Indicating pressure and environmental effects by means of the spectral shift with rhodamine B and fluorescein
Source abstract
Abstract
Fluorescence absorption and emission wavelengths can be influenced by environmental conditions, such as pressure, temperature and concentration. Here those effects are explored with an emphasis on determining the potential of rhodamine B and fluorescein as high-pressure indicators. The red shift of the emission peak maxima of rhodamine B and fluorescein are investigated in dependence of pressure up to 200 MPa using as the solvents water, ethanol and poly(dimethylsiloxane) (PDMS) with rhodamine B and water, polystyrene beads and melamine resin beads with fluorescein. Emission spectra recording and peak fitting is done automatically at time intervals of down to a second and with 0.3 nm wavelength resolution. The wavenumber-pressure relation for rhodamine B reveals increasing divergence from linear behavior in the sequence of the solvents water, ethanol and silicone rubber. Graphical correlation of the data diverging only slightly from linearity with a selection of polarity functions is enabled using the concept of ‘deviation from linearity (DL)’ plots. Using the example of rhodamine B dissolved in PDMS elastomer it is shown that there is a temperature induced irreversible molecular reordering, when scanning between 3 and ∼50°C, and a polarity change in the proximity of the embedded dye molecule. Swelling studies are performed with PDMS containing rhodamine B, where the elastomer is first put in water, then in ethanol and again in water. There a complex solvent exchange process is revealed in the elastomer demonstrating the feasibility of fluorescence spectroscopy, when observing variations in wavelength, to indicate and enlighten molecular rearrangements and swelling dynamics in the polymer, and polarity changes and solvent exchange processes in the dye solvation shell.
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Research context
OpenAlex topics: Photochemistry and Electron Transfer Studies · Luminescence and Fluorescent Materials · Analytical Chemistry and Sensors
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Fraunhofer Institute for Biomedical Engineering IBMT , D-66386 St. Ingbert, Germany
References (44)
Show source-provided references
1. Effect of pressure on the formation of the intramolecular excited complex state in 4-(9-anthrylmethyl)-N,N-dimethylaniline10.1016/0009-2614(85)80412-7 ↗
2. High pressure studies of solvent effects on anthracene spectra10.1073/pnas.71.12.4757 ↗
3. Pressure-induced solvatochromism of the charge-transfer transitions in pyridinium betaines10.1021/j100346a025 ↗
4. Proteins under pressure10.1111/j.1432-1033.1994.tb18774.x ↗
5. High-pressure fluorescence correlation spectroscopy10.1016/S0006-3495(03)74694-3 ↗
6. Alteration of citrine structure by hydrostatic pressure explains the accompanying spectral shift10.1073/pnas.0802252105 ↗
7. In situ monitoring by quantitative Raman spectroscopy of alcoholic fermentation by saccharomyces cerevisiae under high pressure10.1007/s00792-006-0054-x ↗
8. A sensitive pressure sensor for diamond anvil cell experiments up to 2 GPa: FluoSpheres10.1063/1.2234821 ↗
9. Tunable picosecond pulses from a short-cavity dye laser under ultra-high pressure using diamond-anvil cell10.1007/BF00697478 ↗
10. Two examples of pressure tuning spectroscopy in solid polymeric media10.1021/ie0008981 ↗
11. Ultrafast pressure-sensitive paint for shock compression spectroscopy10.1063/1.4880401 ↗
12. Molecular adsorbates under high pressure: a study using surface-enhanced Raman scattering spectroscopy10.1088/1742-6596/500/12/122004 ↗
13. Emission of the contact ion pair of rhodamine dyes observed by single molecule spectroscopy10.1016/S0009-2614(00)00354-7 ↗
14. Electrochromism and solvatochromism10.1002/anie.196901771 ↗
15. Mechanisms of tryptophan fluorescence shifts in proteins10.1016/S0006-3495(01)76183-8 ↗
16. 2007 · 205
