG-CoA reductase overexpression (Fig. 6 .5), are also rich in plasmalogen lipids (up to 11% of their total phospholipids), especially plasmalogen PE (Nagan et al., 1998) . The observation that weak molecular interactions, for example, by membrane proteins, may lead to cubic membrane transformation also suggests that electrostatic interactions play an important role in that process , Snapp et al., 2003 . In a recent experimental study on the effects of divalent cations in the isolation buffers for mitochondria, we were able to demonstrate that the presence of EDTA up to 10 mM preserved mitochondrial cubic membranes in vitro (Fig. 6 .10) (manuscript in preparation). Thus, pH and the nature of the electrolytes in the cellular milieu are likely to be important factors affecting cubic membrane morphology and integrity. In vitro studies using monoolein membranes containing negativelycharged dioleoylphosphatidic acid have shown that the electrostatic interactions caused by surface charge of the membranes (Li et al., 2001) , charged short peptides such as poly-L-lysine , Ca 2+ concentration , and low pH (Okamoto et al., 2008) play an important role in the phase transition between lamellar and cubic phases as well as on the stability of cubic phases. As a consequence of altered electrostatic interactions at the membrane interface, induced either by the A B C 2 µm 2 µm 2 µm Figure 6 .10 Electrostatic effects on cubic membrane organization (Deng, unpublished) . Mitochondria of amoeba Chaos exhibiting cubic membrane arrangements were isolated in a buffer media containing (A) 50 mM, (B) 1 mM, or (C) 10 mM EDTA. Increasing the concentration of EDTA stabilized mitochondria with cubic morphology, suggesting a modulatory function of divalent cations in cubic membrane formation. increase in surface charge density of the membrane or by a decrease in salt concentration, the lipid membrane phase may change from the lamellar to the cubic phase. Such cubic phases may not only form to adopt the altered membrane proteins or charge distribution, but may also provide the means to rapidly adjust cellular physiology to the changing environmental conditions, such as fluctuations of (local) intracellular Ca 2+ levels. The ''breathing'' of cubic membranes, that is, the changes in lattice size as demonstrated in vitro (de Campo et al., 2004) , may represent an immediate biophysical response, which may allow for a rapid adaptation to the water content and ion concentration or charge distribution in a given membrane compartment also in vivo. Notably, cubic membrane morphologies are often associated with deregulated protein synthesis, cellular stress, or more severe pathological conditions. This view, however, is perhaps somewhat biased since morphological abnormalities are typically investigated for diseased cells rather than for ''wild type'' conditions. Nevertheless, the correlation of specific membrane alterations in the course of acute or chronic cellular stresses needs closer consideration. Virus-induced membrane transitions, generally referred to as cytomembraneous inclusions, are a hallmark in experimental and pathological samples (Almsherqi et al., 2005) . However, due to the absence of a clear view of the 3D nature of these membrane structures, they appear under numerous nicknames in the literature, such as ''tubulocrystalline inclusions'' in HCV infected liver (Schaff et al., 1992) , ''convoluted membraneous mass'' in viral St. Louis Encephalitis (Murphy et al., 1968) , and ''TRS'' in SIV (Kaup et al., 2005) and SARS-virus infected Vero cells (Goldsmith et al., 2004) . The unexplained mechanism behind the formation of convoluted cubic membranes upon viral infection starts to unfold based on the structural similarity to crystalloid ER membranes induced by overexpression of HMG-CoA reductase in UT-1, or the parental CHO cells (Fig. 6 .5), as well as in A-431 (human epidermal carcinoma) cells. Some evidence suggests that virus infection and deregulation of HMG-CoA reductase are mechanistically linked, resulting in similar membrane phenotypes. For example, West Nile Virus infection is associated with local cholesterol alterations of the plasma membrane of the host cell that leads to a sequestration of membraneous sites of viral replication . Depletion of cholesterol in the plasma membrane triggers HMG-CoA reductase upregulation and consequently leads to the formation of a crystalloid (cubic or hexagonal) ER membrane. The virus-induced convoluted membrane was reported to be essential for viral replication and survival: administration of cholesterol that reverses the HMG-CoA reducase-induced convoluted membrane formation in the infected cells significantly suppresses viral