Nuclear proteins: finding and binding target sites in chromatin
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- van Royen, M.E., Zotter, A., Ibrahim, S.M. et al. Chromosome Res (2011) 19: 83. doi:10.1007/s10577-010-9172-5
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Fluorescent protein labelling, as well as impressive progress in live cell imaging have revolutionised the view on how essential nuclear functions like gene transcription regulation and DNA repair are organised. Here, we address questions like how DNA-interacting molecules find and bind their target sequences in the vast amount of DNA. In addition, we discuss methods that have been developed for quantitative analysis of data from fluorescence recovery after photobleaching experiments (FRAP).
Keywordsbinding models FRAP high mobility transient chromatin binding diffusion transcription DNA repair
Ataxia telangiectasia mutated (serine/threonine protein kinase)
Ataxia telangiectasia and Rad3 related
Cyan fluorescent protein
Double strand break
Excision repair cross-complementing rodent repair deficiency, complementation group 1/xeroderma pigmentosum, complementation group F
Fluorescence correlation spectroscopy
Fluorescence recovery after photobleaching
Fluorescence resonance energy transfer
Green fluorescent protein
High-mobility group protein B1
Nucleotide excision repair
Replication protein A
TATA box binding protein
Transcription factor II D/H
Xeroderma pigmentosum, complementation group A
Xeroderma pigmentosum, complementation group B
Xeroderma pigmentosum, complementation group C
Xeroderma pigmentosum, complementation group G
Yellow fluorescent protein
How do nuclear proteins find their targets?
To exert its function, a nuclear factor involved in, e.g. DNA repair, gene transcription or replication, has to find its target in the enormous amount of DNA and subsequently bind to it, either to DNA directly or to a protein-DNA-complex. The simplest model to account for this, obviously, is one where molecules move by free diffusion and find their targets by random collisions. More sophisticated models include sliding along the DNA strand (one-dimensional (1D) diffusion), along the chromatin surface (2D diffusion), as well as hopping and jumping over the DNA after initial non-specific binding. Below, we discuss these models in detail.
Diffusion and random collision
Another common idea that was challenged by live cell studies using fluorescently tagged probes is that genes may be silenced by densely packing them into heterochromatin limiting access of factors required to initiate gene transcription, as it was shown that large protein complexes (>500 kD) and dextrans with similar molecular size have free access even to the most dense chromatin domains (Verschure et al. 2003; Gorisch et al. 2003, 2005).
DNA sliding (1D diffusion)
In spite of the findings above, it is frequently argued that protein movement by merely random diffusion, whether anomalous or not, is not sufficient for finding specific target sequences in the vast amount of DNA at the required efficiency. In this line of reasoning, facilitated transport mechanisms should exist that guide a nuclear factor to its specific binding site, or at least, that enhance the chance for the freely mobile factor to find its target. The efficiency of finding specific binding sites may be increased when diffusion and stochastic binding are accompanied by local scanning mechanisms based on sliding of the protein along the DNA (one-dimensional diffusion; Fig. 1a). In more abstract terms, reducing the dimensionality of diffusion-based reactions in biological systems can greatly increase the efficiency of bimolecular interaction (Adam and Delbruck 1968). Several modes of local 1D scanning mechanisms have been experimentally tested (reviewed in Gorman and Greene 2008). In these models, after aspecific binding to DNA, a protein travels along the DNA while remaining in continuous contact with non-specific binding sites or via a series of negligible dissociation and rebinding events (Fig. 1a) (Berg et al. 1981). Most of the early data supporting such models are based on in vitro studies of DNA cleavage by endonucleases, where the length of a stretch of double-stranded DNA containing a specific cleavage site determines the rate at which cleavage occurs (Jack et al. 1982; Langowaski et al. 1983; Terry et al. 1987; Jeltsch et al. 1994, 1996; Jeltsch and Pingoud 1998; Wright et al. 1999; Stanford et al. 2000). Alternative experiments using the endonuclease BbvCI which more frequently cleaves nearby nonpalindromic recognition sites when they are in the same orientation rather than in inverted orientation indicated that the BbvCI travels from the first to the second site over short distances without dissociation and rebinding (Gowers et al. 2005). In addition to endonucleases, several other DNA-binding proteins have been shown to display 1D diffusion along DNA, using single-molecule detection techniques (Shimamoto 1999; Gorman and Greene 2008). These include DNA repair proteins like Rad51 involved in homologous recombination, oxoguanine glycosylase involved in base-excision repair and post-replicative mismatch repair proteins (Msh2–Msh6), but also transcription factors like RNA polymerase (RNAP), T7 RNAP and the lac repressor (LacI), that show facilitated diffusion along anchored DNA stretches interspersed with three-dimensional translocations (Kabata et al. 1993; Harada et al. 1999; Blainey et al. 2006; Graneli et al. 2006; Wang et al. 2006; Gorman et al. 2007). Assuming that protein sliding is mainly driven by electrostatic interactions with the phosphate backbone, it has been suggested that sliding involves spiralling around the DNA helix (Fig. 1a; Schurr 1975; Gorman and Greene 2008). This was indirectly shown as rotational behaviour of a DNA stretch linked to an asymmetrically labelled bead when dragged over an RNA polymerase-coated coverslip using an optical trap (Sakata-Sogawa and Shimamoto 2004). More recently, statistical analysis of single-molecule diffusion data of eight DNA-binding proteins showed that rotation-coupled sliding along the DNA helix is a general phenomenon in vitro (Blainey et al. 2009).
