‘Excimer’ fluorescence - IX. Lifetime studies of pyrene crystals

The increase of the excimer fluorescence lifetime Ƭ D (= 1/ k D ) with increasing purity was used to establish a reproducible criterion of purity for crystalline pyrene. Zone-refining, microsublimation and adsorption chromatography yielded material with similar high values of Ƭ D = 113±2 ns at 293 °K, but recrystallization from solution was ineffective. Single crystals of zone-refined pyrene were grown by sublimation, and Ƭ D and the fluorescence quantum efficiency q D were observed from 100° to 350 °K. Values of k fD = 5·55 × 10 6 s -1 , k 0 iD = 0, and k iD = 4·7 × 10 7 exp [ –0·066 (eV)/ kT ] s -1 are obtained for the rate parameters of fluorescence, temperature-independent intersystem crossing and temperature-dependent intersystem crossing, respectively. Ƭ D for microcrystalline layers ca . 0·5 μ m thick is lower than for single crystals, owing to a crystal-size effect which limits the exciton lifetime. The reduction in Ƭ D is accompanied by the appearance of a surface monomer band in the fluorescence spectrum. The exciton migration process in anthracene and pyrene crystals is discussed. From lifetime data it is concluded that singlet excitons in organic molecular crystals are localized and identical with singlet-excited molecules and that they migrate by a hopping mechanism, rather than through a hypothetical exciton band. The pyrene excimer parameters are similar in the crystal and in solution; it is concluded that the excimer molecular configuration is that of the unexcited crystal dimer but with a reduced spacing between the molecular planes.

Observations were made by the pulsed light source method of the fluorescence lifetimes of 1, 6-dimethyl naphthalene solutions of 10 -4 to 6⋅4 M (pure liquid) in n -heptane from 200 to 295°K, and in cyclohexane and phenylcyelohexane at 295°K. The design and characteristics of discharge lamps containing various gases are described. For dilute solutions up to ca . 1M the lifetime data are consistent with the established monomer/excimer reaction scheme with rate parameters which are independent of concentration. For more concentrated solutions the rate parameters, notably those of internal quenching, are concentration dependent. In dilute n -heptane solution (and in the pure liquid, for which the values are in parentheses) the respective monomer and excimer rate parameters are k fM = 5x10 6 s -1 and k fD = 1⋅4 x 10 6 s -1 (2⋅2 x 10 6 s -1 ) for fluorescence, and k 0 iM = 11⋅6 x 10 6 s -1 and k 0 iD = 5⋅1 x 10 6 s -1 (4⋅2 x 10 6 s -1 ) for the temperature-independent component of intersystem crossing. The respective monomer and excimer temperature-dependent intersystem crossing rate parameters, which are influenced by solvent-solute interactions, have frequency factors of k ' iM = 2⋅7 x 10 8 s -1 and k ' iD = 6⋅0 x 10 9 s -1 (3⋅2x10 10 s -1 ) and activation energies of W iM = 0⋅11 eV and W iD = 0⋅16 eV (0⋅19 eV). Evidence is presented that k fM / k 0 iM = k fD / k 0 iD and that the excimer triplet state is dissociated. The excimer binding energy of B = 0⋅26 ± 0⋅05 eV agrees with previous spectral data.


2002 ◽  
Vol 17 (11) ◽  
pp. 2960-2965 ◽  
Author(s):  
E. Arushanov ◽  
L. Ivanenko ◽  
D. Eckert ◽  
G. Behr ◽  
U. K. Rößler ◽  
...  

Results of magnetization and magnetic susceptibility measurements on undoped and Co-doped FeSi2.5 single crystals are presented. The temperature dependence of the magnetic susceptibility of the Co-doped sample in the range of 5–300 K can be explained by temperature-dependent contributions due to paramagnetic centers and the carriers excited thermally in the extrinsic conductivity region. The values of the paramagnetic Curie temperature and activation energy of the donor levels were estimated. It is also shown that the magnetic susceptibility of Co-doped samples cooled in zero external field and in a field are different. This resembles the properties of spin-glasses and indicates the presence of coupling between magnetic centers.


