2018
DOI: 10.1002/mma.4804
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On the photoelastic constants and the Brewster law for stressed tetragonal crystals

Abstract: An exact knowledge of the mechanical and optical properties of crystals allows not only for theoretical advances, but it is also a useful tool to asses crystal quality in the technological processes of growth and production of advanced crystals like, eg, scintillators. In this paper, we study the elasto‐optic behavior of tetragonal crystals to evaluate the photoelastic constants, associated to various states of stress, in terms of the components of the piezo‐optic tensor. Moreover, we arrive at a generalizatio… Show more

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Cited by 15 publications
(25 citation statements)
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“…The same issue was addressed in[Rinaldi et al 2018]; however, the results obtained there were related to specific cases of stress without the formal and more general treatment we give here; further, the treatment of cubic crystal was missing.…”
mentioning
confidence: 88%
“…The same issue was addressed in[Rinaldi et al 2018]; however, the results obtained there were related to specific cases of stress without the formal and more general treatment we give here; further, the treatment of cubic crystal was missing.…”
mentioning
confidence: 88%
“…In previous papers dedicated to the same problem [8,9], we obtained linear relations for n k (T) by a linearization procedure which involved the eigenvalues B k of B(T):…”
Section: Linearized Relationsmentioning
confidence: 99%
“…The typical solution of this problem is to first find the eigencouples (B k , u k ) of K(T), then take the square root of the inverse of (1.2) and, finally, if we need linearized relations, linearize the result about the unstressed state T = 0, like we did for instance in [8,9]. Such an approach has many limitations, since the possibility to find an explicit expression for the eigencouples (B k , u k ) (here u k is the eigenvector associated with B k ) depends heavily on the crystal symmetry trough M and on the stress tensor T: indeed, in [8,9] we considered a special state of stress. Moreover, for optically uniaxial materials the linearization about the unstressed state may not be well defined since the derivative of n k with respect to T may blow up for T → 0.…”
Section: Introductionmentioning
confidence: 99%
“…where ρ is the mean ray between the ordinary and the extraordinary one, λ is the wavelength of the impinging light, θ 1 , θ 2 are the angles formed by the ray and optic axes, respectively, and ∆ the phase difference between the ordinary and extraordinary rays. These patterns are due to the structure of the crystals and are based on the theory of the Bertin surfaces [22][23][24] (Equation (2)), which are the virtual iso-delay surfaces that the light generates when crossing the sample (Figure 1d,e). As a matter of fact, Bertin's surfaces are the bijective relation between the light direction angle with the optic axes and a point in space and can be expressed as [19,20]:…”
Section: Conoscopic Fringe Patterns and Their Interpretationmentioning
confidence: 99%