However, although it seems clear that many DNA-binding proteins in vitro are able to slide along DNA, studies on living cells to determine to what extent this behaviour contributes to reaction efficiency in vivo are still limited. One interesting study on protein behaviour in living Escherichia coli cells using the lac repressor LacI suggests that one-dimensional diffusion along DNA segments occurs, but in combination with three-dimensional translocation through the cytoplasm (Elf et al. 2007). The most obvious difficulty that may arise in DNA sliding models is the presence of hundreds or thousands of different DNA-binding molecules, each present in tens of thousands of copies, which may considerably hinder each other when moving along the one lane road of DNA. This is a lesser problem in a hypothesised two-dimensional sliding mechanism, where the protein diffuses over the DNA surface, enabling the restriction endonuclease EcoRI to bypass obstacles in vitro (Fig. 1b; Kampmann 2004). In addition, the lack of directionality in one-dimensional diffusion may also lower the probability of reaching distant sites, limiting the efficiency of detecting specific binding sites (Gerland et al. 2002).
Hopping, jumping and intersegmental transfer
In addition to these sliding mechanisms, it has also been hypothesised that proteins may bind repeatedly in the same region in an aspecific manner and only freely diffuse shortly through nuclear space before rebinding at another (specific or non-specific) binding site, in this way, enhancing their chances to find their target sites. These short 3-D diffusion events include short intrasegmental hops along the DNA contour, intersegmental jumps between nearby segments and translocations over longer distances in three-dimensional space (Fig. 1c). Because of the larger probability of binding to nearby sites relative to distant sites, in solution the protein will more frequently bind to sites on the same strand of DNA (Halford and Marko 2004). This model is supported by the decreased association time when the DNA conformation is changed from a coiled structure to extended DNA using optical tweezers (van den Broek et al. 2008). It was determined that cDNA coiling leads to a more efficient search rate for specific binding sites (Fig. 1d; Lomholt et al. 2009). Whether this holds true for chromatin binding in the nucleus depends on the relative proximity of functional elements in different stands of DNA in higher order chromatin organisation. A third alternative is so-called intersegmental transfer (as opposed to intersegmental jumps), which may occur when proteins are capable of binding two sites (Fig. 1d). In this model a protein binds a site distant from its target, and before dissociating binds to another site that is brought into proximity by looping of DNA, thereby generating an intermediate in which the protein is transiently bound to both sites. Because of limited DNA flexibility, intersegmental transfer is restricted to larger steps (≈400 bp) (Bellomy and Record 1990).
Before we move on to discussing the way nuclear proteins bind their targets once they found them, we summarise below recent developments in quantitative analysis of fluorescence recovery after photobleaching. FRAP is widely used, not only to determine the mobility of fluorescently tagged proteins, but also the kinetics of interactions with immobile structures. In other words, with FRAP, we can quantitatively assess on- and off-rates from and to DNA or DNA complexes.
