THE PHOTOPHYSICS OF p-AMINOBENZOIC ACID

Abstract— The lowest-lying allowed UV transition in p -aminobenzoic acid (PABA) is assigned Γ→¹L_a based on quantitative absorption and fluorescence studies, as well as semiempirical PM3 multielec-tron configuration interaction calculations. The oscillator strengths, fluorescence quantum efficiencies and lifetimes are reported for PABA in several polar, nonpolar, protic and aprotic solvents (aerated) at 296 K. Reasonable agreement is found between the observed radiative rate constant and that calculated from the absorption and fluorescence spectra. Shifts in the absorption and fluorescence spectra in aprotic solvents are analyzed in terms of the Onsager reaction field model; results are consistent with an increase in dipole moment of ca 4 D between the relaxed S₀ and S₁, states. No evidence is found for the emission from the amino-twisted form of PABA in all solvents studied although calculations show that the amino-twisted S, state is highly polar, but higher in energy by ca 35 kJ/mol ( in vacuo ). The fluorescence efficiency is excitation wavelength independent in both methylcyclohexane and water. The temperature dependence of the nonradiative rate constant (from S₁) was studied in several solvents. Nonradiative decay may be due to intersystem crossing, which would be fast enough to compete with thermally activated intramolecular NH₂ twisting. The phosphorescence spectrum and lifetime obtained in an EPA glass at 77 K are reported, and the triplet energy of PABA is estimated.     

SPECTROSCOPY OF POLYENES–III. ABSORPTION AND EMISSION SPECTRAL INVESTIGATION OF POLYENE SCHIFF BASES AND PROTONATED SCHIFF BASES RELATED TO VISUAL PIGMENTS

Abstract— A number of n -butylamine Schiff bases of polyenals related to retinals as homologues and analogues, and their protonated forms, have been studied for absorption and emission spectral properties. The polyene Schiff bases exhibit the same general features in their absorption spectra as those of the parallel polyenals except that the ^lB_u←¹A_g and π*← n singlet transitions are at substantially higher energy in the Schiff bases (the shift being larger for the π *← n transition). The Schiff bases with short polyene chainlength ( n = 2, 3 where n is the number of double bonds including C=N) do not fluoresce or phosphoresce in 3-methylpentane in the temperature range 298–77 K. The Schiff bases with intermediate chainlength ( n = 4, 5) show fluorescence at 77 K with intensity strongly dependent on the nature of solvent. The Schiff bases with relatively long chainlength ( n = 5–7) show strong or moderately strong fluorescence at 77 K and very weak fluorescence at 298 K ( n = 7) with intrinsic radiative lifetimes much longer than those estimated from the oscillator strength of the low-energy, strong absorption band (¹B_u←¹ A_g ). A discussion on the possible state order and nature of the fluorescing state of the various polyene Schiff base systems is presented.     

Characterization of emission properties of Er3+ ions in TeO2-CdF2-WO3 glasses

TeO(2)-CdF(2)-WO(3) glasses with various compositions and Er(3+) concentrations were prepared by conventional melting method. Their optical properties were studied by measuring the absorption, luminescence spectra and the decay patterns at room temperature. From the optical absorption spectra the Judd-Ofelt parameters (Ω(t)), transition probabilities, branching ratios of various transitions, and radiative lifetimes were calculated. The absorption and emission cross-section spectra of the (4)I(15/2) to (4)I(13/2) transition of erbium were determined. Emission quantum efficiencies and the average critical distance R(0) which provides a measure for the strength of cross relaxation were determined.     

