The Fluorescence of native DNA at room temperature

Compact Color Biofinder (CoCoBi): Fast, Standoff, Sensitive Detection of Biomolecules and Polyaromatic Hydrocarbons for the Detection of Life

We have developed a compact instrument called the "COmpact COlor BIofinder", or CoCoBi, for the standoff detection of biological materials and organics with polyaromatic hydrocarbons (PAHs) using a nondestructive approach in a wide area. The CoCoBi system uses a compact solid state, conductively cooled neodymium-doped yttrium aluminum garnet (Nd:YAG) nanosecond pulsed laser capable of simultaneously providing two excitation wavelengths, 355 and 532 nm, and a compact, sensitive-gated color complementary metal-oxide-semiconductor camera detector. The system is compact, portable, and determines the location of biological materials and organics with PAHs in an area 1590 cm2 wide, from a target distance of 3 m through live video using fast fluorescence signals. The CoCoBi system is highly sensitive and capable of detecting a PAH concentration below 1 part per billion from a distance of 1 m. The color images provide the simultaneous detection of various objects in the target area using shades of color and morphological features. We demonstrate that this unique feature successfully detected the biological remains present in a 150-million-year-old fossil buried in a fluorescent clay matrix. The CoCoBi was also successfully field-tested in Hawaiian ocean water during daylight hours for the detection of natural biological materials present in the ocean. The wide-area and video-speed imaging capabilities of CoCoBi for biodetection may be highly useful in future NASA rover-lander life detection missions.

OrganiCam: a lightweight time-resolved laser-induced luminescence imager and Raman spectrometer for planetary organic material characterization

OrganiCam is a laser-induced luminescence imager and spectrometer designed for standoff organic and biosignature detection on planetary bodies. OrganiCam uses a diffused laser beam (12° cone) to cover a large area at several meters distance and records luminescence on half of its intensified detector. The diffuser can be removed to record Raman and fluorescence spectra from a small spot from 2 m standoff distance. OrganiCam's small size and light weight makes it ideal for surveying organics on planetary surfaces. We have designed and built a brassboard version of the OrganiCam instrument and performed initial tests of the system.

Construction of a DNA-Based Supramolecular Nanosheet That Emits Bluish-White Light from Charge-Transfer Excited States of the Nucleobases

1,ω-Inosinic acid-bearing bolaamphiphiles dI(18), dI(19), and dI(20) with a 3'-phosphorylated inosine as a universal base connected to each end of an oligomethylene chain were synthesized for the first time. Single-component self-assemblies of these bolaamphiphiles and their binary self-assemblies with salmon sperm DNA were studied by AFM; temperature-dependent UV absorption, fluorescence, and circular dichroism spectroscopy; and gel electrophoresis. The binary self-assembly of dI(20) and salmon sperm DNA (dI(20)-DNA) had a nanosheet structure with a homogeneous thickness of about 6 nm and widths of several micrometers. Interestingly, an aqueous solution of the nanosheets showed a broad absorption band originating from the charge-transfer (CT) states of the nucleobase in the long-wavelength region (>300 nm), and the molar absorptivity per nucleobase was calculated to be approximately 150 times that of single-stranded (dT20 and dA20) and double-stranded (dT20-dA20) oligonucleotides. In addition, a continuous and broad emission band originating from CT excited states of the nucleobases was observed in the visible region. These observations indicate that CT states of the nucleobases were formed and stabilized in the supramolecular nanosheet and that bluish white light was emitted from CT excited states of the nucleobases.

