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Kensuke Osada1,2
1National Institutes for Quantum and Radiological Science and Technology (QST), National Institute of Radiological Sciences (NIRS), Department of Molecular Imaging and Theranostics, 4-9-1 Anagawa, Inage-ku, Chiba, 263-8555, Japan
2PRESTO, Japan Science and Technology Agency, 4-1-8 Honcho, Kawaguchi, Saitama, 332-0012, Japan
DNA undergoes large volume transition from extended coil to compact state by polyion complexation with polycations for minimizing the contact surface area of the charge-neutralized polyplex from water [1-3]. The transition called DNA condensation is the essential mechanism of genomic DNA packaging and is the important process in preparing a nonviral gene delivery system [4-8]. The self-assembly formed from pDNA and block catiomers has been gaining attention as a potential systemic gene delivery system, in which the pDNA is condensed into a core by complexed with cationic block and the neutral blocks surround it as a shell to form a 100-nm-sized core-shell-structured polyplex micelle [9-12]. Polyplex micelles, launched from our group [13, 14], had been developed by the encouragement of the precedent development of polymeric micelles for drug delivery, which are currently under investigation of clinical trials [15, 16]. Originated from the firstly prepared polyplex micelles from PEG-b-P(Lys) [13, 17, 18], a variety of block catiomers or graft catiomers have been elaborated in order to improve the transfection efficiency by modulating parameters of their degree of polymerization (DP), grafting density for the case of graft catiomers, and varying mixing ratio with pDNA as described elsewhere in details [10, 17, 19, 20]. By these efforts, gene transfection efficiency has been remarkably promoted and a feasible formulation had proceeded to human clinical trial with local application [21, 22].
Nonetheless, development of polyplex micelles for systemic application has yet to be reached the level of clinical trial in spite of the structural analogy with polymeric micelles for drug delivery. This is mainly ascribed to the limited bioavailability of pDNA in active form at the final targeted nucleus; particularly, its instability in bloodstream precludes the secure delivery. To this end, the key issue that should be addressed is the packaging of pDNA into polyplex micelles because it regulates the basic character of polyplex micelles such as size, surface potential, stability, shape, and PEG crowding and thereby their biological performances such as blood circulation capacity, protection from nuclease attack, efficiencies of extravasation and migration into tissue, cellular entry efficiency, and transcription efficiency, all of which affect the ultimate gene expression efficiency. For achieving proper packaging, it is imperative to know the character of pDNA as a molecule and the principle mechanism of polyplex micelle formation so as to freely handle the structure. Moreover, it is necessary to know the suitable structure and the required functionalities to accommodate each step of delivery process. These processes should clearly point out the demanding issues for entirely managing the systemic gene delivery, which ultimately lead to a proper molecular design in structure and functionality to prepare polyplex micelles for achieving systemic gene therapy.
In this context, this review first focuses on the packaging of pDNA by block catiomers as the primal subject. Then, the required property and functionality for managing each of the delivery process are focused from intravenous (IV) injection to the last process of transcription. Finally, rational design criteria of block catiomers for systemic gene delivery are outlined.
It is important to first recognize the molecular character of pDNA for the sake of elucidating the mechanism of pDNA packaging. pDNA is a large molecule comprising typically a few kbp, which correspond to millions in molecular weight and a few micrometers in contour length, and has supercoiled closed circular form. DNA behaves as a semiflexible chain in solution with persistence length of 50 nm. Then, it is complexed with a large number of block catiomers for compensating the negative charges of pDNA, e.g. 200 block catiomers are required to compensate negative charges of pDNA of 5000 bp when block catiomers with 50 positive charges in their cationic segment are used. The formed polyplex micelles consist of single pDNA, wherein the concept of CAC is not defined as opposed to the polymeric micelles prepared from amphiphilic block copolymers, which are formed by association of multimolecules. Note that the single pDNA packaging is ensured as long as conducting the complexation at a diluted condition, which allows the accomplishment of the PEG shell formation before the collision of complexed pDNA to associate with neighboring complexed pDNA molecule due to translational motion. Otherwise, the secondary association occurs when the polyplex collision takes place faster than the formation of PEG shell, which is evidenced in the network-like complex formation by conducting the complexation exceeding the overlapping concentration of pDNA strands [23]. Polyplex micelles are characterized as approximately 100 nm particles by dynamic light scattering () and neutral zeta-potential value due to the charge-shielding effect by the PEG shell. When considering packaging of pDNA into polyplex micelles with respect to the aforementioned character of pDNA, several fundamental questions should rise: how the long pDNA changes its conformation within the characteristic topology and how DNA accommodates its stiffness. To these questions, transmission electron microscopic () or AFM observations revealed that pDNA undergoes a variety of packaging to form structural polymorphism [24-31] such as rod shape, doughnut-like shape (toroid), and globular shape (Figure 1.1). This is actually intriguing with respect to the driving force of the DNA condensation because globular shape is the most expected shape for minimizing the surface area. The next section deals with the subject of pDNA packaging to address this question focusing on the rod shape and globular shape.
Figure 1.1 Packaging of pDNA within polyplex micelles by PEG12k-P(Lys)70 block catiomers observed by TEM. Various shapes are observed: (a) rod shape, (b) toroid shape, and (c) globular shape.
The rod shape is the most frequently observed shape among structural polymorphism. A specific folding scheme of pDNA was found from the study based on PEG-b-poly(L-lysine) [PEG-b-P(Lys)] polyplex micelles, named "quantized folding scheme." pDNA is folded by n-times (fn) to form a rod shape consisting of 2(n?+?1) numbers of double-stranded DNA packed as a bundle in the orthogonal cross section (Figure 1.2b). Accordingly, the length is regulated to multiple of 1/[2(n?+?1)] of pDNA contour length as found in the discrete rod length distribution measured from TEM images (Figure 1.2a) [32]. This folding scheme has been observed in various polyplex micelles irrespective of the species of hydrophilic block and cationic block [30, 33] as well as the length of pDNAs; thus, it takes place independent of DNA sequences [34]. Another intriguing scheme is the relevancy with DNA rigidity; DNA is folded back at the rod ends, which is actually unacceptable assuming the persistence length of the double-stranded DNA (50 nm). However, this is made possible by local dissociation of double-stranded structure at the rod ends. The flexible nature of single-stranded DNA with persistence length of a few nanometers or less permits DNA to fold back. S1 nuclease, a single-stranded DNA-specific nuclease, could detect the occurrence of the double-stranded DNA dissociation, presenting a specific fragmentation pattern with lengths exactly corresponded to the multiples of the rod lengths [28, 32, 34].
Figure 1.2 Quantized folding scheme of pDNA to form bundled structure within polyplex micelles. (a) Rod length distribution measured from TEM images. (b) DNA is folded to bundled rod within polyplex micelles. Folded pDNA (i)-(iv) in (b) corresponds to the rod lengths in (a). (c) Double-stranded structure of DNA at the rod ends is locally dissociated to single strand for folding back.
The rod length, determined by fn of pDNA, was changed by DP in P(Lys) block. The rod length shifted to short with increasing P(Lys) DP; major fn was 1-5, 2-8, and 3-9 for polyplex micelles prepared from PEG12k-b-P(Lys) with P(Lys) DP 19, 39, and 70, respectively [35]. This P(Lys) DP dependence is mechanistically accounted based on the PEG contribution. A quantitative analysis of the PEG crowding of polyplex micelles allowed for depicting the rod shape by the balances of free energies for DNA compaction (dFcompaction,DNA?=?Gl...
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