TWENTY-TWO CARBON HOMOLOGUE OF 11-CIS RETINAL. PHOTOPHYSICAL AND PHOTOCHEMICAL PROPERTIES

Abstract— Results concerning absorption-emission spectra and fluorescence quantum yields at 77 and 298K. triplet absorption spectra, and quantum yields of intersystem crossing and photoisomerization at 298 K, are presented for 11- cis β-apo-14'-carotenal (C₂₂-Ald), the immediate higher homologue of 11- cis retinal. The absorption spectra are characterized by two band-systems with maxima at 390–400 and 270–280 nm, respectively. Upon cooling from 298 to 77 K, the intensities of these two band-systems undergo changes in opposite directions indicating 12-s- cis: 12- s-trans conformational changes. No intermediate band-system analogous to the one located at 270–310 nm in cis retinals is observed for 11- cis C₂₂-Ald. In nonpolar hydrocarbon solvents (e. g. cyclohexane) at room temperature, quantum yields of fluorescence (0.01), intersystem crossing (0.6) and photoisomerization (0.4) are all quite pronounced. The photophysical and photochemical properties of 11- cis C₂₂-Ald are discussed in the light of similarities and dissimilarities with those of all- trans C₂₂-Ald and 11- cis retinal under comparable conditions.     

POLARIZED UV-ABSORPTION SPECTRA OF RETINAL ISOMERS—II. ON THE ASSIGNMENT OF THE LOW AND HIGH ENERGY ABSORPTION BANDS

Abstract The polarized UV-absorption spectra of all- trans retinal and both crystal forms of 11- cis , 12-s- cis retinal (presented in the previous paper, Part I) are analyzed using Lowry-Hudson functions to describe the band profiles. The polarization ratios of the polarized bands is used to determine the direction of the corresponding transition moments. For all- trans retinal the polarization spectra show that the absorption between 23 and 36 X 10³ cm⁻¹ is caused by three overlapping bands labeled S, A and B. For 11- cis retinal the B-band is also clearly resolved whereas the S and A bands are separated with much less certainty than for all- trans retinal.
Comparing these bands with the excited state manifold resulting from semiempirical CI-calculations including double excitations, the S-band could be assigned to the ¹A_g⁻→¹A_g-* and the A-band to the ¹A_g⁻→¹B_u+* transition. However, no transition is found in this manifold which could positively be assigned to the B-band because the transitions predicted in this spectral region have negligible oscillator strengths. In all the crystal spectra a further band C is observed around 39 X 10³ cm⁻¹ which is particularly pronounced in the case of 11- cis retinal. For this band an assignment to the ¹A_g⁻→¹A_g+*-transition is proposed.     

VISUAL PIGMENTS—10. SPECTROSCOPY AND PHOTOPHYSICAL DYNAMICS OF RETINOL AND RETINYL ETHER

Abstract— The absorption and emission spectra, lifetimes and quantum yields of all-trans retinol have been examined as a function of solvent and temperature. In addition, the spectroscopy of retinyl ether and 2 other polyene alcohols have been determined. Based on the results obtained, we conclude that the singlet excited state of retinol and retinyl cther is of a forbidden character and of the type loosely called ¹A^-_g. Retinol forms a dimer in an alkane solvent when cooling from 298 to 77 K. A general structure for the dimer is proposed.     

POLARIZED ABSORPTION SPECTRA OF MONOCRYSTALLINE ALL-trans. AND 11-cis., 12-s-cis. RETINAL AT 4.2 K

Abstract Polarized absorption spectra of very thin crystal platelets of all- trans . retinal and both forms of 11- cis ., 12-s- cis . retinal were measured at liquid Helium temperature. Even at 4.2 K the spectra remain vibronically unresolved. They show, however, a distinct shoulder at 23.9 kK for all- trans . and at 22.7 kK for 11- cis ., 12-s- cis . retinal on the low energy side of the main band. An assignment of this transition to the lowest-lying ππ*-state ¹A_g-* is proposed.     

