From Biochemical Kinetics to Systems Biology Peter Schuster - - PowerPoint PPT Presentation

from biochemical kinetics to systems biology
SMART_READER_LITE
LIVE PREVIEW

From Biochemical Kinetics to Systems Biology Peter Schuster - - PowerPoint PPT Presentation

From Biochemical Kinetics to Systems Biology Peter Schuster Institut fr Theoretische Chemie, Universitt Wien, Austria and The Santa Fe Institute, Santa Fe, New Mexico, USA RICAM Special Semester on Quantitative Biology Linz, 05.11.2007


slide-1
SLIDE 1
slide-2
SLIDE 2

From Biochemical Kinetics to Systems Biology

Peter Schuster

Institut für Theoretische Chemie, Universität Wien, Austria and The Santa Fe Institute, Santa Fe, New Mexico, USA

RICAM Special Semester on Quantitative Biology Linz, 05.11.2007

slide-3
SLIDE 3

Web-Page for further information: http://www.tbi.univie.ac.at/~pks

slide-4
SLIDE 4

1. Biochemical kinetics and systems biology 2. Forward and inverse problems 3. Regulation kinetics and bifurcation analysis 4. Reverse engineering of dynamical systems 5. Future problems of quantitative biology

slide-5
SLIDE 5
  • 1. Biochemical kinetics and systems biology

2. Forward and inverse problems 3. Regulation kinetics and bifurcation analysis 4. Reverse engineering of dynamical systems 5. Future problems of quantitative biology

slide-6
SLIDE 6

Biochemical kinetics 1910 – 1960 Conventional enzyme kinetics 1950 – 1975 Theory of biopolymers, macroscopic properties 1958 Gene regulation through repressor binding 1965 – 1975 Allosteric effects, cooperative transitions 1965 – 1975 Theory of cooperative binding to nucleic acids 1990 - Revival of biochemical kinetics in systems biology

slide-7
SLIDE 7

Biochemical kinetics 1910 – 1960 Conventional enzyme kinetics 1950 – 1975 Theory of biopolymers, macroscopic properties 1958 Gene regulation through repressor binding 1965 – 1975 Allosteric effects, cooperative transitions 1965 – 1975 Theory of cooperative binding to nucleic acids 1990 - Revival of biochemical kinetics in systems biology

slide-8
SLIDE 8

Biochemical kinetics 1910 – 1960 Conventional enzyme kinetics 1950 – 1975 Theory of biopolymers, macroscopic properties 1958 Gene regulation through repressor binding 1965 – 1975 Allosteric effects, cooperative transitions 1965 – 1975 Theory of cooperative binding to nucleic acids 1990 - Revival of biochemical kinetics in systems biology

slide-9
SLIDE 9

Biochemical kinetics 1910 – 1960 Conventional enzyme kinetics 1950 – 1975 Theory of biopolymers, macroscopic properties 1958 Gene regulation through repressor binding 1965 – 1975 Allosteric effects, cooperative transitions 1965 – 1975 Theory of cooperative binding to nucleic acids 1990 - Revival of biochemical kinetics in systems biology

slide-10
SLIDE 10

Biochemical kinetics 1910 – 1960 Conventional enzyme kinetics 1950 – 1975 Theory of biopolymers, macroscopic properties 1958 Gene regulation through repressor binding 1965 – 1975 Allosteric effects, cooperative transitions 1965 – 1975 Theory of cooperative binding to nucleic acids 1990 - Revival of biochemical kinetics in systems biology

slide-11
SLIDE 11

Biochemical kinetics 1910 – 1960 Conventional enzyme kinetics 1950 – 1975 Theory of biopolymers, macroscopic properties 1958 Gene regulation through repressor binding 1965 – 1975 Allosteric effects, cooperative transitions 1965 – 1975 Theory of cooperative binding to nucleic acids 1990 - Revival of biochemical kinetics in systems biology

slide-12
SLIDE 12

1 2 3 4 5 6 7 8 9 10 11 12 Regulatory protein or RNA Enzyme Metabolite Regulatory gene Structural gene

A model genome with 12 genes

Sketch of a genetic and metabolic network

slide-13
SLIDE 13

A B C D E F G H I J K L 1

Biochemical Pathways

2 3 4 5 6 7 8 9 10

The reaction network of cellular metabolism published by Boehringer-Ingelheim.

slide-14
SLIDE 14

The citric acid

  • r Krebs cycle

(enlarged from previous slide).

slide-15
SLIDE 15

1. Biochemical kinetics and systems biology

  • 2. Forward and inverse problems

3. Regulation kinetics and bifurcation analysis 4. Reverse engineering of dynamical systems 5. Future problems of quantitative biology

slide-16
SLIDE 16

General conditions Initial conditions : T , p , pH , I , ... :

...

