Control of the torsional angles of nonrigid molecules is key for the development of emerging areas like molecular electronics and nanotechnology. Based on a rigorous calculation of the rotation-torsion-Stark energy levels of nonrigid biphenyl-like molecules, we show that, unlike previously believed, instantaneous rotation-torsion-Stark eigenstates of such molecules, interacting with a strong laser field, present a large degree of derealization in the torsional coordinate even for the lowest energy states. This is due to a strong coupling between overall rotation and torsion leading to a breakdown of the torsional alignment. Thus, adiabatic control of changes on the planarity of this kind of molecule is essentially impossible unless the temperature is on the order of a few Kelvin.Quantum control of molecular degrees of freedom is becoming an important field of research that promises important technological developments. In the last few years impressive progress on the control of molecular alignment and orientation has been achieved [1]. However, control of internal degrees of freedom remains in its infancy due, among other things, to the elusive character of intramolecular vibrational relaxation processes which are prevalent even in relatively small polyatomic molecules. Quantum control of a large amplitude torsional angle has been the subject of several recent investigations [2][3][4][5][6][7].Control of torsional angles is key for the development of new miniaturized communication systems based on energy transfer along molecular wires [2,3]. For example, it has been established that the rate of electron exchange in a ruthenium (Il)-osmium (II) binuclear complex depends on the conformation of a biphenyl bridge [4]. Ramakrishna and Seideman [5] showed that torsional control by an intense laser pulse should be achieved for several nonrigid molecules displaying internal rotation. In the case of biphenyl, using a model where the two phenyl rings can rotate about a fixed axis perpendicular to the direction along which the laser field is propagating, their calculation predicts that the two rings become localized in the same plane for a circularly polarized laser field of intensity around 10 10 W/cm 2 and temperatures up to 77 K. In their time dependent experiments, Madsen and co-workers [6,7] showed that for the similar 3, 5-difluoro-3', 5'-dibromobiphenyl molecule, torsional control of the internal rotation can be achieved using two laser pulses. The first pulse adiabatically aligns the C-C bond between the phenyl rings along its polarization axis. The second pulse imparts a kick to the molecule that is able to initiate torsional motion. These experimental results were corroborated [6,7] using a theoretical model analogous to that of Ref. [5].In conventional spectroscopic studies, large amplitude motions have been traditionally difficult to analyze due to the existence of strong couplings with the overall rotation and with other low-frequency vibrations [8]. Contrarily. dynamics approaches tend to neglect these coupli...