A summary is given of some present ideas on the mechanism of work-hardening of single crystals and polycrystalline materials. In particular, the difference is stressed between the three stages of hardening: stage I, or easy glide; stage II, the region of rapid hardening accompanied by short slip lines; and stage III, the region of slow or parabolic hardening which is temperature-dependent and in which long slip bands are formed.


2015 ◽  
Vol 644 ◽  
pp. 854-861 ◽  
Author(s):  
I. Jankowska-Sumara ◽  
M. Ptak ◽  
M. Mączka ◽  
A. Majchrowski ◽  
T.H. Kim ◽  
...  

2016 ◽  
Vol 29 (12) ◽  
pp. 3041-3047 ◽  
Author(s):  
Boby Joseph ◽  
Alessandro Ricci ◽  
Nicola Poccia ◽  
Valentin G. Ivanov ◽  
Andrey A. Ivanov ◽  
...  

Pramana ◽  
1996 ◽  
Vol 47 (2) ◽  
pp. 133-143 ◽  
Author(s):  
Suruchi Anand ◽  
Prabhat Verma ◽  
S C Abbi ◽  
K P Jain ◽  
M J Tafreshi ◽  
...  

2018 ◽  
Vol 85 (3) ◽  
Author(s):  
Tianbao Cheng ◽  
Daining Fang ◽  
Yazheng Yang

Knowledge of the ideal shear strength of solid single crystals is of fundamental importance. However, it is very hard to determine this quantity at finite temperatures. In this work, a theoretical model for the temperature-dependent ideal shear strength of solid single crystals is established in the view of energy. To test the drawn model, the ideal shear properties of Al, Cu, and Ni single crystals are calculated and compared with that existing in the literature. The study shows that the ideal shear strength first remains approximately constant and then decreases almost linearly as temperature changes from absolute zero to melting point. As an example of application, the “brittleness parameter” of solids at elevated temperatures is quantitatively characterized for the first time.


2020 ◽  
Vol 235 (4-5) ◽  
pp. 117-125
Author(s):  
Myroslava Horiacha ◽  
Maximilian K. Reimann ◽  
Jutta Kösters ◽  
Vasyl‘ I. Zaremba ◽  
Rainer Pöttgen

AbstractThe quaternary gallium-rich intermetallic phases RE2Pt3Ga4In with RE = Y and Gd-Tm were synthesized by arc-melting of the elements and subsequent annealing. Small single crystals were obtained by high-frequency annealing of the samples in sealed tantalum ampoules. The polycrystalline samples were characterized through their X-ray powder patterns. The RE2Pt3Ga4In phases crystallize with a site ordering variant of the orthorhombic Y2Rh3Sn5 type, space group Cmc 21. The structures of Gd2Pt3Ga4In, Dy2Pt3Ga4.14In0.86, Er2Pt3Ga4.17In0.83 and Tm2Pt3Ga4.21In0.79 were refined from single-crystal X-ray diffraction data. The single crystals reveal small homogeneity ranges RE2Pt3Ga4±xIn1±x. The striking geometrical structural building units are slightly distorted trigonal prisms around the three crystallographically independent platinum atoms: Pt1@RE4Ga2, Pt2@RE2Ga4 and Pt3@RE2Ga2In2. Based on these prismatic building units, the RE2Pt3Ga4In structures can be described as intergrowth variants of TiNiSi and NdRh2Sn4 related structural slabs. Temperature dependent magnetic susceptibility studies of Gd2Pt3Ga4In and Tb2Pt3Ga4In show Curie-Weiss behavior and the experimental magnetic moments confirm stable trivalent gadolinium respectively terbium. Gd2Pt3Ga4In and Tb2Pt3Ga4In order antiferromagnetically at TN = 15.8(1) and 26.0(1) K. Magnetization curves at 3 K show field-induced spin reorientations.


2020 ◽  
Vol 11 (7) ◽  
pp. 2490-2496 ◽  
Author(s):  
Giovanni Mannino ◽  
Ioannis Deretzis ◽  
Emanuele Smecca ◽  
Antonino La Magna ◽  
Alessandra Alberti ◽  
...  

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