Extracting the Excitonic Hamiltonian of the Fenna-Matthews-Olson Complex Using Three-Dimensional Third-Order Electronic Spectroscopy

We extend traditional two-dimensional (2D) electronic spectroscopy into a third Fourier dimension without the use of additional optical interactions. By acquiring a set of 2D spectra evenly spaced in waiting time and dividing the area of the spectra into voxels, we can eliminate population dynamics from the data and transform the waiting time dimension into frequency space. The resultant 3D spectrum resolves quantum beating signals arising from excitonic coherences along the waiting frequency dimension, thereby yielding up to 2n-fold redundancy in the set of frequencies necessary to construct a complete set of n excitonic transition energies. Using this technique, we have obtained, to our knowledge, the first fully experimental set of electronic eigenstates for the Fenna-Matthews-Olson (FMO) antenna complex, which can be used to improve theoretical simulations of energy transfer within this protein. Whereas the strong diagonal peaks in the 2D rephasing spectrum of the FMO complex obscure all but one of the crosspeaks at 77 K, extending into the third dimension resolves 19 individual peaks. Analysis of the independently collected nonrephasing data provides the same information, thereby verifying the calculated excitonic transition energies. These results enable one to calculate the Hamiltonian of the FMO complex in the site basis by fitting to the experimental linear absorption spectrum.     

Time dependent – density functional theory characterization of organic dyes for dye-sensitized solar cells

We aim at providing better insight into the parameters that govern the intramolecular charge transfer (ICT) and photo-injection processes in dyes for dye-sensitised solar cells (DSSC). Density functional theory (DFT) and time-dependent DFT (TD-DFT) calculations are utilized to study the geometry, electronic structure, electrostatic potential (ESP) and absorption spectrum, for a representative donor-π bridge-acceptor (D–π–A) dye for DSSC. The coplanar geometry of the dye (D1) facilitates strong conjugation and considerable delocalization originating the π CT interaction from donor to acceptor orbitals and the hyper-conjugative interactions involving Rydberg states. A model simulating the adsorption of the dye on the TiO₂ surface is utilized to estimate binding energies. The effect of fluorine substituents in the π-spacer on the quantum efficiency of DSSCs was investigated. Gibb’s free energy values, redox potentials, excited state lifetime, non-linear optical properties (NLO) and driving forces for D1 and its fluorinated derivatives were computed.     

Purification and characterization of renal ferredoxin from bovine renal mitochondria

A renal ferredoxin was purified from bovine renal mitochondria to electrophoretic purity. The molecular weight of the renal ferredoxin was estimated by gel filtration and SDS-polyacrylamide gel electrophoresis to be 12,500 and 13,000, respectively. The optical absorption spectrum of renal ferredoxin in the oxidized form showed two peaks at 416 and 457 nm in the visible region, and the EPR absorption spectrum showed peaks at gx = gy =1.94 and gz = 2.02 in the reduced form at 13K. These spectra were typical of the 2S-2Fe type ferredoxins. Dissimilarities were recognized in the amino acid composition and isoelectric point between bovine renal ferredoxin and bovine adrenodoxin, but not in the optical, magnetic, and immunochemical properties. The reconstitution of 25-hydroxyvitamin D3-1 alpha-hydroxylase system was performed with the three components of NADPH-adrenodoxin reductase from bovine adrenal mitochondria, renal ferredoxin, and cytochrome P-450(1) alpha from bovine renal mitochondria. The results showed that the renal ferredoxin was essential for the 1 alpha-hydroxylase activity of 25-hydroxyvitamin D3.     

Theory of optical spectra of photosystem II reaction centers: location of the triplet state and the identity of the primary electron donor

Based on the structural analysis of photosystem II of Thermosynechococcus elongatus, a detailed calculation of optical properties of reaction-center (D1-D2) complexes is presented applying a theory developed previously. The calculations of absorption, linear dichroism, circular dichroism, fluorescence spectra, all at 6 K, and the temperature-dependence of the absorption spectrum are used to extract the local optical transition energies of the reaction-center pigments, the so-called site energies, from experimental data. The site energies are verified by calculations and comparison with seven additional independent experiments. Exciton relaxation and primary electron transfer in the reaction center are studied using the site energies. The calculations are used to interpret transient optical data. Evidence is provided for the accessory chlorophyll of the D1-branch as being the primary electron donor and the location of the triplet state at low temperatures.     

7-Amino-actinomycin D as a cytochemical probe. I. Spectral properties.