"Standoff Biofinder" for Fast, Noncontact, Nondestructive, Large-Area Detection of Biological Materials for Planetary Exploration

We developed a prototype instrument called the Standoff Biofinder, which can quickly locate biological material in a 500 cm(2) area from a 2 m standoff distance with a detection time of 0.1 s. All biogenic materials give strong fluorescence signals when excited with UV and visible lasers. In addition, the luminescence decay time of biogenic compounds is much shorter (<100 ns) than the micro- to millisecond decay time of transition metal ions and rare-earth ions in minerals and rocks. The Standoff Biofinder takes advantage of the short lifetime of biofluorescent materials to obtain real-time fluorescence images that show the locations of biological materials among luminescent minerals in a geological context. The Standoff Biofinder instrument will be useful for locating biological material during future NASA rover, lander, and crewed missions. Additionally, the instrument can be used for nondestructive detection of biological materials in unique samples, such as those obtained by sample return missions from the outer planets and asteroids. The Standoff Biofinder also has the capacity to detect microbes and bacteria on space instruments for planetary protection purposes.

KEY WORDS

Standoff Biofinder-Luminescence-Time-resolved fluorescence-Biofluorescence-Planetary exploration-Planetary protection-Noncontact nondestructive biodetection. Astrobiology 16, 715-729.

Competitive Assays of Label-Free DNA Hybridization with Single-Molecule Fluorescence Imaging Detection

Single-molecule imaging of fluorescently labeled biomolecules is a powerful technique for measuring association interactions; however, care must be taken to ensure that the fluorescent labels do not influence the system being probed. Label-free techniques are needed to understand biomolecule interactions free from the influence of an attached label, but these techniques often lack sensitivity and specificity. To solve these challenges, we have developed a competitive assay that uses single-molecule detection to track the population of unlabeled target single-stranded DNA (ssDNA) hybridized with probe DNA immobilized at a glass interface by detecting individual duplexes with a fluorescently labeled "tracer" ssDNA. By labeling a small fraction (<0.2%) of target molecules, the "tracer" DNA tracks the available probe DNA sites without significant competition with the unlabeled target population. Single-molecule fluorescence imaging is a good read-out scheme for competitive assays, as it is sufficiently sensitive to detect tracer DNA on substrates with relatively low densities of probe DNA, ∼10(-3) of a monolayer, so that steric interactions do not hinder DNA hybridization. Competitive assays are used to measure the association constant of complementary strand DNA hybridization of 9- and 10-base pair targets, where the tracer assay predicts the same association constant as a traditional displacement competitive assay. This methodology was used to compare the Ka of hybridization for identical DNA strands differing only by the presence of a fluorescent label tethered to the 5' end of the solution-phase target. The addition of the fluorescent label significantly stabilizes the DNA duplex by 3.6 kJmol(-1), adding more stability than an additional adenine-thymine base-pairing interaction, 2.7 kJmol(-1). This competitive tracer assay could be used to screen a number of labeled and unlabeled target DNA strands to measure the impact of fluorescent labeling on duplex stability. This single-molecule competitive hybridization scheme could be easily adapted into a sensitive assay, where competition between tracer and target oligonucleotides for probe sites could be used to measure concentrations of unlabeled DNA or RNA.

Sequence, structure and energy transfer in DNA

Excitation energy transfer in DNA has similarities to charge transfer, but the transport is of an excited state, not of mass or charge. Use of the fluorescent, modified adenine base 2-aminopurine (2AP) as an energy trap in short (3- to 20-base) single- and double-stranded DNA oligomers is reviewed. Variation of 2AP's neighboring sequence shows (1) relatively efficient transfer from adenine compared to that from cytosine and thymine, (2) efficient transfer from guanine, but only when 2AP is at the 3' end, (3) approximate equality of efficiencies for 3' to 5' and 5' to 3' directional transfer in adenine tracks. The overall, average transfer distance at room temperature is about four adenine bases or less before de-excitation. The transfer fluorescence excitation spectral shape is similar to that of the absorption spectrum of the neighboring normal bases, confirming that initial excitation of the normal bases, followed by emission from 2AP (i.e. energy transfer), is occurring. Transfer apparently may take place both along one strand and cross-strand, depending on the oligomer sequence. Efficiency increases when the temperature is decreased, rising above 50% (overall efficiency) in decamers of adenine below -60 degrees C (frozen media). Modeling of the efficiencies of transfer from the nearest several adenine neighbors of 2AP in these oligomers suggests that the nearest two neighbors transfer with near 100% efficiency. As bases in B DNA, as well as in single-stranded DNA, are separated by less than 5 A (less than the size of a base), standard Förster transfer theory should not apply. Indeed, while both theory and experiment show efficiency decreasing with donor-acceptor distance, the experimental dependence clearly disagrees with Förster 1/r6 dependence. It is not yet clear what the best theoretical approach is, but any calculation must deal accurately with the excited states of bases, including strong base-base interactions and structural fluctuations, and should reflect the increase of efficiency with temperature decrease and the relative insensitivity to strandedness (single, double). Attempts to use DNA as a molecular "fiber optic" face three primary challenges. First, reasonable efficiency over more than a base or two occurs only in adenine stretches at temperatures well below freezing. Second, transfer in these adenine tracks is efficient in both directions. Third, absorption of UV light occurs randomly, making excitation at a specific site on this "fiber optic" a challenge.