DEUTERIUM-ISOTOPE EFFECT ON THE FLUORESCENCE YIELDS AND LIFETIMES OF INDOLE DERIVATIVES–INCLUDING TRYPTOPHAN AND TRYPTAMINE

Abstract— The fluorescence yields and lifetimes of indole, five of its alkyl detivatives, tryptophan, and tryptamine have been determined in degassed, heavy and light water at room temperature. All of the compounds have radiative lifetimes nearly identical to the parent compound indole, and a comparison of these results with recently reported data on tryptophyl derivatives disclosed a striking uniformity in radiative lifetimes between indole and many amino acids and peptides which contain the indole group as the fluorescence unit. The fluorescence rate k _f in H₂O, was found to be 4.5 × 10⁷ sec^-1. The nonradiative decay rates were found to vary between 5.1 and 46 × 10⁷ sec^-1 and from a study of the deuterium-solvent isotope effect and the deuterium-substituent effect a mechanism for nonradiative deactivation is proposed which includes an isotopically dependent proton transfer and a pathway involving energy loss via the ring carbon hydrogen vibrations. Tryptophan at pH 7 was found to have a unique nonradiative decay scheme not evidenced at a pH 1 or pH 10.     

FLUORESCENCE PROPERTIES OF ISOTROPICALLY AND ANISOTROPICALLY EMBEDDED FLAVINS

Abstract— On the basis of corrected fluorescence excitation and emission spectra, flavin photo-processes in anisotropically vesicle-bound flavins have been studied. By means of aliphatic C₁₈H₃₇-chains at positions 3, 7 and 10, the flavin nucleus can be variously anchored within the membrane/water interface (amphiflavin), thereby mimicking the various positions and microenvironments of the isoalloxazine ring in flavoproteins. From polarization spectra, the angles between the different electronic transition moments of isotropically dissolved or membrane-bound flavins have been obtained. Polarization and angle spectra of isotropically and various anisotropically embedded flavins exhibit strong differences, reflecting the specific interaction with the matrices. Based on a slightly modified theory, originally developed by Perrin and Weber, using the concentration dependence of fluorescence polarization, it is found that the radiative flavin-flavin interaction (selfcontact) on the membrane is by a factor of 25 to 54 smaller than in isotropic solution. This is taken as further justification to study anisotropic flavin chemistry on the basis of flavin-loaded vesicles.     

EFFECTS OF SOLVENT ON THE FLUORESCENCE PROPERTIES OF BACTERIOCHLOROPHYLL a

Fluorescence lifetimes (τ_f) of bacteriochlorophyll a (BChl a ) have been measured by the method of time-correlated single-photon counting on dilute (1 μ M ) solutions of the pigment in 15 solvents. There is a pronounced dependence of τ_f on the nature of the solvent. Specifically, τ_f, is longer when the central magnesium is hexacoordinated than when pentacoordinated and shorter when the macrocycle is hydrogen-bonded than when it is not, but the latter effect is more pronounced. Both trends were confirmed by parallel studies on bacteriopheophytin a (BPheo a ). Because of the short lifetimes (˜ 2.2–3.6 ns), quenching of fluorescence by molecular oxygen is not a significant factor in aerated solutions of the bacterial pigments. However, reabsorption artifacts are non-negligible, which necessitates studies on dilute solutions. Fluorescence quantum yields (ø_f) have been estimated for BChl a in 13 solvents by comparing the observed fluorescence lifetimes with the radiative lifetimes calculated from the integrated absorption spectra.     

RESOLUTION ENHANCEMENT AND DECONVOLUTION INTO VIBRONIC BANDS OF THE FLUORESCENCE AND ABSORPTION SPECTRA IN THE RED REGION OF DILUTE SOLUTIONS OF CHLOROPHYLL a IN VARIOUS SOLVENTS

Abstract— The fluorescence spectra of chlorophyll a in less than 10–⁶ mol dm^-3 solutions of benzene, toluene, tetrahydrofurane, EPA and ethanol were determined at both room temperature and at 77 K. Resolution enhancement using Fourier transform methods revealed the presence of vibronic bands with essentially solvent-invariant separation between their origins; this was confirmed by the quantitative deconvolution of the spectra into Gaussian bands. It was concluded that the fluorescence is due to a single spectroscopically distinct species. The absorption spectra in the above solvents include a band absent from the fluorescence spectra which, from its position and intensity, may be identified as the longest wavelength X-polarized electronic transition of chlorophyll a. Differences observed between the shapes of the low-and high-temperature absorption spectra may be attributed primarily to the narrowing of bandwidths with decreasing temperature and to intensity redistribution within the bands; the apparent increase in the integrated intensity on cooling the solutions appears to be due largely to the increase in the volume concentration of the solute as a result of solvent contraction.     

