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    Effects of Chiral Dopants on Liquid

    Crystals in the Nematic Phase

    Kyle Troutman

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    Outline of Discussion

    Introduce liquid crystal science

    Explain the role ofchirality in liquid crystals

    Discuss the ability of various dopants to induce

    chiral phases in liquid crystal hosts

    Delve into the significance and development of

    optically switchable dopants

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    Liquid Crystals?

    Used in display devices

    LCD Televisions, digital watch displays, mood rings

    Biological liquid crystals

    Phospholipids in the plasma membrane

    Lyotropic liquid crystals

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    Discovery!

    First observed by an Austrian chemist, FriedrichReinitzer, in 1888

    The substance seemed to have two distinct meliting

    points

    cloudy, white liquid at 145.5 C

    transparent, clear liquid 178.5 C

    Molecular structure of

    Cholesteryl benzoate

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    Liquid Crystal Mesophase

    The liquid crystal state is between the solidand liquid phases

    Refered to as mesophase

    Display properties of both crystal and liquid

    Sensitive to temperature, electric andmagnetic fields, solvent, and dopant

    molecules Self-Assemble into unique supramolecular

    structures

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    Order Parameter S

    Mesogens align along a common axis called a

    director (n)

    Can align with directional or positionalorientation

    Describes different liquid crystal phases

    Degree of order expressed by parameter S

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    Temperature Effect on parameter S

    Tc = Clearing Temperature

    At temperature Tc

    substance loses all

    order

    Anisotropic liquid

    crystal becomes

    isotropic liquid

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    Liquid Crystal Classification

    Calamitic Discotic

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    Liquid Crystal Phases

    1. Nematic

    2. Smectic A

    3. Chiral Smectic or Smectic C

    4. Chiral Nematic or Cholesteric

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    Nematic Phase (N)

    Molecules exhibit long

    range orientational order

    Mesogen aligns long axis

    with a common director n

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    Smectic Phases

    In the smectic phases molecules flow freely

    within a layer and align with a director n

    In Smectic C* phase the molecules align at

    an angle to the normal z

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    Chirality

    A molecule can only be considered chiral if itlacks an axis of improper rotation

    Lacks an Sn axis

    Rotation by 360/n followed by a reflection perpendicular tothe axis of rotation

    Structure is non-superimposable on its mirrorimage

    Chirality can be induced upon a completelyachiral molecule

    Chirality transfer

    Supramolecular chirality

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    Chiral Nematic

    Also known as cholesteric phase or twisted

    nematic

    Molecules in this phase are chiral

    Helical change in orientation of the director

    Director has helical twist perpendicular to the

    long axis of helix Helical propagation of the director is non-

    superimposable on its mirror image

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    Chiral Nematic

    Pitch (p) is the

    distance in which thedirector rotates 360

    n

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    Doped Liquid Crystals

    Magnitude of cholestericpitch

    Sign of cholesteric pitch

    Right handed helix is

    positive (P)

    Left handed helix isnegative (M)

    P (+) M (-)

    Chiral dopant

    Chiral guest molecule is dissolved into a nematic

    host

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    The efficiency of a dopant to induce helicalorganization

    Helical twisting power ()

    The pitch is inversely proportional to:

    Concentration (c)

    Helical twisting power ()

    Enantiomeric excess (ee)

    Helical Twisting Power

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    Chirality Transfer

    Chirality is amplified and transferred throughout the whole system

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    Advantages of Doped LCs

    Doped liquid crystals have advantages over

    liquid crystals with chiral mesogens

    Pitch of helix is tunable by changing host-guest

    ratio

    Colors can be generated by a single dopant

    Host and dopant self assemble

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    Shape Persistent Dopants

    Mesogenic functionalism

    Chiral coordination complexes

    TADDOL and Dioxolane compounds

    Atropisomer-based dopants

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    Mesogenic Functionalism

    A chiral molecule is

    functionalized to liquid

    crystal mesogen

    Functionalization enhances

    solubility and molecularinteraction with LC host

    Chiral alcohol dopant

    Chiral alcohol attached to mesogen

    (R)-octan-2-ol

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    Amine Functionalization with

