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Department of Chemistry and Biochemistry and the Center for the Study of Early Events in Photosynthesis, Arizona State University, Tempe, Arizona 85287-1604
Correspondence: Address reprint requests to Zivile Katiliene, Fax: 480-965-2747; E-mail: zivile{at}asu.edu.
| ABSTRACT |
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65 Å, which correlates well with the distance between the ends of the dsDNA molecule when bound to NgoMIV according to the crystal structure of this complex. Formation of the looped complexes was also evident in measurements of the diffusion times of freely diffusing DNA molecules with and without NgoMIV. At very high protein concentrations compared to the DNA concentration, FRET and fluorescence correlation spectroscopy results revealed the formation of larger DNA/protein complexes. | INTRODUCTION |
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Some of the type II restriction endonucleases, such as SfiI, Cfr10I, and NgoMIV, also function by making DNA loops. These enzymes bind to two recognition sites on a double-stranded DNA (dsDNA) molecule and cleave it (Deibert et al., 2000
; Embleton et al., 2001
; Halford et al., 2000
; Nobbs and Halford, 1995
; Siksnys et al., 1999
; Watson et al., 2000
). Cleavage occurs much more rapidly when these enzymes simultaneously bind at two restriction sites instead of one; for example SfiI activity increases up to 40 times when the DNA substrate has two recognition sequences (Wentzell et al., 1995
). The binding and cleaving reaction also depends on the distance between the sites. If the restriction sites are very close (less then 30 basepairs (bp) from one another), the enzyme is unable to generate a loop in the DNA molecule due to the rigidity of the short DNA strand and this inhibits the cleavage reaction. However, if the sites are too far away, cleavage is also inhibited or prevented (Bickle and Kruger, 1993
; Siksnys et al., 1999
). The formation of dsDNA loops by SfiI and Cfr10I restriction endonucleases has been visualized by electron microscopy (Friedhoff et al., 2001
; Siksnys et al., 1999
). The DNA looping kinetics of SfiI and Cfr10I endonucleases were investigated using inhibition of the Tn21 resolvase reaction (Milsom et al., 2001
; Oram et al., 1997
). This assay is based on two competing reactions: DNA looping by restriction enzyme and recombination by Tn21 resolvase. Tn21 resolvase can complete its reaction only when the restriction enzyme-DNA complex is dissociated. It was determined that for Cfr10I the looped complexes existed as long as 90 s, whereas with the SfiI enzyme, DNA looped complexes were stable for more than 7 h (Milsom et al., 2001
).
Another type II restriction enzyme that forms DNA loops is NgoMIV. The crystal structure of NgoMIV bound to two short dsDNA fragments was solved to 1.6 Å resolution (Deibert et al., 2000
). This protein consists of four identical subunits of
32 kDa each. It simultaneously binds two copies of the DNA recognition sequence 5'-GCCGGC-3' and cleaves after the 5' G leaving a four base overhang. The protein has dimensions of 60 x 70 x 80 Å, whereas the helices of DNA molecules are separated by
55 Å from each other and have a 60° angle between their helical axes (see Fig. 1). This enzyme apparently binds to two recognition sites on the double-stranded DNA, forming a DNA loop, and then cleaves the DNA at the two recognition sites (Deibert et al., 2000
; Milsom et al., 2001
). However, the DNA looping kinetics by NgoMIV endonuclease were too fast to be resolved in bulk measurements using Tn21 resolvase inhibition (Milsom et al., 2001
).
