Introduction to Solid State Physics for Materials Engineers. Emil Zolotoyabko

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СКАЧАТЬ alt="upper J Subscript i Baseline equals rho Subscript italic i k Baseline normal script upper E Subscript k"/>

      There are two important field tensors of second rank, which are in common use. These are the stress and strain tensors. Stress tensor, σ_ik, connects vector of external force, F_i, applied to a certain crystal area, ΔS, and unit vector, , normal to this area:

(1.11)

Based on the mechanical equilibrium of the stressed solid, it is possible to prove that stress tensor (Eq. (1.11)) is symmetric one, i.e. σ_ik = σ_ki. Regarding strain tensor, it connects the deformation vector, u_i, in the vicinity of a given point and the radius-vector of this point, x_i. Deformation vector determines the difference in the distances between closely located points near x_i in the deformed and non-deformed states of the crystal. To provide local information on the deformed state, strain tensor, e_ik, is defined in the differential form:

(1.12)

Evidently, the strain tensor, defined by Eq. (1.12), is symmetric one, i.e. e_ik = e_ki.

      Furthermore, inter-atomic distances within a crystal are also changed upon heating (see Chapter 3). In that sense, a crystal heated up to some temperature, T₁, is in different “deformation” state as compared with its initial state at temperature, T₀. Thus produced relative change in lattice parameters is mathematically equivalent to strain (Eq. (1.12)). Tensor of second rank, which relates e_ik to the temperature increase, ΔT = T₁ − T₀ (tensor of rank zero, i.e. scalar), is called as tensor of linear expansion coefficients, α_ik:

      (1.13)

      Note that both crystal states, at T = T₀ and T = T_1, are thermodynamically equilibrium states at respective temperatures, and, therefore, no elastic energy is stored in such “deformed crystal,” whenever the temperature change is homogeneous across the crystal. The only energy difference between these two states is in free energy, which is temperature dependent.

      Tensor of second rank may also connect a scalar and two vectors, as tensor of dielectric permittivity, ℰ_ik, does for energy density, W_e, of electromagnetic field within a crystal:

      (1.14)

By using tensor representation for the electric displacement field (see Eq. (1.9)), we find that the energy density is quadratic with respect to the applied electric field, ℰ_i.

Tensor of third rank has three indices i, k, l = 1, 2, 3. It connects tensor of second rank and vector, e.g. stress, σ_ik, and induced electric polarization, P_i:

      (1.15)

      as for direct piezoelectric effect, or strain, e_ik, and applied electric field, ℰ_i:

      (1.16)

      for converse piezoelectric effect, both discussed in detail in Chapter 12. Another example is tensor, r_lik, of the linear electro-optic effect (the Pockels effect, also mentioned in Chapter 12). This tensor of third rank connects the change, Δn_ik, of refractive index, n, (which can be described in terms of the second rank tensor) under applied electric field, with the electric field vector, ℰ_l:

      (1.17)

      For the fourth rank tensor, there are several optional ways for its construction. It may connect two tensors of rank 2, e.g. stress, σ_ik, and strain, e_lm, as the stiffness tensor, C_iklm (tensor of elastic modules used in Chapter 3), does:

(1.18)

      Similar tensor object, π_iklm, is used to describe the photo-elastic effect in crystals, which provides the change of refractive index under applied stress:

      (1.19)

      Another possibility is to connect tensor of second rank (e.g. strain tensor, e_ik) and two vectors (e.g. quadratic form of electric field, ℰ_l ℰ_m) as for electrostriction effect, g_iklm:

(1.20)

      or changes in refractive index, as a function of quadratic form of electric filed, as for quadratic electro-optic effect, r_iklm (see СКАЧАТЬ