    Anthraquinone

    Intramolecular hydrogen bonding locks dopant

    conformation

    amine molecule

    Amine molecule attached to anthraquinone

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    Color test for enantiomeric excess

    High helical twisting power of 18 caused

    liquid crystal to reflect light in the

    visible range

    The color of the liquid crystal is

    dependent on the enantiomeric excess

    of the dopant

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    Chiral Coordination Complexes as

    Dopants

    Chirality of a coordination compound can be

    from chiral ligand or chiral metal center

    Chiral metal center can be (Dextro) or (Levo)

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    Metal coordination improves helical twisting

    power Reduced conformation flexibility

    Chiral propeller shape of metal complex

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    TADDOL and Dioxolane Dopants

    Tartaric acid

    derivative

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    TADDOL and Dioxolane Dopants

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    Methyl groups on 31 and silane bridge on 32

    prevent intramolecular hydrogen bondingbetween the diols

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    Helical twisting poweris greater in guest-hostcombinations wherearyl core distances are

    ofsimilar length

    -stacking interactionsbetween dopant and

    biphenyl LC core

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    - interactions

    Non-covalent intermolecular interaction

    Arise from a combination of van der Waals

    and electrostatic forces Forms supramolecular structure

    - interactions are still actively debated

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    - interactions

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    Proposed Dopant-Mesogen Interaction

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    Atropisomer Dopants

    Atropisomer considered chiral because

    rotation around bond is sterically restricted

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    Atropisomer Dopants

    If substitution at the 2 and 2 positions arecovalently or hydrogen bonded

    Cisoid conformation is preferred

    Substitution by large unlinked constituents Transoid conformation preferred

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    Atropisomer Dopants

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    Proposed model for chirality transfer between binaphthyl

    dopant and liquid crystal mesogen

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    Bistable Switchable Dopants

    Allows control of supramolecular chirality by

    external stimuli

    Can change helical: Sign

    Pitch length (p)

    Photochemical switchable dopants

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    Control of supramolecular chirality using

    external stimuli

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    Bistable Switchable Dopants

    External Stimuli

    pH

    Pressure

    Electric field

    Heat

    Magnetic field

    Light

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    Bistable Switchable Dopants

    Potential use as molecular switch Molecular equivalent of transistor

    Nanotechnology

    Light versus electricity Less heat produced

    Light more efficient and abundant

    Faster data processing

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    Optical Switches

    Type 1

    Dopant switches enantiomeric state by irradiation

    with circularly polarized light

    Switch between P and M helicities

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    Optical Switches

    Type 2

    Dopant switches between diastereomers

    Chirality of dopant is inversed

    Dopant states are not enantiomers

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    Optical Switches

    Type 3

    Switch and chiral auxiliary are separate units

    Chirality change is not as strong

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    Type 1 dopants: bicyclic ketones

    Circularly polarized light induces deracemization with

    enantiomeric excess of 0.4%

    Not strong enough to induce helical change due to low

    helical twisting power

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    Type 1 dopants: bicyclic ketones

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    Type 1 dopants: bicyclic ketones

    Mesogen resembling group incorporated that matches LC ZLI-

    1167 aided in solubility and helical twisting power 13 mol%

    racemic 83

    ZLI-1167 Liquid Crystal Host

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    Type 2 dopants: overcrowded alkenes

    2-(2,6-dimethylphenyl)-9-(2,3-dihydro-1H-naphtho[2,1-b]thiopyran-1-ylidene)-9H-thioxanthene

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    Type 2 dopants: flourene derived

    molecular motor

    High helical twisting power possibly due to structural similarity of dopant

    and biphenyl core of host mesogen

    Thermal isomerisation from unstable to stable form is possible at room

    temperature = allows for reversible color change

    Induces change in

    helical twist sign P-MRotar

    Axle

    Stator

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    Psuedoequatorial position with high

    steric strain

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    Flourene Molecular Motor