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Here, single molecule fluorescence resonance energy transfer methodologies are applied to study the DNA/protein looped complexes as a function of the concentration of NgoMIV restriction endonuclease. FRET occurring between the donor (Cy3) and acceptor (Cy5) molecules, which are attached to the ends of a DNA fragment with appropriate binding sites, allows the measurement of the distance between the DNA ends. In this study, relative populations of different DNA/protein geometries are measured by observing NgoMIV/DNA complexes at equilibrium in solution. This work sets the stage for future studies of the dynamics of this process using immobilized DNA molecules. Such measurements should lend insight into the conformational motion of the DNA molecule caused by its interaction with NgoMIV endonuclease.
| MATERIALS AND METHODS |
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The single molecule measurements were performed in a 10-µl sample volume placed on a 0.13-mm thick glass cover slip (VWR, West Chester, PA) by detecting fluorescence from freely diffusing molecules or complexes. For these measurements, the DNA generated from the PCR reaction was diluted to 10-11 M final concentration in sterilized ultrapure water. NgoMIV restriction endonuclease concentration in the sample was varied from 0 to 3 x 10-6 M first by diluting the enzyme stock solution in the storage buffer (10 mM Tris-HCl (pH 7.3), 30 mM NaCl, 0.1 mM EDTA, 1 mM DTT, 0.5 mg/ml BSA) and then diluting 10 times by adding it to the DNA sample. These sample preparation conditions were chosen to maintain the enzyme under conditions in which no cleavage could occur (there was no magnesium in the enzyme storage buffer), while both maintaining appropriate conditions for binding and minimizing sources of fluorescent contaminants. Use of the Multi-Core buffer containing magnesium (Promega) instead, which is recommended for the optimal enzyme activity, resulted in very fast cleavage of DNA molecules even at room temperature (see below). Data were also obtained using Multi-Core buffer in which magnesium ions were chelated by EDTA. However, the addition of EDTA to the buffer resulted in increase of the background fluorescence. The ultrapure water used for the samples was deoxygenated using argon gas before each measurement to improve the photostability of the Cy3 and Cy5 molecules. A 15-bp dsDNA molecule labeled with Cy3 and Cy5 dye molecules at the 5' ends of the complimentary strands was created as a control for calibration of single molecule FRET between Cy3 and Cy5 dyes. In this 15-bp dsDNA molecule, the donor and acceptor FRET pair are expected to be 51 Å apart. This construct should show an energy transfer efficiency of 55% assuming an R0 (distance at which energy transfer is 50%) of 53 Å, as reported previously for this dye pair (Ishii et al., 1999
). For these control measurements using the 15-bp dsDNA, 50% (v/v) glycerol was added to the samples to slow the diffusion of the DNA molecules in solution.
Apparatus for single molecule detection
Excitation light at 514.5 nm from a CW argon ion laser (Lexel Lasers, Fremont, CA) was used to excite the Cy3 molecules. Single molecule fluorescence was detected using an inverted Nikon microscope (Nikon TE200) with a high numerical aperture Nikon objective (Nikon 100x, 1.4 NA, oil immersion). The fluorescence light collected by the same objective was transmitted through a dichroic mirror (part No. 525DRLP, Omega Optical, Brattleboro, VT) and focused onto a 50-µm diameter pinhole. The fluorescence was then passed through a dichroic mirror (630DRLP, Omega Optical, Brattleboro, VT) to split it into two different wavelength detection channels. Interference band pass filters centered at 570 nm and at 670 nm with 40 nm spectral bandwidths were used to spectrally select the fluorescence from Cy3 and Cy5 molecules, respectively (570 DF 40 and 670 DF 40 from Omega Optical, Brattleboro, VT). Fluorescence in each channel was detected using an avalanche photodiode (SPCM-AQ 151, EG&G, Vaudreuil, Canada). Data collection was performed with two multichannel scaler cards (MCS-plus, EG&G Ortec, Canada), one for each wavelength channel. Fluorescence from both channels was collected at the same time with an integration time of either 0.2 or 1 ms.
