More than 6000 glycosidase sequences and related open reading frames are currently known. They have been classified into some 85 families based upon amino acid sequence similarities [1] providing a rich context in which to explore variations in glycosidase mechanism. Experimental demonstration of pyranoside ring conformations along the reaction pathway may assist the design of transition state analogues both as therapeutic agents and mechanistic probes. Here we report the three-dimensional structures of the Michaelis complex and covalent glycosyl ± enzyme intermediate for a family-26 b-mannanase, both of which display conformational features never previously seen on any glycosidase. When viewed in light of published work on mannosidase inhibition, this work suggests that the transition state for mannoside conditions to those described in Figure 4. These magnetic data are very similar to recent experimental results reported by other groups on complexes of Cu 2 dimers. [26] Theoretical fit using the BB model to the temperature-dependent molar susceptibility data in this case yields fit parameters J À 380 cm À1 and J' À 85 cm À1 . Clearly, the most striking feature is that the field-dependent magnetization does not display a hysteresis loop in this system, the straight line obtained being representative of a more traditional paramagnetic behavior.Our results dramatically underscore the potential afforded by supramolecular chemistry for the design of molecular nanostructured assemblies with desirable physical properties, while emphasizing how the composition of a material is not the only feature one must consider when designing a phase that exhibits molecular magnetism. Future work will focus on the modularity of this system and on chemical modification of the components: substituting the metal; changing the coordinated ligand; substituting the bdc ligand; incorporation of different guest molecules. We expect a significant effect on magnetic properties as it has already been shown that simply varying the apical coordinated ligand has a measurable effect on the magnetism exhibited by the SBU used in our study. Intensity data for 1 were collected at 173 K on a Bruker SMART-APEX diffractometer using Mo Ka radiation (l 0.7107 ä): Cu 6 C 123.08 H 54 N 9.37 O 30.73 , 2536.69 g mol À1 , trigonal, space group P3 ≈ c1, a b 18.6523(11), c 19.8313(18) ä, V 5975.1(7) ä 3 , Z 2, 1 calcd 1.410 g cm À3 , m 1.128 mm À1 , F(000) 2556, 2q max 50.08. Final residuals (for 265 parameters) were R1 0.0491 for 2112 reflections with I > 2sI, and R1 0.0764, wR2 0.1577, GoF 0.985 for all 3520 data. Residual electron density was 0.753 and À 0.574 e ä À3 . Highly disordered solvent molecules in the hexagonal channels were modeled as a group of variable-occupancy carbon atoms. CCDC-165791 contains the supplementary crystallographic