2016
DOI: 10.1021/acs.jpcb.6b04811
|View full text |Cite
|
Sign up to set email alerts
|

Interaction of a Julolidine-Based Neutral Ultrafast Molecular Rotor with Natural DNA: Spectroscopic and Molecular Docking Studies

Abstract: Ultrafast molecular rotors (UMRs) are reported to be one of the best fluorescent sensors to study different microenvironments, including biomolecules. In the present work, we have explored the possibility of application of a julolidine-based neutral UMR, 9-(2,2-dicyano vinyl) julolidine (DCVJ), as a DNA sensor and studied its mode of binding with DNA in detail using spectroscopic and molecular docking techniques. Our spectroscopic studies indicate that association of DCVJ with DNA leads to a very large enhance… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
4
1

Citation Types

2
17
0

Year Published

2019
2019
2023
2023

Publication Types

Select...
6
1

Relationship

1
6

Authors

Journals

citations
Cited by 20 publications
(19 citation statements)
references
References 83 publications
2
17
0
Order By: Relevance
“…The protonated form of CRYP shows a relatively shorter lifetime of 1.69 ns after excitation at 375 nm. ,, The interaction of the drug with RNA is characterized by a biexponential decay in which the short (major) component closely resembles the lifetime of the unbound drug along with a longer (minor) component reflecting the contribution from the bound counterpart of the drug molecules. It is also noted that with increasing RNA concentration, the amplitude of the longer lifetime component gradually increases with a concomitant decrease of the amplitude of the shorter component, which in turn corresponds to a gradually increasing fraction of bound drug molecules. The fluorescence quantum yield (Φ f ) of CRYP has been estimated with respect to the standard quantum yield of flavin adenine dinucleotide (FAD) in aqueous medium (Φ f = 0.03) and is found to be in good agreement with the reported literature . The radiative ( k r ) and nonradiative ( k nr ) decay rate constants were then calculated according to the standard equations: k r = Φ f / τ avg and k nr = 1/ τ avg – k r .…”
Section: Interaction Of Cryp With Rnasupporting
confidence: 81%
“…The protonated form of CRYP shows a relatively shorter lifetime of 1.69 ns after excitation at 375 nm. ,, The interaction of the drug with RNA is characterized by a biexponential decay in which the short (major) component closely resembles the lifetime of the unbound drug along with a longer (minor) component reflecting the contribution from the bound counterpart of the drug molecules. It is also noted that with increasing RNA concentration, the amplitude of the longer lifetime component gradually increases with a concomitant decrease of the amplitude of the shorter component, which in turn corresponds to a gradually increasing fraction of bound drug molecules. The fluorescence quantum yield (Φ f ) of CRYP has been estimated with respect to the standard quantum yield of flavin adenine dinucleotide (FAD) in aqueous medium (Φ f = 0.03) and is found to be in good agreement with the reported literature . The radiative ( k r ) and nonradiative ( k nr ) decay rate constants were then calculated according to the standard equations: k r = Φ f / τ avg and k nr = 1/ τ avg – k r .…”
Section: Interaction Of Cryp With Rnasupporting
confidence: 81%
“…27,28 Ion-dipole interactions represent another attractive force (electrostatic attraction between an ion and a neutral dipolar molecule), 29,30 where the more substantial interaction strengths (20-200 kJ mol −1 ) are known to significantly contributes to the self-assembly of biological macromolecules such as DNA and proteins. [31][32][33][34] Mimicking the structure of the biological iondipole interactions (and their functions) in polyelectrolyte will potentially yield AEMs containing highly ordered morphologies. As AEMs contain high concentration of cationic sites, incorporation of additional polar segments (containing centrally distributed dipoles) onto the polymer backbones will facilitate cation-dipole interactions, which is expected to regulate the self-assembled morphology of the resulting AEMs.…”
Section: Introductionmentioning
confidence: 99%
“…For example, hydrogen bonding and π − π stacking commonly have interaction strengths of 5–60 kJ mol −1 and 0–50 kJ mol −1 , respectively 27,28 . Ion‐dipole interactions represent another attractive force (electrostatic attraction between an ion and a neutral dipolar molecule), 29,30 where the more substantial interaction strengths (20–200 kJ mol −1 ) are known to significantly contributes to the self‐assembly of biological macromolecules such as DNA and proteins 31‐34 . Mimicking the structure of the biological ion‐dipole interactions (and their functions) in polyelectrolyte will potentially yield AEMs containing highly ordered morphologies.…”
Section: Introductionmentioning
confidence: 99%
“…Some examples include the use of julolidines as probes for measurement of blood viscosity, to photoinduced releasing of neurotransmitter amino acids, and as bio‐image (e.g. DNA, RNA, lysosome, and mitochondrial images) sensors …”
Section: Introductionmentioning
confidence: 99%