Fluorescence correlation spectroscopy (FCS) was used to investigate single molecule diffusion times. For this purpose, a Digital Correlator card (Correlator.com, Bridgewater, NJ) was used. Cross-correlation and autocorrelation curves from both detection channels were measured with either 30 or 60 s integration time. The errors for the diffusion time were determined by measuring and fitting the results five times.
| RESULTS AND DISCUSSION |
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corrects for the bleedthrough of Cy3 fluorescence into the Cy5 detection channel (Ha et al., 1999a
was used in all FRET efficiency calculations. For these calculations, fluorescence intensity per bin was required to have a minimum of 30 counts after summing the fluorescence from both the Cy3 and the Cy5 channels, or it was not counted. It should also be noted that in the FRET efficiency calculations, there was no background subtraction performed from either channel, as the average background was less than 1 count in each 1-ms bin. The FRET efficiency calculations also depend on any difference between the detection efficiencies of the two detector channels (Dahan et al., 1999
1. This is consistent with assumptions made in previous studies using the same or similar dyes and similar detection techniques (Dahan et al., 1999
Fig. 2 shows the distribution of FRET efficiencies for single molecule measurements using the 15-bp DNA molecule labeled on one end with Cy3 and the other end with Cy5. A primary peak with a maximum around 0.5 and small peak with a maximal efficiency of 0 is observed. The R0 for the Cy3/Cy5 pair has been determined previously to be 53 Å (Ishii et al., 1999
). Thus, using a value of 2/3 for the orientation factor
2, the 50% efficiency peak should correspond to a distance between the dye molecules of about R0 or 5055 Å. The distance between the donor and acceptor based on the DNA structure results in about a 51 Å separation of the dye molecules, in excellent agreement with the FRET results. The peak at 0% results from the fact that sometimes only Cy3 fluorescence is detected. This could not represent a situation in which the donor and acceptor were far apart because the distance between the two fluorophores is necessarily limited by the DNA structure. Instead, it is likely that there is occasionally photochemical bleaching of the Cy5 acceptor in some molecules, as previously observed in various single molecule FRET measurements (Deniz et al., 1999
; Ying et al., 2000
). In any case, the values estimated for FRET efficiency from the main distribution correspond well to what would be expected from the structure, supporting the assumptions regarding the orientation factor,
2, and the relative detection efficiencies of the two detection channels. The same calculations and assumptions were used for distance determination in the DNA/endonuclease system as well (described below).
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50% of the DNA molecules have the bound enzyme, rather than the maximum of 10% predicted by the stoichiometry. This discrepancy arises because of the way in which fluorescence bins were selected. As mentioned above, for FRET efficiency calculations only the bins with a total Cy3 plus Cy5 intensity of more that 30 counts were used. This results in the preferential selection of the FRET events over the free DNA detection events, as many of the Cy3 only bursts (corresponding to free DNA) are less than 30 counts (see burst size distributions, Fig. 5). The problems associated with the effect of burst thresholds on the ability to quantitatively compare the amounts different subpopulations in a heterogeneous mixture have been discussed previously (Dahan et al., 1999
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10%15% energy transfer efficiency can be resolved (see Fig. 3 c). This may correspond to NgoMIV/DNA complexes that are geometrically distinct from those formed at lower concentrations or could be a consequence of aggregation (discussed in more detail in terms of the structure below). At NgoMIV concentrations of 10-6 to 3 x 10-6 M the 10% efficiency population becomes dominant (Fig. 3 d). To insure that the enzyme used for these measurements was in the native, active form, cleavage of the DNA molecules by NgoMIV was also assessed. Addition of the enzyme to a DNA sample containing the reaction buffer (Multi-Core from Promega) resulted in fast disappearance (a few seconds after the addition of enzyme) of the FRET fluorescence signal and the cross-correlation between Cy3 and Cy5 detection channels. The remaining fluorescence bursts were due to the fast diffusion of the short pieces of DNA labeled with Cy3.
The NgoMIV complexes detected are the result of sequence specific interactions
When the same enzyme concentrations were added to DNA molecules that were identical to the ones described above except for several base substitutions within the restriction sites (see Methods for a detailed description), only the zero peak population in the FRET efficiency distributions was observed at any enzyme concentration (data not shown). This indicates that the appearance of the other geometrically distinct populations of complexes in the measurements (centered at 30% and 10% efficiency) is due to specific interactions between NgoMIV and DNA.
