Organic Letters
Letter
precipitant and DNA. The best crystal obtained was a rod-
shaped specimen (Figure 1A) grown under 0.08 M NaCl, 0.02
regular Watson−Crick base pairs, including the modified L-
type U :A pair (Figure 1D). These data indicate that the
F
M MgCl , 0.04 M sodium cacodylate trihydrate pH 5.5, 35%
fluoro-modification does not generate local and overall
structural perturbation to the left-handed duplex. Moreover,
the high-resolution reveals that the 2′-F-ribose displays the L-
type C3′-endo pucker conformation (Figure 1E), consistent
with the native D-type 2′-F nucleic acid structure.
2
(
v/v) MPD, 0.002 M hexammine cobalt(III) chloride.
Notably, the crystal showed a strong X-ray diffraction to 1.03
Å during data collection. Due to the limited number of
published L-nucleic acid crystal structures as a model, we first
intended to solve this novel fluoro-modified L-DNA structure
by Single-wavelength Anomalous Diffraction (SAD). After
soaking the optimal crystals in the iridium(III) hexamine
chloride solution, although the strong iridium anomalous
signal was observed during data collection and data processing,
our attempts to search for Ir3 heavy atoms with high
occupancy and build helical model failed.
In summary, we have synthesized the L-type uridine
monomer containing 2′-F-modification, as the analogue of L-
uridine and mirror reflection of native 2′-F-uridine. Sub-
sequently, we successfully incorporated the residue into L-DNA
and L-RNA in quantitative yield. Our systematic thermal study
and enzymatic assessment reveal that the fluoro-L-oligonucleo-
tides have notable stability. The CD experiment results validate
that the fluoro-modified L-type DNA and RNA adopt the left-
handed helical conformations, which present the mirror-image
characteristics of their D-type counterparts. Furthermore, our
+
We then turned to the data collected from the unsoaked
crystal and performed molecular replacement. We utilized a
published D-DNA structure containing the same sequence
2
3
(
PDB 1d79 ) and transformed the coordinates into its mirror-
X-ray crystal structure of oligo L-5′-GU GTACAC-3′ is the
F
image reflection across the x axis. Using the created L-DNA as
the search model, we successfully obtained the solution and
determined the structure (PDB 7KW4) using Phaser in the
first structure of chemically modified L-nucleic acid. The
atomic level resolution allows us to examine the structural
insights into the modified A-form L-DNA. Indeed, the modified
L-DNA presents great structural stability, as evidenced by the
overall and local parameters in the L-helix. Although the L-type
2′-F-uridine monomer and its oligonucleotide have been
2
4
CCP4 suite. The space group was assigned as hexagonal
P6 22, with one single strand in an asymmetric unit. After
5
establishing the structure, we re-examined the data from the
3+
25
crystal soaked with Ir . We successfully solved the structure by
molecular replacement, but could not assign any obvious
pioneered before, our study here for the first time
comprehensively demonstrates its superiority and provides
the structural foundation. Therefore, these findings will
provide the theoretical framework for the L-nucleic acid
therapy design where thermostability is important, including
the L-aptamer for disease treatment, L-nanoparticle for drug
delivery, and L-molecular beacon for diagnosis.
3+
electron density belonging to Ir . It seemed that the observed
intense anomalous signal was either from the disordered heavy
atoms, which weakly and nonspecifically bound to L-DNA, or
3
+
from the Ir only adhering to the surface of the crystal. The
possible reasons for our failure likely include the compact
molecular packing inside crystal to inhibit molecular diffusion
or the hexamine iridium(III) chloride only binding to weak
G:U wobble pair.
ASSOCIATED CONTENT
Supporting Information
■
*
sı
As a reflection of the native D-type DNA octamer, our L-
DNA duplex adopts a left-handed A-form conformation. The
structural features of the L-helical geometry resemble those in
the native A-form duplex (Table 2). The base pairs in our L-
Experimental procedures, NMR characterization data
and LC-MS characterizations for all new compounds,
LC-Q-ToF characterizations, melting temperature meas-
urement, serum digestion analysis, circular dichroism
synthetic oligonucleotides (PDF)
Table 2. Average Helical Parameters for L- and D-Nucleic
Acids 8-mer
L-5′-GU GTACAC-3′
D-5′-GTGTACAC-3′ (1d79)
F
Rise (Å)
3.10
3.17
Accession Codes
Roll (deg)
Slide (Å)
Tilt (deg)
Shift (Å)
Twist (deg)
7.12
−1.13
5.22
0.39
−33.02
6.91
−1.15
5.46
0.43
31.98
Atomic coordinates and structure factors for the reported
crystal structures have been deposited with the Protein Data
bank under accession code 7KW4.
Corresponding Author
■
helical duplex has an average stepwise rise of 3.10 Å, roll angel
of 7.12°, slide of −1.13 Å, tilt of 5.22°, and shift of 0.39 Å. The
average base pair twist is −33.02°. All the helical parameters
are close to those of its native counterpart D-DNA, except for
the average twist of base pairs in the opposite direction. All
eight L-ribose rings present the C3′-endo or C3′-endo-2′-exo
conformations. The entire structure represents the mirror
reflection of native D-DNA crystal structure (Figure 1B). We
transformed the published structure of D-5′-GTGTACAC-3′
Wen Zhang − Department of Biochemistry and Molecular
Authors
Yuliya Dantsu − Department of Biochemistry and Molecular
Biology, Indiana University School of Medicine, Indianapolis,
Indiana 46202, United States
(
PDB 1d79) into its mirror reflection and superimposed it with
our determined L-8-mer structure. The two structures are
highly superimposable, and the r.m.s. deviations between them
are 0.088 Å (Figure 1C). The L-DNA duplex contains eight
Ying Zhang − Department of Biochemistry and Molecular
Biology, Indiana University School of Medicine, Indianapolis,
Indiana 46202, United States
5
010
Org. Lett. 2021, 23, 5007−5011