... S ,

u

Boundary conditions

boundary normal unit vector Dirichlet Neumann :

:

:

) ( x

) , ( t r g x S =

  • Time

t Concentration ( ) x t Solution curves: xi(t) Kinetic differential equations ) ; (

2

k x f x D t x + ∇ = ∂ ∂

) , , ( ; ) , , ( ; ) ; (

1 1 m n

k k k x x x k x f t d x d

K K

= = = Reaction diffusion equations

) , ( ˆ t r g x u u x

S =

∇ ⋅ = ∂ ∂

Parameter set

m , , 2 , 1 j ; ) , I , H p , p , T (

j

K K = k

The forward problem of chemical reaction kinetics (Level I)

slide-17
SLIDE 17

General conditions Initial conditions : T , p , pH , I , ... :

...

... S ,

u

Boundary conditions

boundary normal unit vector Dirichlet Neumann :

:

:

) ( x

) , ( t r g x S =

  • Time

t Concentration ( ) x t Solution curves: xi(t) Kinetic differential equations ) ; (

2

k x f x D t x + ∇ = ∂ ∂ ) , , ( ; ) , , ( ; ) ; (

1 1 m n

k k k x x x k x f t d x d K K = = = Reaction diffusion equations

) , ( ˆ t r g x u u x

S =

∇ ⋅ = ∂ ∂

Parameter set

m j I H p p T kj , , 2 , 1 ; ) , , , , ; I ( G K K =

Genome: Sequence IG

The forward problem of biochemical reaction kinetics (Level I)

slide-18
SLIDE 18

The inverse problem of biochemical reaction kinetics (Level I)

Time t Concentration Data from measurements (t ); = 1, 2, ... , x j N

j

xi (t )

j

Kinetic differential equations

) ; (

2

k x f x D t x + ∇ = ∂ ∂ ) , , ( ; ) , , ( ; ) ; (

1 1 m n

k k k x x x k x f t d x d

K K

= = = Reaction diffusion equations General conditions Initial conditions : T , p , pH , I , ... :

...

... S ,

u

Boundary conditions

boundary normal unit vector Dirichlet Neumann :

:

:

) ( x

) , ( t r g x S =

  • )

, ( ˆ t r g x u u x

S =

∇ ⋅ = ∂ ∂

Parameter set

m j I H p p T k j , , 2 , 1 ; ) , , , , ; I ( G K K

=

Genome: Sequence IG

slide-19
SLIDE 19

General conditions Initial conditions : T , p , pH , I , ... :

...

... S ,

u

Boundary conditions

boundary normal unit vector Dirichlet Neumann :

:

:

) (

x

) , ( t r g x S =

  • Kinetic differential equations

) ; ( f

2

k x x D t x + ∇ = ∂ ∂

) , , ( ; ) , , ( ; ) ; ( f

1 1

m n

k k k x x x k x t d x d

K K

= = = Reaction diffusion equations

) , ( ˆ t r g x u u x

S =

∇ ⋅ = ∂ ∂

Parameter set

m j I H p p T k j , , 2 , 1 ; ) , , , , ; I ( G K K =

Genome: Sequence IG

Bifurcation analysis

( , ; ) k k

i j k

kj ki

x t

( )

time

xn

xm

P

xn

xm

P P

xn xm

P

The forward problem of bifurcation analysis (Level II)

slide-20
SLIDE 20

The inverse problem of bifurcation analysis (Level II)

Kinetic differential equations

) ; (

2

k x f x D t x + ∇ = ∂ ∂

) , , ( ; ) , , ( ; ) ; (

1 1 m n

k k k x x x k x f t d x d

K K

= = = Reaction diffusion equations General conditions Initial conditions : T , p , pH , I , ... :

...