The different DNA/NgoMIV complexes detected have different diffusion times
To investigate the specific binding of NgoMIV to DNA in more detail, fluorescence correlation spectroscopy was used to measure the diffusion time (
d) of the DNA molecules or DNA/protein complexes in solution (Kettling et al., 1998
; Rippe, 2000
; Zander et al., 1996
). For these measurements, again 10-11 M DNA with or without restriction sites was investigated, and the NgoMIV concentration was also varied from 0 to 3 x 10-6 M. The FCS data was fitted to find the diffusion time
d of the molecules diffusing through the beam using the equation:
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is time,
d is diffusion time,
0/z0 is the ratio of the diameter over the z-dimension (thickness) of the confocal volume (Brand et al., 1997
0/z0 was fixed as previously determined (Daniel et al., 2002
Results from both autocorrelation (correlation within one channel) and cross-correlation (correlation between the two wavelength channels) measurements (Eigen and Rigler, 1994
) were analyzed using the same equation. The fits of the diffusion times from autocorrelation and cross-correlation data were essentially the same. Below, only the results of cross-correlation data will be presented, as they directly represent the properties of the looped DNA/protein complexes. The Cy3 and Cy5 cross-correlation results obtained at three different concentrations of NgoMIV are shown in Fig. 4. At 0 M enzyme concentration, fitting of the cross-correlation from the free DNA molecules resulted in a diffusion time of 0.29 ± 0.02 ms. It should be noted, here, that the small cross-correlation signal observed in this case represents the 15% bleedthrough of Cy3 fluorescence to the Cy5 detection channel and is essentially equivalent to an autocorrelation trace of the Cy3 channel only. Similar diffusion time values previously obtained from autocorrelation measurements of 59-bp dsDNA labeled with FAM or ROX dyes were
0.32 and 0.37 ms, respectively (Rippe, 2000
).
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Essentially the same diffusion time value is observed over a range of enzyme concentrations from 10-12 to 10-8 M. However, there is an increase in the cross-correlation amplitude with increasing enzyme concentration to 10-9 M, indicating increasing concentration of the bound DNA/protein complexes. At even higher enzyme concentrations, from 10-7 to 3 x 10-6 M, much slower diffusion times are observed, ranging from 0.6 to 1.5 ms (see Fig. 3). This increase in the diffusion time at very high concentrations of the enzyme suggests that under these conditions two NgoMIV molecules can be bound to the same DNA molecule and possibly between DNA molecules, generating large aggregates that diffuse more slowly (see below).
Burst size distribution analysis
Burst size distributions at 10-12 and 10-7 M enzyme concentrations were calculated to evaluate the average number of fluorophores (DNA molecules) per protein/DNA complex (see Fig. 5). To calculate these distributions, bins were selected from the Cy3 detection channel that had more that 10 counts per 1 ms. Adjacent bins that met this criterion where considered to be part of the same burst. The burst size was calculated as the total number of counts in a burst. The burst size distributions shown in Fig. 5 were derived from data collected over a 160-s interval. The results in Fig. 5 clearly show two main differences at low and high enzyme concentrations. First, at the 10-12 M NgoMIV concentration, the total number of qualifying bursts is significantly smaller than at 10-7 M. Also, the number of high intensity bursts is markedly smaller at the lower enzyme concentration. The burst size distribution at 10-12 M enzyme concentration is very similar to that of free DNA labeled with Cy3 (not shown) indicating that the bursts detected predominantly correspond to complexes containing a single Cy3 fluorophore rather than complexes containing multiple Cy3 molecules. This is expected because the DNA concentration is 10-11 M, 10-fold greater than the NgoMIV concentration. However, at 10-7 M enzyme concentration the number of high intensity bursts is much greater (Fig. 5), which suggests that these bursts arise from the presence of several dye molecules per complex in the focal volume. Multifluorophore particles in the focal volume give a higher probability to detect more fluorescence, which would also explain the increase of the total number of bursts. Thus, the burst size distribution at 10-7 M NgoMIV concentration also supports the hypothesis of DNA/protein aggregate formation.
