2016
DOI: 10.1002/chem.201503975
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A Puckered Singlet Cyclopentane‐1,3‐diyl: Detection of the Third Isomer in Homolysis

Abstract: In the photochemical denitrogenation of 1,4-diaryl-2,3-diazabicyclo[2.2.1]heptane (AZ6) bearing sterically hindered substituents, a curious new absorption band at about 450 nm was observed under low-temperature matrix conditions, together with the previously well-characterized planar singlet diradical pl-(1) DR6 with λmax =≈580 nm. The 450 nm species was electron paramagnetic resonance (EPR)-silent. Instead of generating the planar diradical pl-(1) DR6 and the precursor azoalkane AZ6 upon warming, the ring-clo… Show more

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Cited by 11 publications
(20 citation statements)
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“…The higher level of theory at CAS(2,2)+DDCI3/6-31G(d) more precisely reproduced the electronic transition of HOMO (ψ S,3b ) to LUMO (ψ A,3b ) in CP3b, 23 in which 581 nm was computed for the first ππ* electronic transition in the π-single bonding (Figure 7a). The molar extinction coefficient (¾) of CP3b at 571 nm was experimentally determined to be ca.…”
Section: ¹1mentioning
confidence: 74%
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“…The higher level of theory at CAS(2,2)+DDCI3/6-31G(d) more precisely reproduced the electronic transition of HOMO (ψ S,3b ) to LUMO (ψ A,3b ) in CP3b, 23 in which 581 nm was computed for the first ππ* electronic transition in the π-single bonding (Figure 7a). The molar extinction coefficient (¾) of CP3b at 571 nm was experimentally determined to be ca.…”
Section: ¹1mentioning
confidence: 74%
“…25 The bond order of C1C3 was determined to be 0.37 by using the computed electron occupation numbers in ψ S (1.37) and ψ A (0.63) at the (2/2)CASSCF/6-31G(d) level of theory for CP3b. 23 The blue-shifted absorption maximum was observed at 514 nm for CP3c (X = O(CH 2 ) 2 O) with the cyclic acetal moiety (Figure 7b), demonstrating a larger HOMOLUMO energy gap and higher π-bonding character in CP3c compared with CP3b because of the spiroconjugation (Figure 7b). …”
Section: ¹1mentioning
confidence: 99%
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“…The first minimum energy state CP1 a* corresponds to the experimentally observed short‐wavelength emission state (Figure A). Interestingly, the second minimum energy structure that shows a long‐wavelength emission (calcd 480 nm) was found to possess a longer d (C 1 −C 2 ) distance of 2.332 Å with a puckered structure, puc‐ 1 DR1 a* (entry 3, θ CP1 =32.7°, and θ CP2 =20.7°). The puc‐ 1 DR1 a* species should be the emissive species at long wavelengths (exptl 515 nm, Figure A).…”
Section: Methodsmentioning
confidence: 99%
“…Figure 2s hows the:a )excited state PES of CP1 a;b )four selected dihedral angles, q Ph1 , q Ph2 , q CP1 ,a nd q CP2 ;a nd c) two selected bond lengths, d(C 1 ÀC 5 )a nd d(C 2 ÀC 8 ). Interestingly,t he second minimum energy structure that shows al ong-wavelength emission (calcd 480 nm) was found to possess al onger d(C 1 ÀC 2 )d istance of 2.332 with a puckered structure, [27,28] puc-1 DR1 a* (entry 3, q CP1 = 32.78,a nd q CP2 = 20.78). Figure 2a shows that CP1 a has two minimum energy states on the PES in the S 1 state.…”
mentioning
confidence: 99%