The optical absorption and fluorescence characteristics of 7-animo-actinomycin D were determined to evaluate its potential as a fluorescent cytochemical probe. At pH 7.0, the absorption maximum and fluorescence excitation maximum are both at 503 nm; the fluorescence emission is at 675 nm. When this compound forms complexes with DNA in solution, the absorption and fluorescence excitation maxima shift to 543 nm and the fluorescence emission shifts to 655 nm. The fluorescence quantum yield is 0.016 for 7-amino-actinomycin D free in solution and 0.01-0.02 for complexes with native DNA. The 7-amino-actinomycin D also exhibits fluorescence shifts characteristic of binding when put into solution with poly(dG-dC) poly(dG-dC), but not with poly(dI-dC) poly(dI-dC). The spectral characteristics are the same at pH 7.0 whether the solvent is 0.01 M PO4 with 0.0001 M EDTA or Earle's salts with 0.025 M N-2-hydroxyethylpiperazine-N1-2-ethanesulfonic acid.     

Synthesis,luminescence, and excited-state absorption properties of disubstituted perylene diimide derivatives modified at bay region

Three A–π–A or D–π–D perylene diimide ( PDI ) derivatives with varied groups on π-conjugate were synthesized and characterized. The photophysical properties of these compounds were systematically studied by spectral experiments and density functional theory calculations. All compounds displayed intense absorption bands at 300–800 nm wavelengths. However, diverse groups on the π-conjugate influenced the UV–vis absorption. Electron-withdrawing groups on PDI-2 caused a slight red shift at the 350–400 nm wavelength and a blue shift after 400 nm wavelength. At the same time, the electron-donating substituents on PDI-3 caused an obvious red shift of this band. These PDI derivatives exhibited emission in solution at room temperature (λ_em = 500–850 nm). The quantum yield of PDI-3 decreased, while the electron-donating substituents were introduced to the π-conjugated motifs. However, the quantum yield of PDI-2 increased when electron-withdrawing substituents were introduced to the π-conjugated motifs. In addition, PDI-1 and PDI-2 exhibited broad triplet transient absorption in the visible region. These photophysical properties could help us to understand the relationship between structure and photophysical properties of perylene diimide derivatives and exploit more original perylene diimide-based optical functional materials.     

Metallocytochromes c: characterization of electronic absorption and emission spectra of Sn4+ and Zn2+ cytochromes c.

Tin (Sn4+) and zinc (Zn2+) derivatives of horse heart cytochrome c have been prepared and their optical spectra have been characterized. Zinc cytochrome c has visible absorption maxima at 549 and 585 nm and Soret absorption at 423 nm. Tin cytochrome c shows visible absorption maxima at 536 and 574 nm and Soret absorption at 410 nm. Unlike iron cytochrome c in which the emission spectrum of the porphyrin is almost completely quenched by the central metal, the zinc and tin derivatives of cytochrome c are both fluorescent and phosphorescent. The fluorescence maxima of zinc cytochrome c are at 590 and 640 nm and the fluorescence lifetime is 3.2 ns. The fluorescence maxima of Sn cytochrome are at 580 and 636 nm and the fluorescence lifetime is under 1 ns. The quantum yield of fluorescence is Zn greater than Sn while the quantum yield of phosphorescence is Sn greater than Zn. at 77 K the fluorescence and phosphorescence emission spectra of Sn and Zn cytochrome c show evidence of resolution into vibrational bands. The best resolved bands occur at frequency differences 750 cm-1 and 1540--1550 cm-1 from the O-O transition. These frequencies correspond with those obtained by resonance Raman spectroscopy for in-plane deformations of the porphyrin macrocycle.     

Time-resolved absorption, circular dichroism, and emission of tRNA. Evidence that the photo-cross-linking of 4-thiouridine in tRNA occurs from the triplet state

The time-resolved optical density (TROD) and time-resolved circular dichroism (TRCD) spectra of the lowest triplet state of 4-thiouridine (4t-Urd) in aqueous solutions of tRNA are reported. The TROD spectrum is consistent with the triplet state being primarily in the thione tautomer. The intersystem crossing yield to the triplet is 0.35 and 0.27 (+/- 10%), respectively, with and without 10(-2) Mg2+ added to the solution. Upon addition of increasing amounts of I- to solutions of tRNA, the initial triplet yield decreases, the rate of the observed triplet decay increases, and the quantum yield of internal photo-cross-linking decreases for the 4t-Urd chromophore. The results show quantitatively that the near-UV-induced photo-cross-linking reaction in tRNA occurs from the triplet state of 4t-Urd. From the TRCD spectrum the dissymmetry factor (delta epsilon/epsilon) of some of the triplet-triplet absorption bands is shown to be significantly larger than for any of the ground-state absorption bands. Two CD transitions are seen in the triplet-triplet spectrum which are obscured in the TROD spectrum by the strong ground-state bleaching signal near 335 nm. This shows that TRCD may be useful, in some cases, in locating electronic transitions that are not observed in TROD spectra.     