Comparison of FRET distances to structural models
The results described above indicate that the addition of NgoMIV restriction endonuclease to DNA fragments containing appropriate restriction sites results in the formation of DNA/protein complexes in which FRET between the dyes at the two ends of the DNA can be detected at the single molecule level. This conclusion is supported by the observed increase in the diffusion times of DNA molecules (Fig. 4), as well as the FRET efficiency distributions (Fig. 3). The FRET results allow one to estimate the distance between the dye molecules. Gaussian fits of the FRET efficiency distributions result in a center value of 28 ± 2% (see above). If one assumes an R0 of 53 Å for the Cy3/Cy5 FRET pair (Ishii et al., 1999
) and an average value for the orientation factor
2 of 2/3, a distance of 62 ± 1 Å is obtained. The distance between DNA helices determined from the structure of DNA bound to the NgoMIV enzyme is
55 Å. The angle between DNA helices at this point is
60° (Deibert et al., 2000
) (see Figs. 1 and 6). The labeled DNA molecules were created to extend an additional 4 basepairs beyond the restriction site on either end (see Materials and Methods). The DNA molecules used in the crystal structure had a palindromic sequence, which made it impossible to predict the actual direction of the looped DNA helices (see Fig. 1). Assuming the binding occurs in such a way that the two DNA helices extend in the same direction but at an angle of 60° (this would be the configuration with the most relaxed bend in the DNA), the distance between the ends of the DNA fragment used can be calculated to be
65 Å. Though, in principle, the length of the linker between DNA bases and dye molecules could affect the distance between dye molecules attached to the ends of the DNA, the fact that the dye is attached on each end to the 5' phosphate group by a labile C3 linker should result in an average distance between the dyes that is approximately the same as the distance between the ends of the DNA. Using the same assumptions about the structure of the linker and the fluorophore position relative to the ends of the DNA, the 15-bp control DNA molecule that had Cy3 attached to one end and Cy5 to the other gave the expected distance upon analysis of its single molecule FRET emission (see above).
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At high enzyme concentrations, a new population with FRET efficiency of
10% is observed (Fig. 3, c and d). At the same enzyme concentrations, cross-correlation FCS results indicate that the diffusion time of the DNA/protein complexes increases severalfold (Fig. 4). These two effects are also accompanied by a significant increase of the amplitude of fluorescence bursts (see Fig. 5). This is consistent with the concept presented above that at high concentrations large aggregates of NgoMIV and DNA are formed with multiple fluorophores, and therefore increased amounts of fluorescence are detected (see Fig. 6 d). The presence of these large complexes (also called trans complexes) was previously proposed from the gel-shift studies of SfiI endonuclease binding to linear DNA molecules (Watson et al., 2000
). As observed with SfiI, it is likely that two NgoMIV molecules bind to the same DNA molecule at high concentrations of the enzyme (see Fig. 6, c and d). Then, in principle, the large complexes can form as the enzymes link together different DNA molecules. The formation of the large complexes is supported by the increase of diffusion times from cross-correlation measurements as well as the increase of fluorescence signal, which implies the existence of several dye molecules in a single particle passing through the probing volume (multiple DNA molecules per particle).
Taking all these facts into account, there could be several reasons for the 10%15% FRET efficiency population. One possibility is that the aggregation of protein/DNA complexes at high enzyme concentration is such that there are a mixture of geometries, with some Cy3 and Cy5 molecules in close proximity and others separated, resulting in an intermediate average FRET efficiency or even a range of efficiencies (at the highest enzyme concentrations, there seems to be a rather broad distribution of efficiencies). Alternatively, the 10% FRET efficiency population could arise from a specific DNA/protein binding geometry in these large complexes. Two different DNA strands could bind to the same enzyme molecule, but in opposing directions, similar to what has been shown for SfiI endonuclease (Halford et al., 2000
; Watson et al., 2000
) and is represented in Fig. 6, c and d. In this case, from the NgoMIV structure, the angle between the DNA ends would be 120° instead of 60°, and the distance between the DNA ends would be
75 Å, which should correspond to
10% FRET efficiency. However, it is not possible to distinguish between these possibilities from the present data.
| CONCLUSIONS |
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| ACKNOWLEDGEMENTS |
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Submitted on September 3, 2002; accepted for publication February 12, 2003.
| REFERENCES |
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Brand, L., C. Eggeling, C. Zander, K. H. Drexhage, and C. A. M. Seidel. 1997. Single-molecule indentifications of coumarin-120 by time resolved fluorescence detection: comparison of one and two photon excitation in solution. J. Phys. Chem. 101:43134321.