FRAP makes use of the fact that fluorescent molecules can be photobleached, i.e. they can be made irreversibly non-fluorescent by illuminating them at high excitation intensity. After selectively photobleaching a small volume within a larger volume, for instance within a living cell nucleus, the recovery of fluorescence due to movement (for instance by diffusion) of unbleached mobile molecules from outside the bleached region moving into the region is followed at regular time intervals. The extent to and rate at which this happens represent the fractions of mobile and immobile molecules and the speed at which they move. Since the precise quantitative analysis of the resulting FRAP curves is difficult, as discussed below, FRAP is especially powerful if the system under surveillance can be studied in an active and passive state, so that a difference in mobility can be attributed to protein function. For instance, in DNA repair, one can compare protein mobilities in unchallenged cells with those in cells that were exposed to a DNA damage-inducing agent. In transcriptional regulatory systems, like the nuclear hormone receptors, one can compare mobilities of ligand-induced and inactive receptors such as either non-liganded receptors, receptors inhibited by antagonistic ligands or receptor mutants lacking DNA-binding properties (Farla et al. 2005). Such comparative studies can be based on qualitative analysis, i.e., visual inspection of the curves, or semi-quantitative analysis, by calculating the half life of fluorescence recovery. In addition, a permanently immobilised fraction can be readily estimated from the incomplete recovery of fluorescence. Although this straightforward approach is by itself useful, as can be seen from the wealth of mechanistic insight that has been gained from many studies, half-lives (which are frequently reported) only provide information on overall mobility but do not allow detailed quantitative analysis. For example, when relatively small fractions of proteins are engaged in immobilising DNA-binding events, half-life will be only slightly increased compared to fully free protein. Therefore, half-life is not easily translated into quantitative estimates of bound fractions or residence times in immobile DNA–protein complexes.
To obtain more quantitative information from FRAP analysis, sophisticated analytical models have been established. The parameters that one aims to quantitatively assess are effective on- and off-rates to and from immobile DNA–protein complexes, which can be used to calculate the bound fraction and residence time in the complex, parameters that are usually reported. When on-rates increase at constant off-rate, the immobile fraction also increases. When off-rates increase, the immobile fraction becomes smaller at constant on-rate, and, in addition, the residence time becomes shorter. Apart from the parameters to be extracted from the FRAP curve, mathematical or numerical models essentially include a number of fixed parameters representing both microscopic properties, like shape, size and intensity profile of the laser beam focused by the objective lens, as well as properties of the nucleus like shape and size and the intranuclear distribution of the factors under surveillance. Most of these can be obtained experimentally in control measurements. However, incorporating them in mathematical models requires skilled mathematicians (Mueller et al. 2010). In the development of these models, therefore a number of simplifications have been applied. Initially it was frequently assumed that diffusion is in general so fast that it can be neglected in the FRAP model. The simplified models assumed reaction-dominant or diffusion-uncoupled FRAP recovery, where curves can be separated in an extremely short diffusive phase, essentially taking less than a second, and a much longer binding phase over a period of seconds to minutes (Sprague et al. 2004; Sprague and McNally 2005; Beaudouin et al. 2006). However, it was recently suggested that diffusion may also contribute to very slow FRAP recoveries, as long as the time to associate with a binding site is fast compared to diffusion (Mueller et al. 2008, 2010). If in these cases diffusion is neglected this may lead to the false prediction of an additional short-lived binding state. A proper procedure to verify whether FRAP recovery curves are diffusion coupled or uncoupled is by applying bleach pulse areas with increasing size. When diffusion is relatively fast, recovery is hardly affected by the size of the bleach area (Phair et al. 2004; Sprague et al. 2004).
In order to simplify mathematical models, the photobleached region is sometimes modelled as a cylindrical uniform profile (Carrero et al. 2003), or a cylindrical region with a radial Gaussian distribution (Braeckmans et al. 2003; Kang and Kenworthy 2008; Tsibidis and Ripoll 2008; Tsibidis 2009). However, although a cylindrical profile is justified when a low numerical aperature (NA) lens is used, a double-cone profile may be more accurate, even for low NA lenses (Braeckmans et al. 2007; van Royen et al. 2009; Hallen and Layton 2010). Furthermore, unlike a cylindrical bleaching profile, the double-cone profile also implies a significant dependency of the three dimensional situation, because of the axial Gaussian distribution of the laser beam (Mazza et al. 2007, 2008; Hallen and Layton 2010). These and other fixed parameters, like photophysical properties of the fluorophores in use (e.g. blinking and reversible photo-bleaching), and also experimental settings like the duration of bleaching and the consequences for diffusion during bleaching should be carefully considered in the development of a kinetic model (Braga et al. 2004; Mueller et al. 2008, 2010; Kang et al. 2009). Another complication in the development of mathematical models is a heterogeneous distribution of target sites of the labelled proteins. Most models assume a homogeneous distribution of binding sites, ignoring the typical spatial organisation of nuclear processes like gene transcription or DNA replication (Kang and Kenworthy 2008; Mueller et al. 2008). A more accurate binding model would then be one which takes the actual inhomogeneous distribution of binding sites into account by using the acquired imaging data (Beaudouin et al. 2006).