Intrinsic fluorescence of B and Z forms of poly d(G-m5C)·poly d(G-m5C), a synthetic double-stranded DNA: spectra and lifetimes by the maximum entropy method

A study has been made of the fluorescence of poly d(G-m5C).poly d(G-m5C), a synthetic double-stranded DNA, in buffered neutral aqueous solution at room temperature, excited by synchrotron radiation at 280 nm and 250 nm and by a frequency-doubled pulse dye laser at 290 nm. Exciting at 280 nm, the B form shows a uni-modal UV spectrum with lambdaf(max) approximately 340 nm. The Z form has in addition a visible emission lambdaf(max) at 450 nm. The spectral positions remain unchanged on exciting at 250 nm but the relative intensities change considerably. Decay profiles have been obtained at 360 nm and 450 nm for both the B and Z forms and have been analyzed by fitting to a pseudo-continuous distribution of 100 (and occasionally 200) exponentials, ranging from 10 ps to 20 ns, by optimizing the 'entropy' of the signal (the method of maximum entropy). We find the mean lifetimes for both wavelengths of emission and for both structural forms fall into three well-separated regions in the ranges indicated tau1 approximately 0.04-0.21 ns, tau2 approximately 0.9-1.26 ns, and tau3 approximately 5.1-6.5 ns. The UV emission, from its spectral position and half-width, correlates with monomeric emission from m5C (and from C for poly d(G-C)). However the lifetime tau1 is approximately 2 orders of magnitude longer than the monomers and points to an involvement of protonated guanosine (GH+, tauf approximately 200 ps) in the overall absorption/emission sequence. In the UV the tau3 emission is predominant, with fractional time-integrated emission approximately 86% for B DNA and approximately 64% for Z. We suggest it results from exciton (stacked) absorption followed by dissociative emission. For Z DNA the visible (450 nm) emission is dominated by a tau3 species (approximately 91%) with a lifetime of 6.5 ns and we suggest it represents a hetero-excimer emission consequent upon absorption by the strongly overlapped base-stacking, which differs from that in B DNA. The weak emission corresponding to tau2 is made more apparent by scanned gated detection of the emission from laser excitation (290 nm) of single-crystal d(m5C-G)3. A central role is attributed to the tight stacking of the bases in the Z form which correlates with enhanced hypochromism at 250 nm vs. 280 nm and with the reversal of the fluorescence intensity ratios UV-visible between these wavelengths.

Room-temperature steady-state fluorescence properties of poly(dG-dC).poly(dG-dC)

We report the steady-state fluorescence properties of the alternating polynucleotide poly(dG-dC).poly(dG-dC) in low-salt solution at room temperature for excitation at the Hg lines 265, 280 and 297 nm. Its fluorescence spectrum peaks at about 325 nm and, within the experimental error, its shape does not change significantly with the excitation wavelength. The fluorescence anisotropy is found to decrease strongly for short-wavelength excitation, a behavior which is very similar to that exhibited by free guanine. In view of the fact that the anisotropy for free cytosine is virtually constant at the aforementioned three excitation wavelengths, the results suggest that in this polynucleotide the emission stems from guanine. The values of the fluorescence quantum yield for the three excitation wavelengths are found to be very low, 0.8 x 10(-5), 0.8 x 10(-5), and 2.8 x 10(-5), respectively; these are compatible with transfer of energy from the lower-energy electronic state of guanine, before vibronic relaxation is established, to cytosine. Upon denaturation, the fluorescence spectrum becomes very broad and the fluorescence quantum yield increases; these observations support the authenticity of the emission from the nondenatured polynucleotide.

