A perturbative correction to the method of configuration interaction with single substitutions (CIS) is presented. This CIS(D) correction approximately introduces the effect of double substitutions which are absent in CIS excited states. CIS (D) is a secondorder perturbation expansion of the coupled-cluster excited state method, restricted to single and double substitutions, in a series in which CIS is zeroth order, and the first-order correction vanishes. CIS(D) excitation energies are size consistent and the calculational complexity scales with the fifth power of molecular size, akin to second-order Meller-Plesset theory for the ground state. Calculations on singlet excited states of ethylene, formaldehyde, acetaldehyde, butadiene and benzene show that CIS(D) is a uniform improvement over CIS. CIS (D) appears to be a promising method for examining excited states of large molecules, where more accurate methods are not feasible.
Single-chain antigen-binding proteins are novel recombinant polypeptides, composed of an antibody variable light-chain amino acid sequence (VL) tethered to a variable heavy-chain sequence (VH) by a designed peptide that links the carboxyl terminus of the VL sequence to the amino terminus of the VH sequence. These proteins have the same specificities and affinities for their antigens as the monoclonal antibodies whose VL and VH sequences were used to construct the recombinant genes that were expressed in Escherichia coli. Three of these proteins, one derived from the sequence for a monoclonal antibody to growth hormone and two derived from the sequences of two different monoclonal antibodies to fluorescein, were designed, constructed, synthesized, purified, and assayed. These proteins are expected to have significant advantages over monoclonal antibodies in a number of applications.
We have cloned, expressed, and characterized two naturally occurring variations of the IgG-binding domain of streptococcal protein G. The domain is a stable cooperative folding unit of 56 amino acids, which maintains a unique folded structure without disulfide cross-links or tight ligand binding. We have studied the thermodynamics of the unfolding reaction for the two versions of this domain, designated B1 and B2, which differ by six amino acids. They have denaturation temperatures of 87.5 degrees C and 79.4 degrees C, respectively at pH 5.4, as determined by differential scanning calorimetry. Thermodynamic state functions for the unfolding reaction (delta G, delta H, delta S, and delta Cp) have been determined and reveal several interesting insights into the behavior of very small proteins. First, though the B1 domain has a heat denaturation point close to 90 degrees C, it is not unusually stable at physiologically relevant temperatures (delta G = 25 kJ/mol at 37 degrees C). This behavior occurs because the stability profile (delta G vs temperature) is flat and shallow due to the small delta S and delta Cp for unfolding. Related to this point is the second observation that small changes in the free energy of unfolding of the B-domain due to mutation or change in solvent conditions lead to large shifts in the heat denaturation temperature. Third, the magnitude and relative contributions of hydrophobic vs nonhydrophobic forces (per amino acid residue) to the total free energy of folding of the B-domain are remarkably typical of other globular proteins of much larger size.
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