    MBBA could not be used as mesogen because

    it absorbs

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    Polygonal Surface Structure

    polyimide-coated glass surface

    Surface topography of polygonal nematic surface

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    Transition from 1a 1b

    White bar is 50 m

    E7 with 1 wt % of1a dopant

    Irradiated with 365 nm light

    Each square is 15 second interval

    Clockwise rotation

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    Thermal isomeration at 20 C

    Reaction half-life of 9.9 min in

    toluene

    P

    rotation

    1b 1c

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    Work created by molecular motor was used to move 5 X 28 m glass rod

    Photo chemical step 0.67 r.p.m. 1a 1b

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    Thermal step 0.22 r.p.m.1b 1c

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    X8 speed

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    Type 3 dopants: azobenzene derived

    molecular motor

    High helical twisting power

    allows for color switching

    UV light causes 73 to change

    helicity

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    Liquid crystals are self assembling molecules

    Have both crystalline and liquid properties

    Chiral dopants can be added to change from thenematic to the cholesteric phase

    Dopants vary in their ability to induce cholestericchange described by the helical twisting power ()

    Current research is focused on developing opticallyswitchable dopants with high helical twisting powers

    Switchable LCs could be used for nanotechnology, fasterdata processing, or molecular motors

    Conclusion

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    References

    1. Shri Singh. Liquid Crystal Fundamentals, Banaras Hindu University World Scientific PublishingCo. Pte. Ltd. 2002; 72, 43-49.

    2. Demus, D., Goodby, J. W., Gray, G. W., Spiess, H.-W., Vill, V., Eds. Handbook of Liquid CrystalsWiley-VCH:Weinheim, 1998; Vol. 2A, pp 3-23.

    3.Mioskowski, C.; Bourguignon, J.; Candau, S.; Solladie , G. Photochemically Induced CholestericNematic Transition in LiquidCrystals. Chem. Phys. Lett. 1996, 38, 456-459.

    4. I-Hsin Lin, Gary M. Koenig Jr., Juan J. de Pablo, Nicholas L. Abbott. Ordering of SolidMicroparticles at Liquid CrystalWater Interfaces. The Journal of Physical ChemistryB 2008 112 (51), 16552-16558

    5. Joon-Seo Park,, Sarah Teren,, William H. Tepp,, David J. Beebe,, Eric A. Johnson, and, Nicholas L.

    Abbott.,

    Formation ofOligopeptide-Based Polymeric Membranes at Interfaces betweenAqueous Phases and Thermotropic Liquid Crystals Chemistry of Materials 2006 18 (26), 6147-6151

    6. Siok Lian Lai, Shisheng Huang, Xinyan Bi, Kun-Lin Yang Optical Imaging of Surface-ImmobilizedOligonucleotide Probes on DNA Microarrays Using Liquid Crystals Langmuir2009 25 (1), 311-316

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    References

    Special thanks to research by Ben L. Feringa andRienk Eelkema at the University of Groningen,Netherlands

    Rienk Eelkema, Michael M. Pollard, Nathalie Katsonis, Javier Vicario, Dirk J. Broer,, and,

    Ben L. Feringa.

    Rotational ReorganizationofDoped Cholesteric Liquid Crystalline FilmsJournal of the American Chemical Society2006 128 (44), 14397-14407

    Rienk Eelkema and, Ben L. Feringa;Macroscopic Expressionofthe ChiralityofAmino

    Alcohols by a Double AmplificationMechanism in Liquid CrystallineMedia. Journal of

    the American Chemical Society2005 127(39), 13480-13481

    Eelkema R, Pollard M, Vicario J, et al.Molecular machines: Nanomotorrotatesmicroscaleobjects Nature [serial online]. March 09, 2006;440(7081):163-163.

    Alessandro Bosco, Mahthild G. M. Jongejan, Rienk Eelkema, Nathalie Katsonis,

    Emmanuelle Lacaze, Alberta Ferrarini, Ben L. Feringa. PhotoinducedReorganizationof

    Motor-Doped Chiral Liquid Crystals: BridgingMolecular Isomerization and Texture

    RotationJournal of the American Chemical Society2008 130 (44), 14615-14624