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6.3ChargeTransportCalculations
The increase of transmission inDry1 systems canbe explained in termsof theCT
parameters. The EC increase for all Dry1 and some of the Dry2 systems, while
other characteristics like the fluctuations of the IP remain the same. Starting at
the microhydration level Dry2, the structural disorder makes the calculations of
transmission impracticable.
TheLandauer–Büttiker calculationsasperformed in thisworkwereused toobtain
a simple indicator of the molecular conductivity. Basically, the calculated trans-
missions represent a measure of structural and dynamical disorder of the linear
conducting chain, assuming coherent transport. This assumes thatCToccurs in a
single-step fashion, i.e. a hopping picture of transport is excluded. The fact that
this approximation does not capture the CT in DNA fully and that the time or-
der of conformations (the true time dependence of CT parameters) does play a
role, has been shown recently by using the time series of CT parameters as de-
scribed above.[128] Still, even this improved description neglects the polarization
of environment, its response toCTand the effect onCTenergetics. Therefore, the
Landauer transmissions described above aswell as the improved time-dependent
treatment in Ref. 128 are both merely indicative. A hopping picture would also
have to involve on a more systematic footing the effect of environmental polar-
ization,which canbequantifiedbymeansof (outer-sphere) reorganization energy
(RE), oneof the crucial parameters inMarcus’ theoryof electron transfer (see also
chapter 2.6.1).[71, 85] RE is the energy required to transform the structure of the
donorandacceptormoleculesaswell asof theenvironment fromthat correspond-
ing to the initial charge state α to that of the final state β (after the transfer has
taken place). The RE of the solvent represents themajor contribution to the acti-
vation energy for CT and is a decisive factor determining the efficiency of CT in
systems immersed inapolarizablemedium;aqueoussolution isa typical example.
Detailed information onhow to calculate theREofDNAwithMDsimulations is
given in the lastpart of chapter2.6.1
The values of RE for the fully hydrated system are in accordance with previous
works.Withthedescribedapproachtheλs forCTinDNAwerefoundtobe1.21eV
for aadenine–adenineCTevent and1.41 eV for aguanine–guanineCTevent. [93]
Interestingly, nearly identical valueswere obtained for theDry1 system,with the
difference smaller than 0.1 eV, see Fig. 6.4. In Dry2, the spread of the obtained
values is huge due to structural distortions, and so the larger RE observed for
85
Charge Transport in DNA
Insights from Simulations
- Title
- Charge Transport in DNA
- Subtitle
- Insights from Simulations
- Author
- Mario Wolter
- Publisher
- KIT Scientific Publishing
- Date
- 2013
- Language
- English
- License
- CC BY-SA 3.0
- ISBN
- 978-3-7315-0082-7
- Size
- 17.0 x 24.0 cm
- Pages
- 156
- Keywords
- Charge Transport, Charge Transfer, DNA, Molecular Dynamics, Quantum Mechanics
- Categories
- Naturwissenschaften Chemie
Table of contents
- Zusammenfassung 1
- Summary 3
- 1 Introduction 5
- 2 TheoreticalBackground 11
- 3 SimulationSetup 39
- 4 DNAUnderExperimentalConditions 49
- 5 ChargeTransport inStretchedDNA 69
- 6 ChargeTransport inMicrohydratedDNA 79
- 7 AParametrizedModel toSimulateCT inDNA 89
- 8 Conclusion 105
- Appendix 111
- A DNAUnderExperimentalConditions 111
- B CTinMicrohydratedDNA 117
- List ofPublications 137