... S ,

u

Boundary conditions

boundary normal unit vector Dirichlet Neumann :

:

:

) (

x

) , ( t r g x S =

  • )

, ( ˆ t r g x u u x

S =

∇ ⋅ = ∂ ∂

Parameter set

m j I H p p T kj

, , 2 , 1 ; ) , , , , ; I ( G K K

=

Genome: Sequence IG

Bifurcation pattern

( , ; ) k k

i j k

k1 k2

P2

xn xm

P1

x

x

P

x

x

P

slide-21
SLIDE 21

1. Biochemical kinetics and systems biology 2. Forward and inverse problems

  • 3. Regulation kinetics and bifurcation analysis

4. Reverse engineering of dynamical systems 5. Future problems of quantitative biology

slide-22
SLIDE 22

Active states of gene regulation

slide-23
SLIDE 23

Promotor

Repressor

RNA polymerase State : inactive state

III

Promotor

Activator Repressor

RNA polymerase State : inactive state

III

Activator binding site

Inactive states of gene regulation

slide-24
SLIDE 24
slide-25
SLIDE 25

synthesis degradation Cross-regulation of two genes

slide-26
SLIDE 26

2 , 1 , ) ( : Repression ) ( : Activation

n n n

= + = + = j i p K K p F p K p p F

j j i j j j i

Gene regulatory binding functions

slide-27
SLIDE 27

2 P 2 2 P 2 2 1 P 2 1 P 1 1 2 Q 2 1 2 Q 2 2 1 Q 1 2 1 Q 1 1

) ( ) ( p d q k dt dp p d q k dt dp q d p F k dt dq q d p F k dt dq − = − = − = − =

2 2 1 1 2 2 1 1 2 1

] P [ , ] P [ , ] Q [ , ] Q [ . const ] G [ ] G [ p p q q g = = = = = = = 2 , 1 , ) ( : Repression ) ( : Activation

n n n

= + = + = j i p K K p F p K p p F

j j i j j j i

P 2 Q 2 P 2 Q 2 2 P 1 Q 1 P 1 Q 1 1 1 2 2 2 1 2 2 1 1 1

, ) ( , )) ( ( : points Stationary d d k k d d k k p F p p F F p = = = = − ϑ ϑ ϑ ϑ ϑ

Qualitative analysis of cross-regulation of two genes: Stationary points

slide-28
SLIDE 28

⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎝ ⎛ − − ∂ ∂ ∂ ∂ ∂ ∂ ∂ ∂ − − = ⎪ ⎭ ⎪ ⎬ ⎫ ⎪ ⎩ ⎪ ⎨ ⎧ ∂ ∂ = =

P P P P Q Q Q Q Q Q j i ij

d d k k p F k p F k p F k p F k d d x x a

2 1 2 1 2 2 2 1 2 2 2 1 1 1 1 1 2 1

A &

: regulation Cross

2 2 1 1

= ∂ ∂ = ∂ ∂ p F p F

K D K D P P P P Q Q Q Q

P P Q Q d k d k p F k d p F k d = − − − − ∂ ∂ − − ∂ ∂ − − = ε ε ε ε ε

2 2 1 1 1 2 2 2 2 1 1 1

I

  • A

Qualitative analysis of cross-regulation of two genes: Jacobian matrix

slide-29
SLIDE 29

K K D D D K D K K D

P Q P Q P P Q P P Q ⋅ − ⋅ = ⋅ = ⋅

K D

Q Q hence and

( )( ) ( )( ) ( )( )( )( )

P Q P Q

1 2 2 1 2 1 2 1 2 2 1 1 2 2 2 1 2 2 1 2 1 1 1 1

= ∂ ∂ ∂ ∂ − − − − − − − − − = = − − − − ∂ ∂ − ∂ ∂ − − − − − = ⋅ − ⋅ p F p F k k k k d d d d d d k p F k k p F k d d

P P Q Q P Q P Q P Q P Q P Q P Q K K D D

ε ε ε ε ε ε ε ε

1 2 2 1 P 2 P 1 Q 2 Q 1 P 2 P 1 Q 2 Q 1

) ε ( ) ε ( ) ε ( ) ε ( x F x F k k k k D D d d d d ∂ ∂ ∂ ∂ − = = + + + + +

slide-30
SLIDE 30

1 2 2 1 P 2 P 1 Q 2 Q 1 P 2 P 1 Q 2 Q 1

) ε ( ) ε ( ) ε ( ) ε ( x F x F k k k k D D d d d d ∂ ∂ ∂ ∂ − = = + + + + +

Eigenvalues of the Jacobian of the cross-regulatory two gene system

slide-31
SLIDE 31

2 P 2 P 1 Q 2 Q 1 P 2 P 1 P 2 Q 2 P 1 Q 2 P 2 Q 1 P 1 Q 1 Q 2 Q 1 Hopf P 2 P 1 Q 2 Q 1 OneD

) ( ) )( )( )( )( )( ( d d d d d d d d d d d d d d d d D d d d d D + + + + + + + + + = − =

