From elewars.,at,.alchemy.chem.utoronto.ca Wed Jun 15 22:26:20 1994 Received: from alchemy.chem.utoronto.ca for elewars-!at!-alchemy.chem.utoronto.ca by www.ccl.net (8.6.4/930601.1506) id WAA17907; Wed, 15 Jun 1994 22:20:58 -0400 Received: from localhost (elewars %-% at %-% localhost) by alchemy.chem.utoronto.ca (8.6.4/8.6.4) id WAA26081 for chemistry %-% at %-% ccl.net; Wed, 15 Jun 1994 22:20:20 -0400 Date: Wed, 15 Jun 1994 22:20:20 -0400 From: "E. Lewars" Message-Id: <199406160220.WAA26081 -8 at 8- alchemy.chem.utoronto.ca> To: chemistry -8 at 8- ccl.net Subject: C1 symmetry and minima Daniel Kost inquired about pesky imaginary freqs in optimized structures, even when these have C1 sym. It should perhaps be pointed out that there is no reason why a C1 structure has to be a minimum; it could be a first-order saddle point (a transition state), a higher-order saddle point (a mountain top), or not even a stationary point. Obviously the optimized structures he's gettin should be stationary points, and one imag. freq. pins them down as transition states. (Some TS's are "trivial" in that changing a torsional angle is essentially all that's needed to give a minimum). ===