replication . A recent study has also shown that virus-induced membrane complexes might provide partial protection against the host immune response (Hoenen et al., 2007) and hence offer a site for efficient viral replication or facilitate nucleo-cytoplasmic transport of genetic material (Almsherqi et al., 2008) . Cubic membranes (often labeled as TRS) have been reported to occur in the cytoplasm of breast carcinoma (Seman et al., 1971) , subcutaneous myxoma (Stoebner et al., 1972) , malignant lymphoma (Uzman et al., 1971) , in the nucleus of human osteosarcoma cells (Murray et al., 1983) , alveolar cell carcinoma (Ghadially et al., 1985) , and gastric adenocarcinoma (Caruso, 1991) . Since viral infections frequently lead to cubic membrane formation, it would not be surprising to observe cubic membrane structures also in cases of virus-related tumors, such as leukemias, lymphomas, and in virus-induced hepatocellular carcinoma (Uzman et al., 1971) . TRS appear to be nonspecific to tumor differentiation or malignancy as they develop in highly replicative undifferentiated cells as well as in differentiated tumor cells. Therefore, due to the limited number of reported cases of cubic membrane structure in neoplastic cells, they currently are not yet diagnostically useful in the classification of tumors or in clinical prognosis. However, TRS could be used as a marker for viral-induced neoplasia, for example, hairy cell leukemia (Mantovani et al., 1986) . Several muscular and neuromuscular diseases are associated with periodic membrane transformation of t-tubules of striated muscles, usually referred to as honeycomb structures. T-tubular morphological membrane transformation has been described in denervated muscles (Gori, 1972; Madarame et al., 1986; Miledi and Slater, 1969; Pellegrino and Franzini, 1963) , in the muscles with induced experimental myopathy , bupivacaine-induced myonecrosis (Huxley and Taylor, 1958) , and in tenotomized muscles of the rat (Andreev and Wassilev, 1994) . They have also been observed in various human muscles as a consequence of muscular diseases (Borg et al., 1989; Cornog and Gonatas, 1967; Engel and Dale, 1968; Engel and Macdonald, 1970; Gori, 1972; Iorio Di et al., 1989; Miike et al., 1984) . The fact that cubic membrane organization appears under pathological conditions of myopathy support the notion that they may be formed in response to stress conditions, such as a decrease in cell volume in the case of muscular dystrophy. Thus, it could be speculated that the potential function of cubic membrane structures is to maintain cellular integrity by regulating the volume of the cell (organelle) and/or to accommodate stress-induced membrane-resident proteins. Interestingly, induced formation of honeycomb t-tubules may also be part of a developmental program as these membrane structures are also observed in tadpole tail muscles that spontaneously degenerate during metamorphosis (Sasaki et al., 1985) . Frequent transformation of t-tubules into G-type cubic membrane (honeycomb) organization in regenerating muscle fibers post pathological or experimentally induced muscular dystrophy may reflect the adaptive reorganization of the membrane system in the regenerating cell. Cubic membranes (including those labeled as TRS) have been frequently reported to occur under conditions and in cell types with an immunological background, for instance in diseases in which autoantibody production is a main factor in the pathogenesis. These include diffuse connective tissue diseases such as systemic and discoid lupus erythematosus and Sjögren syndrome (Nakamura, 1974) or organ limited diseases, such as thyroiditis, gastritis, myasthenia gravis, and celiac disease (Helder and Feltkamp-Vroom, 1974) . TRS are also reported in autoimmune diseases characterized by deposition of immune complexes or factors, which are discrete in comparison to the diffuse connective tissue diseases like rheumatoid arthritis, nephritis, and amyloidosis (Helder and Feltkamp-Vroom, 1974) . Indeed, cubic membrane organization is frequently reported in immune deficiency diseases such as HIV (Kaup et al., 2005) . Such ultrastructural membrane alterations are often reported in endothelial cells and in lymphocytes; therefore, TRS should be regarded as potential markers of autoimmune diseases that are of a systemic nature. The frequent appearance of cubic membranes in several specialized cell types, in response to environmental conditions, stress or infection, poses the intriguing question as to their specific functions. It is possible that cubic membranes are but an inevitable self-assembled product of the complex molecular mixture of lipids and proteins, the result of ''simple'' molecular packing considerations and inter-molecular interactions. Even though this is appealing to the long and unresolved debate about ''nonlamellar'' lipids in conjunction with cell membranes, an increasing body of evidence suggests that these structural organizations might have to fulfill a purpose and their formation cannot be rationalized solely by spontaneous molecular packing. It is important to stress that the proposed functions of cubic membranes in the following discussion are hypothetical, although recent experimental data provide support to some of these hypotheses. Continuous hyperbolic layers, as represented by cubic membranes, partition space into discrete and unconnected subvolumes. By definition, a multimembraneous structure consisting of (n) membranes, partitions space into (n þ 1) physically distinct, intertwined, but separate subspaces. The identity of each space itself is not a consequence of the existence of a cubic membrane; rather it is an effect of a topologically invariant membrane morphogenesis. Although an intracellular space maintains its identity as long as membrane continuity is preserved, it is only by means of a hyperbolic membrane structure that such spatial relations can be rigorously defined. The identification of cubic membranes in multiple cell types and tissues clearly demonstrates that continuous intracellular membranes are much more frequently adopted than generally acknowledged. Intracellular and inter-organelle trafficking of macromolecules and communication are active areas of research, yet no unified model exists. To what extent intracellular trafficking depends on or can be optimized through specific types of membrane organization, for example, as continuous 3D space partitioners or networks, is unknown. In the three dimensions of a cell, the partitioning of the intracellular space into subvolumes-leading to an interpenetrated pipeline system-could in principle be orchestrated by membrane organization, which ultimately controls spatio-temporal activities, including intracellular trafficking and transportation, and fast response to physiological alterations such as changing temperature, osmolarity or pH. Recognition of the existence of topologically distinct spaces through the formation of cubic membranes implies that cell space is restricted and predetermined to maintain distinct but interconnected subcellular domains. Cubic membranes may induce enrichment-or exclusion-of certain lipids and proteins, as a prerequisite for vesicle-mediated subcellular trafficking. They may also function as partitioners within a membrane, to create subdomains of specific molecular composition and function. It has been repeatedly noted that the stage of cell division and differentiation has a strong influence on the formation of cubic membranes. Cells that undergo rapid cell division and differentiation, such as the differentiating sieve elements, cells during spermatogenesis, or tumor cells are well over-represented in the collection of cubic-membrane forming cells (Table 6 .1). Obviously, during cell division and differentiation events, there is a greater need for regulated spatio-temporal transport, as well as cellular communication, which is particularly well illustrated during spermatogenesis (Table 6 .1). In the case of differentiating sieve elements, cubic membranes might have a particular role in the assimilated transport process. Finally, it is of interest to note that aggregates of ''synaptic vesicles'' often resemble cubic membranes. This can be taken as an indication of a possible on-off mechanism of membrane continuity, which might account for a regulative capacity for the controlled release of transmitter substances. Several more general functionalities are under consideration for cubic membranes. In particular, a cubic bilayer arrangement could serve as a regulator of chemical or physical potentials across the membrane surface. This is indicated in several cases in which cubic membranes have been found to be sensitive to the growth medium. An osmo-regulative capacity of a plasma membrane-associated cubic membrane can be envisioned, which might serve to allow rapid adjustment to osmotic changes. Such a function is, for instance, consistent with the presence of cubic membranes in a variety of epithelial cells (Table 6 .1). Cubic membranes may also be involved in curvature-controlled activation and regulation of membrane enzyme activities. For instance, diacylglycerols, which may function as second messengers to activate protein kinase C (PKC), display a strong propensity to form negatively curved membrane structures. The activity of PKC, however, is not specifically dependent on lipids that induce reverse