slide-32
SLIDE 32

0 s < 0.5

  • ne stable state

E: both genes off 0.5 < s two stable states E: both genes off P: both genes on Regulatory dynamics at D 0 , act.-act., n=2

slide-33
SLIDE 33

Regulatory dynamics at D 0 , act.-rep., n=3 0 s < 1.29

  • ne stable state

P: both genes on 1.29 < s no stable state, stable limit cycle

slide-34
SLIDE 34

Regulatory dynamics at D < DHopf , act.-repr., n=3

slide-35
SLIDE 35

Regulatory dynamics at D > DHopf , act.-repr., n=3

slide-36
SLIDE 36

Regulatory dynamics at D 0 , rep.-rep., n=2 0 s < 0.79

  • ne stable state

P: both genes on 0.79 < s two stable states P1: gene 1 on, gene 2 off P2: gene 1 off, gene 2 on

slide-37
SLIDE 37

Hill coefficient: n Act.-Act. Act.-Rep. Rep.-Rep. 1 S , E S S 2 E , B(E,P) S S , B(P1,P2) 3 E , B(E,P) S , O S , B(P1,P2) 4 E , B(E,P) S , O S , B(P1,P2)

slide-38
SLIDE 38

1 1 ; 2 , 1 , ) ( : te Intermedia ) ( : Repression ) ( : Activation

n 2 3 2 1 m n n n

− ≤ ≤ = + + + + = + = + = n m j i p p p p p F p K K p F p K p p F

j j j j j i j j i j j j i

K κ κ κ

slide-39
SLIDE 39

Regulatory dynamics, int.-act., m=2, n=4

slide-40
SLIDE 40

Regulatory dynamics, rep.-int., m=2, n=4

slide-41
SLIDE 41

( )( ) ( )( ) ( )( )

ε ε ε ε ε ε − − − − ∂ ∂ − − − − − ∂ ∂ − ∂ ∂ − − − − − = ⋅ − ⋅

P Q Q P P Q Q P Q P P Q k k d d

d d p F k k d d p F k k p F k k d d

3 3 2 3 3 3 2 2 1 2 2 2 3 1 1 1 1 1

P Q P Q

2 3 1 2 3 1 3 2 1 3 2 1

p F p F p F k k k k k k D

P P P Q Q Q

∂ ∂ ∂ ∂ ∂ ∂ − =

Upscaling to more genes: n = 3

slide-42
SLIDE 42

An example analyzed and simulated by MiniCellSim

The repressilator: M.B. Ellowitz, S. Leibler. A synthetic oscillatory network of transcriptional

  • regulators. Nature 403:335-338, 2002
slide-43
SLIDE 43

Stable stationary state Limit cycle oscillations Fading oscillations caused by a stable heteroclinic orbit Hopf bifurcation Bifurcation to May-Leonhard system Increasing inhibitor strength

slide-44
SLIDE 44

P1 P2 P3

start start

The repressilator limit cycle

slide-45
SLIDE 45

P1 P2 P2 P2 P3

Stable heteroclinic orbit Unstable heteroclinic orbit

1 1 2 2 2<0 2>0 2=0

Bifurcation from limit cycle to stable heteroclinic orbit at

The repressilator heteroclinic orbit

slide-46
SLIDE 46
slide-47
SLIDE 47

) ε ( ) ε ( ) ε ( ) ε (

P P 1 Q Q 1

= + + + + + D d d d d

n n

K K

1 1 2 1 2 1 2 1 −

∂ ∂ ∂ ∂ ∂ ∂ − =

n n n P n P P Q n Q Q

p F p F p F k k k k k k D K K K

Upscaling to n genes with cyclic symmetry

slide-48
SLIDE 48

Stationarity approximation

( ) ( )

n n P P P P P P P P

K K K K x d x F k dt dx x d x F k dt dx q q d k p q q d k p p d q k dt dp p d q k dt dp

2 2 2 1 1 1 2 2 1 1 2 2 2 1 1 2 2 1 1 1 2 2 2 2 1 2 1 1 1 1 1 1 2 2 2 2 2 1 1 1 1 1

and and and and κ κ κ κ κ κ ⇒ ⇒ − = − = = = = = − = − =

slide-49
SLIDE 49

two stable states E: both genes off P: both genes on

Simplified two gene system (x1,x2): act2-act2

slide-50
SLIDE 50

two stable states P1: gene 1 on, gene 2 off P2: gene 1 off, gene 2 on

Simplified two gene system (x1,x2): rep2-rep2

slide-51
SLIDE 51

full two gene system: (q1,q2,p1,p2) simplified two gene system: (x1,x2)