Dahan, M., A. A. Deniz, T. Ha, D. S. Chemla, P. G. Schultz, and S. Weiss. 1999. Ratiometric measurements and identification of single diffusing molecules. Chem. Phys. 247:85106.
Daniel, D. C., M. Thompson, and N. W. Woodbury. 2002. DNA-binding interactions and conformational fluctuations of Tc3 transposase DNA binding domain examined with single molecule fluorescence spectroscopy. Biophys. J. 82:16541666.
Deibert, M., S. Grazulis, G. Sasnauskas, V. Siksnys, and R. Huber. 2000. Structure of the tetrameric restriction endonuclease NgoMIV in complex with cleaved DNA. Nat. Struct. Biol. 7:792799.[Medline]
Deniz, A. A., M. Dahan, J. R. Grunwell, T. Ha, A. E. Faulhaber, D. S. Chemla, S. Weiss, and P. G. Schultz. 1999. Single-pair fluorescence resonance energy transfer on freely diffusing molecules: observation of Förster distance dependence and subpopulations. Proc. Natl. Acad. Sci. USA. 96:36703675.
Dietrich, A., V. Buschmann, C. Muller, and M. Sauer. 2002. Fluorescence resonance energy transfer (FRET) and competing processes in donor-acceptor substituted DNA strand: a comparative study of ensemble and single-molecule data. J. Biotechnology. 82:211231.[Medline]
Eigen, M., and R. Rigler. 1994. Sorting single molecules: application to diagnostics and evolutionary biotechnology. Proc. Natl. Acad. Sci. USA. 91:57405747.
Embleton, M. L., V. Siksnys, and S. E. Halford. 2001. DNA cleavage reactions by type II restriction enzymes that require two copies of their recognition sites. J. Mol. Biol. 311:503514.[Medline]
Friedhoff, P., R. Lurz, G. Luder, and A. Pingoud. 2001. Sau3AI, a monometric type II restriction endonuclease that dimerizes on the DNA and thereby induces DNA loops. J. Biol. Chem. 276:2358123588.
Ha, T., A. Y. Ting, J. Liang, W. B. Caldwell, A. A. Deniz, D. S. Chemla, P. G. Schultz, and S. Weiss. 1999a. Single-molecule fluorescence spectroscopy of enzyme conformational dynamics and cleavage mechanism. Proc. Natl. Acad. Sci. USA. 96:893898.
Ha, T., X. Zhuang, H. D. Kim, J. W. Orr, J. R. Williamson, and S. Chu. 1999b. Ligand-induced conformational changes observed in single RNA molecules. Proc. Natl. Acad. Sci. USA. 96:90779082.
Halford, S. E., D. M. Gowers, and R. B. Sessions. 2000. Two are better than one. Nat. Struct. Biol. 7:705707.[Medline]
Hess, S. T., S. Huang, A. A. Heikal, and W. W. Webb. 2002. Biological and chemical applications of fluorescence correlation spectroscopy: a review. Biochemistry. 41:697705.[Medline]
Ishii, Y., T. Yoshida, T. Funatsu, T. Wazawa, and T. Yanagida. 1999. Fluorescence resonance energy transfer between single fluorophores attached to a coiled-coil protein in aqueous solution. Chem. Phys. 247:163173.
Kettling, U., A. Koltermann, P. Schwille, and M. Eigen. 1998. Real-time enzyme kinetics monitored by dual-color fluorescence cross-correlation spectroscopy. Proc. Natl. Acad. Sci. USA. 95:14161420.