Temperature dependent luminescence characteristics of Sm3+-doped silicate glass

We report here on the optical characterisation of Sm3+ (5 wt%): SiO2 + Al2O3 + Li2O + Na2O + MgO glass from the measurements of optical absorption spectra (at 300 K), total luminescence spectra (10-300 K) and fluorescence lifetimes (10-300 K) of the prominent emission transitions of the Sm3+ ions. Besides its spectral properties, physical and nonlinearity characterising property parameters have also been computed to understand the optical dispersive power of this glass. By the application of Judd-Ofelt parameters (omega(lambda)) of the measured absorption spectrum, the radiative transition probability factors (A) and stimulated emission cross-section (sigma(p)E) of the observed fluorescent levels have been analysed. Both emission intensity and measured lifetimes of the prominent luminescent transition (4G(5/2) --> 6H(7/2)) concerning Sm3+-glass has been showing a descending trend with the rise in temperature with N2-laser (337.1 nm) as the source of excitation.     

FLUORESCENCE CHARACTERISTICS OF INDOLES IN NON-POLAR SOLVENTS: LIFETIMES, QUANTUM YIELDS AND POLARIZATION SPECTRA

Abstract— Fluorescence lifetimes, quantum yields and polarization spectra were measured for indole, 3-methylindole and 2,3-dimethylindole in non-polar solvents. The results indicate simultaneous emission from thermally equilibrated ¹L_a and ¹L_b levels, with ¹L_a→¹ A dominating the 2,3-dimethylindole emission, and ¹L_b→¹ A dominating the indole emission. These results are consistent with previous assignments of the 0-0 transitions in absorption for these compounds. Radiative rates are: ¹L_a→¹ A , 2·0 × 10⁸ S^-1 and ¹L_b→¹ A . 0·62 → 10⁸ S^-1. In addition, the temperature dependence of the excitation and emission spectra are presented, which show that aggregation occurs with these indoles in hydrocarbons below approximately - 110°C. Possible applications to tryptophyl emission in the hydrophobic interiors of proteins are briefly discussed.     

POLARIZED UV-ABSORPTION SPECTRA OF RETINAL ISOMERS-I. MEASUREMENTS IN EXTREMELY THIN MONOCRYSTAL PLATELETS

Abstract Crystals of all- trans retinal and both different forms of 11- cis , 12-s- cis retinal were grown on quartz slides with faces (101), (001) and (101), respectively, forming thin platelets of less than 0.2 μm thickness. Polarized UV absorption spectra at room temperature were measured in the range from 20 to 43 × 10³ cm⁻¹ with a microscope-spectrophotometer. In this spectral range three diffuse absorption bands were observed for all crystal types at similar wave numbers. A main absorption band was found at 25–28 × 10³ cm⁻¹, and two further bands at 32–34 and 38–40 × 10³ cm⁻¹. In case of all- trans retinal the latter band is by far the weakest in this spectral range. Additionally, the crystal spectrum of all- trans retinal shows a shoulder at the low wavenumber side of the main band which cannot be resolved in the corresponding solution spectrum. In the crystal spectra of 11- cis , 12-s- cis retinal, however, only a strong dissymmetry is observed at this side of the main band.     