Although with the right interpretation, FRAP data are very informative about the mobility of fluorescently labelled proteins, it clearly has its limitations. The integration of complementary techniques like single-molecule tracking (SMT) and fluorescence correlation spectroscopy will be of great value in unravelling the full picture of the dynamic behaviour of proteins. These approaches will be discussed elsewhere in this issue (Erdel et al. 2011; Dange et al. 2011).
How do nuclear proteins bind their targets?
While the above studies clearly show the dynamic interplay between DNA-binding proteins and chromatin in general, there are still a number of questions that remain to be discussed for individual proteins: Do proteins associate with target DNA or DNA–protein complexes until, for instance, repair is completed or transcription is initiated, or do they stay shorter, only to perform their own specific task within the entire process? Do unproductive binding events also occur, and if yes how often? In addition, is there a specific or preferred order in which factors assemble? Below we discuss these issues in detail.
Results from FRAP-studies on single-strand DNA-damage by nucleotide excision repair (NER) point to an action mechanism where repair factors are present in DNA–protein complexes for the time required to repair a single lesion, and leave the spot soon after. First, all investigated NER constituents, including ERCC1/XPF (Houtsmuller et al. 1999), XPB (Hoogstraten et al. 2002), XPA (Rademakers et al. 2003), XPC (Hoogstraten et al. 2008; Nishi et al. 2009) and XPG (Zotter et al. 2006) have similar and relatively long fluorescence recovery times in the order of 3 to 5 min, and show similar immobile fractions, dependent on the number of lesions present. Second, the time it takes to fully repair all single-strand lesions induced by UV-irradiation at 8 J/m2 predicted on the basis these FRAP measurements is in agreement with the total repair time determined by incorporation of labelled nucleotides at different time points after damage induction (Houtsmuller et al. 1999). A different picture arises from studies on double-strand break repair (DSB) dynamics, where residence times of individual factors in DSB foci differ considerably from each other (e.g. RAD54, ~3 s; RAD52, ~5 min; and RAD51, stably bound, see Fig. 3a), and are mostly much shorter than the life span of individual DSB foci, which is in the order of several hours. An interesting, but highly speculative explanation for the observed very rapid interactions of RAD54 is related to its ability to hydrolyse ATP in a DSB-dependent manner (Swagemakers et al. 1998). If its main activity in DSB foci would be hydrolysing ATP, it may be that during each short-term visit RAD54 delivers a small amount of energy by hydrolysing a few ATPs, thereby fuelling the ongoing repair process. In contrast, RAD51, which is very stably associated to DSB foci, may have a scaffolding function. Thus, opposite to the situation in NER, in DSB repair, individual factors do not reside in a DSB focus during its entire life span, but in general have shorter residence times, which may correspond to the time required to perform specific actions within the entire repair process. In transcription, the situation is probably more complex, where different models may explain consecutive steps, from initial binding by regulatory factors such as steroid receptors and cofactors, which may act similarly to NER factors (see also below), followed by assembly of the general transcription machinery and finalised by launching of RNA polymerase II. The general transcription complex may behave more similarly to the DSB repair system, in a sense that residence times differ considerably between individual factors, where the TATA-box-binding protein TBP as a part of TFIID shows relatively long residence times, in the order of tens of minutes (de Graaf et al. 2010), whereas residence times of TFIIH are in the order of several seconds rather than minutes (Hoogstraten et al. 2002). A speculative explanation of the long-term binding of TBP, may be in the observation that its residence times are influenced by the presence or absence of coactivators or repressors, where the latter increase its binding times, suggesting a regulatory role for TBP in addition to its function in initiation (de Graaf et al. 2010). The very rapid interactions of TFIIH in transcription are in contrast with its behaviour in single-strand damage repair, where it is engaged in repair complexes for minutes (Hoogstraten et al. 2002). Interestingly, not only TFIIH, but repair factors in general seem to be more stably associated with repair complexes than transcription factors are with transcription initiation complexes (Fig. 3a). An attractive explanation for this could be that DNA damage demands urgent removal, and is stably bound by repair complexes, whereas transcription (regulation) is an ongoing process, possibly requiring less tight attention. In other words, repair factors better do their job properly, whereas transcription factors may miss a round or two.