hexagonal phases (Senisterra and Epand, 1993) , and thus, reversed cubic phases. In view of the ubiquitous occurrence of cubic membranes it would be of interest to investigate the influence of PKC on cubic phases, and vice versa, to eventually correlate the geometry of the environment to protein activity. Certain cubic membrane structures are apparently strongly linked to specific functions, such as the cubic structure found in the PLB of photosynthetic cells in higher plants. A physical role has been proposed for the selection of D-surface geometry (Guo et al., 1995) , based on theoretical considerations on how the geometry of crystals controls the emission or absorption of certain wavelengths of light through the existence of photonic band-gaps (Babin et al., 2002) . Although the D-surface is isotropic, its geometry is such that it may potentially trap photons. The absorbed energy could then be used by certain molecules that are positioned along a particular lattice direction, and, for instance, trigger conformational changes to revert PLB into an active thylakoid membrane geometry. A similar structural role can be considered for the selection of different subtypes of cubic membrane architecture (photosome) in bioluminescent scaleworms (Bassot, 1964 (Bassot, , 1966 . Interestingly, the photosome membrane organization has a D subtype cubic membrane in the resting (unstimulated) state, however, upon electrical or optical stimulation the membrane configuration changes and acquires P subtype. Do different cubic membrane subtypes manipulate different wavelengths? Does the function of the cubic membrane change with the specific alteration of its geometrical configuration? The answers to these questions clearly deserve further investigations. In addition, several other photoactive cell types exist that contain cubic membranes. Mitochondria in the retinal cone of the tree shrew (Tupaia glis) (Foelix et al., 1987) may adopt an isotropic membrane structure that allows efficient capture of the incoming light; in an alternative model, this multilayer G-surface cubic arrangement of the mitochondrial membrane ( Fig. 6 .7) may preferentially reflect UV light before reaching the outer segment of the retina, thus representing a specialized optical filter system. Although the specific functions of cubic membranes in biological systems are still to be uncovered, recent studies on the physical properties of such highly ordered membrane structures have suggested a range of potential applications, beyond conventional liposome technologies. Dispersed liquid crystalline phases such as bicontinuous cubic dispersions (known as Cubosomes ) have been the focus of recent studies as potential drug delivery agents (Barauskas et al., 2005) . Lipids forming cubic phases in vitro are also well-established matrices, for example, for membrane protein crystallization (Seddon et al., 2004) , but are not considered here in the context of cubic membranes. Cubic membrane function is potentially linked to intracellular trafficking processes for macromolecules. Indeed, isolated mitochondria with cubic membrane organization from starved amoeba cells (see above) have recently been shown to incorporate and retain short oligonucleotides (ODN) with high efficiency (Fig. 6.11 ) (Almsherqi et al., 2008) . Although the molecular basis for the high affinity of ODN to cubic membranes has not been uncovered yet, it is reasonable to assume that it is strongly promoted by electrostatic interactions with the highly curved and extended membrane surface. Furthermore, delivery of ODN-cubic membrane complexes to mammalian cells in culture appears to be very effective and might, therefore, provide an attractive alternative to currently employed cationic lipoplexes and promises high efficacy and reduced cytotoxicity. Use of cubic membranes of biological origin as a carrier for DNA transfection or delivery of other nucleic acids, such as small interfering RNA and/or short hairpin RNA is currently under active investigation (Almsherqi et al., 2008) . The photonic properties of bi-or multicontinuous cubic phases based on triply periodic level surfaces (G, D, and P) have been extensively studied in materials science (Babin et al., 2002; Maldovan et al., 2002; Urbas et al., 2002) . In general, the lattice size of the photonic crystal has to be of the same magnitude as the wavelength range it controls. Photonic crystals based on triply periodic surfaces with the largest photonic band gaps known are of type D and G cubic morphology (Babin et al., 2002) . Similar G-surfaces describe the cubic membrane organization of the inner mitochondrial membranes (Fig. 6.7) in the tree shrew's (Tupaia belangeri) retina (Foelix et al., 1987) and photosynthesis-related membranes in prolamellar bodies of higher plants and chloroplasts of the green algae Zygnema (Fig. 6.6) (Deng, 1998; Deng and Landh, 1995) . Based on these similar cubic geometries and relevant lattice sizes, it is tempting to speculate that perhaps Tupaia mitochondrial membranes and cubic membranes in Zygnema chloroplasts and PLB of higher plants may function as photonic crystals. The 12-layered cubic membrane organization of the mitochondria in retinal cones of tree shrew Tupaia and multilayer grana of photosynthetic membranes may thus enable these membranes to amplify, refract, or absorb certain wavelengths of light. Whether such an elaborate membrane arrangement is a protective response or whether it provides a specialized reaction center for embedded proteins awaits detailed analysis. The frequent appearance of nonlamellar membrane arrangements such as cubic membranes in cells under stressed or pathological conditions points to an intrinsic cellular response mechanisms. The extensive generation of membrane surfaces to facilitate exchange reactions between two (or more) sub-volumes, or the sequestration of specific lipids or proteins into membrane domains of nonlamellar morphology may provide a physiological advantage to cope with various stress phenomena. Current analyses of nonlamellar membrane arrangements are largely restricted to the descriptive level; the identification of inducible membrane systems, such as in virus-infected cells or the reversible transition of mitochondrial inner membranes of amoeba Chaos to cubic morphology upon starvation, however, opens new avenues for understanding the molecular mechanisms and cellular requirements underlying these membrane arrangements. Lipidomics and proteomics techniques on the one hand, and cryo-electron tomography on the other, hold great promise to uncover the mysteries of cubic membranes in living cells, in healthy and diseased states. 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Lack of protection by vitamin E Fine structure and function of interrenal (adrenocortical) cells of dexamethasone-treated trout (Salmo fario L.) 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Taking another look at membrane bound cell spaces Electron microscopy study of heterocyst development in Anaebaena azollae Strasburger Structures in a blue-green alga resembling prolamellar bodies Endoplasmic reticulum-derived pinwheels in wheat infected with wheat spindle streak mosaic virus Cubic lipid-water phases: Structures and biomembrane aspects Structural relationships between lamellar, cubic and hexagonal phases in monoglyceride-water systems. Possibility of cubic structures in biological systems Mitochondrial organization in skeletal muscle of the rat soft palate The ultrastructure of the integument of the American eel, Anguilla rostrata Effect of electrostatic interactions on phase stability of cubic phases of membranes of monoolein/dioleoylphosphatidic acid mixtures The membrane lattice: A novel organelle f the trypanosomatid flagellate Leptomonas collosoma Retinal structure in Latimeria chalumnae Is the high propensity of ethanolamine plasmalogens to form nonlamellar lipid structures manifested in the properties of biomembranes? Characean charasome-complex and plasmalemma vesicle development Structural studies by electron tomography: From cells to molecules Biological significance of lipid polymorpholism: The cubic phase commentary Chlorphentermine-induced ultrastructural changes in liver tissues of four animal species Experimental chloroquine myopathy Cholesterol manipulation by West Nile virus perturbs the cellular immune response Ultrastructural studies on muscular atrophy in Marek's disease. I. Denervation atrophy in chicken skeletal muscle. A light and electron microscopic study Photonic properties of bicontinuous cubic microphases Structure and dynamics of the mitochondrial inner membrane cristae Hairy cell leukemia with ultrastructural finding of 'tubuloreticular inclusions' in hairy cells: A possible marker of a virus-induced disease? 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I. Fine structure of the complex patterns in the mitochondria of Pelomyxa carolinensis Wilson (Chaos chaos L.) Electron microscopy of the in vitro development of mammalian motor end plates Ultrastructure of phloem in palms II. Structural changes, and fate of the organelles in differentiating sieve elements Ultrastructure of phloem in palms III. 