Tight Electronic Coupling within Loosely Held Polyaromatic

Mechanical coupling is a viable alternative for electronic coupling in ... The orientation-dependent resonance energy transfer (RET) can be exploi...
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Tight Electronic Coupling within Loosely Held Polyaromatic Cavities: Tris(N-Salicylideneaniline)-Derived Ligands and Receptors Dongwhan Lee Department of Chemistry, Indiana University Bloomington [email protected]

Dynamic 2-D Conjugation

Long Range Conformational Transmission

Structural distortion of planar conjugated systems can modify the effective conjugation “area” sampled by electrons and excitons.

t − αi e τi

OH

(1)

Global helicity predetermined by local chirality residing on 2˚ alcohol groups.

(1)

#$

···



κ # kRET ∝ ΦD " FD(λ)εA(λ)λ4dλ κR2DA 6 0 τ D kRET ∝ ΦD J (λ) τD RDA 6 % & 2R −θDADA− 3cos J (λ)θDcos θA)2 kRET ∝κ2Kexp = (cos L " # κ2 kRET ∝ ΦD J (λ) τD RDA 6

Artificial systems displaying selfregulatory properties continue to remain an engaging challenge.

fl. intensity (a.u.)

n can be exploited as aβ[L] powerful θ= 2 signal amplification mechanism. 1 cos + β[L] θDA − 3cos θD θA)2n κ = (cos 2

Allosteric Switching

(2)

α2 = 0.03; 0.615 nsec " τ2 = # $ ∞ α1The = 0.97; nsec κτ12 = 0.160 orientation-dependent kRET α∝ = ΦD0.03; τ =6 0.608 nsec FD(λ)εA(λ)λ4dλ 2resonance τD R2DAenergy 0 transfer (RET)

"

OH Ph

KNF Model (sequential conformational transition)

τ1 = 0.170 nsec t τ2 = 0.615 nsec n − ! τ1 = 0.160 nsec τ αi e i I(t) = τ2 = 0.608 nsec

Signal-Amplifying i=1 β[L]n “Inverted Antenna” α1 = 0.97;θτ= 0.170 1= 1+ β[L]nnsec

OH

Ph

i=1

···

(2)

O

H O H

400

500

600

···

700

Wavelength (nm)

1

O + ne → R 1

···

α1 = 0.97; α2 = 0.03; α1 = 0.97; α2 = 0.03;

Ph

···

n !

OH

Mechanical coupling is a viable alternative for electronic coupling in long-range signal transmission.

···

I(t) =

Ph