Bifurcation analysis

slide-52
SLIDE 52

full two gene system: „symmetric“ (q1,q2,p1,p2)

Bifurcation analysis

full two gene system: „asymmetric“ (q1,q2,p1,p2)

slide-53
SLIDE 53

full three gene system: (q1,q2,q3,p1,p2,p3)

Bifurcation analysis

simplified three gene system: (x1,x2,x3)

slide-54
SLIDE 54

1. Biochemical kinetics and systems biology 2. Forward and inverse problems 3. Regulation kinetics and bifurcation analysis

  • 4. Reverse engineering of dynamical systems

5. Future problems of quantitative biology

slide-55
SLIDE 55

( ) ( ) ( ) ( ) ( ) { }

s s s i s i s i m m n

p p p p p p p p p x x x p x f x ∩ Σ ≡ Σ ⊕ = × ∈ = Σ ⊂ ∈ = = = ; P P P ; P P , manifold n bifurcatio P ; , , ; , , ; ;

1 1

K K K & R

( ) ( )

( )

( )

  • perator

forward , ) ( , ) ( K

s i p s i

p p p F p F p F

s

Σ ⊥

= ≡ π

( )

i i i p p

p F c p p p p p F p J

s s

) ( and

  • subject t

) ( min ) ( min

upp low

≤ ≤ ≤ − =

... formulation of the inverse problem

  • J. Lu, H.W. Engl, P. Schuster. Inverse bifurcation analysis: Application to simple gene systems.

AMB Algorithms for Molecular Biology 1, no.11, 2006.

slide-56
SLIDE 56

3 , 2 , 1 = k

Switch or oscillatory behavior in Escherichia coli T.S. Gardner, C.R. Cantor, J.J. Collins. Construction of a genetic toggle switch in Escherichia coli. Nature 403:339-342, 2000. M.R. Atkinson, M.A. Savageau, T.J. Myers, A.J. Ninfa. Development of genetic circuitry exhibiting toggle switch or oscillatory behavior in Escherichia coli. Cell 113:597-607, 2003.

slide-57
SLIDE 57

Inverse bifurcation analysis of switch or oscillatory behavior in Escherichia coli

  • J. Lu, H.W. Engl, P. Schuster. Inverse bifurcation analysis: Application to simple

gene systems. AMB Algorithms for Molecular Biology 1:11, 2006.

slide-58
SLIDE 58

δ δ β β α α = = = =

i i i i

h h , , ,

Inverse bifurcation analysis of the repressilator model

  • S. Müller, J. Hofbauer, L. Endler, C. Flamm, S. Widder, P. Schuster. A generalized

model of the repressilator. J. Math. Biol. 53:905-937, 2006.

slide-59
SLIDE 59

Inverse bifurcation analysis of the repressilator model

  • J. Lu, H.W. Engl, P. Schuster. Inverse bifurcation analysis: Application to simple

gene systems. AMB Algorithms for Molecular Biology 1:11, 2006.

slide-60
SLIDE 60

[ ] [ ] [ ] [ ]

pRB pRB ] E2F1 [ E2F1 pRB

pRB 11 11 1 1

φ − + + = J J K k dt d

m

[ ] [ ] [ ] [ ]

E2F1 pRB ] E2F1 [ E2F1 E2F1

E2F1 12 12 2 2 2 2 2 1

φ − + + + + = J J K a k k dt d

m P

[ ] [ ] [ ] [ ]

AP1 pRB' ] p [ E2F1 AP1

AP1 11 65 15 15 25

φ − + + + = J J RB J J k F dt d

m

A simple dynamical cell cycle model J.J. Tyson, A. Csikasz-Nagy, B. Novak. The dynamics of cell cycle regulation. Bioessays 24:1095-1109, 2002

slide-61
SLIDE 61

A simple dynamical cell cycle model J.J. Tyson, A. Csikasz-Nagy, B. Novak. The dynamics of cell cycle regulation. Bioessays 24:1095-1109, 2002

slide-62
SLIDE 62

Inverse bifurcation analysis of a dynamical cell cycle model

  • J. Lu, H.W. Engl, P. Schuster. Inverse bifurcation analysis: Application to simple

gene systems. AMB Algorithms for Molecular Biology 1:11, 2006.

slide-63
SLIDE 63

1. Biochemical kinetics and systems biology 2. Forward and inverse problems 3. Regulation kinetics and bifurcation analysis 4. Reverse engineering of dynamical systems