Theoretical and experimental studies of radiative lifetimes of excited electronic states in CO

The electronic dipole transition moment functions of the A ²Π-X ²Σ⁺, B ²Σ⁺-X ²Σ⁺ and B ²Σ⁺-A ²Π transitions and the dipole moment function of the X ²Σ⁺ state of CO⁺ have been calculated using large contracted CI wavefunctions. The computed transition moment functions together with experimental potential energy curves were used to obtain radiative lifetimes of the excited electronic states B ²Σ⁺ and A ²Π. Radiative lifetimes of vibrational levels of the X ²Σ⁺ state were derived from the calculated dipole moment function. The high-frequency deflection technique was used to obtain radiative lifetimes of the ν′ = 0, 1,2 and 3 vibrational levels of the B ²Σ⁺ state and also radiative lifetimes of individual rotational levels of ν′ =0. The calculated radiative lifetimes are shorter than the measured ones by about 10%. The experimental ν′ dependence is reproduced by theoretical calculation. The calculated radiative lifetimes for the A ²Π state are in excellent agreement with lifetimes measured with an ion trap technique.     

氨基功能化石墨烯量子点表面缺陷钝化及其发光增强

通过酸氧化法将氧化石墨烯进一步“切割”制备石墨烯量子点（GQDs）,在100℃水热条件下,用氨水处理石墨烯量子点制备得到氨基功能化石墨烯量子点（N-GQDs）。傅里叶变换红外光谱证明NH₃可以有效地进攻环氧基碳和羧基碳,形成羟胺和酰胺基。原子力显微镜结果表明NH₃不仅能够有助于产生更小的量子点,还对石墨烯纳米片有致孔作用。氨基功能化之后,由于C-O-C相关的n-π^*跃迁受到抑制,N-GQDs发光具有更弱的激发波长依赖性,并使其荧光量子产率从0.3%提高至9.6%。时间分辨发光光谱表明,相比含氧基团,含氮基团相关的局域电子激发态具有更长的荧光寿命和更弱的发射光谱依赖性。     

LUMINESCENCE STUDIES OF QUINIZARIN AND DAUNORUBICIN

Abstract— The absorption and emission spectra of quinizarin (1,4-dihydroxy-anthraquinone) have been investigated in hydrocarbon and alcoholic solvents. Fluorescence spectra in 3 different Shpolskii matrices were recorded at 14 K. Vibrational analyses of these spectra revealed the presence of 3, 8, and 9 sites in octane, heptane, and hexane matrices, respectively. The fluorescence lifetime was found to be 6.5 ns in hexane and EPA. Fluorescence photoselection measurements in EPA (77 K) showed that the first 4 electronic transitions of quinizarin are polarized parallel, parallel, perpendicular, and parallel to the long molecular axis and can be assigned, in order of increasing energy, to ¹B₂, ¹B₂, ¹A₁ and ¹B₂ (ππ*)→¹A₁(C_2v,) transitions, respectively. The fluorescent transition is assigned as ¹B₁ (ππ*)→¹A¹. The absence of phosphorescence is attributed to the intramolecular hydrogen bonding present which displaces the parent anthraquinone n →* states above the ππ* states, thereby rendering the intersystem crossing (S₁-T₁) radiationless pathway inefficient.
Photoselection measurements on daunorubicin, a substituted quinizarin and known anticancer drug, revealed an absorption band polarization pattern identical to that of quinizarin. These results are in part at variance with assumptions used in previous work on the intercalation specificity of daunorubicin with DNA.     

