The prospects of all known noncentrosymmetric alkali and/or alkaline earth beryllium borates for nonlinear optical (NLO) generation in the deep-ultraviolet (DUV) spectral region are evaluated by first-principles studies. It is shown that all these crystals possess large enough energy band gaps and relatively strong NLO responses that satisfy the requirement for DUV second-harmonic generation (SHG). However, the practical DUV SHG capabilities of these crystals are mostly limited by the phase-matching condition, as determined not only by the optical birefringence but also by the refractive-index dispersion that is explicitly emphasized for the first time in this work. Therefore, although the K 2 Be 2 BO 3 F family and NaBeB 3 O 6 both have a large birefringence, Δn ≈ 0.08, at a wavelength of 400 nm, the DUV SHG lasers can only be produced in the former but cannot be fulfilled in the latter due to its large refractive-index dispersion in the DUV region. The crystal structural features for large birefringence and the electronic structure origins for different refractive-index dispersion behaviors are discussed. The elucidation of the structure−property relationship presents a useful guide to the exploration of new NLO crystals that can be practically applied for DUV SHG. KEYWORDS: alkali and/or alkaline earth beryllium borates, deep ultraviolet nonlinear optical, phase-matching condition, birefringence, refractive-index dispersion T he demand for deep-ultraviolet (DUV, wavelength λ < 200 nm) coherent light becomes increasingly urgent, owing to its great application in many scientific and technical fields, such as in microcircuit photolithography, high density storage, laser micromachining, and high-precision scientific equipment. 1−5 Up to now, the most effective method to produce DUV lasers with high quality is from all-solid-state lasers using cascaded frequency conversion by DUV nonlinear optical (NLO) crystals. 6−9 The search for new NLO crystals for the DUV spectral region is one of the research hot spots in optoelectronic functional materials. 10−15 It is commonly accepted that the following conditions of optical properties are vital for the DUV NLO performance of a crystal: 16,17 (i) a short-wavelength absorption cutoff (λ cutoff ) of less than 200 nm (i.e., an energy band gap E g > 6.2 eV) for good optical transmission in the DUV region (also corresponding to a large laser damage threshold 18 ); (ii) a relatively large second-harmonic-generation (SHG) response (usually the effective SHG effect should be larger than that of KH 2 PO 4 (KDP, d 36 = 0.39 pm/V)) for a high NLO conversion efficiency, and (iii) a moderate birefringence (Δn should be larger than 0.075 but smaller than 0.11 at a wavelength of 400 nm) for the achievement of the phase-matching condition in the DUV region.For decades, the exploration of DUV NLO crystals has been focused on the noncentrosymmetric alkali and/or alkaline earth beryllium borates, 7−17 mainly due to their very short absorption edges and relatively large NLO effects. In the ...