Electronic Detection of DNA-nicks Using 2D Solid-state Nanopore - - PowerPoint PPT Presentation
Electronic Detection of DNA-nicks Using 2D Solid-state Nanopore - - PowerPoint PPT Presentation
Electronic Detection of DNA-nicks Using 2D Solid-state Nanopore Transistor I use Blue Waters to devise novel 2D nanopore systems for genetic and epigenetic detection Presented by Nagendra Athreya PI: Jean-Pierre Leburton DNA: The Blue Print of
DNA: The Blue Print of Life
2
Tonna, Stephen, Assam El-Osta, Mark E. Cooper, and Chris Tikellis. Nature Reviews Nephrology (2010)
Applications of Decoding the Genome
Personalized Medicine Pharmaceutical Research
Point-of-care Genomic Testing
Nelson MR et. al., Nature Genetics, 47(8):856-60. 2015
3
Sequencing Technologies
New target < $100
Nanopore Sequencing is a potential solution
Illumina Sequencer
4
Principle of Nanopore Sensing
- δI: Average amplitude
- td : Dwell time
- δt: Waiting time between two events
Wanunu, M. (2012, June). Physics of Life Reviews.
Biological Nanopores Solid-state Nanopores
Oxford Nanopore Technologies
5
Towards Electronic Detection of Bio-molecules
Image Courtesy: Bayley, Nature, 467,164-65, 2010
Previous Work
Radenovic Group, EPFL, 2013
1. Tunable sensitivity of detection. 2. Easily integrated into semiconductor 3. Massively parallel detection.
Sheet Current
Leburton Group, UIUC, 2013
6
Modeling Ionic Currents using BW Nodes
System Model Molecular Dynamics Simulation (NAMD) DNA Trajectory Ionic Current
MD System Setup
summed over all K+, Cl- ions
Ionic Current Calculations
- A. Aksimentiev, et. al, Biophysical Journal, 2004
- ~500k atoms
- 5-10 Nodes/simulation
- 2-4 weeks/simulation
2
Electrostatics of nanopore system
7
Modeling Electronic Sheet Currents using BW Nodes
DNA Trajectory Self-Consistent Poisson Equation Solver Potentials induced around pore Electronic Transport Calculations using Non-Equilibrium Green’s Function Formalism/Boltzmann transport Electron Current/Conductance
DNA charge model Transverse Electronic Current Response
- Poisson Solver
- 50 Nodes/simulation
- ~6 hours/job
- Electronic Transport
- ~4000 Nodes!!!
- ~6 hours/job
DNA-nick Detection in 2D Nanopore Membranes
8
- Human Cell is subjected to ~70,000 lesions/day. Majority of them
arise from DNA backbone breaks.
- These breaks in critical gene cause the cell to undergo apoptosis.
- Contrarily, if repair mechanism fails, the DNA breaks cause
chromosomal instability leading to tumorigenesis.
- No existing technology can efficiently detect these DNA-nicks.
- Our efforts are directed towards unraveling the potential of Two-
dimensional solid-state nanopore membranes to detect and map these site-specific nicks along the genome with single-base resolution.
Site of the nick: A-A
9
Potential Profile of Damaged dsDNA translocation
SITE OF THE DNA DAMAGE CURRENT TRACES
T-T C-C G-G
Site Specificity of the nick positions
10
Not recognizable by ionic currents
Voltage (Vcis-Trans) dependence
11
Normal translocation Denaturing of the DNA
Voltage (Vcis-Trans) dependence
12
Breaking point!
13
Future Work
§ Cross-base pairs (A-C, A-G, A-T, C-G, C-T, T-G)
§ Different electrically active 2D materials: § Complete voltage dependence analysis
Semi-conductor (MoS2)
14
ACKNOWLEDGEMENTS
Jean-Pierre Leburton & Aditya Sarathy Olgica Milenkovic
THANK YOU
15
Appendix
16
17
Multigrid Solution of Semiconductor PBE
FMV cycle
Multigrid gives O(N) performance
𝛼 · ) 𝜁(𝐬)𝛼𝜒(𝐬 = −𝑓 ) 𝐿,(𝐬, 𝜒) − 𝐷𝑚0(𝐬, 𝜒 − 𝜍234 − 𝜍56 𝐿,(𝐬, 𝜒) = 𝐷7𝑓
089 :;<
𝐷𝑚0(𝐬, 𝜒) = 𝐷7𝑓
89 :;<
] 𝜍56(𝐬) = 𝑓[𝑂2
,(𝐬) − 𝑂 4 0(𝐬) + 𝑞(𝐬) − 𝑜(𝐬)
𝑞(𝐬) = 𝑂C 2 𝜌 𝐺 ⁄
H I
−𝑓𝜒(𝐬) − 𝐹K 𝑙M𝑈 𝑜(𝐬) = 𝑂6 2 𝜌 𝐺 ⁄
H I
𝐹K + 𝑓𝜒(𝐬) + 𝐹OPQ 𝑙M𝑢 Half Order Fermi-Dirac Function Need to solve 3D Poisson Boltzmann Equation with Newton Multigrid
Gracheva, Maria E., et al. "Simulation of the electric response of DNA translocation through a semiconductor nanopore–capacitor." Nanotechnology17.3 (2006): 622.
18
Graphene Nanopore Sheet Conductance Model
Graphene honeycomb lattice Tight-binding Hamiltonian Non-Equilibrium Green’s Function Landauer-Buttiker Formula
Conductance
- A. Girdhar, C. Sathe, K. Schulten, and J. P. Leburton PNAS (2013)
19
Graphene Nanoribbon Transverse Conductance
Non-equilibrium Green's function (NEGF)
G: Transverse conductance of the sheet; T(E): Transmission coefficient
f(E): Fermi-Dirac distribution
Conductance (G) Fermi Energy (eV)
Transmission T(E) Carrier Energy (eV)
𝐻1 𝐻1𝐷 𝐻𝐷1 𝐻𝐷 = 𝐹 + 𝑗η W 𝑱 − 𝐼1 𝑊1𝐷 𝑊𝐷1 𝐹 + 𝑗η W 𝑱 − 𝐼𝐷
0H
𝐽 = 2𝑓 ℎ ]
^ ^
W 𝑈 (𝐹)[𝑔
H(𝐹) − 𝑔 I(𝐹)]𝑒𝐹
𝛵 = 𝑊
H6 b
𝐹 + 𝑗η W 𝑱 − 𝐼1 0H𝑊
6H
Fisher-Lee Relation
20
All-atom MD Simulations
Current blockade is stronger for lower applied bias!
21
Detection of DNA molecule: Ionic Currents
- C. Sathe, X. Zou, J. P. Leburton, and K. Schulten. ACS Nano 2011.
2 nm 7 nm Note the sharp non-linear potential profile!
60 80 20 40 60 80 100 120 140
Diameter (nm)
20 40 0.5 1 1.5 2 2.5 3 60 80 20 40
z (Å) x (Å) (V)
b c Potential profile 4.3 V 2.5 V 0.8 V
22
Detecting Stepwise ssDNA Translocation
Conductance in the 2D Membranes due to change in electrostatic potential
0.88 0.90 0.92 0.94 10 20 30 40 2 4 6 8 10 Sheet current (nA) Permeated bases (#) Simulation time (ns)
1 2 3 4
- H. Qiu A. Sarathy, J-P Leburton and K. Schulten Nanoletters (2015)
23
Large Scale Parallel DNA Detection in Multi-pore Systems
24
Large Scale Parallel DNA Detection in Multi-pore Systems
25