PICOSECOND LASER SPECTROSCOPY AND OPTICALLY DETECTED MAGNETIC RESONANCE ON A MODEL PHOTOSYNTHETIC SYSTEM

Fluorescence-detected magnetic resonance of triplets in zero magnetic field (FDMR), fluorescence fading (FF) due to triplet-formation, both at 4.2 K, and prompt fluorescence decay kinetics (FDK) at room temperature have been measured for free pheophorbide- a (f-Pheo) and bound (b-Pheo) to a synthetic polypeptide (L-L ys -L-A la -L-A la )_n, dissolved in dimethylformamide (DMF). Fluorescence decay kinetics measurements of f-Pheo in DMF yielded 1-5 ns lifetimes, for b-Pheo in DMF a ~ 50 ps decay-component was found emitting at 730–750 nm. Zero-field splitting parameters |D| and |E| of the lowest triplet state T₁ were determined from FDMR spectra as (337 and 24) 10^-4 cm^-1 for f-Pheo and (359 and 25) 10^-4 cm^-1 for b-Pheo, both in DMF. Decay rate constants of the three spin levels of T¹ of b-Pheo ( K _x= 1200 50 s^-1, k _y= 440 25 s^-1, k _z= 80 5 s^-1) and relative steady-state populations (N_x= 28 2%, N_y= 47 2%, N_z= 26 2%) determined from FF curves predict a fluorescence decrease at the D–E and D + E FDMR transitions, whereas experimentally a fluorescence increase is observed. The FDMR sign-inversion results from singlet-singlet energy transfer from b-Pheo monomers to their aggregates, followed by fast intersystem crossing to T₁. These results indicate that aggregates are formed by two or more b-Pheo molecules at different positions on the folded polypeptide chain. This situation resembles that in chlorophyll-proteins, containing low-lying traps, resulting from interaction of chromophores with other chromophores and with the protein environment.     

Spectroscopic properties of Er3+, Yb3 + and Er3 + /Yb3+ doped metaphosphate glasses

The absorption and emission spectroscopies of Er3+ doped and Er3+/Yb3+ codoped Ca(PO3)2, Sr(PO3)2 and Ba(PO3)2 glasses have been studied. From the Judd-Ofelt intensity parameters, the spontaneous emission probabilities of some relevant transitions and the radiative lifetimes of several excited states of Er3+ have been calculated. The decay curves of the Er3+ emission at 1.5 microm have been measured at different temperatures. The data have been fitted using a stretched exponential function and the obtained experimental lifetimes have been compared with the calculated radiative lifetimes. The difference between the experimental and calculated lifetimes is attributed to the presence of traces of OH groups in the host glasses. The absolute OH content in some glasses has been determined from the infrared spectra. The emission spectra at 1.5 microm of the Er3+ ion in the codoped glasses have been measured at different temperatures. The integrated emission intensities decrease significantly on passing from room temperature to 13 K, suggesting a temperature dependence of the rate of the energy transfer process between Yb3+ and Er3+.     

PHOTOPHYSICAL PROPERTIES OF NUCLEIC ACID COMPONENTS—1. THE PYRIMIDINES: THYMINE, URACIL, N, N-DIMETHYL DERIVATIVES AND THYMIDINE

Abstract— Low-temperature (and some room temperature) absorption and emission, fluorescence and phosphorescence, data including quantum yields and lifetimes have been obtained from the title pyrimidine bases as a function of the nature of the solvent environment. Modest vibrational resolution has been observed for the first time in the absorption spectra, particularly for thymine and uracil. The excitation spectra also show structure. The quantum yields of fluorescence (φ_F) and phosphorescence are independent of the excitation wavelength. Thymine, thymidine and uracil have profoundly different photophysical properties in polar-aprotic vs polar-protic solvents. The N, N-dimethyl substitution of thymine and uracil produces photophysical changes comparable to the solvent change for the unsubsti-tuted bases. The species involved in the emission processes is the keto (lactam) form. It is probable that ^1,3(n,π*) state(s) has(have) changed order relative to a lowest ¹(π,π*) state as a consequence of both the solvent change and N, N-dimethyl substitution. The lowest triplet state is assigned as ³(n π*). We propose that an important factor contributing to the previously reported excitation wavelength dependence of φ_F and φ_T1 (φ_isc) for nucleic-acid components is the equilibrium coexistence of H-bonded and non-H-bonded forms each having different photophysical properties. Consideration is given of the impact of the significantly different photophysical properties of nucleic-acid bases as a function of the nature of the solvent upon the photochemical properties.