The preparation of CdTe nanoparticles and CdTe nanoparticle-labelled microspheres for biological applications.

Different sizes of CdTe semiconductor nanoparticles were prepared in aqueous solution. These nanoparticles exhibit narrow fluorescence with full width at half-maximum (FWHM) of 35-45 nm that spans the visible spectrum, and they also have high PL quantum yield with high resistance to photodegradation. In addition, CdTe quantum dot (QD)-labelled microspheres, comprising polystyrene (PS) cores and CdTe/polyelectrolyte (PE) shells, were also prepared by the layer-by-layer technique in this paper. The optical properties of the CdTe nanoparticles and CdTe-labelled microspheres were investigated by UV-Visible absorption and luminescence spectroscopy, and fluorescence microscopy was employed for microscopic identification behaviour of the luminescent microspheres.     

Fluorescence and phosphorescence of adrenolutin

Adrenolutin 3,5,6-trihydroxy-1-methylindole is an intermediate in the metabolism of adrenaline and in the formation of adrenochromo-melanins. Excitation and emission spectra, quantum yield of the adrenolutin fluorescence in water, D2O, ethanol, methanol, acetone and aqueous phosphate buffer at different pH at 293K temperature are reported. Dependence of the quantum yield of adrenolutin on its concentration are measured. Lifetimes of 0.1 mM adrenolutin in water and ethanol are 32.0 +/- 0.2 ns and 9.2 +/- 0.2 ns respectively. Also fluorescence and phosphorescence spectra of adrenolutin in methanol at 110K are obtained. Degrees of polarization and angles between the dipoles for the three main bands absorption of adrenolutin from measurements at 103K are calculated. Adrenolutin may be classified as one of the most strongly fluorescing metabolites. Broad excitation spectrum and high quantum yields make this compound a potential effective acceptor of excitation energy.     

Absolute action spectrum of E-FADH2 and E-FADH2-MTHF forms of Escherichia coli DNA photolyase

Escherichia coli DNA photolyase mediates photorepair of pyrimidine dimers occurring in UV-damaged DNA. The enzyme contains two chromophores, 1,5-dihydroflavin adenine dinucleotide (FADH2) and 5,10-methenyltetrahydrofolylpolyglutamate (MTHF). To define the roles of the two chromophores in the photochemical reaction(s) resulting in DNA repair and the effect of DNA structure on the photocatalytic step, we determined the absolute action spectra of the enzyme containing only FADH2 (E-FADH2) or both chromophores (E-FADH2-MTHF), with double- and single-stranded substrates and with substrates of different sequences in the immediate vicinity of the thymine dimer. We found that the shape of the action spectrum of E-FADH2 matches that of the absorption spectrum with a quantum yield phi (FADH2) = 0.69. The action spectrum of E-FADH2-MTHF is also in a fairly good agreement with the absorption spectrum with phi (FADH2-MTHF) = 0.59. From these values and from the previously established properties of the two chromophores, we propose that MTHF transfers energy to FADH2 with a quantum yield of phi epsilon T = 0.8 and that 1FADH2 singlet transfers an electron to or from the dimer with a quantum yield phi ET = 0.69. The chemical nature of the chromophores did not change after several catalytic cycles. The enzyme repaired a thymine dimer in five different sequence contexts with the same efficiency. Similarly, single- and double-stranded DNAs were repaired with the same overall quantum yield.     

Thermal sensitivity of the red absorption tail of the photosystem II reaction center complex.