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VII. Membrane denaturation following carbon tetrachloride Evolution de quelques organites cytoplasmiques au cours de la maturation de l'oosphére de Selaginella Kraussiana A. Br Organisation du réticulum endoplasmique dans le cytoplasme basal de l'oosphére de Selaginella Kraussiana A. Br Plant Membranes. Endo and Plasma Membranes of Plant Cells Wiley The fine structure of the eye of the Weinberg snail (Helix pomatia L.) 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Electron microscopical observations on spermatids of Eisenia foetida during the cytoplasmic reduction Tubular bodies in the cytoplasm of spermatids of Planorbarius corneus L. (Basommatophora) Tubular inclusions. Discovery in endothelial cells of a subcutaneous myxoma Dimer ribbons of ATP synthase shape the inner mitochondrial membrane Soft tissue sarcoma with complex membranous and microtubular inclusions Light and electron microscope studies of morphological changes of mitochondria during spermatogenesis in the grasshopper The influence of X-rays on organelle induction and differentiation in grasshopper spermatogenesis Inositol 1,4,5-trisphosphate receptor causes formation of ER cisternal stacks in transfected fibroblasts and in cerebellar Purkinje cells Giant mitochondria in a pleomorphic adenoma of the submandibular gland Ultrastructure of pseudochromes and calottes in spermatogenic cells of the backswimmer, Notonecta undulata (Say) Unusual membrane formations in HEp-2 cells infected with Ilheus virus Occurrence of crystalloids in the sinusoidal endothelial cell of a crabeating monkey liver Changes in the endoplasmic reticulum during differentiation of a sieve element in Gossypium hirsutum Tubuloreticular structures induced by rotavirus infection in HT-29 cells Modified smooth endoplasmic reticulum in type II cells of rabbit taste buds The post-fertilization stages of red-algae: The fine structure of the fusion cell of Erythrocystis Bioconcinuous cubic block copolymer photonic crystals Tubular arrays in the endoplasmic reticulum in human tumor cells The ultrastructure of glandular cells in the external dendritic organ of some marine catfish A model system for studying membrane biogenesis. Overexpression of cytochrome b5 in yeast results in marked proliferation of the intracellular membrane A class of membrane proteins shaping the tubular endoplasmic reticulum Sheets, ribbons and tubules-How organelles get their shape Ca 2+ -sequestering smooth endoplasmic reticulum in an invertebrate photoreceptor. I. Intracellular topography as revealed by OsFeCN staining and in situ Ca accumulation On the crystal structure of the so called prolamellar body in proplastids of etiolated beans. I. Pentagondodecaeder as center of concentric prolamellar body On the crystal structure of the so called prolamellar body in proplastids of etiolated beans. II. Wurtzit lattice as a tubular model of the prolamellar body On the crystal structure of the so called prolamellar body in proplastids of etiolated beans. II. Zincblende as a tubular model of the prolamellar body Formation of the prolamellar body in 18-day, darkgrown seedlings Overproduction of fumarate reductase in Escherichia coli induces a novel intracellular lipid-protein organelle Light and electron microscopic studies of Ascobolus stercorarius. II. Ascus and ascospore ontogeny The fine structure of Joseph cells in the brain of Amphioxus Paracrystalline endoplasmic reticulum is typical of gametogenesis in Hemiptera species The development of the sieve elements of Pinus pinea Endoplasmic reticulum aggregates of ordered structure Increased amounts of HMG-CoA reductase induce ''karmellae'': A proliferation of stacked membrane pairs surrounding the yeast nucleus Formation of crystalloid endoplasmic reticulum in COS cells upon overexpression of microsomal aldehyde dehydrogenase by cDNA transfection Lamellar to tubular conformational changes in the endoplasmic reticulum of the retinal pigment epithelium of the newt, Notophtalmus viridescens The fine structure of the developmental stages of the microsporidian Nosema apis Zander Lattice bodies and filament bundles in apothecial cells of the fungus Ascobolus On the distribution and development of lattice bodies in apothecial cells of the fungus Ascobolus The authors apologize to the colleagues whose work has not been cited due to space limitations. We thank Felix Margadant for critical reading of the manuscript, Mark Mieczkowski for the ''Cubic Membrane Simulation Projection'' program (QMSP), and Aik Kia Khaw for his art work presented in Fig. 6 .4. The technical support by Chwee Wah Low, Li Ling Olivia Tan, and Mei Yin Shoon is gratefully acknowledged. Research in the authors' laboratories is supported by research grants NMRC (R-185-000-058-213) and BMRC from Singapore (R-185-000-065-305) to Y. D. and SFB Lipotox (project F3005) of the Austrian Science Fund to S.D.K.