A Tale of Two Transitions: Unraveling Two Distinct Polymorph Transition Mechanisms in One n-Type Single Crystal for Dynamic Electronics

17 December 2021, Version 1
This content is a preprint and has not undergone peer review at the time of posting.

Abstract

Cooperativity is used by living systems to circumvent energetic and entropic barriers to yield highly efficient molecular processes. Cooperative structural transitions involve the simultaneous, concerted displacement of molecules in a crystalline material, in stark contrast to the more typical molecule-by-molecule nucleation and growth mechanism often breaking the single crystallinity. Cooperative transitions have acquired much attention in the research community for their low transition barriers, ultrafast kinetics, and structural reversibility. On the other hand, cooperative transitions are rarely observed in molecular crystals and the molecular origin is not well understood. Single crystals of 2-dimensional quinoidal terthiophene (2DQTT-o-B), a high-performance n-type organic semiconductor, demonstrate two thermally-activated, reversible phase transitions with one exhibiting a cooperative mechanism and the second exhibiting a nucleation and growth mechanism. In situ microscopy, single crystal and grazing incidence X-ray diffraction (GIXD), along with Raman spectroscopy suggest a reorientation of the alkyl side chains results in a cooperative transition behavior. On the other hand, the nucleation and growth transition is coincident with both side chain melting and the emergence of new spin-spin interactions between conjugated cores, confirmed through in situ electron paramagnetic resonance spectroscopy (EPR). This is the first observation of biradical interactions directly initiating a structural transition. Through studying these fundamental mechanisms, we establish alkyl chain conformation and disorder as integral to rationally controlling these polymorphic behaviors for novel electronic applications.

Keywords

Polymorphism
cooperativity
phase transition
biradical

Supplementary materials

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Supplementary Information
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Supplementary figures and description of Raman peak assignments.
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Movie_S1_I-II_Heating
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video showing the I-II heating transition under polarized optical microscopy
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Movie_S2_II-I_Cooling
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Video showing the II-I cooling transition under polarized optical microscopy
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Movie_S3_II-III_Heating
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Video showing the II-III Heating transition under polarized optical microscopy
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Movie_S4_III-II_Cooling
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Video showing the III-II cooling transition under polarized optical microscopy
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Movie_S5_II-I_Cooling_CrackFormation
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Video showing crack formation during the II-I cooling transition under polarized optical microscopy
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Movie_S6_Heating_thermosalient
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Video showing the thermosalient motion during the I-II transition
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Movie_S7_GIXD_I-II
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Video showing the changes in grazing incidence X-ray diffraction pattern during the I-II transition
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Movie_S8_Quinoidal_1581
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Simulation of the vibrational mode calculated in the quinoidal form Raman spectra at 1581 cm^-1
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Movie_S9_Quinoidal_1584
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Simulation of the vibrational mode calculated in the quinoidal form Raman spectra at 1584 cm^-1
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Movie_S10_Quinoidal_1636
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Simulation of the vibrational mode calculated in the quinoidal form Raman spectra at 1636cm^-1
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Movie_S11_Quinoidal_1878_COstretch
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Simulation of the vibrational mode calculated in the quinoidal form Raman spectra at 1878 cm^-1
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Movie_S12_Quinoidal_1610
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Simulation of the vibrational mode calculated in the quinoidal form Raman spectra at 1610 cm^-1
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Movie_S13_GIXD_II-III
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Video showing the changes in grazing incidence X-ray diffraction pattern during the II-III transition
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Movie_S14_AromaticNoCyano_1618
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Simulation of the vibrational mode calculated in the aromatic form Raman spectra at 1618 cm^-1
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Movie_S15_AromaticNoCyano_1635
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Simulation of the vibrational mode calculated in the aromatic form Raman spectra at 1635 cm^-1
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