Next to these speculative considerations, it should be noted also that it is highly likely, given the increasingly recognised stochastic nature of all molecular behaviour in the cell, that not all observed binding events are actually productive. Very transient interactions in the subsecond range have been reported to occur on a large scale, together with longer binding events. For instance in DNA replication and in AR-regulated transcription, experimental FRAP curves fit best to curves generated by Monte Carlo computer simulations of a scenario where in addition to relatively long binding events, the majority of the proteins are binding transiently to DNA (Xouri et al. 2007; Tanner et al. 2010). These interactions may also contribute to the observed anomalous diffusion discussed above and may represent aspecific binding events, possibly leading to sliding along DNA.
FRAP has been instrumental in determining residence times in DNA–protein complexes, but other approaches have been explored to address the question whether individual factors bind in a preferred or specific order to the complexes in progress. Obviously, factors that identify targets in chromatin, like transcription regulatory factors or DNA damage sensors are early binders, but less knowledge exists on the order, if any, in which the subsequent activities bind (Dinant et al. 2009; Coulon et al. 2010). In DNA repair of single-strand lesions it was shown that in patient or mutant cell lines, each lacking a specific factor, only a subset of the other repair proteins would assemble on a locally induced damage spot within the nucleus. These data suggest a defined order of binding, where the single-strand lesion is first detected then stabilised, unwound, cut out and resynthesised. Along the same lines, but exploring an alternative approach where they used ionising irradiation of a limited volume in the nucleus, and followed the assembly of several GFP-tagged DSB repair-proteins, ample evidence has been provided that these factors assemble in a specific order (Jazayeri et al. 2006; Essers et al. 2006). After IR-induced DNA damage, activated ATM binds Chk2 very transiently resulting in activation and Chk2-mediated cell cycle arrest (Lukas et al. 2003, 2004). This very transient binding is contrasted by the binding of the Mre11-Rad50-Nbs1 complex (MRN) at the damage site, which is followed by consecutive binding of RPA, ATR, Chk1 and the RAD52-group proteins and others (Jazayeri et al. 2006). During the existence of the holocomplex, the involved factors dynamically exchange between the complex and the nucleoplasm, each factor having its own average residence time (Essers et al. 2005).
In an experimentally different set-up, chromatin immunoprecipitation (ChIP) experiments on cultured synchronised cells suggest a cyclic binding pattern in hormone-regulated transcription, where estrogen receptors (ERs), cofactors and finally the general transcription machinery bind in a more or less defined order, and release soon after transcription initiation, leaving the gene for a new round of binding (Metivier et al. 2003). Since the observed cycles were typically in the order of tens of minutes these data initiated discussion on the interpretation of many of the preceding FRAP experiments on nuclear receptors which suggested a much shorter binding time in the order of tens of seconds rather than minutes (e.g. McNally et al. 2000; Farla et al. 2004, 2005; Schaaf and Cidlowski 2003; Rayasam et al. 2005; Marcelli et al. 2006; Klokk et al. 2007; Meijsing et al. 2007). However, an explanation for the apparent inconsistency of ChIP and FRAP data was provided by McNally and co-workers who showed, combining FRAP and single-cell measurements of messenger RNA, that rapid exchange of the yeast copper-inducible transcription factor ACE1p with each copy of an array of endogenous CUP1 promoters occurs, but that the number of available binding sites in the array goes through cycles on a longer time scale in the order of tens of minutes (Karpova et al. 2008). This indicates that during the existence of a productive complex, individual components may continually exchange, similar to RAD54 in DSB repair. Indeed, such exchange has been observed for histones, of which the exchange is increased in transcriptionally active areas, but also occurs in other areas (Kimura et al. 2002).
The combination of acceptor photobleaching FRET and FRAP has provided an alternative approach to investigate binding order. In this method, the increase and the subsequent loss of fluorescence of FRET-donor fluorescence in a small region inside the nucleus after photobleaching the FRET-acceptor, is compared with the recovery of FRET-acceptor fluorescence (van Royen et al. 2007). Application of this approach to androgen receptors double tagged with the FRET-pair CFP and YFP at the N and C terminuses, revealed that androgen receptors undergo a transformational change after binding to regulatory regions of androgen-regulated genes, and that this change uncovers binding sites for cofactors allowing them to bind to the same regions only after ARs have bound.