Kim, H. D., G. U. Nienhaus, T. Ha, J. W. Orr, J. R. Williamson, and S. Chu. 2002. Mg2+-dependent conformational change of RNA studies by fluorescence correlation and FRET on immobilized single molecules. Proc. Natl. Acad. Sci. USA. 99:42844289.
Milsom, S. E., S. E. Halford, M. L. Embleton, and M. D. Szczelkun. 2001. Analysis of DNA looping interactions by type II restriction enzyme that require two copies of their recognition sites. J. Mol. Biol. 311:515527.[Medline]
Nobbs, T. J., and S. E. Halford. 1995. DNA cleavage at two recognition sites by the Sfi I restriction endonuclease: salt dependence of cis and trans interactions between distant DNA sites. J. Mol. Biol. 252:399411.[Medline]
Norman, D. G., R. J. Grainger, D. Uhrin, and D. M. J. Lilley. 2000. Location of cyanine-3 on double stranded DNA: importance for fluorescence resonance energy transfer. Biochemistry. 39:63176324.[Medline]
Oram, M., J. F. Marko, and S. E. Halford. 1997. Communications between distant sites on supercoiled DNA from non-exponential kinetics for DNA synapsis by resolvase. J. Mol. Biol. 270:396412.[Medline]
Pace, C. N., and F. X. Schmid. 1997. How to determine the molar absorbance coefficient of a protein. In Protein Structure, a Practical Approach. T. E. Creighton, editor. IRL Press, Oxford, UK. 253259.
Rippe, K. 2000. Simultaneous binding of two DNA duplexes to NtrC-enhancer complex studied by two-color fluorescence cross-correlation spectroscopy. Biochemistry. 39:21312139.[Medline]
Schleif, R. 1992. DNA looping. Annu. Rev. Biochem. 61:199223.[Medline]
Siksnys, V., R. Skirgaila, G. Sasnauskas, C. Urbanke, D. Cherny, S. Grazulis, and R. Huber. 1999. The Cfr 10I restriction enzyme is functional as a tetramer. J. Mol. Biol. 291:11051118.[Medline]
Voet, D., and J. G. Voet. 1995. Biochemistry. Wiley & Sons, New York.
Watson, M. A., D. M. Gowers, and S. E. Halford. 2000. Alternative geometries of DNA looping: an analysis using the SfiL endonuclease. J. Mol. Bio. 289:758797.
Weiss, S. 1999. Fluorescence spectroscopy of single biomolecules. Science. 283:16761683.
Weiss, S. 2000. Measuring conformational dynamics of biomolecules by single molecule fluorescence spectroscopy. Nat. Struct. Biol. 7:724729.[Medline]
Wentzell, L. M., T. J. Nobbs, and S. E. Halford. 1995. The SfiI restriction endonuclease makes a four-strand DNA break at two copies of its recognition sequence. J. Mol. Biol. 248:581595.[Medline]
Widengren, J., E. Schweinberger, S. Berger, and C. A. M. Seidel. 2001. Two new concepts to measure fluorescence resonance energy transfer via fluorescence correlation spectroscopy: theory and experimental realizations. J. Phys. Chem. A. 105:68516866.
Ying, L., M. I. Wallace, S. Bakasubramanian, and D. Klenerman. 2000. Rotiometric analysis of single-molecule fluorescence resonance energy transfer using logical combinations of threshold criteria: a study of 12-mer DNA. J. Phys. Chem. B. 104:51715178.
Zander, C., M. Sauer, K. H. Drexhage, D. S. Ko, A. Schulz, J. Wolfrum, L. Brand, C. Eggeling, and C. A. M. Seidel. 1996. Detection and characterization of single molecules in aqueous solution. Appl. Phys. B. 63:517523.
Zhuang, X., L. E. Bartley, H. P. Babcock, R. Russell, T. Ha, D. Herschlag, and S. Chu. 2000. A single-molecule study of RNA catalysis and folding. Science. 288:20482051.
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