The red tail of the absorption spectrum of the D1-D2-cytb559 complex, defined as the absorption signal not described by the two Gaussian sub-bands associated with the intense electronic transitions at 680 and 683 nm, exhibits anomalous temperature behavior. This tail was analyzed in the temperature interval between 80 and 300 K in terms of the mean square deviation (sigma2) of the total Qy absorption band and by Gaussian sub-band decomposition. The value of the average optical reorganization energy (Snum) obtained from the temperature dependence of sigma2 for the whole absorption band was 32 cm(-1), and changed to 16-20 cm(-1) after subtraction of the sub-bands describing the red tail. This latter value is in agreement with the hole burning literature data for chlorophyll bound to proteins, and indicates that the rather high value for the apparent optical reorganization energy obtained by analysis of the total Qy band of the D1-D2-cytb559 complex is determined by the temperature sensitivity of the red tail. This suggests that the long wavelength absorption tail might be due to vibrational transitions associated with vibrational modes in the range of 80-150 cm(-1) which are thermally accessible and give rise to an absorption signal on the low-energy side of the (0,0) transition. On the basis of this assumption, the electron-phonon coupling strength (S) for these modes is estimated to be in the range 0.028-0.18. This interpretation furthermore supports the idea that the electronic transition near 683 nm is that of a monomer chlorophyll.     

Fast reactions in carbon monoxide binding to heme proteins.

Using fast flash photolysis, we have measured the binding of CO to carboxymethylated cytochrome c and to heme c octapeptide as a function of temperature (5 degrees-350 degreesK) over an extended time range (100 ns(-1) ks). Experiments used a microsecond dye laser (lambda = 540 nm), and a mode-locked frequency-doubled Nd-glass laser (lambda = 530 nm). At low temperatures (5 degrees-120 degreesK) the rebinding exhibits two components. The slower component (I) is nonexponential in time and has an optical spectrum corresponding to rebiding from an S = 2, CO-free deoxy state. The fast component (I*) is exponential in time with a lifetime shorter than 10 mus and an optical spectrum different from the slow component. In myoglobin and the separated alpha and beta chains of hemoglobin, only process I is visible. The optical absorption spectrum of I* and its time dependence suggest that it may correspond to recombination from an excited state in which the iron has not yet moved out of the heme plane. The temperature dependences of both processes have been measured. Both occur via quantum mechanical tunneling at the lowest temperatures and via over-the-barrier motion at higher temperatures.     

Romanowsky dyes and Romanowsky-Giemsa effect. 2. Eosin Y, erythrosin B, tetrachlorofluorescein, spectroscopic characterization of pure dyes, association of eosin Y

Analytically pure samples of the Romanowsky dyes eosin y, erythrosin b and tetrachlorofluorescein are prepared. DC of the dye samples shows no contaminations. We measured the absorption spectra of the dye dianions in alkaline aqueous solution and of the dye acids in 95% ethanol at very low dye concentrations. The molar extinction coefficients of the long wavelength absorption of the monomeric dye species are determined (Table 1). The extinction coefficients may be used for standardisation of dye samples. The absorption spectra of eosin y in aqueous solution are dependent on concentration. Using a new very sensitive method it was possible to identify two association equilibria from the concentration dependency of the spectra. Dimers are formed even in very dilute solutions, at higher concentrations tetramers. The dissociation constant of the dimers D in monomers M at 293 K, pH = 12, is K21 = 2,9 X 10(-5) M; of the tetramers Q in dimers D K42 = 2,4 X 10(-3) M. From the experimental spectra of eosin solutions at various concentrations, pH = 12, and the equilibrium constants K21, K42 the absorption spectra of the pure monomers, dimers and tetramers are calculated. M has one long wavelength absorption band, VM = 19300 cm-1, epsilon M = 1,03 X 10(5) M-1 cm-1; D also one absorption band, VD = 19300 cm-1, epsilon D = 1,74 X 10(5) M-1 cm-1; Q two absorption bands, VQ1 = 19100, VQ2 = 20200 cm-1, epsilon Q1 = 1,65 X 10(5), epsilon Q2 = 1,96 X 10(5) M-1 cm-1. The absorption spectrum of the dimers is discussed by quantum mechanics.     

Fabrication of 2D and 3D Architectures with Silver Nanostructures Building Blocks and Studying Their Refractive Index Sensitivity

