Photo-Bergman Cyclization of Cu Metalloenediynes
A R T I C L E S
analogues1
9-26
can be photochemically activated to generate
transfer (MLCT) absorption bands in the optical spectrum. These
transitions are derived from significant spatial overlap between
the metal dσ or dπ molecular orbitals and bound ligand σ or π
molecular orbitals. The presence of such absorption features,
however, does not mandate that the participating metal- or
ligand-centered orbitals be the highest occupied molecular
orbital (HOMO) or the lowest unoccupied molecular orbital
(LUMO) of the complex. These localized states can therefore
serve as pathways to reactive electronic configurations that do
not absorb photons in the ground state (e.g., long-range charge-
separated states) and, therefore, are not populated directly by
fully cyclized Bergman products upon UV excitation. Recently,
2
2
the kinetics and electronic structures of enediyne excited
2
7
states giving rise to the observed product distributions, have
been more clearly elucidated. The emerging theme for photo-
Bergman cyclization of simple organic enediyne ligands is that
photoexcitation leads to an alkyne-localized excited π-π* state
that promotes an in-plane geometric distortion, leading to the
Bergman-cyclized 1,4-phenyl diradical intermediate. In con-
trast, population of the lowest-energy π-π* state, which is
localized on the ene functionality, leads to the potential for an
out-of-plane geometric distortion via rotation about the double
bond and localization of unpaired electron density at the alkyne
termini. This leads to sites for H-atom abstraction and the
subsequent formation of dien-yne photoproducts.
1
2
7
3
4
4-46
optical excitation.
Conceptually, this could lead to new
design strategies that utilize MLCT absorption to initiate
Bergman cyclization with visible-region photons photochemi-
cally, which would relax the requirement for high-energy,
alkyne-localized electronic excitation to drive such reactions.
Beyond the excited-state mechanistic details of photoinitiated
Bergman cyclization, the ability of the potent 1,4-phenyl
diradical intermediate to perform DNA degradation via H-atom
abstraction rather than redox reactions gives these metalloene-
diynes potential advantages over other metal-activated thermal
or photochemical agents. Thermal and photochemical DNA
Binding of transition-metal ions to simple enediyne ligands
influences thermal Bergman cyclization temperatures by induc-
ing a geometry that approaches the transition-state structure,
28-41
thereby lowering the activation barrier to cycloaromatization.
However, the potential role of metal ions in photo-Bergman
cyclization reactivity has not been examined. It is well
established that photochemical activation of both σ- and π-bound
metal complexes can lead to ligand dissociation and/or pho-
toreduction reactions.42 In the case of simple organic enediynes,
ligand-centered redox chemistry does not lead to 1,6-Bergman
cyclization. Rather, 1,5-cyclization and subsequent ion-radical
reactions are observed.43 Thus, it is unclear at first glance how
transition metals, especially those that are redox active, may
participate in driving photoinduced Bergman cyclization.
4
7,48
cleavage
by transition-metal complexes frequently occurs
by one of three general mechanisms: (i) one-electron guanine
4
9,50
50-54
oxidation (e.g., Ni(II) peptide
and macrocycle
complex
2
-
55
56-58
reactions with KHSO5, Cr2O7 /H2O2, CuCl2/H2O2,
ReO (4-OMepy) , Ru(bpy)3
O2 ), (ii) oxygen-atom transfer oxidation (e.g., [Ru(IV)(tpy)-
bpy)O] , [Ru(III)(tpy)(bpy)OH] , ) and sugar degradation
+
59
3+ 60,61
3+
2
4
,
and [Co(NH3)6]
via
1
62
2+ 63
2+ 64
(
6
5
by H-atom abstraction (e.g., Fe(II)-bleomycin, Rh-phi com-
One electronic property that redox-active transition-metal
complexes exhibit is the presence of metal-to-ligand charge-
6
6
+
67
plexes, and [Cu(phen)2] complexes ). The most common
of these is nucleobase oxidation at G-sites that is due to the
relatively low redox potential for guanine oxidation, as well as
(
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