Room-temperature fluorescence properties of the polynucleotide polydA.polydT

The room-temperature fluorescence spectrum of the non-alternating polynucleotide polydA.polydT is found to have its maximum at about 325 nm and, when exciting in the spectral region where both adenine (A) and thymine (T) absorb, to coincide with that obtained for excitation at 293 nm where thymine is selectively excited. The fluorescence anisotropy is found to be equal to 0.18 and independent of the excitation and emission wavelengths. These observations are consistent with: (i) emission stemming from T; and (ii) transfer of electronic energy from A to T being not efficient. These inferences are also supported by the observed dependence of the fluorescence quantum yield on the excitation wavelength.

Singlet-singlet energy transfer along the helix of a double-stranded nucleic acid at room temperature

An irreversible electronic energy trap has been formed in calf thymus DNA by methylating about 75% of its G bases at position N-7. This has allowed us to measure for the first time the efficiency of transfer of energy along the helix of a double-stranded nucleic acid at room temperature. It is found that about one out of every three photons absorbed by the other bases is trapped. We have also simulated the data with a stochastic model that uses the dipole-dipole interaction to calculate the efficiency of transfer. In order to approximate the experimental results, the model requires that: (i) the fluorescence quantum yield of T, C, and G in DNA be about 2 x 10(-3), which is about two orders of magnitude larger than the value of the fluorescence quantum yield reported for DNA; and (ii) the fluorescence quantum yield of A in DNA be negligibly small. Requirement (i) is consistent with energy transfer taking place before a very efficient fluorescence quenching process sets in, which could be formation of excited-state complexes (excimers) that do not fluoresce appreciably. Requirement (ii) implies a very short fluorescence lifetime for A, which is consistent with the reported absence of a significant number of photoproducts formed by A in DNA. The simulations find that, on the average, the excitation energy takes about 1.2 steps to reach the trap; that is to say, bases that are nearest and next nearest neighbors of the trap are, in effect, the only energy donors. Both intra- as well as interstrand energy transfer (the latter only for the C-trap base pair) make significant contributions. The value of the efficiency for pairwise base-base intrastrand transfer is about 60%, whereas those for base-trap intra- and interstand transfer are 90% and 80%, respectively. The corresponding values for the rate constant of transfer are 2 x 10(11), 1 x 10(12), and 4 x 10(11) s-1. Transfer is inefficient when A is the donor or the acceptor. In addition to the dipole-dipole term, the only other significant term in the expansion of the interaction potential is the dipole-quadrupole term which, however, makes only a small contribution to the overall transfer efficiency. The electron exchange interaction appears to be much less efficient than the coulombic interaction.

Two-quantum UV photochemistry of nucleic acids: comparison with conventional low-intensity UV photochemistry and radiation chemistry

The action of high-intensity laser u.v. radiation on nucleic acid molecules and their constituents in vitro and in vivo is compared with the results of low-intensity u.v. photolysis and gamma-radiolysis.

Synchrotron excitation of DNA fluorescence

The first lifetime measurements of DNA fluorescence are reported. Natural and synthetic DNA have been excited by 1.76 ns pulses of synchrotron ultraviolet radiation (270 nm) and the time profile of the fluorescence has been measured by synchronous single-photon counting. A post-pulse exponentially decaying emission has been observed with a lifetime of 2.9 +/- 0.4 ns for calf thymus DNA and 3.0 +/- 0.3 ns for poly(dA-T); this is most likely an excimer fluorescence.