In this research project, a colloidal solution of silver nanocubes was synthesized and using these nanocubes as building blocks, 2D and 3D ordered structures on solid supports were fabricated to study their optical properties and refractive index sensitivities. The silver nanocubes were synthesized by the polyol reduction process while their 2D and 3D ordered structures were fabricated by Langmuir-Blodgett trough (LB). Atomic force microscopy (AFM) and scanning electron microscopy (SEM) were employed to investigate the size and shape of the nanostructures as well as the morphologies of 2D and 3D structures. UV-visible absorption spectroscopy was employed to explore their optical properties. Finally, 2D and 3D assemblies of silver nanocubes were employed to investigate their refractive index sensitivity (RIS). The SEM image showed silver nanocubes with nominal edge length of 80 nm. Extinction spectra of 2D and 3D ordered structures are different than those in a colloidal state. Intensity of the plasmon resonance modes is higher for the 3D assembly than that of the 2D assembly. A new band in the low energy region of the spectrum appears for the 3D assembly because of interparticle coupling of the plasmon resonance modes. 3D assembly showed a higher RIS (158.9/ RIU) than of the 2D assembly (150.3/RIU). However, nanocubes are less ordered in 2D substrate than its counterpart 3D. Such 2D and 3D assemblies of silver nanocubes (AgNCs) could be potential candidates for making refractive index-based sensors as well as promising surface-enhanced Raman scattering (SERS) active substrates.     

Effect of 5-deazaflavin on energy transduction during catalysis by Escherichia coli DNA photolyase.

DNA photolyase from Escherichia coli contains 1,5-dihydroFAD (FADH2) plus 5,10-methenyltetrahydropteroylpolyglutamate. The action spectrum observed for apoenzyme reconstituted with 5-deazaFADH2 (EdFADH2) matched its absorption spectrum after correction for the presence of a small amount of inactive 5-deazaFADox. The quantum yield for dimer repair with EdFADH2 (phi EdFADH2 = 0.110) was 6-fold lower than that observed with apoenzyme reconstituted with FADH2. Excited-state redox potential calculations indicate that 5-deazaFADH2 singlet is a better one-electron donor (E = -3.5 V) than FADH2 singlet (E = -2.7 V). Other studies indicate that the quantum yield for electron transfer from reduced flavin singlet to pyrimidine dimer (0.88) is unaffected when FADH2 is replaced by 5-deazaFADH2. Enhanced back electron transfer from pyrimidine dimer radical to flavin radical may account for the decreased quantum yield observed with EdFADH2 since, in the ground state, 5-deazaFADH. is a better oxidant than FADH.. The action spectrum observed for apoenzyme reconstituted with 5-deazaFADH2 plus 5,10-CH(+)-H4folate (EPtedFADH2) matched the absorption spectrum determined for enzyme-bound 5-deazaFADH2, indicating that the pterin chromophore was inactive as a sensitizer. This differs from results obtained with native enzyme, where pterin acts as a sensitizer via efficient singlet-singlet energy transfer to FADH2. The quantum yield for dimer repair by 5-deazaFADH2 bound to EPtedFADH2 (phi EPtedFADH2 = 0.0318) was 28.9% of that observed for EdFADH2. Spectroscopic studies indicate that singlet-singlet energy transfer in EPtedFADH2 is very efficient but only occurs in the "wrong" direction, i.e., from excited 5-deazaFADH2 to pterin.(ABSTRACT TRUNCATED AT 250 WORDS)     

Photosynthetic quantum yield dynamics: from photosystems to leaves

The mechanisms underlying the wavelength dependence of the quantum yield for CO(2) fixation (α) and its acclimation to the growth-light spectrum are quantitatively addressed, combining in vivo physiological and in vitro molecular methods. Cucumber (Cucumis sativus) was grown under an artificial sunlight spectrum, shade light spectrum, and blue light, and the quantum yield for photosystem I (PSI) and photosystem II (PSII) electron transport and α were simultaneously measured in vivo at 20 different wavelengths. The wavelength dependence of the photosystem excitation balance was calculated from both these in vivo data and in vitro from the photosystem composition and spectroscopic properties. Measuring wavelengths overexciting PSI produced a higher α for leaves grown under the shade light spectrum (i.e., PSI light), whereas wavelengths overexciting PSII produced a higher α for the sun and blue leaves. The shade spectrum produced the lowest PSI:PSII ratio. The photosystem excitation balance calculated from both in vivo and in vitro data was substantially similar and was shown to determine α at those wavelengths where absorption by carotenoids and nonphotosynthetic pigments is insignificant (i.e., >580 nm). We show quantitatively that leaves acclimate their photosystem composition to their growth light spectrum and how this changes the wavelength dependence of the photosystem excitation balance and quantum yield for CO(2) fixation. This also proves that combining different wavelengths can enhance quantum yields substantially.     

Energy transfer in the purple membrane of Halobacterium halobium.