Apart from binding in a specific order, it has also been shown that different factors influence, i.e. stimulate or inhibit, each others binding behaviour. For example, the glucocorticoid receptor and high-mobility group box protein 1 interact when bound to chromatin and decrease each others' mobility (Agresti et al. 2005), suggesting a cooperative binding mechanism. Another example of cooperative binding behaviour is provided by detailed analysis of the dynamic behaviour of linker histone H1. Sophisticated FRAP analysis of various GFP-tagged truncated H1 variants each harbouring defined DNA-binding domains revealed two distinct binding mechanisms through different combinations of domains and an additional metastable intermediate binding state (Stasevich et al. 2010). These types of cooperative binding reactions cannot be described by a simple binding reaction model, but require a model of sequential binding events or even more complex models that includes initial complex formation (cf. Fig. 4) (Mueller et al. 2010). Most likely these complex binding events will lead to more variability in its binding kinetics and in particular a varying off-rate.
We have discussed models and supportive data concerning mechanisms by which nuclear proteins translocate to their target sites, and how they interact with DNA or DNA–protein complexes. Taking together the results of various approaches, the predominant mechanism by which proteins travel through the nucleus to find their target sites is one of three-dimensional diffusion. It is however, not yet clear how nuclear factors find the precise nucleotide sequence or DNA damage in the vast amount of DNA. It has been argued that DNA-scanning mechanisms should exist (1D diffusion), enhancing the chance to encounter a target site (Fig. 1a). Indeed it can be calculated that a specific molecule that effectively diffuses at a typical rate of say 1 μm2/s in a (large) nucleus with a diameter of say 30 μm, will collide with for instance a nucleosome with a diameter of 10 nm only once a day. In contrast to this, it can also be argued that, from the viewpoint of a specific binding site awaiting a factor to bind, it is not relevant which of the often thousands or tens of thousands of copies actually binds, which will happen several times per minute. In addition, many nuclear proteins that do not bind DNA directly, may not have intrinsic DNA-binding properties, and may not be able to explore DNA-scanning mechanisms to enhance their binding chances. However, since the investigated endonuclease and other DNA-binding proteins are clearly able to slide along DNA in vitro, it seems likely that at least short stretches of DNA are scanned continually by DNA-interacting factors in vivo, enhancing their binding efficiency. Sliding mechanisms in that view can then be regarded as binding mechanisms rather than finding mechanisms, similar to protein–protein interactions that often start with weak interactions, after which strong interactions are initiated by reorientation of the binding partners. As an alternative to 1D-diffusion, hopping or jumping models have been suggested. However, these hopping events (Fig. 1c) also occur frequently in a model of free diffusion and random collision. It may be that the recently reported fractal organisation of chromatin facilitates hopping behaviour (Bancaud et al. 2009; Lieberman-Aiden et al. 2009). However, further investigation is required to verify whether binding and rebinding of factors for instance in chromatin areas rich in binding sites occurs more frequently than expected on the basis of free diffusion.
In Fig. 3 we provided a semi-quantitative comparison of nuclear proteins involved in several nuclear processes, which allows to make general statements about the large scale differences between residence times of different factors in DNA–protein complexes. Although our interpretations are highly speculative and require much more research, we discussed the possible relationship between the observed residence times and protein function. Moreover, apart from the fact that data are compared from different labs using different FRAP approaches and analytical methods, which we tried to overcome by showing final recovery times (Fig. 3a), the influence of the GFP-tag on a labelled protein may limit to some extent the validity of our comparison. Although GFP-tagged proteins are in general thoroughly tested to be functional in spite of the bulky tag, it would be overly optimistic to assume that there is no influence. Since the potentially limiting effect on function is likely to differ between different proteins, caution is required, especially when precise quantitative data are integrated in systems biology approaches to present a full quantitative model.
Finally, quantitative fluorescence methods, specifically FRAP, and other approaches have revealed a highly dynamic behaviour of nuclear proteins, but to fully unravel the reaction mechanisms by which DNA–protein complexes perform their functions, more research and the application of novel approaches are required. In the field of fluorescence, single-molecule tracking and high-resolution microscopy technology are expected to play an important role in this further research.