17. Spektroskopische Bestimmung des Dipolmomentes Aromatischer Verbindungen im Ersten Angeregten Singulettzustand
18. Universal molecular interactions and their effect on the position of the electronic spectra of molecules in two component solutions, VII. Theory (general case of an isotropic solution)
19. Zur Lösungsmittelabhängigkeit der Wellenzahl von Elektronenbanden Lumineszierender Moleküle und über die Bestimmung der Elektrischen Dipolmomente im Anregungszustand
20. Determination du moment dipolaire d’une molecule dans un etat excite singulet: application a l’indole, au benzimidazole et a l’indazole
21. Determination of excited singlet-state dipole moments of hydroxy and methoxy coumarins using solvatochromic method10.5155/eurjchem.3.1.75-80.498 ↗
22. Solvent effect on the ground and excited state dipole moments of fluorescein10.1016/S0166-1280(01)00513-9 ↗
23. Solvatochromism and barochromism revisited and revealed10.1021/ed085p317 ↗
24. Comparison of COSPEC and two miniature ultraviolet spectrometer systems for SO2 measurements using scattered sunlight10.1007/s00445-005-0026-5 ↗
25. Enhanced emission from liquid-crystal lasers10.1063/1.1829144 ↗
26. Ground and excited state dipole moments of coumarin 337 laser dye10.1016/j.optcom.2010.06.037 ↗
27. Optical dephasing in pentacene-doped PMMA under high pressure10.1063/1.473482 ↗
28. Ground and excited state dipole moments of exalite 404 and exalite 417 UV laser dyes determined from solvatochromic shifts of absorption and fluorescence spectra10.1016/S0166-1280(02)00734-0 ↗
29. Effect of solvents on the dipole moments and fluorescence quantum yield of rhodamine dyes
30. High-pressure study of rhodamine B in solution and adsorbed on oriented single-crystal zinc oxide10.1021/j100260a028 ↗
31. Water density and polarizability deduced from the refractive index determined by interferometric measurements up to 250 MPa10.1063/1.3698481 ↗
32. The Tait Equation: 100 Years On10.1007/BF01133262 ↗
33. Dielectric constant and density of water as a function of pressure at constant temperature10.1590/S0103-97332004000100006 ↗
34. Liquid densities at elevated pressures of 1-alkanols from C1 to C10: a critical evaluation of experimental data10.1021/je00016a055 ↗
35. Effect of pressure on the static relative permittivities of alkan-1-ols at 298.15 K10.1021/je060248p ↗
36. Importance of using Eulerian representation of strain in high pressure studies on liquids10.1063/1.443974 ↗
37. Piezo- and elasto-optic properties of liquids under high pressure. III. Results on twelve more liquids10.1063/1.440696 ↗
38. Novel method for static equation-of-state-development: equation of state of a cross-linked poly(dimethylsiloxane) (PDMS) network to 10 GPa10.1063/1.1879872 ↗
39. Luminescence nanothermometry10.1039/c2nr30764b ↗
40. Photobleaching absorbed rhodamine B to improve temperature measurements in PDMS channels10.1039/B805172K ↗
41. Fluorescence quantum yields of some rhodamine dyes10.1016/0022-2313(82)90045-X ↗
42. A laser-induced fluorescence measurement for aqueous fluid flows with improved temperature sensitivity10.1007/s00348-008-0506-4 ↗
43. 2013 · 97
44. See supplementary material at http://dx.doi.org/10.1063/1.4927687 for graphical user interfaces of control software (Fig. S1); example of wavelength range selection for peak fitting (Fig. S2); fitting parameters of the wavelength-pressure data (Tab. S3); wavelength and intensity shifts with pressure for FITC-melamine resin beads in ethanol (Fig. S4); rare example of reversible shift in wavelength with changing pressure for rhodamine B (1 ⋅ 10−5M) in PDMS (Fig. S5); mathematical basis of ‘deviation from linearity (DL)’ plots (Eqs. S6); derivation of equation(2)(Eqs. S7); DL vs. pressure plots for two more polarity functions different from those in the eqs. (1)-(3) (Fig. S8); example of irreversible wavelength shift of rhodamine B in ethanol, when water is penetrating in the solution during pressure cycling (Fig. S9).