The absorption spectrum of the primary photoproduct (the bathoproduct, or K) of the purple membrane protein (PM) at-196 degrees C has a maximum at 628 nm and an extinction coefficient of 87,000. Knowing the absorption spectrum allowed us to calculate the quantum efficiencies for PM to K and K to PM conversion at -196 degrees C. Direct measurements of these quantum yeilds at -196 degrees C gave 0.33 +/- 0.05 and 0.67 +/- 0.04, respectively. Determination of relative quantum efficiencies for PM to K and K to PM conversion by analysis of the absorption spectra of several photostationary-state mixtures of PM and K at -196 degrees C, however, gave wavelength-dependent quantum efficiencies that appear to be greater than 1. These anomolous results can be readily explained in terms of energy transfer from PM to K within the trimer clusters of pigment molecules which exist in the purple membrane. A model for such a transfer predicts an efficiency of energy transfer from PM to K of about 43%.     

High-Resolution Two-Dimensional Atomic Localization Via Tunable Surface Plasmon Polaritons

The two-dimensional (2D) atomic localization is theoretically investigated via tunable surface plasmon polaritons (SPPs), generated on the metal (Ag) surface coupled to a quantum coherent three-level \(\lambda\)-type medium (\(^{87}\)Rb) embedded as a dielectric host. Such a useful scheme for highly precise atomic localization is reported by using the absorption spectrum of SPPs. Owing to space-dependent light–matter interaction, the sharp localized peaks are observed in a single wavelength domain of 2D space with maximum probability. By properly varying the system parameters, the precision and numbers of the localized peaks are controlled. Consequently, highly efficient and high-resolution atomic localization can be achieved in a region smaller than \(\lambda /20\times \lambda /20\). The spatial resolution of atomic localization is greatly improved as compared to the previously studied cases. These results may have potential useful applications in the fields of quantum nanoplasmonics, nanolithography, and nanophotonics.

     

Fluorescent phosphonate labels for serine hydrolases. Kinetic and spectroscopic properties of (7-nitrobenz-2-oxa-1,3-diazole)aminoalkyl methylphosphonofluoridates and their conjugates with acetylcholinesterase molecular forms

The synthesis, kinetic, and spectral characterization of (7-nitrobenz-2-oxa-1,3-diazole)aminoethyl and (7-nitrobenz-2-oxa-1,3-diazole)aminopentyl methylphosphonofluoridate are described. These homologous organophosphorous agents contain the environmentally sensitive 7-nitrobenz-2-oxa-1,3-diazole chromophore. They inhibit acetylcholinesterase from Torpedo at rates exceeding 10(7) M-1 min-1 to form long-lived conjugates with one chromophore/80-kilodalton subunit. The intensity, position, and line width of the absorption spectra of the conjugates and reactivation kinetics in the presence and absence of the bisquaternary oxime 1,1'-trimethylene-bis(4-formylpyridinium bromide) dioxime indicate that these agents form conjugates in which the NBD-aminoalkyl moieties experience distinctive microscopic environments within the active center. NBD-aminoethyl methylphosphono-acetylcholinesterase undergoes oxime-induced as well as spontaneous reactivation at rates that are 3.6 and 35 times faster, respectively, than the corresponding rates measured for the NBD-aminopentyl conjugate. Hence, reactivation exhibits a marked dependence on structure of the methylphosphonate. Fluorescence emission at wavelengths greater than 520 nm is highly quenched and exhibits quantum efficiencies of less than 5%. Absorption maxima for the covalent NBD-aminoethyl methylphosphono-acetylcholinesterase appear at 475-480 nm while those for the corresponding NBD-aminopentyl methylphosphono-acetylcholinesterase appear at 485-490 nm. Bandwidths of the absorption maxima are substantially broader for the acetylcholinesterase adduct with NBD-aminoethyl methylphosphonofluoridate (3870 cm-1) than for the enzyme adduct with NBD-aminopentyl methylphosphonofluoridate (2870 cm-1). The CD spectrum of NBD-aminopentyl methylphosphono-acetylcholinesterase shows optical activity coincident with the shape and position of the absorption spectrum. In contrast, in addition to optically active transitions at the absorption maxima, the CD spectrum of NBD-aminoethyl methylphosphono-acetylcholinesterase shows intense optical activity at 430 nm, a wavelength region coincident with the region of spectral broadening. The spectral properties of alpha-chymotrypsin conjugates formed by reaction with the two probes are different, and the respective spectra differ also from those observed for the acetylcholinesterase conjugates. These results indicate that there is a reciprocal relationship between the structure of the probe and the structure of the active center.(ABSTRACT TRUNCATED AT 400 WORDS)