We present a combined experimental /theoretical study of the electronic properties of conjugated paraphenylene type molecules under high pressure up to 80 kbar. Pressure is used as a tool to vary the molecular geometry and intermolecular interaction. The influence of the latter two on singlet and triplet excitons as well as polarons is monitored via optical spectroscopy. We have performed band structure calculations for the planar poly( para-phenylene) and calculated the dielectric function. By varying the intermolecular distances and the length of the polymer repeat unit the observed pressure effects can be explained. PACS numbers: 78.66.Qn, 31.50. + w, 71.38. + i Conjugated polymers are ideal candidates for electroluminescent devices [1] which require certain electronic properties in terms of charge and energy transport as well as photon emission. Isolated conjugated molecules are low dimensional electronic systems. However, in the solid state, the electronic properties depend on threedimensional interactions [2,3]. These interactions lead to completely new transitions due to collective states such as aggregates [2] or to shifts of the energy levels of single molecules due to changes in the molecular geometry [4].The focus of this study is the influence of molecular geometry and intermolecular interaction on the electronic properties of films of methylated laddertype poly(paraphenylene) (m-LPPP) [5]-a material of very low defect content [6], used for blue and white light emitting devices [7]. The small inhomogeneous broadening in m-LPPP makes the electronic spectra easily detectable fingerprints for the involved states.A diamond anvil cell was used for hydrostatic pressure studies [8,9]. The photomodulation spectra were taken in an optical access cryostat at 80 K. The 457.9 nm line of an Ar-ion laser was the pump beam, modulated by a mechanical chopper. A halogen lamp was used for the probe beam, which passed through the sample and was then dispersed by a SPEX 1702 single stage monochromator to be detected by photovoltaic detectors with builtin preamplifiers. The small changes DT in transmission were picked up by a lock-in amplifier referenced to the chopper. All photomodulation spectra are DT divided by the transmission T . In Fig. 1 we show the electronic states and transitions in conjugated molecules. Absorption of light occurs via creation of a singlet excited state S 1 , as well as phonons. After photoexcitation, deexcitation occurs via several mechanisms: Nonradiative recombination (NR) leading to a depopulation of S 1 via creation of phonons; radiative recombination of S 1 leading to photoluminescence (PL); population of the lowest lying triplet state T 1 via intersystem crossing (ISC) from S 1 , which can be probed by T 1 ! T N triplet-triplet absorption (TT); dissociation of the S 1 ( bound electron-hole pair) into a free electron hole pair, which creates one positive and one negative polaron, giving rise to intrapolaron absorption (P). Population of triplet and polaron states leads to a small depo...