  • 5. Future problems of quantitative biology
slide-64
SLIDE 64

Challenges of quantitative biology

  • 1. Validation of data from different sources
  • 2. Low particle numbers and stochasticity
  • 3. Conformational heterogeneity of biomolecules
  • 4. High dimensionality of molecular dynamical systems
  • 5. Spatial heterogeneity of cells and cell organelles
slide-65
SLIDE 65

Challenges of quantitative biology

  • 1. Validation of data from different sources
  • 2. Low particle numbers and stochasticity
  • 3. Conformational heterogeneity of biomolecules
  • 4. High dimensionality of molecular dynamical systems
  • 5. Spatial heterogeneity of cells and cell organelles
slide-66
SLIDE 66

Challenges of quantitative biology

  • 1. Validation of data from different sources
  • 2. Low particle numbers and stochasticity
  • 3. Conformational heterogeneity of biomolecules
  • 4. High dimensionality of molecular dynamical systems
  • 5. Spatial heterogeneity of cells and cell organelles
slide-67
SLIDE 67

Challenges of quantitative biology

  • 1. Validation of data from different sources
  • 2. Low particle numbers and stochasticity
  • 3. Conformational heterogeneity of biomolecules
  • 4. High dimensionality of molecular dynamical systems
  • 5. Spatial heterogeneity of cells and cell organelles
slide-68
SLIDE 68

Challenges of quantitative biology

  • 1. Validation of data from different sources
  • 2. Low particle numbers and stochasticity
  • 3. Conformational heterogeneity of biomolecules
  • 4. High dimensionality of molecular dynamical systems
  • 5. Spatial heterogeneity of cells and cell organelles
slide-69
SLIDE 69

Suitable systems for upscaling

  • 1. Linear systems via large eigenvalue problems
  • 2. Cascades
  • 3. Cyclic systems
  • 4. Sufficiently simple networks and flux analysis
slide-70
SLIDE 70

Challenges of quantitative biology

  • 1. Validation of data from different sources
  • 2. Low particle numbers and stochasticity
  • 3. Conformational heterogeneity of biomolecules
  • 4. High dimensionality of molecular dynamical systems
  • 5. Spatial heterogeneity of cells and cell organelles
slide-71
SLIDE 71

The bacterial cell as an example for the simplest form of autonomous life The human body: 1014 cells = 1013 eukaryotic cells + 91013 bacterial (prokaryotic) cells, and 200 eukaryotic cell types The spatial structure of the bacterium Escherichia coli

slide-72
SLIDE 72

Acknowledgement of support

Fonds zur Förderung der wissenschaftlichen Forschung (FWF) Projects No. 09942, 10578, 11065, 13093 13887, and 14898 Wiener Wissenschafts-, Forschungs- und Technologiefonds (WWTF) Project No. Mat05 Jubiläumsfonds der Österreichischen Nationalbank Project No. Nat-7813 European Commission: Contracts No. 98-0189, 12835 (NEST) Austrian Genome Research Program – GEN-AU: Bioinformatics Network (BIN) Österreichische Akademie der Wissenschaften Siemens AG, Austria Universität Wien and the Santa Fe Institute

Universität Wien

slide-73
SLIDE 73

Coworkers

Peter Stadler, Bärbel M. Stadler, Universität Leipzig, GE Paul E. Phillipson, University of Colorado at Boulder, CO Heinz Engl, Philipp Kügler, James Lu, Stefan Müller, RICAM Linz, AT Jord Nagel, Kees Pleij, Universiteit Leiden, NL Walter Fontana, Harvard Medical School, MA Christian Reidys, Christian Forst, Los Alamos National Laboratory, NM Ulrike Göbel, Walter Grüner, Stefan Kopp, Jaqueline Weber, Institut für Molekulare Biotechnologie, Jena, GE Ivo L.Hofacker, Christoph Flamm, Andreas Svrček-Seiler, Universität Wien, AT Kurt Grünberger, Michael Kospach , Andreas Wernitznig, Stefanie Widder, Stefan Wuchty, Universität Wien, AT Jan Cupal, Stefan Bernhart, Lukas Endler, Ulrike Langhammer, Rainer Machne, Ulrike Mückstein, Hakim Tafer, Thomas Taylor, Universität Wien, AT

Universität Wien

slide-74
SLIDE 74

Web-Page for further information: http://www.tbi.univie.ac.at/~pks

slide-75
SLIDE 75